Sample records for early mantle differentiation

  1. Early Terrestrial Mantle Differentiation Recorded in Paleoarchean Komatiites

    NASA Astrophysics Data System (ADS)

    Puchtel, I. S.; Blichert-Toft, J.; Touboul, M.; Horan, M. F.; Walker, R. J.

    2016-12-01

    Geochmical signatures generated in the manle as a result of radioactive decay of short- and long-lived nuclides can be used to constrain the timing of formation and the nature of now mostly vanished early terrestrial reservoirs. The 3.55 Ga komatiites from the Schapenburg Greenstone Remnant (SGR) located in the Barberton Greenstone Belt in South Africa have a unique combination of trace element abundances and isotopic compositions that place strong constraints on the origin of these reservoirs. The SGR komatiites define a Re-Os isochron with an age of 3550±87 Ma and an initial γ187Os = +3.7±0.2 (2SD). The absolute HSE abundances in the mantle source of the SGR komatiite system are estimated to be only 29±5% of those in the present-day bulk silicate Earth (BSE) estimates. The SGR komatiites show coupled depletion, relative to the modern mantle, in 142Nd and 182W (μ142Nd = -5.0±2.8, μ182W = -8.4±4.5), the decay products of the short-lived 146Sm and 182Hf nuclides, respectively, indicating derivation from a mantle domain that was enriched in incompatible elements 30 Ma after Solar System formation. Early Hadean contributors to this mantle domain could include high-pressure fractionates from a primordial magma ocean. By contrast, the long-lived Sm-Nd and Lu-Hf isotope systems (ɛ143Nd = +2.4±0.1, ɛ176Hf = +5.7±0.3) indicate that the mantle domain that the SGR komatiites were ultimately derived from underwent additional processing after the early Hadean, including melt depletion at lower pressures. The preservation of early-formed 182W and 142Nd anomalies in the mantle until at least 3.55 Ga indicates that the products of early planetary differentiation survived both later planetary accretion and convective mantle mixing during the Hadean. This study lends further support to the notion that variable late accretion, by itself, cannot account for all of the observed W isotope and absolute and relative HSE abundance variations in the Archean mantle recorded by

  2. Early differentiation and volatile accretion recorded in deep-mantle neon and xenon.

    PubMed

    Mukhopadhyay, Sujoy

    2012-06-06

    The isotopes (129)Xe, produced from the radioactive decay of extinct (129)I, and (136)Xe, produced from extinct (244)Pu and extant (238)U, have provided important constraints on early mantle outgassing and volatile loss from Earth. The low ratios of radiogenic to non-radiogenic xenon ((129)Xe/(130)Xe) in ocean island basalts (OIBs) compared with mid-ocean-ridge basalts (MORBs) have been used as evidence for the existence of a relatively undegassed primitive deep-mantle reservoir. However, the low (129)Xe/(130)Xe ratios in OIBs have also been attributed to mixing between subducted atmospheric Xe and MORB Xe, which obviates the need for a less degassed deep-mantle reservoir. Here I present new noble gas (He, Ne, Ar, Xe) measurements from an Icelandic OIB that reveal differences in elemental abundances and (20)Ne/(22)Ne ratios between the Iceland mantle plume and the MORB source. These observations show that the lower (129)Xe/(130)Xe ratios in OIBs are due to a lower I/Xe ratio in the OIB mantle source and cannot be explained solely by mixing atmospheric Xe with MORB-type Xe. Because (129)I became extinct about 100 million years after the formation of the Solar System, OIB and MORB mantle sources must have differentiated by 4.45 billion years ago and subsequent mixing must have been limited. The Iceland plume source also has a higher proportion of Pu- to U-derived fission Xe, requiring the plume source to be less degassed than MORBs, a conclusion that is independent of noble gas concentrations and the partitioning behaviour of the noble gases with respect to their radiogenic parents. Overall, these results show that Earth's mantle accreted volatiles from at least two separate sources and that neither the Moon-forming impact nor 4.45 billion years of mantle convection has erased the signature of Earth's heterogeneous accretion and early differentiation.

  3. Evidence for extreme mantle fractionation in early Archaean ultramafic rocks from northern Labrador

    NASA Technical Reports Server (NTRS)

    Collerson, Kenneth D.; Campbell, Lisa M.; Weaver, Barry L.; Palacz, Zenon A.

    1991-01-01

    Samarium-neodymium isotope data for tectonically interleaved fragments of lithospheric mantle and meta-komatiite from the North Atlantic craton provide the first direct record of mantle differentiation before 3,800 Myr ago. The results confirm the magnitude of light-rare-earth-element depletion in the early mantle, and also its depleted neodymium isotope composition. The mantle fragments were able to retain these ancient geochemical signatures by virtue of having been tectonically incorporated in buoyant felsic crust, thus escaping recycling and homogenization by mantle convection.

  4. Deformation of a crystalline olivine aggregate containing two immiscible liquids: Implications for early core-mantle differentiation

    NASA Astrophysics Data System (ADS)

    Cerantola, V.; Walte, N. P.; Rubie, D. C.

    2015-05-01

    Deformation-assisted segregation of metallic and sulphidic liquid from a solid peridotitic matrix is a process that may contribute to the early differentiation of small planetesimals into a metallic core and a silicate mantle. Here we present results of an experimental study using a simplified system consisting of a polycrystalline Fo90-olivine matrix containing a small percentage of iron sulphide and a synthetic primitive MORB melt, in order to investigate whether the silicate melt enhances the interconnection and segregation of FeS liquid under deformation conditions at varying strain rates. The experiments have been performed at 2 GPa, 1450 °C and strain rates between 1 ×10-3s-1 to 1 ×10-5s-1. Our results show that the presence of silicate melt actually hinders the migration and segregation of sulphide liquid by reducing its interconnectivity. At low to moderate strain rates the sulphide liquid pockets preserved a roundish shape, showing the liquid behavior is governed mainly by surface tension rather than by differential stress. Even at the highest strain rates, insignificant FeS segregation and interconnection were observed. On the other hand the basaltic melt was very mobile during deformation, accommodating part of the strain, which led to its segregation from the matrix at high bulk strains leaving the sulphide liquid stranded in the olivine matrix. Hence, we conclude that deformation-induced percolation of sulphide liquid does not contribute to the formation of planetary cores after the silicate solidus is overstepped. A possible early deformation enhanced core-mantle differentiation after overstepping the Fe-S solidus is not possible between the initial formation of silicate melt and the formation of a widespread magma ocean.

  5. Early Earth differentiation [rapid communication

    NASA Astrophysics Data System (ADS)

    Walter, Michael J.; Trønnes, Reidar G.

    2004-09-01

    The birth and infancy of Earth was a time of profound differentiation involving massive internal reorganization into core, mantle and proto-crust, all within a few hundred million years of solar system formation ( t0). Physical and isotopic evidence indicate that the formation of iron-rich cores generally occurred very early in planetesimals, the building blocks of proto-Earth, within about 3 million years of t0. The final stages of terrestrial planetary accretion involved violent and tremendously energetic giant impacts among core-segregated Mercury- to Mars-sized objects and planetary embryos. As a consequence of impact heating, the early Earth was at times partially or wholly molten, increasing the likelihood for high-pressure and high-temperature equilibration among core- and mantle-forming materials. The Earth's silicate mantle harmoniously possesses abundance levels of the siderophile elements Ni and Co that can be reconciled by equilibration between iron alloy and silicate at conditions comparable to those expected for a deep magma ocean. Solidification of a deep magma ocean possibly involved crystal-melt segregation at high pressures, but subsequent convective stirring of the mantle could have largely erased nascent layering. However, primitive upper mantle rocks apparently have some nonchondritic major and trace element refractory lithophile element ratios that can be plausibly linked to early mantle differentiation of ultra-high-pressure mantle phases. The geochemical effects of crystal fractionation in a deep magma ocean are partly constrained by high-pressure experimentation. Comparison between compositional models for the primitive convecting mantle and bulk silicate Earth generally allows, and possibly favors, 10-15% total fractionation of a deep mantle assemblage comprised predominantly of Mg-perovskite and with minor but geochemically important amounts of Ca-perovskite and ferropericlase. Long-term isolation of such a crystal pile is generally

  6. Early Planetary Differentiation: Comparative Planetology

    NASA Technical Reports Server (NTRS)

    Jones, John H.

    2006-01-01

    We currently have extensive data for four different terrestrial bodies of the inner solar system: Earth, the Moon, Mars, and the Eucrite Parent Body [EPB]. All formed early cores; but all(?) have mantles with elevated concentrations of highly sidero-phile elements, suggestive of the addition of a late "veneer". Two appear to have undergone extensive differentiation consistent with a global magma ocean. One appears to be inconsistent with a simple model of "low-pressure" chondritic differentiation. Thus, there seems to be no single, simple paradigm for understand-ing early differentiation.

  7. Convective Differentiation of the Earth's Mantle

    NASA Astrophysics Data System (ADS)

    Hansen, U.; Schmalzl, J.; Stemmer, K.

    2007-05-01

    The differentiation of the Earth is likely to be influenced by convective motions within the early mantle. Double- diffusive convection (d.d.c), driven by thermally and compositionally induced density differences is considered as a vital mechanism behind the dynamic differentiation of the early mantle.. We demonstrate that d.d.c can lead to layer formation on a planetary scale in the diffusive regime where composition stabilizes the system whil heat provides the destabilizing force. Choosing initial conditions in which a stable compositional gradient overlies a hot reservoir we mimic the situation of a planet in a phase after core formation. Differently from earlier studies we fixed the temperature rather than the heat flux at the lower boundary, resembling a more realistic condition for the core-mantle boundary. We have carried out extended series of numerical experiments, ranging from 2D calculations in constant viscosity fluids to fully 3D experiments in spherical geometry with strongly temperature dependent viscosity. The buoyancy ratio R and the Lewis number Le are the important dynamical parameters. In all scenarios we could identify a parameter regime where the non-layered initial structure developed into a state consisting of several, mostly two layers. Initially plumes from the bottom boundary homogenize a first layer which subsequently thickens. The bottom layer heats up and then convection is initiated in the top layer. This creates dynamically (i.e. without jump in the material behavior) a stack of separately convecting layers. The bottom layer is significantly thicker than the top layer. Strongly temperature dependent viscosity leads to a more complex evolution The formation of the bottom layer is followed by the generation of several layers on top. Finally the uppermost layer starts to convect. In general, the multilayer structure collapses into a two layer system. We employed a numerical technique, allowing for a diffusion free treatment of the

  8. Primary differentiation in the early Earth: Nd and Sr isotopic evidence from diamondiferous eclogites for both old depleted and old enriched mantle, Yakutia, Siberia

    NASA Technical Reports Server (NTRS)

    Snyder, Gregory A.; Jerde, Eric A.; Taylor, Lawrence A.; Halliday, Alex N.; Sobolev, Vladimir N.; Sobolev, Nickolai V.; Clayton, Robert N.; Mayeda, Toshiko K.; Deines, Peter

    1993-01-01

    Ancient, stable, continental cratons possess thick, subcontinental-lithospheric mantle 'keels' which favor particularly the emplacement of diamondiferous kimberlites and included peridotites and eclogites. These refractory mantle samples of the roots provide hard constraints on the theories of formation, growth, and evolution of these cratons. Xenoliths containing only primary garnet and clinopyroxene (eclogites), although rare in most kimberlites, can retain the geochemical signatures of their parent protoliths (e.g., subducted oceanic crust, ancient mantle) thus offering the opportunity to address mantle processes which may have taken place at earlier times in the Earth's history. In fact, it has been postulated that some eclogites are residues from the accretion of the early Earth. Nd and Sr isotopic data are presented which may be interpreted as evidence of an early (greater than 4 Ga) mantle differentiation event. The kimberlites of Yakutia are located both marginal and central to the Siberian craton, and a wide variety of xenoliths are present within them. The Siberian mantle samples have received little attention in the western world, largely because suitable suites of Yakutian samples have not been readily available. Importantly, there is evidence that metasomatism of the Siberian lithosphere has been considerably less intense or extensive than for the Kaapvaal craton. Therefore, it should be considerably easier to elicit the igneous/metamorphic histories of Siberian kimberlitic xenoliths. One of the notable features of the Siberian eclogites is the common appearance of diamonds, especially in the Mir and Udachnaya pipes. In all, eight eclogite samples (eight garnet separates and eight clinopyroxene separates) have been analyzed to date on the Udachnaya pipe, seven from our group.

  9. Eastern Indian 3800-million-year-old crust and early mantle differentiation

    USGS Publications Warehouse

    Basu, A.R.; Ray, S.L.; Saha, A.K.; Sarkar, S.N.

    1981-01-01

    Samarium-neodymium data for nine granitic and tonalite gneisses occurring as remnants within the Singhbhum granite batholith in eastern India define an isochron of age 3775 ?? 89 ?? 106 years with an initial 143Nd/144Nd ratio of 0.50798 ?? 0.00007. This age contrasts with the rubidium-strontium age of 3200 ?? 106 years for the same suite of rocks. On the basis of the new samarium-neodynium data, field data, and petrologic data, a scheme of evolution is proposed for the Archean crust in eastern India. The isotopic data provide evidence that parts of the earth's mantle were already differentiated with respect to the chondritic samarium-neodymium ratio 3800 ?? 106 years ago.

  10. Iron Speciation in Minerals and Melts at High Pressure: Implications for the Redox Evolution of the Early Mantle

    NASA Astrophysics Data System (ADS)

    Armstrong, K.; Frost, D. J.; McCammon, C. A.; Rubie, D. C.; Boffa Ballaran, T.; Miyajima, N.

    2016-12-01

    During the differentiation of the early Earth, the silicates of the mantle must have been in equilibrium with core-forming metal iron, as indicated by the depletion of siderophile elements from the mantle. Studies of ancient rocks suggest that by at least 3.9 Ga, the upper mantle was 4-5 log units more oxidized than metal saturation implies (Delano 2001). The process(es) by which the mantle was oxidized is unclear, but has implications for the timing of accretion, differentiation, and volatile delivery to the early Earth, as well as evolution of the early atmosphere. One plausible oxidation mechanism is suggested by the tendency of high-pressure silicate minerals to favor Fe3+ over Fe2+ in their structures, even at metal saturation. This preference in the lower mantle mineral bridgmanite has been proposed to drive the disproportionation reaction of FeO to form Fe­2O3 and iron metal (Frost and McCammon 2008). We have performed experiments at the Ru-RuO2 fO2 buffer which show that silicate melts may mirror this behavior and Fe3+ may be stabilized with pressure for a constant fO2; by 21 GPa, the previously observed trend of Fe3+ decreasing with pressure (O'Neill, 2006) reverses and ferric iron content had increased. If this is also the case at lower oxygen fugacities, FeO disproportionation may have occurred at the base of an early magma ocean, establishing a redox gradient similar to what is presumed for the mantle today. Here we report results of further multianvil and diamond anvil cell experiments exploring the plausibility of FeO disproportionation driving mantle oxidation. Experiments investigating Fe speciation in high pressure melts at variable fO2 will be discussed along with results of diamond anvil cell experiments investigating ferric iron content of lower mantle minerals at metal saturation.

  11. Evidence from coupled (Sm-147)-(Nd-143) and (Sm-146)-(Nd-142) systematics for very early (4.5-Gyr) differentiation of the earth's mantle

    NASA Technical Reports Server (NTRS)

    Harper, Charles L., Jr.; Jacobsen, Stein B.

    1992-01-01

    Evidence for early differentiation of the earth's mantle is presented based on measurements of Nd-143/Nd-144 and Nd-142/Nd-144 ratios in an approximately 3.8 Gyr-old supracrustal rock from Isua, West Greenland. Coupled (Sm-146,147)-(Nd-142,143) systematics suggest that the fractionation of Sm/Nd took place 4.44-4.54 Gyr ago, due to extraction of a light rare earth element-enriched primordial crust.

  12. Experimental Constraints on the Chemical Differentiation of Mercurys Mantle

    NASA Technical Reports Server (NTRS)

    Boujibar, A.; Righter, K.; Pando, K.; Danielson, L.

    2015-01-01

    Mercury is known as being the most reduced terrestrial planet with the highest core/mantle ratio. Results from MESSENGER spacecraft have shown that its surface is FeO-poor (2-4 wt%) and S-rich (up to 6-7 wt%), which confirms the reducing nature of its silicate mantle. In addition several features suggest important melting stages of the Mercurian mantle: widespread volcanic deposits on its surface, a high crustal thickness (approximately 10% of the planet's volume) and chemical compositions of its surface suggesting several stages of differentiation and remelting processes. Therefore it is likely that igneous processes like magma ocean crystallization and continuous melting have induced chemical and mineralogical heterogeneities in the Mercurian mantle. The extent and nature of compositional variations produced by partial melting remains poorly constrained for the particular compositions of Mercury (very reducing conditions, low FeO-contents and high sulfur-contents). Melting experiments with bulk Mercury-analogue compositions are scarce and with poorly con-trolled starting compositions. Therefore additional experimental data are needed to better understand the differentiation processes that lead to the observed chemical compositions of Mercury's surface.

  13. Global-scale water circulation in the Earth's mantle: Implications for the mantle water budget in the early Earth

    NASA Astrophysics Data System (ADS)

    Nakagawa, Takashi; Spiegelman, Marc W.

    2017-04-01

    We investigate the influence of the mantle water content in the early Earth on that in the present mantle using numerical convection simulations that include three processes for redistribution of water: dehydration, partitioning of water into partially molten mantle, and regassing assuming an infinite water reservoir at the surface. These models suggest that the water content of the present mantle is insensitive to that of the early Earth. The initial water stored during planetary formation is regulated up to 1.2 OMs (OM = Ocean Mass; 1.4 ×1021 kg), which is reasonable for early Earth. However, the mantle water content is sensitive to the rheological dependence on the water content and can range from 1.2 to 3 OMs at the present day. To explain the evolution of mantle water content, we computed water fluxes due to subducting plates (regassing), degassing and dehydration. For weakly water dependent viscosity, the net water flux is almost balanced with those three fluxes but, for strongly water dependent viscosity, the regassing dominates the water cycle system because the surface plate activity is more vigorous. The increased convection is due to enhanced lubrication of the plates caused by a weak hydrous crust for strongly water dependent viscosity. The degassing history is insensitive to the initial water content of the early Earth as well as rheological strength. The degassing flux from Earth's surface is calculated to be approximately O (1013) kg /yr, consistent with a coupled model of climate evolution and mantle thermal evolution.

  14. Accessory Mineral Records of Early Earth Crust-Mantle Systematics: an Example From West Greenland

    NASA Astrophysics Data System (ADS)

    Storey, C. D.; Hawkesworth, C. J.

    2008-12-01

    Conditions for the formation and the nature of Earth's early crust are enigmatic due to poor preservation. Before c.4 Ga the only archives are detrital minerals eroded from earlier crust, such as the Jack Hills zircons in western Australia, or extinct isotope systematics. Zircons are particularly powerful since they retain precise records of their ages of crystallisation, and the Lu-Hf radiogenic isotope and O stable isotope systematics of the reservoir from which they crystallised. In principle, this allows insight into the nature of the crust, the mantle reservoir from which the melt was extracted and any reworked material incorporated into that melt. We have used in situ methods to measure U-Pb, O and Lu-Hf within single zircon crystals from tonalitic gneisses from West Greenland in the vicinity of the Isua Supracrustal Belt. They have little disturbed ages of c.3.8 Ga, mantle-like O isotope signatures and Lu-Hf isotope signatures that lie on the CHUR evolution line at 3.8 Ga. These samples have previously been subjected to Pb isotope feldspar and 142Nd whole rock analysis and have helped constrain models in which early differentiation of a proto-crust must have occurred. The CHUR-like Lu-Hf signature, along with mantle-like O signature from these zircons suggests juvenile melt production at 3.8 Ga from undifferentiated mantle, yet the other isotope systems preclude this possibility. Alternatively, this is further strong evidence for a heterogeneous mantle in the early Earth. Whilst zircons afford insight into the nature of the early crust and mantle, it is through the Sm-Nd system that the mantle has traditionally been viewed. Titanite often contains several thousand ppm Nd, making it amenable to precise analysis, and is a common accessory phase. It has a reasonably high closure temperature for Pb and O, and it can retain cores with older ages and distinct REE chemistry. It is often the main accessory phase alongside zircon, and it is the main carrier of Nd

  15. Radiogenic ingrowth in systems with multiple reservoirs: applications to the differentiation of the mantle-crust system

    NASA Astrophysics Data System (ADS)

    Albarède, Francis

    2001-06-01

    the last two ratios and the Nd and Hf secular evolution curves of mantle-derived material require the presence of deep hidden reservoirs that interacts with the depleted upper mantle. It is suggested that the most fertile lithospheric oceanic plates, in particular those loaded with plume heads, preferentially sink to the bottom of the mantle. The terrestrial mantle is therefore most likely chemically heterogeneous and models of Earth compositions based on a primitive lower mantle should be abandoned. In contrast, the transient-dominated 207Pb/ 204Pb and 4He/ 3He ratios can be used to model the early differentiation of the planet.

  16. Early episodes of high-pressure core formation preserved in plume mantle

    NASA Astrophysics Data System (ADS)

    Jackson, Colin R. M.; Bennett, Neil R.; Du, Zhixue; Cottrell, Elizabeth; Fei, Yingwei

    2018-01-01

    The decay of short-lived iodine (I) and plutonium (Pu) results in xenon (Xe) isotopic anomalies in the mantle that record Earth’s earliest stages of formation. Xe isotopic anomalies have been linked to degassing during accretion, but degassing alone cannot account for the co-occurrence of Xe and tungsten (W) isotopic heterogeneity in plume-derived basalts and their long-term preservation in the mantle. Here we describe measurements of I partitioning between liquid Fe alloys and liquid silicates at high pressure and temperature and propose that Xe isotopic anomalies found in modern plume rocks (that is, rocks with elevated 3He/4He ratios) result from I/Pu fractionations during early, high-pressure episodes of core formation. Our measurements demonstrate that I becomes progressively more siderophile as pressure increases, so that portions of mantle that experienced high-pressure core formation will have large I/Pu depletions not related to volatility. These portions of mantle could be the source of Xe and W anomalies observed in modern plume-derived basalts. Portions of mantle involved in early high-pressure core formation would also be rich in FeO, and hence denser than ambient mantle. This would aid the long-term preservation of these mantle portions, and potentially points to their modern manifestation within seismically slow, deep mantle reservoirs with high 3He/4He ratios.

  17. Re-Os Isotopic Constraints on the Chemical Evolution and Differentiation of the Martian Mantle

    NASA Technical Reports Server (NTRS)

    Brandon, Alan D.; Walker, Richard J.

    2002-01-01

    The (187)Re-187Os isotopic systematics of SNC meteorites, thought to be from Mars, provide valuable information regarding the chemical processes that affected the Martian mantle, particularly with regard to the relative abundances of highly siderophile elements (HSE). Previously published data (Birck and Allegre 1994, Brandon et al. 2000), and new data obtained since these studies, indicate that the HSE and Os isotopic composition of the Martian mantle was primarily set in its earliest differentiation history. If so, then these meteorites provide key constraints on the processes that lead to variation in HSE observed in not only Mars, but also Earth, the Moon and other rocky bodies in the Solar System. Processes that likely have an effect on the HSE budgets of terrestrial mantles include core formation, magma ocean crystallization, development of juvenile crust, and the addition of a late veneer. Each of these processes will result in different HSE variation and the isotopic composition of mantle materials and mantle derived lavas. Two observations on the SNC data to present provide a framework for which to test the importance of each of these processes. First, the concentrations of Re and Os in SNC meteorites indicate that they are derived from a mantle that has similar concentrations to the Earth's mantle. Such an observation is consistent with a model where a chondritic late veneer replenished the Earth and Martian mantles subsequent to core formation on each planet. Alternative models to explain this observation do exist, but will require additional data to test the limitations of each. Second, Re-Os isotopic results from Brandon et al. (2000) and new data presented here, show that initial yos correlates with variations in the short-lived systems of (182)Hf- (182)W and (142)Sm-142Nd in the SNC meteorites (epsilon(sub W) and epsilon(sub 142Nd)). These systematics require an isolation of mantle reservoirs during the earliest differentiation history of Mars, and

  18. Seismological Signature of Chemical Differentiation of Earth's Upper Mantle

    NASA Astrophysics Data System (ADS)

    Matsukage, K. N.; Nishihara, Y.; Karato, S.

    2004-12-01

    Chemical differentiation from a primitive rock (such as pyrolite) to harzburgite due to partial melting and melt extraction is one of the most important mechanisms that causes the chemical heterogeneity in Earth's upper mantle. In this study, we investigate the seismic signature of chemical differentiation that helps mapping chemical heterogeneity in the upper mantle. The relation between chemical differentiation and its seismological signature is not straightforward because a large number of unknown parameters are involved although the seismological observations provide only a few parameters (e.g., VP, VS, QP). Therefore it is critical to identify a small number of parameters by which the gross trend of chemical evolution can be described. The variation in major element composition in natural samples reflect complicated processes that include not only partial melting but also other complex processes (e.g., metasomatism, influx melting). We investigate the seismic velocities of hypothetical but well-defined simple chemical differentiation processes (e.g., partial melting of various pressure conditions, addition of Si-rich melt or fluid), which cover the chemical variation of the natural mantle peridotites with various tectonic settings (mid ocean ridge, island arc and continent). The seismic velocities of the peridotites were calculated to 13 GPa and 1730 K. We obtained two major conclusions. First is that the variations of seismic velocities of upper mantle peridotites can be interpreted in terms of a few distinct parameters. For one class of peridotites which is formed by simple partial melting (e.g. mid-ocean ridges peridotites), seismic velocities can be described in terms of one parameter, namely Mg# (=Mg/(Mg+Fe) atomic ratio). In contrast, some of the peridotites in the continental (cratonic) environment with high silica content and high Mg# need at least two parameters (such as Mg# and Opx# (the volume fraction of orthopyroxene)) are needed to characterize

  19. Long-term preservation of early formed mantle heterogeneity by mobile lid convection: Importance of grainsize evolution

    NASA Astrophysics Data System (ADS)

    Foley, Bradford J.; Rizo, Hanika

    2017-10-01

    The style of tectonics on the Hadean and Archean Earth, particularly whether plate tectonics was in operation or not, is debated. One important, albeit indirect, constraint on early Earth tectonics comes from observations of early-formed geochemical heterogeneities: 142Nd and 182W anomalies recorded in Hadean to Phanerozoic rocks from different localities indicate that chemically heterogeneous reservoirs, formed during the first ∼500 Myrs of Earth's history, survived their remixing into the mantle for over 1 Gyrs. Such a long mixing time is difficult to explain because hotter mantle temperatures, expected for the early Earth, act to lower mantle viscosity and increase convective vigor. Previous studies found that mobile lid convection typically erases heterogeneity within ∼100 Myrs under such conditions, leading to the hypothesis that stagnant lid convection on the early Earth was responsible for the observed long mixing times. However, using two-dimensional Cartesian convection models that include grainsize evolution, we find that mobile lid convection can preserve heterogeneity at high mantle temperature conditions for much longer than previously thought, because higher mantle temperatures lead to larger grainsizes in the lithosphere. These larger grainsizes result in stronger plate boundaries that act to slow down surface and interior convective motions, in competition with the direct effect temperature has on mantle viscosity. Our models indicate that mobile lid convection can preserve heterogeneity for ≈0.4-1 Gyrs at early Earth mantle temperatures when the initial heterogeneity has the same viscosity as the background mantle, and ≈1-4 Gyrs when the heterogeneity is ten times more viscous than the background mantle. Thus, stagnant lid convection is not required to explain long-term survival of early formed geochemical heterogeneities, though these heterogeneities having an elevated viscosity compared to the surrounding mantle may be essential for their

  20. Seismic Heterogeneity Caused by Oceanic Crust Differentiation and Segregation in the Convecting Mantle

    NASA Astrophysics Data System (ADS)

    Xie, S.; Tackley, P. J.

    2003-12-01

    This presentation focuses on the seismic signature of mantle heterogeneity associated with crustal differentiation and segregation in the lower mantle. Segregation of subducted oceanic crust above the CMB has often been invoked as a way of explaining the isotopic signature of OIB geochemical endmembers such as HIMU. Here a mantle convection model that includes melting-induced differentiation and plate tectonics is run for billions of years and the resulting thermo-chemical heterogeneity is studied. Statistical diagnostics such as radial correlation functions (Jordan et al., 1993) and spectral heterogeneity maps (Tackley et al., 1994) are used to characterize the observational signature of the thermo-chemical structures and compare them to global seismic tomographic models. In the reference case, crust is denser than the background mantle at the CMB. Due to this density contrast, the crustal material forms a thick and dense layer at the bottom of the mantle, although the layer interface is not sharp as is commonly obtained in models where a layer is inserted a priori. An enormous amount of long-wavelength volumetric heterogeneity is found in the lower mantle. The presence of oceanic crust near the surface also contributes to heterogeneity at the top of the mantle. In cases where the subducted crust is neutrally buoyant or buoyant in the deepest mantle, a large amount of heterogeneity instead exists in the the mid-mantle region, which is not observed in tomographic models of the real Earth. Unlike the reference case with a thick layer at the bottom of the mantle, these cases have heterogeneity right at the CMB, and this strong heterogeneity exists at both short and long wavelength. When comparing to Earth, it appears that models in which dense subducted crust settles into a layer above the CMB are consistent with constraints from seismic tomography; such a layer is therefore a viable location for the storage of geochemical endmembers.

  1. Early differentiation of the Earth and the Moon.

    PubMed

    Bourdon, Bernard; Touboul, Mathieu; Caro, Guillaume; Kleine, Thorsten

    2008-11-28

    We examine the implications of new 182W and 142Nd data for Mars and the Moon for the early evolution of the Earth. The similarity of 182W in the terrestrial and lunar mantles and their apparently differing Hf/W ratios indicate that the Moon-forming giant impact most probably took place more than 60Ma after the formation of calcium-aluminium-rich inclusions (4.568Gyr). This is not inconsistent with the apparent U-Pb age of the Earth. The new 142Nd data for Martian meteorites show that Mars probably has a super-chondritic Sm/Nd that could coincide with that of the Earth and the Moon. If this is interpreted by an early mantle differentiation event, this requires a buried enriched reservoir for the three objects. This is highly unlikely. For the Earth, we show, based on new mass-balance calculations for Nd isotopes, that the presence of a hidden reservoir is difficult to reconcile with the combined 142Nd-143Nd systematics of the Earth's mantle. We argue that a likely possibility is that the missing component was lost during or prior to accretion. Furthermore, the 142Nd data for the Moon that were used to argue for the solidification of the magma ocean at ca 200Myr are reinterpreted. Cumulate overturn, magma mixing and melting following lunar magma ocean crystallization at 50-100Myr could have yielded the 200Myr model age.

  2. On the temporal evolution of long-wavelength mantle structure of the Earth since the early Paleozoic

    NASA Astrophysics Data System (ADS)

    Zhong, Shijie; Rudolph, Maxwell L.

    2015-05-01

    The seismic structure of the Earth's lower mantle is characterized by a dominantly degree-2 pattern with the African and Pacific large low shear velocity provinces (i.e., LLSVP) that are separated by circum-Pacific seismically fast anomalies. It is important to understand the origin of such a degree-2 mantle structure and its temporal evolution. In this study, we investigated the effects of plate motion history and mantle viscosity on the temporal evolution of the lower mantle structure since the early Paleozoic by formulating 3-D spherical shell models of thermochemical convection. For convection models with realistic mantle viscosity and no initial structure, it takes about ˜50 Myr to develop dominantly degree-2 lower mantle structure using the published plate motion models for the last either 120 Ma or 250 Ma. However, it takes longer time to develop the mantle structure for more viscous mantle. While the circum-Pangea subduction in plate motion history models promotes the formation of degree-2 mantle structure, the published pre-Pangea plate motions before 330 Ma produce relatively cold lower mantle in the African hemisphere and significant degree-1 structure in the early Pangea (˜300 Ma) or later times, even if the lower mantle has an initially degree-2 structure and a viscosity as high as 1023 Pas. This suggests that the African LLSVP may not be stationary since the early Paleozoic. With the published plate motion models and lower mantle viscosity of 1022 Pas, our mantle convection models suggest that the present-day degree-2 mantle structure may have largely been formed by ˜200 Ma.

  3. Effects of Earth's rotation on the early differentiation of a terrestrial magma ocean

    NASA Astrophysics Data System (ADS)

    Maas, Christian; Hansen, Ulrich

    2015-11-01

    Similar to other terrestrial planets like Moon and Mars, Earth experienced a magma ocean period about 4.5 billion years ago. On Earth differentiation processes in the magma ocean set the initial conditions for core formation and mantle evolution. During the magma ocean period Earth was rotating significantly faster than today. Further, the viscosity of the magma was low, thus that planetary rotation potentially played an important role for differentiation. However, nearly all previous studies neglect rotational effects. All in all, our results suggest that planetary rotation plays an important role for magma ocean crystallization. We employ a 3-D numerical model to study crystal settling in a rotating and vigorously convecting early magma ocean. We show that crystal settling in a terrestrial magma ocean is crucially affected by latitude as well as by rotational strength and crystal density. Due to rotation an inhomogeneous accumulation of crystals during magma ocean solidification with a distinct crystal settling between pole and equator could occur. One could speculate that this may have potentially strong effects on the magma ocean solidification time and the early mantle composition. It could support the development of a basal magma ocean and the formation of anomalies at the core-mantle boundary in the equatorial region, reaching back to the time of magma ocean solidification.

  4. Archean crust-mantle geochemical differentiation

    NASA Astrophysics Data System (ADS)

    Tilton, G. R.

    Isotope measurements on carbonatite complexes and komatiites can provide information on the geochemical character and geochemical evolution of the mantle, including the sub-continental mantle. Measurements on young samples establish the validity of the method. These are based on Sr, Nd and Pb data from the Tertiary-Mesozoic Gorgona komatiite and Sr and Pb data from the Cretaceous Oka carbonatite complex. In both cases the data describe a LIL element-depleted source similar to that observed presently in MORB. Carbonatite data have been used to study the mantle beneath the Superior Province of the Canadian Shield one billion years (1 AE) ago. The framework for this investigation was established by Bell et al., who showed that large areas of the province appear to be underlain by LIL element-depleted mantle (Sr-85/Sr-86=0.7028) at 1 AE ago. Additionally Bell et al. found four complexes to have higher initial Sr ratios (Sr-87/Sr-86=0.7038), which they correlated with less depleted (bulk earth?) mantle sources, or possibly crustal contamination. Pb isotope relationships in four of the complexes have been studied by Bell et al.

  5. Archean crust-mantle geochemical differentiation

    NASA Technical Reports Server (NTRS)

    Tilton, G. R.

    1983-01-01

    Isotope measurements on carbonatite complexes and komatiites can provide information on the geochemical character and geochemical evolution of the mantle, including the sub-continental mantle. Measurements on young samples establish the validity of the method. These are based on Sr, Nd and Pb data from the Tertiary-Mesozoic Gorgona komatiite and Sr and Pb data from the Cretaceous Oka carbonatite complex. In both cases the data describe a LIL element-depleted source similar to that observed presently in MORB. Carbonatite data have been used to study the mantle beneath the Superior Province of the Canadian Shield one billion years (1 AE) ago. The framework for this investigation was established by Bell et al., who showed that large areas of the province appear to be underlain by LIL element-depleted mantle (Sr-85/Sr-86=0.7028) at 1 AE ago. Additionally Bell et al. found four complexes to have higher initial Sr ratios (Sr-87/Sr-86=0.7038), which they correlated with less depleted (bulk earth?) mantle sources, or possibly crustal contamination. Pb isotope relationships in four of the complexes have been studied by Bell et al.

  6. Early onset of bilateral brachial plexopathy during mantle radiotherapy for Hodgkin's disease.

    PubMed

    Churn, M; Clough, V; Slater, A

    2000-01-01

    We report a case of brachial plexus neuropathy occurring in a 50-year-old man treated with standard mantle radiotherapy for early-stage Hodgkin's disease. A dose of 35 Gy in 20 fractions was given to the mantle field, following by a boost to the right side of the neck (8 Gy in four fractions). The onset of symptoms was early in the course of treatment and a gradual and almost full recovery was observed over 3 years after completion ofradiotherapy. The diagnosis was supported by electromyography. The temporal relationship of the radiotherapy and the onset of the brachial plexus neuropathy suggests a cause and effect, but this association is rarely reported after mantle radiotherapy. We review the aetiology of this condition and postulate possible mechanisms in this patient.

  7. Effects of differentiation on the geodynamics of the early Earth

    NASA Astrophysics Data System (ADS)

    Piccolo, Andrea; Kaus, Boris; White, Richard; Johnson, Tim

    2016-04-01

    Archean geodynamic processes are not well understood, but there is general agreement that the mantle potential temperature was higher than present, and that as a consequence significant amounts of melt were produced both in the mantle and any overlying crust. This has likely resulted in crustal differentiation. An early attempt to model the geodynamic effects of differentiation was made by Johnson et al. (2014), who used numerical modeling to investigate the crust production and recycling in conjunction with representative phase diagrams (based on the inferred chemical composition of the primary melt in accordance with the Archean temperature field). The results of the simulations show that the base of the over-thickened primary basaltic crust becomes gravitational unstable due to the mineral assemblage changes. This instability leads to the dripping of dense material into the mantle, which causes an asthenospheric return flow, local partial melting and new primary crust generation that is rapidly recycled in to mantle. Whereas they gave important insights, the previous simulations were simplified in a number of aspects: 1) the rheology employed was viscous, and both elasticity and pressure-dependent plasticity were not considered; 2) extracted mantle melts were 100% transformed into volcanic rocks, whereas on the present day Earth only about 20-30% are volcanic and the remainder is plutonic; 3) the effect of a free surface was not studied in a systematic manner. In order to better understand how these simplifications affect the geodynamic models, we here present additional simulations to study the effects of each of these parameters. Johnson, T.E., Brown, M., Kaus, B., and VanTongeren, J.A., 2014, Delamination and recycling of Archaean crust caused by gravitational instabilities: Nature Geoscience, v. 7, no. 1, p. 47-52, doi: 10.1038/NGEO2019.

  8. Meteoritic Evidence for Multiple Early Enriched Reservoirs in the Martian Mantle

    NASA Astrophysics Data System (ADS)

    Armytage, R. M. G.; Debaille, V.; Brandon, A. D.; Agee, C. B.

    2018-05-01

    From isotopic systematics, the martian crustal reservoir represented by NWA 7034 cannot be the enriched end-member for the shergottites. This suggests multiple enriched reservoirs in the martian mantle formed by several differentiation events.

  9. Core formation, wet early mantle, and H2O degassing on early Mars

    NASA Technical Reports Server (NTRS)

    Kuramoto, K.; Matsui, T.

    1993-01-01

    Geophysical and geochemical observations strongly suggest a 'hot origin of Mars,' i.e., the early formation of both the core and the crust-mantle system either during or just after planetary accretion. To consider the behavior of H2O in the planetary interior it is specifically important to determine by what mechanism the planet is heated enough to cause melting. For Mars, the main heat source is probably accretional heating. Because Mars is small, the accretion energy needs to be effectively retained in its interior. Therefore, the three candidates of heat retention mechanism are discussed first: (1) the blanketing effect of the primordial H2-He atmosphere; (2) the blanketing effect of the impact-induced H2O-CO2 atmosphere; and (3) the higher deposition efficiency of impact energy due to larger impacts. It was concluded that (3) the is the most plausible mechanism for Mars. Then, its possible consequence on how wet the early martian mantle was is discussed.

  10. A model for the evolution of the Earth's mantle structure since the Early Paleozoic

    NASA Astrophysics Data System (ADS)

    Zhang, Nan; Zhong, Shijie; Leng, Wei; Li, Zheng-Xiang

    2010-06-01

    Seismic tomography studies indicate that the Earth's mantle structure is characterized by African and Pacific seismically slow velocity anomalies (i.e., superplumes) and circum-Pacific seismically fast anomalies (i.e., a globally spherical harmonic degree 2 structure). However, the cause for and time evolution of the African and Pacific superplumes and the degree 2 mantle structure remain poorly understood with two competing proposals. First, the African and Pacific superplumes have remained largely unchanged for at least the last 300 Myr and possibly much longer. Second, the African superplume is formed sometime after the formation of Pangea (i.e., at 330 Ma) and the mantle in the African hemisphere is predominated by cold downwelling structures before and during the assembly of Pangea, while the Pacific superplume has been stable for the Pangea supercontinent cycle (i.e., globally a degree 1 structure before the Pangea formation). Here, we construct a proxy model of plate motions for the African hemisphere for the last 450 Myr since the Early Paleozoic using the paleogeographic reconstruction of continents constrained by paleomagnetic and geological observations. Coupled with assumed oceanic plate motions for the Pacific hemisphere, this proxy model for the plate motion history is used as time-dependent surface boundary condition in three-dimensional spherical models of thermochemical mantle convection to study the evolution of mantle structure, particularly the African mantle structure, since the Early Paleozoic. Our model calculations reproduce well the present-day mantle structure including the African and Pacific superplumes and generally support the second proposal with a dynamic cause for the superplume structure. Our results suggest that while the mantle in the African hemisphere before the assembly of Pangea is predominated by the cold downwelling structure resulting from plate convergence between Gondwana and Laurussia, it is unlikely that the bulk of

  11. Constraining Mantle Differentiation Processes with La-Ce and Sm-Nd Isotope Systematics

    NASA Astrophysics Data System (ADS)

    Willig, M.; Stracke, A.

    2016-12-01

    Cerium (Ce) and Neodymium (Nd) isotopic ratios in oceanic basalts reflect the time integrated La-Ce and Sm-Nd ratios, and hence the extent of light rare earth element element (LREE) depletion or enrichment of their mantle sources. New high precision Ce-Nd isotope data from several ocean islands define a tight array in ԑCe-ԑNd space with ԑNd = -8.2±0.4 ԑCe + 1.3±0.9 (S.D.), in good agreement with previous data [1, 2]. The slope of the ԑCe-ԑNd array and the overall isotopic range are sensitive indicators of the processes that govern the evolution of the mantle's LREE composition. A Monte Carlo approach is employed to simulate continuous mantle-crust differentiation by partial melting and recycling of crustal materials. Partial melting of mantle peridotites produces variably depleted mantle and oceanic crust, which evolve for different time periods, before the oceanic crust is recycled back into the mantle including small amounts of continental crust (GLOSS [3]). Subsequently, depleted mantle and recycled materials of variable age and composition melt, and the respective melts mix in different proportions. Mixing lines strongly curve towards depleted mantle, and tend to be offset from the data for increasingly older and more depleted mantle. Observed ԑCe-ԑNd in ridge [1] and ocean island basalts and the slope of the ԑCe-ԑNd array therefore define upper limits for the extent and age of LREE depletion preserved in mantle peridotites. Very old average mantle depletion ages (> ca. 1-2 Ga) for the bulk of the mantle are difficult to reconcile with the existing ԑCe-ԑNd data, consistent with the range of Nd-Hf-Os model ages in abyssal peridotites [4-6]. Moreover, unless small amounts of continental crust are included in the recycled material, it is difficult to reproduce the relatively shallow slope of the ԑCe-ԑNd array, consistent with constraints from the ԑNd - ԑHf mantle array [7]. [1] Makishima and Masuda, 1994 Chem. Geol. 118, 1-8. [2] Doucelance et al

  12. The evolution of continental roots in numerical thermo-chemical mantle convection models including differentiation by partial melting

    NASA Astrophysics Data System (ADS)

    de Smet, J. H.; van den Berg, A. P.; Vlaar, N. J.

    1999-09-01

    Incorporating upper mantle differentiation through decompression melting in a numerical mantle convection model, we demonstrate that a compositionally distinct root consisting of depleted peridotite can grow and remain stable during a long period of secular cooling. Our modeling results show that in a hot convecting mantle partial melting will produce a compositional layering in a relatively short time of about 50 Ma. Due to secular cooling mantle differentiation finally stops before 1 Ga. The resulting continental root remains stable on a billion year time scale due to the combined effects of its intrinsically lower density and temperature-dependent rheology. Two different parameterizations of the melting phase-diagram are used in the models. The results indicate that during the Archaean melting occurred on a significant scale in the deep regions of the upper mantle, at pressures in excess of 15 GPa. The compositional depths of continental roots extend to 400 km depending on the potential temperature and the type of phase-diagram parameterization used in the model. The results reveal a strong correlation between lateral variations of temperature and the thickness of the continental root. This shows that cold regions in cratons are stabilized by a thick depleted root.

  13. Mantle source heterogeneity of the Early Jurassic basalt of eastern North America

    NASA Astrophysics Data System (ADS)

    Gregory Shellnutt, J.; Dostal, Jaroslav; Yeh, Meng-Wan

    2018-04-01

    One of the defining characteristics of the basaltic rocks from the Early Jurassic Eastern North America (ENA) sub-province of the Central Atlantic Magmatic Province (CAMP) is the systematic compositional variation from South to North. Moreover, the tectono-thermal regime of the CAMP is debated as it demonstrates geological and structural characteristics (size, radial dyke pattern) that are commonly associated with mantle plume-derived mafic continental large igneous provinces but is considered to be unrelated to a plume. Mantle potential temperature ( T P) estimates of the northern-most CAMP flood basalts (North Mountain basalt, Fundy Basin) indicate that they were likely produced under a thermal regime ( T P ≈ 1450 °C) that is closer to ambient mantle ( T P ≈ 1400 °C) conditions and are indistinguishable from other regions of the ENA sub-province ( T Psouth = 1320-1490 °C, T Pnorth = 1390-1480 °C). The regional mantle potential temperatures are consistent along the 3000-km-long ENA sub-province suggesting that the CAMP was unlikely to be generated by a mantle plume. Furthermore, the mantle potential temperature calculation using the rocks from the Northern Appalachians favors an Fe-rich mantle (FeOt = 8.6 wt %) source, whereas the rocks from the South Appalachians favor a less Fe-rich (FeOt = 8.3 wt %) source. The results indicate that the spatial-compositional variation of the ENA basaltic rocks is likely related to differing amounts of melting of mantle sources that reflect the uniqueness of their regional accreted terranes (Carolinia and West Avalonia) and their post-accretion, pre-rift structural histories.

  14. By Permission of the Mantle: Modern and Ancient Deep Earth Volatile Cycles

    NASA Astrophysics Data System (ADS)

    Hirschmann, M. M.

    2011-12-01

    The principle volatile elements, H and C, are of surpassing importance to processes and conditions in the interiors and the surfaces of terrestrial planets, affecting everything from mantle dynamics and large scale geochemical differentiation to climate and habitability. The storage of these volatiles in planetary interiors, their inventory in the near-surface environment and exchange between the interiors and the exosphere are governed by petrologic processes. Were it not for the effective incompatibility of these components in mantle lithologies, there might be no oceans, no habitable climate, and no biosphere on the surface. Consequently, deep Earth volatile cycles represent one of the best examples of how petrology influences nearly all other aspects of Earth science. The exosphere of the modern Earth has a high H/C ratio compared to that of the interior sampled by oceanic basalts. A potential explanation for this is that C is subducted to the deep mantle more efficiently than H, such that the exosphere C reservoir shrinks through geologic time. Unfortunately this hypothesis conflicts with the sedimentary record, which suggests that carbonate storage on the continents has increased rather than decreased with time. It also may not be applicable to the first 3 Ga of Earth history, when hotter typical subduction geotherms greatly reduced the efficiency of C subduction. An important question regarding deep Earth volatile cycles is the inventory of H and C in the interior and the exosphere that descend from Earth's earliest differentiation processes. Originally, much of Earth's volatile inventory was presumably present as a thick atmosphere, in part because volatiles were probably delivered late in the accretion history and owing to both the efficiency of impact degassing and of volatile release from early magma ocean(s). Early mantle H2O may descend from the magma ocean, in which portions of a steam atmosphere are dissolved in the magma and then precipitated with

  15. Numerical Mantle Convection Models of Crustal Formation in an Oceanic Environment in the Early Earth

    NASA Astrophysics Data System (ADS)

    van Thienen, P.; van den Berg, A. P.; Vlaar, N. J.

    2001-12-01

    The generation of basaltic crust in the early Earth by partial melting of mantle rocks, subject to investigation in this study, is thought to be a first step in the creation of proto-continents (consisting largely of felsic material), since partial melting of basaltic material was probably an important source for these more evolved rocks. In the early Archean the earth's upper mantle may have been hotter than today by as much as several hundred degrees centigrade. As a consequence, partial melting in shallow convective upwellings would have produced a layering of basaltic crust and underlying depleted (lherzolitic-harzburgitic) mantle peridotite which is much thicker than found under modern day oceanic ridges. When a basaltic crustal layer becomes sufficiently thick, a phase transition to eclogite may occur in the lower parts, which would cause delamination of this dense crustal layer and recycling of dense eclogite into the upper mantle. This recycling mechanism may have contributed significantly to the early cooling of the earth during the Archean (Vlaar et al., 1994). The delamination mechanism which limits the build-up of a thick basaltic crustal layer is switched off after sufficient cooling of the upper mantle has taken place. We present results of numerical modelling experiments of mantle convection including pressure release partial melting. The model includes a simple approximate melt segregation mechanism and basalt to eclogite phase transition, to account for the dynamic accumulation and recycling of the crust in an upper mantle subject to secular cooling. Finite element methods are used to solve for the viscous flow field and the temperature field, and lagrangian particle tracers are used to represent the evolving composition due to partial melting and accumulation of the basaltic crust. We find that this mechanism creates a basaltic crust of several tens of kilometers thickness in several hundreds of million years. This is accompanied by a cooling of

  16. Early and long-term mantle processing rates derived from xenon isotopes

    NASA Astrophysics Data System (ADS)

    Mukhopadhyay, S.; Parai, R.; Tucker, J.; Middleton, J. L.; Langmuir, C. H.

    2015-12-01

    Noble gases, particularly xenon (Xe), in mantle-derived basalts provide a rich portrait of mantle degassing and surface-interior volatile exchange. The combination of extinct and extant radioactive species in the I-Pu-U-Xe systems shed light on the degassing history of the early Earth throughout accretion, as well as the long-term degassing of the Earth's interior in association with plate tectonics. The ubiquitous presence of shallow-level air contamination, however, frequently obscures the mantle Xe signal. In a majority of the samples, shallow air contamination dominates the Xe budget. For example, in the gas-rich popping rock 2ΠD43, 129Xe/130Xe ratios reach 7.7±0.23 in individual step-crushes, but the bulk composition of the sample is close to air (129Xe/130Xe of 6.7). Thus, the extent of variability in mantle source Xe composition is not well-constrained. Here, we present new MORB Xe data and explore constraints placed on mantle processing rates by the Xe data. Ten step-crushes were obtained on a depleted popping glass that was sealed in ultrapure N2 after dredge retrieval from between the Kane-Atlantis Fracture Zone of the Mid Atlantic Ridge in May 2012. 9 steps yielded 129Xe/130Xe of 7.50-7.67 and one yielded 7.3. The bulk 129Xe/130Xe of the sample is 7.6, nearly identical to the estimated mantle source value of 7.7 for the sample. Hence, the sample is virtually free of shallow-level air contamination. Because sealing the sample in N2upon dredge retrieval largely eliminated air contamination, for many samples, contamination must be added after sample retrieval from the ocean bottom. Our new high-precision Xe isotopic measurements in upper mantle-derived samples provide improved constraints on the Xe isotopic composition of the mantle source. We developed a forward model of mantle volatile evolution to identify solutions that satisfy our Xe isotopic data. We find that accretion timescales of ~10±5 Myr are consistent with I-Pu-Xe constraints, and the last

  17. Evolution of the martian mantle as recorded by igneous rocks

    NASA Astrophysics Data System (ADS)

    Balta, J. B.; McSween, H. Y.

    2013-12-01

    Martian igneous rocks provide our best window into the current state of the martian mantle and its evolution after accretion and differentiation. Currently, those rocks have been examined in situ by rovers, characterized in general from orbiting spacecraft, and analyzed in terrestrial laboratories when found as meteorites. However, these data have the potential to bias our understanding of martian magmatism, as most of the available meteorites and rover-analyzed rocks come from the Amazonian (<2 Ga) and Hesperian (~3.65 Ga) periods respectively, while igneous rocks from the Noachian (>3.8 Ga) have only been examined by orbiters and as the unique meteorite ALH 84001. After initial differentiation, the main planetary-scale changes in the structure of Mars which impact igneous compositions are cooling of the planet and thickening of the crust with time. As the shergottite meteorites give ages <500 Ma1, they might be expected to represent thick-crust, recent volcanism. Using spacecraft measurements of volcanic compositions and whole rock compositions of meteorites, we demonstrate that the shergottite meteorites do not match the composition of the igneous rocks composing the young volcanoes on Mars, particularly in their silica content, and no crystallization or crustal contamination trend reproduces the volcanoes from a shergottite-like parent magma. However, we show that the shergottite magmas do resemble older martian rocks in composition and mineralogy. The Noachian-aged meteorite ALH 84001 has similar radiogenic-element signatures to the shergottites and may derive from a similar mantle source despite the age difference2. Thus, shergottite-like magmas may represent melting of mantle sources that were much more abundant early in martian history. We propose that the shergottites represent the melting products of an originally-hydrous martian mantle, containing at least several hundred ppm H2O. Dissolved water can increase the silica content of magmas and thus

  18. Sulfur in Earth's Mantle and Its Behavior During Core Formation

    NASA Technical Reports Server (NTRS)

    Chabot, Nancy L.; Righter,Kevin

    2006-01-01

    The density of Earth's outer core requires that about 5-10% of the outer core be composed of elements lighter than Fe-Ni; proposed choices for the "light element" component of Earth's core include H, C, O, Si, S, and combinations of these elements [e.g. 1]. Though samples of Earth's core are not available, mantle samples contain elemental signatures left behind from the formation of Earth's core. The abundances of siderophile (metal-loving) elements in Earth's mantle have been used to gain insight into the early accretion and differentiation history of Earth, the process by which the core and mantle formed, and the composition of the core [e.g. 2-4]. Similarly, the abundance of potential light elements in Earth's mantle could also provide constraints on Earth's evolution and core composition. The S abundance in Earth's mantle is 250 ( 50) ppm [5]. It has been suggested that 250 ppm S is too high to be due to equilibrium core formation in a high pressure, high temperature magma ocean on early Earth and that the addition of S to the mantle from the subsequent accretion of a late veneer is consequently required [6]. However, this earlier work of Li and Agee [6] did not parameterize the metalsilicate partitioning behavior of S as a function of thermodynamic variables, limiting the different pressure and temperature conditions during core formation that could be explored. Here, the question of explaining the mantle abundance of S is revisited, through parameterizing existing metal-silicate partitioning data for S and applying the parameterization to core formation in Earth.

  19. The behaviour of tungsten during mantle melting revisited with implications for planetary differentiation time scales

    NASA Astrophysics Data System (ADS)

    Babechuk, Michael G.; Kamber, Balz S.; Greig, Alan; Canil, Dante; Kodolányi, János

    2010-02-01

    Tungsten is a moderately siderophile high-field-strength element that is hydrophile and widely regarded as highly incompatible during mantle melting. In an effort to extend empirical knowledge regarding the behaviour of W during the latter process, we report new high-precision trace element data (W, Th, U, Ba, La, Sm) that represent both terrestrial and planetary reservoirs: MORB (11), abyssal peridotites (8), eucrite basalts (3), and carbonaceous chondrites (8). A full trace element suite is also reported for Cordilleran Permian ophiolite peridotites (12) to better constrain the behaviour of W in the upper mantle. In addition, we report our long-term averages for a number of USGS (BIR-1, BHVO-1, BHVO-2, PCC-1, DTS-1) and GSJ (JA-3, JP-1) standard reference materials, some of which we conclude to be heterogeneous and contaminated with respect to W. The most significant finding of this study is that many of the highly depleted upper mantle peridotites contain far higher W concentrations than expected. In the absence of convincing indications for alteration, re-enrichment or contamination, we propose that the W excess was caused by retention in an Os-Ir alloy phase, whose stability is dependent on fO 2 of the mantle source region. This explanation could help to account for the particularly low W content of N-MORB and implies that the lithophile behaviour of W in basaltic rocks is not an accurate representation of the behaviour in the melt source. These findings then become relevant to the interpretation of W-isotopic data for achondrites, where the fractionation of Hf from W during melting is used to infer the Hf/W of the parent body mantle. This is exemplified by the differentiation chronology of the eucrite parent body (EPB), which has been modeled with a melt source with high Hf/W. By contrast, we explore the alternative scenario with a low mantle Hf/W on the EPB. Using available eucrite literature data, a maximum core segregation age of 1.2 ± 1.2 Myr after the

  20. The Molecular Differentiation of Anatomically Paired Left and Right Mantles of the Pacific Oyster Crassostrea gigas.

    PubMed

    Wei, Lei; Xu, Fei; Wang, Yuzhi; Cai, Zhongqiang; Yu, Wenchao; He, Cheng; Jiang, Qiuyun; Xu, Xiqiang; Guo, Wen; Wang, Xiaotong

    2018-03-28

    Left-right (L-R) asymmetry is controlled by gene regulation pathways for the L-R axis, and in vertebrates, the gene Pitx2 in TGF-β signaling pathway plays important roles in the asymmetrical formation of organs. However, less is known about the asymmetries of anatomically identical paired organs, as well as the transcriptional regulation mechanism of the gene Pitx in invertebrates. Here, we report the molecular biological differences between the left and right mantles of an invertebrate, the Pacific oyster Crassostrea gigas, and propose one possible mechanism underlying those differences. RNA sequencing (RNA-seq) analysis indicated that the paired organs showed different gene expression patterns, suggesting possible functional differences in shell formation, pheromone signaling, nerve conduction, the stress response, and other physiological processes. RNA-seq and real-time qPCR analysis indicated high right-side expression of the Pitx homolog (cgPitx) in oyster mantle, supporting a conserved role for Pitx in controlling asymmetry. Methylation-dependent restriction-site associated DNA sequencing (MethylRAD) identified a methylation site in the promoter region of cgPitx and showed significantly different methylation levels between the left and right mantles. This is the first report, to our knowledge, of such a difference in methylation in spiralians, and it was further confirmed in 18 other individuals by using a pyrosequencing assay. The miRNome analysis and the TGF-β receptor/Smad inhibition experiment further supported that several genes in TGF-β signaling pathway may be related with the L/R asymmetry of oyster mantles. These results suggested that the molecular differentiation of the oyster's paired left and right mantles is significant, TGF-β signaling pathway could be involved in establishing or maintaining the asymmetry, and the cgPitx gene as one of genes in this pathway; the different methylation levels in its promoter regions between L/R mantles was

  1. Chondritic Xenon in the Earth's mantle: new constrains on a mantle plume below central Europe

    NASA Astrophysics Data System (ADS)

    Caracausi, Antonio; Avice, Guillaume; Bernard, Peter; Furi, Evelin; Marty, Bernard

    2016-04-01

    data support the notion that the fraction of plutonium-derived Xe in plume sources (oceanic as well as continental) is higher than in the MORB source reservoir. Hence, the MORB - type reservoirs appear to be well distinguished and more degassed than the plume sources (oceanic as well as continental) supporting the heterogeneity of Earth's mantle. Finally this study highlights that xenon isotopes in the Eifel gas have preserved a chemical signature that is characteristic of other mantle plume sources. This is very intriguing because the presence of a mantle plume in this sector of Central Europe was already inferred from geophysical and geochemical studies(Buikin et al., 2005; Goes et al., 1999). Notably, tomographic images show a low-velocity structure down to 2000 km depth, representing deep mantle upwelling under central Europe, that may feed smaller upper-mantle plumes (Eifel volcanic district-Germany). References Buikin A., Trieloff M., HoppJ., Althaus T., Korochantseva E., Schwarz W.H. &Altherr R., (2005), Noble gas isotopessuggestdeepmantleplume source of late Cenozoicmaficalkalinevolcanism in Europe, Earth Planet. Sci. Lett. 230, 143-162. Goes S., Spakman W. &BijwaardH., (1999), A lowermantle source for centraleuropeanvolcanism, Science, 286, 1928-1931.G. Holland, M. Cassidy, C.J. Ballentine, Meteorite Kr in the Earth's mantle suggests a late accretionary source for the atmosphere, Science, 326, 1522-1525, (2009). Marty, B. Neon and xenon isotopes in MORB: implications for the Earth-atmosphere evolution. Earth Planet. Sci. Lett. 94, 45-56 (1989). Mukhopadhyay S., Early differentiation and volatile accretion recorded in deep-mantle neon and xenon Nature, 486, 101-106, (2013).

  2. Early mantle heterogeneities in the Réunion hotspot source inferred from highly siderophile elements in cumulate xenoliths

    NASA Astrophysics Data System (ADS)

    Peters, Bradley J.; Day, James M. D.; Taylor, Lawrence A.

    2016-08-01

    remarkably homogeneous Os, Pb, and noble-gas isotopic signatures of Réunion, which plot near the convergence point of isotopic data for many hotspots, such a conclusion provides evidence for an early differentiated and subsequently isolated mantle domain that may be partially sampled by some ocean island basalts.

  3. Origin of the Early Sial Crust and U-Pb Isotope-Geochemical Heterogeneity of the Earth's Mantle

    NASA Astrophysics Data System (ADS)

    Mishkin, M. A.; Nozhkin, A. D.; Vovna, G. M.; Sakhno, V. G.; Veldemar, A. A.

    2018-02-01

    It is shown that presence of the Early Precambrian sial crust in the Indo-Atlantic segment of the Earth and its absence in the Pacific has been caused by geochemical differences in the mantle underlying these segments. These differences were examined on the basis of Nd-Hf and U-Pb isotopes in modern basalts. The U-Pb isotope system is of particular interest, since uranium is a member of a group of heat-generating radioactive elements providing heat for plumes. It is shown that in the Indo-Atlantic segment, a distribution of areas of the modern HIMU type mantle is typical, while it is almost completely absent in the Pacific segment. In the Archean, in the upper HIMU type paleo-mantle areas, plume generation and formation of the primordial basic crust occurred; this was followed by its remelting resulting in the appearance of an early sial crust forming cratons of the Indo-Atlantic segment.

  4. Search for a Differentiated Asteroid Family

    NASA Astrophysics Data System (ADS)

    Thomas, Cristina A.; Lim, Lucy F.; Trilling, David E.; Moskovitz, Nicholas

    2014-08-01

    Dynamical asteroid families resulting from catastrophic disruptions represent the interiors of their former parent bodies. Differentiation of a large initially chondritic parent body is expected to produce an ``onion shell" object with a metal core, a thick olivine-rich mantle, and a thin basaltic crust. However, instead of the mineralogical diversity expected from the disruption of a differentiated parent body, most asteroid families tend to show similar spectra among the members. Moreover, spectra of metal-like materials and olivine-dominated assemblages have not been detected in asteroid families in the Main Belt and the expected mantle material is missing from the meteorite record. The deficit of olivine-rich mantle material in the meteorite record and in asteroid observations is known as the ``Missing Mantle" problem. For years the best explanation for the lack of mantle material has been the ``battered to bits" hypothesis that states that all differentiated parent bodies (aside from Vesta) were disrupted very early in the solar system and the resulting olivine-rich material was collisionally broken down until the object diameters fell below our observational limits. However, in a new, competing, hypothesis, Elkins-Tanton et al. (2013) has suggested that previous work has overestimated the amount of olivine produced by the differentiation of a chondritic parent body. We propose to obtain visible spectra of asteroids within the Massalia, Merxia, and Agnia S-type families to search for compositional variations that are indicators of differentiation and to quantitatively constrain the two competing ``Missing Mantle" hypotheses.

  5. Self-Organized Mantle Layering After the Magma-Ocean Period

    NASA Astrophysics Data System (ADS)

    Hansen, U.; Dude, S.

    2017-12-01

    The thermal history of the Earth, it's chemical differentiation and also the reaction of the interior with the atmosphere is largely determined by convective processes within the Earth's mantle. A simple physical model, resembling the situation, shortly after core formation, consists of a compositionally stable stratified mantle, as resulting from fractional crystallization of the magma ocean. The early mantle is subject to heating from below by the Earth's core and cooling from the top through the atmosphere. Additionally internal heat sources will serve to power the mantle dynamics. Under such circumstances double diffusive convection will eventually lead to self -organized layer formation, even without the preexisting jumps is material properties. We have conducted 2D and 3D numerical experiments in Cartesian and spherical geometry, taking into account mantle realistic values, especially a strong temperature dependent viscosity and a pressure dependent thermal expansivity . The experiments show that in a wide parameter range. distinct convective layers evolve in this scenario. The layering strongly controls the heat loss from the core and decouples the dynamics in the lower mantle from the upper part. With time, individual layers grow on the expense of others and merging of layers does occur. We observe several events of intermittent breakdown of individual layers. Altogether an evolution emerges, characterized by continuous but also spontaneous changes in the mantle structure, ranging from multiple to single layer flow. Such an evolutionary path of mantle convection allows to interpret phenomena ranging from stagnation of slabs at various depth to variations in the chemical signature of mantle upwellings in a new framework.

  6. Early formation and long-term stability of continents resulting from decompression melting in a convecting mantle

    NASA Astrophysics Data System (ADS)

    De Smet, J.; Van den Berg, A. P.; Vlaar, N. J.

    2000-07-01

    The origin of stable old continental cratonic roots is still debated. We present numerical modelling results which show rapid initial formation during the Archaean of continental roots of ca. 200 km thick. These results have been obtained from an upper mantle thermal convection model including differentiation by pressure release partial melting of mantle peridotite. The upper mantle model includes time-dependent radiogenic heat production and thermal coupling with a heat reservoir representing the Earth's lower mantle and core. This allows for model experiments including secular cooling on a time-scale comparable to the age of the Earth. The model results show an initial phase of rapid continental root growth of ca. 0.1 billion year, followed by a more gradual increase of continental volume by addition of depleted material produced through hot diapiric, convective upwellings which penetrate the continental root from below. Within ca. 0.6 Ga after the start of the experiment, secular cooling of the mantle brings the average geotherm below the peridotite solidus thereby switching off further continental growth. At this time the thickness of the continental root has grown to ca. 200 km. After 1 Ga of secular cooling small scale thermal instabilities develop at the bottom of the continental root causing continental delamination without breaking up the large scale layering. This delaminated material remixes with the deeper layers. Two more periods, each with a duration of ca. 0.5 Ga and separated by quiescent periods were observed when melting and continental growth was reactivated. Melting ends at 3 Ga. Thereafter secular cooling proceeds and the compositionally buoyant continental root is stabilized further through the increase in mechanical strength induced by the increase of the temperature dependent mantle viscosity. Fluctuating convective velocity amplitudes decrease to below 10 mma -1 and the volume average temperature of the sub-continental convecting mantle has

  7. Global structure of mantle isotopic heterogeneity and its implications for mantle differentiation and convection

    NASA Astrophysics Data System (ADS)

    Iwamori, Hikaru; Albaréde, Francis; Nakamura, Hitomi

    2010-11-01

    In order to further our understanding of the global geochemical structure and mantle dynamics, a global isotopic data set of oceanic basalts was analyzed by Independent Component Analysis (ICA), a relatively new method of multivariate analysis. The data set consists of 2773 mid-ocean ridge basalts (MORB) and 1515 ocean island basalts (OIB) with five isotopic ratios of Pb, Nd and Sr. The data set spatially covers the major oceans and enables us to compare the results with global geophysical observations. Three independent components (ICs) have been found, two of which are essentially identical to those previously found for basalts from the Atlantic and Indian Oceans. The two ICs (IC1 and IC2) span a compositional plane that accounts for 95.7% of the sample variance, while the third IC (IC3) accounts for 3.7%. Based on the geochemical nature of ICs and a forward model concerning trace elemental and isotopic compositions, the origin of the ICs is discussed. IC1 discriminates OIB from MORB, and may be related to elemental fractionation associated with melting and the subsequent radiogenic in growth with an average recycling time of 0.8 to 2.4 Ga. IC2 tracks the regional provenance of both MORB and OIB and may be related to aqueous fluid-rock interaction and the subsequent radiogenic ingrowth with an average recycling time of 0.3 to 0.9 Ga. IC3 fingerprints upper continental crustal material and its high value appears in limited geographical and tectonic settings. Variations in the melt component (IC1) and in the aqueous fluid component (IC2) inherited in the mantle most likely reflect mid-ocean ridge and subduction zone processes, respectively. Long-term accumulation of dense materials rich in the IC1 melt component at the base of the convective mantle accounts for its longer recycling time with respect to that for less dense materials rich in the aqueous fluid component (IC2). IC2 broadly correlates with the seismic velocity structures of the lowermost mantle and

  8. Origin of igneous meteorites and differentiated asteroids

    NASA Astrophysics Data System (ADS)

    Scott, E.; Goldstein, J.; Asphaug, E.; Bottke, W.; Moskovitz, N.; Keil, K.

    2014-07-01

    Introduction: Igneously formed meteorites and asteroids provide major challenges to our understanding of the formation and evolution of the asteroid belt. The numbers and types of differentiated meteorites and non-chondritic asteroids appear to be incompatible with an origin by fragmentation of numerous Vesta-like bodies by hypervelocity impacts in the asteroid belt over 4 Gyr. We lack asteroids and achondrites from the olivine-rich mantles of the parent bodies of the 12 groups of iron meteorites and the ˜70 ungrouped irons, the 2 groups of pallasites and the 4--6 ungrouped pallasites. We lack mantle and core samples from the parent asteroids of the basaltic achondrites that do not come from Vesta, viz., angrites and the ungrouped eucrites like NWA 011 and Ibitira. How could core samples have been extracted from numerous differentiated bodies when Vesta's basaltic crust was preserved? Where is the missing Psyche family of differentiated asteroids including the complementary mantle and crustal asteroids [1]? Why are meteorites derived from far more differentiated parent bodies than chondritic parent bodies even though C and S class chondritic asteroids dominate the asteroid belt? New paradigm. Our studies of meteorites, impact modeling, and dynamical studies suggest a new paradigm in which differentiated asteroids accreted at 1--2 au less than 2 Myr after CAI formation [2]. They were rapidly melted by 26Al and disrupted by hit-and-run impacts [3] while still molten or semi-molten when planetary embryos were accreting. Metallic Fe-Ni bodies derived from core material cooled rapidly with little or no silicate insulation less than 4 Myr after CAI formation [4]. Fragments of differentiated planetesimals were subsequently tossed into the asteroid belt. Meteorite evidence for early disruption of differentiated asteroids. If iron meteorites were samples of Fe-Ni cores of bodies that cooled slowly inside silicate mantles over ˜50--100 Myr, irons from each core would have

  9. Pb evolution in the Martian mantle

    NASA Astrophysics Data System (ADS)

    Bellucci, J. J.; Nemchin, A. A.; Whitehouse, M. J.; Snape, J. F.; Bland, P.; Benedix, G. K.; Roszjar, J.

    2018-03-01

    The initial Pb compositions of one enriched shergottite, one intermediate shergottite, two depleted shergottites, and Nakhla have been measured by Secondary Ion Mass Spectrometry (SIMS). These values, in addition to data from previous studies using an identical analytical method performed on three enriched shergottites, ALH 84001, and Chassigny, are used to construct a unified and internally consistent model for the differentiation history of the Martian mantle and crystallization ages for Martian meteorites. The differentiation history of the shergottites and Nakhla/Chassigny are fundamentally different, which is in agreement with short-lived radiogenic isotope systematics. The initial Pb compositions of Nakhla/Chassigny are best explained by the late addition of a Pb-enriched component with a primitive, non-radiogenic composition. In contrast, the Pb isotopic compositions of the shergottite group indicate a relatively simple evolutionary history of the Martian mantle that can be modeled based on recent results from the Sm-Nd system. The shergottites have been linked to a single mantle differentiation event at 4504 Ma. Thus, the shergottite Pb isotopic model here reflects a two-stage history 1) pre-silicate differentiation (4504 Ma) and 2) post-silicate differentiation to the age of eruption (as determined by concordant radiogenic isochron ages). The μ-values (238U/204Pb) obtained for these two different stages of Pb growth are μ1 of 1.8 and a range of μ2 from 1.4-4.7, respectively. The μ1-value of 1.8 is in broad agreement with enstatite and ordinary chondrites and that proposed for proto Earth, suggesting this is the initial μ-value for inner Solar System bodies. When plotted against other source radiogenic isotopic variables (Sri, γ187Os, ε143Nd, and ε176Hf), the second stage mantle evolution range in observed mantle μ-values display excellent linear correlations (r2 > 0.85) and represent a spectrum of Martian mantle mixing-end members (depleted

  10. Tomographic and Geodynamic Constraints on Convection-Induced Mixing in Earth's Deep Mantle

    NASA Astrophysics Data System (ADS)

    Hafter, D. P.; Forte, A. M.; Bremner, P. M.; Glisovic, P.

    2017-12-01

    Seismological studies reveal two large low-shear-velocity provinces (LLSVPs) in the lowermost mantle (e.g., Su et al. 1994; Wang & Wen 2007; He & Wen 2012), which may represent accumulations of subducted slabs at the CMB (Tan & Gurnis 2005; Christensen & Hoffman 1994) or primordial material generated in the early differentiation of Earth (e.g. Li et al. 2014). The longevity or stability of these large-scale heterogeneities in the deep mantle depends on the vigor and spatial distribution of the convective circulation, which is in turn dependent on the distribution of mantle buoyancy and viscosity (e.g. Glisovic & Forte 2015). Here we explore the state of convective mixing in the mantle using the ASPECT convection code (Kronbichler et al. 2012). A series of experiments are conducted to consider the geochemical and dynamical contributions of LLSVPs to deep-mantle upwellings and corresponding plume-sourced volcanism. The principal feature of these experiments is the use of particle tracers to track geochemical changes in the LLSVPs and mantle plumes in addition to identifying those parts of the mantle that may remain unmixed. We employ 3-D mantle density anomalies derived from joint inversions of seismic, geodynamic and mineral physics constraints and geodynamically-constrained viscosity distributions (Glisovic et al. 2015) to ensure that the predicted flow fields yield a good match to key geophysical constraints (e.g. heat flow, global gravity anomalies and plate velocities).

  11. The early differentiation of Mars inferred from Hf–W chronometry

    DOE PAGES

    Kruijer, Thomas S.; Kleine, Thorsten; Borg, Lars E.; ...

    2017-07-20

    Mars probably accreted within the first 10 million years of Solar System formation and likely underwent magma ocean crystallization and crust formation soon thereafter. In this study, to assess the nature and timescales of these large-scale mantle differentiation processes we applied the short-lived 182Hf– 182W and 146Sm– 142Nd chronometers to a comprehensive suite of martian meteorites, including several shergottites, augite basalt NWA 8159, orthopyroxenite ALH 84001 and polymict breccia NWA 7034. Compared to previous studies the 182W data are significantly more precise and have been obtained for a more diverse suite of martian meteorites, ranging from samples from highly depletedmore » to highly enriched mantle and crustal sources. Our results show that martian meteorites exhibit widespread 182W/ 184W variations that are broadly correlated with 142Nd/ 144Nd, implying that silicate differentiation (and not core formation) is the main cause of the observed 182W/ 184W differences. The combined 182W– 142Nd systematics are best explained by magma ocean crystallization on Mars within ~20–25 million years after Solar System formation, followed by crust formation ~15 million years later. Finally, these ages are indistinguishable from the I–Pu–Xe age for the formation of Mars' atmosphere, indicating that the major differentiation of Mars into mantle, crust, and atmosphere occurred between 20 and 40 million years after Solar System formation and, hence, earlier than previously inferred based on Sm–Nd chronometry alone.« less

  12. The early differentiation of Mars inferred from Hf–W chronometry

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Kruijer, Thomas S.; Kleine, Thorsten; Borg, Lars E.

    Mars probably accreted within the first 10 million years of Solar System formation and likely underwent magma ocean crystallization and crust formation soon thereafter. In this study, to assess the nature and timescales of these large-scale mantle differentiation processes we applied the short-lived 182Hf– 182W and 146Sm– 142Nd chronometers to a comprehensive suite of martian meteorites, including several shergottites, augite basalt NWA 8159, orthopyroxenite ALH 84001 and polymict breccia NWA 7034. Compared to previous studies the 182W data are significantly more precise and have been obtained for a more diverse suite of martian meteorites, ranging from samples from highly depletedmore » to highly enriched mantle and crustal sources. Our results show that martian meteorites exhibit widespread 182W/ 184W variations that are broadly correlated with 142Nd/ 144Nd, implying that silicate differentiation (and not core formation) is the main cause of the observed 182W/ 184W differences. The combined 182W– 142Nd systematics are best explained by magma ocean crystallization on Mars within ~20–25 million years after Solar System formation, followed by crust formation ~15 million years later. Finally, these ages are indistinguishable from the I–Pu–Xe age for the formation of Mars' atmosphere, indicating that the major differentiation of Mars into mantle, crust, and atmosphere occurred between 20 and 40 million years after Solar System formation and, hence, earlier than previously inferred based on Sm–Nd chronometry alone.« less

  13. Effects of spin crossover on iron isotope fractionation in Earth's mantle

    NASA Astrophysics Data System (ADS)

    Qin, T.; Shukla, G.; Wu, Z.; Wentzcovitch, R.

    2017-12-01

    Recent studies have revealed that the iron isotope composition of mid-ocean ridge basalts (MORBs) is +0.1‰ richer in heavy Fe (56Fe) relative to chondrites, while basalts from Mars and Vesta have similar Fe isotopic composition as chondrites. Several hypotheses could explain these observations. For instance, iron isotope fractionation may have occurred during core formation or Earth may have lost some light Fe isotope during the high temperature event in the early Earth. To better understand what drove these isotopic observations, it is important to obtain accurate Fe isotope fractionation factors among mantle and core phases at the relevant P-T conditions. In bridgmanite, the most voluminous mineral in the lower mantle, Fe can occupy more than one crystalline site, be in ferrous and/or ferric states, and may undergo a spin crossover in the lower mantle. Iron isotopic fractionation properties under spin crossover are poorly constrained, while this may be relevant to differentiation of Earth's magma ocean. In this study we address the effect of these multiple states on the iron isotope fractionation factors between mantle and core phases.

  14. Lunar initial Nd-143/Nd-144 - Differential evolution of the lunar crust and mantle

    NASA Technical Reports Server (NTRS)

    Lugmair, G. W.; Marti, K.

    1978-01-01

    The Sm-Nd evolution of Apollo 15 green glass is discussed. The ICE age (intercept with chondritic evolution) of 3.8 + or - 0.4 eons overlaps the range of reported (Ar-39)-(Ar-40) ages and implies a distinct source region for green glass, characterized by very low and unfractionated REE abundances. Evidence is presented that LINd (lunar initial Nd) is compatible with a 'chondritic'-type Nd isotopic evolution as observed in the Juvinas meteorite. This normalization is used to study the Sm-Nd system of various lunar rock types. The results obtained from a limited number of rocks clearly indicate differential Sm-Nd evolution for the lunar crust and mantle. High-Ti basalts returned by the Apollo 11 and 17 missions were derived from distinct source regions. The Nd-143 evolution in KREEP requires a source region which is clearly distinct from any mantle reservoir.

  15. Differentiation of magma oceans and the thickness of the depleted layer on Venus

    NASA Technical Reports Server (NTRS)

    Solomatov, V. S.; Stevenson, D. J.

    1993-01-01

    Various arguments suggest that Venus probably has no asthenosphere, and it is likely that beneath the crust there is a highly depleted and highly viscous mantle layer which was probably formed in the early history of the planet when it was partially or completely molten. Models of crystallization of magma oceans suggest that just after crystallization of a hypothetical magma ocean, the internal structure of Venus consists of a crust up to about 70 km thickness, a depleted layer up to about 500 km, and an enriched lower layer which probably consists of an undepleted 'lower mantle' and heavy enriched accumulates near the core-mantle boundary. Partial or even complete melting of Venus due to large impacts during the formation period eventually results in differentiation. However, the final result of such a differentiation can vary from a completely differentiated mantle to an almost completely preserved homogeneous mantle depending on competition between convection and differentiation: between low viscosity ('liquid') convection and crystal settling at small crystal fractions, or between high viscosity ('solid') convection and percolation at large crystal fractions.

  16. Geologically Controlled Isotope-Time Patterns Reveal Early Differentiation and Crust Formation Processes

    NASA Astrophysics Data System (ADS)

    Bennett, V. C.; Nutman, A. P.

    2014-12-01

    The mechanisms of continental crust production and evolution in the early Earth remain controversial, as are questions of the relative roles of early differentiation versus subsequent tectonic procssing in creating Earth's chemical signatures. Here we present geologic observations integrated with whole rock major, trace element and Sm-Nd isotopic signatures and combined with U-Pb and Lu-Hf isotopic compositions of zircon populations from the same rocks, from the most extensive early rock record comprising the 3.9 Ga to 3.6 Ga terranes of southwest Greenland. These data reveal repeated patterns of formation of juvenile TTG crust and associated mafic and ultramafic rocks in convergent margin settings followed by formation of more evolved granites [1]. Our new zircon Lu-Hf data from rare 3.6-3.7 Ga tonalites within the Itsaq Gneiss Complex, obtained from single component, non-migmatitic gneisses with simple zircon populations, limited within sample Hf isotopic variability and accurate U-Pb ages, now document extraction of juvenile tonalites from a near chondritic mantle source between 3.9 Ga and 3.6 Ga. The more evolved, granitic rocks in each area show slightly negative initial ɛHf in accord with crustal reworking of the older (3.8-3.9 Ga) gniesses. There is no evidence for Hadean material in the sources of the granitoids. The Hf isotope-time patterns are consistent with juvenile crust production from a mantle source that experienced only modest amounts of prior crustal extraction. They are distinct from those predicted by reprocessing of an enriched Hadean mafic crust, as has been proposed for this region [2] and for the source of the Hadean Jack Hills zircons [3]. The well-documented, time decreasing, positive 142Nd anomalies [e.g., 4] from these rocks are further evidence of crustal derivation from a convecting mantle source, rather than reworking of an enriched mafic lithosphere. The 143Nd isotopic -time patterns are more complex, reflecting the interplay

  17. Origin of geochemical mantle components: Role of spreading ridges and thermal evolution of mantle

    NASA Astrophysics Data System (ADS)

    Kimura, Jun-Ichi; Gill, James B.; van Keken, Peter E.; Kawabata, Hiroshi; Skora, Susanne

    2017-02-01

    We explore the element redistribution at mid-ocean ridges (MOR) using a numerical model to evaluate the role of decompression melting of the mantle in Earth's geochemical cycle, with focus on the formation of the depleted mantle component. Our model uses a trace element mass balance based on an internally consistent thermodynamic-petrologic computation to explain the composition of MOR basalt (MORB) and residual peridotite. Model results for MORB-like basalts from 3.5 to 0 Ga indicate a high mantle potential temperature (Tp) of 1650-1500°C during 3.5-1.5 Ga before decreasing gradually to ˜1300°C today. The source mantle composition changed from primitive (PM) to depleted as Tp decreased, but this source mantle is variable with an early depleted reservoir (EDR) mantle periodically present. We examine a two-stage Sr-Nd-Hf-Pb isotopic evolution of mantle residues from melting of PM or EDR at MORs. At high-Tp (3.5-1.5 Ga), the MOR process formed extremely depleted DMM. This coincided with formation of the majority of the continental crust, the subcontinental lithospheric mantle, and the enriched mantle components formed at subduction zones and now found in OIB. During cooler mantle conditions (1.5-0 Ga), the MOR process formed most of the modern ocean basin DMM. Changes in the mode of mantle convection from vigorous deep mantle recharge before ˜1.5 Ga to less vigorous afterward is suggested to explain the thermochemical mantle evolution.

  18. Pristine Igneous Rocks and the Early Differentiation of Planetary Materials

    NASA Technical Reports Server (NTRS)

    Warren, Paul H.

    2005-01-01

    Our studies are highly interdisciplinary, but are focused on the processes and products of early planetary and asteroidal differentiation, especially the genesis of the ancient lunar crust. The compositional diversity that we explore is the residue of process diversity, which has strong relevance for comparative planetology. Most of the accessible lunar crust consists of materials hybridized by impact-mixing. Our lunar research concentrates on the rare pristine (unmixed) samples that reflect the original genetic diversity of the early crust. Among HED basalts (eucrites and clasts in howardites), we distinguish as pristine the small minority that escaped the pervasive thermal metamorphism of the parent asteroid's crust. We have found a correlation between metamorphically pristine HED basalts and the similarly small minority of compositionally evolved "Stannern trend" samples, which are enriched in incompatible elements and titanium compared to main group eucrites, and yet have relatively high mg ratios. Other topics under investigation included: lunar and SNC (martian?) meteorites; igneous meteorites in general; impact breccias, especially metal-rich Apollo samples and polymict eucrites; siderophile compositions of the lunar and martian mantles; and planetary bulk compositions and origins.

  19. Copper systematics during mantle melting and crustal differentiation in arcs: implications for S and Pb budgets of the continental crust

    NASA Astrophysics Data System (ADS)

    Lee, C.; Chin, E. J.; Dasgupta, R.; Luffi, P. I.; Le Roux, V.

    2010-12-01

    During mid-ocean ridge melting, Cu behaves like Sc and is therefore moderately incompatible, as evidenced by the twofold increase in Cu content in MORBs compared to the mantle. However, Cu content in the continental crust is comparable to that of the mantle, implying that during continental crust formation, Cu becomes effectively compatible. Cu is one of the only elements that exhibits Jekyll and Hyde behavior. This switch to being compatible is consistent with the observation that for the majority of arc magmas (as well as MORBs), Cu decreases with increasing SiO2 and decreasing MgO. Using natural samples, we infer new partition coefficients that indicate Cu is incompatible in olivine, pyroxenes, amphiboles, and biotite. The only mineral to exert significant control on Cu partitioning is sulfide. Cu behaves incompatibly during mantle melting because the modal abundance of sulfides relative to silicate minerals is extremely low. The monotonic decrease in Cu in most differentiating arc magmas requires sulfide saturation. In addition, the similar abundances of Cu in many primitive arc magmas compared to MORBs suggests that mantle melting in both environments occurs not only at sulfide saturation but without the need for excess Cu (or S). In a few cases, however, primitive arc magmas begin with high Cu or show increases in Cu with differentiation, which most likely requires unusually high oxygen fugacities in the source or magmatic evolution towards high oxygen fugacity. Such cases may be important for the origin of Cu porphyry deposits, but are generally rare. Because of the close link between Cu and sulfide during magma differentiation, Cu can be used as a proxy for the pre-degassed S content of arc magmas. The S content of continental crust, like many volatile elements, is basically unconstrained, but it can be inferred from Cu, which is much better constrained. Finally, the fact that the continental crust is highly depleted in Cu implies that there is a missing

  20. The Early Differentiation History of Mars from W-182-Nd-142 Isotope Systematics in the SNC Meteorites

    NASA Technical Reports Server (NTRS)

    Foley, C. Nicole; Wadhwa, M.; Borg, L. E.; Janney, P. E.; Hines, R.; Grove, T. L.

    2005-01-01

    We report here the results of an investigation of W and Nd isotopes in the SNC (Shergottite-Nakhlite-Chassignite (martian)) meteorites. We have determined that epsilon W-182 values in the nakhlites are uniform within analytical uncertainties and have an average value of approx. 3. Also, while epsilon W-182 values in the shergottites have a limited range (from 0.3-0.7), their epsilon Nd-142 values vary considerably (from -0.2-0.9). There appears to be no correlation between epsilon W-182 and epsilon Nd-142 in the nakhlites and shergottites. These results shed new light on early differentiation processes on Mars, particularly on the timing and nature of fractionation in silicate reservoirs. Assuming a two-stage model, the metallic core is estimated to have formed at approx. 12 Myr after the beginning of the solar system. Major silicate differentiation established the nakhlite source reservoir before approx. 4542 Ma and the shergottite source reservoirs at 4525 [sup +19 sub -21] Ma. These ages imply that, within the uncertainties afforded by the Hf-182-W-182 and Sm-146-Nd-142 chronometers, the silicate differentiation events that established the source reservoirs of the nakhlites and shergottites may have occurred contemporaneously, possibly during crystallization of a global magma ocean. The distinct W-182-Nd-142 isotope systematics in the nakhlites and the shergottites imply the presence of at least three isotopically distinct silicate reservoirs on Mars, two of which are depleted in incompatible lithophile elements relative to chondrites, and the third is enriched. The two depleted silicate reservoirs most likely reside in the Martian mantle, while the enriched reservoir could be either in the crust or the mantle. Therefore, the W-182-Nd-142 isotope systematics indicate that the nakhlites and the shergottites originated from distinct source reservoirs and cannot be petrogenetically related. A further implication is that the source reservoirs of the nakhlites and

  1. Archean greenstone-tonalite duality: Thermochemical mantle convection models or plate tectonics in the early Earth global dynamics?

    NASA Astrophysics Data System (ADS)

    Kerrich, Robert; Polat, Ali

    2006-03-01

    Mantle convection and plate tectonics are one system, because oceanic plates are cold upper thermal boundary layers of the convection cells. As a corollary, Phanerozoic-style of plate tectonics or more likely a different version of it (i.e. a larger number of slowly moving plates, or similar number of faster plates) is expected to have operated in the hotter, vigorously convecting early Earth. Despite the recent advances in understanding the origin of Archean greenstone-granitoid terranes, the question regarding the operation of plate tectonics in the early Earth remains still controversial. Numerical model outputs for the Archean Earth range from predominantly shallow to flat subduction between 4.0 and 2.5 Ga and well-established steep subduction since 2.5 Ga [Abbott, D., Drury, R., Smith, W.H.F., 1994. Flat to steep transition in subduction style. Geology 22, 937-940], to no plate tectonics but rather foundering of 1000 km sectors of basaltic crust, then "resurfaced" by upper asthenospheric mantle basaltic melts that generate the observed duality of basalts and tonalities [van Thienen, P., van den Berg, A.P., Vlaar, N.J., 2004a. Production and recycling of oceanic crust in the early earth. Tectonophysics 386, 41-65; van Thienen, P., Van den Berg, A.P., Vlaar, N.J., 2004b. On the formation of continental silicic melts in thermochemical mantle convection models: implications for early Earth. Tectonophysics 394, 111-124]. These model outputs can be tested against the geological record. Greenstone belt volcanics are composites of komatiite-basalt plateau sequences erupted from deep mantle plumes and bimodal basalt-dacite sequences having the geochemical signatures of convergent margins; i.e. horizontally imbricated plateau and island arc crust. Greenstone belts from 3.8 to 2.5 Ga include volcanic types reported from Cenozoic convergent margins including: boninites; arc picrites; and the association of adakites-Mg andesites- and Nb-enriched basalts. Archean cratons

  2. Detection of a Sharp Structural Boundary in Lowermost Mantle Beneath Alaska by Core Phase PKPbc-df Differential Travel Times - Observation from the Anomalous South Sandwich Islands to Alaska Path

    NASA Astrophysics Data System (ADS)

    Xin, L.; Kawakatsu, H.; Takeuchi, N.

    2017-12-01

    Differential travel time residuals of PKPbc and PKPdf for the path from South Sandwich Islands (SSI) to Alaska are usually used to constrain anisotropy of the western hemisphere of the Earth's inner-core. For this polar path, it has been found that PKPbc-df differential residuals are generally anomalously larger than data that sample other regions, and also show strong lateral variation. Due to sparse distribution of seismic stations in Alaska in early times, previous researches have been unable to propose a good model to explain this particular data set. Using data recorded by the current dense stations in Alaska for SSI earthquakes, we reexamine the anomalous behavior of core phase PKPbc-df differential travel times and try to explain the origin. The data sample the inner-core for the polar paths, as well as the lowermost mantle beneath Alaska. Our major observations are: (1) fractional travel time residuals of PKPbc-df increase rapidly within 2° (up to 1%). (2) A clear shift of the residual pattern could be seen for earthquakes with different locations. (3) The residual shows systematic lateral variation: at northern part, no steep increase of residual can be seen. A sharp lateral structural boundary with a P-wave velocity contrast of about 3% at lowermost mantle beneath East Alaska is invoked to explain the steep increase of the observed residuals. By combining the effects of a uniformly anisotropic inner-core and the heterogeneity, the observed residual patterns could be well reproduced. This high velocity anomaly might be related with an ancient subducted slab. Lateral variation of the PKPbc-df residuals suggests that the heterogeneity layer is not laterally continuous and may terminate beneath Northeastern Alaska. We also conclude that core phases may be strongly affected by heterogeneities at lowermost mantle, and should be carefully treated if they are used to infer the inner-core structure.

  3. Mantle plumes and hotspot geochemistry

    NASA Astrophysics Data System (ADS)

    Jackson, M. G.; Becker, T. W.; Konter, J.

    2017-12-01

    Ever improving global seismic models, together with expanding databases of mantle derived hotspot lavas, herald advances that relate the geochemistry of hotspots with low seismic shear-wave velocity conduits (plumes) in the mantle. Early efforts linked hotspot geochemistry with deep mantle large low velocity provinces (LLVPs) [1]. More recently, Konter and Becker (2012) [2] observed that the proportion of the C mantle component (inferred from Sr-Nd-Pb isotopes) in hotspot lavas shows an inverse relationship with seismic S-wave velocity anomalies in the shallow mantle (200 km) beneath each hotspot. They proposed that these correlations should also be made based on 3He/4He. Thus, we compare 3He/4He versus seismic S-wave velocity anomalies at 200 km depth. We find that plume-fed hotspots with the highest maximum 3He/4He (i.e., which host more of the C component) have higher hotspot buoyancy fluxes and overlie regions of lower seismic S-wave velocity (interpreted to relate to hotter mantle temperatures) at 200 km depth than hotspots that have only low 3He/4He [3]. This result complements recent work that shows an inverse relationship between maximum 3He/4He and seismic S-wave velocity anomalies in the mantle beneath the western USA [4]. The relationship between 3He/4He, shallow mantle seismic S-wave velocity anomalies, and buoyancy flux is most easily explained by a model where hotter plumes are more buoyant and entrain more of a deep, dense high 3He/4He reservoir than cooler plumes that underlie low 3He/4He hotspots. If the high 3He/4He domain is denser than other mantle components, it will be entrained only by the hottest, most buoyant plumes [3]. Such a deep, dense reservoir is ideally suited to preserving early-formed Hadean domains sampled in modern plume-fed hotspots. An important question is whether, like 3He/4He, seismic S-wave velocity anomalies in the mantle are associated with distinct heavy radiogenic isotopic compositions. C signatures are related to hot

  4. Mantle convection on modern supercomputers

    NASA Astrophysics Data System (ADS)

    Weismüller, Jens; Gmeiner, Björn; Mohr, Marcus; Waluga, Christian; Wohlmuth, Barbara; Rüde, Ulrich; Bunge, Hans-Peter

    2015-04-01

    Mantle convection is the cause for plate tectonics, the formation of mountains and oceans, and the main driving mechanism behind earthquakes. The convection process is modeled by a system of partial differential equations describing the conservation of mass, momentum and energy. Characteristic to mantle flow is the vast disparity of length scales from global to microscopic, turning mantle convection simulations into a challenging application for high-performance computing. As system size and technical complexity of the simulations continue to increase, design and implementation of simulation models for next generation large-scale architectures demand an interdisciplinary co-design. Here we report about recent advances of the TERRA-NEO project, which is part of the high visibility SPPEXA program, and a joint effort of four research groups in computer sciences, mathematics and geophysical application under the leadership of FAU Erlangen. TERRA-NEO develops algorithms for future HPC infrastructures, focusing on high computational efficiency and resilience in next generation mantle convection models. We present software that can resolve the Earth's mantle with up to 1012 grid points and scales efficiently to massively parallel hardware with more than 50,000 processors. We use our simulations to explore the dynamic regime of mantle convection assessing the impact of small scale processes on global mantle flow.

  5. Results of a prospective trial of mantle irradiation alone for selected patients with early-stage Hodgkin's disease.

    PubMed

    Backstrand, K H; Ng, A K; Takvorian, R W; Jones, E L; Fisher, D C; Molnar-Griffin, B J; Silver, B; Tarbell, N J; Mauch, P M

    2001-02-01

    To determine the efficacy of mantle radiation therapy alone in selected patients with early-stage Hodgkin's disease. Between October 1988 and June 2000, 87 selected patients with pathologic stage (PS) IA to IIA or clinical stage (CS) IA Hodgkin's disease were entered onto a single-arm prospective trial of treatment with mantle irradiation alone. Eighty-three of 87 patients had > or = 1 year of follow-up after completion of mantle irradiation and were included for analysis in this study. Thirty-seven patients had PS IA, 40 had PS IIA, and six had CS IA disease. Histologic distribution was as follows: nodular sclerosis (n = 64), lymphocyte predominant (n = 15), mixed cellularity (n = 3), and unclassified (n = 1). Median follow-up time was 61 months. The 5-year actuarial rates of freedom from treatment failure (FFTF) and overall survival were 86% and 100%, respectively. Eleven of 83 patients relapsed at a median time of 27 months. Nine of the 11 relapses contained at least a component below the diaphragm. All 11 patients who developed recurrent disease were alive without evidence of Hodgkin's disease at the time of last follow-up. The 5-year FFTF in the 43 stage I patients was 92% compared with 78% in the 40 stage II patients (P =.04). Significant differences in FFTF were not seen by histology (P =.26) or by European Organization for Research and Treatment of Cancer H-5F eligibility (P =.25). Mantle irradiation alone in selected patients with early-stage Hodgkin's disease is associated with disease control rates comparable to those seen with extended field irradiation. The FFTF is especially favorable among stage I patients.

  6. Mantle transition zone beneath the central Tien Shan: Lithospheric delamination and mantle plumes

    NASA Astrophysics Data System (ADS)

    Kosarev, Grigoriy; Oreshin, Sergey; Vinnik, Lev; Makeyeva, Larissa

    2018-01-01

    We investigate structure of the mantle transition zone (MTZ) under the central Tien Shan in central Asia by using recordings of seismograph stations in Kyrgyzstan, Kazakhstan and adjacent northern China. We apply P-wave receiver functions techniques and evaluate the differential time between the arrivals of seismic phases that are formed by P to SV mode conversion at the 410-km and 660-km seismic boundaries. The differential time is sensitive to the thickness of the MTZ and insensitive to volumetric velocity anomalies above the 410-km boundary. Under part of the southern central Tien Shan with the lowest S wave velocity in the uppermost mantle and the largest thickness of the crust, the thickness of the MTZ increases by 15-20 km relative to the ambient mantle and the reference model IASP91. The increased thickness is a likely effect of low (about - 150 K) temperature. This anomaly is indicative of delamination and sinking of the mantle lithosphere. The low temperature in the MTZ might also be a relic of subduction of the oceanic lithosphere in the Paleozoic, but this scenario requires strong coupling and coherence between structures in the MTZ and in the lithosphere during plate motions in the last 300 Myr. Our data reveal a reduction of thickness of the MTZ of 10-15 km under the Fergana basin, in the neighborhood of the region of small-scale basaltic volcanism at the time near the Cretaceous-Paleogene boundary. The reduced thickness of the MTZ is the effect of a depressed 410-km discontinuity, similar to that found in many hotspots. This depression suggests a positive temperature anomaly of about 100-150 K, consistent with the presence of a thermal mantle plume. A similar depression on the 410-km discontinuity is found underneath the Tarim basin.

  7. Mantle Convection on Modern Supercomputers

    NASA Astrophysics Data System (ADS)

    Weismüller, J.; Gmeiner, B.; Huber, M.; John, L.; Mohr, M.; Rüde, U.; Wohlmuth, B.; Bunge, H. P.

    2015-12-01

    Mantle convection is the cause for plate tectonics, the formation of mountains and oceans, and the main driving mechanism behind earthquakes. The convection process is modeled by a system of partial differential equations describing the conservation of mass, momentum and energy. Characteristic to mantle flow is the vast disparity of length scales from global to microscopic, turning mantle convection simulations into a challenging application for high-performance computing. As system size and technical complexity of the simulations continue to increase, design and implementation of simulation models for next generation large-scale architectures is handled successfully only in an interdisciplinary context. A new priority program - named SPPEXA - by the German Research Foundation (DFG) addresses this issue, and brings together computer scientists, mathematicians and application scientists around grand challenges in HPC. Here we report from the TERRA-NEO project, which is part of the high visibility SPPEXA program, and a joint effort of four research groups. TERRA-NEO develops algorithms for future HPC infrastructures, focusing on high computational efficiency and resilience in next generation mantle convection models. We present software that can resolve the Earth's mantle with up to 1012 grid points and scales efficiently to massively parallel hardware with more than 50,000 processors. We use our simulations to explore the dynamic regime of mantle convection and assess the impact of small scale processes on global mantle flow.

  8. The thermal regimes of the upper mantle beneath Precambrian and Phanerozoic structures up to the thermobarometry data of mantle xenoliths

    NASA Astrophysics Data System (ADS)

    Glebovitsky, V. A.; Nikitina, L. P.; Khiltova, V. Ya.; Ovchinnikov, N. O.

    2004-05-01

    The thermal state of the upper mantle beneath tectonic structures of various ages and types (Archaean cratons, Early Proterozoic accretionary and collisional orogens, and Phanerozoic structures) is characterized by geotherms and by thermal gradients (TG) derived from data on the P- T conditions of mineral equilibria in garnet and garnet-spinel peridotite xenoliths from kimberlites (East Siberia, Northeastern Europe, India, Central Africa, North America, and Canada) and alkali basalts (Southeastern Siberia, Mongolia, southeastern China, southeastern Australia, Central Africa, South America, and the Solomon and Hawaiian islands). The use of the same garnet-orthopyroxene thermobarometer (Theophrastus Contributions to Advanced Studies in Geology. 3: Capricious Earth: Models and Modelling of Geologic Processes and Objects 2000 44) for all xenoliths allowed us to avoid discrepancies in estimation of the P- T conditions, which may be a result of the mismatch between different thermometers and barometers, and to compare the thermal regimes in the mantle in various regions. Thus, it was established that (1) mantle geotherms and geothermal gradients, obtained from the estimation of P- T equilibrium conditions of deep xenoliths, correspond to the age of crust tectonic structures and respectively to the time of lithosphere stabilization; it can be suggested that the ancient structures of the upper mantle were preserved within continental roots; (2) thermal regimes under continental mantle between the Archaean cratons and Palaeoproterozoic belts are different today; (3) the continental mantle under Neoproterozoic and Phanerozoic belts is characterized by significantly higher values of geothermal gradient compared to the mantle under Early Precambrian structures; (4) lithosphere dynamics seems to change at the boundary between Early and Mezo-Neoproterozoic and Precambrian and Phanerozoic.

  9. Core-Exsolved SiO2 Dispersal in the Earth's Mantle

    NASA Astrophysics Data System (ADS)

    Helffrich, George; Ballmer, Maxim D.; Hirose, Kei

    2018-01-01

    SiO2 may have been expelled from the core directly following core formation in the early stages of Earth's accretion and onward through the present day. On account of SiO2's low density with respect to both the core and the lowermost mantle, we examine the process of SiO2 accumulation at the core-mantle boundary (CMB) and its incorporation into the mantle by buoyant rise. Today, if SiO2 is 100-10,000 times more viscous than lower mantle material, the dimensions of SiO2 diapirs formed by the viscous Rayleigh-Taylor instability at the CMB would cause them to be swept into the mantle as inclusions of 100 m-10 km diameter. Under early Earth conditions of rapid heat loss after core formation, SiO2 diapirs of ˜1 km diameter could have risen independently of mantle flow to their level of neutral buoyancy in the mantle, trapping them there due to a combination of intrinsically high viscosity and neutral buoyancy. We examine the SiO2 yield by assuming Si + O saturation at the conditions found at the base of a magma ocean and find that for a range of conditions, dispersed bodies could reach as high as 8.5 vol % in parts of the lower mantle. At such low concentration, their effect on aggregate seismic wave speeds is within observational seismology uncertainty. However, their presence can account for small-scale scattering in the lower mantle due to the bodies' large-velocity contrast. We conclude that the shallow lower mantle (700-1,500 km depth) could harbor SiO2 released in early Earth times.

  10. Did 26Al and impact-induced heating differentiate Mercury?

    NASA Astrophysics Data System (ADS)

    Bhatia, G. K.; Sahijpal, S.

    2017-02-01

    Numerical models dealing with the planetary scale differentiation of Mercury are presented with the short-lived nuclide, 26Al, as the major heat source along with the impact-induced heating during the accretion of planets. These two heat sources are considered to have caused differentiation of Mars, a planet with size comparable to Mercury. The chronological records and the thermal modeling of Mars indicate an early differentiation during the initial 1 million years (Ma) of the formation of the solar system. We theorize that in case Mercury also accreted over an identical time scale, the two heat sources could have differentiated the planets. Although unlike Mars there is no chronological record of Mercury's differentiation, the proposed mechanism is worth investigation. We demonstrate distinct viable scenarios for a wide range of planetary compositions that could have produced the internal structure of Mercury as deduced by the MESSENGER mission, with a metallic iron (Fe-Ni-FeS) core of radius 2000 km and a silicate mantle thickness of 400 km. The initial compositions were derived from the enstatite and CB (Bencubbin) chondrites that were formed in the reducing environments of the early solar system. We have also considered distinct planetary accretion scenarios to understand their influence on thermal processing. The majority of our models would require impact-induced mantle stripping of Mercury by hit and run mechanism with a protoplanet subsequent to its differentiation in order to produce the right size of mantle. However, this can be avoided if we increase the Fe-Ni-FeS contents to 71% by weight. Finally, the models presented here can be used to understand the differentiation of Mercury-like exoplanets and the planetary embryos of Venus and Earth.

  11. The early thermal evolution of Mars

    NASA Astrophysics Data System (ADS)

    Bhatia, G. K.; Sahijpal, S.

    2016-01-01

    Hf-W isotopic systematics of Martian meteorites have provided evidence for the early accretion and rapid core formation of Mars. We present the results of numerical simulations performed to study the early thermal evolution and planetary scale differentiation of Mars. The simulations are confined to the initial 50 Myr (Ma) of the formation of solar system. The accretion energy produced during the growth of Mars and the decay energy due to the short-lived radio-nuclides 26Al, 60Fe, and the long-lived nuclides, 40K, 235U, 238U, and 232Th are incorporated as the heat sources for the thermal evolution of Mars. During the core-mantle differentiation of Mars, the molten metallic blobs were numerically moved using Stoke's law toward the center with descent velocity that depends on the local acceleration due to gravity. Apart from the accretion and the radioactive heat energies, the gravitational energy produced during the differentiation of Mars and the associated heat transfer is also parametrically incorporated in the present work to make an assessment of its contribution to the early thermal evolution of Mars. We conclude that the accretion energy alone cannot produce widespread melting and differentiation of Mars even with an efficient consumption of the accretion energy. This makes 26Al the prime source for the heating and planetary scale differentiation of Mars. We demonstrate a rapid accretion and core-mantle differentiation of Mars within the initial ~1.5 Myr. This is consistent with the chronological records of Martian meteorites.

  12. Determining the Metal/Silicate Partition Coefficient of Germanium: Implications for Core and Mantle Differentiation.

    NASA Technical Reports Server (NTRS)

    King, C.; Righter, K.; Danielson, L.; Pando, K.; Lee, C.

    2010-01-01

    Currently there are several hypotheses for the thermal state of the early Earth. Some hypothesize a shallow magma ocean, or deep magma ocean, or heterogeneous accretion which requires no magma ocean at all. Previous models are unable to account for Ge depletion in Earth's mantle relative to CI chondrites. In this study, the element Ge is used to observe the way siderophile elements partition into the metallic core. The purpose of this research is to provide new data for Ge and to further test these models for Earth's early stages. The partition coefficients (D(sub Ge) = c(sub metal)/c(sub silicate), where D = partition coefficient of Ge and c = concentration of Ge in the metal and silicate, respectively) of siderophile elements were studied by performing series of high pressure, high temperature experiments. They are also dependent on oxygen fugacity, and metal and silicate composition. Ge is a moderately siderophile element found in both the mantle and core, and has yet to be studied systematically at high temperatures. Moreover, previous work has been limited by the low solubility of Ge in silicate melts (less than 100 ppm and close to detection limits for electron microprobe analysis). Reported here are results from 14 experiments studying the partitioning of Ge between silicate and metallic liquids. The Ge concentrations were then analyzed using Laser Ablation Inductively Coupled Mass Spectrometry (LA-ICP-MS) which is sensitive enough to detect ppm levels of Ge in the silicate melt.

  13. Upper mantle fluids evolution, diamond formation, and mantle metasomatism

    NASA Astrophysics Data System (ADS)

    Huang, F.; Sverjensky, D. A.

    2017-12-01

    During mantle metasomatism, fluid-rock interactions in the mantle modify wall-rock compositions. Previous studies usually either investigated mineral compositions in xenoliths and xenocrysts brought up by magmas, or examined fluid compositions preserved in fluid inclusions in diamonds. However, a key study of Panda diamonds analysed both mineral and fluid inclusions in the diamonds [1] which we used to develop a quantitative characterization of mantle metasomatic processes. In the present study, we used an extended Deep Earth Water model [2] to simulate fluid-rock interactions at upper mantle conditions, and examine the fluids and mineral assemblages together simultaneously. Three types of end-member fluids in the Panda diamond fluid inclusions include saline, rich in Na+K+Cl; silicic, rich in Si+Al; and carbonatitic, rich in Ca+Mg+Fe [1, 3]. We used the carbonatitic end-member to represent fluid from a subducting slab reacting with an excess of peridotite + some saline fluid in the host environment. During simultaneous fluid mixing and reaction with the host rock, the logfO2 increased by about 1.6 units, and the pH increased by 0.7 units. The final minerals were olivine, garnet and diamond. The Mg# of olivine decreased from 0.92 to 0.85. Garnet precipitated at an early stage, and its Mg# also decreased with reaction progress, in agreement with the solid inclusions in the Panda diamonds. Phlogopite precipitated as an intermediate mineral and then disappeared. The aqueous Ca, Mg, Fe, Si and Al concentrations all increased, while Na, K, and Cl concentrations decreased during the reaction, consistent with trends in the fluid inclusion compositions. Our study demonstrates that fluids coming from subducting slabs could trigger mantle metasomatism, influence the compositions of sub-lithospherc cratonic mantle, precipitate diamonds, and change the oxygen fugacity and pH of the upper mantle fluids. [1] Tomlinson et al. EPSL (2006); [2] Sverjensky, DA et al., GCA (2014

  14. Evolving Mantle Sources in Postcollisional Early Permian-Triassic Magmatic Rocks in the Heart of Tianshan Orogen (Western China)

    NASA Astrophysics Data System (ADS)

    Tang, Gong-Jian; Cawood, Peter A.; Wyman, Derek A.; Wang, Qiang; Zhao, Zhen-Hua

    2017-11-01

    Magmatism postdating the initiation of continental collision provides insight into the late stage evolution of orogenic belts including the composition of the contemporaneous underlying subcontinental mantle. The Awulale Mountains, in the heart of the Tianshan Orogen, display three types of postcollisional mafic magmatic rocks. (1) A medium to high K calc-alkaline mafic volcanic suite (˜280 Ma), which display low La/Yb ratios (2.2-11.8) and a wide range of ɛNd(t) values from +1.9 to +7.4. This suite of rocks was derived from melting of depleted metasomatized asthenospheric mantle followed by upper crustal contamination. (2) Mafic shoshonitic basalts (˜272 Ma), characterized by high La/Yb ratios (14.4-20.5) and more enriched isotope compositions (ɛNd(t) = +0.2 - +0.8). These rocks are considered to have been generated by melting of lithospheric mantle enriched by melts from the Tarim continental crust that was subducted beneath the Tianshan during final collisional suturing. (3) Mafic dikes (˜240 Ma), with geochemical and isotope compositions similiar to the ˜280 Ma basaltic rocks. This succession of postcollision mafic rock types suggests there were two stages of magma generation involving the sampling of different mantle sources. The first stage, which occurred in the early Permian, involved a shift from depleted asthenospheric sources to enriched lithospheric mantle. It was most likely triggered by the subduction of Tarim continental crust and thickening of the Tianshan lithospheric mantle. During the second stage, in the middle Triassic, there was a reversion to more asthenospheric sources, related to postcollision lithospheric thinning.

  15. A Mercury-like component of early Earth yields uranium in the core and high mantle (142)Nd.

    PubMed

    Wohlers, Anke; Wood, Bernard J

    2015-04-16

    Recent (142)Nd isotope data indicate that the silicate Earth (its crust plus the mantle) has a samarium to neodymium elemental ratio (Sm/Nd) that is greater than that of the supposed chondritic building blocks of the planet. This elevated Sm/Nd has been ascribed either to a 'hidden' reservoir in the Earth or to loss of an early-formed terrestrial crust by impact ablation. Since removal of crust by ablation would also remove the heat-producing elements--potassium, uranium and thorium--such removal would make it extremely difficult to balance terrestrial heat production with the observed heat flow. In the 'hidden' reservoir alternative, a complementary low-Sm/Nd layer is usually considered to reside unobserved in the silicate lower mantle. We have previously shown, however, that the core is a likely reservoir for some lithophile elements such as niobium. We therefore address the question of whether core formation could have fractionated Nd from Sm and also acted as a sink for heat-producing elements. We show here that addition of a reduced Mercury-like body (or, alternatively, an enstatite-chondrite-like body) rich in sulfur to the early Earth would generate a superchondritic Sm/Nd in the mantle and an (142)Nd/(144)Nd anomaly of approximately +14 parts per million relative to chondrite. In addition, the sulfur-rich core would partition uranium strongly and thorium slightly, supplying a substantial part of the 'missing' heat source for the geodynamo.

  16. A Mercury-like component of early Earth yields uranium in the core and high mantle 142Nd

    NASA Astrophysics Data System (ADS)

    Wohlers, Anke; Wood, Bernard J.

    2015-04-01

    Recent 142Nd isotope data indicate that the silicate Earth (its crust plus the mantle) has a samarium to neodymium elemental ratio (Sm/Nd) that is greater than that of the supposed chondritic building blocks of the planet. This elevated Sm/Nd has been ascribed either to a `hidden' reservoir in the Earth or to loss of an early-formed terrestrial crust by impact ablation. Since removal of crust by ablation would also remove the heat-producing elements--potassium, uranium and thorium--such removal would make it extremely difficult to balance terrestrial heat production with the observed heat flow. In the `hidden' reservoir alternative, a complementary low-Sm/Nd layer is usually considered to reside unobserved in the silicate lower mantle. We have previously shown, however, that the core is a likely reservoir for some lithophile elements such as niobium. We therefore address the question of whether core formation could have fractionated Nd from Sm and also acted as a sink for heat-producing elements. We show here that addition of a reduced Mercury-like body (or, alternatively, an enstatite-chondrite-like body) rich in sulfur to the early Earth would generate a superchondritic Sm/Nd in the mantle and an 142Nd/144Nd anomaly of approximately +14 parts per million relative to chondrite. In addition, the sulfur-rich core would partition uranium strongly and thorium slightly, supplying a substantial part of the `missing' heat source for the geodynamo.

  17. Core-exsolved SiO2 Dispersal in the Earth's Mantle

    NASA Astrophysics Data System (ADS)

    Helffrich, G. R.; Ballmer, M.; Hirose, K.

    2017-12-01

    SiO2 may have been expelled from the core following its formation in the early stages of Earth's accretion and onwards through the present day. On account of SiO2's low density with respect to both the core and the lowermost mantle, we examine the process of SiO2 accumulation at the core-mantle boundary (CMB) and its incorporation into the mantle by buoyant rise. Today, the if SiO2 is 100-10000 times more viscous than lower mantle material, the dimensions of SiO2 diapirs formed by the viscous Rayleigh-Taylor instability at the CMB would cause them to be swept into the mantle as inclusions of 100 m - 10 km diameter. Under early Earth conditions of rapid heat loss after core formation, SiO2 diapirs of 5-80 km diameter could have risen independently of mantle flow to their level of neutral buoyancy in the mantle, trapping them there due to a combination of high viscosity and neutral buoyancy. We examine the SiO2 yield by assuming Si+O saturation at the conditions found at the base of a magma ocean and find that for a range of conditions, dispersed bodies could reach as high as 2 volume percent in shallow parts of the lower mantle, with their abundance decreasing with depth. At such low concentrations, their effect on aggregate seismic wavespeeds would be within the uncertainty of the radial Earth model PREM. However, their presence would be revealed by small-scale scattering in the lower mantle due to the bodies' large velocity contrast. We conclude that the shallow lower mantle (700-1500 km depth) could harbor SiO2 released in early Earth times.

  18. MORB mantle hosts the missing Eu (Sr, Nb, Ta and Ti) in the continental crust: New perspectives on crustal growth, crust-mantle differentiation and chemical structure of oceanic upper mantle

    NASA Astrophysics Data System (ADS)

    Niu, Yaoling; O'Hara, Michael J.

    2009-09-01

    We have examined the high quality data of 306 mid-ocean ridge basalt (MORB) glass samples from the East Pacific Rise (EPR), near-EPR seamounts, Pacific Antarctic Ridge (PAR), near-PAR seamounts, Mid-Atlantic Ridge (MAR), and near-MAR seamounts. The data show a correlated variation between Eu/Eu* and Sr/Sr*, and both decrease with decreasing MgO, pointing to the effect of plagioclase crystallization. The observation that samples with MgO > 9.5 wt.% (before plagioclase on the liquidus) show Eu/Eu* > 1 and Sr/Sr* > 1 and that none of the major phases (i.e., olivine, orthopyroxene, clinopyroxene, spinel and garnet) in the sub-ridge mantle melting region can effectively fractionate Eu and Sr from otherwise similarly incompatible elements indicates that the depleted MORB mantle (DMM) possesses excess Sr and Eu, i.e., [Sr/Sr*]DMM > 1 and [Eu/Eu*]DMM > 1. Furthermore, the well-established observation that DNb ≈ DTh, DTa ≈ DU and DTi ≈ DSm during MORB mantle melting, yet primitive MORB melts all have [Nb/Th]PMMORB > 1, [Ta/U]PMMORB > 1 and [Ti/Sm]PMMORB > 1 (where PM indicates primitive mantle normalized), also points to the presence of excess Nb, Ta and Ti in the DMM, i.e., [Nb/Th]PMDMM > 1, [Ta/U]PMDMM > 1 and [Ti/Sm]PMDMM > 1. The excesses of Eu, Sr, Nb, Ta and Ti in the DMM complement the well-known deficiencies of these elements in the bulk continental crust (BCC). These new observations, which support the notion that the DMM and BCC are complementary in terms of the overall abundances of incompatible elements, offer new insights into the crust-mantle differentiation. These observations are best explained by partial melting of amphibolite of MORB protolith during continental collision, which produces andesitic melts with a remarkable compositional (major and trace element abundances as well as key elemental ratios) similarity to the BCC, as revealed by andesites in southern Tibet produced during the India-Asia continental collision. An average amphibolite of MORB

  19. Petrogenesis of early Jurassic basalts in southern Jiangxi Province, South China: Implications for the thermal state of the Mesozoic mantle beneath South China

    NASA Astrophysics Data System (ADS)

    Cen, Tao; Li, Wu-xian; Wang, Xuan-ce; Pang, Chong-jin; Li, Zheng-xiang; Xing, Guang-fu; Zhao, Xi-lin; Tao, Jihua

    2016-07-01

    Early Jurassic bimodal volcanic and intrusive rocks in southern South China show distinct associations and distribution patterns in comparison with those of the Middle Jurassic and Cretaceous rocks in the area. It is widely accepted that these rocks formed in an extensional setting, although the timing of the onset and the tectonic driver for extension are debated. Here, we present systematic LA-ICP-MS zircon U-Pb ages, whole-rock geochemistry and Sr-Nd isotope data for bimodal volcanic rocks from the Changpu Formation in the Changpu-Baimianshi and Dongkeng-Linjiang basins in southern Jiangxi Province, South China. Zircon U-Pb ages indicate that the bimodal volcanic rocks erupted at ca. 190 Ma, contemporaneous with the Fankeng basalts ( 183 Ma). A compilation of geochronological results demonstrates that basin-scale basaltic eruptions occurred during the Early Jurassic within a relatively short interval (< 5 Ma). These Early Jurassic basalts have tholeiitic compositions and OIB-like trace element distribution patterns. Geochemical analyses show that the basalts were derived from depleted asthenospheric mantle, dominated by a volatile-free peridotite source. The calculated primary melt compositions suggest that the basalts formed at 1.9-2.1 GPa, with melting temperatures of 1378 °C-1405 °C and a mantle potential temperature (TP) ranging from 1383 °C to 1407 °C. The temperature range is somewhat hotter than normal mid-ocean-basalt (MORB) mantle but similar to an intra-plate continental mantle setting, such as the Basin and Range Province in western North America. This study provides an important constraint on the Early Jurassic mantle thermal state beneath South China. Reference: Raczek, I., Stoll, B., Hofmann, A.W., Jochum, K.P. 2001. High-precision trace element data for the USGS reference materials BCR-1, BCR-2, BHVO-1, BHVO-2, AGV-1, AGV-2, DTS-1, DTS-2, GSP-1 and GSP-2 by ID-TIMS and MIC-SSMS. Geostandards Newsletter 25(1), 77-86.

  20. Depletion of Vandium in Planetary Mantles: Controlled by Metal, Oxide, or Silicate?

    NASA Technical Reports Server (NTRS)

    Righter, Kevin

    2006-01-01

    Vanadium concentrations in planetary mantles can provide information about the conditions during early accretion and differentiation. Because V is a slightly siderophile element, it is usually assumed that any depletion would be due to core formation and metal-silicate equilibrium. However, V is typically more compatible in phases such as spinel, magnesiowuestite and garnet. Fractionation of all of these phases would cause depletions more marked than those from metal. In this paper consideration of depletions due to metal, oxide and silicate are critically evaluated.

  1. Simultaneous generation of Superpiles and Superplumes in the lower mantle

    NASA Astrophysics Data System (ADS)

    Ballmer, M. D.; Lekic, V.; Ito, G.

    2014-12-01

    volcanism. The predicted sub-horizontal compositional boundary between the basal Superpiles and the overlying Superplumes further provides an explanation for steep vertical gradients in Vs observed at 400-700 km height above the CMB. Such a LLSVP subdivision holds implications for the early and ongoing differentiation and thermal evolution of our planet.

  2. Mantle contribution and tectonic transition in the Aqishan-Yamansu Belt, Eastern Tianshan, NW China: Insights from geochronology and geochemistry of Early Carboniferous to Early Permian felsic intrusions

    NASA Astrophysics Data System (ADS)

    Du, Long; Long, Xiaoping; Yuan, Chao; Zhang, Yunying; Huang, Zongying; Wang, Xinyu; Yang, Yueheng

    2018-04-01

    Late Paleozoic is a key period for the accretion and collision of the southern Central Asian Orogenic Belt (CAOB). Here, we present new zircon U-Pb ages, whole-rock geochemistry and Sr-Nd isotopic compositions for four Late Paleozoic felsic plutons in Eastern Tianshan (or Tienshan in some literatures) in order to constrain the tectonic evolution of the southern CAOB. The granodioritic pluton and its dioritic enclaves were synchronously formed in the Early Carboniferous (336 ± 3 Ma and 335 ± 2 Ma, respectively). These rocks are depleted in Nb, Ta and Ti, and enriched in Rb, Ba, Th and U related to the primitive mantle, which show typical features of arc rocks. They both have similar Sr-Nd isotopic ratios to those granitic rocks from the eastern Central Tianshan Block and have the latest Mesoproterozoic two stage Nd model ages (TDM2) (1111-1195 Ma for the granodioritic pluton and 1104-1108 Ma for the enclaves, respectively), indicating that their source magmas may have been derived from the Mesoproterozoic crust. The albitophyric pluton was also emplaced in the Early Carboniferous (333 ± 3 Ma). Rocks of this pluton have similar εNd(t) values (-0.69 to -0.37) and TDM2 ages (1135-1161 Ma) to those of the granodioritic rocks, suggest similar crustal source for both types of rocks. In contrast, the K-feldspar granitic and monzonitic plutons were emplaced in the Early Permian (292 ± 3 Ma and 281 ± 2 Ma, respectively). Samples of the K-feldspar granitic pluton have high K2O + Na2O, FeO/MgO, Ga/Al, HFSE (e.g., Zr and Hf) and low CaO, Sr and Ba, exhibiting characteristics of A2-type granites, which probably emplaced in a post-collisional extension environment. They have higher εNd(t) values (+2.77 to +3.27) and more juvenile TDM2 ages (799-841 Ma) than the Early Carboniferous plutons, suggesting that they were derived from relatively younger crustal sources. The monzonitic granites are metaluminous to weakly peraluminous with A/CNK ranging from 0.93 to 1.05, and have

  3. Geochemical Constraints on Core-Mantle Interaction from Fe/Mn Ratios

    NASA Astrophysics Data System (ADS)

    Humayun, M.; Qin, L.

    2003-12-01

    The greater density of liquid iron alloy, and its immiscibility with silicate, maintains the physical separation of the core from the mantle. There are no a priori reasons, however, why the Earth's mantle should be chemically isolated from the core. Osmium isotopic variations in mantle plumes have been interpreted in terms of interaction between outer core and the source regions of deep mantle plumes. If chemical transport occurs across the core-mantle boundary its mechanism remains to be established. The Os isotope evidence has also been interpreted as the signatures of subducted Mn-sediments, which are known to have relatively high Pt/Os. In the mantle, Fe occurs mainly as the divalent ferrous ion, and Mn occurs solely as a divalent ion, and both behave in a geochemically coherent manner because of similarity in ionic charge and radius. Thus, the Fe/Mn ratio is a planetary constant insensitive to processes of mantle differentiation by partial melting. Two processes may perturb the ambient mantle Fe/Mn of 60: a) the subduction of Mn-sediments should decrease the Fe/Mn ratio in plume sources, while b) chemical transport from the outer core may increase the Fe/Mn ratio. The differentiation of the liquid outer core to form the solid inner core may increase abundances of the light element constituents (FeS, FeO, etc.) to the point of exsolution from the core at the CMB. The exact rate of this process is determined by the rate of inner core growth. Two end-member models include 1) inner core formation mainly prior to 3.5 Ga with heat release dominated by radioactive sources, or 2) inner core formation occurring mainly in the last 1.5 Ga with heat release dominated by latent heat. This latter model would imply large fluxes of Fe into the sources of modern mantle plumes. Existing Fe/Mn data for Gorgona and Hawaiian samples place limits on both these processes. We describe a new procedure for the precise determination of the Fe/Mn ratio in magmatic rocks by ICP-MS. This

  4. Evolution of the earliest mantle caused by the magmatism-mantle upwelling feedback: Implications for the Moon and the Earth

    NASA Astrophysics Data System (ADS)

    Ogawa, M.

    2017-12-01

    The two most important agents that cause mantle evolution are magmatism and mantle convection. My earlier 2D numerical models of a coupled magmatism-mantle convection system show that these two agents strongly couple each other, when the Rayleigh number Ra is sufficiently high: magmatism induced by a mantle upwelling flow boosts the upwelling flow itself. The mantle convection enhanced by this positive feedback (the magmatism-mantle upwelling, or MMU, feedback) causes vigorous magmatism and, at the same time, strongly stirs the mantle. I explored how the MMU feedback influences the evolution of the earliest mantle that contains the magma ocean, based on a numerical model where the mantle is hot and its topmost 1/3 is partially molten at the beginning of the calculation: The evolution drastically changes its style, as Ra exceeds the threshold for onset of the MMU feedback, around 107. At Ra < 107, basaltic materials generated by the initial widespread magmatism accumulate in the deep mantle to form a layer; the basaltic layer is colder than the overlying shallow mantle. At Ra > 107, however, the mantle remains compositionally more homogeneous in spite of the widespread magmatism, and the deep mantle remains hotter than the shallow mantle, because of the strong convective stirring caused by the feedback. The threshold value suggests that the mantle of a planet larger than Mars evolves in a way substantially different from that in the Moon does. Indeed, in my earlier models, magmatism makes the early mantle compositionally stratified in the Moon, but the effects of strong convective stirring overwhelms that of magmatism to keep the mantle compositionally rather homogeneous in Venus and the Earth. The MMU feedback is likely to be a key to understanding why vestiges of the magma ocean are so scarce in the Earth.

  5. Volcanism on Mars controlled by early oxidation of the upper mantle

    NASA Astrophysics Data System (ADS)

    Tuff, J.; Wade, J.; Wood, B. J.

    2013-06-01

    Detailed information about the chemical composition and evolution of Mars has been derived principally from the SNC (shergottite-nakhlite-chassignite) meteorites, which are genetically related igneous rocks of Martian origin. They are chemically and texturally similar to terrestrial basalts and cumulates, except that they have higher concentrations of iron and volatile elements such as phosphorus and chlorine and lower concentrations of nickel and other chalcophile (sulphur-loving) elements. Most Martian meteorites have relatively young crystallization ages (1.4 billion years to 180 million years ago) and are considered to be derived from young, lightly cratered volcanic regions, such as the Tharsis plateau. Surface rocks from the Gusev crater analysed by the Spirit rover are much older (about 3.7 billion years old) and exhibit marked compositional differences from the meteorites. Although also basaltic in composition, the surface rocks are richer in nickel and sulphur and have lower manganese/iron ratios than the meteorites. This has led to doubts that Mars can be described adequately using the `SNC model'. Here we show, however, that the differences between the compositions of meteorites and surface rocks can be explained by differences in the oxygen fugacity during melting of the same sulphur-rich mantle. This ties the sources of Martian meteorites to those of the surface rocks through an early (>3.7 billion years ago) oxidation of the uppermost mantle that had less influence on the deeper regions, which produce the more recent volcanic rocks.

  6. Long-Term Stability of Plate-Like Behavior Caused by Hydrous Mantle Convection and Water Absorption in the Deep Mantle

    NASA Astrophysics Data System (ADS)

    Nakagawa, Takashi; Iwamori, Hikaru

    2017-10-01

    We investigate the cycling of water (regassing, dehydration, and degassing) in mantle convection simulations as a function of the strength of the oceanic lithosphere and its influence on the evolution of mantle water content. We also consider pseudo-plastic yielding with a friction coefficient for simulating brittle behavior of the plates and the water-weakening effect of mantle materials. This model can generate long-term plate-like behavior as a consequence of the water-weakening effect of mantle minerals. This finding indicates that water cycling plays an essential role in generating tectonic plates. In vigorous plate motion, the mantle water content rapidly increases by up to approximately 4-5 ocean masses, which we define as the "burst" effect. A burst is related to the mantle temperature and water solubility in the mantle transition zone. When the mantle is efficiently cooled down, the mantle transition zone can store water transported by the subducted slabs that can pass through the "choke point" of water solubility. The onset of the burst effect is strongly dependent on the friction coefficient. The burst effect of the mantle water content could have significantly influenced the evolution of the surface water if the burst started early, in which case the Earth's surface cannot preserve the surface water over the age of the Earth.

  7. Redox state of the Archean mantle: Evidence from V partitioning in 3.5-2.4 Ga komatiites

    NASA Astrophysics Data System (ADS)

    Nicklas, Robert W.; Puchtel, Igor S.; Ash, Richard D.

    2018-02-01

    Oxygen fugacity of the mantle is a crucial thermodynamic parameter that controls such fundamental processes as planetary differentiation, mantle melting, and possible core-mantle exchange. Constraining the evolution of the redox state of the mantle is of paramount importance for understanding the chemical evolution of major terrestrial reservoirs, including the core, mantle, and atmosphere. In order to evaluate the secular evolution of the redox state of the mantle, oxygen fugacities of six komatiite systems, ranging in age from 3.48 to 2.41 Ga, were determined using high-precision partitioning data of the redox-sensitive element vanadium between liquidus olivine, chromite and komatiitic melt. The calculated oxygen fugacities range from -0.11 ± 0.30 ΔFMQ log units in the 3.48 Ga Komati system to +0.43 ± 0.26 ΔFMQ log units in the 2.41 Ga Vetreny system. Although there is a slight hint in the data for an increase in the oxygen fugacity of the mantle between 3.48 and 2.41 Ga, these values generally overlap within their respective uncertainties; they are also largely within the range of oxygen fugacity estimates for modern MORB lavas of +0.60 ± 0.30 ΔFMQ log units that we obtained using the same technique. Our results are consistent with the previous findings that argued for little change in the mantle oxygen fugacity since the early Archean and indicate that the mantle had reached its nearly-present day redox state by at least 3.48 Ga.

  8. Compositional mantle layering revealed by slab stagnation at ~1000-km depth

    PubMed Central

    Ballmer, Maxim D.; Schmerr, Nicholas C.; Nakagawa, Takashi; Ritsema, Jeroen

    2015-01-01

    Improved constraints on lower-mantle composition are fundamental to understand the accretion, differentiation, and thermochemical evolution of our planet. Cosmochemical arguments indicate that lower-mantle rocks may be enriched in Si relative to upper-mantle pyrolite, whereas seismic tomography images suggest whole-mantle convection and hence appear to imply efficient mantle mixing. This study reconciles cosmochemical and geophysical constraints using the stagnation of some slab segments at ~1000-km depth as the key observation. Through numerical modeling of subduction, we show that lower-mantle enrichment in intrinsically dense basaltic lithologies can render slabs neutrally buoyant in the uppermost lower mantle. Slab stagnation (at depths of ~660 and ~1000 km) and unimpeded slab sinking to great depths can coexist if the basalt fraction is ~8% higher in the lower mantle than in the upper mantle, equivalent to a lower-mantle Mg/Si of ~1.18. Global-scale geodynamic models demonstrate that such a moderate compositional gradient across the mantle can persist can in the presence of whole-mantle convection. PMID:26824060

  9. Decreasing µ142Nd Variation in the Archean Convecting Mantle from 4.0 to 2.5 Ga: Heterogeneous Domain Mixing or Crustal Recycling?

    NASA Astrophysics Data System (ADS)

    Brandon, A. D.; Debaille, V.

    2014-12-01

    The 146Sm-142Nd (t1/2=68 Ma) chronometer can be used to examine silicate differentiation in the first 400 Ma of Earth history. Early fractionation between Sm and Nd is recorded in cratonic Archean rocks in their 142Nd/144Nd ratios that that deviate up to ±20 ppm, or μ142Nd - ppm deviation relative to the present-day convecting mantle at 0. These values likely record early extraction of incompatible trace element (ITE) enriched material with -μ142Nd, either as crust or late stage residual melt from a magma ocean, and resulting in a complimentary ITE depleted residual mantle with +μ142Nd. If this early-formed ITE-enriched material was re-incorporated rapidly back into the convecting mantle, both ITE-enriched and ITE-depleted mantle domains would have been established in the Hadean. Alternatively, if it was early-formed crust that remained stable it could have slowly eroded and progressively remixed into the convecting mantle as subducted sediment during the Archean. Each of these scenarios could potentially explain the decrease in the maximum variation in µ142Nd from ±20 at 4.0 Ga to 0 at 2.5 Ga [1,2,3]. In the scenario where these variations reflect mixing of mantle domains, this implies long mantle mixing times of greater than 1 Ga in the Archean in order to preserve the early-formed heterogeneities. This can be achieved in a stagnant lid tectonic regime in the Archean with sporadic and short subduction cycles [2]. This scenario would also indicate that mixing times in the convecting mantle were much slower than the previously proposed 100 Ma in the Hadean and Archean. In the alternative scenario, sediment with -µ142Nd was progressively mixed into the mantle via subduction in the Archean [3]. This scenario doesn't require slow mantle mixing times or a stagnant-lid regime. It requires crustal resident times of up to 750 Ma to maintain a steady supply of ancient sediment recycling over the Archean. Each of these scenarios evoke very contrasting conditions for

  10. Discovery Of Low Oxygen Fugacity (fo2) Mineral And Fluid Phases In Lower Mantle -Derived Early Pulse Of The Deccan Flood Basalts

    NASA Astrophysics Data System (ADS)

    Basu, A. R.; Das, S.

    2017-12-01

    Estimation of Earth's lower mantle mineralogy and oxygen fugacity are principally based on indirect geophysical and experimental studies. According to these studies, the mantle becomes increasingly reducing from upper to lower mantle due to the distribution of ferric (Fe3+) and ferrous (Fe2+) iron in perovskite, the dominant mineral phase in the lower mantle. However, the natural occurrence of low oxygen fugacity (fO2), lower mantle mineral and fluid phases are rare, except some for discrete inclusions in superdeep diamonds. In this study, we document that some rocks associated with plume volcanism, such as the Deccan flood basalt volcanic province, preserve the lower mantle mineral phases. We document here unusual primary texture - bearing minerals in olivine-clinopyroxene bearing picrite intrusives associated with the Deccan Traps. The olivine and clinopyroxene of these rocks have high 3He/4He ratio (R/RA 14) as well as Nd, Sr and Pb isotopes identical to those of the Réunion plume, clearly indicating their lower mantle - derivation. These rocks are the initial pulse at 68Ma of the Deccan Trap eruption [1]. Presence of unusual exsolved lamella and rectangular, vermicular intergrowths of diopside and magnetite in olivine indicate a precursory phase with higher Fe3+. The diopside part in rectangular intergrowth show presence of hydrocarbon. Trails of small graphitic carbon crystals are also present both in the cores of these olivine and diopside. We suggest that the hydrocarbons are derived from the lower mantle having much lesser fO2 than the upper mantle. This study unequivocally indicates that direct lower mantle mineralogical signature, including their fo2 can be obtained from early pulse of plume volcanism. References: [1] Basu A R, Renne P R, Dasgupta D K, Teichmann F, Poreda R J, Science 261, 902 - 906; 1993.

  11. Primordial helium entrained by the hottest mantle plumes

    NASA Astrophysics Data System (ADS)

    Jackson, M. G.; Konter, J. G.; Becker, T. W.

    2017-02-01

    Helium isotopes provide an important tool for tracing early-Earth, primordial reservoirs that have survived in the planet’s interior. Volcanic hotspot lavas, like those erupted at Hawaii and Iceland, can host rare, high 3He/4He isotopic ratios (up to 50 times the present atmospheric ratio, Ra) compared to the lower 3He/4He ratios identified in mid-ocean-ridge basalts that form by melting the upper mantle (about 8Ra; ref. 5). A long-standing hypothesis maintains that the high-3He/4He domain resides in the deep mantle, beneath the upper mantle sampled by mid-ocean-ridge basalts, and that buoyantly upwelling plumes from the deep mantle transport high-3He/4He material to the shallow mantle beneath plume-fed hotspots. One problem with this hypothesis is that, while some hotspots have 3He/4He values ranging from low to high, other hotspots exhibit only low 3He/4He ratios. Here we show that, among hotspots suggested to overlie mantle plumes, those with the highest maximum 3He/4He ratios have high hotspot buoyancy fluxes and overlie regions with seismic low-velocity anomalies in the upper mantle, unlike plume-fed hotspots with only low maximum 3He/4He ratios. We interpret the relationships between 3He/4He values, hotspot buoyancy flux, and upper-mantle shear wave velocity to mean that hot plumes—which exhibit seismic low-velocity anomalies at depths of 200 kilometres—are more buoyant and entrain both high-3He/4He and low-3He/4He material. In contrast, cooler, less buoyant plumes do not entrain this high-3He/4He material. This can be explained if the high-3He/4He domain is denser than low-3He/4He mantle components hosted in plumes, and if high-3He/4He material is entrained from the deep mantle only by the hottest, most buoyant plumes. Such a dense, deep-mantle high-3He/4He domain could remain isolated from the convecting mantle, which may help to explain the preservation of early Hadean (>4.5 billion years ago) geochemical anomalies in lavas sampling this reservoir.

  12. On the formation of continental silicic melts in thermochemical mantle convection models: implications for early Earth

    NASA Astrophysics Data System (ADS)

    van Thienen, P.; van den Berg, A. P.; Vlaar, N. J.

    2004-12-01

    Important constituents of Archean cratons, formed in the early and hot history of the Earth, are Tonalite-Trondhjemite-Granodiorite (TTG) plutons and greenstone belts. The formation of these granite-greenstone terrains is often ascribed to plate-tectonic processes. Buoyancy considerations, however, do not allow plate tectonics to take place in a significantly hotter Earth. We therefore propose an alternative mechanism for the coeval and proximate production of TTG plutons and greenstone-like crustal successions. That is, when a locally anomalously thick basaltic crust has been produced by continued addition of extrusive or intrusive basalts due to partial melting of the underlying convecting mantle, the transition of a sufficient amount of basalt in the lower crust to eclogite may trigger a resurfacing event, in which a complete crustal section of over 1000 km long sinks into the mantle in less than 2 million years. Pressure release partial melting in the complementary upwelling mantle produces large volumes of basaltic material replacing the original crust. Partial melting at the base of this newly produced crust may generate felsic melts which are added as intrusives and/or extrusives to the generally mafic crustal succession, adding to what resembles a greenstone belt. Partial melting of metabasalt in the sinking crustal section produces a significant volume of TTG melt which is added to the crust directly above the location of 'subduction', presumably in the form of a pluton. This scenario is self-consistently produced by numerical thermochemical mantle convection models, presented in this paper, including partial melting of mantle peridotite and crustal (meta)basalt. The metamorphic p, T conditions under which partial melting of metabasalt takes place in this scenario are consistent with geochemical trace element data for TTGs, which indicate melting under amphibolite rather than eclogite facies. Other geodynamical settings which we have also investigated

  13. Chondritic xenon in the Earth's mantle.

    PubMed

    Caracausi, Antonio; Avice, Guillaume; Burnard, Peter G; Füri, Evelyn; Marty, Bernard

    2016-05-05

    Noble gas isotopes are powerful tracers of the origins of planetary volatiles, and the accretion and evolution of the Earth. The compositions of magmatic gases provide insights into the evolution of the Earth's mantle and atmosphere. Despite recent analytical progress in the study of planetary materials and mantle-derived gases, the possible dual origin of the planetary gases in the mantle and the atmosphere remains unconstrained. Evidence relating to the relationship between the volatiles within our planet and the potential cosmochemical end-members is scarce. Here we show, using high-precision analysis of magmatic gas from the Eifel volcanic area (in Germany), that the light xenon isotopes identify a chondritic primordial component that differs from the precursor of atmospheric xenon. This is consistent with an asteroidal origin for the volatiles in the Earth's mantle, and indicates that the volatiles in the atmosphere and mantle originated from distinct cosmochemical sources. Furthermore, our data are consistent with the origin of Eifel magmatism being a deep mantle plume. The corresponding mantle source has been isolated from the convective mantle since about 4.45 billion years ago, in agreement with models that predict the early isolation of mantle domains. Xenon isotope systematics support a clear distinction between mid-ocean-ridge and continental or oceanic plume sources, with chemical heterogeneities dating back to the Earth's accretion. The deep reservoir now sampled by the Eifel gas had a lower volatile/refractory (iodine/plutonium) composition than the shallower mantle sampled by mid-ocean-ridge volcanism, highlighting the increasing contribution of volatile-rich material during the first tens of millions of years of terrestrial accretion.

  14. Non-chondritic iron isotope ratios in planetary mantles as a result of core formation

    NASA Astrophysics Data System (ADS)

    Elardo, Stephen M.; Shahar, Anat

    2017-02-01

    Information about the materials and conditions involved in planetary formation and differentiation in the early Solar System is recorded in iron isotope ratios. Samples from Earth, the Moon, Mars and the asteroid Vesta reveal significant variations in iron isotope ratios, but the sources of these variations remain uncertain. Here we present experiments that demonstrate that under the conditions of planetary core formation expected for the Moon, Mars and Vesta, iron isotopes fractionate between metal and silicate due to the presence of nickel, and enrich the bodies' mantles in isotopically light iron. However, the effect of nickel diminishes at higher temperatures: under conditions expected for Earth's core formation, we infer little fractionation of iron isotopes. From our experimental results and existing conceptual models of magma ocean crystallization and mantle partial melting, we find that nickel-induced fractionation can explain iron isotope variability found in planetary samples without invoking nebular or accretionary processes. We suggest that near-chondritic iron isotope ratios of basalts from Mars and Vesta, as well as the most primitive lunar basalts, were achieved by melting of isotopically light mantles, whereas the heavy iron isotope ratios of terrestrial ocean floor basalts are the result of melting of near-chondritic Earth mantle.

  15. [Biochemistry and functional characterization of squid mantle meat (Dosidicus gigas)].

    PubMed

    Abugoch, L; Guarda, A; María Pérez, L; Isabel Donghi, M

    2000-12-01

    A study for the characterization of frozen giant squid mantle (meat) protein stored at -25 degrees C for 8 month was started. In the present research, the following functional properties were investigate: emulsifying, water holding and gel forming capacities. Optimal conditions for the separation and differentiation of miofibrillar and sarcoplasmatic proteins were also studied. It was found that the unfrozen giant squid mantle meat es capable of emulifying 2.817,4 g of oil/g of protein and holding capacity was 3.64 g of water/g of protein. Related to the gel forming capacity, it was not obtain, probably due to excessive storage of the meat. With regard to miofibrilar protein obtention of the squid mantle meat, it was found that two low ionic strength washings (I = 0.05), the sarcoplasmic proteins were practically eliminated from the protein matrix. The differentiation of miofibrilar and sarcoplasmatic proteins was obtained by PAGE-SDS of the squid mantle meat extracted at two different ionic strength (I = 0.05 and I = 0.5). This work demonstrates that the giant squid mantle protein has a high emulsifying and water holding capacity, and it can be used, as a raw material, for the improvement of sausage products. About the gelling products, more studies will be necessary with fresh squid mantle meat to conclude about this functional property.

  16. Lithospheric mantle structure beneath Northern Scotland: Pre-plume remnant or syn-plume signature?

    NASA Astrophysics Data System (ADS)

    Knapp, J.

    2003-04-01

    Upper mantle reflectors (Flannan and W) beneath the northwestern British Isles are some of the best-known and most-studied examples of preserved structure within the continental mantle lithosphere, and are spatially coincident with the surface location of early Iceland plume volcanism in the British Tertiary Province. First observed on BIRPS (British Institutions Reflection Profiling Syndicate) marine deep seismic reflection profiles in the early 1980's, these reflectors have subsequently been imaged and correlated on additional reflection and refraction profiles in the offshore area of northern and western Scotland. The age and tectonic significance of these reflectors remains a subject of wide debate, due in part to the absence of robust characterization of the upper mantle velocity structure in this tectonically complex area. Interpretations advanced over the past two decades for the dipping Flannan reflector range from fossilized subduction complex to large-scale extensional shear zone, and span ages from Proterozoic to early Mesozoic. Crustal geology of the region records early Paleozoic continental collision and late Paleozoic to Mesozoic extension. Significant modification of the British lithosphere in early Tertiary time, including dramatic thinning and extensive basaltic intrusion associated with initiation and development of the Iceland plume, suggests either (1) an early Tertiary age for the Flannan reflector or (2) preservation of ancient features within the mantle lithosphere despite such pervasive modification. Exisitng constraints are consistent with a model for early Tertiary origin of the Flannan reflector as the downdip continuation of the Rockall Trough extensional system of latest Cretaceous to earliest Tertiary age during opening of the northern Atlantic Ocean and initiation of the Iceland plume. Lithopsheric thinning beneath present-day northern Scotland could have served to focus the early expression of plume volcanism (British Tertiary

  17. Mantle Mineral/Silicate Melt Partitioning

    NASA Astrophysics Data System (ADS)

    McFarlane, E. A.; Drake, M. J.

    1992-07-01

    Introduction: The partitioning of elements among mantle phases and silicate melts is of interest in unraveling the early thermal history of the Earth. It has been proposed that the elevated Mg/Si ratio of the upper mantle of the Earth is a consequence of the flotation of olivine into the upper mantle (Agee and Walker, 1988). Agee and Walker (1988) have generated a model via mass balance by assuming average mineral compositions to generate upper mantle peridotite. This model determines that upper mantle peridotite could result from the addition of 32.7% olivine and 0.9% majorite garnet into the upper mantle, and subtraction of 27.6% perovskite from the upper mantle (Agee and Walker, 1988). The present contribution uses experimental data to examine the consequences of such multiple phase fractionations enabling an independent evaluation of the above mentioned model. Here we use Mg-perovskite/melt partition coefficients from both a synthetic and a natural system (KLB-1) obtained from this laboratory. Also used are partition coefficient values for majorite garnet/melt, beta spinel/melt and olivine/melt partitioning (McFarlane et al., 1991b; McFarlane et al., 1992). Multiple phase fractionations are examined using the equilibrium crystallization equation and partition coefficient values. The mineral proportions determined by Agee and Walker (1988) are converted into weight fractions and used to compute a bulk partition coefficient value. Discussion: There has been a significant debate concerning whether measured values of trace element partition coefficients permit large-scale fractionation of liquidus phases from an early terrestrial magma ocean (Kato et al., 1988a,b; Walker and Agee, 1989; Drake, 1989; Drake et al., 1991; McFarlane et al., 1990, 1991). It should be noted that it is unclear which, if any, numerical values of partition coefficients are appropriate for examining this question, and certainly the assumptions for the current model must be more fully

  18. Variation in 142Nd/144Nd of Archean rocks from southwest Greenland : Implications for early Earth mantle dynamics

    NASA Astrophysics Data System (ADS)

    Rizo, H.; Boyet, M.; Blichert-Toft, J.; Rosing, M.; Paquette, J. L.

    2012-04-01

    The short-lived 146Sm-142Nd chronometer (half-life = 103 Ma) has proven successful in bringing constraints on the dynamics of the early Earth mantle. Since the parent isotope, 146Sm, was extant only during the first 300 Ma of the history of the Solar System, the positive 142Nd anomalies measured in southwest Greenland Archean rocks imply that their incompatible element-depleted mantle source formed during the Hadean. Interestingly, the magnitude of these anomalies seems to decrease over time. 3.7-3.8 Ga old rocks from the Amitsoq Complex have revealed +10 to +20 ppm 142Nd anomalies [1, 2, 3, 4, 5, 6, 7], whereas younger 3.0 Ga old samples from the Ivisaartoq greenstone belt yield smaller positive anomalies, ranging from +5.5 to +8.5 ppm [8]. Thus, the chemical heterogeneities detected in the southwest Greenland mantle were formed during the first 150 Ma of Earth's history, and seem to have resisted re-mixing by mantle convection until 3.0 Ga. In this study, we investigate the evolution of the southwest Greenland mantle during the time period of 3.3-3.4 Ga. The samples analyzed come from both the ~3.3 Ga amphibolite unit and the ~3.4 Ga Ameralik basic dyke swarm from the Amitsoq Complex. Coupled Sm-Nd and Lu-Hf bulk-rock ages obtained for seven amphibolites are in good agreement (3351 ± 210 Ma and 3302 ± 260 Ma, respectively) and consistent with the minimum age found by Nutman and Friend (2009) [9] for this formation. We further obtained coherent bulk-rock 147Sm-143Nd and zircon+baddeleyite 207Pb/206Pb ages for the Ameralik dykes (3428 ± 250 Ma and 3421 ± 34 Ma, respectively), in line with ages suggested by Nielsen at al., (2002) [10] and Nutman et al., (2004) [11]. We are currently in the process of analyzing these samples for 142Nd isotopic compositions and the results will be compared with the existing southwest Greenland data in order to shed new light on the evolution and destruction of heterogeneities in the early Earth mantle. [1] Rizo et al., (2011

  19. Multiple seismic reflectors in Earth’s lowermost mantle

    PubMed Central

    Shang, Xuefeng; Shim, Sang-Heon; de Hoop, Maarten; van der Hilst, Robert

    2014-01-01

    The modern view of Earth’s lowermost mantle considers a D″ region of enhanced (seismologically inferred) heterogeneity bounded by the core–mantle boundary and an interface some 150–300 km above it, with the latter often attributed to the postperovskite phase transition (in MgSiO3). Seismic exploration of Earth’s deep interior suggests, however, that this view needs modification. So-called ScS and SKKS waves, which probe the lowermost mantle from above and below, respectively, reveal multiple reflectors beneath Central America and East Asia, two areas known for subduction of oceanic plates deep into Earth’s mantle. This observation is inconsistent with expectations from a thermal response of a single isochemical postperovskite transition, but some of the newly observed structures can be explained with postperovskite transitions in differentiated slab materials. Our results imply that the lowermost mantle is more complex than hitherto thought and that interfaces and compositional heterogeneity occur beyond the D″ region sensu stricto. PMID:24550266

  20. Sub-Moho Reflectors, Mantle Faults and Lithospheric Rheology

    NASA Astrophysics Data System (ADS)

    Brown, L. D.

    2013-12-01

    One of the most unexpected and dramatic observations from the early years of deep reflection profiling of the continents using multichannel CMP techniques was the existing of prominent reflections from the upper mantle. The first of these, the Flannan thrust/fault/feature, was traced by marine profiling of the continental margin offshore Britain by the BIRPS program, which soon found them to be but one of several clear sub-crustal discontinuities in that area. Subsequently, similar mantle reflectors have been observed in many areas around the world, most commonly beneath Precambrian cratonic areas. Many, but not all, of these mantle reflections appear to arise from near the overlying Moho or within the lower crust before dipping well into the mantle. Others occur as subhorizontal events at various depths with the mantle, with one suite seeming to cluster at a depth of about 75 km. The dipping events have been variously interpreted as mantle roots of crustal normal faults or the deep extension of crustal thrust faults. The most common interpretation, however, is that these dipping events are the relicts of ancient subduction zones, the stumps of now detached Benioff zones long since reclaimed by the deeper mantle. In addition to the BIRPS reflectors, the best known examples include those beneath Fennoscandia in northern Europe, the Abitibi-Grenville of eastern Canada, and the Slave Province of northwestern Canada (e.g. on the SNORCLE profile). The most recently reported example is from beneath the Sichuan Basin of central China. The preservation of these coherent, and relatively delicate appearing, features beneath older continental crust and presumably within equally old (of not older) mantle lithosphere, has profound implications for the history and rheology of the lithosphere in these areas. If they represent, as widely believe, some form of faulting with the lithosphere, they provide corollary constraints on the nature of faulting in both the lower crust and

  1. How Irreversible Heat Transport Processes Drive Earth's Interdependent Thermal, Structural, and Chemical Evolution Providing a Strongly Heterogeneous, Layered Mantle

    NASA Astrophysics Data System (ADS)

    Hofmeister, A.; Criss, R. E.

    2013-12-01

    Because magmatism conveys radioactive isotopes plus latent heat rapidly upwards while advecting heat, this process links and controls the thermal and chemical evolution of Earth. We present evidence that the lower mantle-upper mantle boundary is a profound chemical discontinuity, leading to observed heterogeneities in the outermost layers that can be directly sampled, and construct an alternative view of Earth's internal workings. Earth's beginning involved cooling via explosive outgassing of substantial ice (mainly CO) buried with dust during accretion. High carbon content is expected from Solar abundances and ice in comets. Reaction of CO with metal provided a carbide-rich core while converting MgSiO3 to olivine via oxidizing reactions. Because thermodynamic law (and buoyancy of hot particles) indicates that primordial heat from gravitational segregation is neither large nor carried downwards, whereas differentiation forced radioactive elements upwards, formation of the core and lower mantle greatly cooled the Earth. Reference conductive geotherms, calculated using accurate and new thermal diffusivity data, require that heat-producing elements are sequestered above 670 km which limits convection to the upper mantle. These irreversible beginnings limit secular cooling to radioactive wind-down, permiting deduction of Earth's inventory of heat-producing elements from today's heat flux. Coupling our estimate for heat producing elements with meteoritic data indicates that Earth's oxide content has been underestimated. Density sorting segregated a Si-rich, peridotitic upper mantle from a refractory, oxide lower mantle with high Ca, Al and Ti contents, consistent with diamond inclusion mineralogy. Early and rapid differentiation means that internal temperatures have long been buffered by freezing of the inner core, allowing survival of crust as old as ca.4 Ga. Magmatism remains important. Melt escaping though stress-induced fractures in the rigid lithosphere imparts a

  2. What Hf isotopes in zircon tell us about crust-mantle evolution

    NASA Astrophysics Data System (ADS)

    Iizuka, Tsuyoshi; Yamaguchi, Takao; Itano, Keita; Hibiya, Yuki; Suzuki, Kazue

    2017-03-01

    The 176Lu-176Hf radioactive decay system has been widely used to study planetary crust-mantle differentiation. Of considerable utility in this regard is zircon, a resistant mineral that can be precisely dated by the U-Pb chronometer and record its initial Hf isotope composition due to having low Lu/Hf. Here we review zircon U-Pb age and Hf isotopic data mainly obtained over the last two decades and discuss their contributions to our current understanding of crust-mantle evolution, with emphasis on the Lu-Hf isotope composition of the bulk silicate Earth (BSE), early differentiation of the silicate Earth, and the evolution of the continental crust over geologic history. Meteorite zircon encapsulates the most primitive Hf isotope composition of our solar system, which was used to identify chondritic meteorites best representative of the BSE (176Hf/177Hf = 0.282793 ± 0.000011; 176Lu/177Hf = 0.0338 ± 0.0001). Hadean-Eoarchean detrital zircons yield highly unradiogenic Hf isotope compositions relative to the BSE, providing evidence for the development of a geochemically enriched silicate reservoir as early as 4.5 Ga. By combining the Hf and O isotope systematics, we propose that the early enriched silicate reservoir has resided at depth within the Earth rather than near the surface and may represent a fractionated residuum of a magma ocean underlying the proto-crust, like urKREEP beneath the anorthositic crust on the Moon. Detrital zircons from world major rivers potentially provide the most robust Hf isotope record of the preserved granitoid crust on a continental scale, whereas mafic rocks with various emplacement ages offer an opportunity to trace the Hf isotope evolution of juvenile continental crust (from εHf[4.5 Ga] = 0 to εHf[present] = + 13). The river zircon data as compared to the juvenile crust composition highlight that the supercontinent cycle has controlled the evolution of the continental crust by regulating the rates of crustal generation and intra

  3. Chondritic xenon in the Earth’s mantle

    NASA Astrophysics Data System (ADS)

    Caracausi, Antonio; Avice, Guillaume; Burnard, Peter G.; Füri, Evelyn; Marty, Bernard

    2016-05-01

    Noble gas isotopes are powerful tracers of the origins of planetary volatiles, and the accretion and evolution of the Earth. The compositions of magmatic gases provide insights into the evolution of the Earth’s mantle and atmosphere. Despite recent analytical progress in the study of planetary materials and mantle-derived gases, the possible dual origin of the planetary gases in the mantle and the atmosphere remains unconstrained. Evidence relating to the relationship between the volatiles within our planet and the potential cosmochemical end-members is scarce. Here we show, using high-precision analysis of magmatic gas from the Eifel volcanic area (in Germany), that the light xenon isotopes identify a chondritic primordial component that differs from the precursor of atmospheric xenon. This is consistent with an asteroidal origin for the volatiles in the Earth’s mantle, and indicates that the volatiles in the atmosphere and mantle originated from distinct cosmochemical sources. Furthermore, our data are consistent with the origin of Eifel magmatism being a deep mantle plume. The corresponding mantle source has been isolated from the convective mantle since about 4.45 billion years ago, in agreement with models that predict the early isolation of mantle domains. Xenon isotope systematics support a clear distinction between mid-ocean-ridge and continental or oceanic plume sources, with chemical heterogeneities dating back to the Earth’s accretion. The deep reservoir now sampled by the Eifel gas had a lower volatile/refractory (iodine/plutonium) composition than the shallower mantle sampled by mid-ocean-ridge volcanism, highlighting the increasing contribution of volatile-rich material during the first tens of millions of years of terrestrial accretion.

  4. The origin of volatiles in the Earth's mantle

    NASA Astrophysics Data System (ADS)

    Hier-Majumder, Saswata; Hirschmann, Marc M.

    2017-08-01

    The Earth's deep interior contains significant reservoirs of volatiles such as H, C, and N. Due to the incompatible nature of these volatile species, it has been difficult to reconcile their storage in the residual mantle immediately following crystallization of the terrestrial magma ocean (MO). As the magma ocean freezes, it is commonly assumed that very small amounts of melt are retained in the residual mantle, limiting the trapped volatile concentration in the primordial mantle. In this article, we show that inefficient melt drainage out of the freezing front can retain large amounts of volatiles hosted in the trapped melt in the residual mantle while creating a thick early atmosphere. Using a two-phase flow model, we demonstrate that compaction within the moving freezing front is inefficient over time scales characteristic of magma ocean solidification. We employ a scaling relation between the trapped melt fraction, the rate of compaction, and the rate of freezing in our magma ocean evolution model. For cosmochemically plausible fractions of volatiles delivered during the later stages of accretion, our calculations suggest that up to 77% of total H2O and 12% of CO2 could have been trapped in the mantle during magma ocean crystallization. The assumption of a constant trapped melt fraction underestimates the mass of volatiles in the residual mantle by more than an order of magnitude.Plain Language SummaryThe Earth's deep interior contains substantial amounts of volatile elements like C, H, and N. How these elements got sequestered in the Earth's interior has long been a topic of debate. It is generally assumed that most of these elements escaped the interior of the Earth during the first few hundred thousand years to create a primitive atmosphere, leaving the <span class="hlt">mantle</span> reservoir nearly empty. In this work, we show that the key to this paradox involves the very <span class="hlt">early</span> stages of crystallization of the <span class="hlt">mantle</span> from a global</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008Litho.102...12O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008Litho.102...12O"><span>Dynamics of cratons in an evolving <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>O'Neill, C. J.; Lenardic, A.; Griffin, W. L.; O'Reilly, Suzanne Y.</p> <p>2008-04-01</p> <p>The tectonic quiescence of cratons on a tectonically active planet has been attributed to their physical properties such as buoyancy, viscosity, and yield strength. Previous modelling has shown the conditions under which cratons may be stable for the present, but cast doubt on how they survived in a more energetic <span class="hlt">mantle</span> of the past. Here we incorporate an endothermic phase change at 670 km, and a depth-dependent viscosity structure consistent with post-glacial rebound and geoid modelling, to simulate the dynamics of cratons in an "Earth-like" convecting system. We find that cratons are unconditionally stable in such systems for plausible ranges of viscosity ratios between the root and asthenosphere (50-150) and the root/oceanic lithosphere yield strength ratio (5-30). Realistic <span class="hlt">mantle</span> viscosity structures have limited effect on the average background cratonic stress state, but do buffer cratons from extreme stress excursions. An endothermic phase change at 670 km introduces an additional time-dependence into the system, with slab breakthrough into the lower <span class="hlt">mantle</span> associated with 2-3 fold stress increases at the surface. Under Precambrian <span class="hlt">mantle</span> conditions, however, the dominant effect is not more violent <span class="hlt">mantle</span> avalanches, or faster <span class="hlt">mantle</span>/plate velocities, but rather the drastic viscosity drop which results from hotter <span class="hlt">mantle</span> conditions in the past. This results in a large decrease in the cratonic stress field, and promotes craton survival under the evolving <span class="hlt">mantle</span> conditions of the <span class="hlt">early</span> Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.458..252F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.458..252F"><span>Sensitivities of Earth's core and <span class="hlt">mantle</span> compositions to accretion and <span class="hlt">differentiation</span> processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fischer, Rebecca A.; Campbell, Andrew J.; Ciesla, Fred J.</p> <p>2017-01-01</p> <p>The Earth and other terrestrial planets formed through the accretion of smaller bodies, with their core and <span class="hlt">mantle</span> compositions primarily set by metal-silicate interactions during accretion. The conditions of these interactions are poorly understood, but could provide insight into the mechanisms of planetary core formation and the composition of Earth's core. Here we present modeling of Earth's core formation, combining results of 100 N-body accretion simulations with high pressure-temperature metal-silicate partitioning experiments. We explored how various aspects of accretion and core formation influence the resulting core and <span class="hlt">mantle</span> chemistry: depth of equilibration, amounts of metal and silicate that equilibrate, initial distribution of oxidation states in the disk, temperature distribution in the planet, and target:impactor ratio of equilibrating silicate. Virtually all sets of model parameters that are able to reproduce the Earth's <span class="hlt">mantle</span> composition result in at least several weight percent of both silicon and oxygen in the core, with more silicon than oxygen. This implies that the core's light element budget may be dominated by these elements, and is consistent with ≤1-2 wt% of other light elements. Reproducing geochemical and geophysical constraints requires that Earth formed from reduced materials that equilibrated at temperatures near or slightly above the <span class="hlt">mantle</span> liquidus during accretion. The results indicate a strong tradeoff between the compositional effects of the depth of equilibration and the amounts of metal and silicate that equilibrate, so these aspects should be targeted in future studies aiming to better understand core formation conditions. Over the range of allowed parameter space, core and <span class="hlt">mantle</span> compositions are most sensitive to these factors as well as stochastic variations in what the planet accreted as a function of time, so tighter constraints on these parameters will lead to an improved understanding of Earth's core composition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PEPI..277...10L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PEPI..277...10L"><span>Linking lowermost <span class="hlt">mantle</span> structure, core-<span class="hlt">mantle</span> boundary heat flux and <span class="hlt">mantle</span> plume formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Mingming; Zhong, Shijie; Olson, Peter</p> <p>2018-04-01</p> <p>The dynamics of Earth's lowermost <span class="hlt">mantle</span> exert significant control on the formation of <span class="hlt">mantle</span> plumes and the core-<span class="hlt">mantle</span> boundary (CMB) heat flux. However, it is not clear if and how the variation of CMB heat flux and <span class="hlt">mantle</span> plume activity are related. Here, we perform geodynamic model experiments that show how temporal variations in CMB heat flux and pulses of <span class="hlt">mantle</span> plumes are related to morphologic changes of the thermochemical piles of large-scale compositional heterogeneities in Earth's lowermost <span class="hlt">mantle</span>, represented by the large low shear velocity provinces (LLSVPs). We find good correlation between the morphologic changes of the thermochemical piles and the time variation of CMB heat flux. The morphology of the thermochemical piles is significantly altered during the initiation and ascent of strong <span class="hlt">mantle</span> plumes, and the changes in pile morphology cause variations in the local and the total CMB heat flux. Our modeling results indicate that plume-induced episodic variations of CMB heat flux link geomagnetic superchrons to pulses of surface volcanism, although the relative timing of these two phenomena remains problematic. We also find that the density distribution in thermochemical piles is heterogeneous, and that the piles are denser on average than the surrounding <span class="hlt">mantle</span> when both thermal and chemical effects are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFMMR11A..01A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFMMR11A..01A"><span>Birch's <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anderson, D. L.</p> <p>2002-12-01</p> <p>Francis Birch's 1952 paper started the sciences of mineral physics and physics of the Earth's interior. Birch stressed the importance of pressure, compressive strain and volume in <span class="hlt">mantle</span> physics. Although this may seem to be an obvious lesson many modern paradoxes in the internal constitution of the Earth and <span class="hlt">mantle</span> dynamics can be traced to a lack of appreciation for the role of compression. The effect of pressure on thermal properties such as expansivity can gravitational stratify the Earth irreversibly during accretion and can keep it chemically stratified. The widespread use of the Boussinesq approximation in <span class="hlt">mantle</span> geodynamics is the antithesis of Birchian physics. Birch pointed out that eclogite was likely to be an important component of the upper <span class="hlt">mantle</span>. Plate tectonic recycling and the bouyancy of oceanic crust at midmantle depths gives credence to this suggestion. Although peridotite dominates the upper <span class="hlt">mantle</span>, variations in eclogite-content may be responsible for melting- or fertility-spots. Birch called attention to the Repetti Discontinuity near 900 km depth as an important geodynamic boundary. This may be the chemical interface between the upper and lower <span class="hlt">mantles</span>. Recent work in geodynamics and seismology has confirmed the importance of this region of the <span class="hlt">mantle</span> as a possible barrier. Birch regarded the transition region (TR ; 400 to 1000 km ) as the key to many problems in Earth sciences. The TR contains two major discontinuities ( near 410 and 650 km ) and their depths are a good <span class="hlt">mantle</span> thermometer which is now being exploited to suggest that much of plate tectonics is confined to the upper <span class="hlt">mantle</span> ( in Birch's terminology, the <span class="hlt">mantle</span> above 1000 km depth ). The lower <span class="hlt">mantle</span> is homogeneous and different from the upper <span class="hlt">mantle</span>. Density and seismic velocity are very insensitive to temperature there, consistent with tomography. A final key to the operation of the <span class="hlt">mantle</span> is Birch's suggestion that radioactivities were stripped out of the deeper parts of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI13B..05C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI13B..05C"><span>Controls on the time-scales of <span class="hlt">mantle</span> mixing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Crameri, F.; Cagney, N.; Lithgow-Bertelloni, C. R.; Whitehead, J. A.</p> <p>2016-12-01</p> <p>Understanding the processes controlling the <span class="hlt">mantle</span> mixing is crucial to our geochemical interpretation of basalts, and our understanding of the <span class="hlt">mantle</span> heterogeneity. We investigate the influence of various <span class="hlt">mantle</span> conditions on the time scales of mixing using numerical simulations. We examine the effects of Rayleigh number (Ra), depth- and temperature-dependent rheology and internal heating, as well as the role of Prandtl number (Pr), in order to assess how mixing in the <span class="hlt">early</span> magma ocean and experiments (where Pr tends to be 103) differs from that in the present-day <span class="hlt">mantle</span> (Pr 1025). We use the "coarse grained density" method to quantify the mixing state and determine the mixing time. The mixing time is found to be strongly affected by the Rayleigh number, scaling with Ra-0.65, in agreement with previous studies. In contrast, when Ra is held constant, the temperature-dependent rheology has a weak effect. The depth-dependent rheology also has a negligible effect on the mixing time, as material that is initially viscous is transported to the low viscosity near the surface where it undergoes fast mixing. The internal heating rate does not affect the mixing time, provided that it does not increase the fluid temperature above that of the boundary condition. In this case, the decrease in mixing time is shown to be a result of an increase in the effective Ra. Finally, we show that for moderate and low Pr, the mixing time increases with Pr0.45. However, for all Pr greater than about 100, the mixing time is the same at the infinite-Pr value. Our results have several implications for the <span class="hlt">mantle</span>: (1) Ra is the controlling factor on <span class="hlt">mantle</span> mixing. (2) The non-Newtonian rheology of the <span class="hlt">mantle</span> has a very weak effect on <span class="hlt">mantle</span> mixing and can be neglected. (3) A dramatic increase in viscosity in the deep <span class="hlt">mantle</span> has been proposed at a cause of regions of unmixed `primitive' <span class="hlt">mantle</span>. Our results show that this hypothesis is unlikely, as depth dependent rheology does not increase in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920001511&hterms=constitution&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dconstitution','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920001511&hterms=constitution&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dconstitution"><span>Processes of deep terrestrial <span class="hlt">mantles</span> and cores</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jeanloz, Raymond</p> <p>1991-01-01</p> <p>Ultrahigh pressure experiments are currently focused on revealing processes occurring deep inside planets. This is in addition to the traditional emphasis on the constitution of planetary interiors, such as the identification of the high pressure perovskite phase of (Mg,Fe)SiO3 as the predominant mineral inside the Earth, and probably Venus. For example, experiments show that the mechanism of geochemical <span class="hlt">differentiation</span>, separation of partial melts, differs fundamentally in the lower <span class="hlt">mantles</span> of Earth and Venus than at near surface conditions. In addition to structural transformations, changes in chemical bonding caused by pressure can also be significant for planetary interiors. Measurements of AC and DC electrical conductivity can be obtained at ultrahigh pressures and temperatures, to greater than 80 GPa and 3000 K simultaneously, using the laser heated diamond cell. Anhydrous lower <span class="hlt">mantle</span> assemblages (perovskite + or - oxide phases) exhibit an electrical conductivity that depends strongly on Fe content. Contrary to traditional assumptions, temperature affects the conductivity of lower <span class="hlt">mantle</span> assemblages relatively little. The Earth's deep focus seismicity can be explained by the recycling of water into the <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMDI43B..05R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMDI43B..05R"><span>Memories of Earth Formation in the Modern <span class="hlt">Mantle</span>: W Isotopic Composition of Flood Basalt Lavas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rizo Garza, H. L.; Walker, R. J.; Carlson, R.; Horan, M. F.; Mukhopadhyay, S.; Francis, D.; Jackson, M. G.</p> <p>2015-12-01</p> <p>Four and a half billion years of geologic activity has overprinted much of the direct evidence for processes involved in Earth's formation and its initial chemical <span class="hlt">differentiation</span>. Xenon isotopic ratios [1] and 3He/22Ne ratios [2] suggest that heterogeneities formed during Earth's accretion have been preserved to the present time. New opportunities to learn about <span class="hlt">early</span> Earth history have opened up with the development of analytical techniques that allow high precision analysis of short-lived isotopic systems. The Hf-W system (t½ = 8.9 Ma) is particularly valuable for studying events that occurred during the first ~50 Ma of Solar System history. Here we report new data for ~ 60 Ma Baffin Bay and ~ 120 Ma Ontong Java Plateau lava samples. Both are large igneous provinces that may have sampled a primitive, less degassed deep <span class="hlt">mantle</span> reservoir that has remained isolated since shortly after Earth formation [3,4]. Three samples analyzed have 182W/184W ratios that are 10 to 48 ppm higher than our terrestrial standard. These excesses in 182W are the highest ever measured in terrestrial rocks, and may reflect 182W ingrowth in an <span class="hlt">early</span>-formed high Hf/W <span class="hlt">mantle</span> domain that was produced by magma ocean <span class="hlt">differentiation</span> [5]. Long and short-lived Sm-Nd systematics in these samples, however, are inconsistent with this hypothesis. The 182W excessses could rather reflect the derivation of these lavas from a <span class="hlt">mantle</span> reservoir that was isolated from late accretionary additions [6]. The chondritic initial Os isotopic compositions and highly siderophile element abundances of these samples, however, are inconsistent with this interpretation. Tungsten concentrations for the Baffin Bay and Ontong Java Plateau samples range from 23 ppb to 62 ppb, and are negatively correlated with their 182W/184W ratios. We propose that the source reservoirs for these flood basalts likely formed through Hf/W fractionation caused by core-forming events occuring over a protacted time interval during Earth</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMDI43C..08M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMDI43C..08M"><span>Visualizing Earth's Core-<span class="hlt">Mantle</span> Interactions using Nanoscale X-ray Tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mao, W. L.; Wang, J.; Yang, W.; Hayter, J.; Pianetta, P.; Zhang, L.; Fei, Y.; Mao, H.; Hustoft, J. W.; Kohlstedt, D. L.</p> <p>2010-12-01</p> <p><span class="hlt">Early</span>-stage, core-<span class="hlt">mantle</span> <span class="hlt">differentiation</span> and core formation represent a pivotal geological event which defined the major geochemical signatures. However current hypotheses of the potential mechanism for core-<span class="hlt">mantle</span> separation and interaction need more experimental input which has been awaiting technological breakthroughs. Nanoscale x-ray computed tomography (nanoXCT) within a laser-heated diamond anvil cell has exciting potential as a powerful 3D petrographic probe for non-destructive, nanoscale (<40nm) resolution of multiple minerals and amorphous phases (including melts) which are synthesized under the high pressure-temperature conditions found deep within the Earth and planetary interiors. Results from high pressure-temperature experiments which illustrate the potential for this technique will be presented. By extending measurements of the texture, shape, porosity, tortuosity, dihedral angle, and other characteristics of molten Fe-rich alloys in relation to silicates and oxides, along with the fracture systems of rocks under deformation by high pressure-temperature conditions, potential mechanisms of core formation can be tested. NanoXCT can also be used to investigate grain shape, intergrowth, orientation, and foliation -- as well as mineral chemistry and crystallography at core-<span class="hlt">mantle</span> boundary conditions -- to understand whether shape-preferred orientation is a primary source of the observed seismic anisotropy in Earth’s D” layer and to determine the textures and shapes of the melt pockets and channels which would form putative partial melt which may exist in ultralow velocity zones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26PSL.451..149S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26PSL.451..149S"><span>Lunar basalt chronology, <span class="hlt">mantle</span> <span class="hlt">differentiation</span> and implications for determining the age of the Moon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Snape, Joshua F.; Nemchin, Alexander A.; Bellucci, Jeremy J.; Whitehouse, Martin J.; Tartèse, Romain; Barnes, Jessica J.; Anand, Mahesh; Crawford, Ian A.; Joy, Katherine H.</p> <p>2016-10-01</p> <p>Despite more than 40 years of studying Apollo samples, the age and <span class="hlt">early</span> evolution of the Moon remain contentious. Following the formation of the Moon in the aftermath of a giant impact, the resulting Lunar Magma Ocean (LMO) is predicted to have generated major geochemically distinct silicate reservoirs, including the sources of lunar basalts. Samples of these basalts, therefore, provide a unique opportunity to characterize these reservoirs. However, the precise timing and extent of geochemical fractionation is poorly constrained, not least due to the difficulty in determining accurate ages and initial Pb isotopic compositions of lunar basalts. Application of an in situ ion microprobe approach to Pb isotope analysis has allowed us to obtain precise crystallization ages from six lunar basalts, typically with an uncertainty of about ± 10 Ma, as well as constrain their initial Pb-isotopic compositions. This has enabled construction of a two-stage model for the Pb-isotopic evolution of lunar silicate reservoirs, which necessitates the prolonged existence of high-μ reservoirs in order to explain the very radiogenic compositions of the samples. Further, once firm constraints on U and Pb partitioning behaviour are established, this model has the potential to help distinguish between conflicting estimates for the age of the Moon. Nonetheless, we are able to constrain the timing of a lunar <span class="hlt">mantle</span> reservoir <span class="hlt">differentiation</span> event at 4376 ± 18 Ma, which is consistent with that derived from the Sm-Nd and Lu-Hf isotopic systems, and is interpreted as an average estimate of the time at which the high-μ urKREEP reservoir was established and the Ferroan Anorthosite (FAN) suite was formed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NatGe..11..139A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NatGe..11..139A"><span>Deep and persistent melt layer in the Archaean <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrault, Denis; Pesce, Giacomo; Manthilake, Geeth; Monteux, Julien; Bolfan-Casanova, Nathalie; Chantel, Julien; Novella, Davide; Guignot, Nicolas; King, Andrew; Itié, Jean-Paul; Hennet, Louis</p> <p>2018-02-01</p> <p>The transition from the Archaean to the Proterozoic eon ended a period of great instability at the Earth's surface. The origin of this transition could be a change in the dynamic regime of the Earth's interior. Here we use laboratory experiments to investigate the solidus of samples representative of the Archaean upper <span class="hlt">mantle</span>. Our two complementary in situ measurements of the melting curve reveal a solidus that is 200-250 K lower than previously reported at depths higher than about 100 km. Such a lower solidus temperature makes partial melting today easier than previously thought, particularly in the presence of volatiles (H2O and CO2). A lower solidus could also account for the <span class="hlt">early</span> high production of melts such as komatiites. For an Archaean <span class="hlt">mantle</span> that was 200-300 K hotter than today, significant melting is expected at depths from 100-150 km to more than 400 km. Thus, a persistent layer of melt may have existed in the Archaean upper <span class="hlt">mantle</span>. This shell of molten material may have progressively disappeared because of secular cooling of the <span class="hlt">mantle</span>. Crystallization would have increased the upper <span class="hlt">mantle</span> viscosity and could have enhanced mechanical coupling between the lithosphere and the asthenosphere. Such a change might explain the transition from surface dynamics dominated by a stagnant lid on the <span class="hlt">early</span> Earth to modern-like plate tectonics with deep slab subduction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040090318&hterms=evolution+rock&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Devolution%2Brock','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040090318&hterms=evolution+rock&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Devolution%2Brock"><span><span class="hlt">Mantle</span> redox evolution and the oxidation state of the Archean atmosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kasting, J. F.; Eggler, D. H.; Raeburn, S. P.</p> <p>1993-01-01</p> <p>Current models predict that the <span class="hlt">early</span> atmosphere consisted mostly of CO2, N2, and H2O, along with traces of H2 and CO. Such models are based on the assumption that the redox state of the upper <span class="hlt">mantle</span> has not changed, so that volcanic gas composition has remained approximately constant with time. We argue here that this assumption is probably incorrect: the upper <span class="hlt">mantle</span> was originally more reduced than today, although not as reduced as the metal arrest level, and has become progressively more oxidized as a consequence of the release of reduced volcanic gases and the subduction of hydrated, oxidized seafloor. Data on the redox state of sulfide and chromite inclusions in diamonds imply that the process of <span class="hlt">mantle</span> oxidation was slow, so that reduced conditions could have prevailed for as much as half of the earth's history. To be sure, other oxybarometers of ancient rocks give different results, so the question of when the <span class="hlt">mantle</span> redox state has changed remains unresolved. <span class="hlt">Mantle</span> redox evolution is intimately linked to the oxidation state of the primitive atmosphere: A reduced Archean atmosphere would have had a high hydrogen escape rate and should correspond to a changing <span class="hlt">mantle</span> redox state; an oxidized Archean atmosphere should be associated with a constant <span class="hlt">mantle</span> redox state. The converses of these statements are also true. Finally, our theory of <span class="hlt">mantle</span> redox evolution may explain why the Archean atmosphere remained oxygen-deficient until approximately 2.0 billion years ago (Ga) despite a probable <span class="hlt">early</span> origin for photosynthesis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P54A..04B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P54A..04B"><span>On the Role of <span class="hlt">Mantle</span> Overturn during Magma Ocean Solidification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boukaré, C. E.; Parmentier, E.; Parman, S. W.</p> <p>2017-12-01</p> <p>Solidification of potential global magma ocean(s) (MO) <span class="hlt">early</span> in the history of terrestrial planets may play a key role in the evolution of planetary interiors by setting initial conditions for their long-term evolution. Constraining this initial structure of solid <span class="hlt">mantles</span> is thus crucial but remains poorly understood. MO fractional crystallization has been proposed to generate gravitationally unstable Fe-Mg chemical stratification capable of driving solid-state <span class="hlt">mantle</span> overturn. Fractional solidification and overturn hypothesis, while only an ideal limiting case, can explain important geochemical features of both the Moon and Mars. Current overturn models consider generally post-MO overturn where the cumulate pile remains immobile until the end of MO solidification. However, if the cumulate pile overturns during MO solidification, the general picture of <span class="hlt">early</span> planet evolution might differ significantly from the static crystallization models. We show that the timing of <span class="hlt">mantle</span> overturn can be characterized with a dimensionless number measuring the ratio of the MO solidification time and the purely compositional overturn timescale. Syn-solidification overturn occurs if this dimensionless parameter, Rc, exceeds a critical value. Rc is mostly affected by the competition between the MO solidification time and <span class="hlt">mantle</span> viscosity. Overturn that occurs during solidification can result in smaller scales of <span class="hlt">mantle</span> chemical heterogeneity that could persist for long times thus influencing the whole evolution of a planetary body. We will discuss the effects of compaction/percolation on <span class="hlt">mantle</span> viscosity. If partially molten cumulate do not have time to compact during MO solidification, viscosity of cumulates would be significantly lower as the interstitcial melt fraction would be large. Both solid <span class="hlt">mantle</span> remelting during syn-solidification overturn and porous convection of melt retained with the cumulates are expected to reduce the degree of fractional crystallization. Syn</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998Tectp.296...15D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998Tectp.296...15D"><span>Stability and growth of continental shields in <span class="hlt">mantle</span> convection models including recurrent melt production</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Smet, J. H.; van den Berg, A. P.; Vlaar, N. J.</p> <p>1998-10-01</p> <p>The long-term growth and stability of compositionally layered continental upper <span class="hlt">mantle</span> has been investigated by numerical modelling. We present the first numerical model of a convecting <span class="hlt">mantle</span> including <span class="hlt">differentiation</span> through partial melting resulting in a stable compositionally layered continental upper <span class="hlt">mantle</span> structure. This structure includes a continental root extending to a depth of about 200 km. The model covers the upper <span class="hlt">mantle</span> including the crust and incorporates physical features important for the study of the continental upper <span class="hlt">mantle</span> during secular cooling of the Earth since the Archaean. Among these features are: a partial melt generation mechanism allowing consistent recurrent melting, time-dependent non-uniform radiogenic heat production, and a temperature- and pressure-dependent rheology. The numerical results reveal a long-term growth mechanism of the continental compositional root. This mechanism operates through episodical injection of small diapiric upwellings from the deep layer of undepleted <span class="hlt">mantle</span> into the continental root which consists of compositionally distinct depleted <span class="hlt">mantle</span> material. Our modelling results show the layered continental structure to remain stable during at least 1.5 Ga. After this period <span class="hlt">mantle</span> <span class="hlt">differentiation</span> through partial melting ceases due to the prolonged secular cooling and small-scale instabilities set in through continental delamination. This stable period of 1.5 Ga is related to a number of limitations in our model. By improving on these limitations in the future this stable period will be extended to more realistic values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11541323','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11541323"><span>Isotopic constraints on the age and <span class="hlt">early</span> <span class="hlt">differentiation</span> of the Earth.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McCulloch, M T</p> <p>1996-03-01</p> <p>The Earth's age and <span class="hlt">early</span> <span class="hlt">differentiation</span> history are re-evaluated using updated isotopic constraints. From the most primitive terrestrial Pb isotopic compositions found at Isua Greenland, and the Pilbara of Western Australia, combined with precise geochronology of these localities, an age 4.49 +/- 0.02 Ga is obtained. This is interpreted as the mean age of core formation as U/Pb is fractionated due to sequestering of Pb into the Earth's core. The long-lived Rb-Sr isotopic system provides constraints on the time interval for the accretion of the Earth as Rb underwent significant depletion by volatile loss during accretion of the Earth or its precursor planetesimals. A primitive measured 87Sr/86Sr initial ratio of 0.700502 +/- 10 has been obtained for an <span class="hlt">early</span> Archean (3.46 Ga) barite from the Pilbara Block of Western Australia. Using conservative models for the evolution of Rb/Sr in the <span class="hlt">early</span> Archean <span class="hlt">mantle</span> allows an estimate to be placed on the Earth's initial Sr ratio at approximately 4.50 Ga, of 0.69940 +/- 10. This is significantly higher than that measured for the Moon (0.69900 +/- 2) or in the achondrite, Angra dos Reis (0.69894 +/- 2) and for a Rb/Sr ratio of approximately 1/2 of chondrites corresponds to a mean age for accretion of the Earth of 4.48 + /- 0.04 Ga. The now extinct 146Sm-142Nd (T1/2(146)=103 l0(6)yrs) combined with the long-lived 147Sm-143Nd isotopic systematics can also be used to provide limits on the time of <span class="hlt">early</span> <span class="hlt">differentiation</span> of the Earth. High precision analyses of the oldest (3.8-3.9 Ga) Archean gneisses from Greenland (Amitsoq and Akilia gneisses), and Canada (Acasta gneiss) do not show measurable (> +/- l0ppm) variations of 142Nd, in contrast to the 33 ppm 142Nd excess reported for an Archean sample. The general lack of 142Nd variations, combined with the presence of highly positive epsilon 143 values (+4.0) at 3.9 Ga, indicates that the record of large-scale Sm/Nd fractionation events was not preserved in the <span class="hlt">early</span>-Earth from 4</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28188115','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28188115"><span><span class="hlt">Differential</span> <span class="hlt">mantle</span> transcriptomics and characterization of growth-related genes in the diploid and triploid pearl oyster Pinctada fucata.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guan, Yunyan; He, Maoxian; Wu, Houbo</p> <p>2017-06-01</p> <p>To explore the molecular mechanism of triploidy effect in the pearl oyster Pinctada fucata, two RNA-seq libraries were constructed from the <span class="hlt">mantle</span> tissue of diploids and triploids by Roche-454 massive parallel pyrosequencing. The identification of <span class="hlt">differential</span> expressed genes (DEGs) between diploid and triploid may reveal the molecular mechanism of triploidy effect. In this study, 230 down-regulated and 259 up-regulated DEGs were obtained by comparison between diploid and triploid libraries. The gene ontology and KEGG pathway analysis revealed more functional activation in triploids and it may due to the duplicated gene expression in transcriptional level during whole genome duplication (WGD). To confirm the sequencing data, a set of 11 up-regulated genes related to growth and development control and regulation were analyzed by RT-qPCR in independent experiment. According to the validation and annotation of these genes, it is hypothesized that the set of up-regulated expressed genes had the correlated expression pattern involved in shell building or other interactive probable functions during triploidization. The up- regulation of growth-related genes may support the classic hypotheses of 'energy redistribution' from <span class="hlt">early</span> research. The results provide valuable resources to understand the molecular mechanism of triploidy effect in both shell building and producing high-quality seawater pearls. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.V43D..06Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.V43D..06Z"><span><span class="hlt">Mantle</span> Degassing and Atmosphere Evolution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Y.</p> <p>2011-12-01</p> <p>Noble gas isotopes have provided much of our understanding of Earth's <span class="hlt">early</span> history [1-3]. Various degassing models have been developed, including degassing of the whole <span class="hlt">mantle</span>, degassing of all gases at similar relative rate [1], solubility-controlled degassing [2], and steady-state degassing models [4]. This report will evaluate various degassing models using recent data. For example, helium outgassing flux has been lowered by more than a factor of two based on sophisticated ocean general circulation models [5], which also impacts on the estimated degassing flux of carbon. Years of measurements and progress have allowed isotopic ratios of various <span class="hlt">mantle</span> reservoirs being pieced together [6]. For example, 129Xe/130Xe in OIB <span class="hlt">mantle</span> is found to be lower than that in MORB <span class="hlt">mantle</span> [7]. Missing Xe has been found to be a non-issue [8]. Nucleogenic 21Ne production rate relative radiogenic 4He has been revised [9-10], which leads to an interesting neon paradox that nucleogenic 21Ne production in the whole silicate Earth is barely enough to supply nucleogenic 21Ne in air. 40Ar/36Ar ratio in BSE seems to be much lower than any OIB samples, another interesting paradox. Although non-nucleogenic <span class="hlt">mantle</span> neon is solar, nonradiogenic <span class="hlt">mantle</span> argon is atmospheric [11]. For Kr and Xe, the jury is still out. When <span class="hlt">mantle</span> degassing models are evaluated using volatile data of the MORB and OIB, solubility-controlled degassing is able to reconcile more data than other degassing models. On the other hand, the vailable data seem to indicate that atmosphere evolution is more than <span class="hlt">mantle</span> degassing; there may be significant contribution to the atmosphere from impact degassing and other sources. Furthermore, we are now suffering from too many data so that understanding the whole picture is elusive. [1] Allegre et al. (1986/87) EPSL 81, 127-150. [2] Zhang & Zindler (1989) J. Geophys. Res. 94, 13719-13737. [3] Zhang (1998) Geochim. Cosmochim. Acta 62, 3185-3189. [4] Pocelli & Wasserburg (1995</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.U13B..16H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.U13B..16H"><span>Ultra-high precision 142Nd/144Nd measurements of the Proterozoic and implications for mixing in the Earth's <span class="hlt">mantle</span> through time</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hyung, E.; Jacobsen, S. B.</p> <p>2017-12-01</p> <p>The decay of 146Sm to 142Nd is an excellent a tracer for <span class="hlt">early</span> silicate <span class="hlt">differentiation</span> events in the terrestrial planets, as the Sm/Nd ratio is usually fractionated during <span class="hlt">mantle</span> partial melting and magma ocean crystallization. The short half-life (103 or 68 Ma) renders the system extinct within the first 500 Ma of Solar System formation. Samples with 142Nd/144Nd ratios that are substantially different from the bulk silicate Earth value of 142Nd/144Nd provide clear evidence for <span class="hlt">mantle</span> <span class="hlt">differentiation</span> in the Hadean. Published data for the 3.4 to 3.8 Ga old Isua supracrustal rocks and dykes have demonstrated both positive and negative 142Nd/144Nd anomalies (30 ppm range) providing clear evidence for Hadean enriched and depleted <span class="hlt">mantle</span> reservoirs. In contrast, no 142Nd/144Nd anomalies have been found in modern day terrestrial samples with data that have 2σ uncertainties of about 5 ppm or more. Last year we reported improvements in 142Nd/144Nd measurements, using our IsotopX thermal ionization mass spectrometer, and obtained reproducibility of 142Nd/144Nd ratios to better than 2 ppm at the 2σ level. With this external reproducibility we found that all except one modern <span class="hlt">mantle</span>-derived basalt had within error identical 142Nd/144Nd ratios. One sample is about 3.4 ppm lower than the rest of the modern basalt samples, providing evidence for some limited Hadean <span class="hlt">mantle</span> <span class="hlt">differentiation</span> signatures preserved up to present. We have also measured 142Nd/144Nd ratios for Proterozoic and Phanerozoic samples, whose ages range from 300 Ma to 2 Ga, to better than 2 ppm external reproducibility (2σ). Most of these samples also have 142Nd/144Nd ratios that cluster around the modern day value, but there are some samples that are either marginally high by 2 ppm or low by 2 ppm. Thus, while a 20 to 30 ppm range in 142Nd/144Nd is well resolved in the Archean, such large variability is not present in the Proterozoic and Phanerozoic. The relatively rapid changeover at the end of the Archean</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoOD..58..173K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoOD..58..173K"><span>Zirconium and hafnium fractionation in <span class="hlt">differentiation</span> of alkali carbonatite magmatic systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kogarko, L. N.</p> <p>2016-05-01</p> <p>Zirconium and hafnium are valuable strategic metals which are in high demand in industry. The Zr and Hf contents are elevated in the final products of magmatic <span class="hlt">differentiation</span> of alkali carbonatite rocks in the Polar Siberia region (Guli Complex) and Ukraine (Chernigov Massif). <span class="hlt">Early</span> pyroxene fractionation led to an increase in the Zr/Hf ratio in the evolution of the ultramafic-alkali magmatic system due to a higher distribution coefficient of Hf in pyroxene with respect to Zr. The Rayleigh equation was used to calculate a quantitative model of variation in the Zr/Hf ratio in the development of the Guli magmatic system. Alkali carbonatite rocks originated from rare element-rich <span class="hlt">mantle</span> reservoirs, in particular, the metasomatized <span class="hlt">mantle</span>. Carbonated <span class="hlt">mantle</span> xenoliths are characterized by a high Zr/Hf ratio due to clinopyroxene development during metasomatic replacement of orthopyroxene by carbonate fluid melt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.T11B2625C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.T11B2625C"><span>Structure of the Upper <span class="hlt">Mantle</span> and <span class="hlt">Mantle</span> Transition Zone in Central Mongolia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cui, Z.; Meltzer, A.; Stachnik, J.; Fischer, K. M.; Russo, R. M.; Munkhuu, U.; Baasanbat, T.</p> <p>2016-12-01</p> <p>Located between two major Archean cratons, the Siberian Craton to the north and the Tarim and Sino-Korean Cratons to the south, the lithosphere of Central Mongolia was constructed over an extended period of orogenesis associated with the Central Asian Orogenic Belt. Archean to <span class="hlt">Early</span> Proterozoic basement was modified by accreted subduction complexes during the Paleozoic and <span class="hlt">early</span> Mesozoic and basalt magmatism in the Cenozoic. Central and western Mongolia constitute a significant portion of the greater Mongolian plateau, an approximately 2.6 million km2area of Central Asia with an average elevation of 1500 meters. The high topography of the Mongolian Plateau has been attributed to far-field effects of India-Asia convergence, Pacific plate subduction, <span class="hlt">mantle</span> plume activity, convective <span class="hlt">mantle</span> flow, and magmatic underplating. The origin and persistence of continental plateaus through time provides insight into the evolution of continents and interactions between <span class="hlt">mantle</span> dynamics and surface processes. As part of a larger interdisciplinary project to understand the origin of high topography in continental interiors we deployed 112 seismic broadband stations in central Mongolia as three separate subarrays in two separate mobilizations over a four year period (2012-2016). The stations extend from the Hovsgol rift in northern Mongolia, through the Hangay Dome, and into the Gobi Altai in southern Mongolia. We use S wave Receiver functions (SRF) to examine the lithosphere asthenosphere boundary and P wave Receiver functions (PRF) to investigate the <span class="hlt">mantle</span> transition zone (MTZ). Preliminary SRF results from the subarray in the Hangay show lithospheric thinning and E-W variation. The LAB beneath the Hangay is 100km. It gradually thins to 90 km at the western end of the central Hangay and thins more abruptly to 80km at the eastern end of the central Hangay. These results are in agreement with results from joint inversion of receiver functions and surface waves and teleseismic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850024750&hterms=recycling&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Drecycling','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850024750&hterms=recycling&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Drecycling"><span>The relation between the age of the subconducting slab and the recycling of sediments into the <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Abbott, D.; Hoffman, S.</p> <p>1985-01-01</p> <p>The recycling of sediments into the <span class="hlt">mantle</span> has become an important issue because recent papers have suggested that the geochemical inverse models of the evolution of radiogenic isotope abundances over the history of the Earth have nonunique solutions. Both the recycling of continent-derived sediments into the <span class="hlt">mantle</span> and mixing in the <span class="hlt">mantle</span> could produce similar geochemical effects in the mean isotopic ratios of new igneous material emplaced in continents. Recent models of Archaean heat flow and of plate tectonics during <span class="hlt">early</span> Earth history have demonstrated that higher internal heat production of the <span class="hlt">early</span> Earth was mainly dissipated through a higher creation rate of oceanic lithosphere. If the seafloor creation rate was higher on the <span class="hlt">early</span> Earth, then the residence time of any one piece of oceanic lithosphere on the surface would have been shorter. It is possible that a higher rate of recycling of oceanic lithosphere into the <span class="hlt">mantle</span> could have resulted in some transport of sediment into the <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUSM.V72B..03H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUSM.V72B..03H"><span>The History of Exosphere Carbon Storage and Consequences for <span class="hlt">Mantle</span>-Exosphere Volatile Fluxes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hirschmann, M. M.</p> <p>2009-05-01</p> <p>The storage of volatiles in the <span class="hlt">mantle</span> and their fluxes between the <span class="hlt">mantle</span> and the near surface environment (exosphere) are constrained in part from the history of volatile storage in the exosphere. Evidence for the <span class="hlt">early</span> formation of the oceans indicates extensive initial degassing of the <span class="hlt">mantle</span>, but raises the question as to the fate of the carbon that must have been degassed with the H2O. Long-term storage of carbon in the exosphere is thought to require large continental areas, as carbon in the oceanic domain is rapidly returned to the <span class="hlt">mantle</span>. Consequently, <span class="hlt">early</span> degassing of the <span class="hlt">mantle</span> may have been followed by rapid massive return of carbon to the <span class="hlt">mantle</span> via subduction, leading to very high H/C ratios in the <span class="hlt">early</span> exosphere. Alternatively, the C may have been lost to space by impact ablation of a Venus-like CO2-rich atmosphere. Less plausibly, the C could have remained in the exosphere stored in the oceanic domain but somehow escaping recyling to the <span class="hlt">mantle</span>. Assuming that exosphere carbon storage was in fact limited by continental area, gradual regrowth of the carbon exosphere budget would then parallel that of growth of the continents. Interestingly, this suggests that the relatively high H/C ratio of the modern exosphere compared to the <span class="hlt">mantle</span> (Hirschmann and Dasgupta, 2009), is a remnant of very <span class="hlt">early</span> Earth processes which have not been erased by subsequent volatile fluxes. A key problem with this scenario, however, is that the gradual regrowth of the exosphere carbon budget cannot have occurred with parallel growth of the exosphere H2O budget. Otherwise, there would have been substantial growth of the oceans coinciding with continental growth, which violates constraints from continental freeboard. This requires either that outgassing of carbon exceeded that of H2O, or that H2O subduction has been more efficient than CO2 subduction. The former is unlikely unless typical degrees of melting are very small. On the other hand, petrologic constraints generally</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005GMS...160..117V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005GMS...160..117V"><span>Numerical study of the origin and stability of chemically distinct reservoirs deep in Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Thienen, P.; van Summeren, J.; van der Hilst, R. D.; van den Berg, A. P.; Vlaar, N. J.</p> <p></p> <p>Seismic tomography is providing mounting evidence for large scale compositional heterogeneity deep in Earth's <span class="hlt">mantle</span>; also, the diverse geochemical and isotopic signatures observed in oceanic basalts suggest that the <span class="hlt">mantle</span> is not chemically homogeneous. Isotopic studies on Archean rocks indicate that <span class="hlt">mantle</span> inhomogeneity may have existed for most of the Earth's history. One important component may be recycled oceanic crust, residing at the base of the <span class="hlt">mantle</span>. We investigate, by numerical modeling, if such reservoirs may have been formed in the <span class="hlt">early</span> Earth, before plate tectonics (and subduction) were possible, and how they have survived—and evolved—since then. During Earth's <span class="hlt">early</span> evolution, thick basaltic crust may have sunk episodically into the <span class="hlt">mantle</span> in short but vigorous diapiric resurfacing events. These sections of crust may have resided at the base of the <span class="hlt">mantle</span> for very long times. Entrainment of material from the enriched reservoirs thus produced may account for enriched <span class="hlt">mantle</span> and high-μ signatures in oceanic basalts, whereas deep subduction events may have shaped and replenished deep <span class="hlt">mantle</span> reservoirs. Our modeling shows that (1) convective instabilities and resurfacing may have produced deep enriched <span class="hlt">mantle</span> reservoirs before the era of plate tectonics; (2) such formation is qualitatively consistent with the geochemical record, which shows multiple distinct ocean island basalt sources; and (3) reservoirs thus produced may be stable for billions of years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004IJEaS..93.1025X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004IJEaS..93.1025X"><span><span class="hlt">Early</span> Cretaceous gabbroic complex from Yinan, Shandong Province: petrogenesis and <span class="hlt">mantle</span> domains beneath the North China Craton</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Yi-Gang; Ma, Jin-Long; Huang, Xiao-Long; Iizuka, Yoshiyuki; Chung, Sun-Lin; Wang, Yan-Bin; Wu, Xiang-Yang</p> <p>2004-12-01</p> <p>Sensitive high resolution ion microprobe (SHRIMP) zircon U Pb ages, geochemical and Sr-Nd-Pb isotopic data are reported for the gabbroic complex from Yinan (Shandong Province) with the aims of characterizing the nature of the Mesozoic <span class="hlt">mantle</span> beneath the North China Craton. The Yinan gabbros contain alkali feldspar and biotite, and are characterized by moderate Mg#, high SiO2, low FeO and TiO2 contents and a strong enrichment of light rare earth elements [(La/Yb)n=11 50], but no Eu anomaly. They have low Nb/La (0.07 0.29), radiogenic 87Sr/86Sr (0.710) and unradiogenic ɛNd(t) (-15 to -13). These “crustal fingerprints” cannot be attributed to crustal contamination, given the lack of correlation between isotopic ratios and <span class="hlt">differentiation</span> indices and the unreasonably high proportion of crustal contaminant (>20%) required in modeling. Instead, compositional similarities to contemporaneous basalts from nearby regions imply that the Yinan gabbros were not significantly affected by crystal cumulation. Isotopic data available for the Mesozoic mafic magmas reveal two distinct <span class="hlt">mantle</span> domains beneath Shandong. While the EM1-like domain (with low 87Sr/86Sr) is confined to western Shandong, the <span class="hlt">mantle</span> beneath eastern Shandong is dominated by EM2-type (with high 87Sr/86Sr) affinities. This aerial distinction suggests that the EM2-like signature of the Yinan gabbros may have been inherited from westerly-subducted Yangtze crust during the Triassic North China-South China collision. Emplacement of the Yinan gabbros (127 Ma) is likely affiliated with the widespread and protracted extension during the late Mesozoic in this region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2890712','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2890712"><span>Coupled 182W-142Nd constraint for <span class="hlt">early</span> Earth <span class="hlt">differentiation</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Moynier, Frederic; Yin, Qing-Zhu; Irisawa, Keita; Boyet, Maud; Jacobsen, Benjamin; Rosing, Minik T.</p> <p>2010-01-01</p> <p>Recent high precision 142Nd isotope measurements showed that global silicate <span class="hlt">differentiation</span> may have occurred as <span class="hlt">early</span> as 30–75 Myr after the Solar System formation [Bennett V, et al. (2007) Science 318:1907–1910]. This time scale is almost contemporaneous with Earth’s core formation at ∼30 Myr [Yin Q, et al. (2002) Nature 418:949–952]. The 182Hf-182W system provides a powerful complement to the 142Nd results for <span class="hlt">early</span> silicate <span class="hlt">differentiation</span>, because both core formation and silicate <span class="hlt">differentiation</span> fractionate Hf from W. Here we show that eleven terrestrial samples from diverse tectonic settings, including five <span class="hlt">early</span> Archean samples from Isua, Greenland, of which three have been previously shown with 142Nd anomalies, all have a homogeneous W isotopic composition, which is ∼2ε-unit more radiogenic than the chondritic value. By using a 3-stage model calculation that describes the isotopic evolution in chondritic reservoir and core segregation, as well as silicate <span class="hlt">differentiation</span>, we show that the W isotopic composition of terrestrial samples provides the most stringent time constraint for <span class="hlt">early</span> core formation (27.5–38 Myr) followed by <span class="hlt">early</span> terrestrial silicate <span class="hlt">differentiation</span> (38–75 Myr) that is consistent with the terrestrial 142Nd anomalies. PMID:20534492</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoRL..42.7073L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoRL..42.7073L"><span>Seismic anisotropy in the lowermost <span class="hlt">mantle</span> near the Perm Anomaly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Long, Maureen D.; Lynner, Colton</p> <p>2015-09-01</p> <p>The lower <span class="hlt">mantle</span> is dominated by two large structures with anomalously low shear wave velocities, known as Large Low-Shear Velocity Provinces (LLSVPs). Several studies have documented evidence for strong seismic anisotropy at the base of the <span class="hlt">mantle</span> near the edges of the African LLSVP. Recent work has identified a smaller structure with similar low-shear wave velocities beneath Eurasia, dubbed the Perm Anomaly. Here we probe lowermost <span class="hlt">mantle</span> anisotropy near the Perm Anomaly using the <span class="hlt">differential</span> splitting of SKS and SKKS phases measured at stations in Europe. We find evidence for lowermost <span class="hlt">mantle</span> anisotropy in the vicinity of the Perm Anomaly, with geographic trends hinting at lateral variations in anisotropy across the boundaries of the Perm Anomaly as well as across a previously unsampled portion of the African LLSVP border. Our observations suggest that deformation is concentrated at the boundaries of both the Perm Anomaly and the African LLSVP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AGUFM.S12D..03T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AGUFM.S12D..03T"><span>What <span class="hlt">Mantle</span> Processes Determine Isotopic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tackley, P. J.; Xie, S.</p> <p>2003-12-01</p> <p>Isotopic measurements on Mid Ocean Ridge Basalts and Ocean Island Basalts indicate effective `ages' (from e.g., U-Pb or Sm-Nd systems) in the range 1-2 billion years- much less than the age of the Earth, even though melting should have been much more vigorous <span class="hlt">early</span> on and skewed the mean time since melting to older values. This relatively young `age' has generally been explained in terms of stretching of heterogeneities by <span class="hlt">mantle</span> convection, which might reduce them to dimensions too small to be individually distinguishable in short timescales of less than 1 Gyr. On the other hand, published numerical models that use tracers to track <span class="hlt">differentiated</span> material (Christensen and Hofmann, 1994, Davies, 2002) suggest that Earth-like `ages' can be obtained without taking stretching-induced erasure of tracer signatures into account, although this might effectively happen if the lengthscale for sampling the isotope systems was large enough. In those models, the only explicit mechanism for resetting isotope systems was re-melting, but for this to explain the isotopic ages observed for basalts, the global rate of melting in the recent past would have had to be very much higher than present-day values. To investigate stretching vs. re-melting we have conducted numerical experiments of a cooling <span class="hlt">mantle</span> with plate tectonics, <span class="hlt">differentiation</span> and evolution of important isotopic systems. The time of last melting and the total strain is tracked on each tracer (in addition to isotopic information). The results confirm that a model matching today's crustal production rate and with a reasonable secular cooling history generates `ages' that are substantially larger than those observed, with the extent of crustal settling above the CMB making some difference but not enough. The effect of sampling lengthscale on observed `age' is also tested and found to be insufficient to explain the data. Thus, these results reaffirm the importance of stretching as a key mechanism for effectively deleting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70155928','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70155928"><span>Steady incision of Grand Canyon at the million year timeframe: a case for <span class="hlt">mantle</span>-driven <span class="hlt">differential</span> uplift</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Crow, Ryan S.; Karl Karlstrom,; Laura Crossey,; Richard Young,; Michael Ort,; Yemane Asmerom,; Victor Polyak,; Andrew Darling,</p> <p>2014-01-01</p> <p>The Grand Canyon region provides an excellent laboratory to examine the interplay between river incision, magmatism, and the geomorphic and tectonic processes that shape landscapes. Here we apply U-series, Ar–Ar, and cosmogenic burial dating of river terraces to examine spatial variations in incision rates along the 445 km length of the Colorado River through Grand Canyon. We also analyze strath terrace sequences that extend to heights of several hundred meters above the river, and integrate these with speleothem constrained maximum incision rates in several reaches to examine any temporal incision variations at the million-year time frame. This new high-resolution geochronology shows temporally steady long-term incision in any given reach of Grand Canyon but significant variations along its length from 160 m/Ma in the east to 101 m/Ma in the west. Spatial and temporal patterns of incision, and the long timescale of steady incision rule out models where geomorphic controls such as climate oscillations, bedrock strength, sediment load effects, or isostatic response to <span class="hlt">differential</span> denudation are the first order drivers of canyon incision. The incision pattern is best explained by a model of Neogene and ongoing epeirogenic uplift due to an eastward propagating zone of increased upper <span class="hlt">mantle</span> buoyancy that we infer from propagation of Neogene basaltic volcanism and a strong lateral gradient in modern upper <span class="hlt">mantle</span> seismic structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI43C..07P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI43C..07P"><span>Investigating melting induced <span class="hlt">mantle</span> heterogeneities in plate driven <span class="hlt">mantle</span> convection models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Price, M.; Davies, H.; Panton, J.</p> <p>2017-12-01</p> <p>Observations from geochemistry and seismology continue to suggest a range of complex heterogeneity in Earth's <span class="hlt">mantle</span>. In the deep <span class="hlt">mantle</span>, two large low velocity provinces (LLVPs) have been regularly observed in seismic studies, with their longevity, composition and density compared to the surrounding <span class="hlt">mantle</span> debated. The cause of these observed LLVPs is equally uncertain, with previous studies advocating either thermal or thermo-chemical causes. There is also evidence that these structures could provide chemically distinct reservoirs within the <span class="hlt">mantle</span>, with recent studies also suggesting there may be additional reservoirs in the <span class="hlt">mantle</span>, such as bridgmanite-enriched ancient <span class="hlt">mantle</span> structures (BEAMS). One way to test these hypotheses is using computational models of the <span class="hlt">mantle</span>, with models that capture the full 3D system being both complex and computationally expensive. Here we present results from our global <span class="hlt">mantle</span> model TERRA. Using our model, we can track compositional variations in the convecting <span class="hlt">mantle</span> that are generated by self-consistent, evolving melting zones. Alongside the melting, we track trace elements and other volatiles which can be partitioned during melting events, and expelled and recycled at the surface. Utilising plate reconstruction models as a boundary condition, the models generate the tectonic features observed at Earth's surface, while also organising the lower <span class="hlt">mantle</span> into recognisable degree-two structures. This results in our models generating basaltic `oceanic' crusts which are then brought into the <span class="hlt">mantle</span> at tectonic boundaries, providing additional chemical heterogeneity in the <span class="hlt">mantle</span> volume. Finally, by utilising thermodynamic lookup tables to convert the final outputs from the model to seismic structures, together with resolution filters for global tomography models, we are able to make direct comparisons between our results and observations. By varying the parameters of the model, we investigate a range of current hypotheses for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70030515','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70030515"><span><span class="hlt">Mantle</span> structure beneath the western edge of the Colorado Plateau</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Sine, C.R.; Wilson, D.; Gao, W.; Grand, S.P.; Aster, R.; Ni, J.; Baldridge, W.S.</p> <p>2008-01-01</p> <p>Teleseismic traveltime data are inverted for <span class="hlt">mantle</span> Vp and Vs variations beneath a 1400 km long line of broadband seismometers extending from eastern New Mexico to western Utah. The model spans 600 km beneath the moho with resolution of ???50 km. Inversions show a sharp, large-magnitude velocity contrast across the Colorado Plateau-Great Basin transition extending ???200 km below the crust. Also imaged is a fast anomaly 300 to 600 km beneath the NW portion of the array. Very slow velocities beneath the Great Basin imply partial melting and/or anomalously wet <span class="hlt">mantle</span>. We propose that the sharp contrast in <span class="hlt">mantle</span> velocities across the western edge of the Plateau corresponds to <span class="hlt">differential</span> lithospheric modification, during and following Farallon subduction, across a boundary defining the western extent of unmodified Proterozoic <span class="hlt">mantle</span> lithosphere. The deep fast anomaly corresponds to thickened Farallon plate or detached continental lithosphere at transition zone depths. Copyright 2008 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LPICo2084.4016J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LPICo2084.4016J"><span><span class="hlt">Early</span> Episodes of High-Pressure Core Formation Preserved in Plume <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jackson, C. R. M.; Bennett, N. R.; Du, Z.; Cottrell, E.; Fei, Y.</p> <p>2018-05-01</p> <p>New experiments demonstrate that xenon isotopes are sensitive to core formation. This behavior may be crucial in explaining the co-occurrence xenon and tungsten anomalies recently observed in plume <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009E%26PSL.282..306H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009E%26PSL.282..306H"><span>Magnesium stable isotope composition of Earth's upper <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Handler, Monica R.; Baker, Joel A.; Schiller, Martin; Bennett, Vickie C.; Yaxley, Gregory M.</p> <p>2009-05-01</p> <p>The <span class="hlt">mantle</span> is Earth's largest reservoir of Mg containing > 99% of Earth's Mg inventory. However, no consensus exists on the stable Mg isotope composition of the Earth's <span class="hlt">mantle</span> or how variable it is and, in particular, whether the <span class="hlt">mantle</span> has the same stable Mg isotope composition as chondrite meteorites. We have determined the Mg isotope composition of olivine from 22 <span class="hlt">mantle</span> peridotites from eastern Australia, west Antarctica, Jordan, Yemen and southwest Greenland by pseudo-high-resolution MC-ICP-MS on Mg purified to > 99%. The samples include fertile lherzolites, depleted harzburgites and dunites, cryptically metasomatised ('dry') peridotites and modally metasomatised apatite ± amphibole-bearing harzburgites and wehrlites. Olivine from these samples of <span class="hlt">early</span> Archaean through to Permian lithospheric <span class="hlt">mantle</span> have δ25Mg DSM-3 = - 0.22 to - 0.08‰. These data indicate the bulk upper <span class="hlt">mantle</span> as represented by peridotite olivine is homogeneous within current analytical uncertainties (external reproducibility ≤ ± 0.07‰ [2 sd]). We find no systematic δ25Mg variations with location, lithospheric age, peridotite fertility, or degree or nature of <span class="hlt">mantle</span> metasomatism. Although pyroxene may have slightly heavier δ25Mg than coexisting olivine, any fractionation between <span class="hlt">mantle</span> pyroxene and olivine is also within current analytical uncertainties with a mean Δ25Mg pyr-ol = +0.06 ± 0.10‰ (2 sd; n = 5). Our average <span class="hlt">mantle</span> olivine δ25Mg DSM-3 = - 0.14 ± 0.07‰ and δ26Mg DSM-3 = - 0.27 ± 0.14‰ (2 sd) are indistinguishable from the average of data previously reported for terrestrial basalts, confirming that basalts have stable Mg isotope compositions representative of the <span class="hlt">mantle</span>. Olivine from five pallasite meteorites have δ25Mg DSM-3 = - 0.16 to - 0.11‰ that are identical to terrestrial olivine and indistinguishable from the average δ25Mg previously reported for chondrites. These data provide no evidence for measurable heterogeneity in the stable Mg isotope</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15060619','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15060619"><span>Search for methylation-sensitive amplification polymorphisms associated with the <span class="hlt">mantled</span> variant phenotype in oil palm (Elaeis guineensis Jacq).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jaligot, E; Beulé, T; Baurens, F-C; Billotte, N; Rival, A</p> <p>2004-02-01</p> <p>The methylation-sensitive amplification polymorphism (MSAP) technique has been employed on somatic embryo-derived oil palms (Elaeis guineensis Jacq.) to identify methylation polymorphisms correlated with the "<span class="hlt">mantled</span>" somaclonal variation. The variant phenotype displays an unstable feminization of male organs in both male and female flowers. Using MSAP, the methylation status of CCGG sites was compared in three normal versus three <span class="hlt">mantled</span> regenerants sampled in clonal populations obtained through somatic embryogenesis from four genotypically distinct mother palms. Overall, 64 selective primer combinations were used and they have amplified 23 markers exhibiting a <span class="hlt">differential</span> methylation pattern between the two phenotypes. Our results indicate that CCGG sites are poorly affected by the considerable decrease in global DNA methylation that has been previously associated with the <span class="hlt">mantled</span> phenotype. Each of the 23 markers isolated in the present study could discriminate between the two phenotypes only when they were from the same genetic origin. This result hampers at the moment the direct use of MSAP markers for the <span class="hlt">early</span> detection of variants, even though valuable information on putative target sequences will be obtained from a further characterization of these polymorphic markers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4998958','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4998958"><span>An <span class="hlt">early</span> geodynamo driven by exsolution of <span class="hlt">mantle</span> components from Earth’s core</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Badro, James; Siebert, Julien; Nimmo, Francis</p> <p>2016-01-01</p> <p>Terrestrial core formation occurred in the <span class="hlt">early</span> molten Earth by gravitational segregation of immiscible metal and silicate melts, stripping iron-loving elements from the silicate <span class="hlt">mantle</span> to the metallic core1–3, and leaving rock-loving components behind. Here we performed experiments showing that at high enough temperature, Earth’s major rock-loving component, magnesium oxide, can also dissolve in core-forming metallic melts. Our data clearly point to a dissolution reaction, and are in agreement with recent DFT calculations4. Using core formation models5, we further show that a high-temperature event during Earth’s accretion (such as the Moon-forming giant impact6) can contribute significant amounts of magnesium to the <span class="hlt">early</span> core. As it subsequently cools, the ensuing exsolution7 of buoyant magnesium oxide generates a substantial amount of gravitational energy. This energy is comparable to if not significantly higher than that produced by inner core solidification8 — the primary driver of the Earth’s current magnetic field9–11. Since the inner core is too young12 to explain the existence of an ancient field prior to ~1 billion years, our results solve the conundrum posed by the recent paleomagnetic observation13 of an ancient field at least 3.45 Gyr old. PMID:27437583</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMDI31B2598F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMDI31B2598F"><span>Melting and Crystallization at Core <span class="hlt">Mantle</span> Boundary</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fiquet, G.; Pradhan, G. K.; Siebert, J.; Auzende, A. L.; Morard, G.; Antonangeli, D.; Garbarino, G.</p> <p>2015-12-01</p> <p><span class="hlt">Early</span> crystallization of magma oceans may generate original compositional heterogeneities in the <span class="hlt">mantle</span>. Dense basal melts may also be trapped in the lowermost <span class="hlt">mantle</span> and explain <span class="hlt">mantle</span> regions with ultralow seismic velocities (ULVZs) near the core-<span class="hlt">mantle</span> boundary [1]. To test this hypothesis, we first constructed the solidus curve of a natural peridotite between 36 and 140 gigapascals using laser-heated diamond anvil cells. In our experiments, melting at core-<span class="hlt">mantle</span> boundary pressures occurs around 4100 ± 150 K, which is a value that can match estimated <span class="hlt">mantle</span> geotherms. Similar results were found for a chondritic <span class="hlt">mantle</span> [2] whereas much lower pyrolitic melting temperatures were recently proposed from textural and chemical characterizations of quenched samples [3]. We also investigated the melting properties of natural mid ocean ridge basalt (MORB) up to core-<span class="hlt">mantle</span> boundary (CMB) pressures. At CMB pressure (135 GPa), we obtain a MORB solidus temperature of 3950 ±150 K. If our solidus temperatures are in good agreement with recent results proposed for a similar composition [4], the textural and chemical characterizations of our recovered samples made by analytical transmission electron microscope indicate that CaSiO3 perovskite (CaPv) is the liquidus phase in the entire pressure range up to CMB. The partial melt composition is enriched in FeO, which suggests that such partial melts could be gravitationnally stable at the core <span class="hlt">mantle</span> boundary. Our observations are tested against calculations made using a self-consistent thermodynamic database for the MgO-FeO-SiO2 system from 20 GPa to 140 GPa [5]. These observations and calculations provide a first step towards a consistent thermodynamic modelling of the crystallization sequence of the magma ocean, which shows that the existence of a dense iron rich and fusible layer above the CMB at the end of the crystallization is plausible [5], which is in contradiction with the conclusions drawn in [4]. [1] Williams</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR21C..07F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR21C..07F"><span>Melting behavior of Earth's lower <span class="hlt">mantle</span> minerals at high pressures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fu, S.; Yang, J.; Prakapenka, V. B.; Zhang, Y.; Greenberg, E.; Lin, J. F.</p> <p>2017-12-01</p> <p>Melting behavior of the most abundant lower <span class="hlt">mantle</span> minerals, bridgmanite and ferropericlase, at high pressure-temperature (P-T) conditions is of critical importance to understand the dynamic evolution of the <span class="hlt">early</span> Earth and to explain the seismological and geochemical signatures in the present lowermost <span class="hlt">mantle</span>. Theoretical calculations [1] and geodynamical models [2] suggested that partial melting of <span class="hlt">early</span> Earth among MgO-FeO-SiO2 ternary could be located at the eutectic point where a pyrolitic composition formed for the Earth's lower <span class="hlt">mantle</span> and the eutectic crystallization process could provide a plausible mechanism to the origin of the ultra-low velocity zones (ULVZs) near the core-<span class="hlt">mantle</span> boundary. Here we have investigated the melting behavior of ferropericlase and Al,Fe-bearing bridgmanite in laser-heated diamond anvil cells coupled with in situ X-ray diffraction up to 120 GPa. Together with chemical and texture characterizations of the quenched samples, these results are analyzed using thermodynamic models to address the effects of iron on the liquidus and solidus temperatures as well as solid-liquid iron partitioning and the eutectic point in ferropericlase-bridgmanite existing system at lower-<span class="hlt">mantle</span> pressure. In this presentation, we discuss the application of these results to better constrain the seismic observations of the deep lowermost <span class="hlt">mantle</span> such as large low shear wave velocity provinces (LLSVPs) and ULVZs. We will also discuss the geochemical consequences of the ferropericlase-bridgmanite melting due to the changes in the electronic spin and valence states of iron in the system. ADDIN EN.REFLIST 1. Boukaré, C.E., Y. Ricard, and G. Fiquet, Thermodynamics of the MgO-FeO-SiO2 system up to 140 GPa: Application to the crystallization of Earth's magma ocean. Journal of Geophysical Research: Solid Earth, 2015. 120(9): p. 6085-6101. 2. Labrosse, S., J. Hernlund, and N. Coltice, A crystallizing dense magma ocean at the base of the Earth's <span class="hlt">mantle</span>. Nature, 2007</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.U12A..06B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.U12A..06B"><span>Evolution of Subducted Oceanic Crust in Dynamic <span class="hlt">Mantle</span> Models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brandenburg, J.; van Keken, P. E.; Ballentine, C.; Hauri, E.</p> <p>2006-12-01</p> <p>Isotopic ratios measured in oceanic basalts indicate the persistence of a highly <span class="hlt">differentiated</span> and ancient <span class="hlt">mantle</span> component. The provenance and distribution of this component are the subject of much discussion. A number of geodynamic studies have focused on the preservation of a chemically dense layer in the deepest <span class="hlt">mantle</span>, while a smaller set of studies have explored the possibilities for its generation. We present an evaluation of the hypothesis that such a layer may represent the accumulation of subducted oceanic crust, with critical examination of the role that plate tectonics plays in <span class="hlt">mantle</span> <span class="hlt">differentiation</span>. In geodynamic models the treatment of plate tectonics controls crust production, subduction, and modulates the remixing rate. We use two methods for approximating plates in our models; prescription of a velocity boundary condition, and the force-balance method [1]. Emphasis is placed on the force-balance method, in which a numerical solution for the conservation of momentum is constructed by superposition. The force balance method has a minimum of free parameters compared to complex rheological descriptions that yield plate like behavior, and does not have the potential to artificially drive or hinder convection introduced by prescribing velocity boundary conditions. The mixing properties of the various methods are examined by comparison of embedded geochemical models for the isotopic evolution of Pb,U,Sm,Nd,Re,Os, and the noble gases. We find that the incorporation of strong plates leads to a <span class="hlt">mantle</span> with increased stratification of heterogeneity. Sequestration of old oceanic crust in dense pools in the lowermost <span class="hlt">mantle</span> is observed. However, the size and longevity of these dense pools decline considerably as realistic convective vigor is approached. Parameter space analysis is used to quantify this variability within the selection of models that reproduce Earth-like heat flow and plate velocities, and for comparison with the work of other authors. The</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.198..151W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.198..151W"><span>Zinc isotope fractionation during <span class="hlt">mantle</span> melting and constraints on the Zn isotope composition of Earth's upper <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Ze-Zhou; Liu, Sheng-Ao; Liu, Jingao; Huang, Jian; Xiao, Yan; Chu, Zhu-Yin; Zhao, Xin-Miao; Tang, Limei</p> <p>2017-02-01</p> <p>The zinc (Zn) stable isotope system has great potential for tracing planetary formation and <span class="hlt">differentiation</span> processes due to its chalcophile, lithophile and moderately volatile character. As an initial approach, the terrestrial <span class="hlt">mantle</span>, and by inference, the bulk silicate Earth (BSE), have previously been suggested to have an average δ66Zn value of ∼+0.28‰ (relative to JMC 3-0749L) primarily based on oceanic basalts. Nevertheless, data for <span class="hlt">mantle</span> peridotites are relatively scarce and it remains unclear whether Zn isotopes are fractionated during <span class="hlt">mantle</span> melting. To address this issue, we report high-precision (±0.04‰; 2SD) Zn isotope data for well-characterized peridotites (n = 47) from cratonic and orogenic settings, as well as their mineral separates. Basalts including mid-ocean ridge basalts (MORB) and ocean island basalts (OIB) were also measured to avoid inter-laboratory bias. The MORB analyzed have homogeneous δ66Zn values of +0.28 ± 0.03‰ (here and throughout the text, errors are given as 2SD), similar to those of OIB obtained in this study and in the literature (+0.31 ± 0.09‰). Excluding the metasomatized peridotites that exhibit a wide δ66Zn range of -0.44‰ to +0.42‰, the non-metasomatized peridotites have relatively uniform δ66Zn value of +0.18 ± 0.06‰, which is lighter than both MORB and OIB. This difference suggests a small but detectable Zn isotope fractionation (∼0.1‰) during <span class="hlt">mantle</span> partial melting. The magnitude of inter-mineral fractionation between olivine and pyroxene is, on average, close to zero, but spinels are always isotopically heavier than coexisting olivines (Δ66ZnSpl-Ol = +0.12 ± 0.07‰) due to the stiffer Zn-O bonds in spinel than silicate minerals (Ol, Opx and Cpx). Zinc concentrations in spinels are 11-88 times higher than those in silicate minerals, and our modelling suggests that spinel consumption during <span class="hlt">mantle</span> melting plays a key role in generating high Zn concentrations and heavy Zn isotopic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Tectp.658...14H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Tectp.658...14H"><span><span class="hlt">Mantle</span> structure and tectonic history of SE Asia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hall, Robert; Spakman, Wim</p> <p>2015-09-01</p> <p> that detached in the <span class="hlt">Early</span> Miocene such as the Sula slab, now found in the lower <span class="hlt">mantle</span> north of Lombok, and the Proto-South China Sea slab now at depths below 700 km curving from northern Borneo to the Philippines. Based on our tectonic model we interpret virtually all features seen in upper <span class="hlt">mantle</span> and lower <span class="hlt">mantle</span> to depths of at least 1200 km to be the result of Cenozoic subduction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V53B4843S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V53B4843S"><span>Volatile element content of the heterogeneous upper <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shimizu, K.; Saal, A. E.; Hauri, E. H.; Forsyth, D. W.; Kamenetsky, V. S.; Niu, Y.</p> <p>2014-12-01</p> <p>The physical properties of the asthenosphere (e.g., seismic velocity, viscosity, electrical conductivity) have been attributed to either mineral properties at relevant temperature, pressure, and water content or to the presence of a low melt fraction. We resort to the geochemical studies of MORB to unravel the composition of the asthenosphere. It is important to determine to what extent the geochemical variations in axial MORB do represent a homogeneous <span class="hlt">mantle</span> composition and variations in the physical conditions of magma generation and transport; or alternatively, they represent mixing of melts from a heterogeneous upper <span class="hlt">mantle</span>. Lavas from intra-transform faults and off-axis seamounts share a common <span class="hlt">mantle</span> source with axial MORB, but experience less <span class="hlt">differentiation</span> and homogenization. Therefore they provide better estimates for the end-member volatile budget of the heterogeneous upper <span class="hlt">mantle</span>. We present major, trace, and volatile element data (H2O, CO2, Cl, F, S) as well as Sr, Nd, and Pb isotopic compositions [1, 2] of basaltic glasses (MgO > 6.0 wt%) from the NEPR seamounts, Quebrada-Discovery-Gofar transform fault system, and Macquarie Island. The samples range from incompatible trace element (ITE) depleted (DMORB: Th/La<0.035) to enriched (EMORB: Th/La>0.07) spanning the entire range of EPR MORB. The isotopic composition of the samples correlates with the degree of trace element enrichment indicating long-lived <span class="hlt">mantle</span> heterogeneity. Once shallow-level processes (degassing, crystallization, and crustal assimilation) have been considered, we conducted a two-component (DMORB- and EMORB-) <span class="hlt">mantle</span> melting-mixing model. Our model reproduces the major, trace and volatile element contents and isotopic composition of our samples and suggests that (1) 90% of the upper <span class="hlt">mantle</span> is highly depleted in ITE (DMORB source) with only 10% of an enriched component (EMORB source), (2) the EMORB source is peridotitic rather than pyroxenitic, and (3) NMORB do not represent an actual</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12460481','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12460481"><span>Zoned <span class="hlt">mantle</span> convection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Albarède, Francis; Van Der Hilst, Rob D</p> <p>2002-11-15</p> <p>We review the present state of our understanding of <span class="hlt">mantle</span> convection with respect to geochemical and geophysical evidence and we suggest a model for <span class="hlt">mantle</span> convection and its evolution over the Earth's history that can reconcile this evidence. Whole-<span class="hlt">mantle</span> convection, even with material segregated within the D" region just above the core-<span class="hlt">mantle</span> boundary, is incompatible with the budget of argon and helium and with the inventory of heat sources required by the thermal evolution of the Earth. We show that the deep-<span class="hlt">mantle</span> composition in lithophilic incompatible elements is inconsistent with the storage of old plates of ordinary oceanic lithosphere, i.e. with the concept of a plate graveyard. Isotopic inventories indicate that the deep-<span class="hlt">mantle</span> composition is not correctly accounted for by continental debris, primitive material or subducted slabs containing normal oceanic crust. Seismological observations have begun to hint at compositional heterogeneity in the bottom 1000 km or so of the <span class="hlt">mantle</span>, but there is no compelling evidence in support of an interface between deep and shallow <span class="hlt">mantle</span> at mid-depth. We suggest that in a system of thermochemical convection, lithospheric plates subduct to a depth that depends - in a complicated fashion - on their composition and thermal structure. The thermal structure of the sinking plates is primarily determined by the direction and rate of convergence, the age of the lithosphere at the trench, the sinking rate and the variation of these parameters over time (i.e. plate-tectonic history) and is not the same for all subduction systems. The sinking rate in the <span class="hlt">mantle</span> is determined by a combination of thermal (negative) and compositional buoyancy and as regards the latter we consider in particular the effect of the loading of plates with basaltic plateaux produced by plume heads. Barren oceanic plates are relatively buoyant and may be recycled preferentially in the shallow <span class="hlt">mantle</span>. Oceanic plateau-laden plates have a more pronounced</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1344573-dehydrogenation-goethite-earths-deep-lower-mantle','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1344573-dehydrogenation-goethite-earths-deep-lower-mantle"><span>Dehydrogenation of goethite in Earth’s deep lower <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Hu, Qingyang; Kim, Duck Young; Liu, Jin</p> <p>2017-01-31</p> <p>The cycling of hydrogen influences the structure, composition, and stratification of Earth’s interior. Our recent discovery of pyrite-structured iron peroxide (designated as the P phase) and the formation of the P phase from dehydrogenation of goethite FeO 2H implies the separation of the oxygen and hydrogen cycles in the deep lower <span class="hlt">mantle</span> beneath 1,800 km. Here we further characterize the residual hydrogen, x, in the P-phase FeO 2Hx. Using a combination of theoretical simulations and high-pressure–temperature experiments, we calibrated the x dependence of molar volume of the P phase. Within the current range of experimental conditions, we observed a compositionalmore » range of P phase of 0.39 < x < 0.81, corresponding to 19–61% dehydrogenation. Increasing temperature and heating time will help release hydrogen and lower x, suggesting that dehydrogenation could be approaching completion at the high-temperature conditions of the lower <span class="hlt">mantle</span> over extended geological time. Our observations indicate a fundamental change in the mode of hydrogen release from dehydration in the upper <span class="hlt">mantle</span> to dehydrogenation in the deep lower <span class="hlt">mantle</span>, thus <span class="hlt">differentiating</span> the deep hydrogen and hydrous cycles.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMDI21A2263K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMDI21A2263K"><span><span class="hlt">Mantle</span> Plumes and Geologically Recent Volcanism on Mars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kiefer, W. S.</p> <p>2013-12-01</p> <p>Despite its small size, Mars has remained volcanically active until the geologically recent past. Crater retention ages on the volcanos Arsia Mon, Olympus Mons, and Pavonis Mons indicate significant volcanic activity in the last 100-200 million years. The radiometric ages of many shergottites, a type of igneous martian meteorite, indicate igneous activity at about 180 million years ago. These ages correspond to the most recent 2-4% of the age of the Solar System. The most likely explanation for this young martian volcanism is adiabatic decompression melting in upwelling <span class="hlt">mantle</span> plumes. Multiple plumes may be active at any time, with each of the major volcanos in the Tharsis region being formed by a separate plume. Like at least some terrestrial <span class="hlt">mantle</span> plumes, <span class="hlt">mantle</span> plumes on Mars likely form via an instability of the thermal boundary layer at the base of the <span class="hlt">mantle</span>. Because Mars operates in the stagnant lid convection regime, the temperature difference between <span class="hlt">mantle</span> and core is lower than on Earth. This reduces the temperature contrast between <span class="hlt">mantle</span> and core, resulting in <span class="hlt">mantle</span> plumes on Mars that are about 100 K hotter than the average <span class="hlt">mantle</span>. The chemical composition of the martian meteorites indicates that the martian <span class="hlt">mantle</span> is enriched in both iron and sodium relative to Earth's <span class="hlt">mantle</span>. This lowers the dry solidus on <span class="hlt">early</span> Mars by 30-40 K relative to Earth. Migration of sodium to the crust over time decreases this difference in solidus temperature to about 15 K at present, but that is sufficient to increase the current plume magma production rate by a factor of about 2. Hydrous phases in the martian meteorites indicate the presence of a few hundred ppm water in the <span class="hlt">mantle</span> source region, roughly the same as Earth. Finite element simulations of martian plumes using temperature-dependent viscosity and realistic Rayleigh numbers can reproduce the geologically recent magma production rate that is inferred from geologic mapping and the melt fraction inferred from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12460482','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12460482"><span>The thermochemical structure and evolution of Earth's <span class="hlt">mantle</span>: constraints and numerical models.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tackley, Paul J; Xie, Shunxing</p> <p>2002-11-15</p> <p>Geochemical observations place several constraints on geophysical processes in the <span class="hlt">mantle</span>, including a requirement to maintain several distinct reservoirs. Geophysical constraints limit plausible physical locations of these reservoirs to a thin basal layer, isolated deep 'piles' of material under large-scale <span class="hlt">mantle</span> upwellings, high-viscosity blobs/plums or thin strips throughout the <span class="hlt">mantle</span>, or some combination of these. A numerical model capable of simulating the thermochemical evolution of the <span class="hlt">mantle</span> is introduced. Preliminary simulations are more <span class="hlt">differentiated</span> than Earth but display some of the proposed thermochemical processes, including the generation of a high-mu <span class="hlt">mantle</span> reservoir by recycling of crust, and the generation of a high-(3)He/(4)He reservoir by recycling of residuum, although the resulting high-(3)He/(4)He material tends to aggregate near the top, where mid-ocean-ridge melting should sample it. If primitive material exists as a dense basal layer, it must be much denser than subducted crust in order to retain its primitive (e.g. high-(3)He) signature. Much progress is expected in the near future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V13E2896A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V13E2896A"><span><span class="hlt">Early</span> Earth slab stagnation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Agrusta, R.; Van Hunen, J.</p> <p>2016-12-01</p> <p>At present day, the Earth's <span class="hlt">mantle</span> exhibits a combination of stagnant and penetrating slabs within the transition zone, indicating a intermittent convection mode between layered and whole-<span class="hlt">mantle</span> convection. Isoviscous thermal convection calculations show that in a hotter Earth, the natural mode of convection was dominated by double-layered convection, which may imply that slabs were more prone to stagnate in the transition zone. Today, slab penetration is to a large extent controlled by trench mobility for a plausible range of lower <span class="hlt">mantle</span> viscosity and Clapeyron slope of the <span class="hlt">mantle</span> phase transitions. Trench mobility is, in turn, governed by slab strength and density and upper plate forcing. In this study, we systematically investigate the slab-transition zone internation in the <span class="hlt">Early</span> Earth, using 2D self-consistent numerical subduction models. <span class="hlt">Early</span> Earth's higher <span class="hlt">mantle</span> temperature facilitates decoupling between the plates and the underlying asthenosphere, and may result in slab sinking almost without trench retreat. Such behaviour together with a low resistance of a weak lower <span class="hlt">mantle</span> may allow slabs to penetrate. The ability of slab to sink into the lower <span class="hlt">mantle</span> throughout Earth's history may have important implications for Earth's evolution: it would provide efficient mass and heat flux through the transition zone therefore provide an efficient way to cool and mix the Earth's <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980137386','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980137386"><span>Pristine Igneous Rocks and the <span class="hlt">Early</span> <span class="hlt">Differentiation</span> of Planetary Materials</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Warren, Paul H.</p> <p>1998-01-01</p> <p>Our studies are highly interdisciplinary, but are focused on the processes and products of <span class="hlt">early</span> planetary and asteroidal <span class="hlt">differentiation</span>, especially the genesis of the ancient lunar crust. Most of the accessible lunar crust consists of materials hybridized by impact-mixing. Rare pristine (unmixed) samples reflect the original genetic diversity of the <span class="hlt">early</span> crust. We studied the relative importance of internally generated melt (including the putative magma ocean) versus large impact melts in <span class="hlt">early</span> lunar magmatism, through both sample analysis and physical modeling. Other topics under investigation included: lunar and SNC (martian?) meteorites; igneous meteorites in general; impact breccias, especially metal-rich Apollo samples and polymict eucrites; effects of regolith/megaregolith insulation on thermal evolution and geochronology; and planetary bulk compositions and origins. We investigated the theoretical petrology of impact melts, especially those formed in large masses, such as the unejected parts of the melts of the largest lunar and terrestrial impact basins. We developed constraints on several key effects that variations in melting/displacement ratio (a strong function of both crater size and planetary g) have on impact melt petrology. Modeling results indicate that the impact melt-derived rock in the sampled, megaregolith part of the Moon is probably material that was ejected from deeper average levels than the non-impact-melted material (fragmental breccias and unbrecciated pristine rocks). In the largest lunar impacts, most of the impact melt is of <span class="hlt">mantle</span> origin and avoids ejection from the crater, while most of the crust, and virtually all of the impact-melted crust, in the area of the crater is ejected. We investigated numerous extraordinary meteorites and Apollo rocks, emphasizing pristine rocks, siderophile and volatile trace elements, and the identification of primary partial melts, as opposed to partial cumulates. Apollo 15 sample 15434,28 is an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1811035V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1811035V"><span>Rheological properties of the lower crust and upper <span class="hlt">mantle</span> beneath Baja California: a microstructural study of xenoliths from San Quintin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Van der Werf, Thomas F.; Chatzaras, Vasileios; Tikoff, Basil; Drury, Martyn R.</p> <p>2016-04-01</p> <p>Baja California is an active transtensional rift zone, which links the San Andreas Fault with the East Pacific Rise. The erupted basalts of the Holocene San Quintin volcanic field contain xenoliths, which sample the lower crust and upper <span class="hlt">mantle</span> beneath Baja California. The aim of this research is to gain insight in the rheology of the lower crust and the upper <span class="hlt">mantle</span> by investigating the xenolith microstructure. Microstructural observations have been used to determine the dominant deformation mechanisms. <span class="hlt">Differential</span> stresses were estimated from recrystallized grain size piezometry of plagioclase and clinopyroxene for the lower crust and olivine for the upper <span class="hlt">mantle</span>. The degree of deformation can be inferred from macroscopic foliations and the deformation microstructures. Preliminary results show that both the lower crust and the upper <span class="hlt">mantle</span> have been affected by multiple stages of deformation and recrystallization. In addition the dominant deformation mechanism in both the lower crust and the upper <span class="hlt">mantle</span> is dislocation creep based on the existence of strong crystallographic preferred orientations. The <span class="hlt">differential</span> stress estimates for the lower crust are 10-29 MPa using plagioclase piezometry and 12-35 MPa using clinopyroxene piezometry. For the upper <span class="hlt">mantle</span>, <span class="hlt">differential</span> stress estimates are 10-20 MPa. These results indicate that the strength of the lower crust and the upper <span class="hlt">mantle</span> are very similar. Our data do not fit with the general models of lithospheric strength and may have important implications for the rheological structure of the lithosphere in transtensional plate margins and for geodynamic models of the region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.199....1C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.199....1C"><span>Metal-silicate partitioning of U: Implications for the heat budget of the core and evidence for reduced U in the <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chidester, Bethany A.; Rahman, Zia; Righter, Kevin; Campbell, Andrew J.</p> <p>2017-02-01</p> <p>Earth's core might require an internal heat source, such as radioactive decay, to explain the presence of the magnetic field through geologic time. To investigate whether U would be an important heat source in the core, we performed metal-silicate partitioning experiments of U at P-T (up to 67 GPa and 5400 K) conditions more relevant to a magma ocean scenario than has previously been reported. This study finds the partitioning of U to be strongly dependent on ƒO2, temperature, the S content of the metal and the SiO2 content of the silicate during core-<span class="hlt">mantle</span> <span class="hlt">differentiation</span>. <span class="hlt">Differentiation</span> at mean conditions of 42-58 GPa and 3900-4200 K would put 1.4-3.5 ppb U (2-8 wt% S) in the core, amounting to a maximum of 1.4 (+1/-0.7) TW of heat 4.5 billion years ago. This is likely not enough heat to mitigate <span class="hlt">early</span> widespread <span class="hlt">mantle</span> melting. It was also found that U likely exists in the 2+ oxidation state in silicate melts in the deep Earth, a state which has not been previously observed in nature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V33A3080M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V33A3080M"><span><span class="hlt">Early</span> onset of magma ocean crystallization revealed by coupled 146,147Sm-142,143Nd systematics of Nulliak ultramafics (3.78 Ga, Labrador)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morino, P.; Caro, G.; Reisberg, L. C.</p> <p>2015-12-01</p> <p><span class="hlt">Early</span> onset of magma ocean crystallization revealed by coupled 146,147Sm-142,143Nd systematics of Nulliak ultramafics (3.78 Ga, Labrador) Precillia Morino1, Guillaume Caro1, Laurie Reisberg 1 1CRPG-CNRS, Université de Lorraine, Nancy, France Coupled 146,147Sm-142,143Nd systematics provides constraints on the timing of magma ocean crystallization on Mars, the Moon and Vesta. Estimates for the Earth's <span class="hlt">mantle</span>, however, are less accurate owing to the sparsity of Eoarchean <span class="hlt">mantle</span>-derived rocks with undisturbed 147Sm-143Nd systematics. This study attempts to establish a coherent 142,143Nd dataset for the Eoarchean <span class="hlt">mantle</span> using well-preserved ultramafic rocks from the Nulliak assemblage (Labrador). Samples include meta-dunites, -pyroxenites and -peridotites exhibiting only minor serpentinization and limited element mobility. The presence of "Barberton type" komatiitic compositions (low Al/Ti, HREE depletion) is suggestive of a deep <span class="hlt">mantle</span> source. 146,147Sm-142,143Nd and 187Re-187Os analyses yield a crystallization age of 3.78±0.09 Ga with ɛ143Ndi=1.5±0.2 and ɛ142Nd=8.6±2 ppm. This 142,143Nd signature yields a model age of <span class="hlt">mantle</span> <span class="hlt">differentiation</span> of 4.43±0.05 Ga (assuming a BSE with chondritic Sm/Nd and ɛ142Nd=0). Superchondritic Sm/Nd compositions for the BSE would translate into older model ages. Irrespective of the choice of primitive <span class="hlt">mantle</span> composition, Nulliak ultramafics provide <span class="hlt">differentiation</span> ages 100 Ma older than those estimated from Akilia tonalites but remarkably similar to that estimated from the 2.7 Ga Theo's flow (Abitibi). If Nulliak ultramafics originated from deep melting of a hot plume, their model age could reflect the <span class="hlt">early</span> onset of magma ocean crystallization in the lowermost <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018DDA....4910102C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018DDA....4910102C"><span><span class="hlt">Early</span> Dynamics of the Moon's Core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cuk, Matija; Hamilton, Douglas; Stewart, Sarah T.</p> <p>2018-04-01</p> <p>The Moon has a small molten iron core (Williams et al. 2006). Remanent magnetization in lunar rocks likely derives from a past lunar dynamo (Wieczorek 2018 and references therein), which may have been powered by <span class="hlt">differential</span> precession between the <span class="hlt">mantle</span> and the core. The rotations of the lunar <span class="hlt">mantle</span> and core were largely decoupled for much of lunar history, with a large mutual offset during the Cassini State Transition (Meyer and Wisdom, 2011). It is likely that the past work underestimated lunar obliquities, and therefore core offsets, during <span class="hlt">early</span> lunar history (Cuk et al. 2016). Here we investigate the dynamics of the lunar core and <span class="hlt">mantle</span> using a Lie-Poisson numerical integrator (Touma and Wisdom 2001) which includes interactions between triaxial core and <span class="hlt">mantle</span>, as well as all gravitational and tidal effects included in the model of Cuk et al. (2016). Since we assume a rigid triaxial <span class="hlt">mantle</span>, this model is applicable to the Moon only once it has acquired its current shape, which probably happened before the Moon reached 25 Earth radii. While some details of the core dynamics depend on our assumptions about the shape of the lunar core-<span class="hlt">mantle</span> boundary, we can report some robust preliminary findings. The presence of the core does not change significantly the evolutionary scenario of Cuk et al. (2016). The core and <span class="hlt">mantle</span> are indeed decoupled, with the core having a much smaller obliquity to the ecliptic than the <span class="hlt">mantle</span> for almost all of the lunar history. The core was largely in an equivalent of Cassini State 2, with the vernal equinoxes (wrt the ecliptic) of the core and the <span class="hlt">mantle</span> being anti-aligned. The core-<span class="hlt">mantle</span> spin axis offset has been very large during the Moon's first billion years (this is true both in canonical and high-inclination tidal evolution), causing the lunar core to be sub-synchronous. If the ancient lunar magnetic dipole was rotating around the core axis that was inclined to the Moon's spin axis, then the magnetic poles would move across</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990JGR....9515779H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990JGR....9515779H"><span>Origin of <span class="hlt">mantle</span> peridotite: Constraints from melting experiments to 16.5 GPa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Herzberg, Claude; Gasparik, Tibor; Sawamoto, Hiroshi</p> <p>1990-09-01</p> <p> removal of orthopyroxene, followed by fractional crystallization of olivine, clinopyroxene, and garnet. The possibility exists that the thermal minimum is compositionally identical to <span class="hlt">mantle</span> peridotite in the 10-15 GPa range. If this can be confirmed by experiment, the upper <span class="hlt">mantle</span> can be understood as having originated by the fractional crystallization of peridotite liquids in a large-scale <span class="hlt">differentiation</span> event, consistent with magma ocean models for an <span class="hlt">early</span> Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PEPI..265...67A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PEPI..265...67A"><span>Toward a coherent model for the melting behavior of the deep Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrault, D.; Bolfan-Casanova, N.; Bouhifd, M. A.; Boujibar, A.; Garbarino, G.; Manthilake, G.; Mezouar, M.; Monteux, J.; Parisiades, P.; Pesce, G.</p> <p>2017-04-01</p> <p>Knowledge of melting properties is critical to predict the nature and the fate of melts produced in the deep <span class="hlt">mantle</span>. <span class="hlt">Early</span> in the Earth's history, melting properties controlled the magma ocean crystallization, which potentially induced chemical segregation in distinct reservoirs. Today, partial melting most probably occurs in the lowermost <span class="hlt">mantle</span> as well as at mid upper-<span class="hlt">mantle</span> depths, which control important aspects of <span class="hlt">mantle</span> dynamics, including some types of volcanism. Unfortunately, despite major experimental and theoretical efforts, major controversies remain about several aspects of <span class="hlt">mantle</span> melting. For example, the liquidus of the <span class="hlt">mantle</span> was reported (for peridotitic or chondritic-type composition) with a temperature difference of ∼1000 K at high <span class="hlt">mantle</span> depths. Also, the Fe partitioning coefficient (DFeBg/melt) between bridgmanite (Bg, the major lower <span class="hlt">mantle</span> mineral) and a melt was reported between ∼0.1 and ∼0.5, for a <span class="hlt">mantle</span> depth of ∼2000 km. Until now, these uncertainties had prevented the construction of a coherent picture of the melting behavior of the deep <span class="hlt">mantle</span>. In this article, we perform a critical review of previous works and develop a coherent, semi-quantitative, model. We first address the melting curve of Bg with the help of original experimental measurements, which yields a constraint on the volume change upon melting (ΔVm). Secondly, we apply a basic thermodynamical approach to discuss the melting behavior of mineralogical assemblages made of fractions of Bg, CaSiO3-perovskite and (Mg,Fe)O-ferropericlase. Our analysis yields quantitative constraints on the SiO2-content in the pseudo-eutectic melt and the degree of partial melting (F) as a function of pressure, temperature and <span class="hlt">mantle</span> composition; For examples, we find that F could be more than 40% at the solidus temperature, except if the presence of volatile elements induces incipient melting. We then discuss the melt buoyancy in a partial molten lower <span class="hlt">mantle</span> as a function of pressure</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR24A..04L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR24A..04L"><span>Elasticity of the Earth's Lower <span class="hlt">Mantle</span> Minerals at High Pressures: Implications to Understanding Seismic Observations of the Deep <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lin, J. F.; Yang, J.; Fu, S.</p> <p>2017-12-01</p> <p>Elasticity of the candidate lower-<span class="hlt">mantle</span> minerals at relevant P-T conditions of the region provides critical information in understanding seismic profiles, compositional and mineralogical models, and geodynamic processes of the Earth's interior. Here we will discuss recent major research advances in the investigation of the elasticity of major lower-<span class="hlt">mantle</span> minerals in a high-pressure diamond anvil cell coupled with Brillouin Light Scattering, Impulsive Stimulated Scattering (ISS), and X-ray diffraction. These have permitted direct and reliable measurements of both Vp and Vs to derive full elastic constants of single-crystal ferropericlase and (Fe, Al)-bearing bridgmanite as well as velocity profiles of polycrystalline silicate post-perovskite at relevant lower-<span class="hlt">mantle</span> pressures. The effects of the spin transition on the single-crystal elasticity of ferropericlase are now well understood experimentally and theoretically1,2: the spin transition causes drastic softening in elastic constants involving the compressive stress component (C11 and C12) due to the additional Gibbs free energy term arising from the mixing of the high-spin and low-spin states, while the elastic constant(s) related to the shear stress component (C44) is not affected. This leads to significant reduction in VP/VS ratio within the spin transition of ferropericlase in the mid-lower <span class="hlt">mantle</span>. The derived single-crystal Cij of bridgmanite at lower <span class="hlt">mantle</span> pressures display relatively small elastic Vp and Vs anisotropies as compared to the ferropericlase counterpart. Using thermoelastic modelling, we will discuss the application of the elasticity of ferropericlase, bridgmanite, and silicate post-perovskite at relevant conditions of the Earth's lower <span class="hlt">mantle</span> to <span class="hlt">differentiate</span> the role of the thermal vs. chemical perturbations as well as the spin transition and iron partitioning effects in the reported seismic lateral heterogeneity in lower <span class="hlt">mantle</span> as well as the D″ zone region3,4. We will address how recent</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28280925','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28280925"><span>A SoxC gene related to larval shell development and co-expression analysis of different shell formation genes in <span class="hlt">early</span> larvae of oyster.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Gang; Huan, Pin; Liu, Baozhong</p> <p>2017-06-01</p> <p>Among the potential larval shell formation genes in mollusks, most are expressed in cells surrounding the shell field during the <span class="hlt">early</span> phase of shell formation. The only exception (cgi-tyr1) is expressed in the whole larval <span class="hlt">mantle</span> and thus represents a novel type of expression pattern. This study reports another gene with such an expression pattern. The gene encoded a SoxC homolog of the Pacific oyster Crassostrea gigas and was named cgi-soxc. Whole-mount in situ hybridization revealed that the gene was highly expressed in the whole larval <span class="hlt">mantle</span> of <span class="hlt">early</span> larvae. Based on its spatiotemporal expression, cgi-soxc is hypothesized to be involved in periostracum biogenesis, biomineralization, and regulation of cell proliferation. Furthermore, we investigated the interrelationship between cgi-soxc expression and two additional potential shell formation genes, cgi-tyr1 and cgi-gata2/3. The results confirmed co-expression of the three genes in the larval <span class="hlt">mantle</span> of <span class="hlt">early</span> D-veliger. Nevertheless, cgi-gata2/3 was only expressed in the <span class="hlt">mantle</span> edge, and the other two genes were expressed in all <span class="hlt">mantle</span> cells. Based on the spatial expression patterns of the three genes, two cell groups were identified from the larval <span class="hlt">mantle</span> (tyr1 + /soxc + /gata2/3 + cells and tyr1 + /soxc + /gata2/3 - cells) and are important to study the <span class="hlt">differentiation</span> and function of this tissue. The results of this study enrich our knowledge on the structure and function of larval <span class="hlt">mantle</span> and provide important information to understand the molecular mechanisms of larval shell formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810141C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810141C"><span><span class="hlt">Mantle</span> Sulfur Cycle: A Case for Non-Steady State ?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cartigny, Pierre; Labidi, Jabrane</p> <p>2016-04-01</p> <p>Data published over the last 5 years show that the <span class="hlt">early</span> inference that <span class="hlt">mantle</span> is isotopically homogeneous is no more valid. Instead, new generation data on lavas range over a significant 34S/32S variability of up to 5‰ with δ 34S values often correlated to Sr- and Nd-isotope compositions. This new set of data also reveals the Earth's <span class="hlt">mantle</span> to have a sub-chondritic 34S/32S ratio, by about ˜ 1‰. We will present at the conference our published and unpublished data on samples characterizing the different <span class="hlt">mantle</span> components (i.e. EM1, EM2, HIMU and LOMU). All illustrate 34S-enrichments compared to MORB with Δ 33S and Δ 36S values indistinguishable from CDT or chondrites at the 0.03‰ level. These data are consistent with the recycling of subducted components carrying sulfur with Δ 33S and Δ 36S-values close to zero. Archean rocks commonly display Δ 33S and Δ 36S values deviating from zero by 1 to 10 ‰. The lack of variations for Δ 33S and Δ 36S values in present day lava argue against the sampling of any subducted protolith of Archean age in their <span class="hlt">mantle</span> source. Instead, our data are consistent with the occurrence of Proterozoic subducted sulfur in the source of the EM1, EM2, LOMU and HIMU endmember at the St-Helena island. This is in agreement with the age of those components <span class="hlt">early</span> derived through the use of the Pb isotope systematic. Currently, the negative δ 34S-values of the depleted <span class="hlt">mantle</span> seem to be associated with mostly positive values of enriched components. This would be inconsistent with the concept a steady state of sulfur. Assuming that the overall observations of recycled sulfur are not biased, the origin of such a non-steady state remains unclear. It could be related to the relatively compatible behavior of sulfur during partial melting, as the residue of present-day melting can be shown to always contain significant amounts of sulfide (50{%} of what is observed in a fertile source). This typical behavior likely prevents an efficient</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23803848','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23803848"><span>Stability of active <span class="hlt">mantle</span> upwelling revealed by net characteristics of plate tectonics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Conrad, Clinton P; Steinberger, Bernhard; Torsvik, Trond H</p> <p>2013-06-27</p> <p>Viscous convection within the <span class="hlt">mantle</span> is linked to tectonic plate motions and deforms Earth's surface across wide areas. Such close links between surface geology and deep <span class="hlt">mantle</span> dynamics presumably operated throughout Earth's history, but are difficult to investigate for past times because the history of <span class="hlt">mantle</span> flow is poorly known. Here we show that the time dependence of global-scale <span class="hlt">mantle</span> flow can be deduced from the net behaviour of surface plate motions. In particular, we tracked the geographic locations of net convergence and divergence for harmonic degrees 1 and 2 by computing the dipole and quadrupole moments of plate motions from tectonic reconstructions extended back to the <span class="hlt">early</span> Mesozoic era. For present-day plate motions, we find dipole convergence in eastern Asia and quadrupole divergence in both central Africa and the central Pacific. These orientations are nearly identical to the dipole and quadrupole orientations of underlying <span class="hlt">mantle</span> flow, which indicates that these 'net characteristics' of plate motions reveal deeper flow patterns. The positions of quadrupole divergence have not moved significantly during the past 250 million years, which suggests long-term stability of <span class="hlt">mantle</span> upwelling beneath Africa and the Pacific Ocean. These upwelling locations are positioned above two compositionally and seismologically distinct regions of the lowermost <span class="hlt">mantle</span>, which may organize global <span class="hlt">mantle</span> flow as they remain stationary over geologic time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAESc.145..233X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAESc.145..233X"><span>Continental basalts record the crust-<span class="hlt">mantle</span> interaction in oceanic subduction channel: A geochemical case study from eastern China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Zheng; Zheng, Yong-Fei</p> <p>2017-09-01</p> <p>Continental basalts, erupted in either flood or rift mode, usually show oceanic island basalts (OIB)-like geochemical compositions. Although their depletion in Sr-Nd isotope compositions is normally ascribed to contributions from the asthenospheric <span class="hlt">mantle</span>, their enrichment in large ion lithophile elements (LILE) and light rare earth elements (LREE) is generally associated with variable enrichments in the Sr-Nd isotope compositions. This indicates significant contributions from crustal components such as igneous oceanic crust, lower continental crust and seafloor sediment. Nevertheless, these crustal components were not incorporated into the <span class="hlt">mantle</span> sources of continental basalts in the form of solidus rocks. Instead they were processed into metasomatic agents through low-degree partial melting in order to have the geochemical fractionation of the largest extent to achieve the enrichment of LILE and LREE in the metasomatic agents. Therefore, the <span class="hlt">mantle</span> sources of continental basalts were generated by metasomatic reaction of the depleted mid-ocean ridge basalts (MORB) <span class="hlt">mantle</span> with hydrous felsic melts. Nevertheless, mass balance considerations indicate <span class="hlt">differential</span> contributions from the <span class="hlt">mantle</span> and crustal components to the basalts. While the depleted MORB <span class="hlt">mantle</span> predominates the budget of major elements, the crustal components predominate the budget of melt-mobile incompatible trace elements and their pertinent radiogenic isotopes. These considerations are verified by model calculations that are composed of four steps in an ancient oceanic subduction channel: (1) dehydration of the subducting crustal rocks at subarc depths, (2) anataxis of the dehydrated rocks at postarc depths, (3) metasomatic reaction of the depleted MORB <span class="hlt">mantle</span> peridotite with the felsic melts to generate ultramafic metasomatites in the lower part of the <span class="hlt">mantle</span> wedge, and (4) partial melting of the metasomatites for basaltic magmatism. The composition of metasomatites is quantitatively dictated by</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24957109','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24957109"><span>Characterization of ibrutinib-sensitive and -resistant <span class="hlt">mantle</span> lymphoma cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ma, Jiao; Lu, Pin; Guo, Ailin; Cheng, Shuhua; Zong, Hongliang; Martin, Peter; Coleman, Morton; Wang, Y Lynn</p> <p>2014-09-01</p> <p>Ibrutinib inhibits Bruton tyrosine kinase (BTK), a key component of <span class="hlt">early</span> B-cell receptor (BCR) signalling pathways. A multicentre phase 2 trial of ibrutinib in patients with relapsed/refractory <span class="hlt">mantle</span> cell lymphoma (MCL) demonstrated a remarkable response rate. However, approximately one-third of patients have primary resistance to the drug while other patients appear to lose response and develop secondary resistance. Understanding the molecular mechanisms underlying ibrutinib sensitivity is of paramount importance. In this study, we investigated cell lines and primary MCL cells that display <span class="hlt">differential</span> sensitivity to ibrutinib. We found that the primary cells display a higher BTK activity than normal B cells and MCL cells show <span class="hlt">differential</span> sensitivity to BTK inhibition. Genetic knockdown of BTK inhibits the growth, survival and proliferation of ibrutinib-sensitive but not resistant MCL cell lines, suggesting that ibrutinib acts through BTK to produce its anti-tumour activities. Interestingly, inhibition of ERK1/2 and AKT, but not BTK phosphorylation per se, correlates well with cellular response to BTK inhibition in cell lines as well as in primary tumours. Our study suggests that, to prevent primary resistance or to overcome secondary resistance to BTK inhibition, a combinatory strategy that targets multiple components or multiple pathways may represent the most effective approach. © 2014 John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.223..300L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.223..300L"><span>A reconnaissance view of tungsten reservoirs in some crustal and <span class="hlt">mantle</span> rocks: Implications for interpreting W isotopic compositions and crust-<span class="hlt">mantle</span> W cycling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Jingao; Pearson, D. Graham; Chacko, Thomas; Luo, Yan</p> <p>2018-02-01</p> <p>High-precision measurements of W isotopic ratios have enabled increased exploration of <span class="hlt">early</span> Earth processes. However, when applying W isotopic data to understand the geological processes, it is critical to recognize the potential mobility of W and hence evaluate whether measured W contents and isotopic compositions reflect the primary petrogenetic processes or instead are influenced by the effects of secondary inputs/mobility. Furthermore, if we are to better understand how W is partitioned between different minerals during melting and metasomatic processes it is important to document the likely sinks for W during these processes. In addition, an understanding of the main hosts for W in the crust and <span class="hlt">mantle</span> is critically important to constrain how W is cycled and stored in the crust-<span class="hlt">mantle</span> geochemical cycle. As a first step to investigate these issues, we have carried out in situ concentration measurements of W and other HFSEs in mineral phases within a broad spectrum of crustal and <span class="hlt">mantle</span> rocks, along with whole-rock concentration measurements. Mass balance shows that for tonalitic gneiss and amphibolite, the major rock-forming minerals can adequately account for the bulk W budget, and for the pristine ultramafic rocks, olivine and orthopyroxene are the major controlling phases for W whereas for metasomatized ultramafic rocks, significant W is hosted in Ti-bearing trace phases (e.g., rutile, lindsleyite) along grain boundaries or is inferred to reside in cryptic W-bearing trace phases. Formation or decomposition of these phases during secondary processes could cause fractionation of W from other HFSEs, and also dramatically modify bulk W concentrations in rocks. For rocks that experienced subsequent W enrichment/alteration, their W isotopic compositions may not necessarily represent their <span class="hlt">mantle</span> sources, but could reflect later inputs. The relatively small suite of rocks analyzed here serves as a reconnaissance study but allows some preliminary speculations on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JAESc..37..229W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JAESc..37..229W"><span>Co-rich sulfides in <span class="hlt">mantle</span> peridotites from Penghu Islands, Taiwan: Footprints of Proterozoic <span class="hlt">mantle</span> plumes under the Cathaysia Block</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Kuo-Lung; O'Reilly, Suzanne Y.; Honda, Masahiko; Matsumoto, Takuya; Griffin, William L.; Pearson, Norman J.; Zhang, Ming</p> <p>2010-02-01</p> <p> Proterozoic evolution ( Li et al. (2008) Precambrian Research 160, 179-210 and references therein). Olivine in a peridotite sample from the TCY locality has distinctly high 3He/ 4He (11 R A), whereas other peridotites from the KP and TCY localities have 3He/ 4He ˜6.7 R A, lower than MORB. The high 3He/ 4He further suggests that materials from the deep <span class="hlt">mantle</span> have interacted with the host peridotite of Co-rich sulfides. We thus propose that the Co-rich sulfide melts may have been trapped in the lower <span class="hlt">mantle</span> during core-<span class="hlt">mantle</span> <span class="hlt">differentiation</span> and then transported to shallow depths by <span class="hlt">mantle</span> plumes that entrained lower <span class="hlt">mantle</span> materials at several different time periods. This study provides the first substantial evidence from the lithosperic <span class="hlt">mantle</span> beneath the Cathaysia Block to support the activity of <span class="hlt">mantle</span> plumes related to the breakup of the supercontinents Nena/Columbia and Rodinia in Proterozoic time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16179070','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16179070"><span>XBtg2 is required for notochord <span class="hlt">differentiation</span> during <span class="hlt">early</span> Xenopus development.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sugimoto, Kaoru; Hayata, Tadayoshi; Asashima, Makoto</p> <p>2005-09-01</p> <p>The notochord is essential for normal vertebrate development, serving as both a structural support for the embryo and a signaling source for the patterning of adjacent tissues. Previous studies on the notochord have mostly focused on its formation and function in <span class="hlt">early</span> organogenesis but gene regulation in the <span class="hlt">differentiation</span> of notochord cells itself remains poorly defined. In the course of screening for genes expressed in developing notochord, we have isolated Xenopus homolog of Btg2 (XBtg2). The mammalian Btg2 genes, Btg2/PC3/TIS21, have been reported to have multiple functions in the regulation of cell proliferation and <span class="hlt">differentiation</span> but their roles in <span class="hlt">early</span> development are still unclear. Here we characterized XBtg2 in <span class="hlt">early</span> Xenopus laevis embryogenesis with focus on notochord development. Translational inhibition of XBtg2 resulted in a shortened and bent axis phenotype and the abnormal structures in the notochord tissue, which did not undergo vacuolation. The XBtg2-depleted notochord cells expressed <span class="hlt">early</span> notochord markers such as chordin and Xnot at the <span class="hlt">early</span> tailbud stage, but failed to express <span class="hlt">differentiation</span> markers of notochord such as Tor70 and 5-D-4 antigens in the later stages. These results suggest that XBtg2 is required for the <span class="hlt">differentiation</span> of notochord cells such as the process of vacuolar formation after determination of notochord cell fate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940015658','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940015658"><span>Inversion of gravity and bathymetry in oceanic regions for long-wavelength variations in upper <span class="hlt">mantle</span> temperature and composition</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Solomon, Sean C.; Jordan, Thomas H.</p> <p>1993-01-01</p> <p>Long-wavelength variations in geoid height, bathymetry, and SS-S travel times are all relatable to lateral variations in the characteristic temperature and bulk composition of the upper <span class="hlt">mantle</span>. The temperature and composition are in turn relatable to <span class="hlt">mantle</span> convection and the degree of melt extraction from the upper <span class="hlt">mantle</span> residuum. Thus the combined inversion of the geoid or gravity field, residual bathymetry, and seismic velocity information offers the promise of resolving fundamental aspects of the pattern of <span class="hlt">mantle</span> dynamics. The use of <span class="hlt">differential</span> body wave travel times as a measure of seismic velocity information, in particular, permits resolution of lateral variations at scales not resolvable by conventional global or regional-scale seismic tomography with long-period surface waves. These intermediate scale lengths, well resolved in global gravity field models, are crucial for understanding the details of any chemical or physical layering in the <span class="hlt">mantle</span> and of the characteristics of so-called 'small-scale' convection beneath oceanic lithosphere. In 1991 a three-year project to the NASA Geophysics Program was proposed to carry out a systematic inversion of long-wavelength geoid anomalies, residual bathymetric anomalies, and <span class="hlt">differential</span> SS-S travel time delays for the lateral variation in characteristic temperature and bulk composition of the oceanic upper <span class="hlt">mantle</span>. The project was funded as a three-year award, beginning on 1 Jan. 1992.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.478...47L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.478...47L"><span>The source location of <span class="hlt">mantle</span> plumes from 3D spherical models of <span class="hlt">mantle</span> convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Mingming; Zhong, Shijie</p> <p>2017-11-01</p> <p><span class="hlt">Mantle</span> plumes are thought to originate from thermal boundary layers such as Earth's core-<span class="hlt">mantle</span> boundary (CMB), and may cause intraplate volcanism such as large igneous provinces (LIPs) on the Earth's surface. Previous studies showed that the original eruption sites of deep-sourced LIPs for the last 200 Myrs occur mostly above the margins of the seismically-observed large low shear velocity provinces (LLSVPs) in the lowermost <span class="hlt">mantle</span>. However, the mechanism that leads to the distribution of the LIPs is not clear. The location of the LIPs is largely determined by the source location of <span class="hlt">mantle</span> plumes, but the question is under what conditions <span class="hlt">mantle</span> plumes form outside, at the edges, or above the middle of LLSVPs. Here, we perform 3D geodynamic calculations and theoretical analyses to study the plume source location in the lowermost <span class="hlt">mantle</span>. We find that a factor of five decrease of thermal expansivity and a factor of two increase of thermal diffusivity from the surface to the CMB, which are consistent with mineral physics studies, significantly reduce the number of <span class="hlt">mantle</span> plumes forming far outside of thermochemical piles (i.e., LLSVPs). An increase of <span class="hlt">mantle</span> viscosity in the lowermost <span class="hlt">mantle</span> also reduces number of plumes far outside of piles. In addition, we find that strong plumes preferentially form at/near the edges of piles and are generally hotter than that forming on top of piles, which may explain the observations that most LIPs occur above LLSVP margins. However, some plumes originated at pile edges can later appear above the middle of piles due to lateral movement of the plumes and piles and morphologic changes of the piles. ∼65-70% strong plumes are found within 10 degrees from pile edges in our models. Although plate motion exerts significant controls over the large-scale <span class="hlt">mantle</span> convection in the lower <span class="hlt">mantle</span>, <span class="hlt">mantle</span> plume formation at the CMB remains largely controlled by thermal boundary layer instability which makes it difficult to predict geographic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12..675B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12..675B"><span>Osmium isotopes suggest fast and efficient mixing in the oceanic upper <span class="hlt">mantle</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bizimis, Michael; Salters, Vincent</p> <p>2010-05-01</p> <p>The depleted upper <span class="hlt">mantle</span> (DUM; the source of MORB) is thought to represent the complementary reservoir of continental crust extraction. Previous studies have calculated the "average" DUM composition based on the geochemistry of MORB. However the Nd isotope compositions of abyssal peridotites have been shown to extend to more depleted compositions than associated MORB. While this argues for the presence of both relatively depleted and enriched material within the upper <span class="hlt">mantle</span>, the extent of compositional variability, length scales of heterogeneity and timescales of mixing in the upper <span class="hlt">mantle</span> are not well constrained. Model calculations show that 2Ga is a reasonable mean age of depletion for DUM while Hf - Nd isotopes show the persistence of a depleted terrestrial reservoir by the <span class="hlt">early</span> Archean (3.5-3.8Ga). U/Pb zircon ages of crustal rocks show three distinct peaks at 1.2, 1.9, and 2.7Ga and these are thought to represent the ages of three major crustal growth events. A fundamental question therefore is whether the present day upper <span class="hlt">mantle</span> retains a memory of multiple ancient depletion events, or has been effectively homogenized. This has important implications for the nature of convection and time scales of survival of heterogeneities in the upper <span class="hlt">mantle</span>. Here we compare published Os isotope data from abyssal peridotites and ophiolitic Os-Ir alloys with new data from Hawaiian spinel peridotite xenoliths. The Re-Os isotope system has been shown to yield useful depletion age information in peridotites, so we use it here to investigate the distribution of Re-depletion ages (TRD) in these <span class="hlt">mantle</span> samples as a proxy for the variability of DUM. The probability density functions (PDF) of TRD from osmiridiums, abyssal and Hawaiian peridotites are all remarkably similar and show a distinct peak at 1.2-1.3 Ga (errors for TRD are set at 0.2Ga to suppress statistically spurious age peaks). The Hawaiian peridotites further show a distinct peak at 1.9-2Ga, but no oceanic <span class="hlt">mantle</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040040130&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearths%2Bouter%2Bcore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040040130&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearths%2Bouter%2Bcore"><span>Density Anomalies in the <span class="hlt">Mantle</span> and the Gravitational Core-<span class="hlt">Mantle</span> Interaction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuang, Weijia; Liu, Lanbo</p> <p>2003-01-01</p> <p>Seismic studies suggest that the bulk of the <span class="hlt">mantle</span> is heterogeneous, with density variations in depth as well as in horizontal directions (latitude and longitude). This density variation produces a three- dimensional gravity field throughout the Earth. On the other hand, the core density also varies in both time and space, due to convective core flow. Consequently, the fluid outer core and the solid <span class="hlt">mantle</span> interact gravitationally due to the mass anomalies in both regions. This gravitational core-<span class="hlt">mantle</span> interaction could play a significant role in exchange of angular momentum between the core and the <span class="hlt">mantle</span>, and thus the change in Earth's rotation on time scales of decades and longer. Aiming at estimating the significance of the gravitational core-<span class="hlt">mantle</span> interaction on Earth's rotation variation, we introduce in our MoSST core dynamics model a heterogeneous <span class="hlt">mantle</span>, with a density distribution derived from seismic results. In this model, the core convection is driven by the buoyancy forces. And the density variation is determined dynamically with the convection. Numerical simulation is carried out with different parameter values, intending to extrapolate numerical results for geophysical implications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70011540','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70011540"><span>Effects of selective fusion on the thermal history of the earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Lee, W.H.K.</p> <p>1968-01-01</p> <p>A comparative study on the thermal history of the earth's <span class="hlt">mantle</span> was made by numerical solutions of the heat equation including and excluding selective fusion of silicates. Selective fusion was approximated by melting in a multicomponent system and redistribution of radioactive elements. Effects of selective fusion on the thermal models are (1) lowering (by several hundred degrees centigrade) and stabilizing the internal temperature distribution, and (2) increasing the surface heat-flow. It was found that models with selective fusion gave results more compatible with observations of both present temperature and surface heat-flow. The results therefore suggest continuous <span class="hlt">differentiation</span> of the earth's <span class="hlt">mantle</span> throughout geologic time, and support the hypothesis that the earth's atmosphere, oceans, and crust have been accumulated throughout the earth's history by degassing and selective fusion of the <span class="hlt">mantle</span>. ?? 1968.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1983GeCoA..47.1191T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1983GeCoA..47.1191T"><span>Evolution of depleted <span class="hlt">mantle</span>: The lead perspective</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tilton, George R.</p> <p>1983-07-01</p> <p>Isotopic data have established that, compared to estimated bulk earth abundances, the sources of oceanic basaltic lavas have been depleted in large ion lithophile elements for at least several billions of years. Various data on the Tertiary-Mesozoic Gorgona komatiite and Cretaceous Oka carbonatite show that those rocks also sample depleted <span class="hlt">mantle</span> sources. This information is used by analogy to compare Pb isotopic data from 2.6 billion year old komatiite and carbonatite from the Suomussalmi belt of eastern Finland and Munro Township, Ontario that are with associated granitic rocks and ores that should contain marked crustal components. Within experimental error no differences are detected in the isotopic composition of initial Pb in either of the rock suites. These observations agree closely with Sr and Nd data from other laboratories showing that depleted <span class="hlt">mantle</span> could not have originated in those areas more than a few tenths of billions of years before the rocks were emplaced. On a world-wide basis the Pb isotope data are consistent with production of depleted <span class="hlt">mantle</span> by continuous <span class="hlt">differentiation</span> processes acting over approximately the past 3 billion years. The data show that Pb evolution is more complex than the simpler models derived from the Rb-Sr and Sm-Nd systems. The nature of the complexity is still poorly understood.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.V41B2292H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.V41B2292H"><span>Rhenium - osmium heterogeneity of enriched <span class="hlt">mantle</span> basalts explained by composition and behaviour of <span class="hlt">mantle</span>-derived sulfides</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harvey, J.; Dale, C. W.; Gannoun, A.; Burton, K. W.</p> <p>2010-12-01</p> <p>Analyses of enriched <span class="hlt">mantle</span> (EM) -basalts, using lithophile element-based isotope systems have long provided evidence for discrete, but variable <span class="hlt">mantle</span> reservoirs [1]. Upon partial melting, the isotopic fingerprint of each reservoir is imparted upon the partial melt produced. However, recent work involving the Re-Os isotope systematics of EM-basalts [2] suggests that it may not be so simple to delimit these previously well defined <span class="hlt">mantle</span> reservoirs; the “<span class="hlt">mantle</span> zoo” [3] may contain more reservoirs than previously envisaged. However, a simple model, with varying contributions from two populations of compositionally distinct <span class="hlt">mantle</span> sulfides can readily account for the observed heterogeneities in Re-Os isotope systematics of such basalts without additional <span class="hlt">mantle</span> reservoirs. Rhenium-osmium elemental and isotopic analyses of individual sulfide grains separated from spinel lherzolites from Kilbourne Hole, NM, USA demonstrate that two discrete populations of <span class="hlt">mantle</span> sulfide exist in terms of both Re-Os systematics and textural relationship with co-existing silicates. One population, with a rounded morphology, is preserved in silicate grains and typically possesses high [Os], low [Re] with unradiogenic, typically sub-chondritic, 187Os/188Os attributable to long term isolation in a low-Re environment. By contrast, irregular-shaped sulfides, preserved along silicate grain boundaries, possess low [Os], higher [Re] and a wider range of, but generally supra-chondritic, 187Os/188Os ([Os] typically ≤ 1-2 ppm, 187Os/188Os ≤ 0.3729; this study). This population is thought to represent metasomatic sulfide (e.g. [4,5]). Uncontaminated silicate phases contain negligible Os (<100 ppt) therefore the Os elemental and isotope composition of basalts is dominated by volumetrically insignificant sulfide ([Os] ≤ 37 ppm, this study). During the <span class="hlt">early</span> stages of partial melting, supra-chondritic interstitial sulfides are mobilized and incorporated into the melt, adding their radiogenic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CoMP..172...74V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CoMP..172...74V"><span>Geochemical characteristics of the La Réunion <span class="hlt">mantle</span> plume source inferred from olivine-hosted melt inclusions from the adventive cones of Piton de la Fournaise volcano (La Réunion Island)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Valer, Marina; Schiano, Pierre; Bachèlery, Patrick</p> <p>2017-09-01</p> <p>Major and trace element compositions were obtained for bulk rocks and melt inclusions hosted in olivine crystals (Fo > 85) from the adventive cones of the Piton de La Fournaise volcano (La Réunion Island). Ratios of highly incompatible trace elements for these magmas are used to identify the nature of the La Réunion <span class="hlt">mantle</span> plume source. Although adventive cone lavas display unusual major element compositions compared to the historical lavas of the volcano (e.g., lower CaO/Al2O3), trace element data suggest that the magmas emitted by the adventive cones originate from a common chemical source. This source may correspond to either a homogeneous mixed source of different <span class="hlt">mantle</span> components or a near-primitive less-<span class="hlt">differentiated</span> <span class="hlt">mantle</span> source. The melt inclusions display ratios of highly incompatible elements (e.g., Th/La, Nb/La) which are similar to primitive <span class="hlt">mantle</span> values, and lower Nb/U ratios compared to most oceanic basalts. These results and previous isotopic and trace element data suggest that La Réunion plume samples a source which is intermediate between a primitive-like <span class="hlt">mantle</span> domain and a slightly depleted one almost unaffected by the recycling processes. This source could have originated from <span class="hlt">early</span> depletion of the primitive <span class="hlt">mantle</span>. Assuming a depletion 4.45 Gyr ago, 10% melting of this slightly depleted source could explain the enriched trace element concentrations of the melt inclusions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130010073','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130010073"><span>Modelling of Equilibrium Between <span class="hlt">Mantle</span> and Core: Refractory, Volatile, and Highly Siderophile Elements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Righter, K.; Danielson, L.; Pando, K.; Shofner, G.; Lee, C. -T.</p> <p>2013-01-01</p> <p>Siderophile elements have been used to constrain conditions of core formation and <span class="hlt">differentiation</span> for the Earth, Mars and other <span class="hlt">differentiated</span> bodies [1]. Recent models for the Earth have concluded that the <span class="hlt">mantle</span> and core did not fully equilibrate and the siderophile element contents of the <span class="hlt">mantle</span> can only be explained under conditions where the oxygen fugacity changes from low to high during accretion and the <span class="hlt">mantle</span> and core do not fully equilibrate [2,3]. However these conclusions go against several physical and chemical constraints. First, calculations suggest that even with the composition of accreting material changing from reduced to oxidized over time, the fO2 defined by metal-silicate equilibrium does not change substantially, only by approximately 1 logfO2 unit [4]. An increase of more than 2 logfO2 units in <span class="hlt">mantle</span> oxidation are required in models of [2,3]. Secondly, calculations also show that metallic impacting material will become deformed and sheared during accretion to a large body, such that it becomes emulsified to a fine scale that allows equilibrium at nearly all conditions except for possibly the length scale for giant impacts [5] (contrary to conclusions of [6]). Using new data for D(Mo) metal/silicate at high pressures, together with updated partitioning expressions for many other elements, we will show that metal-silicate equilibrium across a long span of Earth s accretion history may explain the concentrations of many siderophile elements in Earth's <span class="hlt">mantle</span>. The modeling includes refractory elements Ni, Co, Mo, and W, as well as highly siderophile elements Au, Pd and Pt, and volatile elements Cd, In, Bi, Sb, Ge and As.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18823398','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18823398"><span>Quantifying potential recharge in <span class="hlt">mantled</span> sinkholes using ERT.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schwartz, Benjamin F; Schreiber, Madeline E</p> <p>2009-01-01</p> <p>Potential recharge through thick soils in <span class="hlt">mantled</span> sinkholes was quantified using <span class="hlt">differential</span> electrical resistivity tomography (ERT). Conversion of time series two-dimensional (2D) ERT profiles into 2D volumetric water content profiles using a numerically optimized form of Archie's law allowed us to monitor temporal changes in water content in soil profiles up to 9 m in depth. Combining Penman-Monteith daily potential evapotranspiration (PET) and daily precipitation data with potential recharge calculations for three sinkhole transects indicates that potential recharge occurred only during brief intervals over the study period and ranged from 19% to 31% of cumulative precipitation. Spatial analysis of ERT-derived water content showed that infiltration occurred both on sinkhole flanks and in sinkhole bottoms. Results also demonstrate that <span class="hlt">mantled</span> sinkholes can act as regions of both rapid and slow recharge. Rapid recharge is likely the result of flow through macropores (such as root casts and thin gravel layers), while slow recharge is the result of unsaturated flow through fine-grained sediments. In addition to developing a new method for quantifying potential recharge at the field scale in unsaturated conditions, we show that <span class="hlt">mantled</span> sinkholes are an important component of storage in a karst system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17..748K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17..748K"><span>Metasomatic processes in the <span class="hlt">mantle</span> beneath the Arkhangelsk province, Russia: evidence from garnet in <span class="hlt">mantle</span> peridotite xenoliths, Grib pipe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kargin, Alexei; Sazonova, Lyudmila; Nosova, Anna; Kovalchuk, Elena; Minevrina, Elena</p> <p>2015-04-01</p> <p>The Arkhangelsk province is located in the northern East European Craton and includes more than 80 bodies of kimberlite, alkaline picrite and other ultramafic and mafic rocks. They erupted through the Archean-<span class="hlt">Early</span> Proterozoic basement into the Riphean-Paleozoic sedimentary cover. The Grib kimberlite pipe is located in the central part of the Arkhangelsk province in the Verkhotina (Chernoozerskoe) kimberlite field. The age of the Grib kimberlite is 376+-3 Ma (Rb-Sr by phlogopite). The Grib kimberlite pipe is the moderate-Ti kimberlites (TiO2 1-2 wt %) with strongly fractionated REE pattern , (La/Yb)n = 38-87. The Nd isotopic composition of the Grib pipe ranges epsilon Nd from -0.4 to + 1.0 and 87Sr/86Sr(t) from 0.7042 to 0.7069 (Kononova et al., 2006). Geochemical (Jeol JXA-8200 electron microprobe; SIMS; LA-ICP-MS) composition of clinopyroxene and garnet from <span class="hlt">mantle</span>-derived xenoliths of the Grib kimberlite pipe was studied to provide new insights into metasomatic processes in the <span class="hlt">mantle</span> beneath the Arkhangelsk province. Based on both major and trace element data, five geochemical groups of peridotitic garnet were distinguished. The partial melting of metasomatic peridotite with crystallization of a garnet-clinopyroxene association, and orthopyroxene assimilation by protokimberlitic melts was simulated and a model of garnet and clinopyroxene metasomatic origin was proposed. The model includes three stages: 1. <span class="hlt">Mantle</span> peridotite was fertilized by subduction-derived sediment partial melts/fluids at the lithosphere-asthenosphere boundary to yield a CO2-bearing <span class="hlt">mantle</span> peridotite (source I). 2. The partial melting of the carbonate-bearing <span class="hlt">mantle</span> source 1 produced carbonatite-like melts (a degree of partial melting was 1,5 %), which could form the carbonatite-kimberlite rocks of the Mela River (Arkhangelsk province, 50 km North-West of Grib kimberlite) and also produce the metasomatic reworking of (carbonate-bearing) <span class="hlt">mantle</span> peridotite (<span class="hlt">mantle</span> source II) and form type-1</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2007/1047/srp/srp039/of2007-1047srp039.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2007/1047/srp/srp039/of2007-1047srp039.pdf"><span><span class="hlt">Early</span> Precambrian <span class="hlt">mantle</span> derived rocks in the southern Prince Charles Mountains, East Antarctica: age and isotopic constraints</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Mikhalsky, E.V.; Henjes-Kunst, F.; Roland, N.W.</p> <p>2007-01-01</p> <p>Mafic and ultramafic rocks occurring as lenses, boudins, and tectonic slabs within metamorphic units in the southern Mawson Escarpment display <span class="hlt">mantle</span> characteristics of either a highly enriched, or highly depleted nature. Fractionation of these <span class="hlt">mantle</span> rocks from their sources may be as old as Eoarchaean (ca 3850 Ma) while their tectonic emplacement probably occurred prior to 2550 Ma (U-Pb SHRIMP data). These results provide for the first time evidence for Archaean suturing within East Antarctica. Similar upper <span class="hlt">mantle</span> sources are likely present in the northern Mawson Escarpment. A younger age limit of these rocks is 2200 Ma, as indicated by presumably metamorphic zircon ages while their magmatic age may be constrained by single zircon dates at 2450-2250 Ma. The area of the northern Mawson Escarpment is most likely of ensimatic origin and includes mafic rocks which were derived from distinct <span class="hlt">mantle</span> source(s) during Palaeoproterozoic time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.468..119W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.468..119W"><span>A nonmagnetic <span class="hlt">differentiated</span> <span class="hlt">early</span> planetary body</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weiss, Benjamin P.; Wang, Huapei; Sharp, Thomas G.; Gattacceca, Jérôme; Shuster, David L.; Downey, Brynna; Hu, Jinping; Fu, Roger R.; Kuan, Aaron T.; Suavet, Clément; Irving, Anthony J.; Wang, Jun; Wang, Jiajun</p> <p>2017-06-01</p> <p>Paleomagnetic studies of meteorites have shown that the solar nebula was likely magnetized and that many <span class="hlt">early</span> planetary bodies generated dynamo magnetic fields in their advecting metallic cores. The surface fields on these bodies were recorded by a diversity of chondrites and achondrites, ranging in intensity from several μT to several hundred μT. In fact, an achondrite parent body without evidence for paleomagnetic fields has yet to be confidently identified, hinting that <span class="hlt">early</span> solar system field generation and the dynamo process in particular may have been common. Here we present paleomagnetic measurements of the ungrouped achondrite NWA 7325 indicating that it last cooled in a near-zero field (<∼1.7 μT), estimated to have occurred at 4563.09 ± 0.26 million years ago (Ma) from Al-Mg chronometry. Because NWA 7325 is highly depleted in siderophile elements, its parent body nevertheless underwent large-scale metal-silicate <span class="hlt">differentiation</span> and likely formed a metallic core. This makes NWA 7325 the first recognized example of an essentially unmagnetized igneous rock from a <span class="hlt">differentiated</span> <span class="hlt">early</span> solar system body. These results indicate that all magnetic fields, including those from any core dynamo on the NWA 7325 parent body, the solar nebula, young Sun, and solar wind, were <1.7 μT at the location of NWA 7325 at 4563 Ma. This supports a recent conclusion that the solar nebula had dissipated by ∼4 million years after solar system formation. NWA 7325 also serves as an experimental control that gives greater confidence in the positive identification of remanent magnetization in other achondrites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860013631','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860013631"><span>Komatiite genesis in the Archaean <span class="hlt">mantle</span>, with implications for the tectonics of Archaean greenstone belts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Elthon, D.</p> <p>1986-01-01</p> <p>The presence of ultramafic lavas (komatiites) associated with Archean greenstone belts has been suggested to indicate very high increments (50-80%) of partial melting of the Archean <span class="hlt">mantle</span>. Such extensive melting of the Earth's <span class="hlt">mantle</span> during the Archean might have profound effects on the <span class="hlt">early</span> tectonic and chemical evolution of the planet, although problems associated with keeping the komatiite liquid in equilibrium with the residual <span class="hlt">mantle</span> at such high increments of melting has cast doubt upon aspects of extensive melting. Two important aspects of the origin of komatiites are discussed below.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3918783','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3918783"><span>Inhibition of master transcription factors in pluripotent cells induces <span class="hlt">early</span> stage <span class="hlt">differentiation</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>De, Debojyoti; Jeong, Myong-Ho; Leem, Young-Eun; Svergun, Dmitri I.; Wemmer, David E.; Kang, Jong-Sun; Kim, Kyeong Kyu; Kim, Sung-Hou</p> <p>2014-01-01</p> <p>The potential for pluripotent cells to <span class="hlt">differentiate</span> into diverse specialized cell types has given much hope to the field of regenerative medicine. Nevertheless, the low efficiency of cell commitment has been a major bottleneck in this field. Here we provide a strategy to enhance the efficiency of <span class="hlt">early</span> <span class="hlt">differentiation</span> of pluripotent cells. We hypothesized that the initial phase of <span class="hlt">differentiation</span> can be enhanced if the transcriptional activity of master regulators of stemness is suppressed, blocking the formation of functional transcriptomes. However, an obstacle is the lack of an efficient strategy to block protein–protein interactions. In this work, we take advantage of the biochemical property of seventeen kilodalton protein (Skp), a bacterial molecular chaperone that binds directly to sex determining region Y-box 2 (Sox2). The small angle X-ray scattering analyses provided a low resolution model of the complex and suggested that the transactivation domain of Sox2 is probably wrapped in a cleft on Skp trimer. Upon the transduction of Skp into pluripotent cells, the transcriptional activity of Sox2 was inhibited and the expression of Sox2 and octamer-binding transcription factor 4 was reduced, which resulted in the expression of <span class="hlt">early</span> <span class="hlt">differentiation</span> markers and appearance of <span class="hlt">early</span> neuronal and cardiac progenitors. These results suggest that the initial stage of <span class="hlt">differentiation</span> can be accelerated by inhibiting master transcription factors of stemness. This strategy can possibly be applied to increase the efficiency of stem cell <span class="hlt">differentiation</span> into various cell types and also provides a clue to understanding the mechanism of <span class="hlt">early</span> <span class="hlt">differentiation</span>. PMID:24434556</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014E%26PSL.394..186M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014E%26PSL.394..186M"><span>How Mercury can be the most reduced terrestrial planet and still store iron in its <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Malavergne, Valérie; Cordier, Patrick; Righter, Kevin; Brunet, Fabrice; Zanda, Brigitte; Addad, Ahmed; Smith, Thomas; Bureau, Hélène; Surblé, Suzy; Raepsaet, Caroline; Charon, Emeline; Hewins, Roger H.</p> <p>2014-05-01</p> <p>Mercury is notorious as the most reduced planet with the highest metal/silicate ratio, yet paradoxically data from the MESSENGER spacecraft show that its iron-poor crust is high in sulfur (up to ˜6 wt%, ˜80× Earth crust abundance) present mainly as Ca-rich sulfides on its surface. These particularities are simply impossible on the other terrestrial planets. In order to understand the role played by sulfur during the formation of Mercury, we investigated the phase relationships in Mercurian analogs of enstatite chondrite-like composition experimentally under conditions relevant to <span class="hlt">differentiation</span> of Mercury (˜1 GPa and 1300-2000 °C). Our results show that Mg-rich and Ca-rich sulfides, which both contain Fe, crystallize successively from reduced silicate melts upon cooling below 1550 °C. As the iron concentration in the reduced silicates stays very low (≪1 wt%), these sulfides represent new host phases for both iron and sulfur in the run products. Extrapolated to Mercury, these results show that Mg-rich sulfide crystallization provides the first viable and fundamental means for retaining iron as well as sulfur in the <span class="hlt">mantle</span> during <span class="hlt">differentiation</span>, while sulfides richer in Ca would crystallize at shallower levels. The distribution of iron in the <span class="hlt">differentiating</span> <span class="hlt">mantle</span> of Mercury was mainly determined by its partitioning between metal (or troilite) and Mg-Fe-Ca-rich sulfides rather than by its partitioning between metal (or troilite) and silicates. Moreover, the primitive <span class="hlt">mantle</span> might also be boosted in Fe by a reaction at the core <span class="hlt">mantle</span> boundary (CMB) between Mg-rich sulfides of the <span class="hlt">mantle</span> and FeS-rich outer core materials to produce (Fe, Mg)S. The stability of Mg-Fe-Ca-rich sulfides over a large range of depths up to the surface of Mercury would be consistent with sulfur, calcium and iron abundances measured by MESSENGER.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeCoA.195..142K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeCoA.195..142K"><span>Open system models of isotopic evolution in Earth's silicate reservoirs: Implications for crustal growth and <span class="hlt">mantle</span> heterogeneity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumari, Seema; Paul, Debajyoti; Stracke, Andreas</p> <p>2016-12-01</p> <p>An open system evolutionary model of the Earth, comprising continental crust (CC), upper and lower <span class="hlt">mantle</span> (UM, LM), and an additional isolated reservoir (IR) has been developed to study the isotopic evolution of the silicate Earth. The model is solved numerically at 1 Myr time steps over 4.55 Gyr of Earth history to reproduce both the present-day concentrations and isotope ratios of key radioactive decay systems (Rb-Sr, Sm-Nd, and U-Th-Pb) in these terrestrial reservoirs. Various crustal growth scenarios - continuous versus episodic and <span class="hlt">early</span> versus late crustal growth - and their effect on the evolution of Sr-Nd-Pb isotope systematics in the silicate reservoirs have been evaluated. Modeling results where the present-day UM is ∼60% of the total <span class="hlt">mantle</span> mass and a lower <span class="hlt">mantle</span> that is non-primitive reproduce the estimated geochemical composition and isotope ratios in Earth's silicate reservoirs. The isotopic evolution of the silicate Earth is strongly affected by the mode of crustal growth; only an exponential crustal growth pattern with crustal growth since the <span class="hlt">early</span> Archean satisfactorily explains the chemical and isotopic evolution of the crust-<span class="hlt">mantle</span> system and accounts for the so-called Pb paradoxes. Assuming that the OIB source is located in the deeper <span class="hlt">mantle</span>, our model could, however, not reproduce its target ɛNd of +4.6 for the UM, which has been estimated from the average isotope ratios of 32 individual ocean island localities. Hence, either <span class="hlt">mantle</span> plumes sample the LM in a non-representative way, or the simplified model set-up does not capture the full complexity of Earth's lower <span class="hlt">mantle</span> (Nd isotope) evolution. Compared to the results obtained for a 4.55 Ga Earth, a model assuming a protracted U-Pb evolution of silicate Earth by ca. 100 Myr reproduces a slightly better fit for the Pb isotope ratios in Earth's silicate reservoirs. One notable feature of successful models is the <span class="hlt">early</span> depletion of incompatible elements (as well as rapid decrease in Th/U) in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012CoMP..163..189T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012CoMP..163..189T"><span>Cumulate xenoliths from St. Vincent, Lesser Antilles Island Arc: a window into upper crustal <span class="hlt">differentiation</span> of <span class="hlt">mantle</span>-derived basalts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tollan, P. M. E.; Bindeman, I.; Blundy, J. D.</p> <p>2012-02-01</p> <p>In order to shed light on upper crustal <span class="hlt">differentiation</span> of <span class="hlt">mantle</span>-derived basaltic magmas in a subduction zone setting, we have determined the mineral chemistry and oxygen and hydrogen isotope composition of individual cumulus minerals in plutonic blocks from St. Vincent, Lesser Antilles. Plutonic rock types display great variation in mineralogy, from olivine-gabbros to troctolites and hornblendites, with a corresponding variety of cumulate textures. Mineral compositions differ from those in erupted basaltic lavas from St. Vincent and in published high-pressure (4-10 kb) experimental run products of a St. Vincent high-Mg basalt in having higher An plagioclase coexisting with lower Fo olivine. The oxygen isotope compositions (δ18O) of cumulus olivine (4.89-5.18‰), plagioclase (5.84-6.28‰), clinopyroxene (5.17-5.47‰) and hornblende (5.48-5.61‰) and hydrogen isotope composition of hornblende (δD = -35.5 to -49.9‰) are all consistent with closed system magmatic <span class="hlt">differentiation</span> of a <span class="hlt">mantle</span>-derived basaltic melt. We employed a number of modelling exercises to constrain the origin of the chemical and isotopic compositions reported. δ18OOlivine is up to 0.2‰ higher than modelled values for closed system fractional crystallisation of a primary melt. We attribute this to isotopic disequilibria between cumulus minerals crystallising at different temperatures, with equilibration retarded by slow oxygen diffusion in olivine during prolonged crustal storage. We used melt inclusion and plagioclase compositions to determine parental magmatic water contents (water saturated, 4.6 ± 0.5 wt% H2O) and crystallisation pressures (173 ± 50 MPa). Applying these values to previously reported basaltic and basaltic andesite lava compositions, we can reproduce the cumulus plagioclase and olivine compositions and their associated trend. We conclude that <span class="hlt">differentiation</span> of primitive hydrous basalts on St. Vincent involves crystallisation of olivine and Cr-rich spinel at depth</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014E%26PSL.389..143S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014E%26PSL.389..143S"><span><span class="hlt">Mantle</span> eclogites and garnet pyroxenites - the meaning of two-point isochrons, Sm-Nd and Lu-Hf closure temperatures and the cooling of the subcratonic <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shu, Qiao; Brey, Gerhard P.; Gerdes, Axel; Hoefer, Heidi E.</p> <p>2014-03-01</p> <p>The Earth's <span class="hlt">mantle</span> is a huge metamorphic complex which undergoes permanent changes ruled by plate tectonics. It also has enclaves underneath Archean crust which are exempt from the convecting <span class="hlt">mantle</span> since at least 2.5 Ga. Since then, this <span class="hlt">mantle</span> may cool slowly as a result of diminishing heat input from the asthenosphere, of declining heat production from radioactive decay and of denudation of the crust. Under such circumstances, two point garnet-clinopyroxene isochrons from <span class="hlt">mantle</span> xenoliths (here garnet pyroxenites and eclogites) reflect either cooling ages or eruption ages depending on whether the <span class="hlt">mantle</span> portion under consideration was below or above the closure temperature of a radiogenic system. Available literature data from the Slave and Kaapvaal craton for the Sm-Nd and Lu-Hf isotope systems and our own new data from Bellsbank (Kaapvaal) provide a whole range of two-point isochron ages from younger than the kimberlite eruption age to <span class="hlt">early</span> Proterozoic. The meaning of ages other than the kimberlite eruption age is unclear. We use here a compilation of Sm-Nd and Lu-Hf two-point isochron age data from this study and the literature, to assess the meaning of such isochrons. This is achieved by plotting the temperature of last equilibration as derived from the Fe-Mg exchange between garnet and clinopyroxene versus the two-point isochron age. There is a low temperature alignment for both systems of increasing age with decreasing temperature and an alignment around the kimberlite eruption ages at high temperatures. We interpret the intersect between the low temperature limb and the kimberlite eruption age as closure temperature which gives about 920 °C for the Lu-Hf system and about 850 °C for the Sm-Nd system. The differences of the cooling ages between the two isotope systems for individual samples combined with the closure temperatures from this study are used to deduce the cooling of the Slave and Kaapvaal subcratonic <span class="hlt">mantle</span> from the <span class="hlt">early</span> Proterozoic until</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ESRv..129...85S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ESRv..129...85S"><span>Formation of plate boundaries: The role of <span class="hlt">mantle</span> volatilization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seno, Tetsuzo; Kirby, Stephen H.</p> <p>2014-02-01</p> <p>In the <span class="hlt">early</span> Earth, convection occurred with the accumulation of thick crust over a weak boundary layer downwelling into the <span class="hlt">mantle</span> (Davies, G.F., 1992. On the emergence of plate tectonics. Geology 20, 963-966.). This would have transitioned to stagnant-lid convection as the <span class="hlt">mantle</span> cooled (Solomatov, V.S., Moresi, L.-N., 1997. Three regimes of <span class="hlt">mantle</span> convection with non-Newtonian viscosity and stagnant lid convection on the terrestrial planets. Geophys. Res. Lett. 24, 1907-1910.) or back to a magma ocean as the <span class="hlt">mantle</span> heated (Sleep, N., 2000. Evolution of the mode of convection within terrestrial planets. J. Geophys. Res. 105(E7): 17563-17578). Because plate tectonics began operating on the Earth, subduction must have been initiated, thus avoiding these shifts. Based on an analogy with the continental crust subducted beneath Hindu Kush and Burma, we propose that the lithosphere was hydrated and/or carbonated by H2O-CO2 vapors released from magmas generated in upwelling plumes and subsequently volatilized during underthrusting, resulting in lubrication of the thrust above, and subduction of the lithosphere along with the overlying thick crust. Once subduction had been initiated, serpentinized forearc <span class="hlt">mantle</span> may have formed in a wedge-shaped body above a dehydrating slab. In relict arcs, suture zones, or rifted margins, any agent that warms and dehydrates the wedge would weaken the region surrounding it, and form various types of plate boundaries depending on the operating tectonic stress. Thus, once subduction is initiated, formation of plate boundaries might be facilitated by a major fundamental process: weakening due to the release of pressurized water from the warming serpentinized forearc <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.2165K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.2165K"><span>Modeling crust-<span class="hlt">mantle</span> evolution using radiogenic Sr, Nd, and Pb isotope systematics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumari, Seema; Paul, Debajyoti</p> <p>2015-04-01</p> <p>The present-day elemental and isotopic composition of Earth's terrestrial reservoirs can be used as geochemical constraints to study evolution of the crust-<span class="hlt">mantle</span> system. A flexible open system evolutionary model of the Earth, comprising continental crust (CC), upper depleted <span class="hlt">mantle</span> (UM) -source of mid-ocean ridge basalts (MORB), and lower <span class="hlt">mantle</span> (LM) reservoir with a D" layer -source of ocean island basalts (OIB), and incorporating key radioactive isotope systematics (Rb-Sr, Sm-Nd, and U-Th-Pb), is solved numerically at 1 Ma time step for 4.55 Ga, the age of the Earth. The best possible solution is the one that produces the present-day concentrations as well as isotopic ratios in terrestrial reservoirs, compiled from published data. Different crustal growth scenarios (exponential, episodic, <span class="hlt">early</span> and late growth), proposed in earlier studies, and its effect on the evolution of isotope systematics of terrestrial reservoirs is studied. Model simulations strongly favor a layered <span class="hlt">mantle</span> structure satisfying majority of the isotopic constraints. In the successful model, which is similar to that proposed by Kellogg et al. (1999), the present-day UM comprises of 60% of <span class="hlt">mantle</span> mass and extends to a depth 1600 km, whereas the LM becomes non-primitive and more enriched than the bulk silicate Earth, mainly due to addition of recycled crustal material. Modeling suggest that isotopic evolution of reservoirs is affected by the mode of crustal growth. Only two scenarios satisfied majority of the Rb-Sr and Sm-Nd isotopic constraints but failed to reproduce the present-day Pb-isotope systematics; exponential growth of crust (mean age, tc=2.3 Ga) and delayed and episodic growth (no growth for initial 900 Ma, tc=2.05 Ga) proposed by Patchett and Arndt (1986). However, assuming a slightly young Earth (4.45 Ga) better satisfies the Pb-isotope systematics. Although, the delayed crustal growth model satisfied Sr-Nd isotopic constraints, presence of <span class="hlt">early</span> Hadean crust (4.03 and 4.4 Ga</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70024690','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70024690"><span>Seismic evidence for a tilted <span class="hlt">mantle</span> plume and north-south <span class="hlt">mantle</span> flow beneath Iceland</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Shen, Y.; Solomon, S.C.; Bjarnason, I. Th; Nolet, G.; Morgan, W.J.; Allen, R.M.; Vogfjord, K.; Jakobsdottir, S.; Stefansson, R.; Julian, B.R.; Foulger, G.R.</p> <p>2002-01-01</p> <p>Shear waves converted from compressional waves at <span class="hlt">mantle</span> discontinuities near 410- and 660-km depth recorded by two broadband seismic experiments in Iceland reveal that the center of an area of anomalously thin <span class="hlt">mantle</span> transition zone lies at least 100 km south of the upper-<span class="hlt">mantle</span> low-velocity anomaly imaged tomographically beneath the hotspot. This offset is evidence for a tilted plume conduit in the upper <span class="hlt">mantle</span>, the result of either northward flow of the Icelandic asthenosphere or southward flow of the upper part of the lower <span class="hlt">mantle</span> in a no-net-rotation reference frame. ?? 2002 Elsevier Science B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Litho.308..262E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Litho.308..262E"><span>The <span class="hlt">mantle</span> source of island arc magmatism during <span class="hlt">early</span> subduction: Evidence from Hf isotopes in rutile from the Jijal Complex (Kohistan arc, Pakistan)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ewing, Tanya A.; Müntener, Othmar</p> <p>2018-05-01</p> <p>The Cretaceous-Paleogene Kohistan arc complex, northern Pakistan, is renowned as one of the most complete sections through a preserved paleo-island arc. The Jijal Complex represents a fragment of the plutonic roots of the Kohistan arc, formed during its <span class="hlt">early</span> intraoceanic history. We present the first Hf isotope determinations for the Jijal Complex, made on rutile from garnet gabbros. These lithologies are zircon-free, but contain rutile that formed as an <span class="hlt">early</span> phase. Recent developments in analytical capabilities coupled with a careful analytical and data reduction protocol allow the accurate determination of Hf isotope composition for rutile with <30 ppm Hf for the first time. Rutile from the analysed samples contains 5-35 ppm Hf, with sample averages of 13-17 ppm. Rutile from five samples from the Jijal Complex mafic section, sampling 2 km of former crustal thickness, gave indistinguishable Hf isotope compositions with εHf(i) ranging from 11.4 ± 3.2 to 20.1 ± 5.7. These values are within error of or only slightly more enriched than modern depleted <span class="hlt">mantle</span>. The analysed samples record variable degrees of interaction with late-stage melt segregations, which produced symplectitic overprints on the main mineral assemblage as well as pegmatitic segregations of hydrous minerals. The indistinguishable εHf(i) across this range of lithologies demonstrates the robust preservation of the Hf isotope composition of rutile. The Hf isotope data, combined with previously published Nd isotope data for the Jijal Complex garnet gabbros, favour derivation from an inherently enriched, Indian Ocean type <span class="hlt">mantle</span>. This implies a smaller contribution from subducted sediments than if the source was a normal (Pacific-type) depleted <span class="hlt">mantle</span>. The Jijal Complex thus had only a limited recycled continental crustal component in its source, and represents a largely juvenile addition of new continental crust during the <span class="hlt">early</span> phases of intraoceanic magmatism. The ability to determine the Hf</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P51A2577J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P51A2577J"><span>Self-Consistent Generation of Primordial Continental Crust in Global <span class="hlt">Mantle</span> Convection Models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jain, C.; Rozel, A.; Tackley, P. J.</p> <p>2017-12-01</p> <p>We present the generation of primordial continental crust (TTG rocks) using self-consistent and evolutionary thermochemical <span class="hlt">mantle</span> convection models (Tackley, PEPI 2008). Numerical modelling commonly shows that <span class="hlt">mantle</span> convection and continents have strong feedbacks on each other. However in most studies, continents are inserted a priori while basaltic (oceanic) crust is generated self-consistently in some models (Lourenco et al., EPSL 2016). Formation of primordial continental crust happened by fractional melting and crystallisation in episodes of relatively rapid growth from late Archean to late Proterozoic eras (3-1 Ga) (Hawkesworth & Kemp, Nature 2006) and it has also been linked to the onset of plate tectonics around 3 Ga. It takes several stages of <span class="hlt">differentiation</span> to generate Tonalite-Trondhjemite-Granodiorite (TTG) rocks or proto-continents. First, the basaltic magma is extracted from the pyrolitic <span class="hlt">mantle</span> which is both erupted at the surface and intruded at the base of the crust. Second, it goes through eclogitic transformation and then partially melts to form TTGs (Rudnick, Nature 1995; Herzberg & Rudnick, Lithos 2012). TTGs account for the majority of the Archean continental crust. Based on the melting conditions proposed by Moyen (Lithos 2011), the feasibility of generating TTG rocks in numerical simulations has already been demonstrated by Rozel et al. (Nature, 2017). Here, we have developed the code further by parameterising TTG formation. We vary the ratio of intrusive (plutonic) and extrusive (volcanic) magmatism (Crisp, Volcanol. Geotherm. 1984) to study the relative volumes of three petrological TTG compositions as reported from field data (Moyen, Lithos 2011). Furthermore, we systematically vary parameters such as friction coefficient, initial core temperature and composition-dependent viscosity to investigate the global tectonic regime of <span class="hlt">early</span> Earth. Continental crust can also be destroyed by subduction or delamination. We will investigate</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27389974','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27389974"><span>Long-term outcome for patients with <span class="hlt">early</span> stage marginal zone lymphoma and <span class="hlt">mantle</span> cell lymphoma.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barzenje, Dlawer Abdulla; Holte, Harald; Fosså, Alexander; Ghanima, Waleed; Liestøl, Knut; Delabie, Jan; Kolstad, Arne</p> <p>2017-03-01</p> <p>In this study with prolonged follow up, we compared clinical outcome, including cause of death and incidence of second cancer, for patients with <span class="hlt">early</span> stage extranodal marginal zone lymphoma (EMZL, 49 patients), nodal marginal zone lymphoma (NMZL, nine patients) and <span class="hlt">mantle</span> cell lymphoma (MCL, 42 patients) with emphasis on potential benefit of radiotherapy. Radiotherapy was given to 40 patients with EMZL (nine had surgery only) and all NMZL patients. MCL patients received radiotherapy (17 patients), chemotherapy followed by radiotherapy (13 patients) or chemotherapy alone (12 patients). Compared to a matched control population no increased risk of second cancer or cardiovascular disease was observed. Radiotherapy alone was effective in EMZL and NMZL with low-relapse rates (20% and 33%) and a 10-year overall survival of 78% and 56%, respectively. High-relapse rate and inferior OS in MCL underline the need for extended staging with endoscopy and PET/CT and possibly for novel strategies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4199955','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4199955"><span>Role for <span class="hlt">early-differentiated</span> natural killer cells in infectious mononucleosis</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Azzi, Tarik; Lünemann, Anna; Murer, Anita; Ueda, Seigo; Béziat, Vivien; Malmberg, Karl-Johan; Staubli, Georg; Gysin, Claudine; Berger, Christoph; Münz, Christian</p> <p>2014-01-01</p> <p>A growing body of evidence suggests that the human natural killer (NK)-cell compartment is phenotypically and functionally heterogeneous and is composed of several <span class="hlt">differentiation</span> stages. Moreover, NK-cell subsets have been shown to exhibit adaptive immune features during herpes virus infection in experimental mice and to expand preferentially during viral infections in humans. However, both phenotype and role of NK cells during acute symptomatic Epstein-Barr virus (EBV) infection, termed infectious mononucleosis (IM), remain unclear. Here, we longitudinally assessed the kinetics, the <span class="hlt">differentiation</span>, and the proliferation of subsets of NK cells in pediatric IM patients. Our results indicate that acute IM is characterized by the preferential proliferation of <span class="hlt">early-differentiated</span> CD56dim NKG2A+ immunoglobulin-like receptor- NK cells. Moreover, this NK-cell subset exhibits features of terminal <span class="hlt">differentiation</span> and persists at higher frequency during at least the first 6 months after acute IM. Finally, we demonstrate that this NK-cell subset preferentially degranulates and proliferates on exposure to EBV-infected B cells expressing lytic antigens. Thus, <span class="hlt">early-differentiated</span> NK cells might play a key role in the immune control of primary infection with this persistent tumor-associated virus. PMID:25205117</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V52B..03M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V52B..03M"><span>Fe3+ partitioning during basalt <span class="hlt">differentiation</span> on Mars: insights into the oxygen fugacity of the shergottite <span class="hlt">mantle</span> source(s).</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Medard, E.; Martin, A. M.; Collinet, M.; Righter, K.; Grove, T. L.; Newville, M.; Lanzirotti, A.</p> <p>2014-12-01</p> <p>The partitioning of Fe3+ between silicate melts and minerals is a key parameter to understand magmatic processes, as it is directly linked to oxygen fugacity (fO2). fO2 is, a priori, not a constant during magmatic processes, and its evolution depends on the compatibility of Fe3+. We have experimentally determined the partition coefficients of Fe3+ between augite, pigeonite, and silicate melt, and use them to constrain the fO2of the martian <span class="hlt">mantle</span> and of <span class="hlt">differentiated</span> martian basalts. A series of experiments on various martian basaltic compositions were performed under controlled fO2 in one-atmosphere gas-mixing furnaces. Fe3+/Fetotal ratios in silicate melts and pyroxenes were determined using synchrotron Fe K-edge XANES on the 13 IDE beamline at APS (Argonne). Fe3+ mineral/melt partition coefficients (DFe3+) for augite and pigeonite were obtained with a relative uncertainty of 10-15 %. Both are constant over a wide range of oxygen fugacity (FMQ-2.5 to FMQ+2.0). DFe3+ for augite and pigeonite are broadly consistent with previous data by [1], but DFe3+ for augite is significantly higher (by a factor of 2) than the indirect determinations of [2]. Since augites in [2] are extremely poor in iron compared to ours (0.18 wt% vs 13 wt% FeO), this strongly suggests that DFe3+ varies with Mg#, indicating that Fe3+is more compatible than previously thought in terrestrial <span class="hlt">mantle</span> pyroxenes (3 wt% FeO) as well. Crystallization paths for shergottite parental melts have been calculated using the MELTS software, combined with our partition coefficients. fO2 in the residual melts is calculated from the models of [3] and [4]. It stays relatively constant at high temperatures, but increases very strongly during the latest stages of crystallization. These results explain the large range of fO2 determined in enriched shergottites. In order to estimate the fO2 of the martian <span class="hlt">mantle</span>, only the highest temperature phases in the most primitive martian samples should be used. The most</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1436247-nonmagnetic-differentiated-early-planetary-body','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1436247-nonmagnetic-differentiated-early-planetary-body"><span>A nonmagnetic <span class="hlt">differentiated</span> <span class="hlt">early</span> planetary body</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Weiss, Benjamin P.; Wang, Huapei; Sharp, Thomas G.; ...</p> <p>2017-06-19</p> <p>Paleomagnetic studies of meteorites have shown that the solar nebula was likely magnetized and that many <span class="hlt">early</span> planetary bodies generated dynamo magnetic fields in their advecting metallic cores. The surface fields on these bodies were recorded by a diversity of chondrites and achondrites, ranging in intensity from several μT to several hundred μT. In fact, an achondrite parent body without evidence for paleomagnetic fields has yet to be confidently identified, hinting that <span class="hlt">early</span> solar system field generation and the dynamo process in particular may have been common. Here we present paleomagnetic measurements of the ungrouped achondrite NWA 7325 indicating thatmore » it last cooled in a near-zero field (<~1.7μT), estimated to have occurred at 4563.09 ± 0.26 million years ago (Ma) from Al–Mg chronometry. Because NWA 7325 is highly depleted in siderophile elements, its parent body nevertheless underwent large-scale metal-silicate <span class="hlt">differentiation</span> and likely formed a metallic core. This makes NWA 7325 the first recognized example of an essentially unmagnetized igneous rock from a <span class="hlt">differentiated</span> <span class="hlt">early</span> solar system body. These results indicate that all magnetic fields, including those from any core dynamo on the NWA 7325 parent body, the solar nebula, young Sun, and solar wind, were <1.7 μT at the location of NWA 7325 at 4563 Ma. Finally, this supports a recent conclusion that the solar nebula had dissipated by ~4 million years after solar system formation. NWA 7325 also serves as an experimental control that gives greater confidence in the positive identification of remanent magnetization in other achondrites.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1396590-nonmagnetic-differentiated-early-planetary-body','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1396590-nonmagnetic-differentiated-early-planetary-body"><span>A Nonmagnetic <span class="hlt">Differentiated</span> <span class="hlt">Early</span> Planetary Body</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Weiss, Benjamin P.; Wang, Jun</p> <p>2017-06-15</p> <p>Paleomagnetic studies of meteorites have shown that the solar nebula was likely magnetized and that many <span class="hlt">early</span> planetary bodies generated dynamo magnetic fields in their advecting metallic cores. The surface fields on these bodies were recorded by a diversity of chondrites and achondrites, ranging in intensity from several μT to several hundred μT. In fact, an achondrite parent body without evidence for paleomagnetic fields has yet to be confidently identified, hinting that <span class="hlt">early</span> solar system field generation and the dynamo process in particular may have been common. Here we present paleomagnetic measurements of the ungrouped achondrite NWA 7325 indicating thatmore » it last cooled in a near-zero field (<∼1.7μT), estimated to have occurred at 4563.09 ± 0.26 million years ago (Ma) from Al–Mg chronometry. Because NWA 7325 is highly depleted in siderophile elements, its parent body nevertheless underwent large-scale metal-silicate <span class="hlt">differentiation</span> and likely formed a metallic core. This makes NWA 7325 the first recognized example of an essentially unmagnetized igneous rock from a <span class="hlt">differentiated</span> <span class="hlt">early</span> solar system body. These results indicate that all magnetic fields, including those from any core dynamo on the NWA 7325 parent body, the solar nebula, young Sun, and solar wind, were <1.7 μT at the location of NWA 7325 at 4563 Ma. This supports a recent conclusion that the solar nebula had dissipated by ∼4 million years after solar system formation. NWA 7325 also serves as an experimental control that gives greater confidence in the positive identification of remanent magnetization in other achondrites.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12460472','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12460472"><span>Osmium isotopes and <span class="hlt">mantle</span> convection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hauri, Erik H</p> <p>2002-11-15</p> <p>The decay of (187)Re to (187)Os (with a half-life of 42 billion years) provides a unique isotopic fingerprint for tracing the evolution of crustal materials and <span class="hlt">mantle</span> residues in the convecting <span class="hlt">mantle</span>. Ancient subcontinental <span class="hlt">mantle</span> lithosphere has uniquely low Re/Os and (187)Os/(188)Os ratios due to large-degree melt extraction, recording ancient melt-depletion events as old as 3.2 billion years. Partial melts have Re/Os ratios that are orders of magnitude higher than their sources, and the subduction of oceanic or continental crust introduces into the <span class="hlt">mantle</span> materials that rapidly accumulate radiogenic (187)Os. Eclogites from the subcontinental lithosphere have extremely high (187)Os/(188)Os ratios, and record ages as old as the oldest peridotites. The data show a near-perfect partitioning of Re/Os and (187)Os/(188)Os ratios between peridotites (low) and eclogites (high). The convecting <span class="hlt">mantle</span> retains a degree of Os-isotopic heterogeneity similar to the lithospheric <span class="hlt">mantle</span>, although its amplitude is modulated by convective mixing. Abyssal peridotites from the ocean ridges have low Os isotope ratios, indicating that the upper <span class="hlt">mantle</span> had undergone episodes of melt depletion prior to the most recent melting events to produce mid-ocean-ridge basalt. The amount of rhenium estimated to be depleted from the upper <span class="hlt">mantle</span> is 10 times greater than the rhenium budget of the continental crust, requiring a separate reservoir to close the mass balance. A reservoir consisting of 5-10% of the <span class="hlt">mantle</span> with a rhenium concentration similar to mid-ocean-ridge basalt would balance the rhenium depletion of the upper <span class="hlt">mantle</span>. This reservoir most likely consists of mafic oceanic crust recycled into the <span class="hlt">mantle</span> over Earth's history and provides the material that melts at oceanic hotspots to produce ocean-island basalts (OIBs). The ubiquity of high Os isotope ratios in OIB, coupled with other geochemical tracers, indicates that the <span class="hlt">mantle</span> sources of hotspots contain significant quantities</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR24A..03S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR24A..03S"><span>The role of thermodynamics in <span class="hlt">mantle</span> convection: is <span class="hlt">mantle</span>-layering intermittent?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stixrude, L. P.; Cagney, N.; Lithgow-Bertelloni, C. R.</p> <p>2016-12-01</p> <p>We examine the thermal evolution of the Earth using a 1D model in which mixing length theory is used to characterise the role of thermal convection. Unlike previous work, our model accounts for the complex role of thermodynamics and phase changes through the use of HeFESTo (Stixrude & Lithgow-Bertelloni, Geophys. J. Int. 184, 2011), a comprehensive thermodynamic model that enables self-consistent computation of phase equilibria, physical properties (e.g. density, thermal expansivity etc.) and <span class="hlt">mantle</span> isentropes. Our model also accounts for the freezing of the inner core, radiogenic heating and Arrhenius rheology, and is validated by comparing our results to observations, including the present-day size of the inner core and the heat flux at the surface.If phase changes and the various thermodynamic effects on <span class="hlt">mantle</span> properties are neglected, the results are weakly dependent on the initial conditions, as has been observed in several previous studies. However, when these effects are accounted for, the initial temperature profile has a strong influence on the thermal evolution of the <span class="hlt">mantle</span>, because small changes in the temperature and phase-assemblage can lead to large changes in the local physical properties and the adiabatic gradient.The inclusion of thermodynamic effects leads to some new and interesting insights. We demonstrate that the Clapeyron slope and the thermal gradient at the transition zone both vary significantly with time; this causes the <span class="hlt">mantle</span> to switch between a layered state, in which convection across the transition zone is weak or negligible, and an un-layered state, in which there is no resistance to mass transfer between the upper and lower <span class="hlt">mantles</span>.Various plume models describe plumes either rising directly from the CMB to the lithosphere, or stalling at the transition zone before spawning new plumes in the upper <span class="hlt">mantle</span>. The observance of switching behaviour indicates that both models may be applicable depending on the state of the <span class="hlt">mantle</span>: plumes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoJI.200.1155M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoJI.200.1155M"><span><span class="hlt">Mantle</span> beneath the Gibraltar Arc from receiver functions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morais, Iolanda; Vinnik, Lev; Silveira, Graça; Kiselev, Sergey; Matias, Luís</p> <p>2015-02-01</p> <p>P and S receiver functions (PRF and SRF) from 19 seismograph stations in the Gibraltar Arc and the Iberian Massif reveal new details of the regional deep structure. Within the high-velocity <span class="hlt">mantle</span> body below southern Spain the 660-km discontinuity is depressed by at least 20 km. The Ps phase from the 410-km discontinuity is missing at most stations in the Gibraltar Arc. A thin (˜50 km) low-S-velocity layer atop the 410-km discontinuity is found under the Atlantic margin. At most stations the S410p phase in the SRFs arrives 1.0-2.5 s earlier than predicted by IASP91 model, but, for the propagation paths through the upper <span class="hlt">mantle</span> below southern Spain, the arrivals of S410p are delayed by up to +1.5 s. The <span class="hlt">early</span> arrivals can be explained by elevated Vp/Vs ratio in the upper <span class="hlt">mantle</span> or by a depressed 410-km discontinuity. The positive residuals are indicative of a low (˜1.7 versus ˜ 1.8 in IASP91) Vp/Vs ratio. Previously, the low ratio was found in depleted lithosphere of Precambrian cratons. From simultaneous inversion of the PRFs and SRFs we recognize two types of the <span class="hlt">mantle</span>: `continental' and `oceanic'. In the `continental' upper <span class="hlt">mantle</span> the S-wave velocity in the high-velocity lid is 4.4-4.5 km s-1, the S-velocity contrast between the lid and the underlying <span class="hlt">mantle</span> is often near the limit of resolution (0.1 km s-1), and the bottom of the lid is at a depth reaching 90-100 km. In the `oceanic' domain, the S-wave velocities in the lid and the underlying <span class="hlt">mantle</span> are typically 4.2-4.3 and ˜ 4.0 km s-1, respectively. The bottom of the lid is at a shallow depth (around 50 km), and at some locations the lid is replaced by a low S-wave velocity layer. The narrow S-N-oriented band of earthquakes at depths from 70 to 120 km in the Alboran Sea is in the `continental' domain, near the boundary between the `continental' and `oceanic' domains, and the intermediate seismicity may be an effect of ongoing destruction of the continental lithosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P51A2578F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P51A2578F"><span>The influence of <span class="hlt">mantle</span> refertilisation on the formation of TTGs in a plume-lid tectonics setting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fischer, R.; Gerya, T.</p> <p>2017-12-01</p> <p>Higher amounts of radiogenic elements and leftover primordial heat in the <span class="hlt">early</span> Earth both contribute to the increased temperature in the Earth's interior and it is mainly this increased <span class="hlt">mantle</span> potential temperature that controls the dynamics of the crust and upper <span class="hlt">mantle</span> and the predominant style of tectonics in the <span class="hlt">Early</span> Earth. The increased upper <span class="hlt">mantle</span> temperature precludes the modern plate tectonics regime and stabilizes another type of global tectonics often called plume-lid tectonics (Fischer and Gerya, 2016) or 'plutonic squishy lid' tectonics(Rozel et al., 2017). Plume-lid tectonics is dominated by intrusive <span class="hlt">mantle</span>-derived magmatism which results in a thickening of the overlaying crust. The overthickened basaltic crust is transformed into eclogite and episodically recycled back into the <span class="hlt">mantle</span>. Melt extraction from hydrated partially molten basaltic crust leads to the production of primordial tonalite-trondhjemite-granodiorite (TTG) continental crust. TTGs make up over half of the Archean crust and can be classied into low-, medium- and high-pressure types (Moyen, 2011). Field studies show that the three different types (low-, medium- and high-pressure) appear in a ratio of 20%, 60% and 20% (Moyen, 2011). Numerical models of plume-lid tectonics generally agree very well with these values (Rozel et al., 2017) but also show that the ratio between the three different TTG types varies greatly during the two phases of the plume-lid tectonics cycle: growth phase and overturn phase. Melt productivity of the <span class="hlt">mantle</span> decreases rapidly after removal of the garnet and clinopyroxene components. Addition of new garnet and clinopyroxene-rich material into the harzburgitic residue should lead to a refertilised lherzolite which could potentially yield new melt (Bédard, 2006). Mixing of eclogite drips back into the <span class="hlt">mantle</span> can lead to the geochemical refertilisation of already depleted <span class="hlt">mantle</span> and allow for further extraction of melt (Bédard, 2006). We will explore this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060056235','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060056235"><span>Asteroidal <span class="hlt">Differentiation</span> Processes Deduced from Ultramafic Achondrite Ureilite Meteorites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Downes, Hilary; Mittlefehldt, David W.; Hudson, Pierre; Romanek, Christopher S.; Franchi, Ian</p> <p>2006-01-01</p> <p>Ureilites are the second largest achondrite group. They are ultramafic achondrites that have experienced igneous processing whilst retaining some degree of nebula-derived chemical heterogeneity. They differ from other achondrites in that they contain abundant carbon and their oxygen isotope compositions are very heterogeneous and similar to those of the carbonaceous chondrite anhydrous mineral line. Their carbonaceous nature and some compositional characteristics indicative of nebular origin suggest that they are primitive materials that form a link between nebular processes and <span class="hlt">early</span> periods of planetesimal accretion. However, despite numerous studies, the exact origin of ureilites remains unclear. Current opinion is that they represent the residual <span class="hlt">mantle</span> of an asteroid that underwent silicate and Fe-Ni-S partial melting and melt removal. Recent studies of short-lived chronometers indicate that the parent asteroid of the ureilites <span class="hlt">differentiated</span> very <span class="hlt">early</span> in the history of the Solar System. Therefore, they contain important information about processes that formed small rocky planetesimals in the <span class="hlt">early</span> Solar System. In effect, they form a bridge between nebula processes and <span class="hlt">differentiation</span> in small planetesimals prior to accretion into larger planets and so a correct interpretation of ureilite petrogenesis is essential for understanding this critical step.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.U41B0413V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.U41B0413V"><span>Searching for Seismic Signatures of a Plume Source at the Base of the <span class="hlt">Mantle</span> Below the Galapagos Island Hotspot</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vanacore, E.; Niu, F.</p> <p>2007-12-01</p> <p>This study analyzes SKS and SKKS waveforms recorded on the BOLIVAR array in Venezuela and the BANJO array in South America from earthquake sources located in Tonga and Alaska regions to characterize the lower <span class="hlt">mantle</span> beneath the Galapagos Islands. The data analysis applies two independent methods, residual <span class="hlt">differential</span> SKKS-SKS travel times and anisotropy measurements, to examine the historically unsampled region. The residual <span class="hlt">differential</span> travel time observations were performed using 21 earthquakes from the Tonga trench with magnitudes greater than 5.5 Mw that were recorded on the Bolivar array. Only data that was deemed to have a high SNR for both the SKS and SKKS phases were retained for analysis. Significant positive values of <span class="hlt">differential</span> travel time that indicate low velocity along the SKKS raypaths are detected east of ~\\m270° longitude. The anisotropy data set consists of 31 intermediate and deep focus earthquakes from the Tonga and Aleutian trenches recorded on the BOLIVAR and BANJO arrays respectively. The anisotropy fast axis angle and time lag of the two phases are calculated using the 1-layer cross-convolution method of Menke and Levin (2003) with a maximum time lag window of 3 seconds. We retain results with an amplitude normalized squared L2 norm value of 0.6 or less for analysis. Because the raypaths of the SKS and SKKS phases are similar in the upper <span class="hlt">mantle</span> and sample different regions of the lower <span class="hlt">mantle</span>, we attribute inconsistencies between the two anisotropy to difference of the <span class="hlt">mantle</span> structure near the CMB. We define significant difference in the azimuth of the fast axis as any difference between the SKSac and SKKSac measurements greater than 15 degrees. The dataset is dominated by inconsistent fast axis azimuth measurements between the SKSac and SKKSac phases, but does not isolate a single geographic region. Comparison of the splitting time measurements yields that inconsistency between the two phases is more significant, greater than 0.5 s</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12460480','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12460480"><span><span class="hlt">Mantle</span>-circulation models with sequential data assimilation: inferring present-day <span class="hlt">mantle</span> structure from plate-motion histories.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bunge, Hans-Peter; Richards, M A; Baumgardner, J R</p> <p>2002-11-15</p> <p>Data assimilation is an approach to studying geodynamic models consistent simultaneously with observables and the governing equations of <span class="hlt">mantle</span> flow. Such an approach is essential in <span class="hlt">mantle</span> circulation models, where we seek to constrain an unknown initial condition some time in the past, and thus cannot hope to use first-principles convection calculations to infer the flow history of the <span class="hlt">mantle</span>. One of the most important observables for <span class="hlt">mantle</span>-flow history comes from models of Mesozoic and Cenozoic plate motion that provide constraints not only on the surface velocity of the <span class="hlt">mantle</span> but also on the evolution of internal <span class="hlt">mantle</span>-buoyancy forces due to subducted oceanic slabs. Here we present five <span class="hlt">mantle</span> circulation models with an assimilated plate-motion history spanning the past 120 Myr, a time period for which reliable plate-motion reconstructions are available. All models agree well with upper- and mid-<span class="hlt">mantle</span> heterogeneity imaged by seismic tomography. A simple standard model of whole-<span class="hlt">mantle</span> convection, including a factor 40 viscosity increase from the upper to the lower <span class="hlt">mantle</span> and predominantly internal heat generation, reveals downwellings related to Farallon and Tethys subduction. Adding 35% bottom heating from the core has the predictable effect of producing prominent high-temperature anomalies and a strong thermal boundary layer at the base of the <span class="hlt">mantle</span>. Significantly delaying <span class="hlt">mantle</span> flow through the transition zone either by modelling the dynamic effects of an endothermic phase reaction or by including a steep, factor 100, viscosity rise from the upper to the lower <span class="hlt">mantle</span> results in substantial transition-zone heterogeneity, enhanced by the effects of trench migration implicit in the assimilated plate-motion history. An expected result is the failure to account for heterogeneity structure in the deepest <span class="hlt">mantle</span> below 1500 km, which is influenced by Jurassic plate motions and thus cannot be modelled from sequential assimilation of plate motion histories</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI52A..04S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI52A..04S"><span>Core-<span class="hlt">Mantle</span> Boundary Complexities beneath the Mid-Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, D.; Helmberger, D. V.; Jackson, J. M.</p> <p>2016-12-01</p> <p>The detailed core-<span class="hlt">mantle</span> boundary (CMB) structures beneath the Mid-Pacific are important to map the boundary of Large Low Shear Velocity Province (LLSVP) and the location of ultra-low velocity zone (ULVZ) related to the LLSVP and the D" layer, which are crucial for answering the key questions regarding to the <span class="hlt">mantle</span> dynamics. Seismic data from deep earthquakes in the Fiji-Tonga region recorded by stations of USArray provide great sampling of the CMB beneath the Mid-Pacific. Here we explore the USArray data with different seismic phases to study the CMB complexities beneath the Mid-Pacific. First, we examined the <span class="hlt">differential</span> travel time and amplitude between ScS and S for data at western US and confirm the northeastern boundary of the mid-Pacific LLSVP. The delayed ScS-S travel times and smaller amplitude of ScS require the existence of ULVZ locally. Secondly, the Sdiff data recorded by stations at central US shows variation in multi-pathing, that is, the presence of secondary arrivals following the S phase at diffracted distances (Sdiff) which suggests that the waveform complexity is due to structures at the eastern edge of the mid-Pacific LLSVP. This study reinforces previous studies that indicate late arrivals occurring after the primary Sdiff arrivals. A tapered wedge structure with low shear velocity allows for wave energy trapping, producing the observed waveform complexity and delayed arrivals at large distances. The location of the low velocity anomaly agrees with that inferred from the ScS-S measurements. We also observed advanced SV arrivals, which can be explained by the emerging of the D" discontinuity to the east of the boundary of the LLSVP to produce a "pseudo anisotropy". Thirdly, the arrivals of the SPdKS phase support the presence of an ULVZ within a two-humped LLSVP. A sharp 10 secs jump of the <span class="hlt">differential</span> travel time between S and SKS (TS-SKS) across distance range of 5° is observed. The associated SKS waveform distortions suggest that the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25205117','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25205117"><span>Role for <span class="hlt">early-differentiated</span> natural killer cells in infectious mononucleosis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Azzi, Tarik; Lünemann, Anna; Murer, Anita; Ueda, Seigo; Béziat, Vivien; Malmberg, Karl-Johan; Staubli, Georg; Gysin, Claudine; Berger, Christoph; Münz, Christian; Chijioke, Obinna; Nadal, David</p> <p>2014-10-16</p> <p>A growing body of evidence suggests that the human natural killer (NK)-cell compartment is phenotypically and functionally heterogeneous and is composed of several <span class="hlt">differentiation</span> stages. Moreover, NK-cell subsets have been shown to exhibit adaptive immune features during herpes virus infection in experimental mice and to expand preferentially during viral infections in humans. However, both phenotype and role of NK cells during acute symptomatic Epstein-Barr virus (EBV) infection, termed infectious mononucleosis (IM), remain unclear. Here, we longitudinally assessed the kinetics, the <span class="hlt">differentiation</span>, and the proliferation of subsets of NK cells in pediatric IM patients. Our results indicate that acute IM is characterized by the preferential proliferation of <span class="hlt">early-differentiated</span> CD56(dim) NKG2A(+) immunoglobulin-like receptor(-) NK cells. Moreover, this NK-cell subset exhibits features of terminal <span class="hlt">differentiation</span> and persists at higher frequency during at least the first 6 months after acute IM. Finally, we demonstrate that this NK-cell subset preferentially degranulates and proliferates on exposure to EBV-infected B cells expressing lytic antigens. Thus, <span class="hlt">early-differentiated</span> NK cells might play a key role in the immune control of primary infection with this persistent tumor-associated virus. © 2014 by The American Society of Hematology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22696609-synchrotron-ftir-microspectroscopy-reveals-early-adipogenic-differentiation-human-mesenchymal-stem-cells-single-cell-level','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22696609-synchrotron-ftir-microspectroscopy-reveals-early-adipogenic-differentiation-human-mesenchymal-stem-cells-single-cell-level"><span>Synchrotron FTIR microspectroscopy reveals <span class="hlt">early</span> adipogenic <span class="hlt">differentiation</span> of human mesenchymal stem cells at single-cell level</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Liu, Zhixiao; University of Chinese Academy of Science, Beijing 100049; Tang, Yuzhao</p> <p></p> <p>Human mesenchymal stem cells (hMSCs) have been used as an ideal in vitro model to study human adipogenesis. However, little knowledge of the <span class="hlt">early</span> stage <span class="hlt">differentiation</span> greatly hinders our understanding on the mechanism of the adipogenesis processes. In this study, synchrotron radiation-based Fourier transform infrared (SR-FTIR) microspectroscopy was applied to track the global structural and compositional changes of lipids, proteins and nucleic acids inside individual hMSCs along the time course. The multivariate analysis of the SR-FTIR spectra distinguished the dynamic and significant changes of the lipids and nucleic acid at <span class="hlt">early</span> <span class="hlt">differentiation</span> stage. Importantly, changes of lipid structure during <span class="hlt">early</span> daysmore » (Day 1–3) of <span class="hlt">differentiation</span> might serve as a potential biomarker in identifying the state in <span class="hlt">early</span> <span class="hlt">differentiation</span> at single cell level. These results proved that SR-FTIR is a powerful tool to study the stem cell fate determination and <span class="hlt">early</span> lipogenesis events. - Highlights: • Molecular events occur in the <span class="hlt">early</span> adipogenic <span class="hlt">differentiation</span> stage of hMSCs are studied by SR-FTIR. • SR-FTIR data suggest that lipids may play an important role in hMSCs determination. • As potential biomarkers, lipids peaks can identify the state of cell in <span class="hlt">early</span> <span class="hlt">differentiation</span> stage at single-cell level.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI43C..08H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI43C..08H"><span>Alternate Histories of the Core-<span class="hlt">Mantle</span> Boundary Region: Discrimination by Heat Flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hernlund, J. W.</p> <p>2017-12-01</p> <p>Interactions between material that would become Earth's core and <span class="hlt">mantle</span> began prior to accretion. For example, during and just after the supernova event that is thought to have produced the matter that comprises our solar system, a substantial amount of its iron and other heavy elements were forged in nucleosynthetic processes, establishing a pattern of elemental and isotopic abundances that is reflected in the composition of our planet today, and sets the relative size of the core and <span class="hlt">mantle</span>. As Earth accreted, metals and silicates were delivered together in mostly small increments, and formation of the core required separation and gravitational settling of the metal to the center, probably facilitated by extensive melting. This process over-printed previous metal-silicate interactions, owing to chemical interactions and re-equilibration at higher pressures and temperatures. The heat of core formation was dissipated largely in the <span class="hlt">mantle</span> if metal descended as diapirs, or was retained in the metal if it was able to crack the <span class="hlt">mantle</span> and sink by rapid turbulent injection into the core. These processes established the first temperature contrast between the core and the <span class="hlt">mantle</span>, controlling the extent to which the core could become a giant heat capacitor and supply thermal energy heat to the <span class="hlt">mantle</span>. Beginning from this very <span class="hlt">early</span> stage we are able to correlate different hypothesized processes with their variable implications for core-<span class="hlt">mantle</span> boundary (CMB) heat flow through time. In fact, CMB heat flow is a thread that runs through almost every important question regarding the evolution of the core and <span class="hlt">mantle</span>. Whole <span class="hlt">mantle</span> convection vs. layered convection, the abundance of radioactive isotopes, age of the inner core, sustenance of the ancient geodynamo, the possibility of basal magma oceans, core-<span class="hlt">mantle</span> chemical interactions, etc., all have close connections to CMB heat flow. Here I will attempt to discriminate hypotheses for many processes into high vs. low CMB heat</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70017042','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70017042"><span>Seismic evidence for silicate melt atop the 410-km <span class="hlt">mantle</span> discontinuity</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Revenaugh, Justin; Sipkin, S.A.</p> <p>1994-01-01</p> <p>LABORATORY results demonstrating that basic to ultrabasic melts become denser than olivine-rich <span class="hlt">mantle</span> at pressures above 6 GPa (refs 1-3) have important implications for basalt petrogenesis, <span class="hlt">mantle</span> <span class="hlt">differentiation</span> and the storage of volatiles deep in the Earth. A density cross-over between melt and solid in the extensively molten Archaean <span class="hlt">mantle</span> has been inferred from komatiitic volcanism and major-element mass balances, but present-day evidence of dense melt below the seismic low-velocity zone is lacking. Here we present <span class="hlt">mantle</span> shear-wave impedance profiles obtained from multiple-ScS reverberation mapping for corridors connecting western Pacific subduction zone earthquakes with digital seismograph stations in eastern China, imaging a ~5.8% impedance decrease roughly 330 km beneath the Sea of Japan, Yellow Sea and easternmost Asia. We propose that this represents the upper surface of a layer of negatively buoyant melt lying on top of the olivine ??? ??- phase transition (the 410-km seismic discontinuity). Volatile-rich fluids expelled from the partial melt zone as it freezes may migrate upwards, acting as metasomatic agents and perhaps as the deep 'proto-source' of kimberlites. The remaining, dense, crystalline fraction would then concentrate above 410 km, producing a garnet-rich layer that may flush into the transition zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28500352','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28500352"><span>Whole-<span class="hlt">mantle</span> convection with tectonic plates preserves long-term global patterns of upper <span class="hlt">mantle</span> geochemistry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barry, T L; Davies, J H; Wolstencroft, M; Millar, I L; Zhao, Z; Jian, P; Safonova, I; Price, M</p> <p>2017-05-12</p> <p>The evolution of the planetary interior during plate tectonics is controlled by slow convection within the <span class="hlt">mantle</span>. Global-scale geochemical differences across the upper <span class="hlt">mantle</span> are known, but how they are preserved during convection has not been adequately explained. We demonstrate that the geographic patterns of chemical variations around the Earth's <span class="hlt">mantle</span> endure as a direct result of whole-<span class="hlt">mantle</span> convection within largely isolated cells defined by subducting plates. New 3D spherical numerical models embedded with the latest geological paleo-tectonic reconstructions and ground-truthed with new Hf-Nd isotope data, suggest that uppermost <span class="hlt">mantle</span> at one location (e.g. under Indian Ocean) circulates down to the core-<span class="hlt">mantle</span> boundary (CMB), but returns within ≥100 Myrs via large-scale convection to its approximate starting location. Modelled tracers pool at the CMB but do not disperse ubiquitously around it. Similarly, <span class="hlt">mantle</span> beneath the Pacific does not spread to surrounding regions of the planet. The models fit global patterns of isotope data and may explain features such as the DUPAL anomaly and long-standing differences between Indian and Pacific Ocean crust. Indeed, the geochemical data suggests this mode of convection could have influenced the evolution of <span class="hlt">mantle</span> composition since 550 Ma and potentially since the onset of plate tectonics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT.......346H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......346H"><span><span class="hlt">Mantle</span> dynamics following supercontinent formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heron, Philip J.</p> <p></p> <p>This thesis presents <span class="hlt">mantle</span> convection numerical simulations of supercontinent formation. Approximately 300 million years ago, through the large-scale subduction of oceanic sea floor, continental material amalgamated to form the supercontinent Pangea. For 100 million years after its formation, Pangea remained relatively stationary, and subduction of oceanic material featured on its margins. The present-day location of the continents is due to the rifting apart of Pangea, with supercontinent dispersal being characterized by increased volcanic activity linked to the generation of deep <span class="hlt">mantle</span> plumes. The work presented here investigates the thermal evolution of <span class="hlt">mantle</span> dynamics (e.g., <span class="hlt">mantle</span> temperatures and sub-continental plumes) following the formation of a supercontinent. Specifically, continental insulation and continental margin subduction are analyzed. Continental material, as compared to oceanic material, inhibits heat flow from the <span class="hlt">mantle</span>. Previous numerical simulations have shown that the formation of a stationary supercontinent would elevate sub-continental <span class="hlt">mantle</span> temperatures due to the effect of continental insulation, leading to the break-up of the continent. By modelling a vigorously convecting <span class="hlt">mantle</span> that features thermally and mechanically distinct continental and oceanic plates, this study shows the effect of continental insulation on the <span class="hlt">mantle</span> to be minimal. However, the formation of a supercontinent results in sub-continental plume formation due to the re-positioning of subduction zones to the margins of the continent. Accordingly, it is demonstrated that continental insulation is not a significant factor in producing sub-supercontinent plumes but that subduction patterns control the location and timing of upwelling formation. A theme throughout the thesis is an inquiry into why geodynamic studies would produce different results. <span class="hlt">Mantle</span> viscosity, Rayleigh number, continental size, continental insulation, and oceanic plate boundary evolution are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3191542','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3191542"><span>Spatial analysis of biomineralization associated gene expression from the <span class="hlt">mantle</span> organ of the pearl oyster Pinctada maxima</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2011-01-01</p> <p>Background Biomineralization is a process encompassing all mineral containing tissues produced within an organism. One of the most dynamic examples of this process is the formation of the mollusk shell, comprising a variety of crystal phases and microstructures. The organic component incorporated within the shell is said to dictate this architecture. However general understanding of how this process is achieved remains ambiguous. The <span class="hlt">mantle</span> is a conserved organ involved in shell formation throughout molluscs. Specifically the <span class="hlt">mantle</span> is thought to be responsible for secreting the protein component of the shell. This study employs molecular approaches to determine the spatial expression of genes within the <span class="hlt">mantle</span> tissue to further the elucidation of the shell biomineralization. Results A microarray platform was custom generated (PmaxArray 1.0) from the pearl oyster Pinctada maxima. PmaxArray 1.0 consists of 4992 expressed sequence tags (ESTs) originating from <span class="hlt">mantle</span> tissue. This microarray was used to analyze the spatial expression of ESTs throughout the <span class="hlt">mantle</span> organ. The <span class="hlt">mantle</span> was dissected into five discrete regions and analyzed for <span class="hlt">differential</span> gene expression with PmaxArray 1.0. Over 2000 ESTs were determined to be <span class="hlt">differentially</span> expressed among the tissue sections, identifying five major expression regions. In situ hybridization validated and further localized the expression for a subset of these ESTs. Comparative sequence similarity analysis of these ESTs revealed a number of the transcripts were novel while others showed significant sequence similarities to previously characterized shell related genes. Conclusions This investigation has mapped the spatial distribution for over 2000 ESTs present on PmaxArray 1.0 with reference to specific locations of the <span class="hlt">mantle</span>. Expression profile clusters have indicated at least five unique functioning zones in the <span class="hlt">mantle</span>. Three of these zones are likely involved in shell related activities including formation of nacre</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PEPI..183..245I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PEPI..183..245I"><span>Water partitioning in the Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Inoue, Toru; Wada, Tomoyuki; Sasaki, Rumi; Yurimoto, Hisayoshi</p> <p>2010-11-01</p> <p>We have conducted H2O partitioning experiments between wadsleyite and ringwoodite and between ringwoodite and perovskite at 1673 K and 1873 K, respectively. These experiments were performed in order to constrain the relative distribution of H2O in the upper <span class="hlt">mantle</span>, the <span class="hlt">mantle</span> transition zone, and the lower <span class="hlt">mantle</span>. We successfully synthesized coexisting mineral assemblages of wadsleyite-ringwoodite and ringwoodite-perovskite that were large enough to measure the H2O contents by secondary ion mass spectrometry (SIMS). Combining our previous H2O partitioning data (Chen et al., 2002) with the present results, the determined water partitioning between olivine, wadsleyite, ringwoodite, and perovskite under H2O-rich fluid saturated conditions are 6:30:15:1, respectively. Because the maximum H2O storage capacity in wadsleyite is ∼3.3 wt% (e.g. Inoue et al., 1995), the possible maximum H2O storage capacity in the olivine high-pressure polymorphs are as follows: ∼0.7 wt% in olivine (upper <span class="hlt">mantle</span> just above 410 km depth), ∼3.3 wt% in wadsleyite (410-520 km depth), ∼1.7 wt% in ringwoodite (520-660 km depth), and ∼0.1 wt% in perovskite (lower <span class="hlt">mantle</span>). If we assume ∼0.2 wt% of the H2O content in wadsleyite in the <span class="hlt">mantle</span> transition zone estimated by recent electrical conductivity measurements (e.g. Dai and Karato, 2009), the estimated H2O contents throughout the <span class="hlt">mantle</span> are as follows; ∼0.04 wt% in olivine (upper <span class="hlt">mantle</span> just above 410 km depth), ∼0.2 wt% in wadsleyite (410-520 km depth), ∼0.1 wt% in ringwoodite (520-660 km depth) and ∼0.007 wt% in perovskite (lower <span class="hlt">mantle</span>). Thus, the <span class="hlt">mantle</span> transition zone should contain a large water reservoir in the Earth's <span class="hlt">mantle</span> compared to the upper <span class="hlt">mantle</span> and the lower <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150009507','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150009507"><span>Evolution of the Oxidation State of the Earth's <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Danielson, L. R.; Righter, K.; Keller, L.; Christoffersen, E.; Rahman, Z.</p> <p>2015-01-01</p> <p>The oxidation state of the Earth's <span class="hlt">mantle</span> during formation remains an unresolved question, whether it was constant throughout planetary accretion, transitioned from reduced to oxidized, or from oxidized to reduced. We investigate the stability of Fe3(+) at depth, in order to constrain processes (water, late accretion, dissociation of FeO) which may reduce or oxidize the Earth's <span class="hlt">mantle</span>. In our previous experiments on shergottite compositions, variable fO2, T, and P less than 4 GPa, Fe3(+)/sigma Fe decreased slightly with increasing P, similar to terrestrial basalt. For oxidizing experiments less than 7GPa, Fe3(+)/sigma Fe decreased as well, but it's unclear from previous modelling whether the deeper <span class="hlt">mantle</span> could retain significant Fe3(+). Our current experiments expand our pressure range deeper into the Earth's <span class="hlt">mantle</span> and focus on compositions and conditions relevant to the <span class="hlt">early</span> Earth. Preliminary multi-anvil experiments with Knippa basalt as the starting composition were conducted at 5-7 GPa and 1800 C, using a molybdenum capsule to set the fO2 near IW, by buffering with Mo-MoO3. TEM and EELS analyses revealed the run products quenched to polycrystalline phases, with the major phase pyroxene containing approximately equal to Fe3(+)/2(+). Experiments are underway to produce glassy samples that can be measured by EELS and XANES, and are conducted at higher pressures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=ductile&id=EJ285782','ERIC'); return false;" href="https://eric.ed.gov/?q=ductile&id=EJ285782"><span>The Earth's <span class="hlt">Mantle</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>McKenzie, D. P.</p> <p>1983-01-01</p> <p>The nature and dynamics of the earth's <span class="hlt">mantle</span> is discussed. Research indicates that the silicate <span class="hlt">mantle</span> is heated by the decay of radioactive isotopes and that the heat energizes massive convention currents in the upper 700 kilometers of the ductile rock. These currents and their consequences are considered. (JN)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.V43D..03B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.V43D..03B"><span>Hf and Nd Isotope Evidence for Production of an Incompatible Trace Element Enriched Crustal Reservoir in <span class="hlt">Early</span> Earth (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brandon, A. D.; Debaille, V.; Lapen, T. J.</p> <p>2010-12-01</p> <p>, <span class="hlt">early</span>-formed ITE-enriched reservoir [4]. This <span class="hlt">early</span>-formed enriched ITE reservoir is indistinguishable in age and 176Lu/177Hf to those that formed in the Moon and Mars [5,6]. Hence all three terrestrial bodies must have undergone similar <span class="hlt">early</span> <span class="hlt">differentiation</span> and each formed and sustained their requisite <span class="hlt">early</span>-formed ITE-enriched reservoirs at or near their surfaces. For all three terrestrial bodies, their <span class="hlt">early</span>-formed ITE-enriched reservoirs appear to be the result of solidification of late stage residual liquids from their respective MO’s at or prior to 4.4 Ga. In Earth, mixing of an <span class="hlt">early</span>-formed ITE-enriched reservoir back into the <span class="hlt">mantle</span> likely occurred back into the convecting <span class="hlt">mantle</span> at or before 3.9 Ga. For the Moon and Mars, the lack of plate tectonics preserved their <span class="hlt">early</span>-formed ITE-enriched lithospheric reservoirs. [1] Tolstikhin and Hofmann, PEPI (2005) 148, 109. [2] Boyet and Carlson, Science (2005) 309, 576. [3] Bennett et al., Science (2007) 218, 1907. [3] Kemp et al., EPSL (2010) 296, 45. [5] Taylor et al. (2009) 279, 157. [6] Lapen et al., Science (2010) 328, 347.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Litho.240..119A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Litho.240..119A"><span>Nature of the lithospheric <span class="hlt">mantle</span> beneath the Arabian Shield and genesis of Al-spinel micropods: Evidence from the <span class="hlt">mantle</span> xenoliths of Harrat Kishb, Western Saudi Arabia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahmed, Ahmed H.; Moghazi, Abdel Kader M.; Moufti, Mohamed R.; Dawood, Yehia H.; Ali, Kamal A.</p> <p>2016-01-01</p> <p>The Harrat Kishb area of western Saudi Arabia is part of the Cenozoic volcanic fields in the western margin of the Arabian Shield. Numerous fresh ultramafic xenoliths are entrained in the basanite lava of Harrat Kishb, providing an opportunity to study the nature and petrogenetic processes involved in the evolution of the lithospheric <span class="hlt">mantle</span> beneath the Arabian Shield. Based on the petrological characteristics and mineralogical compositions, the majority of the <span class="hlt">mantle</span> xenoliths ( 92%) are peridotites (lherzolites and pyroxene-bearing harzburgites); the remaining xenoliths ( 8%) are unusual spinel-rich wehrlites containing black Al-spinel micropods. The two types of <span class="hlt">mantle</span> xenoliths display magmatic protogranular texture. The peridotite xenoliths have high bulk-rock Mg#, high forsterite (Fo90-Fo92) and NiO (0.24-0.46 wt.%) contents of olivine, high clinopyroxene Mg# (0.91-0.93), variable spinel Cr# (0.10-0.49, atomic ratio), and approximately flat chondrite-normalized REE patterns. These features indicate that the peridotite xenoliths represent residues after variable degrees of melt extraction from fertile <span class="hlt">mantle</span>. The estimated P (9-16 kbar) and T (877-1227 °C) as well as the oxidation state (ΔlogfO2 = - 3.38 to - 0.22) under which these peridotite xenoliths originated are consistent with formation conditions similar to most sub-arc abyssal-type peridotites worldwide. The spinel-rich wehrlite xenoliths have an unusual amount ( 30 vol.%) of Al-spinel as peculiar micropods with very minor Cr2O3 content (< 1 wt.%). Olivines of the spinel-rich wehrlites have low-average Fo (Fo81) and NiO (0.18 wt.%) contents, low-average cpx Mg# (0.79), high average cpx Al2O3 content (8.46 wt.%), and very low-average spinel Cr# (0.01). These features characterize <span class="hlt">early</span> <span class="hlt">mantle</span> cumulates from a picritic melt fraction produced by low degrees of partial melting of a garnet-bearing <span class="hlt">mantle</span> source. The relatively high Na2O and Al2O3 contents of cpx suggest that the spinel-rich wehrlites are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMDI13D2451I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMDI13D2451I"><span>The maximum water storage capacities in nominally anhydrous minerals in the <span class="hlt">mantle</span> transition zone and lower <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Inoue, T.; Yurimoto, H.</p> <p>2012-12-01</p> <p>Water is the most important volatile component in the Earth, and affects the physicochemical properties of <span class="hlt">mantle</span> minerals, e.g. density, elastic property, electrical conductivity, thermal conductivity, rheological property, melting temperature, melt composition, element partitioning, etc. So many high pressure experiments have been conducted so far to determine the effect of water on <span class="hlt">mantle</span> minerals. To clarify the maximum water storage capacity in nominally anhydrous <span class="hlt">mantle</span> minerals in the <span class="hlt">mantle</span> transition zone and lower <span class="hlt">mantle</span> is an important issue to discuss the possibility of the existence of water reservoir in the Earth <span class="hlt">mantle</span>. So we have been clarifying the maximum water storage capacity in <span class="hlt">mantle</span> minerals using MA-8 type (KAWAI-type) high pressure apparatus and SIMS (secondary ion mass spectroscopy). Upper <span class="hlt">mantle</span> mineral, olivine can contain ~0.9 wt% H2O in the condition just above 410 km discontinuity in maximum (e.g. Chen et al., 2002; Smyth et al., 2006). On the other hand, <span class="hlt">mantle</span> transition zone mineral, wadsleyite and ringwoodite can contain significant amount (about 2-3 wt.%) of H2O (e.g. Inoue et al., 1995, 1998, 2010; Kawamoto et al., 1996; Ohtani et al., 2000). But the lower <span class="hlt">mantle</span> mineral, perovskite can not contain significant amount of H2O, less than ~0.1 wt% (e.g. Murakami et al., 2002; Inoue et al., 2010). In addition, garnet and stishovite also can not contain significant amount of H2O (e.g. Katayama et al., 2003; Mookherjee and Karato, 2010; Litasov et al., 2007). On the other hand, the water storage capacities of <span class="hlt">mantle</span> minerals are supposed to be significantly coupled with Al by a substitution with Mg2+, Si4+ or Mg2+ + Si4+, because Al3+ is the trivalent cation, and H+ is the monovalent cation. To clarify the degree of the substitution, the water contents and the chemical compositions of Al-bearing minerals in the <span class="hlt">mantle</span> transition zone and the lower <span class="hlt">mantle</span> were also determined in the Al-bearing systems with H2O. We will introduce the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.199..287B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.199..287B"><span>Silica-enriched <span class="hlt">mantle</span> sources of subalkaline picrite-boninite-andesite island arc magmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bénard, A.; Arculus, R. J.; Nebel, O.; Ionov, D. A.; McAlpine, S. R. B.</p> <p>2017-02-01</p> <p>Primary arc melts may form through fluxed or adiabatic decompression melting in the <span class="hlt">mantle</span> wedge, or via a combination of both processes. Major limitations to our understanding of the formation of primary arc melts stem from the fact that most arc lavas are aggregated blends of individual magma batches, further modified by <span class="hlt">differentiation</span> processes in the sub-arc <span class="hlt">mantle</span> lithosphere and overlying crust. Primary melt generation is thus masked by these types of second-stage processes. Magma-hosted peridotites sampled as xenoliths in subduction zone magmas are possible remnants of sub-arc <span class="hlt">mantle</span> and magma generation processes, but are rarely sampled in active arcs. Published studies have emphasised the predominantly harzburgitic lithologies with particularly high modal orthopyroxene in these xenoliths; the former characteristic reflects the refractory nature of these materials consequent to extensive melt depletion of a lherzolitic protolith whereas the latter feature requires additional explanation. Here we present major and minor element data for pristine, <span class="hlt">mantle</span>-derived, lava-hosted spinel-bearing harzburgite and dunite xenoliths and associated primitive melts from the active Kamchatka and Bismarck arcs. We show that these peridotite suites, and other <span class="hlt">mantle</span> xenoliths sampled in circum-Pacific arcs, are a distinctive peridotite type not found in other tectonic settings, and are melting residues from hydrous melting of silica-enriched <span class="hlt">mantle</span> sources. We explore the ability of experimental studies allied with <span class="hlt">mantle</span> melting parameterisations (pMELTS, Petrolog3) to reproduce the compositions of these arc peridotites, and present a protolith ('hybrid <span class="hlt">mantle</span> wedge') composition that satisfies the available constraints. The composition of peridotite xenoliths recovered from erupted arc magmas plausibly requires their formation initially via interaction of slab-derived components with refractory <span class="hlt">mantle</span> prior to or during the formation of primary arc melts. The liquid</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMDI43A2610M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMDI43A2610M"><span>Origin and Constraints on Ilmenite-rich Partial Melt in the Lunar Lower <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mallik, A.; Fuqua, H.; Bremner, P. M.; Panovska, S.; Diamond, M. R.; Lock, S. J.; Nishikawa, Y.; Jiménez-Pérez, H.; Shahar, A.; Panero, W. R.; Lognonne, P. H.; Faul, U.</p> <p>2015-12-01</p> <p>Existence of a partially molten layer at the lunar core-<span class="hlt">mantle</span> boundary has been proposed to explain the lack of observed far-side deep moonquakes, the observation of reflected seismic phases from deep moonquakes, and the dissipation of tidal energy within the lunar interior [1,2]. However, subsequent models explored the possibility that dissipation due to elevated temperatures alone can explain the observed dissipation factor (Q) and tidal love numbers [3]. Using thermo-chemical and dynamic modeling (including models of the <span class="hlt">early</span> lunar <span class="hlt">mantle</span> convection), we explore the hypothesis that an ilmenite-rich layer forms below crustal anorthosite during lunar magma ocean crystallization and may sink to the base of the <span class="hlt">mantle</span> to create a partial melt layer at the lunar core-<span class="hlt">mantle</span> boundary. Self-consistent physical parameters (including gravity, pressure, density, VP and Vs) are forward calculated for a well-mixed <span class="hlt">mantle</span> with uniform bulk composition versus a <span class="hlt">mantle</span> with preserved mineralogical stratigraphy from lunar magma ocean crystallization. These parameters are compared against observed mass, moment of inertia, real and imaginary parts of the Love numbers, and seismic travel times to further limit the acceptable models for the Moon. We have performed a multi-step grid search with over twenty thousand forward calculations varying thicknesses of chemically/mineralogically distinct layers within the Moon to evaluate if a partially molten layer at the base of the lunar <span class="hlt">mantle</span> is well-constrained by the observed data. Furthermore, dynamic <span class="hlt">mantle</span> modeling was employed on the best-fit model versions to determine the survivability of a partially molten layer at the core-<span class="hlt">mantle</span> boundary. This work was originally initiated at the CIDER 2014 program. [1] Weber et al. (2011). Science 331(6015), 309-12. [2] Khan et al. (2014). JGR 119. [3] Nimmo et al. (2012). JGR 117, 1-11.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.T51E..08V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.T51E..08V"><span>The Role of the <span class="hlt">Mantle</span> on Structural Reactivation at the Plate Tectonics Scale (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vauchez, A. R.; Tommasi, A.</p> <p>2009-12-01</p> <p>During orogeny, rifting, and in major strike-slip faults, the lithospheric <span class="hlt">mantle</span> undergoes solid-state flow to accommodate the imposed strain. This deformation occurs mostly through crystal plasticity processes, like dislocation creep, and results in the development of a crystallographic preferred orientation (CPO) of olivine and pyroxene. Because these minerals, especially olivine, display strongly anisotropic physical properties, their preferred orientation confers anisotropic properties at the scale of the rock. When the deformation event comes to its end, the CPO are "frozen" and remain stable for millions or even billions years if no other deformation subsequently affects the lithospheric <span class="hlt">mantle</span>. This means that anisotropic properties preserving a memory of previous deformation events may subsist in the continental <span class="hlt">mantle</span> over very long periods of time. One of the main consequences of a well-developed olivine CPO is an anisotropic <span class="hlt">mantle</span> viscosity and hence a deformation dependant on the orientation of the tectonic solicitations relative to the orientation of the olivine CPO inherited from the past orogenic events. The most obvious expression of this anisotropic mechanical behaviour is the influence of the inherited tectonic fabric on continental rifting. Most continental rifts that lead to successful continental breakup, like in the <span class="hlt">early</span> Atlantic or the western Indian systems, formed parallel to ancient collisional belts. Moreover, the <span class="hlt">early</span> stages of deformation in these systems are characterized by a transtensional strain regime involving a large component of strike-slip shearing parallel to the inherited fabric. The link between the lithospheric <span class="hlt">mantle</span> fabric and the rift structure is further supported by seismic anisotropy measurements in major rifts (e.g., the East-African Rift) or at passive continental margins (e.g., the Atlantic Ocean) that show fast split S-waves polarized in a direction parallel to both the inherited fabric and the trend of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI13B..01H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI13B..01H"><span>Evidence for Primordial Water in Earths Deep <span class="hlt">Mantle</span>: D/h Ratios in Baffin Island and Icelandic Picrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hallis, L. J.; Huss, G. R.; Nagashima, K.; Taylor, J.; Hilton, D. R.; Mottl, M. J.; Meech, K. J.; Halldorsson, S. A.</p> <p>2016-12-01</p> <p>Experimentally based chemical models suggest Jeans escape could have caused an increase in Earth's atmospheric D/H ratio of between a factor of 2 and 9 since the planets formation1. Plate tectonic mixing ensures this change has been incorporated into the <span class="hlt">mantle</span>. In addition, collisions with hydrogen bearing planetesimals or cometary material after Earth's accretion could have altered the D/H ratio of the planet's surface and upper <span class="hlt">mantle</span>2. Therefore, to determine Earth's original D/H ratio, a reservoir that has been completely unaffected by these surface and upper <span class="hlt">mantle</span> changes is required. Most studies suggest that high 3He/4He ratios in some OIBs indicate the existence of relatively undegassed regions in the deep <span class="hlt">mantle</span> compared to the upper <span class="hlt">mantle</span>, which retain a greater proportion of their primordial He3-4. <span class="hlt">Early</span> Tertiary (60-million-year-old) picrites from Baffin Island and west Greenland, which represent volcanic rocks from the proto/<span class="hlt">early</span> Iceland <span class="hlt">mantle</span> plume, contain the highest recorded terrestrial 3He/4He ratios3-4. These picrites also have Pb and Nd isotopic ratios consistent with primordial <span class="hlt">mantle</span> ages (4.45 to 4.55 Ga)5, indicating the persistence of an ancient, isolated reservoir in the <span class="hlt">mantle</span>. The undegassed and primitive nature6of this reservoir suggests that it could preserve Earth's initial D/H ratio. We measured the D/H ratios of olivine-hosted glassy melt inclusions in Baffin Island and Icelandic picrites to establish whether their deep <span class="hlt">mantle</span> source region exhibits a different D/H ratio to known upper <span class="hlt">mantle</span> and surface reservoirs. Baffin Island D/H ratios were found to extend lower than any previously measured <span class="hlt">mantle</span> values (δD -97 to -218 ‰), suggesting that areas of the deep <span class="hlt">mantle</span> do preserve a more primitive hydrogen reservoir, hence are unaffected by plate tectonic mixing. Comparing our measured low D/H ratios to those of known extra-terrestrial materials can help determine where Earths water came from. References: [1] Genda and Ikoma</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004Tectp.386...41V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004Tectp.386...41V"><span>Production and recycling of oceanic crust in the <span class="hlt">early</span> Earth</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Thienen, P.; van den Berg, A. P.; Vlaar, N. J.</p> <p>2004-08-01</p> <p>Because of the strongly different conditions in the <span class="hlt">mantle</span> of the <span class="hlt">early</span> Earth regarding temperature and viscosity, present-day geodynamics cannot simply be extrapolated back to the <span class="hlt">early</span> history of the Earth. We use numerical thermochemical convection models including partial melting and a simple mechanism for melt segregation and oceanic crust production to investigate an alternative suite of dynamics which may have been in operation in the <span class="hlt">early</span> Earth. Our modelling results show three processes that may have played an important role in the production and recycling of oceanic crust: (1) Small-scale ( x×100 km) convection involving the lower crust and shallow upper <span class="hlt">mantle</span>. Partial melting and thus crustal production takes place in the upwelling limb and delamination of the eclogitic lower crust in the downwelling limb. (2) Large-scale resurfacing events in which (nearly) the complete crust sinks into the (eventually lower) <span class="hlt">mantle</span>, thereby forming a stable reservoir enriched in incompatible elements in the deep <span class="hlt">mantle</span>. New crust is simultaneously formed at the surface from segregating melt. (3) Intrusion of lower <span class="hlt">mantle</span> diapirs with a high excess temperature (about 250 K) into the upper <span class="hlt">mantle</span>, causing massive melting and crustal growth. This allows for plumes in the Archean upper <span class="hlt">mantle</span> with a much higher excess temperature than previously expected from theoretical considerations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070009871','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070009871"><span>Lu-Hf and Sm-Nd Isotopic Studies of Shergottites and Nakhlites: Implications for Martian <span class="hlt">Mantle</span> Sources</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Debaille, V.; Yin, Q.-Z.; Brandon, A. D.; Jacobsen, B.; Treiman, A. H.</p> <p>2007-01-01</p> <p>We present a new Lu-Hf and Sm-Nd isotope systematics study of four enriched shergottites (Zagami, Shergotty, NWA856 and Los Angeles), and three nakhlites (Nakhla, MIL03346 and Yamato 000593) in order to further understand processes occurring during the <span class="hlt">early</span> <span class="hlt">differentiation</span> of Mars and the crystallization of its magma ocean. Two fractions of the terrestrial petrological analogue of nakhlites, the Archaean Theo's flow (Ontario, Canada) were also measured. The coupling of Nd and Hf isotopes provide direct insights on the mineralogy of the melt sources. In contrast to Sm/Nd, Lu/Hf ratios can be very large in minerals such as garnet. Selective partial melting of garnet bearing <span class="hlt">mantle</span> sources can therefore lead to characteristic Lu/Hf signatures that can be recognized with Hf-176/Hf-177Hf ratios.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.U34A..04A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.U34A..04A"><span>The survival of geochemical <span class="hlt">mantle</span> heterogeneities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Albarede, F.</p> <p>2004-12-01</p> <p>The last decade witnessed major changes in our perception of the geochemical dynamics of the <span class="hlt">mantle</span>. Data bases such as PETDB and GEOROC now provide highly constrained estimates of the geochemical properties of dominant rock types and of their statistics, while the new generation of ICP mass spectrometers triggered a quantum leap in the production of high-precision isotopic and elemental data. Such new advances offer a fresh view of <span class="hlt">mantle</span> heterogeneities and their survival through convective mixing. A vivid example is provided by the new high-density coverage of the Mid-Atlantic ridge by nearly 500 Pb, Nd, and Hf isotopic data. This new data set demonstrates a rich harmonic structure which illustrates the continuing stretching and refolding of subducted plates by <span class="hlt">mantle</span> convection. Just as for oceanic chemical variability, the survival of <span class="hlt">mantle</span> geochemical heterogeneities though <span class="hlt">mantle</span> circulation can be seen as a competition between stirring and renewal. The modern residence (renewal) times of the incompatible lithophile elements in the <span class="hlt">mantle</span> calculated using data bases vary within a rather narrow range (4-9 Gy). The <span class="hlt">mantle</span> is therefore not currently at geochemical steady-state and the effect of its primordial layering on modern <span class="hlt">mantle</span> geochemistry is still strong. Up to 50 percent of incompatible lithophile elements may never have been extracted into the oceanic crust, which generalizes a conclusion reached previously for 40Ar. A balance between the buoyancy flux and viscous dissipation provides frame-independent estimates of the rates of mixing by <span class="hlt">mantle</span> convection: primordial geochemical anomalies with initial length scales comparable to <span class="hlt">mantle</span> depths of plate lengths are only marginally visible at the scale of <span class="hlt">mantle</span> melting underneath mid-ocean ridges (≈~50~km). They may show up, however, in hot spot basalts and even more in melt inclusions. Up to 50 percent primordial material may be present in the <span class="hlt">mantle</span>, but scattered throughout as small (<~10~km</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24961247','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24961247"><span><span class="hlt">Early</span> <span class="hlt">differential</span> processing of material images: Evidence from ERP classification.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wiebel, Christiane B; Valsecchi, Matteo; Gegenfurtner, Karl R</p> <p>2014-06-24</p> <p>Investigating the temporal dynamics of natural image processing using event-related potentials (ERPs) has a long tradition in object recognition research. In a classical Go-NoGo task two characteristic effects have been emphasized: an <span class="hlt">early</span> task independent category effect and a later task-dependent target effect. Here, we set out to use this well-established Go-NoGo paradigm to study the time course of material categorization. Material perception has gained more and more interest over the years as its importance in natural viewing conditions has been ignored for a long time. In addition to analyzing standard ERPs, we conducted a single trial ERP pattern analysis. To validate this procedure, we also measured ERPs in two object categories (people and animals). Our linear classification procedure was able to largely capture the overall pattern of results from the canonical analysis of the ERPs and even extend it. We replicate the known target effect (<span class="hlt">differential</span> Go-NoGo potential at frontal sites) for the material images. Furthermore, we observe task-independent <span class="hlt">differential</span> activity between the two material categories as <span class="hlt">early</span> as 140 ms after stimulus onset. Using our linear classification approach, we show that material categories can be <span class="hlt">differentiated</span> consistently based on the ERP pattern in single trials around 100 ms after stimulus onset, independent of the target-related status. This strengthens the idea of <span class="hlt">early</span> <span class="hlt">differential</span> visual processing of material categories independent of the task, probably due to differences in low-level image properties and suggests pattern classification of ERP topographies as a strong instrument for investigating electrophysiological brain activity. © 2014 ARVO.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T42C..03V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T42C..03V"><span>Uppermost <span class="hlt">Mantle</span> Deformation and Hydration Beneath the Gorda Plate Inferred from Pn Travel-times</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>VanderBeek, B. P.; Toomey, D. R.</p> <p>2017-12-01</p> <p>Deformation of the uppermost oceanic <span class="hlt">mantle</span> is thought to occur primarily in response to divergence beneath mid-ocean ridges with little subsequent deformation off-axis. A notable exception to this is the Gorda plate where sinuous magnetic anomalies and numerous intra-plate earthquakes indicate diffuse, plate-wide deformation. Thus, the Gorda region provides a natural laboratory to investigate the non-rigid behavior of tectonic plates. We invert Pn (the seismic head wave refracted below the Moho) arrival times from 770 local earthquakes for epicentral and <span class="hlt">mantle</span> anisotropic velocity parameters to understand how the surficial pattern of deformation translates into the uppermost 10 km of the <span class="hlt">mantle</span>. Specifically, we ask does the pattern of seismic anisotropy reflect spreading-induced fabrics or has it been re-worked by extensive deformation of the Gorda plate? If it has been re-worked, does it reflect pervasive faulting of the uppermost <span class="hlt">mantle</span> or plate-scale ductile deformation? And, are isotropic velocities anomalously slow suggesting significant <span class="hlt">mantle</span> hydration? Preliminary results show that the average <span class="hlt">mantle</span> velocity beneath Gorda is 7.55 km/s. Velocities vary azimuthally by 4% and the fast-propagation direction is sub-parallel to Pacific absolute plate motion (APM). In comparison, the uppermost <span class="hlt">mantle</span> beneath the Juan de Fuca (JdF) plate is characterized by 4.6% anisotropy with a mean velocity of 7.85 km/s [VanderBeek and Toomey, 2017]; the fast propagation direction trends between the paleo-spreading direction and JdF APM. The reduced Gorda velocities may indicate a greater extent of fault-controlled hydration of the shallow <span class="hlt">mantle</span> compared to the JdF plate. In both regions, the anisotropic structure argues against the notion that shallow <span class="hlt">mantle</span> deformation ceases away from the ridge. Instead, shearing across Gorda due to <span class="hlt">differential</span> motion between the Pacific and JdF plates [e.g. Bodmer et al., 2015] may cause broad scale ductile deformation and the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012E%26PSL.321..198H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012E%26PSL.321..198H"><span>Iron isotopes in ancient and modern komatiites: Evidence in support of an oxidised <span class="hlt">mantle</span> from Archean to present</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hibbert, K. E. J.; Williams, H. M.; Kerr, A. C.; Puchtel, I. S.</p> <p>2012-03-01</p> <p>The <span class="hlt">mantle</span> of the modern Earth is relatively oxidised compared to the initially reducing conditions inferred for core formation. The timing of the oxidation of the <span class="hlt">mantle</span> is not conclusively resolved but has important implications for the timing of the development of the hydrosphere and atmosphere. In order to examine the timing of this oxidation event, we present iron isotope data from three exceptionally well preserved komatiite localities, Belingwe (2.7 Ga), Vetreny (2.4 Ga) and Gorgona (0.089 Ga). Measurements of Fe isotope compositions of whole-rock samples are complemented by the analysis of olivine, spinel and pyroxene separates. Bulk-rock and olivine Fe isotope compositions (δ57Fe) define clear linear correlations with indicators of magmatic <span class="hlt">differentiation</span> (Mg#, Cr#). The mean Fe isotope compositions of the 2.7-2.4 Ga and 0.089 Ga samples are statistically distinct and this difference can be explained by greater extent of partial melting represented by the older samples and higher <span class="hlt">mantle</span> ambient temperatures in the Archean and <span class="hlt">early</span> Proterozoic relative to the present day. Significantly, samples of all ages define continuous positive linear correlations between bulk rock δ57Fe and V/Sc and δ57Fe and V, and between V/Sc and V with TiO2, providing evidence for the incompatible behaviour of V (relative to Sc) and of isotopically heavy Fe. Partial melting models calculated using partition coefficients for V at oxygen fugacities (fO2s) of 0 and + 1 relative to the fayalite-magnetite-quartz buffer (FMQ) best match the data arrays, which are defined by all samples, from late Archean to Tertiary. These data, therefore, provide evidence for komatiite generation under moderately oxidising conditions since the late Archean, and argue against a change in <span class="hlt">mantle</span> fO2 concomitant with atmospheric oxygenation at ~ 2.4 Ga.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.228....1P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.228....1P"><span>182W and HSE constraints from 2.7 Ga komatiites on the heterogeneous nature of the Archean <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Puchtel, Igor S.; Blichert-Toft, Janne; Touboul, Mathieu; Walker, Richard J.</p> <p>2018-05-01</p> <p>While the isotopically heterogeneous nature of the terrestrial <span class="hlt">mantle</span> has long been established, the origin, scale, and longevity of the heterogeneities for different elements and isotopic systems are still debated. Here, we report Nd, Hf, W, and Os isotopic and highly siderophile element (HSE) abundance data for the Boston Creek komatiitic basalt lava flow (BCF) in the 2.7 Ga Abitibi greenstone belt, Canada. This lava flow is characterized by strong depletions in Al and heavy rare earth elements (REE), enrichments in light REE, and initial ε143Nd = +2.5 ± 0.2 and intial ε176Hf = +4.2 ± 0.9 indicative of derivation from a deep <span class="hlt">mantle</span> source with time-integrated suprachondritic Sm/Nd and Lu/Hf ratios. The data plot on the terrestrial Nd-Hf array suggesting minimal involvement of <span class="hlt">early</span> magma ocean processes in the fractionation of lithophile trace elements in the <span class="hlt">mantle</span> source. This conclusion is supported by a mean μ142Nd = -3.8 ± 2.8 that is unresolvable from terrestrial standards. By contrast, the BCF exhibits a positive 182W anomaly (μ182W = +11.7 ± 4.5), yet is characterized by chondritic initial γ187Os = +0.1 ± 0.3 and low inferred source HSE abundances (35 ± 5% of those estimated for the present-day Bulk Silicate Earth, BSE). Collectively, these characteristics are unique among Archean komatiite systems studied so far. The deficit in the HSE, coupled with the chondritic Os isotopic composition, but a positive 182W anomaly, are best explained by derivation of the parental BCF magma from a <span class="hlt">mantle</span> domain characterized by a predominance of HSE-deficient, <span class="hlt">differentiated</span> late accreted material. According to the model presented here, the <span class="hlt">mantle</span> domain that gave rise to the BCF received only ∼35% of the present-day HSE complement in the BSE before becoming isolated from the rest of the convecting <span class="hlt">mantle</span> until the time of komatiite emplacement at 2.72 Ga. These new data provide strong evidence for a highly heterogeneous Archean <span class="hlt">mantle</span> in terms of absolute</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V42A..01C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V42A..01C"><span>A Geochemical View on the Interplay Between Earth's <span class="hlt">Mantle</span> and Crust</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chauvel, C.</p> <p>2017-12-01</p> <p>Over most of Earth history, oceanic and continental crust was created and destroyed. The formation of both types of crust involves the crystallization and <span class="hlt">differentiation</span> of magmas producing by <span class="hlt">mantle</span> melting. Their destruction proceeds by mechanical erosion and weathering above sea level, chemical alteration on the seafloor, and bulk recycling in subduction zones. All these processes enrich of some chemical element and deplete others but each process has its own effect on chemical elements. While the flux of material from <span class="hlt">mantle</span> to crust is well understood, the return flux is much more complex. In contrast to <span class="hlt">mantle</span> processes, erosion, weathering, chemical alteration and sedimentary processes strongly decouple elements such as the rare earths and high-field strength elements due to their different solubilities in surface fluids and mineralogical sorting during transport. Soluble elements such as strontium or uranium are quantitatively transported to the ocean by rivers and decoupled from less soluble elements. Over geological time, such decoupling significantly influences the extent to which chemical elements remain at the Earth's surface or find their way back to the <span class="hlt">mantle</span> through subduction zones. For example, elements like Hf or Nd are retained in heavy minerals on continents whereas U and Sr are transported to the oceans and then in subduction zones to the <span class="hlt">mantle</span>. The consequence is that different radiogenic isotopic systems give disparate age estimates for the continental crust; e.g, Hf ages could be too old. In subduction zones, chemical elements are also decoupled, due to contrasting behavior during dehydration or melting in subducting slabs. The material sent back into the <span class="hlt">mantle</span> is generally enriched in non-soluble elements while most fluid-mobile elements return to the crust. This, in turn, affects the relationship between the Rb-Sr, Sm-Nd, Lu-Hf and U-Th-Pb isotopic systems and creates correlations unlike those based on magmatic processes. By</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950046221&hterms=Open+Field&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DOpen%2BField','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950046221&hterms=Open+Field&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DOpen%2BField"><span>Interplanetary magnetic field control of <span class="hlt">mantle</span> precipitation and associated field-aligned currents</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Xu, Dingan; Kivelson, Margaret G.; Walker, Ray J.; Newell, Patrick T.; Meng, C.-I.</p> <p>1995-01-01</p> <p>Dayside reconnection, which is particularly effective for a southward interplanetary magnetic field (IMF), allows magnetosheath particles to enter the magnetosphere where they form the plasma <span class="hlt">mantle</span>. The motions of the reconnected flux tube produce convective flows in the ionosphere. It is known that the convection patterns in the polar cap are skewed to the dawnside for a positive IMF B(sub y) (or duskside for a negative IMF B(sub y)) in the northern polar cap. Correspondingly, one would expect to find asymmetric distributions of <span class="hlt">mantle</span> particle precipitation, but previous results have been unclear. In this paper the correlation between B(sub y) and the distribution of <span class="hlt">mantle</span> particle precipitation is studied for steady IMF conditions with southward IMF. Ion and electron data from the Defense Meteorological Satellite Program (DMSP) F6 and F7 satellites are used to identify the <span class="hlt">mantle</span> region and IMP 8 is used as a solar wind monitor to characterize the IMF. We study the local time extension of <span class="hlt">mantle</span> precipitation in the prenoon and postnoon regions. We find that, in accordance with theoretical expectations for a positive (negative) IMF B(sub y), <span class="hlt">mantle</span> particle precipitation mainly appears in the prenoon region of the northern (southern) hemisphere. The <span class="hlt">mantle</span> particle precipitation can extend to as <span class="hlt">early</span> as 0600 magnetic local time (MLT) in the prenoon region but extends over a smaller local time region in the postnoon sector (we did not find <span class="hlt">mantle</span> plasma beyond 1600 MLT in our data set although coverage is scant in this area). Magnetometer data from F7 are used to determine whether part of the region 1 current flows on open field lines. We find that at times part of the region 1 sense current extends into the region of <span class="hlt">mantle</span> particle precipitation, and is therefore on open field lines. In other cases, region 1 currents are absent on open field lines. Most of the observed features can be readily interpreted in terms of the open magnetosphere model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910065445&hterms=iodine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Diodine','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910065445&hterms=iodine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Diodine"><span><span class="hlt">Early</span> outgassing of Mars supported by <span class="hlt">differential</span> water solubility of iodine and xenon</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Musselwhite, Donald S.; Drake, Michael J.; Swindle, Timothy D.</p> <p>1991-01-01</p> <p>The Martian atmosphere has a high X-129/Xe-132 ratio compared to the Martian <span class="hlt">mantle</span>. As Xe-129 is the daughter product of the extinct nuclide I-129, a means of fractionating iodine from xenon <span class="hlt">early</span> in Martian history appears necessary to account for the X-129/Xe-132 ratios of its known reservoirs. A model is presented here to account for the Marian xenon data which relies on the very different solubilities of xenon and iodine in water to fractionate them after outgassing. Atmospheric xenon is lost by impact erosion during heavy bombardment, followed by release of Xe-129 produced from I-129 decay in the crust.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGP12A..02Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGP12A..02Y"><span>Spin Transition in the Lower <span class="hlt">Mantle</span>: Deep Learning and Pattern Recognition of Superplumes from the Mid-<span class="hlt">mantle</span> and Mid-<span class="hlt">mantle</span> Slab Stagnation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yuen, D. A.; Shahnas, M. H.; De Hoop, M. V.; Pysklywec, R.</p> <p>2016-12-01</p> <p>The broad, slow seismic anomalies under Africa and Pacific cannot be explained without ambiguity. There is no well-established theory to explain the fast structures prevalent globally in seismic tomographic images that are commonly accepted to be the remnants of fossil slabs at different depths in the <span class="hlt">mantle</span>. The spin transition from high spin to low spin in iron in ferropericlase and perovskite, two major constituents of the lower <span class="hlt">mantle</span> can significantly impact their physical properties. We employ high resolution 2D-axisymmetric and 3D-spherical control volume models to reconcile the influence of the spin transition-induced anomalies in density, thermal expansivity, and bulk modulus in ferropericlase and perovskite on <span class="hlt">mantle</span> dynamics. The model results reveal that the spin transition effects increase the mixing in the lower regions of <span class="hlt">mantle</span>. Depending on the changes of bulk modulus associated with the spin transition, these effects may also cause both stagnation of slabs and rising plumes at mid-<span class="hlt">mantle</span> depths ( 1600 km). The stagnation may be followed by downward or upward penetration of cold or hot <span class="hlt">mantle</span> material, respectively, through an avalanche process. The size of these mid-<span class="hlt">mantle</span> plumes reaches 1500 km across with a radial velocity reaching 20 cm/yr near the seismic transition zone and plume heads exceeding 2500 km across. We will employ a deep-learning algorithm to formulate this challenge as a classification problem where modelling/computation aids in the learning stage for detecting the particular patterns.The parameters based on which the convection models are developed are poorly constrained. There are uncertainties in initial conditions, heterogeneities and boundary conditions in the simulations, which are nonlinear. Thus it is difficult to reconstruct the past configuration over long time scales. In order to extract information and better understand the parameters in <span class="hlt">mantle</span> convection, we employ deep learning algorithm to search for different</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI51B0294C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI51B0294C"><span>Evolution of the lithospheric <span class="hlt">mantle</span> beneath Mt. Baekdu (Changbaishan)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, S. H.; Park, K.; Cho, M.; Lee, D. C.</p> <p>2017-12-01</p> <p>Major and trace element compositions of minerals as well as Sr-Nd-Hf isotopic compositions of clinopyroxenes from spinel peridotite xenoliths entrained in Late Cenozoic trachybasalt from Mt. Baekdu (Changbaishan) were used to elucidate lithospheric <span class="hlt">mantle</span> formation and evolution in the eastern North China Craton (NCC). The analyzed peridotites were mainly spinel lherzolites with rare harzburgites. They consisted of olivine, enstatite, diopside and spinel. Plots of the Cr# in spinel against the Mg# in coexisting olivine or spinel suggested an affinity with abyssal peridotites. Comparisons of Cr# and TiO2 in spinel were also compatible with an abyssal peridotite-like composition; however, harzburgites were slightly enriched in TiO2 because of the reaction with MORB-like melt. Temperatures estimated using two-pyroxene thermometry ranged from 750 to 1,010°C, reflecting their lithospheric <span class="hlt">mantle</span> origin. The REE patterns in clinopyroxenes of the peridotites varied from LREE-depleted to spoon shaped to LREE-enriched, reflecting secondary overprinting effects of metasomatic melts or fluids on the residues from primordial melting. The calculated trace element pattern of metasomatic melt equilibrated with clinopyroxene in Mt. Baekdu peridotite showed strong enrichment in LILEs, Th and U together with slight fractionation in HREEs and considerable depletion in Nb and Ti. The Sr-Nd-Hf isotopic compositions of clinopyroxenes separated from the peridotites varied from more depleted than present-day MORB to bulk Earth values. However, some clinopyroxene showed a decoupling between Nd and Sr isotopes, deviating from the <span class="hlt">mantle</span> array with a high 87Sr/86Sr ratio. This sample also showed a significant Nd-Hf isotope decoupling lying well above the <span class="hlt">mantle</span> array. The Lu-Hf and Sm-Nd model ages of residual clinopyroxenes yielded <span class="hlt">Early</span> Proterozoic to Phanerozoic ages. No signature of Archean cratonic <span class="hlt">mantle</span> was present. Therefore, Mt. Baekdu peridotite is residual lithospheric <span class="hlt">mantle</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.2643W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.2643W"><span><span class="hlt">Mantle</span> convection and the distribution of geochemical reservoirs in the silicate shell of the Earth</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Walzer, Uwe; Hendel, Roland</p> <p>2010-05-01</p> <p>We present a dynamic 3-D spherical-shell model of <span class="hlt">mantle</span> convection and the evolution of the chemical reservoirs of the Earth`s silicate shell. Chemical <span class="hlt">differentiation</span>, convection, stirring and thermal evolution constitute an inseparable dynamic system. Our model is based on the solution of the balance equations of mass, momentum, energy, angular momentum, and four sums of the number of atoms of the pairs 238U-206Pb, 235U-207Pb, 232Th-208Pb, and 40K-40Ar. Similar to the present model, the continental crust of the real Earth was not produced entirely at the start of the evolution but developed episodically in batches [1-7]. The details of the continental distribution of the model are largely stochastic, but the spectral properties are quite similar to the present real Earth. The calculated Figures reveal that the modeled present-day <span class="hlt">mantle</span> has no chemical stratification but we find a marble-cake structure. If we compare the observational results of the present-day proportion of depleted MORB <span class="hlt">mantle</span> with the model then we find a similar order of magnitude. The MORB source dominates under the lithosphere. In our model, there are nowhere pure unblended reservoirs in the <span class="hlt">mantle</span>. It is, however, remarkable that, in spite of 4500 Ma of solid-state <span class="hlt">mantle</span> convection, certain strong concentrations of distributed chemical reservoirs continue to persist in certain volumes, although without sharp abundance boundaries. We deal with the question of predictable and stochastic portions of the phenomena. Although the convective flow patterns and the chemical <span class="hlt">differentiation</span> of oceanic plateaus are coupled, the evolution of time-dependent Rayleigh number, Rat , is relatively well predictable and the stochastic parts of the Rat(t)-curves are small. Regarding the juvenile growth rates of the total mass of the continents, predictions are possible only in the first epoch of the evolution. Later on, the distribution of the continental-growth episodes is increasingly stochastic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24695310','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24695310"><span>Highly siderophile elements in Earth's <span class="hlt">mantle</span> as a clock for the Moon-forming impact.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jacobson, Seth A; Morbidelli, Alessandro; Raymond, Sean N; O'Brien, David P; Walsh, Kevin J; Rubie, David C</p> <p>2014-04-03</p> <p>According to the generally accepted scenario, the last giant impact on Earth formed the Moon and initiated the final phase of core formation by melting Earth's <span class="hlt">mantle</span>. A key goal of geochemistry is to date this event, but different ages have been proposed. Some argue for an <span class="hlt">early</span> Moon-forming event, approximately 30 million years (Myr) after the condensation of the first solids in the Solar System, whereas others claim a date later than 50 Myr (and possibly as late as around 100 Myr) after condensation. Here we show that a Moon-forming event at 40 Myr after condensation, or earlier, is ruled out at a 99.9 per cent confidence level. We use a large number of N-body simulations to demonstrate a relationship between the time of the last giant impact on an Earth-like planet and the amount of mass subsequently added during the era known as Late Accretion. As the last giant impact is delayed, the late-accreted mass decreases in a predictable fashion. This relationship exists within both the classical scenario and the Grand Tack scenario of terrestrial planet formation, and holds across a wide range of disk conditions. The concentration of highly siderophile elements (HSEs) in Earth's <span class="hlt">mantle</span> constrains the mass of chondritic material added to Earth during Late Accretion. Using HSE abundance measurements, we determine a Moon-formation age of 95 ± 32 Myr after condensation. The possibility exists that some late projectiles were <span class="hlt">differentiated</span> and left an incomplete HSE record in Earth's <span class="hlt">mantle</span>. Even in this case, various isotopic constraints strongly suggest that the late-accreted mass did not exceed 1 per cent of Earth's mass, and so the HSE clock still robustly limits the timing of the Moon-forming event to significantly later than 40 Myr after condensation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LPICo2084.4018H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LPICo2084.4018H"><span>Unique NWA 11119/11558, NWA 7325 (and Pairs) and Almahata Sitta Individuals MS-MU 011/035: New Light on Very <span class="hlt">Early</span> Parent Body <span class="hlt">Differentiation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hoffmann, V. H.; Mikouchi, T.; Hochleitner, R.; Kaliwoda, M.; Wimmer, K.</p> <p>2018-05-01</p> <p>The preliminary results would support our conclusion that these unique meteorites may probe the crust/upper <span class="hlt">mantle</span> of a yet unknown planetary body which existed only in a very <span class="hlt">early</span> period of time of our planetary system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1986E%26PSL..81...29R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1986E%26PSL..81...29R"><span>Extreme isotopic variations in the upper <span class="hlt">mantle</span>: evidence from Ronda</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reisberg, Laurie; Zindler, Alan</p> <p>1986-12-01</p> <p>The Ronda Ultramafic Complex in southern Spain represents a piece of the Earth's <span class="hlt">mantle</span> which has been tectonically emplaced into the crust. Nd and Sr isotopic analyses are presented for leached, hand-picked Cr-diopside separates prepared from 15 rock and 18 river sediment samples from Ronda. These results demonstrate that within this small, contiguous body there exists the entire range of Nd isotopic compositions, and much of the range of Sr compositions, found in rocks derived from the sub-oceanic <span class="hlt">mantle</span>. The sediment cpx samples show that the average isotopic composition of the massif becomes progressively less "depleted" moving from SW to NE along the long axis of the massif. The rock cpx samples document 143Nd/ 144Nd variations from 0.5129 to 0.5126 and 87Sr/ 86Sr variations from 0.7031 to 0.7039 within a uniform outcrop less than 10 m in extent. Thus, extreme isotopic fluctuations exist over a wide range of wavelengths. Sr and Nd isotopes are generally inversely correlated, forming a trend on a Nd-Sr diagram that sharply crosscuts that of the "<span class="hlt">mantle</span> array". Many of the 143Nd/ 144Nd values, and all of the Sm/Nd values, from one section of the massif are lower than that SCV015SCV0 of the bulk earth, implying that this region existed, or was influenced by a component which existed, in a LREE-enriched environment for a significant period of time. Among the sediment cpxs there is a positive correlation between 143Nd/ 144Nd and 147Sm/ 144Nd. The rock cpx separates display considerably more scatter. A simple, single-stage <span class="hlt">differentiation</span> event starting with a uniform <span class="hlt">mantle</span> source cannot explain these results. At least one episode of mixing with a LREE-enriched component is required. If these results from Ronda are typical of the upper <span class="hlt">mantle</span>, basalts with different isotopic compositions need not derive from spatially separated <span class="hlt">mantle</span> sources.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DPS....4911025T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DPS....4911025T"><span>Searching for a <span class="hlt">Differentiated</span> Asteroid Family: A Spectral Survey of the Massalia, Merxia, and Agnia Families</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thomas, Cristina A.; Moskovitz, Nicholas; Lim, Lucy F.; Trilling, David E.</p> <p>2017-10-01</p> <p>Asteroid families were formed by catastrophic collisions or large cratering events that caused fragmentation of the parent body and ejection of asteroidal fragments with velocities sufficient to prevent re-accretion. Due to these formation processes, asteroid families provide us with the opportunity to probe the interiors of the former parent bodies. <span class="hlt">Differentiation</span> of a large initially chondritic parent body is expected to result in an “onion shell" object with an iron-nickel core, a thick olivine-dominated <span class="hlt">mantle</span>, and a thin plagioclase/pyroxene crust. However, most asteroid families tend to show similar spectra (and therefore composition) among the members. Spectroscopic studies have observed a paucity of metal-like materials and olivine-dominated assemblages within Main Belt asteroid families.The deficit of olivine-rich <span class="hlt">mantle</span> material in the meteorite record and in asteroid observations is known as the “Missing <span class="hlt">Mantle</span>" problem. For years the best explanation has been the “battered to bits" hypothesis: <span class="hlt">differentiated</span> parent bodies (aside from Vesta) were disrupted very <span class="hlt">early</span> in the Solar System and the olivine-rich material was collisionally broken down over time. Alternatively, Elkins-Tanton et al. (2013) have suggested that previous work has overestimated the amount of olivine produced by the <span class="hlt">differentiation</span> of a chondritic parent body.We have completed a visible and near-infrared wavelength spectral survey of asteroids in the Massalia, Merxia, and Agnia S-type Main Belt asteroid families. These families were carefully chosen for the spectroscopic survey because they have compositions most closely associated with a history of thermal metamorphism and because they represent a range of collisional formation scenarios. Additionally, members of the Merxia and Agnia families were identified as products of <span class="hlt">differentiation</span> by Sunshine et al. (2004).Our spectral analyses suggest that the observed families contain products of partial <span class="hlt">differentiation</span>. We will</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940019897','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940019897"><span>Lunar mare volcanism: Mixing of distinct, <span class="hlt">mantle</span> source regions with KREEP-like component</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shervais, John W.; Vetter, Scott K.</p> <p>1993-01-01</p> <p>Mare basalts comprise less than 1% of the lunar crust, but they constitute our primary source of information on the moon's upper <span class="hlt">mantle</span>. Compositional variations between mare basalt suites reflect variations in the mineralogical and geochemical composition of the lunar <span class="hlt">mantle</span> which formed during <span class="hlt">early</span> lunar <span class="hlt">differentiation</span> (4.5-4.4 AE). Three broad suites of mare basalt are recognized: very low-Ti (VLT) basalts with TiO2 less than 1 wt%, low-Ti basalts with TiO2 = 2-4 wt%, and high-Ti basalts with TiO2 = 10-14 wt%. Important subgroups include the Apollo 12 ilmenite basalts (TiO2 = 5-6 wt%), aluminous low-Ti mare basalts (TiO2 = 2-4 wt%, Al2O3 = 10-14 wt%), and the newly discovered Very High potassium (VHK) aluminous low-Ti basalts, with K2O = 0.4-1.5 wt%. The mare basalt source region has geochemical characteristics complementary to the highlands crust and is generally thought to consist of mafic cumulates from the magma ocean which formed the felsic crust by feldspar flotation. The progressive enrichment of mare basalts in Fe/Mg, alkalis, and incompatible trace elements in the sequence VLT basalt yields low-Ti basalt yields high-Ti basalt is explained by the remelting of mafic cumulates formed at progressively shallower depths in the evolving magma ocean. This model is also consistent with the observed decrease in compatible element concentrations and the progressive increase in negative Eu anomalies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P51A2130M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P51A2130M"><span>On the effects of planetary rotation on the <span class="hlt">differentiation</span> of a terrestrial magma ocean in spherical geometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maas, C.; Hansen, U.</p> <p>2016-12-01</p> <p>During a later stage of the accretion about 4.5 billion years ago the <span class="hlt">early</span> Earth experienced several giant impacts that lead to one or more deep terrestrial magma oceans of global extent. The crystallization of these vigorously convecting magma oceans is of key importance for the chemical structure of the Earth, the subsequent <span class="hlt">mantle</span> evolution as well as for the initial conditions for the onset of plate tectonics. Due to the fast planetary rotation of the <span class="hlt">early</span> Earth and the small magma viscosity, rotation probably had a profound effect on <span class="hlt">early</span> <span class="hlt">differentiation</span> processes of the <span class="hlt">mantle</span> and could for example influence the presence and distribution of chemical heterogeneities in the Earth <span class="hlt">mantle</span> [e.g. Matyska et al., 1994, Garnero and McNamara, 2008].Our previous work in Cartesian geometry studied crystal settling in the polar and equatorial regions separately from each other and revealed a strong influence of rotation as well as of latitude on the crystal settling in a terrestrial magma ocean [Maas and Hansen, 2015]. Based on the preceding study we recently developed a spherical shell model that allows for new insights into the crystal settling in-between the pole and the equator as well as the migration of crystals between these regions. Further the spherical model allows us to include the centrifugal force on the crystals, which significantly affects the lateral and radial distribution of crystals. All in all the first numerical experiments in spherical geometry agree with the results of Maas and Hansen [2015] and show that the crystal distribution crucially depends on latitude, rotational strength and crystal density. ReferencesE. J. Garnero and A. K. McNamara. Structure and dynamics of earth's lower <span class="hlt">mantle</span>. Science, 320(5876):626-628, 2008.C. Maas and U. Hansen. Effects of earth's rotation on the <span class="hlt">early</span> dierentiation of a terrestrial magma ocean. Journal of Geophysical Research: Solid Earth, 120(11):7508-7525, 2015.C. Matyska, J. Moser, and D. A. Yuen. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013GeoRL..40.3562M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013GeoRL..40.3562M"><span><span class="hlt">Mantle</span> transition zone thinning beneath eastern Africa: Evidence for a whole-<span class="hlt">mantle</span> superplume structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mulibo, Gabriel D.; Nyblade, Andrew A.</p> <p>2013-07-01</p> <p>to S conversions from the 410 and 660 km discontinuities observed in receiver function stacks reveal a <span class="hlt">mantle</span> transition zone that is ~30-40 km thinner than the global average in a region ~200-400 km wide extending in a SW-NE direction from central Zambia, across Tanzania and into Kenya. The thinning of the transition zone indicates a ~190-300 K thermal anomaly in the same location where seismic tomography models suggest that the lower <span class="hlt">mantle</span> African superplume structure connects to thermally perturbed upper <span class="hlt">mantle</span> beneath eastern Africa. This finding provides compelling evidence for the existence of a continuous thermal structure extending from the core-<span class="hlt">mantle</span> boundary to the surface associated with the African superplume.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.V11A2488R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.V11A2488R"><span>Compositional Variation of Terrestrial <span class="hlt">Mantle</span> Apatites and Implications for the Halogen and Water Budgets of the Terrestrial <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roden, M.; Patino Douce, A. E.; Chaumba, J. B.; Fleisher, C.; Yogodzinski, G. M.</p> <p>2011-12-01</p> <p> with merrillite are typically Cl- and F-rich in the case of Mars but F-rich in the case of the Moon and Vesta (2-4). In a single reported example of terrestrial <span class="hlt">mantle</span> xenoliths containing apatite and and a similar volatile-poor Ca-phosphate, whitlockite, the apatite contained significant Cl and H2O but was F-rich and similar to some lunar apatites. Our thermodynamic analysis of apatite-merrillite equilibria suggests that high phosphorous chemical potentials combined with high halogen and low water fugacities are required for the coexistence of a volatile-poor Ca-phosphate with apatite, and point out the relatively unique and typically water-rich nature of the upper <span class="hlt">mantle</span> of the Earth compared to other <span class="hlt">differentiated</span> planetary bodies. References 1. S. O'Reilly & W. Griffin, 2000, Lithos 53: 217. 2. A. Patiño Douce et al., 2011, Chem Geol. in press 3. F. McCubbin et al. 2009, LPSC abs 2246 4. A. Sarafian et al. 2011, Meteor. Soc. Abs 5023</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatGe..10..400S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatGe..10..400S"><span>Geodynamics: Hot <span class="hlt">mantle</span> rising</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shorttle, Oliver</p> <p>2017-06-01</p> <p>The long-term cooling of Earth's <span class="hlt">mantle</span> is recorded in the declining temperature and volume of its volcanic outpourings over time. However, analyses of 89-million-year-old lavas from Costa Rica suggest that extremely hot <span class="hlt">mantle</span> still lurks below.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030110807&hterms=sharma&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsharma','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030110807&hterms=sharma&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsharma"><span>No Nd-142 Excess in the <span class="hlt">Early</span> Archean Isua Gneiss IE 715-28</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Papanastassiou, D. A.; Sharma, M.; Ngo, H. H.; Wasserburg, G. J.; Dymek, R. F.</p> <p>2003-01-01</p> <p>There is abundant evidence for the existence of 146Sm in the <span class="hlt">early</span> solar system and for preservation of effects in the 146Sm-142Nd system in <span class="hlt">differentiated</span> meteorites ([1]; see recent discussion in Stewart et al. 1994). Information from the 182Hf-182W system, as revised by new careful work [2-3] also indicates that the Earth s core formed relatively <span class="hlt">early</span>. It is in principle possible for <span class="hlt">early</span>-formed crust and <span class="hlt">mantle</span> reservoirs on Earth to have preserved evidence for 146Sm if such reservoirs were produced with high Sm/Nd fractionation and if they have remained isolated and closed since 4.3 Ga. The mean life of 146Sm of 149 Ma is sufficiently long to make this an intriguing possibility.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=34063','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=34063"><span><span class="hlt">Mantle</span> dynamics and seismic tomography</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Tanimoto, Toshiro; Lay, Thorne</p> <p>2000-01-01</p> <p>Three-dimensional imaging of the Earth's interior, called seismic tomography, has achieved breakthrough advances in the last two decades, revealing fundamental geodynamical processes throughout the Earth's <span class="hlt">mantle</span> and core. Convective circulation of the entire <span class="hlt">mantle</span> is taking place, with subducted oceanic lithosphere sinking into the lower <span class="hlt">mantle</span>, overcoming the resistance to penetration provided by the phase boundary near 650-km depth that separates the upper and lower <span class="hlt">mantle</span>. The boundary layer at the base of the <span class="hlt">mantle</span> has been revealed to have complex structure, involving local stratification, extensive structural anisotropy, and massive regions of partial melt. The Earth's high Rayleigh number convective regime now is recognized to be much more interesting and complex than suggested by textbook cartoons, and continued advances in seismic tomography, geodynamical modeling, and high-pressure–high-temperature mineral physics will be needed to fully quantify the complex dynamics of our planet's interior. PMID:11035784</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1512499P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1512499P"><span>Consequences of an unstable chemical stratification on <span class="hlt">mantle</span> dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Plesa, Ana-Catalina; Tosi, Nicola; Breuer, Doris</p> <p>2013-04-01</p> <p><span class="hlt">Early</span> in the history of terrestrial planets, the fractional crystallization of primordial magma oceans may have led to the formation of large scale chemical heterogeneities. These may have been preserved over the entire planetary evolution as suggested for Mars by the isotopic analysis of the so-called SNC meteorites. The fractional crystallization of a magma ocean leads to a chemical stratification characterized by a progressive enrichment in heavy elements from the core-<span class="hlt">mantle</span> boundary to the surface. This results in an unstable configuration that causes the overturn of the <span class="hlt">mantle</span> and the subsequent formation of a stable chemical layering. Assuming scaling parameters appropriate for Mars, we first performed simulations of 2D thermo-chemical convection in Cartesian geometry with the numerical code YACC [1]. We investigated systems heated either solely from below or from within by varying systematically the buoyancy ratio B, which measures the relative importance of chemical to thermal buoyancy, and the <span class="hlt">mantle</span> rheology, by considering systems with constant, strongly temperature-dependent and plastic viscosity. We ran a large set of simulations spanning a wide parameter space in order to understand the basic physics governing the magma ocean cumulate overturn and its consequence on <span class="hlt">mantle</span> dynamics. Moreover, we derived scaling laws that relate the time over which chemical heterogeneities can be preserved (mixing time) and the critical yield stress (maximal yield stress that allows the lithosphere to undergo brittle failure) to the buoyancy ratio. We have found that the mixing time increases exponentially with B, while the critical yield stress shows a linear dependence. We investigated then Mars' <span class="hlt">early</span> thermo-chemical evolution using the code GAIA in a 2D cylindrical geometry [2] and assuming a detailed magma ocean crystallization sequence as obtained from geochemical modeling [3]. We used an initial composition profile adapted from [3], accounted for an exothermic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Litho.300...72B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Litho.300...72B"><span>Refertilized <span class="hlt">mantle</span> keel below the Southern Alps domain (North-East Italy): Evidence from Marosticano refractory <span class="hlt">mantle</span> peridotites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brombin, Valentina; Bonadiman, Costanza; Coltorti, Massimo; Fahnestock, M. Florencia; Bryce, Julia G.; Marzoli, Andrea</p> <p>2018-02-01</p> <p>The Veneto Volcanic Province (VVP), a Cenozoic magmatic province in northeastern Italy, is one of the widest volcanic areas of the Adria plate. It consists of five main magmatic districts, and its most primitive products commonly host <span class="hlt">mantle</span> xenoliths. In this study, we present a newly discovered xenolith suite from the Marosticano district that contains peridotites with compositional characteristics of mineral assemblages that provide insight into an unexpected nature of the sub-continental lithospheric <span class="hlt">mantle</span> (SCLM) of the Adria plate. In contrast to xenoliths from other VVP sites previously studied (i.e., Val d'Adige and Lessini Mts.), Marosticano xenoliths exhibit highly refractory compositions typical of on-craton peridotites. High olivine forsteritic contents (Fo: 91-93) indicate high degrees of partial melting (> 25%) that should have been associated with the complete consumption of clinopyroxene. Major and trace element compositions further link these peridotite fragments to <span class="hlt">early</span> Proterozoic cratonic <span class="hlt">mantle</span>. The occurrence of clinopyroxene within such rocks suggests Marosticano clinopyroxene testify to a metasomatic legacy. The i) LREE-enrichments of Marosticano clinopyroxene and ii) the dissolved CO2 mole fractions (up to 1.0) for the inferred clinopyroxene-forming melt are consistent with carbonatite/CO2-rich silicatic melts as metasomatic agents. The latter could be responsible for the equilibrium temperatures (1033-1117 °C) and oxidizing conditions [ΔlogfO2 (FMQ) = - 0.6 - + 1.1], anomalously high for a cratonic environment but similar to the off-craton VVP xenoliths. The cratonic signature and carbonatite/CO2-rich silicate metasomatism found together in the Marosticano <span class="hlt">mantle</span> xenoliths reveal that ancient features can be preserved in SCLM in a young, active geodynamic setting such as the Adria plate boundary. In this framework Lessini Mts. and Val d'Adige xenoliths could be interpreted as circumcratonic reminiscent domains affected by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V24C..04L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V24C..04L"><span>Facilitating atmosphere oxidation through <span class="hlt">mantle</span> convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, K. K. M.; Gu, T.; Creasy, N.; Li, M.; McCammon, C. A.; Girard, J.</p> <p>2017-12-01</p> <p>Earth's <span class="hlt">mantle</span> connects the surface with the deep interior through convection, and the evolution of its redox state will affect the distribution of siderophile elements, recycling of refractory isotopes, and the oxidation state of the atmosphere through volcanic outgassing. While the rise of oxygen in the atmosphere, i.e., the Great Oxidation Event (GOE) occurred 2.4 billion years ago (Ga), multiple lines of evidence point to oxygen production in the atmosphere well before 2.4 Ga. In contrast to the fluctuations of atmospheric oxygen, vanadium in Archean <span class="hlt">mantle</span> lithosphere suggests that the <span class="hlt">mantle</span> redox state has been constant for 3.5 Ga. Indeed, the connection between the redox state of the deep Earth and the atmosphere is enigmatic as is the effect of redox state on <span class="hlt">mantle</span> dynamics. Here we show a redox-induced density contrast affects <span class="hlt">mantle</span> convection and may potentially cause the oxidation of the upper <span class="hlt">mantle</span>. We compressed two synthetic enstatite chondritic samples with identical bulk compositions but formed under different oxygen fugacities (fO2) to lower <span class="hlt">mantle</span> pressures and temperatures and find Al2O3 forms its own phase separate from the dominant bridgmanite phase in the more reduced composition, in contrast to a more Al-rich, bridgmanite-dominated assemblage for a more oxidized starting composition. As a result, the reduced material is 1-1.5% denser than the oxidized material. Subsequent experiments on other plausible <span class="hlt">mantle</span> compositions, which differ only in redox state of the starting glass materials, show similar results: distinct mineral assemblages and density contrasts up to 4%. Our geodynamic simulations suggest that such a density contrast causes a rapid ascent and accumulation of oxidized material in the upper <span class="hlt">mantle</span>, with descent of the denser reduced material to the core-<span class="hlt">mantle</span> boundary. The resulting heterogeneous redox conditions in Earth's interior may have contributed to the large low-shear velocity provinces in the lower <span class="hlt">mantle</span> and the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.V42B..05H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.V42B..05H"><span>The Contribution of Recycled Crust to <span class="hlt">Mantle</span> Inventories of Trace elements, Hydrogen, and Carbon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hirschmann, M. M.</p> <p>2008-12-01</p> <p>It is clear that crustal recycling has had a profound impact on the non-volatile trace element budget of the <span class="hlt">mantle</span>, but its impact on <span class="hlt">mantle</span> carbon and hydrogen are less well-understood. If an active crust recycling mechanism such as plate tectonics has operated since <span class="hlt">early</span> in Earth history, and if magmatic production has diminished through time according to the decay in heat production, then the mass of recycled crust may dominate the <span class="hlt">mantle</span> inventory of many trace elements. For example, Earth evolution models suggest time- integrated crust production equal to 7-15% of the <span class="hlt">mantle</span>, and this accounts for ~25 to >100% of the <span class="hlt">mantle</span> inventory of LREE and HFSE elements, depending on the mean concentration of these elements in the average crust produced. A key question is the role of recycling in the budgets of H and C. Consideration of the near-surface reservoirs and fluxes of C and H indicates that these principal volatiles have residence times of billions of years, and so they may be grouped with continental crust as a single long-lived near-surface geochemical reservoir (NSGR) that results from extraction from the <span class="hlt">mantle</span> by melting combined with selective return to the <span class="hlt">mantle</span> by subduction. The primitive <span class="hlt">mantle</span>-normalized mass concentrations of H and C and the NSGR are equal to 90-200 and 1.5-18, respectively, with the primitive <span class="hlt">mantle</span> inventories of H and C as the chief uncertainty. When the NSGR is plotted on a compatibility diagram, H and C form extreme positive and negative anomalies relative to their mineral/melt partition coefficients, meaning that there is much more H and much less C in the NSGR than would be predicted based solely on their magmatic flux from the <span class="hlt">mantle</span>. The most straightforward interpretation is that H subduction is highly inefficient, but that recycled C amounts to at least half and possibly dominates the <span class="hlt">mantle</span> C budget. This interpretation is supported by H/C mass ratios of the <span class="hlt">mantle</span> sources inferred from undegassed oceanic basalts (H</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900005420','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900005420"><span>Workshop on the Archean <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ashwal, L. D. (Editor)</p> <p>1989-01-01</p> <p>The Workshop on the Archaen <span class="hlt">mantle</span> considers and discusses evidence for the nature of earth's Archaen <span class="hlt">mantle</span>, including its composition, age and structure, influence on the origin and evolution of earth's crust, and relationship to <span class="hlt">mantle</span> and crustal evolution of the other terrestrial planets. The summaries of presentations and discussions are based on recordings made during the workshop and on notes taken by those who agreed to serve as summarizers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000AREPS..28..391N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000AREPS..28..391N"><span>Seismic Imaging of <span class="hlt">Mantle</span> Plumes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nataf, Henri-Claude</p> <p></p> <p>The <span class="hlt">mantle</span> plume hypothesis was proposed thirty years ago by Jason Morgan to explain hotspot volcanoes such as Hawaii. A thermal diapir (or plume) rises from the thermal boundary layer at the base of the <span class="hlt">mantle</span> and produces a chain of volcanoes as a plate moves on top of it. The idea is very attractive, but direct evidence for actual plumes is weak, and many questions remain unanswered. With the great improvement of seismic imagery in the past ten years, new prospects have arisen. <span class="hlt">Mantle</span> plumes are expected to be rather narrow, and their detection by seismic techniques requires specific developments as well as dedicated field experiments. Regional travel-time tomography has provided good evidence for plumes in the upper <span class="hlt">mantle</span> beneath a few hotspots (Yellowstone, Massif Central, Iceland). Beneath Hawaii and Iceland, the plume can be detected in the transition zone because it deflects the seismic discontinuities at 410 and 660 km depths. In the lower <span class="hlt">mantle</span>, plumes are very difficult to detect, so specific methods have been worked out for this purpose. There are hints of a plume beneath the weak Bowie hotspot, as well as intriguing observations for Hawaii. Beneath Iceland, high-resolution tomography has just revealed a wide and meandering plume-like structure extending from the core-<span class="hlt">mantle</span> boundary up to the surface. Among the many phenomena that seem to take place in the lowermost <span class="hlt">mantle</span> (or D''), there are also signs there of the presence of plumes. In this article I review the main results obtained so far from these studies and discuss their implications for plume dynamics. Seismic imaging of <span class="hlt">mantle</span> plumes is still in its infancy but should soon become a turbulent teenager.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.T44B..02Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.T44B..02Z"><span>Os and HSE of the hot upper <span class="hlt">mantle</span> beneath southern Tibet: Indian <span class="hlt">mantle</span> affinity?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Z.; Dale, C. W.; Pearson, D. G.; Niu, Y.; Zhu, D.; Mo, X.</p> <p>2011-12-01</p> <p>The subduction of the Indian plate (including cratonic continental crust and/or upper <span class="hlt">mantle</span>) beneath southern Tibet is widely accepted from both geological and geophysical studies. <span class="hlt">Mantle</span>-derived xenoliths from this region provide a means of directly investigating the <span class="hlt">mantle</span> underlying the southern part of the plateau. Studies of xenoliths hosted in the Sailipu ultrapotassic volcanic rocks, erupted at ~17 Ma, have indicated that the subcontinental <span class="hlt">mantle</span> of southern Tibetan Plateau is hot and strongly influenced by metasomatism (Zhao et al., 2008a, b; Liu et al., 2011). Here we report comprehensive EPMA and LA-ICP-MS major and trace element data for the Sailipu xenoliths and also whole rock Os isotope and HSE data in order to constrain the depletion history of the <span class="hlt">mantle</span> and to identify the presence of any potential Indian cratonic <span class="hlt">mantle</span>. The xenoliths, ranging in size from 0.5cm to 1.5cm in diameter, are mostly peridotites. The calculated temperatures are 1010-1230°C at the given pressures of ~1.6-2.0 GPa (n=47). These P-T conditions are similar to rift-related upper <span class="hlt">mantle</span> regimes (e.g. Kenya), indicating the influence of regional extension beneath southern Tibet in the Miocene. A series of compositional discriminations for minerals (Cpx, Opx, Ol, and Phl), e.g. Fo<90, suggest that the xenoliths are non-cratonic spinel-peridotite (cratonic peridotite olivine Fo> ~91), with a clear metasomatic signature We obtained Os isotope data and abundances of highly siderophile elements (HSE, including Os, Ir, Ru, Pt, Pd and Re) on a set of six olivine-dominated peridotite samples from Sailipu volcanics, less than 1 cm in dimension. They allow us to further constrain the nature and state of the upper <span class="hlt">mantle</span> beneath the southern Tibet. Sailipu samples display low total HSE abundances (Os+Ir+Ru+Pt+Pd+Re) ranging from 8.7 to 25 ppb, with nearly constant Os, Ir , and Ru, but rather varied Pt (2-13), Pd (0.4-5.2), and Re (0.01-0.5). Chondrite-normalised Pd/Ir ratios range from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMDI43A4346R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMDI43A4346R"><span>Of <span class="hlt">Mantle</span> Plumes, Their Existence, and Their Nature: Insights from Whole <span class="hlt">Mantle</span> SEM-Based Seismic Waveform Tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Romanowicz, B. A.; French, S. W.</p> <p>2014-12-01</p> <p>Many questions remain on the detailed morphology of <span class="hlt">mantle</span> convection patterns. While high resolution P wave studies show a variety of subducted slab behaviors, some stagnating in the transition zone, others penetrating into the lower <span class="hlt">mantle</span> (e.g. Fukao & Obayashi, 2013), low velocity structures - the upwelling part of flow - are more difficult to resolve at the same scale. Indeed, depth extent and morphology of the low velocity roots of hotspot volcanoes is still debated, along with the existence of "<span class="hlt">mantle</span> plumes". Using spectral element waveform tomography, we previously constructed a global, radially anisotropic, upper <span class="hlt">mantle</span> Vs model (SEMum2, French et al., 2013) and have now extended it to the whole <span class="hlt">mantle</span> by adding shorter period waveform data (SEMUCB-WM1, French & Romanowicz, GJI, in revision). This model shows long wavelength structure in good agreement with other recent global Vs models derived under stronger approximations (Ritsema et al. 2011; Kustowski, et al. 2008), but exhibits better focused, finer scale structure throughout the <span class="hlt">mantle</span>. SEMUCB-WM1 confirms the presence in all major ocean basins of the quasi-periodic, upper <span class="hlt">mantle</span> low velocity anomalies, previously seen in SEMum2. At the same time, lower <span class="hlt">mantle</span> low velocity structure is dominated by a small number (~15 globally) of quasi-vertical anomalies forming discrete "column"" rooted at the base of the <span class="hlt">mantle</span>. Most columns are positioned near major hotspots, as defined by buoyancy flux, and are wider (~800-1000 km diameter) than expected from the thermal plume model - suggestive of thermo-chemical plumes, which may be stable for long times compared to purely thermal ones. Some columns reach the upper <span class="hlt">mantle</span>, while others deflect horizontally near 1000 km - the same depth where many slabs appear to stagnate. As they reach the transition zone, the wide columnar structure can be lost, as these "plumes" appear to meander through the upper <span class="hlt">mantle</span>, perhaps entrained by more vigorous, lower viscosity</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013E%26PSL.383..153Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013E%26PSL.383..153Z"><span><span class="hlt">Mantle</span> dynamics and generation of a geochemical <span class="hlt">mantle</span> boundary along the East Pacific Rise - Pacific/Antarctic ridge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Guo-Liang; Chen, Li-Hui; Li, Shi-Zhen</p> <p>2013-12-01</p> <p>A large-scale <span class="hlt">mantle</span> compositional discontinuity was identified along the East Pacific Rise (EPR) and the Pacific-Antarctic Ridge (PAR) with an inferred transition located at the EPR 23°S-32°S. Because of the EPR-Easter hotspot interactions in this area, the nature of this geochemical discontinuity remains unclear. IODP Sites U1367 and U1368 drilled into the ocean crust that was accreted at ∼33.5 Ma and ∼13.5 Ma, respectively, between 28°S and 30°S on the EPR. We use lavas from Sites U1367 and U1368 to track this <span class="hlt">mantle</span> discontinuity away from the EPR. The <span class="hlt">mantle</span> sources for basalts at Sites U1367 and U1368 represent, respectively, northern and southern Pacific <span class="hlt">mantle</span> sub-domains in terms of Sr-Nd-Pb-Hf isotopes. The significant isotopic differences between the two IODP sites are consistent with addition of ancient subduction-processed ocean crust to the south Pacific <span class="hlt">mantle</span> sub-domain. Our modeling result shows that a trace element pattern similar to that of U1368 E-MORB can be formed by melting a subduction-processed typical N-MORB. The trace element and isotope compositions for Site U1368 MORBs can be formed by mixing a HIMU <span class="hlt">mantle</span> end-member with Site U1367 MORBs. Comparison of our data with those from the EPR-PAR shows a geochemical <span class="hlt">mantle</span> boundary near the Easter microplate that separates the Pacific upper <span class="hlt">mantle</span> into northern and southern sub-domains. On the basis of reconstruction of initial locations of the ocean crust at the two sites, we find that the <span class="hlt">mantle</span> boundary has moved northward to the Easter microplate since before 33.5 Ma. A model, in which along-axis asthenospheric flow to where asthenosphere consumption is strongest, explains the movement of the apparent <span class="hlt">mantle</span> boundary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V21C2752M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V21C2752M"><span><span class="hlt">Mantle</span> upwelling and trench-parallel <span class="hlt">mantle</span> flow in the northern Cascade arc indicated by basalt geochemistry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mullen, E.; Weis, D.</p> <p>2013-12-01</p> <p>Cascadia offers a unique perspective on arc magma genesis as an end-member ';hot' subduction zone in which relatively little water may be available to promote <span class="hlt">mantle</span> melting. The youngest and hottest subducting crust (~5 Myr at the trench) occurs in the Garibaldi Volcanic Belt, at the northern edge of the subducting Juan de Fuca plate [1]. Geochemical data from GVB primitive basalts provide insights on <span class="hlt">mantle</span> melting where a slab edge coincides with high slab temperatures. In subduction zones worldwide, including the Cascades, basalts are typically calc-alkaline and produced from a depleted <span class="hlt">mantle</span> wedge modified by slab input. However, basalts from volcanic centers overlying the northern slab edge (Salal Glacier and Bridge River Cones) are alkalic [2] and lack a trace element subduction signature [3]. The <span class="hlt">mantle</span> source of the alkalic basalts is significantly more enriched in incompatible elements than the slab-modified depleted <span class="hlt">mantle</span> wedge that produces calc-alkaline basalts in the southern GVB (Mt. Baker and Glacier Peak) [3]. The alkalic basalts are also generated at temperatures and pressures of up to 175°C and 1.5 GPa higher than those of the calc-alkaline basalts [3], consistent with decompression melting of fertile, hot <span class="hlt">mantle</span> ascending through a gap in the Nootka fault, the boundary between the subducting Juan de Fuca plate and the nearly stagnant Explorer microplate. <span class="hlt">Mantle</span> upwelling may be related to toroidal <span class="hlt">mantle</span> flow around the slab edge, which has been identified in southern Cascadia [4]. In the GVB, the upwelling fertile <span class="hlt">mantle</span> is not confined to the immediate area around the slab edge but has spread southward along the arc axis, its extent gradually diminishing as the slab-modified depleted <span class="hlt">mantle</span> wedge becomes dominant. Between Salal Glacier/Bridge River and Glacier Peak ~350 km to the south, there are increases in isotopic ratios (ɛHf = 8.3 to13.0, ɛNd = 7.3 to 8.5, and 208Pb*/206*Pb* = 0.914 to 0.928) and trace element indicators of slab</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI44A..04W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI44A..04W"><span>Update on the Search for Chemical Interactions Between the Core and <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Walker, R. J.</p> <p>2017-12-01</p> <p> increases in HSE, within the portion of the affected <span class="hlt">mantle</span>. Experiments, however, will be necessary to verify this presumption. The spatial correlation between ultra-low velocity zones and isotopically anomalous OIB suggest they may be repositories of the core signal. If so, they may also represent left overs of an <span class="hlt">early</span> basal magma ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910018331','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910018331"><span>Lateral variation in upper <span class="hlt">mantle</span> temperature and composition beneath mid-ocean ridges inferred from shear-wave propagation, geoid, and bathymetry. Ph.D. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sheehan, Anne Francis</p> <p>1991-01-01</p> <p>Resolution of both the extent and mechanism of lateral heterogeneity in the upper <span class="hlt">mantle</span> constraints the nature and scales of <span class="hlt">mantle</span> convection. Oceanic regions are of particular interest as they are likely to provide the closest glimpse at the patterns of temperature anomalies and convective flow in the upper <span class="hlt">mantle</span> because of their young age and simple crustal structure relative to continental regions. Lateral variations were determined in the seismic velocity and attenuation structure of the lithosphere and astenosphere beneath the oceans, and these seismological observations were combined with the data and theory of geoid and bathymetry anomalies in order to test and improve current models for seafloor spreading and <span class="hlt">mantle</span> convection. Variations were determined in <span class="hlt">mantle</span> properties on a scale of about 1000 km, comparable to the thickness of the upper <span class="hlt">mantle</span>. Seismic velocity, geoid, and bathymetry anomalies are all sensitive to variations in upper <span class="hlt">mantle</span> density, and inversions were formulated to combine quantitatively these different data and to search for a common origin. Variations in <span class="hlt">mantle</span> density can be either of thermal or compositional origin and are related to <span class="hlt">mantle</span> convection or <span class="hlt">differentiation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/EJ889229.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/EJ889229.pdf"><span>A Review of Recent Studies on <span class="hlt">Differential</span> Reinforcement during Skill Acquisition in <span class="hlt">Early</span> Intervention</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Vladescu, Jason C.; Kodak, Tiffany</p> <p>2010-01-01</p> <p>Although the use of <span class="hlt">differential</span> reinforcement has been recommended in previous investigations and in <span class="hlt">early</span> intervention curriculum manuals, few studies have evaluated the best method for providing <span class="hlt">differential</span> reinforcement to maximize independent responding. This paper reviews previous research on the effectiveness of <span class="hlt">differential</span> reinforcement…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010GeoJI.180...49D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010GeoJI.180...49D"><span>Response of <span class="hlt">mantle</span> transition zone thickness to plume buoyancy flux</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Das Sharma, S.; Ramesh, D. S.; Li, X.; Yuan, X.; Sreenivas, B.; Kind, R.</p> <p>2010-01-01</p> <p>The debate concerning thermal plumes in the Earth's <span class="hlt">mantle</span>, their geophysical detection and depth characterization remains contentious. Available geophysical, petrological and geochemical evidence is at variance regarding the very existence of <span class="hlt">mantle</span> plumes. Utilizing P-to-S converted seismic waves (P receiver functions) from the 410 and 660 km discontinuities, we investigate disposition of these boundaries beneath a number of prominent hotspot regions. The thickness of the <span class="hlt">mantle</span> transition zone (MTZ), measured as P660s-P410s <span class="hlt">differential</span> times (tMTZ), is determined. Our analyses suggest that the MTZ thickness beneath some hotspots correlates with the plume strength. The relationship between tMTZ, in response to the thermal perturbation, and the strength of plumes, as buoyancy flux B, follows a power law. This B-tMTZ behavior provides unprecedented insights into the relation of buoyancy flux and excess temperature at 410-660 km depth below hotspots. We find that the strongest hotspots, which are located in the Pacific, are indeed plumes originating at the MTZ or deeper. According to the detected power law, even the strongest plumes may not shrink the transition zone by significantly more than ~40 km (corresponding to a maximum of 300-400° excess temperature).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFM.U11B..04L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFM.U11B..04L"><span>The Elephants' Graveyard: Constraints from <span class="hlt">Mantle</span> Plumes on the Fate of Subducted Slabs and Implications for the Style of <span class="hlt">Mantle</span> Convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lassiter, J. C.</p> <p>2007-12-01</p> <p>The style of <span class="hlt">mantle</span> convection (e.g., layered- vs. whole-<span class="hlt">mantle</span> convection) is one of the most hotly contested questions in the Geological Sciences. Geochemical arguments for and against <span class="hlt">mantle</span> layering have largely focused on mass-balance evidence for the existence of "hidden" geochemical reservoirs. However, the size and location of such reservoirs are largely unconstrained, and most geochemical arguments for <span class="hlt">mantle</span> layering are consistent with a depleted <span class="hlt">mantle</span> comprising most of the <span class="hlt">mantle</span> mass and a comparatively small volume of enriched, hidden material either within D" or within seismically anomalous "piles" beneath southern Africa and the South Pacific. The mass flux associated with subduction of oceanic lithosphere is large and plate subduction is an efficient driver of convective mixing in the <span class="hlt">mantle</span>. Therefore, the depth to which oceanic lithosphere descends into the <span class="hlt">mantle</span> is effectively the depth of the upper <span class="hlt">mantle</span> in any layered <span class="hlt">mantle</span> model. Numerous geochemical studies provide convincing evidence that many <span class="hlt">mantle</span> plumes contain material which at one point resided close to the Earth's surface (e.g., recycled oceanic crust ± sediments, possibly subduction-modified <span class="hlt">mantle</span> wedge material). Fluid dynamic models further reveal that only the central cores of <span class="hlt">mantle</span> plumes are involved in melt generation. The presence of recycled material in the sources of many ocean island basalts therefore cannot be explained by entrainment of this material during plume ascent, but requires that recycled material resides within or immediately above the thermo-chemical boundary layer(s) that generates <span class="hlt">mantle</span> plumes. More recent Os- isotope studies of <span class="hlt">mantle</span> xenoliths from OIB settings reveal the presence not only of recycled crust in <span class="hlt">mantle</span> plumes, but also ancient melt-depleted harzburgite interpreted to represent ancient recycled oceanic lithosphere [1]. Thus, there is increasing evidence that subducted slabs accumulate in the boundary layer(s) that provide the source</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.491..216B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.491..216B"><span>Timing of <span class="hlt">mantle</span> overturn during magma ocean solidification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boukaré, C.-E.; Parmentier, E. M.; Parman, S. W.</p> <p>2018-06-01</p> <p>Solidification of magma oceans (MOs) formed <span class="hlt">early</span> in the evolution of planetary bodies sets the initial condition for their evolution on much longer time scales. Ideal fractional crystallization would generate an unstable chemical stratification that subsequently overturns to form a stably stratified <span class="hlt">mantle</span>. The simplest model of overturn assumes that cumulates remain immobile until the end of MO solidification. However, overturning of cumulates and thermal convection during solidification may act to reduce this stratification and introduce chemical heterogeneity on scales smaller than the MO thickness. We explore overturning of cumulates before the end of MO crystallization and the possible consequences for <span class="hlt">mantle</span> structure and composition. In this model, increasingly dense iron-rich layers, crystallized from the overlying residual liquid MO, are deposited on a thickening cumulate layer. Overturn during solidification occurs if the dimensionless parameter, Rc, measuring the ratio of the MO time of crystallization τMO to the timescale associated with compositional overturn τov = μ / ΔρgH exceeds a threshold value. If overturn did not occur until after solidification, this implies that the viscosity of the solidified <span class="hlt">mantle</span> must have been sufficiently high (possibly requiring efficient melt extraction from the cumulate) for a given rate of solidification. For the lunar MO, possible implications for the generation of the Mg-suites and mare basalt are suggested.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015E%26PSL.424..109L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015E%26PSL.424..109L"><span>The longevity of Archean <span class="hlt">mantle</span> residues in the convecting upper <span class="hlt">mantle</span> and their role in young continent formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Jingao; Scott, James M.; Martin, Candace E.; Pearson, D. Graham</p> <p>2015-08-01</p> <p>The role played by ancient melt-depleted lithospheric <span class="hlt">mantle</span> in preserving continental crust through time is critical in understanding how continents are built, disrupted and recycled. While it has become clear that much of the extant Archean crust is underpinned by Archean <span class="hlt">mantle</span> roots, reports of Proterozoic melt depletion ages for peridotites erupted through Phanerozoic terranes raise the possibility that ancient buoyant lithospheric <span class="hlt">mantle</span> acts as a "life-raft" for much of the Earth's continental crust. Here we report the largest crust-lithospheric <span class="hlt">mantle</span> age decoupling (∼2.4 Ga) so far observed on Earth and examine the potential cause for such extreme age decoupling. The Phanerozoic (<300 Ma) continental crust of West Otago, New Zealand, is intruded by Cenozoic diatremes that have erupted cratonic <span class="hlt">mantle</span>-like highly depleted harzburgites and dunites. These peridotites have rhenium depletion Os model ages that vary from 0.5 to 2.7 Ga, firmly establishing the record of an Archean depletion event. However, the vast range in depletion ages does not correlate with melt depletion or metasomatic tracer indices, providing little support for the presence of a significant volume of ancient <span class="hlt">mantle</span> root beneath this region. Instead, the chemical and isotopic data are best explained by mixing of relict components of Archean depleted peridotitic <span class="hlt">mantle</span> residues that have cycled through the asthenosphere over Ga timescales along with more fertile convecting <span class="hlt">mantle</span>. Extensive melt depletion associated with the "docking" of these melt residues beneath the young continental crust of the Zealandia continent explains the decoupled age relationship that we observe today. Hence, the newly formed lithospheric root incorporates a mixture of ancient and modern <span class="hlt">mantle</span> derived from the convecting <span class="hlt">mantle</span>, cooled and accreted in recent times. We argue that in this case, the ancient components played no earlier role in continent stabilization, but their highly depleted nature along with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.V32B..05P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.V32B..05P"><span>Towards driving <span class="hlt">mantle</span> convection by mineral physics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Piazzoni, A. S.; Bunge, H.; Steinle-Neumann, G.</p> <p>2005-12-01</p> <p>Models of <span class="hlt">mantle</span> convection have become increasingly sophisticated over the past decade, accounting, for example, for 3 D spherical geometry, and changes in <span class="hlt">mantle</span> rheology due to variations in temperature and stress. In light of such advances it is surprising that growing constraints on <span class="hlt">mantle</span> structure derived from mineral physics have not yet been fully brought to bear on <span class="hlt">mantle</span> convection models. In fact, despite much progress in our understanding of <span class="hlt">mantle</span> mineralogy a partial description of the equation of state is often used to relate density changes to pressure and temperature alone, without taking into account compositional and mineralogical models of the <span class="hlt">mantle</span>. Similarly, for phase transitions an incomplete description of thermodynamic constraints is often used, resulting in significant uncertainties in model behavior. While a number of thermodynamic models (some with limited scope) have been constructed recently, some lack the rigor in thermodynamics - for example with respect to the treatment of solid solution - that is needed to make predictions about <span class="hlt">mantle</span> structure. Here we have constructed a new thermodynamic database for the <span class="hlt">mantle</span> and have coupled the resulting density dynamically with <span class="hlt">mantle</span> convection models. The database is build on a self-consistent Gibb's free energy minimization of the system MgO-FeO-SiO2-CaO-Al2O3 that is appropriate for standard (dry) chemical models of the Earth's <span class="hlt">mantle</span> for relevant high pressure and temperature phases. We have interfaced the database with a high-resolution 2-D convection code (2DTERRA), dynamically coupling the thermodynamic model (density) with the conservation equations of <span class="hlt">mantle</span> flow. The coupled model is run for different parameterizations of viscosity, initial temperature conditions, and varying the internal vs. external heating. We compare the resulting flow and temperature fields to cases with the Boussinesq approximation and other classical descriptions of the equation of state in <span class="hlt">mantle</span></p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11902564','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11902564"><span><span class="hlt">Mantle</span>-cell lymphoma.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barista, I; Romaguera, J E; Cabanillas, F</p> <p>2001-03-01</p> <p>During the past decade, <span class="hlt">mantle</span>-cell lymphoma has been established as a new disease entity. The normal counterparts of the cells forming this malignant lymphoma are found in the <span class="hlt">mantle</span> zone of the lymph node, a thin layer surrounding the germinal follicles. These cells have small to medium-sized nuclei, are commonly indented or cleaved, and stain positively with CD5, CD20, cyclin D1, and FMC7 antibodies. Because of its morphological appearance and a resemblance to other low-grade lymphomas, many of which grow slowly, this lymphoma was initially thought to be an indolent tumour, but its natural course was not thoroughly investigated until the 1990s, when the BCL1 oncogene was identified as a marker for this disease. <span class="hlt">Mantle</span>-cell lymphoma is a discrete entity, unrelated to small lymphocytic or small-cleaved-cell lymphomas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920060793&hterms=history+Earth&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dhistory%2BEarth','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920060793&hterms=history+Earth&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dhistory%2BEarth"><span>Internally heated <span class="hlt">mantle</span> convection and the thermal and degassing history of the earth</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Williams, David R.; Pan, Vivian</p> <p>1992-01-01</p> <p>An internally heated model of parameterized whole <span class="hlt">mantle</span> convection with viscosity dependent on temperature and volatile content is examined. The model is run for 4l6 Gyr, and temperature, heat flow, degassing and regassing rates, stress, and viscosity are calculated. A nominal case is established which shows good agreement with accepted <span class="hlt">mantle</span> values. The effects of changing various parameters are also tested. All cases show rapid cooling <span class="hlt">early</span> in the planet's history and strong self-regulation of viscosity due to the temperature and volatile-content dependence. The effects of weakly stress-dependent viscosity are examined within the bounds of this model and are found to be small. <span class="hlt">Mantle</span> water is typically outgassed rapidly to reach an equilibrium concentration on a time scale of less than 200 Myr for almost all models, the main exception being for models which start out with temperatures well below the melting temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR54A..05B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR54A..05B"><span>Large-scale compositional heterogeneity in the Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ballmer, M.</p> <p>2017-12-01</p> <p>Seismic imaging of subducted Farallon and Tethys lithosphere in the lower <span class="hlt">mantle</span> has been taken as evidence for whole-<span class="hlt">mantle</span> convection, and efficient <span class="hlt">mantle</span> mixing. However, cosmochemical constraints point to a lower-<span class="hlt">mantle</span> composition that has a lower Mg/Si compared to upper-<span class="hlt">mantle</span> pyrolite. Moreover, geochemical signatures of magmatic rocks indicate the long-term persistence of primordial reservoirs somewhere in the <span class="hlt">mantle</span>. In this presentation, I establish geodynamic mechanisms for sustaining large-scale (primordial) heterogeneity in the Earth's <span class="hlt">mantle</span> using numerical models. <span class="hlt">Mantle</span> flow is controlled by rock density and viscosity. Variations in intrinsic rock density, such as due to heterogeneity in basalt or iron content, can induce layering or partial layering in the <span class="hlt">mantle</span>. Layering can be sustained in the presence of persistent whole <span class="hlt">mantle</span> convection due to active "unmixing" of heterogeneity in low-viscosity domains, e.g. in the transition zone or near the core-<span class="hlt">mantle</span> boundary [1]. On the other hand, lateral variations in intrinsic rock viscosity, such as due to heterogeneity in Mg/Si, can strongly affect the mixing timescales of the <span class="hlt">mantle</span>. In the extreme case, intrinsically strong rocks may remain unmixed through the age of the Earth, and persist as large-scale domains in the mid-<span class="hlt">mantle</span> due to focusing of deformation along weak conveyor belts [2]. That large-scale lateral heterogeneity and/or layering can persist in the presence of whole-<span class="hlt">mantle</span> convection can explain the stagnation of some slabs, as well as the deflection of some plumes, in the mid-<span class="hlt">mantle</span>. These findings indeed motivate new seismic studies for rigorous testing of model predictions. [1] Ballmer, M. D., N. C. Schmerr, T. Nakagawa, and J. Ritsema (2015), Science Advances, doi:10.1126/sciadv.1500815. [2] Ballmer, M. D., C. Houser, J. W. Hernlund, R. Wentzcovitch, and K. Hirose (2017), Nature Geoscience, doi:10.1038/ngeo2898.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140012819','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140012819"><span>Stable Magnesium Isotope Variation in Melilite <span class="hlt">Mantle</span> of Allende Type B1 CAI EK 459-5-1</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kerekgyarto, A. G.; Jeffcoat, C. R.; Lapen, T. J.; Andreasen, R.; Righter, M.; Ross, D. K.</p> <p>2014-01-01</p> <p>Ca-Al-rich inclusions (CAIs) are the earliest formed crystalline material in our solar system and they record <span class="hlt">early</span> Solar System processes. Here we present petrographic and delta Mg-25 data of melilite <span class="hlt">mantles</span> in a Type B1 CAI that records <span class="hlt">early</span> solar nebular processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29318501','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29318501"><span>Function of FEZF1 during <span class="hlt">early</span> neural <span class="hlt">differentiation</span> of human embryonic stem cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Xin; Su, Pei; Lu, Lisha; Feng, Zicen; Wang, Hongtao; Zhou, Jiaxi</p> <p>2018-01-01</p> <p>The understanding of the mechanism underlying human neural development has been hampered due to lack of a cellular system and complicated ethical issues. Human embryonic stem cells (hESCs) provide an invaluable model for dissecting human development because of unlimited self-renewal and the capacity to <span class="hlt">differentiate</span> into nearly all cell types in the human body. In this study, using a chemical defined neural induction protocol and molecular profiling, we identified Fez family zinc finger 1 (FEZF1) as a potential regulator of <span class="hlt">early</span> human neural development. FEZF1 is rapidly up-regulated during neural <span class="hlt">differentiation</span> in hESCs and expressed before PAX6, a well-established marker of <span class="hlt">early</span> human neural induction. We generated FEZF1-knockout H1 hESC lines using CRISPR-CAS9 technology and found that depletion of FEZF1 abrogates neural <span class="hlt">differentiation</span> of hESCs. Moreover, loss of FEZF1 impairs the pluripotency exit of hESCs during neural specification, which partially explains the neural induction defect caused by FEZF1 deletion. However, enforced expression of FEZF1 itself fails to drive neural <span class="hlt">differentiation</span> in hESCs, suggesting that FEZF1 is necessary but not sufficient for neural <span class="hlt">differentiation</span> from hESCs. Taken together, our findings identify one of the earliest regulators expressed upon neural induction and provide insight into <span class="hlt">early</span> neural development in human.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.465...59K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.465...59K"><span>A view into crustal evolution at <span class="hlt">mantle</span> depths</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kooijman, Ellen; Smit, Matthijs A.; Ratschbacher, Lothar; Kylander-Clark, Andrew R. C.</p> <p>2017-05-01</p> <p>Crustal foundering is an important mechanism in the <span class="hlt">differentiation</span> and recycling of continental crust. Nevertheless, little is known about the dynamics of the lower crust, the temporal scale of foundering and its role in the dynamics of active margins and orogens. This particularly applies to active settings where the lower crust is typically still buried and direct access is not possible. Crustal xenoliths derived from <span class="hlt">mantle</span> depth in the Pamir provide a unique exception to this. The rocks are well-preserved and comprise a diverse set of lithologies, many of which re-equilibrated at high-pressure conditions before being erupted in their ultrapotassic host lavas. In this study, we explore the petrological and chronological record of eclogite and felsic granulite xenoliths. We utilized accessory minerals - zircon, monazite and rutile - for coupled in-situ trace-element analysis and U-(Th-)Pb chronology by laser-ablation (split-stream) inductively coupled plasma mass spectrometry. Each integrated analysis was done on single mineral zones and was performed in-situ in thin section to maintain textural context and the ability to interpret the data in this framework. Rutile thermo-chronology exclusively reflects eruption (11.17 ± 0.06Ma), which demonstrates the reliability of the U-Pb rutile thermo-chronometer and its ability to date magmatic processes. Conversely, zircon and monazite reveal a series of discrete age clusters between 55-11 Ma, with the youngest being identical to the age of eruption. Matching age populations between samples, despite a lack of overlapping ages for different chronometers within samples, exhibit the effectiveness of our multi-mineral approach. The REE systematics and age data for zircon and monazite, and Ti-in-zircon data together track the history of the rocks at a million-year resolution. The data reveal that the rocks resided at 30-40 km depth along a stable continental geotherm at 720-750 °C until 24-20 Ma, and were subsequently</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011Litho.125..956S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011Litho.125..956S"><span>Asphaltene-bearing <span class="hlt">mantle</span> xenoliths from Hyblean diatremes, Sicily</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scirè, Salvatore; Ciliberto, Enrico; Crisafulli, Carmelo; Scribano, Vittorio; Bellatreccia, Fabio; Ventura, Giancarlo Della</p> <p>2011-08-01</p> <p>Microscopic blebs of sulfur-bearing organic matter (OM) commonly occur between the secondary calcite grains and fibrous phyllosilicates in extensively serpentinized and carbonated <span class="hlt">mantle</span>-derived ultramafic xenoliths from Hyblean nephelinite diatremes, Sicily, Italy. Rarely, coarse bituminous patches give the rock a blackish color. Micro Fourier transform infrared spectra (μ-FTIR) point to asphaltene-like structures in the OM, due to partially condensed aromatic rings with aliphatic tails consisting of a few C atoms. X-ray photoelectron spectroscopy (XPS) analysis indicates the occurrence of minor S═O (either sulphonyl or sulphoxide) functional groups in the OM. Solubility tests in toluene, thermo-gravimetric (TGA) and <span class="hlt">differential</span> thermal (DTA) analyses confirm the presence of asphaltene structures. It is proposed that asphaltenes derive from the in situ aromatization (with decrease in H/C ratio) of previous light aliphatic hydrocarbons. Field evidence excludes that hydrocarbon from an external source percolated through the xenolith bearing tuff-breccia. The discriminating presence of hydrocarbon in a particular type of xenolith only and the lack of hydrocarbon in the host breccia matrix, are also inconsistent with an interaction between the ascending eruptive system and a supposed deep-seated oil reservoir. Assuming that the Hyblean unexposed basement consists of <span class="hlt">mantle</span> ultramafics and mafic intrusive rocks having hosted an <span class="hlt">early</span> abyssal-type hydrothermal system, one can put forward the hypothesis that the hydrocarbon production was related to hydrothermal activity in a serpentinite system. Although a bacteriogenesis or thermogenesis cannot be ruled out, the coexisting serpentine, Ni-Fe ores and hydrocarbon strongly suggest a Fischer-Tropsch-type (FTT) synthesis. Subsequent variations in the chemical and physical conditions of the system, for example an increase in the water/rock ratio, gave rise to partial oxidation and late carbonation of the serpentinite</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5223A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5223A"><span>Teaching machines to find <span class="hlt">mantle</span> composition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Atkins, Suzanne; Tackley, Paul; Trampert, Jeannot; Valentine, Andrew</p> <p>2017-04-01</p> <p>The composition of the <span class="hlt">mantle</span> affects many geodynamical processes by altering factors such as the density, the location of phase changes, and melting temperature. The inferences we make about <span class="hlt">mantle</span> composition also determine how we interpret the changes in velocity, reflections, attenuation and scattering seen by seismologists. However, the bulk composition of the <span class="hlt">mantle</span> is very poorly constrained. Inferences are made from meteorite samples, rock samples from the Earth and inferences made from geophysical data. All of these approaches require significant assumptions and the inferences made are subject to large uncertainties. Here we present a new method for inferring <span class="hlt">mantle</span> composition, based on pattern recognition machine learning, which uses large scale in situ observations of the <span class="hlt">mantle</span> to make fully probabilistic inferences of composition for convection simulations. Our method has an advantage over other petrological approaches because we use large scale geophysical observations. This means that we average over much greater length scales and do not need to rely on extrapolating from localised samples of the <span class="hlt">mantle</span> or planetary disk. Another major advantage of our method is that it is fully probabilistic. This allows us to include all of the uncertainties inherent in the inference process, giving us far more information about the reliability of the result than other methods. Finally our method includes the impact of composition on <span class="hlt">mantle</span> convection. This allows us to make much more precise inferences from geophysical data than other geophysical approaches, which attempt to invert one observation with no consideration of the relationship between convection and composition. We use a sampling based inversion method, using hundreds of convection simulations run using StagYY with self consistent mineral physics properties calculated using the PerpleX package. The observations from these simulations are used to train a neural network to make a probabilistic inference</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1610232M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1610232M"><span>Petrology of exhumed <span class="hlt">mantle</span> rocks at passive margins: ancient lithosphere and rejuvenation processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Müntener, Othmar; McCarthy, Anders; Picazo, Suzanne</p> <p>2014-05-01</p> <p>, an alternative is that these depleted domains represent snapshots of melting processes that are related to Permian and/or even older crust forming processes. The findings of the these refractory <span class="hlt">mantle</span> rocks over the entire Western Alpine arc and the similarity in model ages of depletion suggests a connection to the <span class="hlt">Early</span> Permian magmatic activity. Shallow and deep crustal magmatism in the Permian is widespread over Western Europe and the distribution of these mafic rocks are likely to pre-determine the future areas of crustal thinning and exhumation during formation of the Thethyan passive margins.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880050792&hterms=Modeling+mechanical+properties&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DModeling%2Bmechanical%2Bproperties','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880050792&hterms=Modeling+mechanical+properties&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DModeling%2Bmechanical%2Bproperties"><span>Dynamical effects on the core-<span class="hlt">mantle</span> boundary from depth-dependent thermodynamical properties of the lower <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zhang, Shuxia; Yuen, David A.</p> <p>1988-01-01</p> <p>A common assumption in modeling dynamical processes in the lower <span class="hlt">mantle</span> is that both the thermal expansivity and thermal conductivity are reasonably constant. Recent work from seismic equation of state leads to substantially higher values for the thermal conductivity and much lower thermal expansivity values in the deep <span class="hlt">mantle</span>. The dynamical consequences of incorporating depth-dependent thermodynamic properties on the thermal-mechanical state of the lower <span class="hlt">mantle</span> are examined with the spherical-shell mean-field equations. It is found that the thermal structure of the seismically resolved anomalous zone at the base of the <span class="hlt">mantle</span> is strongly influenced by these variable properties and, in particular, that the convective distortion of the core-<span class="hlt">mantle</span> boundary (CMB) is reduced with the decreasing thermal expansivity. Such a reduction of the dynamically induced topography from pure thermal convection would suggest that some other dynamical mechanism must be operating at the CMB.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25186903','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25186903"><span>Asymmetric three-dimensional topography over <span class="hlt">mantle</span> plumes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Burov, Evgueni; Gerya, Taras</p> <p>2014-09-04</p> <p>The role of <span class="hlt">mantle</span>-lithosphere interactions in shaping surface topography has long been debated. In general, it is supposed that <span class="hlt">mantle</span> plumes and vertical <span class="hlt">mantle</span> flows result in axisymmetric, long-wavelength topography, which strongly differs from the generally asymmetric short-wavelength topography created by intraplate tectonic forces. However, identification of <span class="hlt">mantle</span>-induced topography is difficult, especially in the continents. It can be argued therefore that complex brittle-ductile rheology and stratification of the continental lithosphere result in short-wavelength modulation and localization of deformation induced by <span class="hlt">mantle</span> flow. This deformation should also be affected by far-field stresses and, hence, interplay with the 'tectonic' topography (for example, in the 'active/passive' rifting scenario). Testing these ideas requires fully coupled three-dimensional numerical modelling of <span class="hlt">mantle</span>-lithosphere interactions, which so far has not been possible owing to the conceptual and technical limitations of earlier approaches. Here we present new, ultra-high-resolution, three-dimensional numerical experiments on topography over <span class="hlt">mantle</span> plumes, incorporating a weakly pre-stressed (ultra-slow spreading), rheologically realistic lithosphere. The results show complex surface evolution, which is very different from the smooth, radially symmetric patterns usually assumed as the canonical surface signature of <span class="hlt">mantle</span> upwellings. In particular, the topography exhibits strongly asymmetric, small-scale, three-dimensional features, which include narrow and wide rifts, flexural flank uplifts and fault structures. This suggests a dominant role for continental rheological structure and intra-plate stresses in controlling dynamic topography, <span class="hlt">mantle</span>-lithosphere interactions, and continental break-up processes above <span class="hlt">mantle</span> plumes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940011863','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940011863"><span>Water in Earth's <span class="hlt">mantle</span>: Hydrogen analysis of <span class="hlt">mantle</span> olivine, pyroxenes and garnet using the SIMS</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kurosawa, Masanori; Yurimoto, Hisayoshi; Sueno, Shigeho</p> <p>1993-01-01</p> <p>Hydrogen (or water) in the Earth's interior plays a key role in the evolution and dynamics of the planet. However, the abundance and the existence form of the hydrogen have scarcely been clear in practice. Hydrogen in the <span class="hlt">mantle</span> was incorporated in the interior during the formation of the Earth. The incorporated hydrogen was hardly possible to concentrate locally inside the Earth considering its high mobility and high reactivity. The hydrogen, preferably, could be distributed homogeneously over the <span class="hlt">mantle</span> and the core by the subsequent physical and chemical processes. Therefore, hydrogen in the <span class="hlt">mantle</span> could be present in the form of trace hydrogen in nominally anhydrous <span class="hlt">mantle</span> minerals. The hydrogen and the other trace elements in <span class="hlt">mantle</span> olivines, orthopyroxenes, clinopyroxenes, and garnets were determined using secondary ion mass spectrometry (SIMS) for elucidating (1) the exact hydrogen contents, (2) the correlation between the hydrogen and the other trace elements, (3) the dependence of the hydrogen contents on the depth, and (4) the dependence of the whole rock water contents on the depth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.V11D0611B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.V11D0611B"><span>Constant average olivine Mg# in cratonic <span class="hlt">mantle</span> reflects Archaean <span class="hlt">mantle</span> melting to the exhaustion of orthopyroxene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bernstein, S.; Kelemen, P. B.; Hanghoj, K.</p> <p>2006-12-01</p> <p>Shallow (garnet-free) cratonic <span class="hlt">mantle</span>, occurring as xenoliths in kimberlites and alkaline basaltic lavas, has high Mg# (100x Mg/(Mg+Fe)>92) and is poor in Al and Ca compared to off-cratonic <span class="hlt">mantle</span>. Many xenoliths show rhenium-depletion age of > 3 Ga, and are thus representative of depleted <span class="hlt">mantle</span> peridotite that form an integral part of the stable nuclei of Archaean (2.5-3.8 Ga) cratons. Accordingly, the depleted composition of the xenolith suites is linked to Archaean melt extraction events. We have compiled data for many suites of shallow cratonic <span class="hlt">mantle</span> xenoliths worldwide, including samples from cratons of Kaapvaal, Tanzania, Siberia, Slave, North China and Greenland, and encompassing both the classic orthopyroxene-rich peridotites of Kaapvaal and orthopyroxene-poor peridotites from Greenland. The suites show a remarkably small range in average olivine Mg# of 92.8 +/- 0.2. Via comparison with data for experimental melting of <span class="hlt">mantle</span> peridotite compositions, we explain consistent olivine Mg# in the shallow cratonic <span class="hlt">mantle</span> as the result of <span class="hlt">mantle</span> melting and melt extraction to the point of orthopyroxene exhaustion, leaving a nearly monomineralic olivine, or dunitic, residue. Experimental data for peridotite melting at pressures less than 4 GPa and data on natural rocks suggest that <span class="hlt">mantle</span> olivine has a Mg# of about 92.8 at the point of orthopyroxene exhaustion. If the melt extraction was efficient, no further melting could take place without a considerable temperature increase or melt/fluid flux through the dunite residue at high temperatures. While the high Mg#, dunite-dominated xenolith suites from e.g. Greenland represent simple residues from <span class="hlt">mantle</span> melting, the orthopyroxene-rich xenolith suites with identical Mg# as known from e. g. Kaapvaal must reflect some additional processes. We envisage their derivation from dunite protoliths via subsequent melt/rock reaction with silica-rich melts or, in some cases, possibly as residues at higher average melting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.V52A..06S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.V52A..06S"><span>Boron Isotope Evidence for Shallow Fluid Transfer Across Subduction Zones by Serpentinized <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scambelluri, M.; Tonarini, S.; Agostini, S.; Cannaò, E.</p> <p>2012-12-01</p> <p>). No significant B loss and 11B fractionation occurs with burial. Their B and 11B abundance shows that high budgets acquired during shallow hydration are transferred to HP fluids, providing the heavy-boron component requested for arcs. The B compositions of Erro-Tobbio are unexpected for slabs, deputed to loose B and 11B during dehydration: its isotopic composition can be achieved diluting in the <span class="hlt">mantle</span> shallow subduction-fluids (30 km). The serpentinizing fluids and the fluid-transfer mechanism in Erro-Tobbio are clarified integrating B with O-H and Sr isotopes. Low δD (-102permil), high δ18O (8permil) of <span class="hlt">early</span> serpentinites suggest low-temperature hydration by metamorphic fluids. 87Sr/86Sr (0.7044 to 0.7065) is lower than oceanic serpentinites formed from seawater. We conclude that alteration was distant from mid-ocean ridges and occurred at the slab-<span class="hlt">mantle</span> interface or in forearc environments. We thus provide evidence for delivery of water and 11B at sub-arcs by serpentinized <span class="hlt">mantle</span> altered by subduction-fluid infiltration atop of the slab since the <span class="hlt">early</span> stages of burial, witnessing shallow fluid transfer across the subduction zone. Similarity of the B composition of Erro Tobbio with other Alpine serpentinized peridotites suggests that these materials might have spent much of their subduction lifetime at the plate interface, fed by B and 11Bich fluids uprising from the slab.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.6500Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.6500Y"><span>Short-scale Heterogeneity in the Lowermost <span class="hlt">Mantle</span> Revealed Through Partition Modeling of Seismic Body Waves</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Young, M. K.; Tkalcic, H.; Bodin, T.</p> <p>2012-04-01</p> <p>The existence of both chemical and thermal heterogeneities on a variety of scales in the lowermost <span class="hlt">mantle</span> has been invoked to explain various types of seismological observations and the Earth's dynamics. Understanding the size and magnitude of these heterogeneities is important in the context of whole <span class="hlt">mantle</span> dynamics. However, due to inaccurate approximation of data noise and the inadequate definition of the misfit function in the optimization framework, the size of heterogeneities has not been well constrained in present tomographic models of the lowermost <span class="hlt">mantle</span>. Moreover, we need to be able to clearly see through the core-<span class="hlt">mantle</span> boundary to properly understand the Earth's core. For example, in order to investigate anisotropy in the inner core, it is important to quantify the contribution to seismic travel times from the Earth's <span class="hlt">mantle</span>. Furthermore, it is impossible to reconstruct the topography of the Earth's core without a full understanding of <span class="hlt">mantle</span> heterogeneities. In addition, P-wave velocity maps of the lowermost <span class="hlt">mantle</span> are rare in comparison to S-wave maps, yet both are needed to properly understand the physical and chemical state of the lowermost <span class="hlt">mantle</span>. Here we use a Partition Modeling approach, in which trans-dimensional and hierarchical sampling methods are used to solve the above problems. The advantage of such an inversion method is that the number of model parameters, the size of the velocity cells, and the data noise are treated as unknowns in the problem. In this sense, the approach lets us consider the issue of model parameterization as part of the inversion process. A large ensemble of models is averaged to produce a final solution complete with uncertainty estimates. We map the P-wave velocity structure of the lowermost <span class="hlt">mantle</span> from a dataset of hand-picked PKPab-df, PKPbc-df, and PcP-P <span class="hlt">differential</span> travel times. We focus on covering gaps in spatial sampling of the lowermost <span class="hlt">mantle</span> from PKPab-df and PcP-P of previous studies. Travel time</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25673102','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25673102"><span>Pangea breakup and northward drift of the Indian subcontinent reproduced by a numerical model of <span class="hlt">mantle</span> convection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yoshida, Masaki; Hamano, Yozo</p> <p>2015-02-12</p> <p>Since around 200 Ma, the most notable event in the process of the breakup of Pangea has been the high speed (up to 20 cm yr(-1)) of the northward drift of the Indian subcontinent. Our numerical simulations of 3-D spherical <span class="hlt">mantle</span> convection approximately reproduced the process of continental drift from the breakup of Pangea at 200 Ma to the present-day continental distribution. These simulations revealed that a major factor in the northward drift of the Indian subcontinent was the large-scale cold <span class="hlt">mantle</span> downwelling that developed spontaneously in the North Tethys Ocean, attributed to the overall shape of Pangea. The strong lateral <span class="hlt">mantle</span> flow caused by the high-temperature anomaly beneath Pangea, due to the thermal insulation effect, enhanced the acceleration of the Indian subcontinent during the <span class="hlt">early</span> stage of the Pangea breakup. The large-scale hot upwelling plumes from the lower <span class="hlt">mantle</span>, initially located under Africa, might have contributed to the formation of the large-scale cold <span class="hlt">mantle</span> downwelling in the North Tethys Ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4325333','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4325333"><span>Pangea breakup and northward drift of the Indian subcontinent reproduced by a numerical model of <span class="hlt">mantle</span> convection</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Yoshida, Masaki; Hamano, Yozo</p> <p>2015-01-01</p> <p>Since around 200 Ma, the most notable event in the process of the breakup of Pangea has been the high speed (up to 20 cm yr−1) of the northward drift of the Indian subcontinent. Our numerical simulations of 3-D spherical <span class="hlt">mantle</span> convection approximately reproduced the process of continental drift from the breakup of Pangea at 200 Ma to the present-day continental distribution. These simulations revealed that a major factor in the northward drift of the Indian subcontinent was the large-scale cold <span class="hlt">mantle</span> downwelling that developed spontaneously in the North Tethys Ocean, attributed to the overall shape of Pangea. The strong lateral <span class="hlt">mantle</span> flow caused by the high-temperature anomaly beneath Pangea, due to the thermal insulation effect, enhanced the acceleration of the Indian subcontinent during the <span class="hlt">early</span> stage of the Pangea breakup. The large-scale hot upwelling plumes from the lower <span class="hlt">mantle</span>, initially located under Africa, might have contributed to the formation of the large-scale cold <span class="hlt">mantle</span> downwelling in the North Tethys Ocean. PMID:25673102</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014E%26PSL.390..146G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014E%26PSL.390..146G"><span>Reconstructing the Cenozoic evolution of the <span class="hlt">mantle</span>: Implications for <span class="hlt">mantle</span> plume dynamics under the Pacific and Indian plates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Glišović, Petar; Forte, Alessandro M.</p> <p>2014-03-01</p> <p>The lack of knowledge of the initial thermal state of the <span class="hlt">mantle</span> in the geological past is an outstanding problem in <span class="hlt">mantle</span> convection. The resolution of this problem also requires the modelling of 3-D <span class="hlt">mantle</span> evolution that yields maximum consistency with a wide suite of geophysical constraints. Quantifying the robustness of the reconstructed thermal evolution is another major concern. To solve and estimate the robustness of the time-reversed (inverse) problem of <span class="hlt">mantle</span> convection, we analyse two different numerical techniques: the quasi-reversible (QRV) and the backward advection (BAD) methods. Our investigation extends over the 65 Myr interval encompassing the Cenozoic era using a pseudo-spectral solution for compressible-flow thermal convection in 3-D spherical geometry. We find that the two dominant issues for solving the inverse problem of <span class="hlt">mantle</span> convection are the choice of horizontally-averaged temperature (i.e., geotherm) and mechanical surface boundary conditions. We find, in particular, that the inclusion of thermal boundary layers that yield Earth-like heat flux at the top and bottom of the <span class="hlt">mantle</span> has a critical impact on the reconstruction of <span class="hlt">mantle</span> evolution. We have developed a new regularisation scheme for the QRV method using a time-dependent regularisation function. This revised implementation of the QRV method delivers time-dependent reconstructions of <span class="hlt">mantle</span> heterogeneity that reveal: (1) the stability of Pacific and African ‘large low shear velocity provinces’ (LLSVP) over the last 65 Myr; (2) strong upward deflections of the CMB topography at 65 Ma beneath: the North Atlantic, the south-central Pacific, the East Pacific Rise (EPR) and the eastern Antarctica; (3) an anchored deep-<span class="hlt">mantle</span> plume ascending directly under the EPR (Easter and Pitcairn hotspots) throughout the Cenozoic era; and (4) the appearance of the transient Reunion plume head beneath the western edge of the Deccan Plateau at 65 Ma. Our reconstructions of Cenozoic <span class="hlt">mantle</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V52A..05D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V52A..05D"><span>Experimental Partitioning of Chalcophile Elements between <span class="hlt">Mantle</span> Silicate Minerals and Basaltic Melt at High Pressures and Temperatures - Implications for Sulfur Geochemistry of <span class="hlt">Mantle</span> and Crust</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dasgupta, R.; Jego, S.; Ding, S.; Li, Y.; Lee, C. T.</p> <p>2015-12-01</p> <p>The behavior of chalcophile elements during <span class="hlt">mantle</span> melting, melt extraction, and basalt <span class="hlt">differentiation</span> is critical for formation of ore deposits and geochemical model and evolution of crust-<span class="hlt">mantle</span> system. While chalcophile elements are strongly partitioned into sulfides, their behavior with different extent of melting, in particular, in the absence of sulfides, can only be modeled with complete knowledge of the partitioning behavior of these elements between dominant <span class="hlt">mantle</span> minerals and basaltic melt with or without dissolved sulfide (S2-). However, experimental data on mineral-melt partitioning are lacking for many chalcophile elements. Crystallization experiments were conducted at 3 GPa and 1450-1600 °C using a piston cylinder and synthetic silicate melt compositions similar to low-degree partial melt of peridotite. Starting silicate mixes doped with 100-300 ppm of each of various chalcophile elements were loaded into Pt/graphite double capsules. To test the effect of dissolved sulfur in silicate melt on mineral-melt partitioning of chalcophile elements, experiments were conducted on both sulfur-free and sulfur-bearing (1100-1400 ppm S in melt) systems. Experimental phases were analyzed by EPMA (for major elements and S) and LA-ICP-MS (for trace elements). All experiments produced an assemblage of cpx + melt ± garnet ± olivine ± spinel and yielded new partition coefficients (D) for Sn, Zn, Mo, Sb, Bi, Pb, and Se for cpx/melt, olivine/melt, and garnet/melt pairs. Derived Ds (mineral/basalt) reveal little effect of S2- in the melt on mineral-melt partition coefficients of the measured chalcophile elements, with Ds for Zn, Mo, Bi, Pb decreasing by less than a factor of 2 from S-free to S-bearing melt systems or remaining similar, within error, between S-free and S-bearing melt systems. By combining our data with existing partitioning data between sulfide phases and silicate melt we model the fractionation of these elements during <span class="hlt">mantle</span> melting and basalt</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5565H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5565H"><span>Effect of planetary rotation on the <span class="hlt">differentiation</span> of a terrestrial magma ocean in spherical geometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, Ulrich; Maas, Christian</p> <p>2017-04-01</p> <p>About 4.5 billion years ago the <span class="hlt">early</span> Earth experienced several giant impacts that lead to one or more deep terrestrial magma oceans of global extent. The crystallization of these vigorously convecting magma oceans is of key importance for the chemical structure of the Earth, the subsequent <span class="hlt">mantle</span> evolution as well as for the initial conditions for the onset of plate tectonics. Due to the fast planetary rotation of the <span class="hlt">early</span> Earth and the small magma viscosity, rotation probably had a profound effect on <span class="hlt">early</span> <span class="hlt">differentiation</span> processes and could for example influence the presence and distribution of chemical heterogeneities in the Earth's <span class="hlt">mantle</span> [e.g. Matyska et al., 1994, Garnero and McNamara, 2008]. Previous work in Cartesian geometry revealed a strong influence of rotation as well as of latitude on the crystal settling in a terrestrial magma ocean [Maas and Hansen, 2015]. Based on the preceding study we developed a spherical shell model that allows to study crystal settling in-between pole and equator as well as the migration of crystals between these regions. Further we included centrifugal forces on the crystals, which significantly affect the lateral and radial distribution of the crystals. Depending on the strength of rotation the particles accumulate at mid-latitude or at the equator. At high rotation rates the dynamics of fluid and particles are dominated by jet-like motions in longitudinal direction that have different directions on northern and southern hemisphere. All in all the first numerical experiments in spherical geometry agree with Maas and Hansen [2015] that the crystal distribution crucially depends on latitude, rotational strength and crystal density. References E. J. Garnero and A. K. McNamara. Structure and dynamics of earth's lower <span class="hlt">mantle</span>. Science, 320(5876):626-628, 2008. C. Maas and U. Hansen. Eff ects of earth's rotation on the <span class="hlt">early</span> di erentiation of a terrestrial magma ocean. Journal of Geophysical Research: Solid Earth, 120</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.T41C0896S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.T41C0896S"><span>Anelastic <span class="hlt">Mantle</span> Structure beneath the Northern Philippine Sea from Phase Pair Method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shito, A.; Shibutani, T.</p> <p>2001-12-01</p> <p>Anelasticity of the <span class="hlt">mantle</span> provides important constraints on its dynamics, in complement to elasticity, however, studies of lateral variation in attenuation are few, especially at short periods. In this study, we determine the body wave attenuation structure of the <span class="hlt">mantle</span> beneath the northern part of the Philippine Sea. Elastic tomography studies [e.g. van der Hilst et al., 1991; Fukao et al., 1992] show a stagnant Pacific lithosphere just above the 660 km discontinuity in this region. This stagnation was caused by the trench retreat due to the back arc spreading during the past 17 - 30 Ma [Seno et al., 1993; van der Hilst, 1995; Shito and Shibutani, 2001]. Anelastic properties of the <span class="hlt">mantle</span> and lithosphere may play important roles in the interaction of the slab and <span class="hlt">mantle</span> of this area. To study the attenuation structure, we examine the difference of the observed attenuation between P and S waves. The S-P phase pair method measures δ t* using the <span class="hlt">differential</span> spectral decay between S and P waves arriving at the same station, assuming a constant Qα }/Q{β over the frequency band of 0.5 to 1.25 Hz. We use 20 earthquakes in the Izu-Bonin slab which were recorded at 43 broad-band stations of the J-array and FREESIA networks in Japan. About 700 phase pairs are used to invert for the 2-D attenuation structure. The resultant preliminary Q model shows the local variations of attenuation in the subduction zone. The slab is imaged as a low attenuation area (Qα > 1000), while Qα values in the range of 100 - 350 are found in the <span class="hlt">mantle</span> wedge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150003798','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150003798"><span>Water Content of Earth's Continental <span class="hlt">Mantle</span> Is Controlled by the Circulation of Fluids or Melts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peslier, Anne; Woodland, Alan B.; Bell, David R.; Lazarov, Marina; Lapen, Thomas J.</p> <p>2014-01-01</p> <p>A key mission of the ARES Directorate at JSC is to constrain models of the formation and geological history of terrestrial planets. Water is a crucial parameter to be measured with the aim to determine its amount and distribution in the interior of Earth, Mars, and the Moon. Most of that "water" is not liquid water per se, but rather hydrogen dissolved as a trace element in the minerals of the rocks at depth. Even so, the middle layer of <span class="hlt">differentiated</span> planets, the <span class="hlt">mantle</span>, occupies such a large volume and mass of each planet that when it is added at the planetary scale, oceans worth of water could be stored in its interior. The <span class="hlt">mantle</span> is where magmas originate. Moreover, on Earth, the <span class="hlt">mantle</span> is where the boundary between tectonic plates and the underlying asthenosphere is located. Even if <span class="hlt">mantle</span> rocks in Earth typically contain less than 200 ppm H2O, such small quantities have tremendous influence on how easily they melt (i.e., the more water there is, the more magma is produced) and deform (the more water there is, the less viscous they are). These two properties alone emphasize that to understand the distribution of volcanism and the mechanism of plate tectonics, the water content of the <span class="hlt">mantle</span> must be determined - Earth being a template to which all other terrestrial planets can be compared.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI43C..03W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI43C..03W"><span>The Fine Geochemical Structure of the Hawaiian <span class="hlt">Mantle</span> Plume: Relation to the Earth's Lowermost <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weis, D.; Harrison, L.</p> <p>2017-12-01</p> <p>The Hawaiian <span class="hlt">mantle</span> plume has been active for >80 Ma with the highest magmatic flux, also distinctly increasing with time. The identification of two clear geochemical trends (Loa-Kea) among Hawaiian volcanoes in all isotope systems has implications for the dynamics and internal structure of the plume conduit and source in the deep <span class="hlt">mantle</span>. A compilation of modern isotopic data on Hawaiian shield volcanoes and from the Northwest Hawaiian Ridge (NWHR), focusing specifically on high-precision Pb isotopes integrated with Sr, Nd and Hf isotopes, indicates the presence of source differences for Loa- and Kea-trend volcanoes that are maintained throughout the 1 Ma activity of each volcano. These differences extend back in time on all the Hawaiian Islands ( 5 Ma), and as far back as 47 Ma on the NWHR. In all isotope systems, the Loa-trend basalts are more heterogeneous by a factor of 1.5 than the Kea-trend basalts. The Hawaiian <span class="hlt">mantle</span> plume overlies the boundary between ambient Pacific lower <span class="hlt">mantle</span> on the Kea side and the Pacific LLSVP on the Loa side. Geochemical differences between Kea and Loa trends reflect preferential sampling of these two distinct sources of deep <span class="hlt">mantle</span> material, with additional contribution of ULVZ material sporadically on the Loa side. Plume movement up the gently sloping edge of the LLSVP resulted in entrainment of greater amounts of LLSVP-enriched material over time, and explains why the Hawaiian <span class="hlt">mantle</span> plume dramatically strengthens over time, contrary to plume models. Similar indications of preferential sampling at the edges of the African LLSVP are found in Kerguelen and Tristan da Cunha basalts in the Indian and Atlantic oceans, respectively. The anomalous low-velocity zones at the core-<span class="hlt">mantle</span> boundary store geochemical heterogeneities that are enriched in recycled material (EM-I type) with different compositions under the Pacific and under Africa, and that are sampled by strong <span class="hlt">mantle</span> plumes such as Hawaii and Kerguelen.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUSM.V51A..13P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUSM.V51A..13P"><span><span class="hlt">Mantle</span> Plume Temperature Variations Immediately Following Continental Breakup of the Northern North Atlantic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Parkin, C. J.; White, R. S.; Kusznir, N. J.</p> <p>2005-05-01</p> <p>The amount of melt generated by <span class="hlt">mantle</span> decompression beneath an oceanic spreading centre and hence the oceanic crustal thickness is controlled in part by the temperature of the <span class="hlt">mantle</span>. By measuring the thickness of the oceanic crust formed immediately after breakup of the northern North Atlantic during the <span class="hlt">early</span> Tertiary, we are able to deduce the maximum elevated <span class="hlt">mantle</span> temperatures caused by the presence of the Iceland <span class="hlt">mantle</span> plume. Crustal thickness variations are caused by temporal variations in the <span class="hlt">mantle</span> plume temperature: at the present Reykjanes Ridge spreading centre the plume temperature pulses on a 3-5 Myr timescale with temperature variations of c.30 K. We show results from two long-offset profiles acquired over oceanic crust; firstly a 170km line perpendicular to the Faroes rifted continetal margin where oceanic spreading developed close to the Iceland <span class="hlt">mantle</span> plume; and secondly, a 200km line perpendicular to the Hatton rifted continental margin where oceanic spreading developed 800km south of the plume. Each survey recorded long-offset refractions and reflections on OBS (Ocean Bottom Seismometers); 25 instruments, with a spacing of 2-3 km, were used for the Faroes line; and 45 instruments, with a spacing of 4-10 km were used for the Hatton-Rockall line. Accurate information for sediment velocity and thickness was acquired for the Faroes profile using a 12 km long streamer; whilst adequate sediment information was determined for the Hatton-Rockall profile using a 2.4 km streamer. By incorporating sediment structure into a joint reflection and refraction tomographic inversion of the wide-angle OBS data, we have been able to map crustal thickness across the oceanic crust in both regions. Crustal sections across the Faroes and Hatton lines cover the first 14 Myr and 17 Myr respectively, corresponding to the time interval from continental breakup through to mature seafloor spreading. With no apparent decrease in spreading rate observed thinning of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21119913','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21119913"><span>A review of recent studies on <span class="hlt">differential</span> reinforcement during skill acquisition in <span class="hlt">early</span> intervention.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vladescu, Jason C; Kodak, Tiffany</p> <p>2010-01-01</p> <p>Although the use of <span class="hlt">differential</span> reinforcement has been recommended in previous investigations and in <span class="hlt">early</span> intervention curriculum manuals, few studies have evaluated the best method for providing <span class="hlt">differential</span> reinforcement to maximize independent responding. This paper reviews previous research on the effectiveness of <span class="hlt">differential</span> reinforcement as treatment and describes important areas of future research.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999GeoRL..26.1501C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999GeoRL..26.1501C"><span>Can lower <span class="hlt">mantle</span> slab-like seismic anomalies be explained by thermal coupling between the upper and lower <span class="hlt">mantles</span>?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Čížková, Hana; Čadek, Ondřej; van den Berg, Arie P.; Vlaar, Nicolaas J.</p> <p></p> <p>Below subduction zones, high resolution seismic tomographic models resolve fast anomalies that often extend into the deep lower <span class="hlt">mantle</span>. These anomalies are generally interpreted as slabs penetrating through the 660-km seismic discontinuity, evidence in support of whole-<span class="hlt">mantle</span> convection. However, thermal coupling between two flow systems separated by an impermeable interface might provide an alternative explanation of the tomographic results. We have tested this hypothesis within the context of an axisymmetric model of <span class="hlt">mantle</span> convection in which an impermeable boundary is imposed at a depth of 660 km. When an increase in viscosity alone is imposed across the impermeable interface, our results demonstrate the dominant role of mechanical coupling between shells, producing lower <span class="hlt">mantle</span> upwellings (downwellings) below upper <span class="hlt">mantle</span> downwellings (upwellings). However, we find that the effect of mechanical coupling can be significantly weakened if a narrow low viscosity zone exists beneath the 660-km discontinuity. In such a case, both thermally induced ‘slabs’ in the lower <span class="hlt">mantle</span> and thermally activated plumes that rise from the upper/lower <span class="hlt">mantle</span> boundary are observed even though mass transfer between the shells does not exist.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920071998&hterms=geofisica&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dgeofisica','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920071998&hterms=geofisica&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dgeofisica"><span>Postglacial rebound with a non-Newtonian upper <span class="hlt">mantle</span> and a Newtonian lower <span class="hlt">mantle</span> rheology</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gasperini, Paolo; Yuen, David A.; Sabadini, Roberto</p> <p>1992-01-01</p> <p>A composite rheology is employed consisting of both linear and nonlinear creep mechanisms which are connected by a 'transition' stress. Background stress due to geodynamical processes is included. For models with a non-Newtonian upper-<span class="hlt">mantle</span> overlying a Newtonian lower-<span class="hlt">mantle</span>, the temporal responses of the displacements can reproduce those of Newtonian models. The average effective viscosity profile under the ice-load at the end of deglaciation turns out to be the crucial factor governing <span class="hlt">mantle</span> relaxation. This can explain why simple Newtonian rheology has been successful in fitting the uplift data over formerly glaciated regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V51F..07W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V51F..07W"><span>Ophiolite Perspectives on Oceanic <span class="hlt">Mantle</span> Heterogeneity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Walker, R. J.; O'Driscoll, B.; Day, J. M.; Ash, R. D.; Daly, J. S.</p> <p>2014-12-01</p> <p>. The former age corresponds, within error, to the accepted age of the ophiolite (497 ± 2 Ma). The meaning of the latter age is uncertain, but may correspond to the <span class="hlt">early</span> stages of Iapetus opening. The data imply that the oceanic <span class="hlt">mantle</span> represented by both ophiolites resembles a 'patchwork' of peridotites of different ages and compositions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.V51B0529J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.V51B0529J"><span>Recycling and <span class="hlt">Mantle</span> Stirring Determined by 142Nd/144Nd Isotopic Ratios</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jacobsen, S. B.; Ranen, M. C.</p> <p>2004-12-01</p> <p>It is now well established that 146Sm was live in the <span class="hlt">early</span> solar system with an initial uniform 146Sm/144Sm ratio of ~0.008. Harper and Jacobsen (1992) discovered that a sample from Isua (~3.8 Ga old) had a positive 142Nd/144Nd anomaly of 33 ppm when compared to normal terrestrial and chondritic Nd. Furthermore, Jacobsen and Harper (1996) reported results from other Isua as well as Acasta (~4 Ga old) samples. Three other Isua samples had a possible small range (about -15 to +15), while two Acasta samples had no anomalies (normal to within 5 ppm). The presence of 142Nd anomalies at Isua has recently been confirmed by two other groups (Boyet et al. 2003; Caro et al. 2003). The available data demonstrate both the existence of <span class="hlt">early</span> depleted <span class="hlt">mantle</span> and that the <span class="hlt">early</span> <span class="hlt">mantle</span> was isotopically heterogeneous. As discussed by Jacobsen and Harper (1996), the recycling rate can be determined by tracing the decay of the average 142Nd/144Nd value of the depleted <span class="hlt">mantle</span>. In addition, by using the 142Nd/144Nd heterogeneity in the depleted <span class="hlt">mantle</span> through time we can determine the stirring rate of the <span class="hlt">mantle</span> (Kellogg, Jacobsen and O'Connell, 2002) as a function of time. For this project our goal is to obtain a resolution in 142Nd/144Nd measurements of ~1 ppm. We have thus compared results obtained for the Nd isotope composition and 142Nd enriched standards for three different TIMS instruments: The Finnigan MAT 262 at Harvard, the Isoprobe-T and Finnigan TRITON mass spectrometers in GV Instrument's and Thermo Electron's demo laboratories in Manchester and Bremen, respectively. The Finnigan TRITON was designed in response to a request from the senior author for such an instrument. The results obtained so far demonstrate that all three instruments yield the same 142Nd/144Nd, 143Nd/144Nd and 145Nd/144Nd isotopic ratios to within a few ppm, while 148Nd/144Nd and 150Nd/144Nd ratios agree to within 10-20 ppm, when all ratios are normalized to 146Nd/144Nd using the exponential law. Due to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1851713','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1851713"><span>Gene function in <span class="hlt">early</span> mouse embryonic stem cell <span class="hlt">differentiation</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sene, Kagnew Hailesellasse; Porter, Christopher J; Palidwor, Gareth; Perez-Iratxeta, Carolina; Muro, Enrique M; Campbell, Pearl A; Rudnicki, Michael A; Andrade-Navarro, Miguel A</p> <p>2007-01-01</p> <p>Background Little is known about the genes that drive embryonic stem cell <span class="hlt">differentiation</span>. However, such knowledge is necessary if we are to exploit the therapeutic potential of stem cells. To uncover the genetic determinants of mouse embryonic stem cell (mESC) <span class="hlt">differentiation</span>, we have generated and analyzed 11-point time-series of DNA microarray data for three biologically equivalent but genetically distinct mESC lines (R1, J1, and V6.5) undergoing undirected <span class="hlt">differentiation</span> into embryoid bodies (EBs) over a period of two weeks. Results We identified the initial 12 hour period as reflecting the <span class="hlt">early</span> stages of mESC <span class="hlt">differentiation</span> and studied probe sets showing consistent changes of gene expression in that period. Gene function analysis indicated significant up-regulation of genes related to regulation of transcription and mRNA splicing, and down-regulation of genes related to intracellular signaling. Phylogenetic analysis indicated that the genes showing the largest expression changes were more likely to have originated in metazoans. The probe sets with the most consistent gene changes in the three cell lines represented 24 down-regulated and 12 up-regulated genes, all with closely related human homologues. Whereas some of these genes are known to be involved in embryonic developmental processes (e.g. Klf4, Otx2, Smn1, Socs3, Tagln, Tdgf1), our analysis points to others (such as transcription factor Phf21a, extracellular matrix related Lama1 and Cyr61, or endoplasmic reticulum related Sc4mol and Scd2) that have not been previously related to mESC function. The majority of identified functions were related to transcriptional regulation, intracellular signaling, and cytoskeleton. Genes involved in other cellular functions important in ESC <span class="hlt">differentiation</span> such as chromatin remodeling and transmembrane receptors were not observed in this set. Conclusion Our analysis profiles for the first time gene expression at a very <span class="hlt">early</span> stage of mESC <span class="hlt">differentiation</span>, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V33A2720K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V33A2720K"><span>Secondary overprinting of S-Se-Te signatures in the Earth's <span class="hlt">mantle</span>: Implications for the Late Veneer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koenig, S.; Luguet, A.; Lorand, J.; Pearson, D.</p> <p>2013-12-01</p> <p>Sulphur, Selenium and Tellurium are both chalcophile and highly siderophile elements (HSE) with near-chondritic ratios and absolute abundances in the terrestrial <span class="hlt">mantle</span> that exceed those predicted by core-<span class="hlt">mantle</span> <span class="hlt">differentiation</span>[1]. These 'excess' HSE abundances have been attributed to addition of ca. 0.5% of chondrite-like material that hit the Earth in its accretionary stage between 4 to 3.8 billion years ago after core-<span class="hlt">mantle</span> <span class="hlt">differentiation</span> (Late Veneer[2]). Therefore, like other HSE, S, Se and Te are considered potential tracers for the composition of the Late Veneer, provided that their bulk silicate Earth abundances are properly constrained. In contrast to ca. 250 ppm S, Se and Te are ultra-trace elements in the terrestrial <span class="hlt">mantle</span>. Like all HSE, they are furthermore controlled by base metal sulphides (BMS) and micrometric platinum group minerals (PGMs)[3]. This strong control exerted by the host mineralogy and petrology on the S-Se-Te systematics at both the micro-scale and the whole-rock scale makes detailed mineralogical and petrological studies of BMS and PGM a pre-requisite to fully understand and accurately interpret the whole-rock signatures. Here we combine in-situ sulphide data and detailed mineralogical observations with whole-rock S-Se-Te-HSE signatures of both lherzolites and harburgites from different geodynamic settings. We demonstrate that the near-chondritic Se and Te signature of 'fertile' <span class="hlt">mantle</span> rocks (Se/Te ≈9×5) is not a primitive signature of the Earth's <span class="hlt">mantle</span>, but rather reflects strong enrichment in metasomatic HSE host phases, which erased previous pristine signatures. Consequently, current attempts to identify a potential Late Veneer composition are seriously flawed because, neither refertilisation/metasomatism nor true melt depletion (e.g. harzburgitic residues) have been taken into account for the Primitive Upper <span class="hlt">Mantle</span> composition estimate[4]. Our combined whole rock and in-situ sulphide data indicate a refertilisation trend</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2884364','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2884364"><span>A REVIEW OF RECENT STUDIES ON <span class="hlt">DIFFERENTIAL</span> REINFORCEMENT DURING SKILL ACQUISITION IN <span class="hlt">EARLY</span> INTERVENTION</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Vladescu, Jason C; Kodak, Tiffany</p> <p>2010-01-01</p> <p>Although the use of <span class="hlt">differential</span> reinforcement has been recommended in previous investigations and in <span class="hlt">early</span> intervention curriculum manuals, few studies have evaluated the best method for providing <span class="hlt">differential</span> reinforcement to maximize independent responding. This paper reviews previous research on the effectiveness of <span class="hlt">differential</span> reinforcement as treatment and describes important areas of future research. PMID:21119913</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950041672&hterms=Manga&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DManga','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950041672&hterms=Manga&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DManga"><span>The interaction of plume heads with compositional discontinuities in the Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Manga, Michael; Stone, Howard A.; O'Connell, Richard J.</p> <p>1993-01-01</p> <p>The effects of compositional discontinuities of density and viscosity in the Earth's <span class="hlt">mantle</span> on the ascent of <span class="hlt">mantle</span> plume heads is studied using a boundary integral numerical technique. Three specific problems are considered: (1) a plume head rising away from a deformable interface, (2) a plume head passing through an interface, and (3) a plume head approaching the surface of the Earth. For the case of a plume attached to a free-surface, the calculated time-dependent plume shapesare compared with experimental results. Two principle modes of plume head deformation are observed: plume head elingation or the formation of a cavity inside the plume head. The inferred structure of <span class="hlt">mantle</span> plumes, namely, a large plume head with a long tail, is characteristic of plumes attached to their source region, and also of buoyant material moving away from an interface and of buoyant material moving through an interface from a high- to low-viscosity region. As a rising plume head approaches the upper <span class="hlt">mantle</span>, most of the lower <span class="hlt">mantle</span> will quickly drain from the gap between the plume head and the upper <span class="hlt">mantle</span> if the plume head enters the upper <span class="hlt">mantle</span>. If the plume head moves from a high- to low-viscosity region, the plume head becomes significantly elongated and, for the viscosity contrasts thought to exist in the Earth, could extend from the 670 km discontinuity to the surface. Plume heads that are extended owing to a viscosity decrease in the upper <span class="hlt">mantle</span> have a cylindrical geometry. The dynamic surface topography induced by plume heads is bell-shaped when the top of the plume head is at depths greater than about 0.1 plume head radii. As the plume head approaches the surface and spreads, the dynamic topography becomes plateau-shaped. The largest stresses are produced in the <span class="hlt">early</span> stages of plume spreading when the plume head is still nearly spherical, and the surface expression of these stresses is likely to be dominated by radial extension. As the plume spreads, compressional</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.T51E2505B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.T51E2505B"><span>Limit of Predictability in <span class="hlt">Mantle</span> Convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bello, L.; Coltice, N.; Rolf, T.; Tackley, P. J.</p> <p>2013-12-01</p> <p>Linking <span class="hlt">mantle</span> convection models with Earth's tectonic history has received considerable attention in recent years: modeling the evolution of supercontinent cycles, predicting present-day <span class="hlt">mantle</span> structure or improving plate reconstructions. Predictions of future supercontinents are currently being made based on seismic tomography images, plate motion history and <span class="hlt">mantle</span> convection models, and methods of data assimilation for <span class="hlt">mantle</span> flow are developing. However, so far there are no studies of the limit of predictability these models are facing. Indeed, given the chaotic nature of <span class="hlt">mantle</span> convection, we can expect forecasts and hindcasts to have a limited range of predictability. We propose here to use an approach similar to those used in dynamic meteorology, and more recently for the geodynamo, to evaluate the predictability limit of <span class="hlt">mantle</span> dynamics forecasts. Following the pioneering works in weather forecast (Lorenz 1965), we study the time evolution of twin experiments, started from two very close initial temperature fields and monitor the error growth. We extract a characteristic time of the system, known as the e-folding timescale, which will be used to estimate the predictability limit. The final predictability time will depend on the imposed initial error and the error tolerance in our model. We compute 3D spherical convection solutions using StagYY (Tackley, 2008). We first evaluate the influence of the Rayleigh number on the limit of predictability of isoviscous convection. Then, we investigate the effects of various rheologies, from the simplest (isoviscous <span class="hlt">mantle</span>) to more complex ones (plate-like behavior and floating continents). We show that the e-folding time increases with the wavelength of the flow and reaches 10Myrs with plate-like behavior and continents. Such an e-folding time together with the uncertainties in <span class="hlt">mantle</span> temperature distribution suggests prediction of <span class="hlt">mantle</span> structure from an initial given state is limited to <50 Myrs. References: 1</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70188976','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70188976"><span>Seismic structure of the central US crust and upper <span class="hlt">mantle</span>: Uniqueness of the Reelfoot Rift</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Pollitz, Fred; Mooney, Walter D.</p> <p>2014-01-01</p> <p>Using seismic surface waves recorded with Earthscope's Transportable Array, we apply surface wave imaging to determine 3D seismic velocity in the crust and uppermost <span class="hlt">mantle</span>. Our images span several Proterozoic and <span class="hlt">early</span> Cambrian rift zones (Mid-Continent Rift, Rough Creek Graben—Rome trough, Birmingham trough, Southern Oklahoma Aulacogen, and Reelfoot Rift). While ancient rifts are generally associated with low crustal velocity because of the presence of thick sedimentary sequences, the Reelfoot Rift is unique in its association with low <span class="hlt">mantle</span> seismic velocity. Its <span class="hlt">mantle</span> low-velocity zone (LVZ) is exceptionally pronounced and extends down to at least 200 km depth. This LVZ is of variable width, being relatively narrow (∼50km">∼50km wide) within the northern Reelfoot Rift, which hosts the New Madrid Seismic Zone (NMSZ). We hypothesize that this <span class="hlt">mantle</span> volume is weaker than its surroundings and that the Reelfoot Rift consequently has relatively low elastic plate thickness, which would tend to concentrate tectonic stress within this zone. No other intraplate ancient rift zone is known to be associated with such a deep <span class="hlt">mantle</span> low-velocity anomaly, which suggests that the NMSZ is more susceptible to external stress perturbations than other ancient rift zones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29847803','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29847803"><span>Enhancer and Transcription Factor Dynamics during Myeloid <span class="hlt">Differentiation</span> Reveal an <span class="hlt">Early</span> <span class="hlt">Differentiation</span> Block in Cebpa null Progenitors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pundhir, Sachin; Bratt Lauridsen, Felicia Kathrine; Schuster, Mikkel Bruhn; Jakobsen, Janus Schou; Ge, Ying; Schoof, Erwin Marten; Rapin, Nicolas; Waage, Johannes; Hasemann, Marie Sigurd; Porse, Bo Torben</p> <p>2018-05-29</p> <p>Transcription factors PU.1 and CEBPA are required for the proper coordination of enhancer activity during granulocytic-monocytic (GM) lineage <span class="hlt">differentiation</span> to form myeloid cells. However, precisely how these factors control the chronology of enhancer establishment during <span class="hlt">differentiation</span> is not known. Through integrated analyses of enhancer dynamics, transcription factor binding, and proximal gene expression during successive stages of murine GM-lineage <span class="hlt">differentiation</span>, we unravel the distinct kinetics by which PU.1 and CEBPA coordinate GM enhancer activity. We find no evidence of a pioneering function of PU.1 during late GM-lineage <span class="hlt">differentiation</span>. Instead, we delineate a set of enhancers that gain accessibility in a CEBPA-dependent manner, suggesting a pioneering function of CEBPA. Analyses of Cebpa null bone marrow demonstrate that CEBPA controls PU.1 levels and, unexpectedly, that the loss of CEBPA results in an <span class="hlt">early</span> <span class="hlt">differentiation</span> block. Taken together, our data provide insights into how PU.1 and CEBPA functionally interact to drive GM-lineage <span class="hlt">differentiation</span>. Copyright © 2018 The Author(s). Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70012374','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70012374"><span>Nd-isotopes in selected <span class="hlt">mantle</span>-derived rocks and minerals and their implications for <span class="hlt">mantle</span> evolution</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Basu, A.R.; Tatsumoto, M.</p> <p>1980-01-01</p> <p>The Sm-Nd systematics in a variety of <span class="hlt">mantle</span>-derived samples including kimberlites, alnoite, carbonatite, pyroxene and amphibole inclusions in alkali basalts and xenolithic eclogites, granulites and a pyroxene megacryst in kimberlites are reported. The additional data on kimberlites strengthen our earlier conclusion that kimberlites are derived from a relatively undifferentiated chondritic <span class="hlt">mantle</span> source. This conclusion is based on the observation that the e{open}Nd values of most of the kimberlites are near zero. In contrast with the kimberlites, their garnet lherzolite inclusions show both time-averaged Nd enrichment and depletion with respect to Sm. Separated clinopyroxenes in eclogite xenoliths from the Roberts Victor kimberlite pipe show both positive and negative e{open}Nd values suggesting different genetic history. A whole rock lower crustal scapolite granulite xenolith from the Matsoku kimberlite pipe shows a negative e{open}Nd value of -4.2, possibly representative of the base of the crust in Lesotho. It appears that all inclusions, mafic and ultramafic, in kimberlites are unrelated to their kimberlite host. The above data and additional Sm-Nd data on xenoliths in alkali basalts, alpine peridotite and alnoite-carbonatites are used to construct a model for the upper 200 km of the earth's <span class="hlt">mantle</span> - both oceanic and continental. The essential feature of this model is the increasing degree of fertility of the <span class="hlt">mantle</span> with depth. The kimberlite's source at depths below 200 km in the subcontinental <span class="hlt">mantle</span> is the most primitive in this model, and this primitive layer is also extended to the suboceanic <span class="hlt">mantle</span>. However, it is clear from the Nd-isotopic data in the xenoliths of the continental kimberlites that above 200 km the continental <span class="hlt">mantle</span> is distinctly different from their suboceanic counterpart. ?? 1980 Springer-Verlag.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860017700','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860017700"><span><span class="hlt">Early</span> <span class="hlt">differentiation</span> of the Moon: Experimental and modeling studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Longhi, J.</p> <p>1986-01-01</p> <p>Major accomplishments include the mapping out of liquidus boundaries of lunar and meteoritic basalts at low pressure; the refinement of computer models that simulate low pressure fractional crystallization; the development of a computer model to calculate high pressure partial melting of the lunar and Martian interiors; and the proposal of a hypothesis of <span class="hlt">early</span> lunar <span class="hlt">differentiation</span> based upon terrestrial analogs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JGRB..109.3410M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JGRB..109.3410M"><span>Numerical simulations of the <span class="hlt">mantle</span> lithosphere delamination</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morency, C.; Doin, M.-P.</p> <p>2004-03-01</p> <p>Sudden uplift, extension, and increased igneous activity are often explained by rapid mechanical thinning of the lithospheric <span class="hlt">mantle</span>. Two main thinning mechanisms have been proposed, convective removal of a thickened lithospheric root and delamination of the <span class="hlt">mantle</span> lithosphere along the Moho. In the latter case, the whole <span class="hlt">mantle</span> lithosphere peels away from the crust by the propagation of a localized shear zone and sinks into the <span class="hlt">mantle</span>. To study this mechanism, we perform two-dimensional (2-D) numerical simulations of convection using a viscoplastic rheology with an effective viscosity depending strongly on temperature, depth, composition (crust/<span class="hlt">mantle</span>), and stress. The simulations develop in four steps. (1) We first obtain "classical" sublithospheric convection for a long time period (˜300 Myr), yielding a slightly heterogeneous lithospheric temperature structure. (2) At some time, in some simulations, a strong thinning of the <span class="hlt">mantle</span> occurs progressively in a small area (˜100 km wide). This process puts the asthenosphere in direct contact with the lower crust. (3) Large pieces of <span class="hlt">mantle</span> lithosphere then quickly sink into the <span class="hlt">mantle</span> by the horizontal propagation of a detachment level away from the "asthenospheric conduit" or by progressive erosion on the flanks of the delaminated area. (4) Delamination pauses or stops when the lithospheric <span class="hlt">mantle</span> part detaches or when small-scale convection on the flanks of the delaminated area is counterbalanced by heat diffusion. We determine the parameters (crustal thicknesses, activation energies, and friction coefficients) leading to delamination initiation (step 2). We find that delamination initiates where the Moho temperature is the highest, as soon as the crust and <span class="hlt">mantle</span> viscosities are sufficiently low. Delamination should occur on Earth when the Moho temperature exceeds ˜800°C. This condition can be reached by thermal relaxation in a thickened crust in orogenic setting or by corner flow lithospheric erosion in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1513389S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1513389S"><span>Comparing the composition of the earliest basalts erupted by the Iceland and Afar <span class="hlt">mantle</span> plumes.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stuart, Finlay M.</p> <p>2013-04-01</p> <p>The first basalts erupted by <span class="hlt">mantle</span> plumes are typically generated by <span class="hlt">mantle</span> melting at temperatures 200-300°C higher than average ambient <span class="hlt">mantle</span>. This is consistent with the derivation of from a thermal boundary layer at the core-<span class="hlt">mantle</span> boundary. <span class="hlt">Mantle</span> plume temperatures decrease with time, likely as large plume heads give way to thin plume conduits. Consequently the <span class="hlt">early</span>, hot plume basalts are a window into the deep <span class="hlt">mantle</span>. At it's simplest they provide a test of whether the discrete plume source regions are primordial <span class="hlt">mantle</span> that have been isolated since soon after Earth accretion, or have substantial contributions from subducted slabs. Here I present new isotopic and trace element determinations of the earliest picritic basalts from the ~30 Ma Afar plume in Ethiopia. They will be compared with similar material from the ~60 Ma proto-Iceland plume (PIP) in an effort to test prevailing models regarding the source of <span class="hlt">mantle</span> plumes. The extremely primordial nature of the helium in the PIP picrites (3He/4He ~ 50 Ra) contrasts with much lower values of the Ethiopian flood basalt province (~21 Ra). The Iceland plume 3He/4He has decreased (linearly) with time, mirroring the secular cooling of the Iceland <span class="hlt">mantle</span> plume identified by decreasing MgO and FeO in primary melts. In 60 million years the Iceland plume 3He/4He is still higher than the maximum Afar plume value. The Sr-Nd-Pb isotopic composition of the high 3He/4He Ethiopian flood basalt province picrites are remarkably homogenous (e.g. 87Sr/86Sr = 0.70396-0.70412; 206Pb/204Pb = 18.82-19.01). In comparison the PIP picrites have ranges that span nearly the global range of E-MORB and N-MORB. The Afar and proto-Iceland <span class="hlt">mantle</span> plumes are clearly not initiated in a single deep <span class="hlt">mantle</span> domain with the same depletion/enrichment and degassing histories, and the same scale of heterogeneity. This implies that there is more than one plume source region/mechanism that is capable of generating comparable volumes of basalt melt</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26037825','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26037825"><span>Magma Ocean Depth and Oxygen Fugacity in the <span class="hlt">Early</span> Earth--Implications for Biochemistry.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Righter, Kevin</p> <p>2015-09-01</p> <p>A large class of elements, referred to as the siderophile (iron-loving) elements, in the Earth's <span class="hlt">mantle</span> can be explained by an <span class="hlt">early</span> deep magma ocean on the <span class="hlt">early</span> Earth in which the <span class="hlt">mantle</span> equilibrated with metallic liquid (core liquid). This stage would have affected the distribution of some of the classic volatile elements that are also essential ingredients for life and biochemistry - H, C, S, and N. Estimates are made of the H, C, S, and N contents of Earth's <span class="hlt">early</span> <span class="hlt">mantle</span> after core formation, considering the effects of variable temperature, pressure, oxygen fugacity, and composition on their partitioning. Assessment is made of whether additional, exogenous, sources are required to explain the observed <span class="hlt">mantle</span> concentrations, and areas are identified where additional data and experimentation would lead to an improved understanding of this phase of Earth's history.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.197..132T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.197..132T"><span>Europium and strontium anomalies in the MORB source <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, Ming; McDonough, William F.; Ash, Richard D.</p> <p>2017-01-01</p> <p>Lower crustal recycling depletes the continental crust of Eu and Sr and returns Eu and Sr enriched materials into the <span class="hlt">mantle</span> (e.g., Tang et al., 2015, Geology). To test the hypothesis that the MORB source <span class="hlt">mantle</span> balances the Eu and Sr deficits in the continental crust, we carried out high precision Eu/Eu∗ and Sr/Sr∗ measurement for 72 MORB glasses with MgO >8.5% from the Pacific, Indian, and Atlantic mid-ocean ridges. MORB glasses with MgO ⩾ 9 wt.% have a mean Eu/Eu∗ of 1.025 ± 0.025 (2 σm, n = 46) and Sr/Sr∗ of 1.242 ± 0.093 (2 σm, n = 41) and these ratios are positively correlated. These samples show both positive and negative Eu and Sr anomalies, with no correlations between Eu/Eu∗ vs. MgO or Sr/Sr∗ vs. MgO, suggesting that the anomalies are not produced by plagioclase fractionation at MgO >9 wt.% and, thus, other processes must be responsible for generating the anomalies. We term these MORB samples primitive MORBs, as they record the melt Eu/Eu∗ and Sr/Sr∗ before plagioclase fractionation. Consequently, the mean oceanic crust, including cumulates, has a bulk Eu/Eu∗ of ∼1 and 20% Sr excess. Considering that divalent Sr and Eu(II) diffuse faster than trivalent Pr, Nd, Sm, and Gd, we evaluated this kinetic effect on Sm-Eu-Gd and Pr-Sr-Nd fractionations during spinel peridotite partial melting in the MORB source <span class="hlt">mantle</span>. Our modeling shows that the correlated Eu and Sr anomalies seen in primitive MORBs may result from disequilibrium <span class="hlt">mantle</span> melting. Melt fractions produced during <span class="hlt">early</span>- and late-stage melting may carry positive and negative Eu and Sr anomalies, respectively, that overlap with the ranges documented in primitive MORBs. Because the net effect of disequilibrium melting is to produce partial melts with bulk positive Eu and Sr anomalies, the MORB source <span class="hlt">mantle</span> must have Eu/Eu∗ < 1.025 ± 0.025 (2 σm) and Sr/Sr∗ < 1.242 ± 0.093 (2 σm). Although we cannot rule out the possibility that recycled lower continental crustal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoJI.204.1237N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoJI.204.1237N"><span>Total meltwater volume since the Last Glacial Maximum and viscosity structure of Earth's <span class="hlt">mantle</span> inferred from relative sea level changes at Barbados and Bonaparte Gulf and GIA-induced J˙2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakada, Masao; Okuno, Jun'ichi; Yokoyama, Yusuke</p> <p>2016-02-01</p> <p>Inference of globally averaged eustatic sea level (ESL) rise since the Last Glacial Maximum (LGM) highly depends on the interpretation of relative sea level (RSL) observations at Barbados and Bonaparte Gulf, Australia, which are sensitive to the viscosity structure of Earth's <span class="hlt">mantle</span>. Here we examine the RSL changes at the LGM for Barbados and Bonaparte Gulf ({{RSL}}_{{L}}^{{{Bar}}} and {{RSL}}_{{L}}^{{{Bon}}}), <span class="hlt">differential</span> RSL for both sites (Δ {{RSL}}_{{L}}^{{{Bar}},{{Bon}}}) and rate of change of degree-two harmonics of Earth's geopotential due to glacial isostatic adjustment (GIA) process (GIA-induced J˙2) to infer the ESL component and viscosity structure of Earth's <span class="hlt">mantle</span>. <span class="hlt">Differential</span> RSL, Δ {{RSL}}_{{L}}^{{{Bar}},{{Bon}}} and GIA-induced J˙2 are dominantly sensitive to the lower-<span class="hlt">mantle</span> viscosity, and nearly insensitive to the upper-<span class="hlt">mantle</span> rheological structure and GIA ice models with an ESL component of about (120-130) m. The comparison between the predicted and observationally derived Δ {{RSL}}_{{L}}^{{{Bar}},{{Bon}}} indicates the lower-<span class="hlt">mantle</span> viscosity higher than ˜2 × 1022 Pa s, and the observationally derived GIA-induced J˙2 of -(6.0-6.5) × 10-11 yr-1 indicates two permissible solutions for the lower <span class="hlt">mantle</span>, ˜1022 and (5-10) × 1022 Pa s. That is, the effective lower-<span class="hlt">mantle</span> viscosity inferred from these two observational constraints is (5-10) × 1022 Pa s. The LGM RSL changes at both sites, {{RSL}}_{{L}}^{{{Bar}}} and {{RSL}}_{{L}}^{{{Bon}}}, are also sensitive to the ESL component and upper-<span class="hlt">mantle</span> viscosity as well as the lower-<span class="hlt">mantle</span> viscosity. The permissible upper-<span class="hlt">mantle</span> viscosity increases with decreasing ESL component due to the sensitivity of the LGM sea level at Bonaparte Gulf ({{RSL}}_{{L}}^{{{Bon}}}) to the upper-<span class="hlt">mantle</span> viscosity, and inferred upper-<span class="hlt">mantle</span> viscosity for adopted lithospheric thicknesses of 65 and 100 km is (1-3) × 1020 Pa s for ESL˜130 m and (4-10) × 1020 Pa s for ESL˜125 m. The former solution of (1-3) × 1020</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LPICo2084.4011K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LPICo2084.4011K"><span>Using the South Pole-Aitken (SPA) Impact Melt Composition to Infer Upper <span class="hlt">Mantle</span> Mineralogy and Timing of Potential <span class="hlt">Mantle</span> Overturn</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kring, D. A.; Needham, D. H.</p> <p>2018-05-01</p> <p>Observed melt composition within the SPA basin are consistent with an impact prior to <span class="hlt">mantle</span> overturn, when the upper <span class="hlt">mantle</span> contained clinopyroxene rather than olivine. Potentially, the impact triggered <span class="hlt">mantle</span> overturn.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.U52A0011K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.U52A0011K"><span>Feldspar palaeo-isochrons from <span class="hlt">early</span> Archaean TTGs: Pb-isotope evidence for a high U/Pb terrestrial Hadean crust</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kamber, B. S.; Whitehouse, M. J.; Moorbath, S.; Collerson, K. D.</p> <p>2001-12-01</p> <p>Feldspar lead-isotope data for 22 <span class="hlt">early</span> Archaean (3.80-3.82 Ga) tonalitic gneisses from an area south of the Isua greenstone belt (IGB),West Greenland, define a steep linear trend in common Pb-isotope space with an apparent age of 4480+/-77 Ma. Feldspars from interleaved amphibolites yield a similar array corresponding to a date of 4455+/-540 Ma. These regression lines are palaeo-isochrons that formed during feldspar-whole rock Pb-isotope homogenisation a long time (1.8 Ga) after rock formation but confirm the extreme antiquity (3.81 Ga) of the gneissic protoliths [1; this study]. Unlike their whole-rock counterparts, feldspar palaeo-isochrons are immune to rotational effects caused by the vagaries of U/Pb fractionation. Hence, comparison of their intercept with <span class="hlt">mantle</span> Pb-isotope evolution models yields meaningful information regarding the source history of the magmatic precursors. The locus of intersection between the palaeo-isochrons and terrestrial <span class="hlt">mantle</span> Pb-isotope evolution lines shows that the gneissic precursors of these 3.81 Ga gneisses were derived from a source with a substantially higher time-integrated U/Pb ratio than the <span class="hlt">mantle</span>. Similar requirements for a high U/Pb source have been found for IGB BIF [2], IGB carbonate [3], and particularly IGB galenas [4]. Significantly, a single high U/Pb source that separated from the MORB-source <span class="hlt">mantle</span> at ca. 4.3 Ga with a 238U/204Pb of ca. 10.5 provides a good fit to all these observations. In contrast to many previous models based on Nd and Hf-isotope evidence we propose that this reservoir was not a <span class="hlt">mantle</span> source but the Hadean basaltic crust which, in the absence of an operating subduction process, encased the <span class="hlt">early</span> Earth. <span class="hlt">Differentiation</span> of the <span class="hlt">early</span> high U/Pb basaltic crust could have occurred in response to gravitational sinking of cold <span class="hlt">mantle</span> material or meteorite impact, and produced zircon-bearing magmatic rocks. The subchondritic Hf-isotope ratios of ca. 3.8 Ga zircons support this model [5] provided that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.489..258C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.489..258C"><span><span class="hlt">Mantle</span> flow influence on subduction evolution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chertova, Maria V.; Spakman, Wim; Steinberger, Bernhard</p> <p>2018-05-01</p> <p>The impact of remotely forced <span class="hlt">mantle</span> flow on regional subduction evolution is largely unexplored. Here we investigate this by means of 3D thermo-mechanical numerical modeling using a regional modeling domain. We start with simplified models consisting of a 600 km (or 1400 km) wide subducting plate surrounded by other plates. <span class="hlt">Mantle</span> inflow of ∼3 cm/yr is prescribed during 25 Myr of slab evolution on a subset of the domain boundaries while the other side boundaries are open. Our experiments show that the influence of imposed <span class="hlt">mantle</span> flow on subduction evolution is the least for trench-perpendicular <span class="hlt">mantle</span> inflow from either the back or front of the slab leading to 10-50 km changes in slab morphology and trench position while no strong slab dip changes were observed, as compared to a reference model with no imposed <span class="hlt">mantle</span> inflow. In experiments with trench-oblique <span class="hlt">mantle</span> inflow we notice larger effects of slab bending and slab translation of the order of 100-200 km. Lastly, we investigate how subduction in the western Mediterranean region is influenced by remotely excited <span class="hlt">mantle</span> flow that is computed by back-advection of a temperature and density model scaled from a global seismic tomography model. After 35 Myr of subduction evolution we find 10-50 km changes in slab position and slab morphology and a slight change in overall slab tilt. Our study shows that remotely forced <span class="hlt">mantle</span> flow leads to secondary effects on slab evolution as compared to slab buoyancy and plate motion. Still these secondary effects occur on scales, 10-50 km, typical for the large-scale deformation of the overlying crust and thus may still be of large importance for understanding geological evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5200905','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5200905"><span><span class="hlt">Early</span> molecular events during retinoic acid induced <span class="hlt">differentiation</span> of neuromesodermal progenitors</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Cunningham, Thomas J.; Colas, Alexandre</p> <p>2016-01-01</p> <p>ABSTRACT Bipotent neuromesodermal progenitors (NMPs) residing in the caudal epiblast drive coordinated body axis extension by generating both posterior neuroectoderm and presomitic mesoderm. Retinoic acid (RA) is required for body axis extension, however the <span class="hlt">early</span> molecular response to RA signaling is poorly defined, as is its relationship to NMP biology. As endogenous RA is first seen near the time when NMPs appear, we used WNT/FGF agonists to <span class="hlt">differentiate</span> embryonic stem cells to NMPs which were then treated with a short 2-h pulse of 25 nM RA or 1 µM RA followed by RNA-seq transcriptome analysis. <span class="hlt">Differential</span> expression analysis of this dataset indicated that treatment with 25 nM RA, but not 1 µM RA, provided physiologically relevant findings. The 25 nM RA dataset yielded a cohort of previously known caudal RA target genes including Fgf8 (repressed) and Sox2 (activated), plus novel <span class="hlt">early</span> RA signaling targets with nearby conserved RA response elements. Importantly, validation of top-ranked genes in vivo using RA-deficient Raldh2−/− embryos identified novel examples of RA activation (Nkx1-2, Zfp503, Zfp703, Gbx2, Fgf15, Nt5e) or RA repression (Id1) of genes expressed in the NMP niche or progeny. These findings provide evidence for <span class="hlt">early</span> instructive and permissive roles of RA in controlling <span class="hlt">differentiation</span> of NMPs to neural and mesodermal lineages. PMID:27793834</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.T41E2998H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.T41E2998H"><span>Modeling Continental Rifts and Melting Under Precambrian <span class="hlt">Mantle</span> Conditions: Effects of <span class="hlt">Mantle</span> Potential Temperature and Rheology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, M.; Moucha, R.; Rooney, T. O.; Stein, S.; Stein, C. A.</p> <p>2016-12-01</p> <p>The Mid-Continent Rift System (MCRS) is a 2000 kilometer-long failed rift which formed within the Precambrian continent of Laurentia ca. 1.1 Ga. The MCRS is part of the Keweenaw large igneous province (LIP), and is dominantly composed of flood basalts, with subordinate rhyolite. While continental rifts and LIPs are frequently spatially related, it is unusual for a rift to be filled with flood basalts. Existing work has suggested that the presence of large volumes of flood basalts within the MCRS is the result of the rift interacting with anomalously hot <span class="hlt">mantle</span> material, possibly a <span class="hlt">mantle</span> plume. However, ambient <span class="hlt">mantle</span> conditions were much hotter during the late Proterozoic than in the modern <span class="hlt">mantle</span>. This raises the question - could rifting alone generate the significant volume of decompressive melt from the ambient atmosphere without the need for a <span class="hlt">mantle</span> plume? In this contribution, we utilize a 2D particle-in-cell thermomechanical visco-elasto-plastic code (e.g. Gerya, 2010; & references therein) to numerically explore the parameter space: specifically, the <span class="hlt">mantle</span> potential temperature, plume excess temperature and volume, extension rates and rheology, and estimate the amount of melt produced in a Precambrian continental rift setting. *This submission is a result of Hansen's participation in GLADE, a nine week summer REU program directed by Dave Stegman (SIO/UCSD).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.212.2206N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.212.2206N"><span>Inference of viscosity jump at 670 km depth and lower <span class="hlt">mantle</span> viscosity structure from GIA observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakada, Masao; Okuno, Jun'ichi; Irie, Yoshiya</p> <p>2018-03-01</p> <p>A viscosity model with an exponential profile described by temperature (T) and pressure (P) distributions and constant activation energy (E_{{{um}}}^{{*}} for the upper <span class="hlt">mantle</span> and E_{{{lm}}}^* for the lower <span class="hlt">mantle</span>) and volume (V_{{{um}}}^{{*}} and V_{{{lm}}}^*) is employed in inferring the viscosity structure of the Earth's <span class="hlt">mantle</span> from observations of glacial isostatic adjustment (GIA). We first construct standard viscosity models with an average upper-<span class="hlt">mantle</span> viscosity ({\\bar{η }_{{{um}}}}) of 2 × 1020 Pa s, a typical value for the oceanic upper-<span class="hlt">mantle</span> viscosity, satisfying the observationally derived three GIA-related observables, GIA-induced rate of change of the degree-two zonal harmonic of the geopotential, {\\dot{J}_2}, and <span class="hlt">differential</span> relative sea level (RSL) changes for the Last Glacial Maximum sea levels at Barbados and Bonaparte Gulf in Australia and for RSL changes at 6 kyr BP for Karumba and Halifax Bay in Australia. Standard viscosity models inferred from three GIA-related observables are characterized by a viscosity of ˜1023 Pa s in the deep <span class="hlt">mantle</span> for an assumed viscosity at 670 km depth, ηlm(670), of (1 - 50) × 1021 Pa s. Postglacial RSL changes at Southport, Bermuda and Everglades in the intermediate region of the North American ice sheet, largely dependent on its gross melting history, have a crucial potential for inference of a viscosity jump at 670 km depth. The analyses of these RSL changes based on the viscosity models with {\\bar{η }_{{{um}}}} ≥ 2 × 1020 Pa s and lower-<span class="hlt">mantle</span> viscosity structures for the standard models yield permissible {\\bar{η }_{{{um}}}} and ηlm (670) values, although there is a trade-off between the viscosity and ice history models. Our preferred {\\bar{η }_{{{um}}}} and ηlm (670) values are ˜(7 - 9) × 1020 and ˜1022 Pa s, respectively, and the {\\bar{η }_{{{um}}}} is higher than that for the typical value of oceanic upper <span class="hlt">mantle</span>, which may reflect a moderate laterally heterogeneous upper-<span class="hlt">mantle</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.S32A..06T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.S32A..06T"><span>Improved P-wave Tomography of the Lowermost <span class="hlt">Mantle</span> and Consequences for <span class="hlt">Mantle</span> and Core Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tkalcic, H.; Young, M. K.; Muir, J. B.</p> <p>2014-12-01</p> <p>The core <span class="hlt">mantle</span> boundary (CMB) separates the liquid iron core from the slowly-convecting solid <span class="hlt">mantle</span>. The ~300 km thick barrier above the boundary has proven to be far more than a simple dividing layer; rather it is a complex region with a range of proposed phenomena such as thermal and compositional heterogeneity, partial melting and anisotropy. Characterizing the heterogeneity in the lowermost <span class="hlt">mantle</span> through seismic tomography will prove crucial to accurately understanding key geodynamical processes within our planet, not just in the <span class="hlt">mantle</span> above, but also a possible "mapping" onto the inner core boundary (ICB) through a thermochemical convection in the outer core, which in turn might control the growth of the inner core (e.g. Aubert et al., 2008; Gubbins et al., 2011). Here we obtain high-resolution compressional wave (P-wave) velocity images and uncertainty estimates for the lowermost <span class="hlt">mantle</span> using travel time data collected by waveform cross-correlation. Strikingly, independent datasets of seismic phases that "see" the lowermost <span class="hlt">mantle</span> in a different way yield similar P-wave velocity distributions at lower harmonic degrees. We also consider the effect of CMB topography. The images obtained are void of explicit model parameterization and regularization (through transdimensional Bayesian tomography) and contain features on multiple spatial scales. Subsequent spectral analyses reveal a power of heterogeneity three times larger than previous estimates. The P-wave tomograms of the lowermost <span class="hlt">mantle</span> contain the harmonic degree 2-structure, similar to tomographic images derived from S-wave data (e.g. Ritsema et al. 2011), but with additional higher harmonic degrees (notably, 3-7). In other words, the heterogeneity size is uniformly distributed between about 500 and 6000 km. Inter alia, the resulting heterogeneity spectrum provides a bridge between the long-wavelength features of most global models and the very short-scale dimensions of scatterers mapped in independent</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.P21A1582S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.P21A1582S"><span>Thermodynamic properties, melting temperature and viscosity of the <span class="hlt">mantles</span> of Super Earths</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stamenkovic, V.; Spohn, T.; Breuer, D.</p> <p>2010-12-01</p> <p>The recent dicscovery of extrasolar planets with radii of about twice the Earth radius and masses of several Earth masses such as e.g., Corot-7b (approx 5Mearth and 1.6Rearth, Queloz et al. 2009) has increased the interest in the properties of rock at extremely high pressures. While the pressure at the Earth’s core-<span class="hlt">mantle</span> boundary is about 135GPa, pressures at the base of the <span class="hlt">mantles</span> of extraterrestrial rocky planets - if these are at all <span class="hlt">differentiated</span> into <span class="hlt">mantles</span> and cores - may reach Tera Pascals. Although the properties and the mineralogy of rock at extremely high pressure is little known there have been speculations about <span class="hlt">mantle</span> convection, plate tectonics and dynamo action in these “Super-Earths”. We assume that the <span class="hlt">mantles</span> of these planets can be thought of as consisting of perovskite but we discuss the effects of the post-perovskite transition and of MgO. We use the Keane equation of state and the Slater relation (see e.g., Stacey and Davies 2004) to derive an infinite pressure value for the Grüneisen parameter of 1.035. To derive this value we adopted the infinite pressure limit for K’ (pressure derivative of the bulk modulus) of 2.41 as derived by Stacey and Davies (2004) by fitting PREM. We further use the Lindeman law to calculate the melting curve. We gauge the melting curve using the available experimental data for pressures up to 120GPa. The melting temperature profile reaches 6000K at 135GPa and increases to temperatures between 12,000K and 24,000K at 1.1TPa with a preferred value of 21,000K. We find the adiabatic temperature increase to reach 2,500K at 135GPa and 5,400K at 1.1TPa. To calculate the pressure dependence of the viscosity we assume that the rheology is diffusion controlled and calculate the partial derivative with respect to pressure of the activation enthalpy. We cast the partial derivative in terms of an activation volume and use the semi-empirical homologous temperature scaling (e.g., Karato 2008). We find that the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005GMS...160....9H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005GMS...160....9H"><span>Noble gas models of <span class="hlt">mantle</span> structure and reservoir mass transfer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harrison, Darrell; Ballentine, Chris J.</p> <p></p> <p>Noble gas observations from different <span class="hlt">mantle</span> samples have provided some of the key observational data used to develop and support the geochemical "layered" <span class="hlt">mantle</span> model. This model has dominated our conceptual understanding of <span class="hlt">mantle</span> structure and evolution for the last quarter of a century. Refinement in seismic tomography and numerical models of <span class="hlt">mantle</span> convection have clearly shown that geochemical layering, at least at the 670 km phase change in the <span class="hlt">mantle</span>, is no longer tenable. Recent adaptations of the <span class="hlt">mantle</span>-layering model that more successfully reconcile whole-<span class="hlt">mantle</span> convection with the simplest data have two common features: (i) the requirement for the noble gases in the convecting <span class="hlt">mantle</span> to be sourced, or "fluxed", by a deep long-lived volatile-rich <span class="hlt">mantle</span> reservoir; and (ii) the requirement for the deep <span class="hlt">mantle</span> reservoirs to be seismically invisible. The fluxing requirement is derived from the low mid-ocean ridge basalt (MORB)-source <span class="hlt">mantle</span> 3He concentration, in turn calculated from the present day 3He flux from mid-ocean ridges into the oceans (T½ ˜ 1,000 yr) and the ocean crust generation rate (T½ ˜ 108 yr). Because of these very different residence times we consider the 3He concentration constraint to be weak. Furthermore, data show 3He/22Ne ratios derived from different <span class="hlt">mantle</span> reservoirs to be distinct and require additional complexities to be added to any model advocating fluxing of the convecting <span class="hlt">mantle</span> from a volatile-rich <span class="hlt">mantle</span> reservoir. Recent work also shows that the convecting <span class="hlt">mantle</span> 20Ne/22Ne isotopic composition is derived from an implanted meteoritic source and is distinct from at least one plume source system. If Ne isotope heterogeneity between convecting <span class="hlt">mantle</span> and plume source <span class="hlt">mantle</span> is confirmed, this result then excludes all <span class="hlt">mantle</span> fluxing models. While isotopic heterogeneity requires further quantification, it has been shown that higher 3He concentrations in the convecting <span class="hlt">mantle</span>, by a factor of 3.5, remove the need for the noble</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985EOSTr..66..537Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985EOSTr..66..537Z"><span>Continental Basalts and <span class="hlt">Mantle</span> Xenoliths</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zartman, Robert E.</p> <p></p> <p>In this decade of the International Lithosphere Program, much scientific attention is being directed toward the deep continental crust and subadjacent <span class="hlt">mantle</span>. The petrologic, geochemical, and isotopic signatures of basaltic magmas, which transect much of the lithosphere as they ascend from their site of melting, and of contained cognate and accidental xenoliths, which are found along the path of ascent, give us, perhaps, the best clues to composition and structure in the third dimension. Continental Basalts and <span class="hlt">Mantle</span> Xenoliths provides an opportunity to sample the British school of thought on subjects such as differences between oceanic and continental basalts, effects of <span class="hlt">mantle</span> metasomatism, and relationships between events in the subcontinental <span class="hlt">mantle</span> and those in the overlying crust. This volume is recommended by the publisher as being of interest to senior undergraduates and postgraduate researchers; I would extend that readership to all scientists who seek access to a potpourri of recent findings and current ideas in a rapidly evolving field of research.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015DPS....4730813T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015DPS....4730813T"><span>Searching for a <span class="hlt">Differentiated</span> Asteroid Family: A Spectral Survey of the Massalia, Merxia, and Agnia Families</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thomas, Cristina A.; Lim, Lucy; Moskovitz, Nicholas; Trilling, David</p> <p>2015-11-01</p> <p>Asteroid families were formed by catastrophic collisions or large cratering events that caused fragmentation of the parent body and ejection of asteroidal fragments with velocities sufficient to prevent re-accretion. Due to these formation processes, asteroid families should provide us with the opportunity to probe the interiors of the former parent bodies. <span class="hlt">Differentiation</span> of a large initially chondritic parent body is expected to result in an "onion shell" object with an iron-nickel core, a thick olivine-dominated <span class="hlt">mantle</span>, and a thin plagioclase/pyroxene crust. However, most asteroid families tend to show similar spectra (and therefore composition) among the members. Spectroscopic studies have observed a paucity of metal-like materials and olivine-dominated assemblages within the Main Belt asteroid families.The deficit of olivine-rich <span class="hlt">mantle</span> material in the meteorite record and in asteroid observations is known as the "Missing <span class="hlt">Mantle</span>" problem. For years the best explanation has been the "battered to bits" hypothesis: that all <span class="hlt">differentiated</span> parent bodies (aside from Vesta) were disrupted very <span class="hlt">early</span> in the Solar System and the resulting olivine-rich material was collisionally broken down over time until the object diameters fell below our observational limits. In a competing hypothesis, Elkins-Tanton et al. (2013) have suggested that previous work has overestimated the amount of olivine produced by the <span class="hlt">differentiation</span> of a chondritic parent body.We are conducting a visible and near-infrared wavelength spectral survey of asteroids in the Massalia, Merxia, and Agnia S-type Main Belt asteroid families. These families were carefully chosen for the proposed spectroscopic survey because they have compositions most closely associated with a history of thermal metamorphism and because they represent a range of collisional formation scenarios. In addition, the relatively young ages (under 400 Myr) of these families permit testing of the “battering to bits'' timescale. We</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28666956','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28666956"><span>Coordination of cellular <span class="hlt">differentiation</span>, polarity, mitosis and meiosis - New findings from <span class="hlt">early</span> vertebrate oogenesis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Elkouby, Yaniv M; Mullins, Mary C</p> <p>2017-10-15</p> <p>A mechanistic dissection of <span class="hlt">early</span> oocyte <span class="hlt">differentiation</span> in vertebrates is key to advancing our knowledge of germline development, reproductive biology, the regulation of meiosis, and all of their associated disorders. Recent advances in the field include breakthroughs in the identification of germline stem cells in Medaka, in the cellular architecture of the germline cyst in mice, in a mechanistic dissection of chromosomal pairing and bouquet formation in meiosis in mice, in tracing oocyte symmetry breaking to the chromosomal bouquet of meiosis in zebrafish, and in the biology of the Balbiani body, a universal oocyte granule. Many of the major events in <span class="hlt">early</span> oogenesis are universally conserved, and some are co-opted for species-specific needs. The chromosomal events of meiosis are of tremendous consequence to gamete formation and have been extensively studied. New light is now being shed on other aspects of <span class="hlt">early</span> oocyte <span class="hlt">differentiation</span>, which were traditionally considered outside the scope of meiosis, and their coordination with meiotic events. The emerging theme is of meiosis as a common groundwork for coordinating multifaceted processes of oocyte <span class="hlt">differentiation</span>. In an accompanying manuscript we describe methods that allowed for investigations in the zebrafish ovary to contribute to these breakthroughs. Here, we review these advances mostly from the zebrafish and mouse. We discuss oogenesis concepts across established model organisms, and construct an inclusive paradigm for <span class="hlt">early</span> oocyte <span class="hlt">differentiation</span> in vertebrates. Copyright © 2017 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V24A..08V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V24A..08V"><span>An Impaired View of Earth's <span class="hlt">Early</span> History</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vervoort, J. D.; Kemp, A. I.; Bauer, A.; Bowring, S. A.; Fisher, C.</p> <p>2014-12-01</p> <p>The Hf and Nd isotope records of Earth's <span class="hlt">early</span> history are sparse, difficult to interpret, and controversial, much like the few remnants of crust older than 4 Ga. New analytical techniques have been brought to bear on this problem but despite this recent work­-or, perhaps, because of it-the record is no clearer than it was 15 years ago. Several studies, based on highly variable calculated initial isotopic compositions, have argued for highly heterogeneous crust and <span class="hlt">mantle</span> reservoirs in the <span class="hlt">early</span> Earth1,2 and an ultra-depleted Eoarchean <span class="hlt">mantle</span>3. These data come mostly from two sources: Hf-Nd isotope analyses of ultramafic rocks and Hf isotope analyses of zircons by solution or laser ablation. An important question for understanding the chemical evolution of the <span class="hlt">early</span> Earth is: Do these data offer a unique window into the <span class="hlt">early</span> Earth or are they artefacts not representative of crust/<span class="hlt">mantle</span> evolution, giving an impaired view of the Earth's <span class="hlt">early</span> history? In complex samples, measured isotopic compositions can result from open-system behavior in easily altered ultramafic compositions, in multicomponent, polymetamorphic gneisses, or in zircons with multiple generations of growth. Perhaps most importantly, accurate age assignment is often lacking, compromised, or impossible in these rocks, making calculation of initial epsilon Hf and Nd values ambiguous at best. In order to gain insight into crust <span class="hlt">mantle</span> evolution in the <span class="hlt">early</span> Earth we need, above all, a robust and unambiguous isotopic record to work with. This can be achieved by integrating zircon U-Pb and Hf and whole-rock Hf and Nd isotope compositions in relatively undisturbed igneous rocks with well-constrained ages. When this approach is used apparent isotopic heterogeneity decreases and a simpler model for crust-<span class="hlt">mantle</span> evolution in the <span class="hlt">early</span> Earth emerges. Careful screening of geological relationships, petrology, and geochemistry of samples from the <span class="hlt">early</span> Earth should be done before interpreting isotopic data</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRB..121.4895C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRB..121.4895C"><span>Axial-type olivine crystallographic preferred orientations: The effect of strain geometry on <span class="hlt">mantle</span> texture</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chatzaras, Vasileios; Kruckenberg, Seth C.; Cohen, Shaina M.; Medaris, L. Gordon; Withers, Anthony C.; Bagley, Brian</p> <p>2016-07-01</p> <p>The effect of finite strain geometry on crystallographic preferred orientation (CPO) is poorly constrained in the upper <span class="hlt">mantle</span>. Specifically, the relationship between shape preferred orientation (SPO) and CPO in <span class="hlt">mantle</span> rocks remains unclear. We analyzed a suite of 40 spinel peridotite xenoliths from Marie Byrd Land, West Antarctica. X-ray computed tomography allows for quantification of spinel SPO, which ranges from prolate to oblate shape. Electron backscatter diffraction analysis reveals a range of olivine CPO patterns, including A-type, axial-[010], axial-[100], and B-type patterns. Until now, these CPO types were associated with different deformation conditions, deformation mechanisms, or strain magnitudes. Microstructures and deformation mechanism maps suggest that deformation in all studied xenoliths is dominated by dislocation-accommodated grain boundary sliding. For the range of temperatures (780-1200°C), extraction depths (39-72 km), <span class="hlt">differential</span> stresses (2-60 MPa), and water content (up to 500 H/106Si) of the xenolith suite, variations in olivine CPO do not correlate with changes in deformation conditions. Here we establish for the first time in naturally deformed <span class="hlt">mantle</span> rocks that finite strain geometry controls the development of axial-type olivine CPOs; axial-[010] and axial-[100] CPOs form in relation to oblate and prolate fabric ellipsoids, respectively. Girdling of olivine crystal axes results from intracrystalline slip with activation of multiple slip systems and grain boundary sliding. Our results demonstrate that <span class="hlt">mantle</span> deformation may deviate from simple shear. Olivine texture in field studies and seismic anisotropy in geophysical investigations can provide critical constraints for the 3-D strain in the upper <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T33G..07P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T33G..07P"><span>Isotopic evidence for a large-scale plume-derived <span class="hlt">mantle</span> domain between the Indian and Pacific <span class="hlt">mantles</span> beneath the Southern Ocean.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, S. H.; Langmuir, C. H.; Scott, S. R.; Sims, K. W. W.; Lin, J.; Kim, S. S.; Blichert-Toft, J.; Choi, H.; Yang, Y. S.; Michael, P. J.</p> <p>2017-12-01</p> <p>Earth's upper <span class="hlt">mantle</span> is characterized by Indian- and Pacific-type domains with distinctive isotope characteristics. The boundary between these two <span class="hlt">mantle</span> regions has been hypothesized to be located at the Australian-Antarctic-Discordance (AAD), where regions west and east of the AAD are Indian- and Pacific-type, respectively. It was further posited that the Pacific <span class="hlt">mantle</span> feeds into the Indian <span class="hlt">mantle</span> as the boundary is moving westward. These scenarios have important implications for the dynamics of <span class="hlt">mantle</span> convection in the area. In the present model, regions east of the AAD are assumed to be entirely Pacific-type <span class="hlt">mantle</span>, but our recent recovery of basalts from a 2,000-km sampling gap along the Australian-Antarctic Ridge (AAR), located east of the AAD on the Pacific side, challenges this picture. Here we show that the Hf, Nd, Pb, and Sr isotopic compositions of AAR MORB are distinct from those of Pacific and Indian MORB. Rather, the AAR lavas show mixing relationships with volcanoes from the Hikurangi seamounts, the Balleney and Scott Islands, the West Antarctic Rift System, New Zealand, and east Australia. According to tectonic reconstruction models, these volcanoes are related to super-plume activity that caused Gondwana to break up at 90 Ma. These results imply that a large-scale plume-derived <span class="hlt">mantle</span> domain exists between the Indian and Pacific <span class="hlt">mantle</span> domains, and that <span class="hlt">mantle</span> dynamics along the AAD should be reinterpreted in light of interaction with a super-plume.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMDI13A1677L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMDI13A1677L"><span>Upper <span class="hlt">Mantle</span> Anisotropy Under Fast Spreading Mid-ocean Ridges: 2-D Whole <span class="hlt">Mantle</span> Convection Model With Subduction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, C.; Zhou, Y.; King, S. D.</p> <p>2008-12-01</p> <p>Analyses of seismic anisotropy caused by spatial alignments of anisotropic minerals (e.g., olivine) have been widely used to infer <span class="hlt">mantle</span> flow directions in the upper <span class="hlt">mantle</span>. Deep seismic anisotropy beneath fast spreading mid-ocean ridges (e.g., East Pacific Rise) has been recently observed at depths of 200-300 km and even down to the transition zone, with polarization changes in radial anisotropy from VSH < VSV (shallow) to VSH < VSV (deep). We investigate the origin of the observed deep seismic anisotropy and polarization changes beneath the EPR in 2-D Cartesian numerical models using both kinematically (prescribed velocity) and dynamically (negative buoyancy) driven ridge spreading. Because subduction is thought to be an important controlling factor in the style of ridge spreading and <span class="hlt">mantle</span> convection, we consider a subduction zone developing at the prescribed weak zone. A whole <span class="hlt">mantle</span> domain expressed by a one by four box (2890 by 11560 km) is used to minimize the boundary effects on the subducting slab. For the upper <span class="hlt">mantle</span> rheology, we consider composite viscosity of diffusion and dislocation creep for dry olivine to evaluate the effects of lateral variation of <span class="hlt">mantle</span> viscosity and the rheological changes from dislocation to diffusion creep under the mid-ocean ridge. For the lower <span class="hlt">mantle</span> rheology, we use diffusion creep for dry olivine by increasing grain size to match relevant lower <span class="hlt">mantle</span> viscosity. We also consider the 660 km phase transition with density and viscosity jump as well as Clapeyron slope. Anisotropy is evaluated using finite-strain ellipses based on the assumption that a-axes of olivine crystals are parallel to the major axes of the finite-strain ellipses. Our preliminary results show 1) in general, the development of VSH < VSV anisotropy is confined only in a narrow region under the ridge axis at depths of 200- 300 km; 2) strong VSH > VSV anisotropy can be found in the 'asthenosphere' beneath the entire spreading oceanic lithosphere; and 3</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880020821&hterms=Hofmann&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DHofmann','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880020821&hterms=Hofmann&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DHofmann"><span>Growth of continental crust: Clues from Nd isotopes and Nb-Th relationships in <span class="hlt">mantle</span>-derived magmas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Arndt, N. T.; Chauvel, C.; Jochum, K.-P.; Gruau, G.; Hofmann, A. W.</p> <p>1988-01-01</p> <p>Isotope and trace element geochemistry of Precambrian <span class="hlt">mantle</span> derived rocks and implications for the formation of the continental crust is discussed. Epsilon Nd values of Archean komatiites are variable, but range up to at least +5, suggesting that the Archean <span class="hlt">mantle</span> was heterogeneous and, in part, very depleted as far back as 3.4 to 3.5 Ga. This may be taken as evidence for separation of continental crust very <span class="hlt">early</span> in Earth history. If these komatiite sources were allowed to evolve in a closed system, they would produce modern day reservoirs with much higher epsilon Nd values than is observed. This implies recycling of some sort of enriched material, perhaps subducted sediments, although other possibilities exist. Archean volcanics show lower Nb/Th than modern volcanics, suggesting a more primitive <span class="hlt">mantle</span> source than that observed nowadays. However, Cretaceous komatiites from Gorgona island have similar Nb/Th to Archean volcanics, indicating either the Archean <span class="hlt">mantle</span> source was indeed more primitive, or Archean magmas were derived from a deep ocean island source like that proposed for Gorgona.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988gcc..work...38A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988gcc..work...38A"><span>Growth of continental crust: Clues from Nd isotopes and Nb-Th relationships in <span class="hlt">mantle</span>-derived magmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arndt, N. T.; Chauvel, C.; Jochum, K.-P.; Gruau, G.; Hofmann, A. W.</p> <p></p> <p>Isotope and trace element geochemistry of Precambrian <span class="hlt">mantle</span> derived rocks and implications for the formation of the continental crust is discussed. Epsilon Nd values of Archean komatiites are variable, but range up to at least +5, suggesting that the Archean <span class="hlt">mantle</span> was heterogeneous and, in part, very depleted as far back as 3.4 to 3.5 Ga. This may be taken as evidence for separation of continental crust very <span class="hlt">early</span> in Earth history. If these komatiite sources were allowed to evolve in a closed system, they would produce modern day reservoirs with much higher epsilon Nd values than is observed. This implies recycling of some sort of enriched material, perhaps subducted sediments, although other possibilities exist. Archean volcanics show lower Nb/Th than modern volcanics, suggesting a more primitive <span class="hlt">mantle</span> source than that observed nowadays. However, Cretaceous komatiites from Gorgona island have similar Nb/Th to Archean volcanics, indicating either the Archean <span class="hlt">mantle</span> source was indeed more primitive, or Archean magmas were derived from a deep ocean island source like that proposed for Gorgona.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2853553','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2853553"><span>Magnetic resonance imaging with pathological correlation in a case of <span class="hlt">mantle</span> cell lymphoma of the parotid gland: a case report</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2010-01-01</p> <p>Introduction <span class="hlt">Mantle</span> cell lymphoma is a rare non-Hodgkin's lymphoma. It is a subtype of B-cell lymphoma with frequent involvement of the bone marrow and the gastrointestinal tract. Isolated parotid gland involvement seldom occurs. Here we report an unusual case of isolated infiltration of the parotid gland by <span class="hlt">mantle</span> cell lymphoma. The aim of our study is to correlate magnetic resonance imaging findings with the histological features of the disease. To the best of our knowledge, no similar radiological findings of <span class="hlt">mantle</span> cell lymphoma have been published before. Case presentation A 72-year-old Caucasian woman presented with a painful left parotid enlargement. She was diagnosed with <span class="hlt">mantle</span> cell lymphoma involving the left submandibular gland seven years prior to presentation. Her whole body CT scan showed the absence of pathologically enlarged lymph nodes. However, a magnetic resonance imaging showed enlargement of her left parotid gland and an abnormal parenchyma with mixed-type solid and cystic lesions. A biopsy of her left parotid gland and subsequent histological examination confirmed a <span class="hlt">mantle</span> cell lymphoma (common variant) relapse. Conclusion Although rare, the involvement of parotid gland with <span class="hlt">mantle</span> cell lymphoma must be considered in the <span class="hlt">differential</span> diagnosis of parotid tumors. PMID:20350332</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Litho.296..623S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Litho.296..623S"><span><span class="hlt">Mantle</span> wedge exhumation beneath the Dora-Maira (U)HP dome unravelled by local earthquake tomography (Western Alps)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Solarino, Stefano; Malusà, Marco G.; Eva, Elena; Guillot, Stéphane; Paul, Anne; Schwartz, Stéphane; Zhao, Liang; Aubert, Coralie; Dumont, Thierry; Pondrelli, Silvia; Salimbeni, Simone; Wang, Qingchen; Xu, Xiaobing; Zheng, Tianyu; Zhu, Rixiang</p> <p>2018-01-01</p> <p>In continental subduction zones, the behaviour of the <span class="hlt">mantle</span> wedge during exhumation of (ultra)high-pressure [(U)HP] rocks provides a key to distinguish among competing exhumation mechanisms. However, in spite of the relevant implications for understanding orogenic evolution, a high-resolution image of the <span class="hlt">mantle</span> wedge beneath the Western Alps is still lacking. In order to fill this gap, we perform a detailed analysis of the velocity structure of the Alpine belt beneath the Dora-Maira (U)HP dome, based on local earthquake tomography independently validated by receiver function analysis. Our results point to a composite structure of the <span class="hlt">mantle</span> wedge above the subducted European lithosphere. We found that the Dora-Maira (U)HP dome lays directly above partly serpentinized peridotites (Vp 7.5 km/s; Vp/Vs = 1.70-1.72), documented from 10 km depth down to the top of the eclogitized lower crust of the European plate. These serpentinized peridotites, possibly formed by fluid release from the subducting European slab to the Alpine <span class="hlt">mantle</span> wedge, are juxtaposed against dry <span class="hlt">mantle</span> peridotites of the Adriatic upper plate along an active fault rooted in the lithospheric <span class="hlt">mantle</span>. We propose that serpentinized <span class="hlt">mantle</span>-wedge peridotites were exhumed at shallow crustal levels during late Eocene transtensional tectonics, also triggering the rapid exhumation of (U)HP rocks, and were subsequently indented under the Alpine metamorphic wedge in the <span class="hlt">early</span> Oligocene. Our findings suggest that <span class="hlt">mantle</span>-wedge exhumation may represent a major feature of the deep structure of exhumed continental subduction zones. The deep orogenic levels here imaged by seismic tomography may be exposed today in older (U)HP belts, where <span class="hlt">mantle</span>-wedge serpentinites are commonly associated with coesite-bearing continental metamorphic rocks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1817009S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1817009S"><span>The He isotope composition of the earliest picrites erupted by the Ethiopia plume, implications for <span class="hlt">mantle</span> plume source</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stuart, Finlay; Rogers, Nick; Davies, Marc</p> <p>2016-04-01</p> <p>The earliest basalts erupted by <span class="hlt">mantle</span> plumes are Mg-rich, and typically derived from <span class="hlt">mantle</span> with higher potential temperature than those derived from the convecting upper <span class="hlt">mantle</span> at mid-ocean ridges and ocean islands. The chemistry and isotopic composition of picrites from CFB provide constraints on the composition of deep Earth and thus the origin and <span class="hlt">differentiation</span> history. We report new He-Sr-Nd-Pb isotopic composition of the picrites from the Ethiopian flood basalt province from the Dilb (Chinese Road) section. They are characterized by high Fe and Ti contents for MgO = 10-22 wt. % implying that the parent magma was derived from a high temperature low melt fraction, most probably from the Afar plume head. The picrite 3He/4He does not exceed 21 Ra, and there is a negative correlation with MgO, the highest 3He/4He corresponding to MgO = 15.4 wt. %. Age-corrected 87Sr/86Sr (0.70392-0.70408) and 143Nd/144Nd (0.512912-0.512987) display little variation and are distinct from MORB and OIB. Age-corrected Pb isotopes display a significant range (e.g. 206Pb/204Pb = 18.70-19.04) and plot above the NHRL. These values contrast with estimates of the modern Afar <span class="hlt">mantle</span> plume which has lower 3He/4He and Sr, Nd and Pb isotope ratios that are more comparable with typical OIB. These results imply either interaction between melts derived from the Afar <span class="hlt">mantle</span> plume and a lithospheric component, or that the original Afar <span class="hlt">mantle</span> plume had a rather unique radiogenic isotope composition. Regardless of the details of the origins of this unusual signal, our observations place a minimum 3He/4He value of 21 Ra for the Afar <span class="hlt">mantle</span> plume, significantly greater than the present day value of 16 Ra, implying a significant reduction over 30 Myr. In addition the Afar source was less degassed than convecting <span class="hlt">mantle</span> but more degassed than <span class="hlt">mantle</span> sampled by the proto-Iceland plume (3He/4He ~50 Ra). This suggests that the largest <span class="hlt">mantle</span> plumes are not sourced in a single deep <span class="hlt">mantle</span> domain with a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T33B0703M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T33B0703M"><span>Hydrous melt-rock reaction in the shallow <span class="hlt">mantle</span> wedge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mitchell, A.; Grove, T. L.</p> <p>2017-12-01</p> <p>In subduction zone magmatism, hotter, deeper hydrous <span class="hlt">mantle</span> melts rise and interact with the shallower, cooler depleted <span class="hlt">mantle</span> in the uppermost part of the <span class="hlt">mantle</span> wedge. Here, we experimentally investigate these hydrous reactions using three different ratios of a 1.6 GPa <span class="hlt">mantle</span> melt and an overlying 1.2 GPa harzburgite from 1060 to 1260 °C. At low ratios of melt/<span class="hlt">mantle</span> (20:80 and 5:95), the crystallizing assemblages are dunites, harzburgites, and lherzolites (as a function of temperature). When the ratio of deeper melt to overlying <span class="hlt">mantle</span> is 70:30, the crystallizing assemblage is a wehrlite. This shows that wehrlites, which are observed in ophiolites and <span class="hlt">mantle</span> xenoliths, can be formed by large amounts of deeper melt fluxing though the <span class="hlt">mantle</span> wedge during ascent. In all cases, orthopyroxene dissolves in the melt, and olivine crystallizes along with pyroxenes and spinel. The amount of reaction between deeper melts and overlying <span class="hlt">mantle</span>, simulated here by the three starting compositions, imposes a strong influence on final melt compositions, particularly in terms of depletion. At the lowest melt/<span class="hlt">mantle</span> ratios, the resulting melt is an extremely depleted Al-poor, high-Si andesite. As the fraction of melt to <span class="hlt">mantle</span> increases, final melts resemble primitive basaltic andesites found in arcs globally. Wall rock temperature is a key variable; over a span of <80 °C, reaction with deeper melt creates the entire range of <span class="hlt">mantle</span> lithologies from a depleted dunite to a harzburgite to a refertilized lherzolite. Together, the experimental phase equilibria, melt compositions, and calculated reaction coefficients provide a framework for understanding how melt-wall rock reaction occurs in the natural system during melt ascent in the <span class="hlt">mantle</span> wedge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950043363&hterms=homogenization&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhomogenization','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950043363&hterms=homogenization&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhomogenization"><span>Thermal and chemical convection in planetary <span class="hlt">mantles</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dupeyrat, L.; Sotin, C.; Parmentier, E. M.</p> <p>1995-01-01</p> <p>Melting of the upper <span class="hlt">mantle</span> and extraction of melt result in the formation of a less dense depleted <span class="hlt">mantle</span>. This paper describes series of two-dimensional models that investigate the effects of chemical buoyancy induced by these density variations. A tracer particles method has been set up to follow as closely as possible the chemical state of the <span class="hlt">mantle</span> and to model the chemical buoyant force at each grid point. Each series of models provides the evolution with time of magma production, crustal thickness, surface heat flux, and thermal and chemical state of the <span class="hlt">mantle</span>. First, models that do not take into account the displacement of plates at the surface of Earth demonstrate that chemical buoyancy has an important effect on the geometry of convection. Then models include horizontal motion of plates 5000 km wide. Recycling of crust is taken into account. For a sufficiently high plate velocity which depends on the thermal Rayleigh number, the cell's size is strongly coupled with the plate's size. Plate motion forces chemically buoyant material to sink into the <span class="hlt">mantle</span>. Then the positive chemical buoyancy yields upwelling as depleted <span class="hlt">mantle</span> reaches the interface between the upper and the lower <span class="hlt">mantle</span>. This process is very efficient in mixing the depleted and undepleted <span class="hlt">mantle</span> at the scale of the grid spacing since these zones of upwelling disrupt the large convective flow. At low spreading rates, zones of upwelling develop quickly, melting occurs, and the model predicts intraplate volcanism by melting of subducted crust. At fast spreading rates, depleted <span class="hlt">mantle</span> also favors the formation of these zones of upwelling, but they are not strong enough to yield partial melting. Their rapid displacement toward the ridge contributes to faster large-scale homogenization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI11B..05W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI11B..05W"><span>Substructures of the <span class="hlt">mantle</span> transition-zone discontinuities and compositional heterogeneities in the mid-<span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wei, S. S.; Shearer, P. M.</p> <p>2017-12-01</p> <p>The <span class="hlt">mantle</span> transition-zone discontinuities are usually attributed to isochemical phase transformations of olivine and its high-pressure polymorphs. However, recent seismic observations have shown complexities in these discontinuities that cannot be explained by conventional models of thermal variations. Here we analyse SS precursor stacking results to investigate global <span class="hlt">mantle</span> transition-zone properties. The precursor waveforms provide information on the seismic velocity and density profiles across and near the major <span class="hlt">mantle</span> discontinuities. A sporadic low-velocity layer immediately above the 410-km discontinuity is observed worldwide, including East Asia, western North America, eastern South America, and 33-50% of the resolved Pacific Ocean. The 520-km discontinuity exhibits significant variations in its sharpness and depth, and occasionally appears to be split. Structures underlying the 660-km discontinuity show even larger complexities: a sub-discontinuity at 700-800 km depth is detected in some regions, of which some require a positive velocity gradient whereas others have a negative gradient. All of these lateral variations show no geographical correlation with discontinuity topography or tomographic models of seismic velocity, suggesting that they are not caused by regional thermal anomalies. Alternatively, our observations can be explained by compositional heterogeneities in the mid-<span class="hlt">mantle</span>, including major minerals and volatile content, which may result in additional phase transformations and partial melting. These compositional heterogeneities should be taken into account in future geodynamic models of <span class="hlt">mantle</span> convection and the deep water cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR24A..07M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR24A..07M"><span>The Stirring of Oceanic Crust in the <span class="hlt">Mantle</span>: How it Changes with Time?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McNamara, A. K.; Li, M.</p> <p>2017-12-01</p> <p>The Large Low Shear Velocity Provinces (LLSVPs) beneath Africa and the Pacific are considerably-sized seismic anomalies in the lower <span class="hlt">mantle</span> that likely play a key role in global <span class="hlt">mantle</span> convection. Unfortunately, we do not know what they are, and hypotheses include thermal megaplumes, plume clusters, primordial piles, thermochemical superplumes, and large accumulations of ancient, subducted oceanic crust. Discovering which of these are the cause of LLSVPs will provide fundamental understanding toward the nature of global-scale <span class="hlt">mantle</span> convection. Here, we focus on two of the possibilities: primordial piles and accumulations of subducted oceanic crust. In previous work, it seemed clear that each provide a distinguishably-different morphology: primordial piles are clearly defined entities with sharp edges and tops, whereas accumulations of oceanic crust appear quite messy and have fuzzy, advective boundaries, particularly at their tops. Therefore, it was thought that by performing seismic studies that define the tops of LLSVPs, we could distinguish between these possibilities. Here, we ask the following question: Can piles formed by ancient oceanic crust eventually "clean themselves up" and evolve into structures that more-resemble what we think primordial piles should look like at the present day? Here, we present geodynamics work that demonstrates that this is indeed the case. The driving mechanism is a thinning of oceanic crust through time (as the <span class="hlt">mantle</span> cools, there is less melt at ridges, and therefore, crust is thinner). We find that in the <span class="hlt">early</span>, hotter Earth, if crust is on the order of 20-30 km thick, it will accumulate into messy piles at the base of the <span class="hlt">mantle</span>. As crust thins beyond a critical thinness, it will stop accumulating and be stirred into the background <span class="hlt">mantle</span> instead. Once crust stops accumulating in the lower <span class="hlt">mantle</span>, the pre-existing messy piles begin to sharpen into well-defined piles with sharp edges and tops. Furthermore, we find that this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.2121A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.2121A"><span>The Universal Cpx Jd-Di barometer for <span class="hlt">mantle</span> peridotite eclogite and pyroxenites and it using for the <span class="hlt">mantle</span> petrology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ashchepkov, Igor</p> <p>2015-04-01</p> <p> trace he boundary between the lower upper part of subcontinental lithospheric <span class="hlt">mantle</span> (SCLM) at 3 -4 GPa marking pyroxenite eclogites layer. Ca- rich eclogites and especially grospydites in SCLM beneath Precambrian kimberlites occurs near pyroxenite layer but in younger <span class="hlt">mantle</span> sections they became common in the lower parts marking presence of the subducted sediments. The Mg Cr- less group eclogites commonly diamondiferous and referring to the ancient island arc complexes are also common in the middle part of <span class="hlt">mantle</span> sections and near 5-6 GPa. The group is often dominated in the young kimberlites and sometimes is highly diamondiferous. Commonly P-Fe# for eclogites in the lower SCLM part show rising Fe# with decreasing pressures which very of then reflect the <span class="hlt">differentiation</span> of the magmatic systems commonly rather significant. Commonly the Fe#-values for the eclogites show that they can't be simple subucted oceanic basalts but material remelted not only during the low angle "hot"subduction but also under the influence of the kimberlite melts including protokimberlite magmas. The Mg - rich and Fe rich pyroxenites also show the extending in pressures trends which suggest the anatexic melting under the influence of volatiles or under the plum magma hybridization. RBRF grants 05-05-64718, 03-05-64146; 11 -05-00060a; 11-05-91060-PICS. Projects 77-2, 65-03, 02-05 IGM SD RAS and ALROSA Stock Company.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Litho.264..277A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Litho.264..277A"><span>Formation and modification of chromitites in the <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arai, Shoji; Miura, Makoto</p> <p>2016-11-01</p> <p>Podiform chromitites have long supplied us with unrivaled information on various <span class="hlt">mantle</span> processes, including the peridotite-magma reaction, deep-seated magmatic evolution, and <span class="hlt">mantle</span> dynamics. The recent discovery of ultrahigh-pressure (UHP) chromitites not only sheds light on a different aspect of podiform chromitites, but also changes our understanding of the whole picture of podiform chromitite genesis. In addition, new evidence was recently presented for hydrothermal modification/formation chromite/chromitite in the <span class="hlt">mantle</span>, which is a classical but innovative issue. In this context, we present here an urgently needed comprehensive review of podiform chromitites in the upper <span class="hlt">mantle</span>. Wall-rock control on podiform chromitite genesis demonstrates that the peridotite-magma reaction at the upper <span class="hlt">mantle</span> condition is an indispensable process. We may need a large system in the <span class="hlt">mantle</span>, far larger than the size of outcrops or mining areas, to fulfill the Cr budget requirement for podiform chromitite genesis. The peridotite-magma reaction over a large area may form a melt enriched with Na and other incompatible elements, which mixes with a less evolved magma supplied from the depth to create chromite-oversaturated magma. The incompatible-element-rich magma trapped by the chromite mainly precipitates pargasite and aspidolite (Na analogue of phlogopite), which are stable under upper <span class="hlt">mantle</span> conditions. Moderately depleted harzburgites, which contain chromite with a moderate Cr# (0.4-0.6) and a small amount of clinopyroxene, are the best reactants for the chromitite-forming reaction, and are the best hosts for podiform chromitites. Arc-type chromitites are dominant in ophiolites, but some are of the mid-ocean ridge type; chromitites may be common beneath the ocean floor, although it has not yet been explored for chromitite. The low-pressure (upper <span class="hlt">mantle</span>) igneous chromitites were conveyed through <span class="hlt">mantle</span> convection or subduction down to the <span class="hlt">mantle</span> transition zone to form</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12460477','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12460477"><span>Chemical and seismological constraints on <span class="hlt">mantle</span> heterogeneity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Helffrich, George</p> <p>2002-11-15</p> <p>Recent seismological studies that use scattered waves to detect heterogeneities in the <span class="hlt">mantle</span> reveal the presence of a small, distributed elastic heterogeneity in the lower <span class="hlt">mantle</span> which does not appear to be thermal in nature. The characteristic size of these heterogeneities appears to be ca. 8 km, suggesting that they represent subducted recycled oceanic crust. With this stimulus, old ideas that the <span class="hlt">mantle</span> is heterogeneous in structure, rather than stratified, are reinterpreted and a simple, end-member model for the heterogeneity structure is proposed. The volumetrically largest components in the model are recycled oceanic crust, which contains the heat-producing elements, and <span class="hlt">mantle</span> depleted of these and other incompatible trace elements. About 10% of the <span class="hlt">mantle</span>'s mass is made up of recycled oceanic crust, which is associated with the observed small-scale seismic heterogeneity. The way this heterogeneity is distributed is in convectively stretched and thinned bodies ranging downwards in size from 8 km. With the present techniques to detect small bodies through scattering, only ca. 55% of the <span class="hlt">mantle</span>'s small-scale heterogeneities are detectable seismically.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.489...84D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.489...84D"><span>Carbonate stability in the reduced lower <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dorfman, Susannah M.; Badro, James; Nabiei, Farhang; Prakapenka, Vitali B.; Cantoni, Marco; Gillet, Philippe</p> <p>2018-05-01</p> <p>Carbonate minerals are important hosts of carbon in the crust and <span class="hlt">mantle</span> with a key role in the transport and storage of carbon in Earth's deep interior over the history of the planet. Whether subducted carbonates efficiently melt and break down due to interactions with reduced phases or are preserved to great depths and ultimately reach the core-<span class="hlt">mantle</span> boundary remains controversial. In this study, experiments in the laser-heated diamond anvil cell (LHDAC) on layered samples of dolomite (Mg, Ca)CO3 and iron at pressure and temperature conditions reaching those of the deep lower <span class="hlt">mantle</span> show that carbon-iron redox interactions destabilize the MgCO3 component, producing a mixture of diamond, Fe7C3, and (Mg, Fe)O. However, CaCO3 is preserved, supporting its relative stability in carbonate-rich lithologies under reducing lower <span class="hlt">mantle</span> conditions. These results constrain the thermodynamic stability of redox-driven breakdown of carbonates and demonstrate progress towards multiphase <span class="hlt">mantle</span> petrology in the LHDAC at conditions of the lowermost <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1426861-carbonate-stability-reduced-lower-mantle','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1426861-carbonate-stability-reduced-lower-mantle"><span>Carbonate stability in the reduced lower <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Dorfman, Susannah M.; Badro, James; Nabiei, Farhang; ...</p> <p>2018-05-01</p> <p>Carbonate minerals are important hosts of carbon in the crust and <span class="hlt">mantle</span> with a key role in the transport and storage of carbon in Earth’s deep interior over the history of the planet. Whether subducted carbonates efficiently melt and break down due to interactions with reduced phases or are preserved to great depths and ultimately reach the core-<span class="hlt">mantle</span> boundary remains controversial. In this study, experiments in the laser-heated diamond anvil cell (LHDAC) on layered samples of dolomite (Mg,Ca)CO3 and iron at pressure and temperature conditions reaching those of the deep lower <span class="hlt">mantle</span> show that carbon-iron redox interactions destabilize the MgCO3more » component, producing a mixture of diamond, Fe7C3, and (Mg,Fe)O. However, CaCO3 is preserved, supporting its relative stability in carbonate-rich lithologies under reducing lower <span class="hlt">mantle</span> conditions. These results constrain the thermodynamic stability of redox-driven breakdown of carbonates and demonstrate progress towards multiphase <span class="hlt">mantle</span> petrology in the LHDAC at conditions of the lowermost <span class="hlt">mantle</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29898964','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29898964"><span><span class="hlt">Early</span> Generated B-1-Derived B Cells Have the Capacity To Progress To Become <span class="hlt">Mantle</span> Cell Lymphoma-like Neoplasia in Aged Mice.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hayakawa, Kyoko; Formica, Anthony M; Nakao, Yuka; Ichikawa, Daiju; Shinton, Susan A; Brill-Dashoff, Joni; Smith, Mitchell R; Morse, Herbert C; Hardy, Richard R</p> <p>2018-06-13</p> <p>In mice, fetal/neonatal B-1 cell development generates murine CD5 + B cells (B1a) with autoreactivity. We analyzed B1a cells at the neonatal stage in a V H 11/D/J H knock-in mouse line (V H 11t) that generates an autoreactive antiphosphatidylcholine BCR. Our study revealed that antiphosphatidylcholine B1a cells develop in liver, mature in spleen, and distribute in intestine/colon, mesenteric lymph node (mLN), and body cavity as the outcome of B-1 cell development before B-2 cell development. Throughout life, self-renewing B-1 B1a cells circulate through intestine, mesenteric vessel, and blood. The body cavity-deposited B1a cells also remigrate. In old age, some B1a cells proceed to monoclonal B cell lymphocytosis. When neonatal B-1 B1a cells express an antithymocyte/Thy-1 autoreactivity (ATA) BCR transgene in the C.B17 mouse background, ATA B cells increase in PBL and strongly develop lymphomas in aging mice that feature splenomegaly and mLN hyperplasia with heightened expression of CD11b, IL-10, and activated Stat3. At the adult stage, ATA B cells were normally present in the <span class="hlt">mantle</span> zone area, including in intestine. Furthermore, frequent association with mLN hyperplasia suggests the influence by intestinal microenvironment on lymphoma development. When cyclin D1 was overexpressed by the Eμ-cyclin D1 transgene, ATA B cells progressed to further diffused lymphoma in aged mice, including in various lymph nodes with accumulation of IgM hi IgD lo CD5 + CD23 - CD43 + cells, resembling aggressive human <span class="hlt">mantle</span> cell lymphoma. Thus, our findings reveal that <span class="hlt">early</span> generated B cells, as an outcome of B-1 cell development, can progress to become lymphocytosis, lymphoma, and <span class="hlt">mantle</span> cell lymphoma-like neoplasia in aged mice. Copyright © 2018 by The American Association of Immunologists, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFMDI23A1661H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFMDI23A1661H"><span>Geographic boundary of the “Pacific Anomaly” near the Earth’s core-<span class="hlt">mantle</span> boundary</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Y.; Wen, L.</p> <p>2009-12-01</p> <p>Seismic tomography have revealed a broad, seismically low velocity anomaly in the Earth’s lower <span class="hlt">mantle</span> beneath the Pacific (we term it the “Pacific Anomaly”), surrounded by the circum-Pacific high velocity zone. Here, we determine geographical boundary and average shear velocity structure of the Pacific Anomaly near the core-<span class="hlt">mantle</span> boundary based on travel time analysis of ScSH-SH and ScS2-SS phases. We further constrain the detailed structure of the transition from the base of the Pacific Anomaly to the northern high velocity zone along two perpendicular cross sections on the basis of forward waveform modeling of the seismic data. Two cross-sections include one great arc across the Anomaly from New Zealand to Alaska and another from Solomon Islands to North America. Our seismic data are collected from those recorded in the China National Digital Seismographic Network, and many permanent and temporal arrays from the Incorporated Research Institutions for Seismology. The observed ScS-SH and ScS2-SS <span class="hlt">differential</span> travel time residuals allow the entire geographic boundary of the anomaly to be clearly defined. The seismic data suggest that the average shear velocity reduction inside the anomaly reaches -5% in the lowermost 300 km of the <span class="hlt">mantle</span>. Waveform analysis of the seismic data sampling the edge of the anomaly further validates the model of the boundary previously deduced by <span class="hlt">differential</span>-travel-time-residual data, and suggests that the northern boundary is characterized by a shear velocity model with the low-velocity region accompanied by a high velocity structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoJI.210..774D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoJI.210..774D"><span>Lowermost <span class="hlt">mantle</span> anisotropy near the eastern edge of the Pacific LLSVP: constraints from SKS-SKKS splitting intensity measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Deng, Jie; Long, Maureen D.; Creasy, Neala; Wagner, Lara; Beck, Susan; Zandt, George; Tavera, Hernando; Minaya, Estela</p> <p>2017-08-01</p> <p>Seismic anisotropy has been documented in many portions of the lowermost <span class="hlt">mantle</span>, with particularly strong anisotropy thought to be present along the edges of large low shear velocity provinces (LLSVPs). The region surrounding the Pacific LLSVP, however, has not yet been studied extensively in terms of its anisotropic structure. In this study, we use seismic data from southern Peru, northern Bolivia and Easter Island to probe lowermost <span class="hlt">mantle</span> anisotropy beneath the eastern Pacific Ocean, mostly relying on data from the Peru Lithosphere and Slab Experiment and Central Andean Uplift and Geodynamics of High Topography experiments. <span class="hlt">Differential</span> shear wave splitting measurements from phases that have similar ray paths in the upper <span class="hlt">mantle</span> but different ray paths in the lowermost <span class="hlt">mantle</span>, such as SKS and SKKS, are used to constrain anisotropy in D″. We measured splitting for 215 same station-event SKS-SKKS pairs that sample the eastern Pacific LLSVP at the base of the <span class="hlt">mantle</span>. We used measurements of splitting intensity(SI), a measure of the amount of energy on the transverse component, to objectively and quantitatively analyse any discrepancies between SKS and SKKS phases. While the overall splitting signal is dominated by the upper-<span class="hlt">mantle</span> anisotropy, a minority of SKS-SKKS pairs (∼10 per cent) exhibit strongly discrepant splitting between the phases (i.e. the waveforms require a difference in SI of at least 0.4), indicating a likely contribution from lowermost <span class="hlt">mantle</span> anisotropy. In order to enhance lower <span class="hlt">mantle</span> signals, we also stacked waveforms within individual subregions and applied a waveform differencing technique to isolate the signal from the lowermost <span class="hlt">mantle</span>. Our stacking procedure yields evidence for substantial splitting due to lowermost <span class="hlt">mantle</span> anisotropy only for a specific region that likely straddles the edge of Pacific LLSVP. Our observations are consistent with the localization of deformation and anisotropy near the eastern boundary of the Pacific LLSVP</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Geote..51..535T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Geote..51..535T"><span>Sublithospheric flows in the <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Trifonov, V. G.; Sokolov, S. Yu.</p> <p>2017-11-01</p> <p>The estimated rates of upper <span class="hlt">mantle</span> sublithospheric flows in the Hawaii-Emperor Range and Ethiopia-Arabia-Caucasus systems are reported. In the Hawaii-Emperor Range system, calculation is based on motion of the asthenospheric flow and the plate moved by it over the branch of the Central Pacific plume. The travel rate has been determined based on the position of variably aged volcanoes (up to 76 Ma) with respect to the active Kilauea Volcano. As for the Ethiopia-Arabia-Caucasus system, the age of volcanic eruptions (55-2.8 Ma) has been used to estimate the asthenospheric flow from the Ethiopian-Afar superplume in the northern bearing lines. Both systems are characterized by variations in a rate of the upper <span class="hlt">mantle</span> flows in different epochs from 4 to 12 cm/yr, about 8 cm/yr on average. Analysis of the global seismic tomographic data has made it possible to reveal rock volumes with higher seismic wave velocities under ancient cratons; rocks reach a depth of more than 2000 km and are interpreted as detached fragments of the thickened continental lithosphere. Such volumes on both sides of the Atlantic Ocean were submerged at an average velocity of 0.9-1.0 cm/yr along with its opening. The estimated rates of the <span class="hlt">mantle</span> flows clarify the deformation properties of the <span class="hlt">mantle</span> and regulate the numerical models of <span class="hlt">mantle</span> convection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR23A2663F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR23A2663F"><span>Abnormal Elasticity of Single-Crystal Magnesiosiderite across the Spin Transition in Earth's Lower <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fu, S.; Yang, J.; Lin, J. F.</p> <p>2016-12-01</p> <p>Carbon can be transported into deep Earth's interior via subduction of carbonated oceanic crust, hosted as Mg-Fe bearing carbonates. The existence of stable carbonate can significantly affect our understanding on geochemical and geophysical properties of the planet. <span class="hlt">Early</span> studies have shown that iron spin-pairing transition could occur in the iron-enriched carbonates, generally called magnesiosiderite, under lower <span class="hlt">mantle</span> conditions. The pressure-induced spin state change is accompanied by a sudden volume collaps. However, the effects of the spin-pairing transition on single-crystal elasticity of magnesiosiderite under high pressure conditions are still unclear. Understanding the elasticity of single-crystal magnesiosiderite at relevant lower <span class="hlt">mantle</span> conditions plays an important role in better understanding the seismic signatures in the carbon-enriched region, and to constrain carbon storage and recycling in the <span class="hlt">mantle</span>. In order to solve all individual elastic constants (C11, C22, C33, C44, C55, C66, C12, C23, and C13) of magnesiosiderite at high pressures via Christoffel's equations, we employed Brillouin Light Scattering (BLS) to measure shear wave (Vs) and compressional wave velocities (Vp) as a function of the azimuthal angle under lower <span class="hlt">mantle</span> pressures, accompanied by Impulsive Stimulate Light Scattering (ISS) to measure the Vp when pressures are too high to measure it by BLS. A general thermoelastic modelling was developed to fit the elastic softening within the spin transition. We will further discuss the effects of pressures, as well as iron spin states, on the single-crystal elasticity and seismic parameters (Vp and Vs anisotropy AVp, AVs, etc) at lower <span class="hlt">mantle</span> conditions. These results could provide clues in explaining regional seismic heterogeneities in deep <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000orem.book..339S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000orem.book..339S"><span>Evolution of the Moon's <span class="hlt">Mantle</span> and Crust as Reflected in Trace-Element Microbeam Studies of Lunar Magmatism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shearer, C. K.; Floss, C.</p> <p></p> <p>Ion microprobe trace-element studies of lunar cumulates [ferroan anorthosites (FAN), highlands Mg suite (HMS), and highlands alkali suite (HAS)] and volcanic glasses have provided an additional perspective in reconstructing lunar magmatism and <span class="hlt">early</span> <span class="hlt">differentiation</span>. Calculated melt compositions for the FANs indicate that a simple lunar magma ocean (LMO) model does not account for differences between FANs with highly magnesian mafic minerals and “typical” ferroan anorthosites. The HMS and HAS appear to have crystallized from magmas that had incompatible trace-element concentrations equal to or greater than KREEP. Partial melting of distinct, hybridized sources is consistent with these calculated melt compositions. However, the high-Mg silicates with relatively low Ni content that are observed in the HMS are suggestive of other possible processes (reduction, metal removal). The compositions of the picritic glasses indicate that they were produced by melting of hybrid cumulate sources produced by mixing of <span class="hlt">early</span> and late LMO cumulates. The wide compositional range of near-primitive mare basalts indicates small degrees of localized melting preserved the signature of distinct <span class="hlt">mantle</span> reservoirs. The relationship between ilmenite anomalies and 182W in the mare basalts suggests that the LMO crystallized over a short period of time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70015833','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70015833"><span>Midcontinent rift volcanism in the Lake Superior region: Sr, Nd, and Pb isotopic evidence for a <span class="hlt">mantle</span> plume origin</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Nicholson, S.W.; Shirey, S.B.</p> <p>1990-01-01</p> <p>Between 1091 and 1098 Ma, most of a 15- to 20-km thickness of dominantly tholeiitic basalt erupted in the Midcontinent Rift System of the Lake Superior region, North America. The Portage Lake Volcanics in Michigan, which are the younget MRS flood basalts, fall into distinctly high- and low-TiO2 types having different liquid lines of descent. Incompatible trace elements in both types of tholeiites are enriched compared to depleted or primitive <span class="hlt">mantle</span> and both basalt types are isotopically indistinguishable. The isotopic enrichment of the MRS source compared to depleted <span class="hlt">mantle</span> is striking and must have occurred at least 700 m.y. before 1100 Ma. There are two likely sources for such magmatism: subcontinental lithospheric <span class="hlt">mantle</span> enriched during the <span class="hlt">early</span> Proterozoic or enriched <span class="hlt">mantle</span> derived from an upwelling plume. Decompression melting of an upwelling enriched <span class="hlt">mantle</span> plume in a region of lithosphere thinned by extension could have successfully generated the enormous volume (850 ?? 103 km3) of relatively homogeneous magma in a restricted time interval. -from Authors</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950004787','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950004787"><span><span class="hlt">Early</span> <span class="hlt">differentiation</span> of the Moon: Experimental and modeling studies and experimental and modeling studies of massif anorthosites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Longhi, John</p> <p>1994-01-01</p> <p>NASA grant NAG9-329 was in effect from 3/1/89 to 8/31/94, the last 18 months being a no-cost extension. While the grant was in effect, the P.I., coworkers, and students gave 22 talks and poster sessions at professional meetings, published 12 articles in referred journals (one more is in press, and another is in review), and edited 2 workshop reports relevant to this project. Copies of all the publications are appended to this report. The major accomplishments during the grant period have derived from three quarters: 1) the application of quantitative models of fractional crystallization and partial melting to various problems in planetary science, such as the petrogenesis of picritic glasses and mare basalts and the implications of the SNC meteorites for martian evolution; 2) an experimental study of silicate liquid immiscibility relevant to <span class="hlt">early</span> lunar <span class="hlt">differentiation</span> and the petrogenesis of evolved highlands rocks; and 3) experimental studies of massif anorthosites and related rocks that provide terrestrial analogs for the proposed origin of lunar anorthosites by multistage processes. The low-pressure aspects of the quantitative models were developed by the P.I. in the 1980s with NASA support and culminated with a paper comparing the crystallization of terrestrial and lunar lavas. The basis for the high-pressure modifications to the quantitative models is a data set gleaned from high pressure melting experiments done at Lamont and is supplemented by published data from other labs that constrain the baric and compositional dependences of various liquidus phase boundaries such as olivine/orthopyroxene, relevant to the melting of the <span class="hlt">mantles</span> of the terrestrial planets. With these models it is possible to predict not only the thermal and compositional evolution of magmatic liquids ranging in composition from lumar mare basalt to terrestrial calc-alkaline basalts, but also the small increments of fractional melting that are produced when <span class="hlt">mantle</span> rises adiabatically</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910811H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910811H"><span>The <span class="hlt">mantle</span> lithosphere and the Wilson Cycle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heron, Philip; Pysklywec, Russell; Stephenson, Randell</p> <p>2017-04-01</p> <p>In the view of the conventional theory of plate tectonics (e.g., the Wilson Cycle), crustal inheritance is often considered important in tectonic evolution. However, the role of the <span class="hlt">mantle</span> lithosphere is usually overlooked due to its difficulty to image and uncertainty in rheological makeup. Deep seismic imaging has shown potential scarring in continental <span class="hlt">mantle</span> lithosphere to be ubiquitous. Recent studies have interpreted <span class="hlt">mantle</span> lithosphere heterogeneities to be pre-existing structures, and as such linked to the Wilson Cycle and inheritance. In our study, we analyze intraplate deformation driven by <span class="hlt">mantle</span> lithosphere heterogeneities from ancient Wilson Cycle processes and compare this to crustal inheritance deformation. We present 2-D numerical experiments of continental convergence to generate intraplate deformation, exploring the limits of continental rheology to understand the dominant lithosphere layer across a broad range of geological settings. By implementing a "jelly sandwich" rheology, characteristic of stable continental lithosphere, we find that during compression the strength of the <span class="hlt">mantle</span> lithosphere is integral in controlling deformation from a structural anomaly. We posit that if the continental <span class="hlt">mantle</span> is the strongest layer within the lithosphere, then such inheritance may have important implications for the Wilson Cycle. Furthermore, our models show that deformation driven by <span class="hlt">mantle</span> lithosphere scarring can produce tectonic patterns related to intraplate orogenesis originating from crustal sources, highlighting the need for a more formal discussion of the role of the <span class="hlt">mantle</span> lithosphere in plate tectonics. We outline the difficulty in unravelling the causes of tectonic deformation, alongside discussing the role of deep lithosphere processes in plate tectonics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMGP41C1147F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMGP41C1147F"><span><span class="hlt">Mantle</span> Metasomatism under Island Arcs, Magnetic Implications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Friedman, S. A.; Ferre, E. C.; Arai, S.</p> <p>2013-12-01</p> <p>The wedge of upper <span class="hlt">mantle</span> beneath oceanic and island arcs receives an abundant flux of fluids derived from dehydration of subducted slabs. These fluids may cause metasomatism, serpentinization or partial melting at increasing distance from the trench. Each one of these processes profoundly modifies the oxygen fugacity, mineral assemblage, rheology and seismic properties of <span class="hlt">mantle</span> rocks. <span class="hlt">Mantle</span> xenoliths in arcs are relatively rare compared to other tectonic settings yet, due to their rapid ascent, they provide the best record of <span class="hlt">mantle</span> rocks at depth. Previous studies on the metasomatism of the arc <span class="hlt">mantle</span> wedge focused on the geochemistry and mineralogy of these xenoliths. Here we present new rock magnetic and paleomagnetic results to track changes in the magnetic assemblage of <span class="hlt">mantle</span> peridotites. Peridotites undergo a wide range of fluid-reactions that involve formation of magnetically remanent phases such as magnetite, maghemite, hematite or monosulfide solutions. Samples for this study originate from three localities displaying different degrees of metasomatism: a) Five samples from Ichinomegata crater, Megata volcano, in NE Japan are characteristically lherzolitic with metasomatic pargasite present; b) Six samples from Kurose, Hakata Bay, in SW Japan are mainly harzburgites that contain rare, late stage metasomatic sulfides; and c) Ten samples from the Iraya volcano, Batan Island, in the Philippines are lherzolites, harzburgites, and dunites that contain metasomatic olivine, orthopyroxene, clinopyroxene and pargasite. Both remanent and induced magnetizations of these <span class="hlt">mantle</span> peridotites exhibit systematic variations as a function of the degrees of metasomatism. The contribution of these <span class="hlt">mantle</span> peridotites to long wavelength magnetic anomalies might be significant.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.199...91L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.199...91L"><span>Molybdenum isotope fractionation in the <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liang, Yu-Hsuan; Halliday, Alex N.; Siebert, Chris; Fitton, J. Godfrey; Burton, Kevin W.; Wang, Kuo-Lung; Harvey, Jason</p> <p>2017-02-01</p> <p> concentrations of all the ultramafic xenoliths of 40-400 ppb, similar to or, significantly higher than, current estimates for the BSE (39 ppb). On this basis a revised best estimate of the Mo content in the BSE based on these concentrations would be in the range 113-180 ppb, significantly higher than previously assumed. These values are similar to the levels of depletion in the other refractory moderately siderophile elements W, Ni and Co. A simpler explanation may be that the subcontinental lithospheric <span class="hlt">mantle</span> has been selectively enriched in Mo leading to the higher concentrations observed. Cryptic melt metasomatism would be difficult to reconcile with the high Mo/Ce of the most LREE depleted xenoliths. Ancient Mo-enriched subducted components would be expected to have heavy δ98/95Mo, which is not observed. The Mo isotope composition of the BSE, cannot be reliably resolved from that of chondrites at this time despite experimental evidence for metal-silicate fractionation. An identical isotopic composition might result from core-<span class="hlt">mantle</span> <span class="hlt">differentiation</span> under very high temperatures such as were associated with the Moon-forming Giant Impact, or from the BSE inventory reflecting addition of moderately siderophile elements from an oxidised Moon-forming impactor (O'Neill, 1991). However, the latter would be inconsistent with the non-chondritic radiogenic W isotopic composition of the BSE. Based on <span class="hlt">mantle</span> fertility arguments, Mo in the BSE could even be lighter (lower 98/95Mo) than that in chondrites, which might be explained by loss of S rich liquids from the BSE during core formation (Wade et al., 2012). Such a late removal model is no longer required to explain the Mo concentration of the BSE if its abundance is in fact much higher, and similar to the values for ultramafic xenoliths.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GGG....17.2643B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GGG....17.2643B"><span>Deformation in the <span class="hlt">mantle</span> wedge associated with Laramide flat-slab subduction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Behr, Whitney M.; Smith, Douglas</p> <p>2016-07-01</p> <p>Laramide crustal deformation in the Rocky Mountains of the west-central United States is often considered to relate to a narrow segment of shallow subduction of the Farallon slab, but there is no consensus as to how deformation along the slab-<span class="hlt">mantle</span> lithosphere interface was accommodated. Here we investigate deformation in <span class="hlt">mantle</span> rocks associated with hydration and shear above the flat-slab at its contact with the base of the North American plate. The rocks we focus on are deformed, hydrated, ultramafic inclusions hosted within diatremes of the Navajo Volcanic Field in the central Colorado Plateau that erupted during the waning stages of the Laramide orogeny. We document a range of deformation textures, including granular peridotites, porphyroclastic peridotites, mylonites, and cataclasites, which we interpret to reflect different proximities to a slab-<span class="hlt">mantle</span>-interface shear zone. Mineral assemblages and chemistries constrain deformation to hydrous conditions in the temperature range ˜550-750°C. Despite the presence of hydrous phyllosilicates in modal percentages of up to 30%, deformation was dominated by dislocation creep in olivine. The mylonites exhibit an uncommon lattice preferred orientation (LPO) in olivine, known as B-type LPO in which the a-axes are aligned perpendicular to the flow direction. The low temperature, hydrated setting in which these fabrics formed is consistent with laboratory experiments that indicate B-type LPOs form under conditions of high stress and high water contents; furthermore, the <span class="hlt">mantle</span> wedge context of these LPOs is consistent with observations of trench-parallel anisotropy in the <span class="hlt">mantle</span> wedge above many modern subduction zones. <span class="hlt">Differential</span> stress magnitudes in the mylonitic rocks estimated using paleopiezometry range from 290 to 444 MPa, and calculated effective viscosities using a wet olivine flow law are on the order of 1019-1023 Pa s. The high stress magnitudes, high effective viscosities, and high strains recorded in these</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1911230H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1911230H"><span>The Stability of Tibetan <span class="hlt">Mantle</span> Lithosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Houseman, Gregory; England, Philip</p> <p>2017-04-01</p> <p>The large area of thickened crust beneath the Tibetan Plateau is a consequence of sustained continental convergence between India and the Eurasian land mass during the last 50 m.y. Although the Tibetan crust has thickened, there has been much debate about the consequences for its sub-crustal <span class="hlt">mantle</span> lithosphere. The onset of crustal thinning in the late Miocene appears to require an increase in the gravitational potential energy of the plateau at that time. One explanation for that increase depended on the idea that the <span class="hlt">mantle</span> lithosphere beneath Tibet had been replaced by asthenosphere, either by some form of convective thinning or by a delamination process akin to retreating subduction acting on the unstable lithospheric <span class="hlt">mantle</span> layer. Such ideas seem consistent with the history of magmatism and volcanism on the plateau. However, the dispersion of surface waves crossing the plateau implies that a relatively cold and fast layer of <span class="hlt">mantle</span> remains beneath the plateau to depths of at least 250 km. Because the surface wave data appear inconsistent with the idea that <span class="hlt">mantle</span> lithosphere has been removed, we investigate an alternative explanation that could explain the apparent increase in gravitational potential energy of the Tibetan lithosphere. If that <span class="hlt">mantle</span> lithosphere has remained largely in place due to an intrinsic compositional buoyancy but, on thickening, has become unstable to an internal convective overturn, then: (1) <span class="hlt">mantle</span> material at near asthenospheric temperatures would be emplaced below the crust, and (2) colder <span class="hlt">mantle</span> from beneath the Moho could become stranded above about 250 km depth. This mechanism is feasible if the Tibetan sub-continental <span class="hlt">mantle</span> lithosphere is depleted and intrinsically less dense than the underlying asthenosphere. The mechanism is broadly consistent with the surface wave analyses (which cannot resolve the short horizontal wavelengths on which overturn is likely to occur), and it predicts the kind of short-wavelength variations that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140002779','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140002779"><span>The Paradox of a Wet (High H2O) and Dry (Low H2O/Ce) <span class="hlt">Mantle</span>: High Water Concentrations in <span class="hlt">Mantle</span> Garnet Pyroxenites from Hawaii</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peslier, Anne H.; Bizimis, Michael</p> <p>2013-01-01</p> <p>Water dissolved as trace amounts in anhydrous minerals has a large influence on the melting behavior and physical properties of the <span class="hlt">mantle</span>. The water concentration of the oceanic <span class="hlt">mantle</span> is inferred from the analyses of Mid-Ocean Ridge Basalt (MORB) and Oceanic Island Basalt (OIB). but there is little data from actual <span class="hlt">mantle</span> samples. Moreover, enriched mineralogies (pyroxenites, eclogites) are thought as important sources of heterogeneity in the <span class="hlt">mantle</span>, but their water concentrations and their effect on the water budget and cycling in the <span class="hlt">mantle</span> are virtually unknown. Here, we analyzed by FTIR water in garnet clinopyroxenite xenoliths from Salt Lake Crater, Oahu, Hawaii. These pyroxenites are high-pressure (>20kb) crystal fractionates from alkalic melts. The clinopyroxenes (cpx) have 260 to 576 ppm wt H2O, with the least <span class="hlt">differentiated</span> samples (Mg#>0.8) in the 400-500 ppm range. Orthopyroxene (opx) contain 117-265 ppm H2O, about half of that of cpx, consistent with other natural sample studies, but lower than cpx/opx equilibrium from experimental data. The pyroxenite cpx and opx H2O concentrations are at the high-end of on-and off-craton peridotite xenolith concentrations and those of Hawaiian spinel peridotites. In contrast, garnet has extremely low water contents (<5ppm H2O). There is no correlation between H2O in cpx and lithophile element concentrations. Phlogopite is present in some samples, and its modal abundance shows a positive correlation in Mg# with cpx, implying equilibrium. However, there is no correlation between H2O concentrations and or the presence of phlogopite. These data imply that cpx and opx may be at water saturation, far lower than experimental data suggest. Reconstructed bulk rock pyroxenite H2O ranges from 200-460 ppm (average 331 +/- 75 ppm), 2 to 8 times higher than H2O estimates for the MORB source (50-200 ppm), but in the range of E-MORB, OIB and the source of rejuvenated Hawaiian magmas. The average bulk rock pyroxenite H2O/Ce is 69</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ClinicalTrials.gov/ct2/show/study/NCT02489123','CLINICALTRIALS'); return false;" href="https://ClinicalTrials.gov/ct2/show/study/NCT02489123"><span>Enzalutamide in Treating Patients With Relapsed or Refractory <span class="hlt">Mantle</span> Cell Lymphoma</span></a></p> <p><a target="_blank" href="http://www.clinicaltrials.gov/ct/screen/SimpleSearch">ClinicalTrials.gov</a></p> <p></p> <p>2018-03-27</p> <p>Ann Arbor Stage I <span class="hlt">Mantle</span> Cell Lymphoma; Ann Arbor Stage II <span class="hlt">Mantle</span> Cell Lymphoma; Ann Arbor Stage III <span class="hlt">Mantle</span> Cell Lymphoma; Ann Arbor Stage IV <span class="hlt">Mantle</span> Cell Lymphoma; Recurrent <span class="hlt">Mantle</span> Cell Lymphoma; Refractory <span class="hlt">Mantle</span> Cell Lymphoma</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......106L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......106L"><span>Dynamics of Compressible Convection and Thermochemical <span class="hlt">Mantle</span> Convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Xi</p> <p></p> <p>The Earth's long-wavelength geoid anomalies have long been used to constrain the dynamics and viscosity structure of the <span class="hlt">mantle</span> in an isochemical, whole-<span class="hlt">mantle</span> convection model. However, there is strong evidence that the seismically observed large low shear velocity provinces (LLSVPs) in the lowermost <span class="hlt">mantle</span> are chemically distinct and denser than the ambient <span class="hlt">mantle</span>. In this thesis, I investigated how chemically distinct and dense piles influence the geoid. I formulated dynamically self-consistent 3D spherical convection models with realistic <span class="hlt">mantle</span> viscosity structure which reproduce Earth's dominantly spherical harmonic degree-2 convection. The models revealed a compensation effect of the chemically dense LLSVPs. Next, I formulated instantaneous flow models based on seismic tomography to compute the geoid and constrain <span class="hlt">mantle</span> viscosity assuming thermochemical convection with the compensation effect. Thermochemical models reconcile the geoid observations. The viscosity structure inverted for thermochemical models is nearly identical to that of whole-<span class="hlt">mantle</span> models, and both prefer weak transition zone. Our results have implications for mineral physics, seismic tomographic studies, and <span class="hlt">mantle</span> convection modelling. Another part of this thesis describes analyses of the influence of <span class="hlt">mantle</span> compressibility on thermal convection in an isoviscous and compressible fluid with infinite Prandtl number. A new formulation of the propagator matrix method is implemented to compute the critical Rayleigh number and the corresponding eigenfunctions for compressible convection. Heat flux and thermal boundary layer properties are quantified in numerical models and scaling laws are developed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.216...96W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.216...96W"><span>Silver contents and Cu/Ag ratios in Martian meteorites and the implications for planetary <span class="hlt">differentiation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Zaicong; Becker, Harry</p> <p>2017-11-01</p> <p> <span class="hlt">mantle</span> compared to bulk Mars. Bulk Mars is richer in moderately volatile elements than Earth, however, the Martian <span class="hlt">mantle</span> displays a much stronger depletion of the moderately volatile elements Cu and Ag, e.g., by a factor of 15 for Cu. This observation is consistent with experimental studies suggesting that core formation at low P-T conditions on Mars led to more siderophile behavior of Cu and Ag than at high P-T conditions as proposed for Earth. In contrast, Cu/Ag ratios of the <span class="hlt">mantles</span> of Mars and Earth (Cu/AgEarth = 3500 ± 1000) display only a difference by a factor of 3, which implies restricted fractionation of Cu and Ag even at high P-T conditions. The concentration data support the notion that siderophile element partitioning during planetary core formation scales with the size of the planetary body, which is particularly important for the <span class="hlt">differentiation</span> of large terrestrial planets such as Earth. Collectively, the Ag and Cu data on magmatic products from the <span class="hlt">mantles</span> of Mars and Earth and the data on chondrites confirm experimental predictions and support the limited fractionation of Cu and Ag during planetary core formation and high-temperature magmatic evolution, and probably also in <span class="hlt">early</span> solar nebular processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912589B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912589B"><span>Late Miocene extensional systems in northern Tunisia and their relation with SE directed delamination of the African subcontinental <span class="hlt">mantle</span> lithosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Booth-Rea, Guillermo; Gaidi, Seif; Melki, Fetheddine; Pérez-Peña, Vicente; Marzougui, Wissem; Azañón, Jose Miguel; Galve, Jorge Pedro</p> <p>2017-04-01</p> <p>Recent work has proposed the delamination of the subcontinental <span class="hlt">mantle</span> lithosphere under northern Tunisia during the late Miocene. This process is required to explain the present location of the Tunisian segment of the African slab, imaged by seismic tomography, hanging under the Gulf of Gabes to the south of Tunisia. Thus, having retreated towards the SE several hundred km from its original position under the Tellian-Atlas nappe contact that crops out along the north of Tunisia. However, no tectonic structures have been described which could be related to this mechanism of lithospheric <span class="hlt">mantle</span> peeling. Here we describe for the first time extensional fault systems in northern Tunisia that strongly thinned the Tellian nappes, exhuming rocks from the Tunisian Atlas in the core of folded extensional detachments. Two normal fault systems with sub-orthogonal extensional transport occur. These were active during the late Miocene associated to the extrusion of 13 Ma granodiorite and 9 Ma rhyodacite in the footwall of the Nefza detachment. We have <span class="hlt">differentiated</span> an extensional system formed by low-angle normal faults with NE- and SW-directed transport cutting through the <span class="hlt">Early</span> to Middle Miocene Tellian nappen stack and a later system of low and high-angle normal faults that cuts down into the underlying Tunisian Atlas units with SE-directed transport, which root in the Nefza detachment. Both normal fault systems have been later folded and cut by thrusts during Plio-Quaternary NW-SE directed compression. These findings change the interpretation of the tectonic evolution of Tunisia that has always been framed in a transpressive to compressive setting, manifesting the extensional effects of Late Miocene lithospheric <span class="hlt">mantle</span> delamination under northern Tunisia.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.T13C2737J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.T13C2737J"><span>Self-Consistent Generation of Continental Crust in Global <span class="hlt">Mantle</span> Convection Models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jain, C.; Rozel, A. B.; Tackley, P.</p> <p>2016-12-01</p> <p>Numerical modelling commonly shows that <span class="hlt">mantle</span> convection and continents have strong feedbacks on each other (Philips and Coltice, JGR 2010; Heron and Lowman, JGR 2014), but the continents are always inserted a priori while basaltic (oceanic) crust is generated self-consistently in such models (Rolf et al., EPSL 2012). We aim to implement self-consistent generation of continental crust in global models of <span class="hlt">mantle</span> convection using StagYY (Tackley, PEPI 2008). The silica-rich continental crust appears to have been formed by fractional melting and crystallization in episodes of relatively rapid growth from late Archaean to late Proterozoic eras (3-1 Ga) (Hawkesworth & Kemp, Nature 2006). It takes several stages of <span class="hlt">differentiation</span> to generate continental crust. First, the basaltic magma is extracted from the pyrolitic <span class="hlt">mantle</span>. Second, it goes through eclogitic transformation and then partially melts to form Na-rich Tonalite-Trondhjemite-Granodiorite (TTG) which rise to form proto-continents (Rudnick, Nature 1995; Herzberg & Rudnick, Lithos 2012). TTGs dominate the grey gneiss complexes which make up most of the continental crust. Based on the melting conditions proposed by Moyen (Lithos, 2011), we parameterize TTG formation and henceforth, the continental crust. Continental crust can also be destroyed by subduction or delamination. We will investigate continental growth and destruction history in the models spanning the age of the Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.6187J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.6187J"><span>Self-consistent generation of continental crust in global <span class="hlt">mantle</span> convection models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jain, Charitra; Rozel, Antoine; Tackley, Paul</p> <p>2017-04-01</p> <p>Numerical modeling commonly shows that <span class="hlt">mantle</span> convection and continents have strong feedbacks on each other (Philips and Coltice, JGR 2010; Heron and Lowman, JGR 2014), but the continents are always inserted a priori while basaltic (oceanic) crust is generated self-consistently in such models (Rolf et al., EPSL 2012). We aim to implement self-consistent generation of continental crust in global models of <span class="hlt">mantle</span> convection using StagYY (Tackley, PEPI 2008). The silica-rich continental crust appears to have been formed by fractional melting and crystallization in episodes of relatively rapid growth from late Archean to late Proterozoic eras (3-1 Ga) (Hawkesworth & Kemp, Nature 2006). It takes several stages of <span class="hlt">differentiation</span> to generate continental crust. First, the basaltic magma is extracted from the pyrolitic <span class="hlt">mantle</span>. Second, it goes through eclogitic transformation and then partially melts to form Na-rich Tonalite-Trondhjemite-Granodiorite (TTG) which rise to form proto-continents (Rudnick, Nature 1995; Herzberg & Rudnick, Lithos 2012). TTGs dominate the grey gneiss complexes which make up most of the continental crust. Based on the melting conditions proposed by Moyen (Lithos, 2011), we parameterize TTG formation and henceforth, the continental crust. Continental crust can also be destroyed by subduction or delamination. We will investigate continental growth and destruction history in the models spanning the age of the Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9572726','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9572726"><span>Plutonium-fission xenon found in Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kunz; Staudacher; Allegre</p> <p>1998-05-08</p> <p>Data from mid-ocean ridge basalt glasses indicate that the short-lived radionuclide plutonium-244 that was present during an <span class="hlt">early</span> stage of the development of the solar system is responsible for roughly 30 percent of the fissiogenic xenon excesses in the interior of Earth today. The rest of the fissiogenic xenon can be ascribed to the spontaneous fission of still live uranium-238. This result, in combination with the refined determination of xenon-129 excesses from extinct iodine-129, implies that the accretion of Earth was finished roughly 50 million to 70 million years after solar system formation and that the atmosphere was formed by <span class="hlt">mantle</span> degassing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GGG....16.1449N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GGG....16.1449N"><span>Water circulation and global <span class="hlt">mantle</span> dynamics: Insight from numerical modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakagawa, Takashi; Nakakuki, Tomoeki; Iwamori, Hikaru</p> <p>2015-05-01</p> <p>We investigate water circulation and its dynamical effects on global-scale <span class="hlt">mantle</span> dynamics in numerical thermochemical <span class="hlt">mantle</span> convection simulations. Both dehydration-hydration processes and dehydration melting are included. We also assume the rheological properties of hydrous minerals and density reduction caused by hydrous minerals. Heat transfer due to <span class="hlt">mantle</span> convection seems to be enhanced more effectively than water cycling in the <span class="hlt">mantle</span> convection system when reasonable water dependence of viscosity is assumed, due to effective slab dehydration at shallow depths. Water still affects significantly the global dynamics by weakening the near-surface oceanic crust and lithosphere, enhancing the activity of surface plate motion compared to dry <span class="hlt">mantle</span> case. As a result, including hydrous minerals, the more viscous <span class="hlt">mantle</span> is expected with several orders of magnitude compared to the dry <span class="hlt">mantle</span>. The average water content in the whole <span class="hlt">mantle</span> is regulated by the dehydration-hydration process. The large-scale thermochemical anomalies, as is observed in the deep <span class="hlt">mantle</span>, is found when a large density contrast between basaltic material and ambient <span class="hlt">mantle</span> is assumed (4-5%), comparable to mineral physics measurements. Through this study, the effects of hydrous minerals in <span class="hlt">mantle</span> dynamics are very important for interpreting the observational constraints on <span class="hlt">mantle</span> convection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMDI31A1952L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMDI31A1952L"><span>Subducting Slabs: Jellyfishes in the Earth's <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Loiselet, C.; Braun, J.; Husson, L.; Le Carlier de Veslud, C.; Thieulot, C.; Yamato, P.; Grujic, D.</p> <p>2010-12-01</p> <p>The constantly improving resolution of geophysical data, seismic tomography and seismicity in particular, shows that the lithosphere does not subduct as a slab of uniform thickness but is rather thinned in the upper <span class="hlt">mantle</span> and thickened around the transition zone between the upper and lower <span class="hlt">mantle</span>. This observation has traditionally been interpreted as evidence for the buckling and piling of slabs at the boundary between the upper and lower <span class="hlt">mantle</span>, where a strong contrast in viscosity may exist and cause resistance to the penetration of slabs into the lower <span class="hlt">mantle</span>. The distribution and character of seismicity reveal, however, that slabs undergo vertical extension in the upper <span class="hlt">mantle</span> and compression near the transition zone. In this paper, we demonstrate that during the subduction process, the shape of low viscosity slabs (1 to 100 times more viscous than the surrounding <span class="hlt">mantle</span>) evolves toward an inverted plume shape that we coin jellyfish. Results of a 3D numerical model show that the leading tip of slabs deform toward a rounded head skirted by lateral tentacles that emerge from the sides of the jellyfish head. The head is linked to the body of the subducting slab by a thin tail. A complete parametric study reveals that subducting slabs may achieve a variety of shapes, in good agreement with the diversity of natural slab shapes evidenced by seismic tomography. Our work also suggests that the slab to <span class="hlt">mantle</span> viscosity ratio in the Earth is most likely to be lower than 100. However, the sensitivity of slab shapes to upper and lower <span class="hlt">mantle</span> viscosities and densities, which remain poorly constrained by independent evidence, precludes any systematic deciphering of the observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010GGG....11.8016L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010GGG....11.8016L"><span>Subducting slabs: Jellyfishes in the Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Loiselet, Christelle; Braun, Jean; Husson, Laurent; Le Carlier de Veslud, Christian; Thieulot, Cedric; Yamato, Philippe; Grujic, Djordje</p> <p>2010-08-01</p> <p>The constantly improving resolution of geophysical data, seismic tomography and seismicity in particular, shows that the lithosphere does not subduct as a slab of uniform thickness but is rather thinned in the upper <span class="hlt">mantle</span> and thickened around the transition zone between the upper and lower <span class="hlt">mantle</span>. This observation has traditionally been interpreted as evidence for the buckling and piling of slabs at the boundary between the upper and lower <span class="hlt">mantle</span>, where a strong contrast in viscosity may exist and cause resistance to the penetration of slabs into the lower <span class="hlt">mantle</span>. The distribution and character of seismicity reveal, however, that slabs undergo vertical extension in the upper <span class="hlt">mantle</span> and compression near the transition zone. In this paper, we demonstrate that during the subduction process, the shape of low viscosity slabs (1 to 100 times more viscous than the surrounding <span class="hlt">mantle</span>) evolves toward an inverted plume shape that we coin jellyfish. Results of a 3D numerical model show that the leading tip of slabs deform toward a rounded head skirted by lateral tentacles that emerge from the sides of the jellyfish head. The head is linked to the body of the subducting slab by a thin tail. A complete parametric study reveals that subducting slabs may achieve a variety of shapes, in good agreement with the diversity of natural slab shapes evidenced by seismic tomography. Our work also suggests that the slab to <span class="hlt">mantle</span> viscosity ratio in the Earth is most likely to be lower than 100. However, the sensitivity of slab shapes to upper and lower <span class="hlt">mantle</span> viscosities and densities, which remain poorly constrained by independent evidence, precludes any systematic deciphering of the observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170001706','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170001706"><span>Distinct Chlorine Isotopic Reservoirs on Mars: Implications for Character, Extent and Relative Timing of Crustal Interaction with <span class="hlt">Mantle</span>-Derived Magmas, Evolution of the Martian Atmosphere, and the Building Blocks of an <span class="hlt">Early</span> Mars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shearer, C. K.; Messenger, S.; Sharp, Z. D.; Burger, P. V.; Nguyen, N.; McCubbin, F. M.</p> <p>2017-01-01</p> <p>The style, magnitude, timing, and mixing components involved in the interaction between <span class="hlt">mantle</span> derived Martian magmas and Martian crust have long been a point of debate. Understanding this process is fundamental to deciphering the composition of the Martian crust and its interaction with the atmosphere, the compositional diversity and oxygen fugacity variations in the Martian <span class="hlt">mantle</span>, the bulk composition of Mars and the materials from which it accreted, and the noble gas composition of Mars and the Sun. Recent studies of the chlorine isotopic composition of Martian meteorites imply that although the variation in delta (sup 37) Cl is limited (total range of approximately14 per mille), there appears to be distinct signatures for the Martian crust and <span class="hlt">mantle</span>. However, there are potential issues with this interpretation. New Cl isotope data from the SAM (Sample Analysis at Mars) instrument on the Mars Science Lab indicate a very wide range of Cl isotopic compositions on the Martian surface. Recent measurements by [10] duplicated the results of [7,8], but placed them within the context of SAM surface data. In addition, Martian meteorite Chassigny contains trapped noble gases with isotopic ratios similar to solar abundance, and has long been considered a pristine, <span class="hlt">mantle</span> derived sample. However, previous studies of apatite in Chassigny indicate that crustal fluids have interacted with regions interstitial to the cumulus olivine. The initial Cl isotope measurements of apatite in Chassigny suggest an addition of crustal component to this lithology, apparently contradicting the rare gas data. Here, we examine the Cl isotopic composition of multiple generations and textures of apatite in Chassigny to extricate the crustal and <span class="hlt">mantle</span> components in this meteorite and to reveal the style and timing of the addition of crustal components to <span class="hlt">mantle</span>-derived magmas. These data reveal distinct Martian Cl sources whose signatures have their origins linked to both the <span class="hlt">early</span> Solar</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28651627','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28651627"><span>Induction of endoplasmic reticulum calcium pump expression during <span class="hlt">early</span> leukemic B cell <span class="hlt">differentiation</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Aït Ghezali, Lamia; Arbabian, Atousa; Roudot, Hervé; Brouland, Jean-Philippe; Baran-Marszak, Fanny; Salvaris, Evelyn; Boyd, Andrew; Drexler, Hans G; Enyedi, Agnes; Letestu, Remi; Varin-Blank, Nadine; Papp, Bela</p> <p>2017-06-26</p> <p>Endoplasmic reticulum (ER) calcium storage and release play important roles in B lymphocyte maturation, survival, antigen-dependent cell activation and immunoglobulin synthesis. Calcium is accumulated in the endoplasmic reticulum (ER) by Sarco/Endoplasmic Reticulum Calcium ATPases (SERCA enzymes). Because lymphocyte function is critically dependent on SERCA activity, it is important to understand qualitative and quantitative changes of SERCA protein expression that occur during B lymphoid <span class="hlt">differentiation</span> and leukemogenesis. In this work we investigated the modulation of SERCA expression during the pharmacologically induced <span class="hlt">differentiation</span> of leukemic precursor B lymphoblast cell lines that carry the E2A-PBX1 fusion oncoprotein. Changes of SERCA levels during <span class="hlt">differentiation</span> were determined and compared to those of established <span class="hlt">early</span> B lymphoid <span class="hlt">differentiation</span> markers. SERCA expression of the cells was compared to that of mature B cell lines as well, and the effect of the direct inhibition of SERCA-dependent calcium transport on the <span class="hlt">differentiation</span> process was investigated. We show that E2A-PBX1 + leukemia cells simultaneously express SERCA2 and SERCA3-type calcium pumps; however, their SERCA3 expression is markedly inferior to that of mature B cells. Activation of protein kinase C enzymes by phorbol ester leads to phenotypic <span class="hlt">differentiation</span> of the cells, and this is accompanied by the induction of SERCA3 expression. Direct pharmacological inhibition of SERCA-dependent calcium transport during phorbol ester treatment interferes with the <span class="hlt">differentiation</span> process. These data show that the calcium pump composition of the ER is concurrent with increased SERCA3 expression during the <span class="hlt">differentiation</span> of precursor B acute lymphoblastic leukemia cells, that a cross-talk exists between SERCA function and the control of <span class="hlt">differentiation</span>, and that SERCA3 may constitute an interesting new marker for the study of <span class="hlt">early</span> B cell phenotype.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18451293','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18451293"><span>Structure and dynamics of Earth's lower <span class="hlt">mantle</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Garnero, Edward J; McNamara, Allen K</p> <p>2008-05-02</p> <p>Processes within the lowest several hundred kilometers of Earth's rocky <span class="hlt">mantle</span> play a critical role in the evolution of the planet. Understanding Earth's lower <span class="hlt">mantle</span> requires putting recent seismic and mineral physics discoveries into a self-consistent, geodynamically feasible context. Two nearly antipodal large low-shear-velocity provinces in the deep <span class="hlt">mantle</span> likely represent chemically distinct and denser material. High-resolution seismological studies have revealed laterally varying seismic velocity discontinuities in the deepest few hundred kilometers, consistent with a phase transition from perovskite to post-perovskite. In the deepest tens of kilometers of the <span class="hlt">mantle</span>, isolated pockets of ultralow seismic velocities may denote Earth's deepest magma chamber.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12364804','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12364804"><span>How <span class="hlt">mantle</span> slabs drive plate tectonics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Conrad, Clinton P; Lithgow-Bertelloni, Carolina</p> <p>2002-10-04</p> <p>The gravitational pull of subducted slabs is thought to drive the motions of Earth's tectonic plates, but the coupling between slabs and plates is not well established. If a slab is mechanically attached to a subducting plate, it can exert a direct pull on the plate. Alternatively, a detached slab may drive a plate by exciting flow in the <span class="hlt">mantle</span> that exerts a shear traction on the base of the plate. From the geologic history of subduction, we estimated the relative importance of "pull" versus "suction" for the present-day plates. Observed plate motions are best predicted if slabs in the upper <span class="hlt">mantle</span> are attached to plates and generate slab pull forces that account for about half of the total driving force on plates. Slabs in the lower <span class="hlt">mantle</span> are supported by viscous <span class="hlt">mantle</span> forces and drive plates through slab suction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V21C3041D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V21C3041D"><span>Iron-carbonate interaction at Earth's core-<span class="hlt">mantle</span> boundary</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dorfman, S. M.; Badro, J.; Nabiei, F.; Prakapenka, V.; Gillet, P.</p> <p>2015-12-01</p> <p>Carbon storage and flux in the deep Earth are moderated by oxygen fugacity and interactions with iron-bearing phases. The amount of carbon stored in Earth's <span class="hlt">mantle</span> versus the core depends on carbon-iron chemistry at the core-<span class="hlt">mantle</span> boundary. Oxidized carbonates subducted from Earth's surface to the lowermost <span class="hlt">mantle</span> may encounter reduced Fe0 metal from disproportionation of Fe2+ in lower <span class="hlt">mantle</span> silicates or mixing with the core. To understand the fate of carbonates in the lowermost <span class="hlt">mantle</span>, we have performed experiments on sandwiches of single-crystal (Ca0.6Mg0.4)CO3 dolomite and Fe foil in the laser-heated diamond anvil cell at lower <span class="hlt">mantle</span> conditions of 49-110 GPa and 1800-2500 K. Syntheses were conducted with in situ synchrotron X-ray diffraction to identify phase assemblages. After quench to ambient conditions, samples were sectioned with a focused Ga+ ion beam for composition analysis with transmission electron microscopy. At the centers of the heated spots, iron melted and reacted completely with the carbonate to form magnesiowüstite, iron carbide, diamond, magnesium-rich carbonate and calcium carbonate. In samples heated at 49 and 64 GPa, the two carbonates exhibit a eutectoid texture. In the sample heated at 110 GPa, the carbonates form rounded ~150-nm-diameter grains with a higher modal proportion of interspersed diamonds. The presence of reduced iron in the deep lower <span class="hlt">mantle</span> and core-<span class="hlt">mantle</span> boundary region will promote the formation of diamonds in carbonate-bearing subducted slabs. The complete reaction of metallic iron to oxides and carbides in the presence of <span class="hlt">mantle</span> carbonate supports the formation of these phases at the Earth's core-<span class="hlt">mantle</span> boundary and in ultra-low velocity zones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V11D3081M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V11D3081M"><span>Effect of <span class="hlt">Mantle</span> Wedge Hybridization by Sediment Melt on Geochemistry of Arc Magma and Arc <span class="hlt">Mantle</span> Source - Insights from Laboratory Experiments at High Pressures and Temperatures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mallik, A.; Dasgupta, R.; Tsuno, K.; Nelson, J. M.</p> <p>2015-12-01</p> <p> compare the major and trace element characteristics of bulk rock and minerals found in orthopyroxenites from supra-subduction zones with the residua formed in our experiments, to <span class="hlt">differentiate</span> between melt versus fluid, and sediment- versus basalt-derived flux in the <span class="hlt">mantle</span> wedge. [1] Mallik et al. (2015) CMP169(5) [2] Sekine & Wyllie (1982) CMP 81(3)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.T21A0864V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.T21A0864V"><span>Numerical <span class="hlt">Mantle</span> Convection Models With a Flexible Thermodynamic Interface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van den Berg, A. P.; Jacobs, M. H.; de Jong, B. H.</p> <p>2001-12-01</p> <p>Accurate material properties are needed for deep <span class="hlt">mantle</span> (P,T) conditions in order to predict the longterm behavior of convection planetary <span class="hlt">mantles</span>. Also the interpretation of seismological observations concerning the deep <span class="hlt">mantle</span> in terms of <span class="hlt">mantle</span> flow models calls for a consistent thermodynamical description of the basic physical parameters. We have interfaced a compressible convection code using the anelastic liquid approach based on finite element methods, to a database containing a full thermodynamic description of <span class="hlt">mantle</span> silicates (Ita and King, J. Geophys. Res., 99, 15,939-15,940, 1994). The model is based on high resolution (P,T) tables of the relevant thermodynamic properties containing typically 50 million (P,T) table gridpoints to obtain resolution in (P,T) space of 1 K and an equivalent of 1 km. The resulting model is completely flexible such that numerical <span class="hlt">mantle</span> convection experiments can be performed for any <span class="hlt">mantle</span> composition for which the thermodynamic database is available. We present results of experiments for 2D cartesian models using a data base for magnesium-iron silicate in a pyrolitic composition (Stixrude and Bukowinski, Geoph.Monogr.Ser., 74, 131-142, 1993) and a recent thermodynamical model for magnesium silicate for the complete <span class="hlt">mantle</span> (P,T) range, (Jacobs and Oonk, Phys. Chem. Mineral, 269, inpress 2001). Preliminary results of bulksound velocity distribution derived in a consistent way from the convection results and the thermodynamic database show a `realistic' <span class="hlt">mantle</span> profile with bulkvelocity variations decreasing from several percent in the upper <span class="hlt">mantle</span> to less than a percent in the deep lower <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.474..466B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.474..466B"><span>The ruthenium isotopic composition of the oceanic <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bermingham, K. R.; Walker, R. J.</p> <p>2017-09-01</p> <p>The approximately chondritic relative, and comparatively high absolute <span class="hlt">mantle</span> abundances of the highly siderophile elements (HSE), suggest that their concentrations in the bulk silicate Earth were primarily established during a final ∼0.5 to 1% of ;late accretion; to the <span class="hlt">mantle</span>, following the cessation of core segregation. Consequently, the isotopic composition of the HSE Ru in the <span class="hlt">mantle</span> reflects an amalgamation of the isotopic compositions of late accretionary contributions to the silicate portion of the Earth. Among cosmochemical materials, Ru is characterized by considerable mass-independent isotopic variability, making it a powerful genetic tracer of Earth's late accretionary building blocks. To define the Ru isotopic composition of the oceanic <span class="hlt">mantle</span>, the largest portion of the accessible <span class="hlt">mantle</span>, we report Ru isotopic data for materials from one Archean and seven Phanerozoic oceanic <span class="hlt">mantle</span> domains. A sample from a continental lithospheric <span class="hlt">mantle</span> domain is also examined. All samples have identical Ru isotopic compositions, within analytical uncertainties, indicating that Ru isotopes are well mixed in the oceanic <span class="hlt">mantle</span>, defining a μ100Ru value of 1.2 ± 7.2 (2SD). The only known meteorites with the same Ru isotopic composition are enstatite chondrites and, when corrected for the effects of cosmic ray exposure, members of the Main Group and sLL subgroup of the IAB iron meteorite complex which have a collective CRE corrected μ100Ru value of 0.9 ± 3.0. This suggests that materials from the region(s) of the solar nebula sampled by these meteorites likely contributed the dominant portion of late accreted materials to Earth's <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFM.T71D1196B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFM.T71D1196B"><span><span class="hlt">Mantle</span> Circulation Models with variational data assimilation: Inferring past <span class="hlt">mantle</span> flow and structure from plate motion histories and seismic tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bunge, H.; Hagelberg, C.; Travis, B.</p> <p>2002-12-01</p> <p>EarthScope will deliver data on structure and dynamics of continental North America and the underlying <span class="hlt">mantle</span> on an unprecedented scale. Indeed, the scope of EarthScope makes its mission comparable to the large remote sensing efforts that are transforming the oceanographic and atmospheric sciences today. Arguably the main impact of new solid Earth observing systems is to transform our use of geodynamic models increasingly from conditions that are data poor to an environment that is data rich. Oceanographers and meteorologists already have made substantial progress in adapting to this environment, by developing new approaches of interpreting oceanographic and atmospheric data objectively through data assimilation methods in their models. However, a similarly rigorous theoretical framework for merging EarthScope derived solid Earth data with geodynamic models has yet to be devised. Here we explore the feasibility of data assimilation in <span class="hlt">mantle</span> convection studies in an attempt to fit global geodynamic model calculations explicitly to tomographic and tectonic constraints. This is an inverse problem not quite unlike the inverse problem of finding optimal seismic velocity structures faced by seismologists. We derive the generalized inverse of <span class="hlt">mantle</span> convection from a variational approach and present the adjoint equations of <span class="hlt">mantle</span> flow. The substantial computational burden associated with solutions to the generalized inverse problem of <span class="hlt">mantle</span> convection is made feasible using a highly efficient finite element approach based on the 3-D spherical fully parallelized <span class="hlt">mantle</span> dynamics code TERRA, implemented on a cost-effective topical PC-cluster (geowulf) dedicated specifically to large-scale geophysical simulations. This dedicated geophysical modeling computer allows us to investigate global inverse convection problems having a spatial discretization of less than 50 km throughout the <span class="hlt">mantle</span>. We present a synthetic high-resolution modeling experiment to demonstrate that mid</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI41A0325Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI41A0325Y"><span>Iron Isotopic Fractionation in Earth's Lower <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, H.; Lin, J. F.; Hu, M. Y.; Bi, W.; Zhao, J.; Alp, E. E.; Roskosz, M.; Dauphas, N.; Okuchi, T.</p> <p>2017-12-01</p> <p>The Earth's bulk chemical composition is vital for deciphering the origin of this planet. Our estimation of the iron isotopic composition of the bulk Earth relies on the iron isotopic composition difference between the metallic core and silicate <span class="hlt">mantle</span>. Previous studies1,2,3 on this fractionation scale have mostly focused on the alloying effects of light elements in the iron metal phases, while the pressure effects of the silicate <span class="hlt">mantle</span> phases especially due to iron partitioning4 in the lower <span class="hlt">mantle</span> minerals have not been fully addressed. For instance, Polyakov (2009) simply assumed equal iron distribution between ferropericlase and post-perovskite in his model. Shahar et al. (2016) only used bridgmanite as a proxy for the <span class="hlt">mantle</span> while another lower <span class="hlt">mantle</span> mineral ferropericlase was neglected. Here we have investigated the force constant of iron bonds in lower-<span class="hlt">mantle</span> ferropericlase and bridgmanite crystals up to 104GPa using NRIXS(Nuclear Resonant Inelastic X-ray Scattering) and SMS(Synchrotron Mössbauer Spectroscopy) in a diamond anvil cell at sector-3 of the Advance Photon Source. These results are used to evaluate the pressure effects as well as the spin/valence states of iron5,6 on the force constant of iron bonds and the iron isotope distributions within the lower <span class="hlt">mantle</span> and at the core-<span class="hlt">mantle</span> boundary. We found that the liquid-solid iron isotopic fractionation during magma ocean crystallization was limited, however, the inter-mineral fractionation between ferropericlase and bridgmanite could be significant influenced by the spin/valence states at the lowermost <span class="hlt">mantle</span> conditions. 1.Polyakov, V. B. Science 323, 912-914 (2009). 2.Shahar, A. et al. Science 352, 580-582 (2016). 3.Liu, J. et al. Nat. Commun. 8, 14377 (2017). 4.Irifune, T. et al. Science 327, 193-195 (2010). 5.Lin, J. F., Speziale, S., Mao, Z. & Marquardt, Rev. Geophys. 51, 244-275 (2013). 6.Mao, Z. et al. Am. Mineral. 102 (2017).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Litho.288..282A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Litho.288..282A"><span><span class="hlt">Early</span> Paleozoic high-Mg granodiorite from the Erlangping unit, North Qinling orogen, central China: Partial melting of metasomatic <span class="hlt">mantle</span> during the initial back-arc opening</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abdallsamed, Mohammed I. M.; Wu, Yuan-Bao; Zhang, Wenxiang; Zhou, Guangyan; Wang, Hao; Yang, Saihong</p> <p>2017-09-01</p> <p>This study discussed the petrological classification, petrogenesis, and tectonic significance of <span class="hlt">early</span> Paleozoic high-Mg granodiorite from the Erlangping unit, in the North Qinling orogen. To achieve this target, we conducted integrated investigation of in situ zircon U-Pb dating, whole-rock geochemical, as well as Sr-Nd-Hf-O isotopic compositions for the Kanfenggou pluton from the Erlangping unit. LA-ICP-MS zircon dating for the Kanfenggou samples yields U-Pb ages of 442.9 ± 6.2 and 438.0 ± 6.7 Ma, suggesting that the pluton was emplaced at ca. 440 Ma. Whole-rock geochemical compositions of the samples display intermediate SiO2 (60.48-64.67 wt%) and K2O (1.21 to 2.10 wt%), but high Al2O3 (15.44 to 16.51 wt%) and Na2O (4.01 to 4.81 wt%) contents. The granodiorite samples are characterized by elevated MgO ranging from 2.30 to 3.44 wt% and Mg# values of 53.35to 56.66, implying they are high-Mg granodiorites. They are characterized by very high Ba (524-1132 ppm) and Sr (684-980 ppm) contents, but depleted in HREE, and high (La/Yb)N ratios of 6.34 to 16.5 and slightly negative to weak positive Eu anomalies (Eu/Eu* = 0.68-1.09). These evidence that the Kanfenggou pluton belongs to the sanukitoid series. The high-Mg granodiorite samples exhibit a <span class="hlt">mantle</span> signature with high Mg# values (53.35-56.66), Cr (45.8 to 93.3 ppm) and Ni (28.2 to 48.2 ppm) contents, but enriched in LILE, pointing to an enriched <span class="hlt">mantle</span> source. The samples show relatively depleted radiogenic isotopic compositions with initial 87Sr/86Sr ratios varying from 0.7044 to 0.7047, εNd(t) values from 0.31 to 4.21, and zircon εHf (t) values from 7.3 to 8.3. The zircons have a mean δ18O value of 5.20 ± 0.17 ‰. Based on the trace element geochemical features, the metasomatic agent was suggested to be the fluids generated from dehydration of subducted slab. Therefore, we suggest two-stage processes for the formation of the Erlangping high-Mg granodiorites: (1) interaction between slab fluids and <span class="hlt">mantle</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.U44A..02B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.U44A..02B"><span>Plate and Plume Flux: Constraints for paleomagnetic reference frames and interpretation of deep <span class="hlt">mantle</span> seismic heterogeneity. (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bunge, H.; Schuberth, B. S.; Shephard, G. E.; Müller, D.</p> <p>2010-12-01</p> <p>Plate and plume flow are dominant modes of <span class="hlt">mantle</span> convection, as pointed out by Geoff Davies <span class="hlt">early</span> on. Driven, respectively, from a cold upper and a hot lower thermal boundary layer these modes are now sufficiently well imaged by seismic tomographers to exploit the thermal boundary layer concept as an effective tool in exploring two long standing geodynamic problems. One relates to the choice of an absolute reference frame in plate tectonic reconstructions. Several absolute reference frames have been proposed over the last decade, including those based on hotspot tracks displaying age progression and assuming either fixity or motion, as well as palaeomagnetically-based reference frames, a subduction reference frame and hybrid versions. Each reference frame implies a particular history of the location of subduction zones through time and thus the evolution of <span class="hlt">mantle</span> heterogeneity via mixing of subducted slab material in the <span class="hlt">mantle</span>. Here we compare five alternative absolute plate motion models in terms of their consequences for deep <span class="hlt">mantle</span> structure. Taking global paleo-plate boundaries and plate velocities back to 140 Ma derived from the new plate tectonic reconstruction software GPlates and assimilating them into vigorous 3-D spherical <span class="hlt">mantle</span> circulation models, we infer geodynamic <span class="hlt">mantle</span> heterogeneity and compare it to seismic tomography for each absolute rotation model. We also focus on the challenging problem of interpreting deep <span class="hlt">mantle</span> seismic heterogeneity in terms of thermal and compositional variations. Using published thermodynamically self-consistent <span class="hlt">mantle</span> mineralogy models in the pyrolite composition, we find strong plume flux from the CMB, with a high temperature contrast (on the order of 1000 K) across the lower thermal boundary layer is entirely sufficient to explain elastic heterogeneity in the deep <span class="hlt">mantle</span> for a number of quantitative measures. A high excess temperatures of +1000--1500 K for plumes in the lowermost <span class="hlt">mantle</span> is particularly important in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70190580','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70190580"><span>Abundant carbon in the <span class="hlt">mantle</span> beneath Hawai`i</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Anderson, Kyle R.; Poland, Michael</p> <p>2017-01-01</p> <p>Estimates of carbon concentrations in Earth’s <span class="hlt">mantle</span> vary over more than an order of magnitude, hindering our ability to understand <span class="hlt">mantle</span> structure and mineralogy, partial melting, and the carbon cycle. CO2 concentrations in <span class="hlt">mantle</span>-derived magmas supplying hotspot ocean island volcanoes yield our most direct constraints on <span class="hlt">mantle</span> carbon, but are extensively modified by degassing during ascent. Here we show that undegassed magmatic and <span class="hlt">mantle</span> carbon concentrations may be estimated in a Bayesian framework using diverse geologic information at an ocean island volcano. Our CO2 concentration estimates do not rely upon complex degassing models, geochemical tracer elements, assumed magma supply rates, or rare undegassed rock samples. Rather, we couple volcanic CO2 emission rates with probabilistic magma supply rates, which are obtained indirectly from magma storage and eruption rates. We estimate that the CO2content of <span class="hlt">mantle</span>-derived magma supplying Hawai‘i’s active volcanoes is 0.97−0.19+0.25 wt%—roughly 40% higher than previously believed—and is supplied from a <span class="hlt">mantle</span> source region with a carbon concentration of 263−62+81 ppm. Our results suggest that <span class="hlt">mantle</span> plumes and ocean island basalts are carbon-rich. Our data also shed light on helium isotope abundances, CO2/Nb ratios, and may imply higher CO2 emission rates from ocean island volcanoes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatGe..10..704A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatGe..10..704A"><span>Abundant carbon in the <span class="hlt">mantle</span> beneath Hawai`i</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anderson, Kyle R.; Poland, Michael P.</p> <p>2017-09-01</p> <p>Estimates of carbon concentrations in Earth’s <span class="hlt">mantle</span> vary over more than an order of magnitude, hindering our ability to understand <span class="hlt">mantle</span> structure and mineralogy, partial melting, and the carbon cycle. CO2 concentrations in <span class="hlt">mantle</span>-derived magmas supplying hotspot ocean island volcanoes yield our most direct constraints on <span class="hlt">mantle</span> carbon, but are extensively modified by degassing during ascent. Here we show that undegassed magmatic and <span class="hlt">mantle</span> carbon concentrations may be estimated in a Bayesian framework using diverse geologic information at an ocean island volcano. Our CO2 concentration estimates do not rely upon complex degassing models, geochemical tracer elements, assumed magma supply rates, or rare undegassed rock samples. Rather, we couple volcanic CO2 emission rates with probabilistic magma supply rates, which are obtained indirectly from magma storage and eruption rates. We estimate that the CO2 content of <span class="hlt">mantle</span>-derived magma supplying Hawai`i’s active volcanoes is 0.97-0.19+0.25 wt%--roughly 40% higher than previously believed--and is supplied from a <span class="hlt">mantle</span> source region with a carbon concentration of 263-62+81 ppm. Our results suggest that <span class="hlt">mantle</span> plumes and ocean island basalts are carbon-rich. Our data also shed light on helium isotope abundances, CO2/Nb ratios, and may imply higher CO2 emission rates from ocean island volcanoes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.478..143B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.478..143B"><span>Carbon isotopic variation in ureilites: Evidence for an <span class="hlt">early</span>, volatile-rich Inner Solar System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barrat, Jean-Alix; Sansjofre, Pierre; Yamaguchi, Akira; Greenwood, Richard C.; Gillet, Philippe</p> <p>2017-11-01</p> <p>We analyzed the C isotopic compositions of 32 unbrecciated ureilites, which represent <span class="hlt">mantle</span> debris from a now disrupted, C-rich, <span class="hlt">differentiated</span> body. The δ13C values of their C fractions range from -8.48 to +0.11‰. The correlations obtained between δ13C, δ18O and Δ17O values and the compositions of the olivine cores, indicate that the ureilite parent body (UPB) accreted from two reservoirs displaying distinct O and C isotopic compositions. The range of Fe/Mg ratios shown by its <span class="hlt">mantle</span> was not the result of melting processes involving reduction with C ("smelting"), but was chiefly inherited from the mixing of these two components. Because smelting reactions are pressure-dependent, this result has strong implications for the size of the UPB, and points to a large parent body, at least 690 km in diameter. It demonstrates that C-rich primitive matter distinct from that represented by carbonaceous chondrites was present in some areas of the <span class="hlt">early</span> inner Solar System, and could have contributed to the growth of the terrestrial planets. We speculate that <span class="hlt">differentiated</span>, C-rich bodies, or debris produced by their disruption, were an additional source of volatiles during the later accretion stages of the rocky planets, including Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997JGR...10220395R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997JGR...10220395R"><span>A strongly negative shear velocity gradient and lateral variability in the lowermost <span class="hlt">mantle</span> beneath the Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ritsema, Jeroen; Garnero, Edward; Lay, Thorne</p> <p>1997-01-01</p> <p>A new approach for constraining the seismic shear velocity structure above the core-<span class="hlt">mantle</span> boundary is introduced, whereby SH-SKS <span class="hlt">differential</span> travel times, amplitude ratios of SV/SKS, and Sdiff waveshapes are simultaneously modeled. This procedure is applied to the lower <span class="hlt">mantle</span> beneath the central Pacific using da.ta from numerous deep-focus southwest Pacific earthquakes recorded in North America. We analyze 90 broadband and 248 digitized analog recordings for this source-receiver geometry. SH-SKS times are highly variable and up to 10 s larger than standard reference model predictions, indicating the presence of laterally varying low shear velocities in the study area. The travel times, however, do not constrain the depth extent or velocity gradient of the low-velocity region. SV/SKS amplitude ratios and SH waveforms are sensitive to the radial shear velocity profile, and when analyzed simultaneously with SH-SKS times, rnveal up to 3% shear velocity reductions restricted to the lowermost 190±50 km of the <span class="hlt">mantle</span>. Our preferred model for the central-eastern Pacific region (Ml) has a strong negative gradient (with 0.5% reduction in velocity relative to the preliminary reference Earth model (PREM) at 2700 km depth and 3% reduction at 2891 km depth) and slight velocity reductions from 2000 to 2700 km depth (0-0.5% lower than PREM). Significant small-scale (100-500 km) shear velocity heterogeneity (0.5%-1%) is required to explain scatter in the <span class="hlt">differential</span> times and amplitude ratios.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoJI.205.1756R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoJI.205.1756R"><span>The <span class="hlt">mantle</span> transition zone beneath the Afar Depression and adjacent regions: implications for <span class="hlt">mantle</span> plumes and hydration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reed, C. A.; Gao, S. S.; Liu, K. H.; Yu, Y.</p> <p>2016-06-01</p> <p>The Afar Depression and its adjacent areas are underlain by an upper <span class="hlt">mantle</span> marked by some of the world's largest negative velocity anomalies, which are frequently attributed to the thermal influences of a lower-<span class="hlt">mantle</span> plume. In spite of numerous studies, however, the existence of a plume beneath the area remains enigmatic, partially due to inadequate quantities of broad-band seismic data and the limited vertical resolution at the <span class="hlt">mantle</span> transition zone (MTZ) depth of the techniques employed by previous investigations. In this study, we use an unprecedented quantity (over 14 500) of P-to-S receiver functions (RFs) recorded by 139 stations from 12 networks to image the 410 and 660 km discontinuities and map the spatial variation of the thickness of the MTZ. Non-linear stacking of the RFs under a 1-D velocity model shows robust P-to-S conversions from both discontinuities, and their apparent depths indicate the presence of an upper-<span class="hlt">mantle</span> low-velocity zone beneath the entire study area. The Afar Depression and the northern Main Ethiopian Rift are characterized by an apparent 40-60 km depression of both MTZ discontinuities and a normal MTZ thickness. The simplest and most probable interpretation of these observations is that the apparent depressions are solely caused by velocity perturbations in the upper <span class="hlt">mantle</span> and not by deeper processes causing temperature or hydration anomalies within the MTZ. Thickening of the MTZ on the order of 15 km beneath the southern Arabian Plate, southern Red Sea and western Gulf of Aden, which comprise the southward extension of the Afro-Arabian Dome, could reflect long-term hydration of the MTZ. A 20 km thinning of the MTZ beneath the western Ethiopian Plateau is observed and interpreted as evidence for a possible <span class="hlt">mantle</span> plume stem originating from the lower <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Tectp.723..309V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Tectp.723..309V"><span>Atlas of the underworld: Slab remnants in the <span class="hlt">mantle</span>, their sinking history, and a new outlook on lower <span class="hlt">mantle</span> viscosity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van der Meer, Douwe G.; van Hinsbergen, Douwe J. J.; Spakman, Wim</p> <p>2018-01-01</p> <p>Across the entire <span class="hlt">mantle</span> we interpret 94 positive seismic wave-speed anomalies as subducted lithosphere and associate these slabs with their geological record. We document this as the Atlas of the Underworld, also accessible online at www.atlas-of-the-underworld.org, a compilation comprising subduction systems active in the past 300 Myr. Deeper slabs are correlated to older geological records, assuming no relative horizontal motions between adjacent slabs following break-off, using knowledge of global plate circuits, but without assuming a <span class="hlt">mantle</span> reference frame. The longest actively subducting slabs identified reach the depth of 2500 km and some slabs have impinged on Large Low Shear Velocity Provinces in the deepest <span class="hlt">mantle</span>. Anomously fast sinking of some slabs occurs in regions affected by long-term plume rising. We conclude that slab remnants eventually sink from the upper <span class="hlt">mantle</span> to the core-<span class="hlt">mantle</span> boundary. The range in subduction-age versus - depth in the lower <span class="hlt">mantle</span> is largely inherited from the upper <span class="hlt">mantle</span> history of subduction. We find a significant depth variation in average sinking speed of slabs. At the top of the lower <span class="hlt">mantle</span> average slab sinking speeds are between 10 and 40 mm/yr, followed by a deceleration to 10-15 mm/yr down to depths around 1600-1700 km. In this interval, in situ time-stationary sinking rates suggest deceleration from 20 to 30 mm/yr to 4-8 mm/yr, increasing to 12-15 mm/yr below 2000 km. This corroborates the existence of a slab deceleration zone but we do not observe long-term (> 60 My) slab stagnation, excluding long-term stagnation due to compositional effects. Conversion of slab sinking profiles to viscosity profiles shows the general trend that <span class="hlt">mantle</span> viscosity increases in the slab deceleration zone below which viscosity slowly decreases in the deep <span class="hlt">mantle</span>. This is at variance with most published viscosity profiles that are derived from different observations, but agrees qualitatively with recent viscosity profiles suggested</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PNAS..115.4099H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PNAS..115.4099H"><span>Effects of iron on the lattice thermal conductivity of Earth's deep <span class="hlt">mantle</span> and implications for <span class="hlt">mantle</span> dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hsieh, Wen-Pin; Deschamps, Frédéric; Okuchi, Takuo; Lin, Jung-Fu</p> <p>2018-04-01</p> <p>Iron may critically influence the physical properties and thermochemical structures of Earth's lower <span class="hlt">mantle</span>. Its effects on thermal conductivity, with possible consequences on heat transfer and <span class="hlt">mantle</span> dynamics, however, remain largely unknown. We measured the lattice thermal conductivity of lower-<span class="hlt">mantle</span> ferropericlase to 120 GPa using the ultrafast optical pump-probe technique in a diamond anvil cell. The thermal conductivity of ferropericlase with 56% iron significantly drops by a factor of 1.8 across the spin transition around 53 GPa, while that with 8–10% iron increases monotonically with pressure, causing an enhanced iron substitution effect in the low-spin state. Combined with bridgmanite data, modeling of our results provides a self-consistent radial profile of lower-<span class="hlt">mantle</span> thermal conductivity, which is dominated by pressure, temperature, and iron effects, and shows a twofold increase from top to bottom of the lower <span class="hlt">mantle</span>. Such increase in thermal conductivity may delay the cooling of the core, while its decrease with iron content may enhance the dynamics of large low shear-wave velocity provinces. Our findings further show that, if hot and strongly enriched in iron, the seismic ultralow velocity zones have exceptionally low conductivity, thus delaying their cooling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29610319','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29610319"><span>Effects of iron on the lattice thermal conductivity of Earth's deep <span class="hlt">mantle</span> and implications for <span class="hlt">mantle</span> dynamics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hsieh, Wen-Pin; Deschamps, Frédéric; Okuchi, Takuo; Lin, Jung-Fu</p> <p>2018-04-17</p> <p>Iron may critically influence the physical properties and thermochemical structures of Earth's lower <span class="hlt">mantle</span>. Its effects on thermal conductivity, with possible consequences on heat transfer and <span class="hlt">mantle</span> dynamics, however, remain largely unknown. We measured the lattice thermal conductivity of lower-<span class="hlt">mantle</span> ferropericlase to 120 GPa using the ultrafast optical pump-probe technique in a diamond anvil cell. The thermal conductivity of ferropericlase with 56% iron significantly drops by a factor of 1.8 across the spin transition around 53 GPa, while that with 8-10% iron increases monotonically with pressure, causing an enhanced iron substitution effect in the low-spin state. Combined with bridgmanite data, modeling of our results provides a self-consistent radial profile of lower-<span class="hlt">mantle</span> thermal conductivity, which is dominated by pressure, temperature, and iron effects, and shows a twofold increase from top to bottom of the lower <span class="hlt">mantle</span>. Such increase in thermal conductivity may delay the cooling of the core, while its decrease with iron content may enhance the dynamics of large low shear-wave velocity provinces. Our findings further show that, if hot and strongly enriched in iron, the seismic ultralow velocity zones have exceptionally low conductivity, thus delaying their cooling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110008787','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110008787"><span>The <span class="hlt">Mantle</span> and Basalt-Crust Interaction Below the Mount Taylor Volcanic Field, New Mexico</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schrader, Christian M.; Crumpler, Larry S.; Schmidt, Marick E.</p> <p>2010-01-01</p> <p>The Mount Taylor Volcanic Field (MTVF) lies on the Jemez Lineament on the southeastern margin of the Colorado Plateau. The field is centered on the Mt. Taylor composite volcano and includes Mesa Chivato to the NE and Grants Ridge to the WSW. MTVF magmatism spans approximately 3.8-1.5 Ma (K-Ar). Magmas are dominantly alkaline with mafic compositions ranging from basanite to hy-basalt and felsic compositions ranging from ne-trachyte to rhyolite. We are investigating the state of the <span class="hlt">mantle</span> and the spatial and temporal variation in basalt-crustal interaction below the MTVF by examining <span class="hlt">mantle</span> xenoliths and basalts in the context of new mapping and future Ar-Ar dating. The earliest dated magmatism in the field is a basanite flow south of Mt. Taylor. <span class="hlt">Mantle</span> xenolith-bearing alkali basalts and basanites occur on Mesa Chivato and in the region of Mt. Taylor, though most basalts are peripheral to the main cone. Xenolith-bearing magmatism persists at least into the <span class="hlt">early</span> stages of conebuilding. Preliminary examination of the <span class="hlt">mantle</span> xenolith suite suggests it is dominantly lherzolitic but contains likely examples of both melt-depleted (harzburgitic) and melt-enriched (clinopyroxenitic) <span class="hlt">mantle</span>. There are aphyric and crystal-poor hawaiites, some of which are hy-normative, on and near Mt. Taylor, but many of the more evolved MTVF basalts show evidence of complex histories. Mt. Taylor basalts higher in the cone-building sequence contain >40% zoned plagioclase pheno- and megacrysts. Other basalts peripheral to Mt. Taylor and at Grants Ridge contain clinopyroxene and plagioclase megacrysts and cumulate-textured xenoliths, suggesting they interacted with lower crustal cumulates. Among the questions we are addressing: What was the chemical and thermal state of the <span class="hlt">mantle</span> recorded by the basaltic suites and xenoliths and how did it change with time? Are multiple parental basalts (Si-saturated vs. undersaturated) represented and, if so, what changes in the <span class="hlt">mantle</span> or in the tectonic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1814162C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1814162C"><span>On retrodictions of global <span class="hlt">mantle</span> flow with assimilated surface velocities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Colli, Lorenzo; Bunge, Hans-Peter; Schuberth, Bernhard S. A.</p> <p>2016-04-01</p> <p>Modeling past states of Earth's <span class="hlt">mantle</span> and relating them to geologic observations such as continental-scale uplift and subsidence is an effective method for testing <span class="hlt">mantle</span> convection models. However, <span class="hlt">mantle</span> convection is chaotic and two identical <span class="hlt">mantle</span> models initialized with slightly different temperature fields diverge exponentially in time until they become uncorrelated, thus limiting retrodictions (i.e., reconstructions of past states of Earth's <span class="hlt">mantle</span> obtained using present information) to the recent past. We show with 3-D spherical <span class="hlt">mantle</span> convection models that retrodictions of <span class="hlt">mantle</span> flow can be extended significantly if knowledge of the surface velocity field is available. Assimilating surface velocities produces in some cases negative Lyapunov times (i.e., e-folding times), implying that even a severely perturbed initial condition may evolve toward the reference state. A history of the surface velocity field for Earth can be obtained from past plate motion reconstructions for time periods of a <span class="hlt">mantle</span> overturn, suggesting that <span class="hlt">mantle</span> flow can be reconstructed over comparable times.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoRL..42.8341C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoRL..42.8341C"><span>On retrodictions of global <span class="hlt">mantle</span> flow with assimilated surface velocities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Colli, Lorenzo; Bunge, Hans-Peter; Schuberth, Bernhard S. A.</p> <p>2015-10-01</p> <p>Modeling past states of Earth's <span class="hlt">mantle</span> and relating them to geologic observations such as continental-scale uplift and subsidence is an effective method for testing <span class="hlt">mantle</span> convection models. However, <span class="hlt">mantle</span> convection is chaotic and two identical <span class="hlt">mantle</span> models initialized with slightly different temperature fields diverge exponentially in time until they become uncorrelated, thus limiting retrodictions (i.e., reconstructions of past states of Earth's <span class="hlt">mantle</span> obtained using present information) to the recent past. We show with 3-D spherical <span class="hlt">mantle</span> convection models that retrodictions of <span class="hlt">mantle</span> flow can be extended significantly if knowledge of the surface velocity field is available. Assimilating surface velocities produces in some cases negative Lyapunov times (i.e., e-folding times), implying that even a severely perturbed initial condition may evolve toward the reference state. A history of the surface velocity field for Earth can be obtained from past plate motion reconstructions for time periods of a <span class="hlt">mantle</span> overturn, suggesting that <span class="hlt">mantle</span> flow can be reconstructed over comparable times.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI11A0270B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI11A0270B"><span>The influence of water on <span class="hlt">mantle</span> convection and plate tectonics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brändli, S.; Tackley, P. J.</p> <p>2017-12-01</p> <p>Water has a significant influence to <span class="hlt">mantle</span> rheology and therefore also to the convection of the <span class="hlt">mantle</span> and the plate tectonics. The viscosity of the <span class="hlt">mantle</span> can be decreased by up to two orders of magnitude when water is present in the <span class="hlt">mantle</span>. Another effect of the water is the change in the solidus of the <span class="hlt">mantle</span> and therefore the melting regime. This two effects of water in the <span class="hlt">mantle</span> have a significant influence to <span class="hlt">mantle</span> convection and plate tectonics. The influx of water to the <span class="hlt">mantle</span> is driven by plate tectonics as wet oceanic lithosphere is subducted into the <span class="hlt">mantle</span> and then brought back to the lithosphere and the surface by MOR-, arc- and hotspot volcanism. Studies show that the amount of water in the <span class="hlt">mantle</span> is about three times bigger than the amount of water in the oceans. To model this water cycle multiple additions to StagYY are necessary. With the enhanced code we calculated multiple steady state models with a wide range of parameters to study the effect of water on the <span class="hlt">mantle</span> rheology and the behavior of the lithosphere. The results will help us to understand the earths interior and its reaction and behavior under partially hydrated conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.7484P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.7484P"><span>Tomography images of the Alpine roots and surrounding upper <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Plomerova, Jaroslava; Babuska, Vladislav</p> <p>2017-04-01</p> <p>Teleseismic body-wave tomography represents powerful tool to study regional velocity structure of the upper <span class="hlt">mantle</span> and to image velocity anomalies, such as subducted lithosphere plates in collisional zones. In this contribution, we recapitulate 3D models of the upper <span class="hlt">mantle</span> beneath the Alps, which developed at a collision zone of the Eurasian and African plates. Seismic tomography studies indicate a leading role of the rigid <span class="hlt">mantle</span> lithosphere that functioned as a major stress guide during the plate collisions. Interactions of the European lithosphere with several micro-plates in the south resulted in an arcuate shape of this mountain range on the surface and in a complicated geometry of the Alpine subductions in the <span class="hlt">mantle</span>. <span class="hlt">Early</span> models with one bended lithosphere root have been replaced with more advanced models showing two separate lithosphere roots beneath the Western and Eastern Alps (Babuska et al., Tectonophysics 1990; Lippitsch et al., JGR 2003). The standard isotropic velocity tomography, based on pre-AlpArray data (the currently performed passive seismic experiment in the Alps and surroundings) images the south-eastward dipping curved slab of the Eurasian lithosphere in the Western Alps. On the contrary, beneath the Eastern Alps the results indicate a very steep northward dipping root that resulted from the collision of the European plate with the Adriatic microplate. Dando et al. (2011) interpret high-velocity heterogeneities at the bottom of their regional tomographic model as a graveyard of old subducted lithospheres. High density of stations, large amount of rays and dense ray-coverage of the volume studied are not the only essential pre-requisites for reliable tomography results. A compromise between the amount of pre-processed data and the high-quality of the tomography input (travel-time residuals) is of the high importance as well. For the first time, the existence of two separate roots beneath the Alps has been revealed from carefully pre</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatGe..10..625B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatGe..10..625B"><span>Deep <span class="hlt">mantle</span>: Enriched carbon source detected</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barry, Peter H.</p> <p>2017-09-01</p> <p>Estimates of carbon in the deep <span class="hlt">mantle</span> vary by more than an order of magnitude. Coupled volcanic CO2 emission data and magma supply rates reveal a carbon-rich <span class="hlt">mantle</span> plume source region beneath Hawai'i with 40% more carbon than previous estimates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JAESc.111..604Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JAESc.111..604Y"><span>Late Mesozoic-Cenozoic intraplate magmatism in Central Asia and its relation with <span class="hlt">mantle</span> diapirism: Evidence from the South Khangai volcanic region, Mongolia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yarmolyuk, Vladimir V.; Kudryashova, Ekaterina A.; Kozlovsky, Alexander M.; Lebedev, Vladimir A.; Savatenkov, Valery M.</p> <p>2015-11-01</p> <p>The South Khangai volcanic region (SKVR) comprises fields of Late Mesozoic-Cenozoic volcanic rocks scattered over southern and central Mongolia. Evolution of the region from the Late Jurassic to the Late Cenozoic includes 13 successive igneous episodes that are more or less evenly distributed in time. Major patterns in the distribution of different-aged volcanic complexes were controlled by a systematic temporal migration of volcanic centers over the region. The total length of their trajectory exceeds 1600 km. Principle characteristics of local magmatism are determined. The composition of igneous rocks varies from basanites to rhyolites (predominantly, high-K rocks), with geochemistry close to that of OIB. The rock composition, however, underwent transformations in the Mesozoic-Cenozoic. Rejuvenation of mafic rocks is accompanied by decrease in the contents of HREE and increase of Nb and Ta. According to isotope data, the SKVR magmatic melts were derived from three isotope sources that differed in the Sr, Nd, and Pb isotopic compositions and successively alternated in time. In the <span class="hlt">Early</span> Cretaceous, the predominant source composition was controlled by interaction of the EMII- and PREMA-type <span class="hlt">mantle</span> materials. The PREMA-type <span class="hlt">mantle</span> material dominated quantitatively in the Late Cretaceous and initial <span class="hlt">Early</span> Cenozoic. From the latest <span class="hlt">Early</span> Cenozoic to Late Cenozoic, the magma source also contained the EMI-type material along with the PREMA-type. The structural fabric, rock composition, major evolutionary pattern, and inner structure of SKVR generally comply with the criteria used to distinguish the <span class="hlt">mantle</span> plume-related regions. Analogous features can be seen in other regions of recent volcanism in Central Asia (South Baikal, Udokan, Vitim, and Tok Stanovik). The structural autonomy of these regions suggests that distribution of the Late Mesozoic-Cenozoic volcanism in Central Asia was controlled by a group of relatively small hot finger-type <span class="hlt">mantle</span> plumes associated with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70188875','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70188875"><span><span class="hlt">Mantle</span> peridotite in newly discovered far-inland subduction complex, southwest Arizona: Initial report</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Haxel, Gordon B.; Jacobson, Carl E.; Wittke, James H.</p> <p>2015-01-01</p> <p>The latest Cretaceous to <span class="hlt">early</span> Palaeogene Orocopia Schist and related units are generally considered a low-angle subduction complex that underlies much of southern California and Arizona. A recently discovered exposure of Orocopia Schist at Cemetery Ridge west of Phoenix, Arizona, lies exceptionally far inland from the continental margin. Unexpectedly, this body of Orocopia Schist contains numerous blocks, as large as ~300 m, of variably serpentinized <span class="hlt">mantle</span> peridotite. These are unique; elsewhere in the Orocopia and related schists, peridotite is rare and completely serpentinized. Peridotite and metaperidotite at Cemetery Ridge are of three principal types: (1) serpentinite and tremolite serpentinite, derived from dunite; (2) partially serpentinized harzburgite and olivine orthopyroxenite (collectively, harzburgite); and (3) granoblastic or schistose metasomatic rocks, derived from serpentinite, made largely of actinolite, calcic plagioclase, hercynite, and chlorite. In the serpentinite, paucity of relict olivine, relatively abundant magnetite (5%), and elevated Fe3+/Fe indicate advanced serpentinization. Harzburgite contains abundant orthopyroxene, only slightly serpentinized, and minor to moderate (1–15%) relict olivine. <span class="hlt">Mantle</span> tectonite fabric is locally preserved. Several petrographic and geochemical characteristics of the peridotite at Cemetery Ridge are ambiguously similar to either abyssal or <span class="hlt">mantle</span>-wedge (suprasubduction) peridotites and serpentinites. Least ambiguous are orthopyroxene compositions. Orthopyroxene is distinctively depleted in Al2O3, Cr2O3, and CaO, indicating <span class="hlt">mantle</span>-wedge affinities. Initial interpretation of field and petrologic data suggests that the peridotite blocks in the Orocopia Schist subduction complex at Cemetery Ridge may be derived from the leading corner or edge of a <span class="hlt">mantle</span> wedge, presumably in (pre-San Andreas fault) southwest California. However, derivation from a subducting plate is not precluded.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70042015','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70042015"><span>The North American upper <span class="hlt">mantle</span>: density, composition, and evolution</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Mooney, Walter D.; Kaban, Mikhail K.</p> <p>2010-01-01</p> <p>The upper <span class="hlt">mantle</span> of North America has been well studied using various seismic methods. Here we investigate the density structure of the North American (NA) upper <span class="hlt">mantle</span> based on the integrative use of the gravity field and seismic data. The basis of our study is the removal of the gravitational effect of the crust to determine the <span class="hlt">mantle</span> gravity anomalies. The effect of the crust is removed in three steps by subtracting the gravitational contributions of (1) topography and bathymetry, (2) low-density sedimentary accumulations, and (3) the three-dimensional density structure of the crystalline crust as determined by seismic observations. Information regarding sedimentary accumulations, including thickness and density, are taken from published maps and summaries of borehole measurements of densities; the seismic structure of the crust is based on a recent compilation, with layer densities estimated from P-wave velocities. The resultant <span class="hlt">mantle</span> gravity anomaly map shows a pronounced negative anomaly (−50 to −400 mGal) beneath western North America and the adjacent oceanic region and positive anomalies (+50 to +350 mGal) east of the NA Cordillera. This pattern reflects the well-known division of North America into the stable eastern region and the tectonically active western region. The close correlation of large-scale features of the <span class="hlt">mantle</span> anomaly map with those of the topographic map indicates that a significant amount of the topographic uplift in western NA is due to buoyancy in the hot upper <span class="hlt">mantle</span>, a conclusion supported by previous investigations. To separate the contributions of <span class="hlt">mantle</span> temperature anomalies from <span class="hlt">mantle</span> compositional anomalies, we apply an additional correction to the <span class="hlt">mantle</span> anomaly map for the thermal structure of the uppermost <span class="hlt">mantle</span>. The thermal model is based on the conversion of seismic shear-wave velocities to temperature and is consistent with <span class="hlt">mantle</span> temperatures that are independently estimated from heat flow and heat production data</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991E%26PSL.107..539L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991E%26PSL.107..539L"><span>A Pan African age for the HP-HT granulite gneisses of Zabargad island: implications for the <span class="hlt">early</span> stages of the Red Sea rifting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lancelot, Joël R.; Bosch, Delphine</p> <p>1991-12-01</p> <p>Up to now the age of granulite gneisses intruded by the Zabargad <span class="hlt">mantle</span> diapir has been an unsolved problem. These gneisses may represent either a part of the adjacent continental crust primarily <span class="hlt">differentiated</span> during the Pan African orogeny, or new crust composed of Miocene clastic sediments deposited in a developing rift, crosscut by a diabase dike swarm and gabbroic intrusions, and finally metamorphosed and deformed by the <span class="hlt">mantle</span> diapir. Previous geochronological results obtained on Zabargad island and Al Lith and Tihama-Asir complexes (Saudi Arabia) suggest an <span class="hlt">Early</span> Miocene age of emplacement for the Zabargad <span class="hlt">mantle</span> diapir during the <span class="hlt">early</span> opening of the Red Sea rift. In contrast, Sm sbnd Nd and Rb sbnd Sr internal isochrons yield Pan African dates for felsic and basic granulites collected 500-600 m from the contact zone with the peridotites. Devoid of evidence for retrograde metamorphic, minerals from a felsic granulite provide well-defined Rb sbnd Sr and Sm sbnd Nd dates of 655 ± 8 and 699 ± 34 Ma for the HP-HT metamorphic event (10 kbar, 850°C). The thermal event related to the diapir emplacement is not recorded in the Sm sbnd Nd and Rb sbnd Sr systems of the studied gneisses; in contrast, the development of a retrograde amphibolite metamorphic paragenesis strongly disturbed the Rb sbnd Sr isotopic system of the mafic granulite. The initial 143Nd/ 144Nd ratio of the felsic granulite is higher than the contemporaneous value for CHUR and is in agreement with other Nd isotopic data for samples of upper crust from the Arabian shield. This result suggests that source rocks of the felsic granulite were derived at 1.0 to 1.2 Ga from either an average MORB-type <span class="hlt">mantle</span> or a local 2.2 Ga LREE-depleted <span class="hlt">mantle</span>. Zabargad gneisses represent a part of the disrupted lower continental crust of the Pan African Afro-Arabian shield. During <span class="hlt">early</span> stages of the Red Sea rifting in the Miocene, these Precambrian granulites were intruded and dragged upwards by a rising peridotite</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMDI34A..01C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMDI34A..01C"><span><span class="hlt">Mantle</span>-driven geodynamo features - accounting for non-thermal lower <span class="hlt">mantle</span> features</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choblet, G.; Amit, H.</p> <p>2011-12-01</p> <p>Lower <span class="hlt">mantle</span> heterogeneity responsible for spatial variations of the CMB heat flux could control long term geodynamo properties such as deviations from axial symmetry in the magnetic field and the core flow, frequency of geomagnetic reversals and anisotropic growth of the inner core. In this context, a classical interpretation of tomographic mapping of the lowermost <span class="hlt">mantle</span> is to correlate linearly seismic velocities to heat flux anomalies. This implicitly assumes that temperature alone controls the tomographic anomalies. In addition, the limited spatial resolution of tomographic images precludes modeling sharp CMB heat flux structures.. There has been growing evidence however that non-thermal origins are also be expected for seismic velocity anomalies: the three main additional control parameters are (i) compositional anomalies possibly associated to the existence of a deep denser layer, (ii) the phase transition in magnesium perovskite believed to occur in the lowermost <span class="hlt">mantle</span> and (iii) the possible presence of partial melts. Numerical models of <span class="hlt">mantle</span> dynamics have illustrated how the first two parameters could distort the linear relationship between shear wave velocity anomalies and CMB heat flux (Nakagawa and Tackley, 2008). In this presentation we will consider the effect of such alternative interpretations of seismic velocity anomalies in order to prescribe CMB heat flux as an outer boundary for dynamo simulations. We first focus on the influence of post-perovskite. Taking into account this complexity could result in an improved agreement between the long term average properties of simulated dynamos and geophysical observations, including the Atlantic/Pacific hemispherical dichotomy in core flow activity, the single intense paleomagnetic field structure in the southern hemisphere, and possibly degree 1 dominant mode of inner-core seismic heterogeneity. We then account for sharp anomalies that are not resolved by the global tomographic probe. For instance</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI41A0331H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI41A0331H"><span>Long-Lived <span class="hlt">Mantle</span> Plumes Sample Multiple Deep <span class="hlt">Mantle</span> Geochemical Domains: The Example of the Hawaiian-Emperor Chain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harrison, L.; Weis, D.</p> <p>2017-12-01</p> <p>Oceanic island basalts provide the opportunity for the geochemist to study the deep <span class="hlt">mantle</span> source removed from continental sources of contamination and, for long-lived systems, the evolution of <span class="hlt">mantle</span> sources with time. In the case of the Hawaiian-Emperor (HE) chain, formation by a long-lived (>81 Myr), deeply-sourced <span class="hlt">mantle</span> plume allows for insight into plume dynamics and deep <span class="hlt">mantle</span> geochemistry. The geochemical record of the entire chain is now complete with analysis of Pb-Hf-Nd-Sr isotopes and elemental compositions of the Northwest Hawaiian Ridge (NWHR), which consists of 51 volcanoes spanning 42 Ma between the bend in the chain and the Hawaiian Islands. This segment of the chain previously represented a significant data gap where Hawaiian plume geochemistry changed markedly, along with magmatic flux: only Kea compositions have been observed on Emperor seamounts (>50 Ma), whereas the Hawaiian Islands (<6 Ma) present both Kea and Loa compositions. A database of 700 Hawaiian Island shield basalts Pb-Hf-Nd-Sr isotopic compositions were compiled to construct a logistical regression model of Loa or Kea affinity that sorts data into a dichotomous category and provides insight into the relationship between independent variables. We use this model to predict whether newly analyzed NWHR samples are Loa or Kea composition based on their Pb-Sr-Nd-Hf isotopic compositions. The logistical regression model is significantly better at prediciting Loa or Kea affinity than the constant only model (χ2=263.3, df=4, p<0.0001), with Pb and Sr isotopes providing the most predicitive power. Daikakuji, West Nihoa, Nihoa, and Mokumanamana erupt Loa-type lavas, suggesting that the Loa source is sampled ephemerally during the NWHR and increases in presence and volume towards the younger section of the NWHR (younger than Midway 20-25 Ma). These results complete the picture of Hawaiian <span class="hlt">mantle</span> plume geochemistry and geodynamics for 81 Myr, and show that the Hawaiian <span class="hlt">mantle</span> plume has</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27872769','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27872769"><span><span class="hlt">Mantle</span> Cell Hyperplasia of Peripheral Lymph Nodes as Initial Manifestation of Sickle Cell Disease.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Monabbati, Ahmad; Noori, Sadat; Safaei, Akbar; Ramzi, Mani; Eghbali, Seyedsajjad; Adib, Ali</p> <p>2016-01-01</p> <p>Sickle cell disease (SCD) is a well known hemoglobinopathy with usual manifestations including anemia, hyperbilirubinemia, and vasoocclusive complications. Despite presence of mild splenomegaly in <span class="hlt">early</span> phase of the disease, lymphadenopathy is not an often finding of SCD. We introduce an undiagnosed case of SCD who presented in third decade of his life with multiple cervical lymphadenopathies and mild splenomegaly persistent for about five years. Histopathologic examination of the resected lymph nodes showed expansion of the <span class="hlt">mantle</span> cell layers of secondary follicles as well as several monomorphic <span class="hlt">mantle</span> cell nodules. To rule out possibility of a malignant process involving lymph nodes, an immunohistochemical panel was ordered which was in favor of benign <span class="hlt">mantle</span> cell hyperplasia. Immunoglobulin gene rearrangement study showed no clonal bands and confirmed benign nature of the process. Respecting mild abnormalities on Complete Blood Count, peripheral blood smear was reviewed revealing some typical sickle red blood cells as well as rare nucleated red blood cells. Solubility test for hemoglobin (HB) S was positive. Hemoglobin electrophoresis confirmed diagnosis of homozygous HbS disease.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoRL..42..290S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoRL..42..290S"><span>Role of <span class="hlt">mantle</span> flow in Nubia-Somalia plate divergence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stamps, D. S.; Iaffaldano, G.; Calais, E.</p> <p>2015-01-01</p> <p>Present-day continental extension along the East African Rift System (EARS) has often been attributed to diverging sublithospheric <span class="hlt">mantle</span> flow associated with the African Superplume. This implies a degree of viscous coupling between <span class="hlt">mantle</span> and lithosphere that remains poorly constrained. Recent advances in estimating present-day opening rates along the EARS from geodesy offer an opportunity to address this issue with geodynamic modeling of the <span class="hlt">mantle</span>-lithosphere system. Here we use numerical models of the global <span class="hlt">mantle</span>-plates coupled system to test the role of present-day <span class="hlt">mantle</span> flow in Nubia-Somalia plate divergence across the EARS. The scenario yielding the best fit to geodetic observations is one where torques associated with gradients of gravitational potential energy stored in the African highlands are resisted by weak continental faults and <span class="hlt">mantle</span> basal drag. These results suggest that shear tractions from diverging <span class="hlt">mantle</span> flow play a minor role in present-day Nubia-Somalia divergence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V53A..01M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V53A..01M"><span>Resolving the potential <span class="hlt">mantle</span> reservoirs that influence volcanism in the West Antarctic Rift System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maletic, E. L.; Darrah, T.</p> <p>2017-12-01</p> <p>Lithospheric extension and magmatism are key characteristics of active continental rift zones and are often associated with long-lasting alkaline magmatic provinces. In these settings, a relationship between lithospheric extension and <span class="hlt">mantle</span> plumes is often assumed for the forces leading to rift evolution and the existence of a plume is commonly inferred, but typically only extension is supported by geological evidence. A prime example of long-lasting magmatism associated with an extensive area of continental rifting is the West Antarctic Rift System (WARS), a 2000 km long zone of ongoing extension within the Antarctic plate. The WARS consists of high alkaline silica-undersaturated igneous rocks with enrichments in light rare earth elements (LREEs). The majority of previous geochemical work on WARS volcanism has focused on bulk classification, modal mineralogy, major element composition, trace element chemistry, and radiogenic isotopes (e.g., Sr, Nd, and Pb isotopes), but very few studies have evaluated volatile composition of volcanics from this region. Previous explanations for WARS volcanism have hypothesized a plume beneath Marie Byrd Land, decompression melting of a fossilized plume head, decompression melting of a stratified <span class="hlt">mantle</span> source, and mixing of recycled oceanic crust with one or more enriched <span class="hlt">mantle</span> sources from the deep <span class="hlt">mantle</span>, though researchers are yet to reach a consensus. Unlike trace elements and radiogenic isotopes which can be recycled between the crust and <span class="hlt">mantle</span> and which are commonly controlled by degrees of partial melting and prior melt <span class="hlt">differentiation</span>, noble gases are present in low concentrations and chemically inert, allowing them to serve as reliable tracers of volatile sources and subsurface processes. Here, we present preliminary noble gas isotope (e.g., 3He/4He, CO2/3He, CH4/3He, 40Ar/36Ar, 40Ar*/4He) data for a suite of lava samples from across the WARS. By coupling major and trace element chemistry with noble gas elemental and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28790325','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28790325"><span>Horizontal <span class="hlt">mantle</span> flow controls subduction dynamics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ficini, E; Dal Zilio, L; Doglioni, C; Gerya, T V</p> <p>2017-08-08</p> <p>It is generally accepted that subduction is driven by downgoing-plate negative buoyancy. Yet plate age -the main control on buoyancy- exhibits little correlation with most of the present-day subduction velocities and slab dips. "West"-directed subduction zones are on average steeper (~65°) than "East"-directed (~27°). Also, a "westerly"-directed net rotation of the lithosphere relative to the <span class="hlt">mantle</span> has been detected in the hotspot reference frame. Thus, the existence of an "easterly"-directed horizontal <span class="hlt">mantle</span> wind could explain this subduction asymmetry, favouring steepening or lifting of slab dip angles. Here we test this hypothesis using high-resolution two-dimensional numerical thermomechanical models of oceanic plate subduction interacting with a <span class="hlt">mantle</span> flow. Results show that when subduction polarity is opposite to that of the <span class="hlt">mantle</span> flow, the descending slab dips subvertically and the hinge retreats, thus leading to the development of a back-arc basin. In contrast, concordance between <span class="hlt">mantle</span> flow and subduction polarity results in shallow dipping subduction, hinge advance and pronounced topography of the overriding plate, regardless of their age-dependent negative buoyancy. Our results are consistent with seismicity data and tomographic images of subduction zones. Thus, our models may explain why subduction asymmetry is a common feature of convergent margins on Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeCoA.185...21J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeCoA.185...21J"><span>Peridotite xenoliths from the Polynesian Austral and Samoa hotspots: Implications for the destruction of ancient 187Os and 142Nd isotopic domains and the preservation of Hadean 129Xe in the modern convecting <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jackson, M. G.; Shirey, S. B.; Hauri, E. H.; Kurz, M. D.; Rizo, H.</p> <p>2016-07-01</p> <p>The Re-Os systematics in 13 peridotite xenoliths hosted in young (<0.39 myr) rejuvenated lavas from the Samoan island of Savai'i and 8 peridotite xenoliths from 6 to 10 myr old lavas from the Austral island of Tubuai have been examined to evaluate the history of the oceanic <span class="hlt">mantle</span> in this region. Modal mineralogy, trace element compositions and 187Os/188Os ratios suggest that these peridotites are not cognate or residual to <span class="hlt">mantle</span> plumes but rather samples of Pacific oceanic lithosphere created at the ridge. Savai'i and Tubuai islands lie along a flow line in the Pacific plate, and provide two snapshots (separated by over 40 Ma in time) of Pacific <span class="hlt">mantle</span> that originated in the same region of the East Pacific rise. Tubuai xenoliths exhibit 187Os/188Os from 0.1163 to 0.1304, and Savai'i (Samoa) xenoliths span a smaller range from 0.1173 to 0.1284. The 187Os/188Os ratios measured in Tubuai xenoliths are lower than (and show no overlap with) basalts from Tubuai. The 187Os/188Os of the Savai'i xenoliths overlap the isotopic compositions of lavas from the island of Savai'i, but also extend to lower 187Os/188Os than the lavas. 3He/4He measurements of a subset of the xenoliths range from 2.5 to 6.4 Ra for Tubuai and 10.8 to 12.4 Ra for Savai'i. Like abyssal peridotites and xenoliths from oceanic hotspots that sample the convecting <span class="hlt">mantle</span>, Os isotopes from the Savai'i and Tubuai xenolith suites are relatively unradiogenic, but do not preserve a record of depleted <span class="hlt">early</span>-formed (Hadean and Archean) <span class="hlt">mantle</span> domains expected from earlier cycles of ridge-related depletion, continent extraction, or subcontinental lithospheric <span class="hlt">mantle</span> erosion. The lack of preservation of <span class="hlt">early</span>-formed, geochemically-depleted Os-isotopic and 142Nd/144Nd domains in the modern convecting <span class="hlt">mantle</span> contrasts with the preservation of <span class="hlt">early</span>-formed (<span class="hlt">early</span>-Hadean) 129Xe/130Xe isotopic heterogeneities in the convecting <span class="hlt">mantle</span>. This can be explained if the initial isotopic signatures in Re-Os and Sm-Nd systems</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CoMP..172...92G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CoMP..172...92G"><span>Incipient boninitic arc crust built on denudated <span class="hlt">mantle</span>: the Khantaishir ophiolite (western Mongolia)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gianola, Omar; Schmidt, Max W.; Jagoutz, Oliver; Sambuu, Oyungerel</p> <p>2017-12-01</p> <p>The 570 Ma old Khantaishir ophiolite is built by up to 4 km harzburgitic <span class="hlt">mantle</span> with abundant pyroxenites and dunites followed by 2 km of hornblende-gabbros and gabbronorites and by a 2.5 km thick volcanic unit composed of a dyke + sill complex capped by pillow lavas and some volcanoclastics. The volcanics are mainly basaltic andesites and andesites (or boninites) with an average of 58.2 ± 1.0 wt% SiO2, X Mg = 0.61 ± 0.03 ( X Mg = molar MgO/(MgO + FeOtot), TiO2 = 0.4 ± 0.1 wt% and CaO = 7.5 ± 0.6 wt% (errors as 2 σ). Normalized trace element patterns show positive anomalies for Pb and Sr, a negative Nb-anomaly, large ion lithophile elements (LILE) concentrations between N- and E-MORB and distinctly depleted HREE. These characteristics indicate that the Khantaishir volcanics were derived from a refractory <span class="hlt">mantle</span> source modified by a moderate slab-component, similar to boninites erupted along the Izu-Bonin-Mariana subduction system and to the Troodos and Betts Cove ophiolites. Most strikingly and despite almost complete outcrops over 260 km2, there is no remnant of any pre-existing MORB crust, suggesting that the magmatic suite of this ophiolite formed on completely denudated <span class="hlt">mantle</span>, most likely upon subduction initiation. The architecture of this 4-5 km thick <span class="hlt">early</span> arc crust resembles oceanic crust formed at mid ocean ridges, but lacks a sheeted dyke complex; volcanic edifices are not observed. Nevertheless, low melting pressures combined with moderate H2O-contents resulted in high-Si primitive melts, in abundant hornblende-gabbros and in a fast enrichment in bulk SiO2. Fractional crystallization modeling starting from the observed primitive melts (56.6 wt% SiO2) suggests that 25 wt% pyroxene + plagioclase fractionation is sufficient to form the average Khantaishir volcanic crust. Most of the fractionation happened in the <span class="hlt">mantle</span>, the observed pyroxenite lenses and layers in and at the top of the harzburgites account for the required cumulate volumes. Finally</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001E%26PSL.186..513P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001E%26PSL.186..513P"><span>187Os-enriched domain in an Archean <span class="hlt">mantle</span> plume: evidence from 2.8 Ga komatiites of the Kostomuksha greenstone belt, NW Baltic Shield</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Puchtel, Igor S.; Brügmann, Gerhard E.; Hofmann, Albrecht W.</p> <p>2001-04-01</p> <p>The Re-Os data on Archean komatiites from the Kostomuksha greenstone belt in the Baltic Shield are presented. This greenstone belt has been previously interpreted to represent a former oceanic plateau formed by the emplacement of an ancient plume head [Puchtel et al., Earth Planet. Sci. Lett. 155 (1998) 57-74]. Samples of flowtop breccia, spinifex-textured and cumulate komatiites and a chromite separate, all collected from the core of a 300 m deep diamond drill hole, yielded a Re-Os isochron with an age of 2795±40 Ma and an initial 187Os/188Os of 0.1117±0.0011 (γ187Os=+3.6±1.0). The high positive γ187Os(T) implies that the komatiites were derived from a <span class="hlt">mantle</span> source with a time-integrated suprachondritic Re/Os ratio. Recycling of oceanic lithosphere to produce the enriched 187Os isotope signature is considered unlikely, as 15-25% crustal component is required to be incorporated into the plume source as <span class="hlt">early</span> as 3.5-4.3 Ga. Such a substantial proportion of mafic material in the source would likely destroy the major and trace element characteristics of the komatiites. Our tentative interpretation is that the 187Os-enrichment in the Kostomuksha plume represents an outer core signature. If confirmed by the ongoing Pt-Os isotope studies, the results would provide evidence for the existence of whole-<span class="hlt">mantle</span> convection in the late Archean, and might place constraints on the timing of core <span class="hlt">differentiation</span> in the <span class="hlt">early</span> Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRB..121.6966H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRB..121.6966H"><span>Identifying <span class="hlt">mantle</span> lithosphere inheritance in controlling intraplate orogenesis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heron, Philip J.; Pysklywec, Russell N.; Stephenson, Randell</p> <p>2016-09-01</p> <p>Crustal inheritance is often considered important in the tectonic evolution of the Wilson Cycle. However, the role of the <span class="hlt">mantle</span> lithosphere is usually overlooked due to its difficulty to image and uncertainty in rheological makeup. Recently, increased resolution in lithosphere imaging has shown potential scarring in continental <span class="hlt">mantle</span> lithosphere to be ubiquitous. In our study, we analyze intraplate deformation driven by <span class="hlt">mantle</span> lithosphere heterogeneities from ancient Wilson Cycle processes and compare this to crustal inheritance deformation. We present 2-D numerical experiments of continental convergence to generate intraplate deformation, exploring the limits of continental rheology to understand the dominant lithosphere layer across a broad range of geological settings. By implementing a "jelly sandwich" rheology, common in stable continental lithosphere, we find that during compression the strength of the <span class="hlt">mantle</span> lithosphere is integral in generating deformation from a structural anomaly. We posit that if the continental <span class="hlt">mantle</span> is the strongest layer within the lithosphere, then such inheritance may have important implications for the Wilson Cycle. Furthermore, our models show that deformation driven by <span class="hlt">mantle</span> lithosphere scarring can produce tectonic patterns related to intraplate orogenesis originating from crustal sources, highlighting the need for a more formal discussion of the role of the <span class="hlt">mantle</span> lithosphere in plate tectonics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI31A2608V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI31A2608V"><span>Investigation of upper <span class="hlt">mantle</span> seismic discontinuities beneath the Indian Ocean using array seismology methods</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Driel, J.; Reiss, A. S.; Thomas, C.</p> <p>2016-12-01</p> <p>The topography of upper <span class="hlt">mantle</span> seismic discontinuities can be used to constrain regional variations in composition and temperature of the Earths <span class="hlt">mantle</span>. The 410 km discontinuity is caused by the solid-solid phase transition from olivine to wadsleyite. Due to its positive Clapeyron slope, the discontinuity is depressed in hot regimes. The phase transition from ringwoodite to bridgemanite and magnesiowüstite in contrast has a negative Clapeyron slope and therefore is elevated when hot material is present. Cold material is expected to yield an opposing topographic signature, culminating in an elevated 410 km and a depressed 660 km discontinuity. As part of the RHUM-RUM project (Réunion Hotspot and Upper <span class="hlt">Mantle</span> - Réunions Unterer Mantel) we extract relevant geophysical parameters, by investigating the properties of upper <span class="hlt">mantle</span> seismic discontinuities beneath the Indian Ocean. The topography of the 410 and 660 km discontinuities, which define the upper and lower bounds of the <span class="hlt">mantle</span> transition zone, have been mapped using PP and SS underside reflections. This study has utilised over 8500 events with Mw ≥ 5.8, distributed over the entire Indian Ocean. Our robust data set yields a dense coverage of points, which are defined by consistently crossing ray paths. Array seismology methods, such as vespagrams and slowness-backazimuth analysis, are used to enhance the signal-to-noise-ratio and detect and identify weak precursor signals. The <span class="hlt">differential</span> travel times are corrected for crustal features and converted into depth values of the discontinuities by comparing the measured travel times with theoretical ones derived from ray tracing through the 1D reference Earth model ak135. A `travel-time' stacking method has also been applied for 4° radius bins around each of the bounce points. The addition of a secondary method derives greater stability of our results and allows an enhanced error analysis procedure. In order to better constrain the mineralogical processes taking</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003PhDT.......181H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003PhDT.......181H"><span>Free and forced convection in Earth's upper <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hall, Paul S.</p> <p></p> <p>Convective motion within Earth's upper <span class="hlt">mantle</span> occurs as a combination of two primary modes: (1) buoyant upwelling due to the formation of gravitational instabilities at thermochemical boundary layers, and (2) passive flow associated with the divergence of lithospheric plates at mid-ocean ridges and their re-entry into the <span class="hlt">mantle</span> at subduction zones. The first mode is driven by variations in density and is therefore classified as 'free' convection. Examples of free convection within the Earth include the diapiric flow of hydrous and/or partially molten <span class="hlt">mantle</span> at subduction zones and <span class="hlt">mantle</span> plumes. The second mode, while ultimately driven by density on a global scale, can be treated kinematically on the scale of the upper <span class="hlt">mantle</span>. This type of flow is designated 'forced' convection. On the scale of individual buoyant upwellings in the upper <span class="hlt">mantle</span>, the forced convection associated with plate tectonics acts to modify the morphology of the flow associated with free convection. Regions in which such interactions occur are typically associated with transfer of significant quantities of both mass and energy (i.e., heat) between the deep interior and the surface of the Earth and thus afford a window into the dynamics of the Earth's interior. The dynamics and the consequences of the interaction between these two modes of convection is the focus of this dissertation. I have employed both laboratory and numerical modeling techniques to investigate the interaction between free and forced convection in this study. Each of these approaches has its own inherent strengths and weaknesses. These approaches are therefore complementary, and their use in combination is particularly powerful. I have focused on two examples interaction between free and forced convection in the upper <span class="hlt">mantle</span> in this study. Chapter I considers the interaction between ascending diapirs of hydrous and/or partially molten <span class="hlt">mantle</span> and flow in the <span class="hlt">mantle</span> wedge at subduction zones using laboratory models. Chapter</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015DPS....4741609S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015DPS....4741609S"><span>Atmospheres of partially <span class="hlt">differentiated</span> super-Earth exoplanets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schaefer, Laura; Sasselov, Dimitar</p> <p>2015-11-01</p> <p>Terrestrial exoplanets have been discovered in a range of sizes, densities and orbital locations that defy our expectations based upon the Solar System. Planets discovered to date with radii less than ~1.5-1.6 Earth radii all seem to fall on an iso-density curve with the Earth [1]. However, mass and radius determinations, which depend on the known properties of the host star, are not accurate enough to distinguish between a fully <span class="hlt">differentiated</span> three-layer planet (core, <span class="hlt">mantle</span>, ocean/atmosphere) and an incompletely <span class="hlt">differentiated</span> planet [2]. Full <span class="hlt">differentiation</span> of a planet will depend upon the conditions at the time of accretion, including the abundance of short-lived radioisotopes, which will vary from system to system, as well as the number of giant impacts the planet experiences. Furthermore, separation of metal and silicates at the much larger pressures found inside super-Earths will depend on how the chemistry of these materials change at high pressures. There are therefore hints emerging that not all super-Earths will be fully <span class="hlt">differentiated</span>. Incomplete <span class="hlt">differentiation</span> will result in a more reduced <span class="hlt">mantle</span> oxidation state and may have implications for the composition of an outgassed atmosphere. Here we will present the first results from a chemical equilibrium model of the composition of such an outgassed atmosphere and discuss the possibility of distinguishing between fully and incompletely <span class="hlt">differentiated</span> planets through atmospheric observations.[1] Rogers, L. 2015. ApJ, 801, 41. [2] Zeng, L. & Sasselov, D. 2013. PASP, 125, 227.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1813620B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1813620B"><span>Compositional layering within the large low shear-wave velocity provinces (LLSVPs) in the lower <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ballmer, Maxim; Lekic, Vedran; Schumacher, Lina; Ito, Garrett; Thomas, Christine</p> <p>2016-04-01</p> <p>Seismic tomography reveals two antipodal LLSVPs in the Earth's <span class="hlt">mantle</span>, each extending from the core-<span class="hlt">mantle</span> boundary (CMB) up to ~1000 km depth. The LLSVPs are thought to host primordial <span class="hlt">mantle</span> materials that bear witness of <span class="hlt">early</span>-Earth processes, and/or subducted basalt that has accumulated in the <span class="hlt">mantle</span> over billions of years. A compositional distinction between the LLSVPs and the ambient <span class="hlt">mantle</span> is supported by anti-correlation of bulk-sound and shear-wave velocity (Vs) anomalies as well as abrupt lateral gradients in Vs along LLSVP margins. Both of these observations, however, are mainly restricted to the LLSVP bottom domains (2300~2900 km depth), or hereinafter referred to as "deep distinct domains" (DDD). Seismic sensitivity calculations suggest that DDDs are more likely to be composed of primordial <span class="hlt">mantle</span> material than of basaltic material. On the other hand, the seismic signature of LLSVP shallow domains (1000~2300 km depth) is consistent with a basaltic composition, though a purely thermal origin cannot be ruled out. Here, we explore the dynamical, seismological, and geochemical implications of the hypothesis that the LLSVPs are compositionally layered with a primordial bottom domain (or DDD) and a basaltic shallow domain. We test this hypothesis using 2D thermochemical <span class="hlt">mantle</span>-convection models. Depending on the density difference between primordial and basaltic materials, the materials either mix or remain separate as they join to form thermochemical piles in the deep <span class="hlt">mantle</span>. Separation of both materials within these piles provides an explanation for LLSVP seismic properties, including substantial internal vertical gradients in Vs observed at 400-700 km height above the CMB, as well as out-of-plane reflections on LLSVP sides over a range of depths. Predicted geometry of thermochemical piles is compared to LLSVP and DDD shapes as constrained by seismic cluster analysis. Geodynamic models predict short-lived "secondary" plumelets to rise from LLSVP roofs and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.V51B2521P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.V51B2521P"><span>The Xenon record of Earth's <span class="hlt">early</span> differentiaiton</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peto, M. K.; Mukhopadhyay, S.; Kelley, K. A.</p> <p>2011-12-01</p> <p>Xenon isotopes in <span class="hlt">mantle</span> derived rocks provide information on the <span class="hlt">early</span> <span class="hlt">differentiation</span> of the silicate <span class="hlt">mantle</span> of our planet. {131,132 134,136}Xe isotopes are produced by the spontaneous fission of two different elements: the now extinct radionuclide 244Pu, and the long-lived 238U. These two parent nuclides, however, yield rather different proportion of fissiogenic Xenon isotopes. Hence, the proportion of Pu- to U-derived fission xenon is indicative of the degree and rate of outgassing of a <span class="hlt">mantle</span> reservoir. Recent data obtained from Iceland in our lab confirm that the Xenon isotopic composition of the plume source(s) is characterized by lower 136Xe/130Xe ratios than the MORB source and the Iceland plume is more enriched in the Pu-derived Xenon component. These features are interpreted as reflecting different degrees of outgassing and appear not to be the result of preferential recycling of Xenon to the deep <span class="hlt">mantle</span>. To further investigate how representative the Icelandic measurements might be of other <span class="hlt">mantle</span> plumes, we measured noble gases (He, Ne, Ar, Xe) in gas-rich basalt glasses from the Rochambeau Ridge (RR) in the Northern Lau Basin. Recent work suggests the presence of a "Samoan-like" OIB source in the northern Lau Basin and our measurements were performed on samples with plume-like 3He/4He ratios (15-28 RA) [1]. The Xenon isotopic measurements indicate that the maximum measured 136Xe/130Xe ratios in the Rochambeau samples are similar to Iceland. In particular, for one of the gas rich samples we were able to obtain 77 different isotopic measurements through step-crushing. Preliminary investigation of this sample suggests higher Pu- to U-derived fission Xenon than in MORBs. To quantitatively evaluate the degree and rate of outgassing of the plume and MORB reservoirs, particularly during the first few hundred million years of Earth's history, we have modified a geochemical reservoir model that was previously developed to investigate <span class="hlt">mantle</span> overturn and mixing</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4991929','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4991929"><span>Can <span class="hlt">mantle</span> convection be self-regulated?</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Korenaga, Jun</p> <p>2016-01-01</p> <p>The notion of self-regulating <span class="hlt">mantle</span> convection, in which heat loss from the surface is constantly adjusted to follow internal radiogenic heat production, has been popular for the past six decades since Urey first advocated the idea. Thanks to its intuitive appeal, this notion has pervaded the solid earth sciences in various forms, but approach to a self-regulating state critically depends on the relation between the thermal adjustment rate and <span class="hlt">mantle</span> temperature. I show that, if the effect of <span class="hlt">mantle</span> melting on viscosity is taken into account, the adjustment rate cannot be sufficiently high to achieve self-regulation, regardless of the style of <span class="hlt">mantle</span> convection. The evolution of terrestrial planets is thus likely to be far from thermal equilibrium and be sensitive to the peculiarities of their formation histories. Chance factors in planetary formation are suggested to become more important for the evolution of planets that are more massive than Earth. PMID:27551689</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V22B..01H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V22B..01H"><span>Geochemical Diversity of the <span class="hlt">Mantle</span>: 50 Years of Acronyms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hart, S. R.</p> <p>2014-12-01</p> <p>50 years ago, Gast, Tilton and Hedge demonstrated that the oceanic <span class="hlt">mantle</span> is isotopically heterogeneous. 28 years ago, Zindler and Hart formalized the concept of geochemical <span class="hlt">mantle</span> components, with an attendant, to some, odious, acronym soup. Work on a marriage of <span class="hlt">mantle</span> geochemistry and dynamics continues unabated. We know unequivocally that the <span class="hlt">mantle</span> is chemically heterogeneous; we do not know the scale lengths of these heterogeneities. We know unequivocally that these heterogeneities have persisted for eons (Gy); we do not know where they were formed or where they are stored. Through the kind auspices of the Plume Model, we plausibly have access to the whole <span class="hlt">mantle</span>. The most accessible and well understood <span class="hlt">mantle</span> reservoir is the upper depleted MORB <span class="hlt">mantle</span> (DMM). Classically, this <span class="hlt">mantle</span> was depleted by extraction of oceanic and continental crust from a "chondritic" bulk silicate Earth. In this post-Boyet and Carlson world, the complementary enriched reservoir may instead be hidden in the deepest <span class="hlt">mantle</span>. In this case, DMM will become an endangered acronym. Hofmann and White (1982) argued that radiogenic Pb <span class="hlt">mantle</span> (HIMU) is re-cycled ocean crust, and this is a comfortably viable model. It does require some ad hoc chemical manipulations during subduction. Given 2 Gy of aggregate <span class="hlt">mantle</span> strains, the mafic component in HIMU may be of small length scale (< 50 m), possibly subsumed into the dominant peridotitic lithology. This <span class="hlt">mantle</span> species is globally widespread. Enriched <span class="hlt">mantles</span> (EM1 and EM2) almost certainly reflect recycling of enriched continental material. This was splendidly verified by Jackson et al (2007), with 87Sr/86Sr in Samoan EM2 lavas up to 0.721. The lithology and length scale of EM1 and EM2 is unconstrained. EM1 is globally present; EM2 is confined to the SW Pacific hotspots. FOZO is a work in progress; many would like to see it become extinct! The trace element signatures of HIMU and FOZO <span class="hlt">mantles</span> have been constrained using melting models; in both</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.V13E..02W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.V13E..02W"><span>Tracing <span class="hlt">mantle</span> processes with Fe isotopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weyer, S.; Ionov, D.</p> <p>2006-12-01</p> <p>High precision Fe isotope measurements have been performed on various <span class="hlt">mantle</span> peridotites (fertile lherzolites, harzburgites, metasomatised Fe-enriched rocks) and volcanic rocks (mainly oceanic basalts) from different localities and tectonic settings. Pimitive peridotites (Mg# = 0.894) yield delta56Fe = 0.02 and are significantly lighter than the basalts (average delta56Fe = 0.11). Furthermore, the peridotites display a negative correlation of iron isotopes with Mg#. Taken together, these findings imply that Fe isotopes fractionate during partial melting, with heavy isotopes preferentially entering the melt [1, 2]. A particularly good correlation of the Fe isotope composition and Mg# shown by poorly metasomatised spinel lherzolites of three localities (Horoman, Kamchatka and Lherz) was used to model Fe isotope fractionation during partial melting, resulting in alphamantle-melt = 1.0003. This value implies higher Fe isotope fractionation between residual <span class="hlt">mantle</span> and <span class="hlt">mantle</span>-derived melts (i.e. Delta56Femantle-melt = 0.2-0.3) than the observed difference between the peridotites and the basalts in this study. Our data on plagioclase lherzolites from Horoman and spinel lherzolites from other localities indicate that the difference in Fe isotope composition between <span class="hlt">mantle</span> and basalts may be reduced by partial re-equilibration between the isotopically heavy basalts and the isotopically light depleted lithospheric <span class="hlt">mantle</span> during melt ascent. Besides partial melting, the Fe isotope composition of <span class="hlt">mantle</span> peridotites can also be significantly modified by metasomatic events. At two localities (Tok, Siberia and Tariat, Mongolia) Fe isotopes correlates with the Fe concentration of the peridotites, which was increased up to 14.5% FeO by melt percolation. Such processes can be accompanied by chromatographic effects and produce a range of Fe isotope compositions in the percolation columns, from extremely light to heavy (delta56Fe = -0.42 to +0.17). We propose that Fe isotopes can be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890054376&hterms=convection+currents&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dconvection%2Bcurrents','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890054376&hterms=convection+currents&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dconvection%2Bcurrents"><span>Three-dimensional spherical models of convection in the earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bercovici, Dave; Schubert, Gerald; Glatzmaier, Gary A.</p> <p>1989-01-01</p> <p>Three-dimensional spherical models of <span class="hlt">mantle</span> convection in the earth reveal that upwelling cylindrical plumes and downwelling planar sheets are the primary features of <span class="hlt">mantle</span> circulation. Thus subduction zones and descending sheetlike slabs in the <span class="hlt">mantle</span> are fundamental characteristics of thermal convection in a spherical shell and are not merely the consequences of the rigidity of the slabs, which are cooler than the surrounding <span class="hlt">mantle</span>. Cylindrical <span class="hlt">mantle</span> plumes that cause hot spots such as Hawaii are probably the only form of active upwelling and are therefore not just secondary convective currents separate from the large-scale <span class="hlt">mantle</span> circulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI23A0413C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI23A0413C"><span>Structure of Lithospheric and Upper <span class="hlt">Mantle</span> Discontinuities beneath Central Mongolia from Receiver Functions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cui, Z.; Meltzer, A.; Fischer, K. M.; Stachnik, J. C.; Munkhuu, U.; Tsagaan, B.; Russo, R. M.</p> <p>2017-12-01</p> <p>The origin and preservation of high-elevation low-relief surfaces in continental interiors remains an open questions. Central Mongolia constitutes a major portion of the Mongolian Plateau and is an excellent place to link deep earth and surface processes. The lithosphere of Mongolia was constructed through accretionary orogenesis associated with the Central Asian Orogenic Belt (CAOB) from the late Paleozoic to the <span class="hlt">early</span> Triassic. Alkaline volcanic basalt derived from sublithospheric sources has erupted sporadically in Mongolia since 30 Ma. Constraining the depth variation of lithospheric and upper <span class="hlt">mantle</span> discontinuities is crucial for understanding the interaction between upper <span class="hlt">mantle</span> structure and surface topography. We conducted receiver functions (RF) analyses suitable data recorded at112 seismic broadband stations in central Mongolia to image the LAB and <span class="hlt">mantle</span> transition zone beneath Central Mongolia. A modified H-κ stacking was performed to determine crustal average thickness (H) and Vp/Vs ratio (κ). Central Mongolia is characterized by thick crust (43-57 km) enabling use of both P wave RF and to S wave RF to image the LAB. The PRF traces in the depth domain are stacked based on piercing point locations for the 410 and 660 discontinuities using 0.6 ° × 0.6 ° bins in a grid. From south to north, the average lithospheric thickness is 85km in Gobi Altai gradually thinning northeastward to 78km in the southern Hangay Dome, 72 km in the northern Hangay Dome then increases to 75km in Hovsgol area. While there is overall thinning of the lithosphere from SW to NE, beneath the Hangay, there is a slight increase beneath the highest topography. The thickness of the <span class="hlt">mantle</span> transition zone (MTZ) beneath central Mongolia is similar to global averages. This evidence argues against the hypothesis that a <span class="hlt">mantle</span> plume exists beneath Central Mongolia causing low velocity anomalies in the upper <span class="hlt">mantle</span>. To the east of the Hovsgol area in northern Mongolia, the MTZ thickens</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19570930','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19570930"><span><span class="hlt">Differentiating</span> <span class="hlt">early</span>-onset persistent versus childhood-limited conduct problem youth.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barker, Edward D; Maughan, Barbara</p> <p>2009-08-01</p> <p>Among young children who demonstrate high levels of conduct problems, less than 50% will continue to exhibit these problems into adolescence. Such developmental heterogeneity presents a serious challenge for intervention and diagnostic screening in <span class="hlt">early</span> childhood. The purpose of the present study was to inform diagnostic screening and preventive intervention efforts by identifying youths whose conduct problems persist. The authors examined 1) the extent to which <span class="hlt">early</span>-onset persistent versus childhood-limited trajectories can be identified from repeated assessments of childhood and <span class="hlt">early</span>-adolescent conduct problems and 2) how prenatal and <span class="hlt">early</span> postnatal risks <span class="hlt">differentiate</span> these two groups. To identify heterogeneity in <span class="hlt">early</span>-onset conduct problems, the authors used data from a large longitudinal population-based cohort of children followed from the prenatal period to age 13. Predictive risk factors examined were prenatal and postnatal measures of maternal distress (anxiety, depression), emotional and practical support, and family and child characteristics (from birth to 4 years of age). Findings revealed a distinction between <span class="hlt">early</span>-onset persistent versus childhood-limited conduct problems in youths. Robust predictors of the <span class="hlt">early</span>-onset persistent trajectory were maternal anxiety during pregnancy (32 weeks gestation), partner cruelty to the mother (from age 0 to 4 years), harsh parenting, and higher levels of child undercontrolled temperament. Sex differences in these risks were not identified. Interventions aiming to reduce childhood conduct problems should address prenatal risks in mothers and <span class="hlt">early</span> postnatal risks in both mothers and their young children.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70036519','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70036519"><span><span class="hlt">Mantle</span> to surface degassing of alkalic magmas at Erebus volcano, Antarctica</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Oppenheimer, C.; Moretti, R.; Kyle, P.R.; Eschenbacher, A.; Lowenstern, J. B.; Hervig, R.L.; Dunbar, N.W.</p> <p>2011-01-01</p> <p>Continental intraplate volcanoes, such as Erebus volcano, Antarctica, are associated with extensional tectonics, <span class="hlt">mantle</span> upwelling and high heat flow. Typically, erupted magmas are alkaline and rich in volatiles (especially CO2), inherited from low degrees of partial melting of <span class="hlt">mantle</span> sources. We examine the degassing of the magmatic system at Erebus volcano using melt inclusion data and high temporal resolution open-path Fourier transform infrared (FTIR) spectroscopic measurements of gas emissions from the active lava lake. Remarkably different gas signatures are associated with passive and explosive gas emissions, representative of volatile contents and redox conditions that reveal contrasting shallow and deep degassing sources. We show that this unexpected degassing signature provides a unique probe for magma <span class="hlt">differentiation</span> and transfer of CO2-rich oxidised fluids from the <span class="hlt">mantle</span> to the surface, and evaluate how these processes operate in time and space. Extensive crystallisation driven by CO2 fluxing is responsible for isobaric fractionation of parental basanite magmas close to their source depth. Magma deeper than 4kbar equilibrates under vapour-buffered conditions. At shallower depths, CO2-rich fluids accumulate and are then released either via convection-driven, open-system gas loss or as closed-system slugs that ascend and result in Strombolian eruptions in the lava lake. The open-system gases have a reduced state (below the QFM buffer) whereas the closed-system gases preserve their deep oxidised signatures (close to the NNO buffer). ?? 2011 Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Alzheimer+AND+characteristics&id=EJ769184','ERIC'); return false;" href="https://eric.ed.gov/?q=Alzheimer+AND+characteristics&id=EJ769184"><span>The Potential of Gait Analysis to Contribute to <span class="hlt">Differential</span> Diagnosis of <span class="hlt">Early</span> Stage Dementia: Current Research and Future Directions</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Morgan, Debra; Funk, Melanie; Crossley, Margaret; Basran, Jenny; Kirk, Andrew; Bello-Haas, Vanina Dal</p> <p>2007-01-01</p> <p><span class="hlt">Early</span> <span class="hlt">differential</span> diagnosis of dementia is becoming increasingly important as new pharmacologic therapies are developed, as these treatments are not equally effective for all types of dementia. <span class="hlt">Early</span> detection and <span class="hlt">differential</span> diagnosis also facilitates informed family decision making and timely access to appropriate services. Information about…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.1046K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.1046K"><span>Mesoproterozoic orangeites of Karelia (Kostomuksha-Lentiira): evidence for composition of <span class="hlt">mantle</span> lithosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kargin, Alexey; Nosova, Anna; Larionova, Yulia; Kononova, Voctoria; Borisovskiy, Sergey; Kovalchuk, Elena; Griboedova, Irina</p> <p>2014-05-01</p> <p>The 1.23-1.20 Ga old diamondiferous lamproites and orangeites (kimberlites of II group) of the Kostomuksha-Taloveys and the Lentiira-Kuhmo dyke fields intrude the Archaean crust of the Karelian craton, NE of the East European Platform. Mineral (a trend of compositional evolution of mica, presence of carbonate minerals in basis, composition of olivine) and geochemical (major elements, ratio of trace elements, primitive <span class="hlt">mantle</span> normalized trace elements patterns) characteristics of these rocks suggest an orangeitic rather than lamproitic or lamprophyric nature. The composition of Phl-Ol orangeites suggests intensive processes of fractional crystallization for their melts. Cpx-Phl-Ol orangeites indicate higher intensity of lithospheric <span class="hlt">mantle</span> assimilation then other orangeitic types. Phl-Carb orangeites of the Taloveys area and Cpx-Phl-Ol one of the Lentiira area are closest to primary melts. The Ol-Phl-Cpx orangeites of the Lentiira area contain three generations of unaltered olivine that vary in composition and origin: a) xenocryst derived from depleted <span class="hlt">mantle</span> peridotite; b) orangeitic olivine phenocryst and c) and olivine like <span class="hlt">early</span> stage crystallization of megacryst assemblage or a product of metasomatic interaction between <span class="hlt">mantle</span> peridotite and protokimberlitic melt. Orangeites of Kostomuksha-Lentiira have low- and medium-radiogenic value of (87Sr/86Sr)1200 that range from 0.7038 to 0.7067. Phl-Carb orangeites of Taloveys have less radiogenic isotopic composition of Nd (eNd -11 ... -12) then Cpx-Phl-Ol and Phl-Ol orangeites of Kostomuksha (eNd -6.9 ... -9.4). The study of Sm-Nd and Rb-Sr isotopic systems suggests that an ancient metasomatic <span class="hlt">mantle</span> source took part in origin of orangeites. We propose a two-steps model of origin of their source (Kargin et al., 2014): 1) The metasomatic component of <span class="hlt">mantle</span> source (like as MARID-type veins) formed during Lapland-Kola and/or Svecofennian orogeny events (2.1-1.8 Ga ago). 2) The intrusion of orangeites is comparable by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI11A0268S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI11A0268S"><span>The Presence of Dense Material in the Deep <span class="hlt">Mantle</span>: Implications for Plate Motion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stein, C.; Hansen, U.</p> <p>2017-12-01</p> <p>The dense material in the deep <span class="hlt">mantle</span> strongly interacts with the convective flow in the <span class="hlt">mantle</span>. On the one hand, it has a restoring effect on rising plumes. On the other hand, the dense material is swept about by the flow forming dense piles. Consequently this affects the plate motion and, in particular, the onset time and the style of plate tectonics varies considerably for different model scenarios. In this study we apply a thermochemical <span class="hlt">mantle</span> convection model combined with a rheological model (temperature- and stress-dependent viscosity) that allows for plate formation according to the convective flow. The model's starting condition is the post-magma ocean period. We analyse a large number of model scenarios ranging from variations in thickness, density and depth of a layer of dense material to different initial temperatures.Furthermore, we present a mechanism in which the dense layer at the core-<span class="hlt">mantle</span> boundary forms without prescribing the thickness or the density contrast. Due to advection-assisted diffusion, long-lived piles can be established that act on the style of convection and therefore on plate motion. We distinguish between the subduction-triggered regime with <span class="hlt">early</span> plate tectonics and the plume-triggered regime with a late onset of plate tectonics. The formation of piles by advection-assisted diffusion is a typical phenomenon that appears not only at the lower boundary, but also at internal boundaries that form in the layering phase during the evolution of the system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Litho.276....1N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Litho.276....1N"><span>European Lithospheric <span class="hlt">Mantle</span>; geochemical, petrological and geophysical processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ntaflos, Th.; Puziewicz, J.; Downes, H.; Matusiak-Małek, M.</p> <p>2017-04-01</p> <p>The second European <span class="hlt">Mantle</span> Workshop occurred at the end of August 2015, in Wroclaw, Poland, attended by leading scientists in the study the lithospheric <span class="hlt">mantle</span> from around the world. It built upon the results of the first European <span class="hlt">Mantle</span> Workshop (held in 2007, in Ferrara, Italy) published in the Geological Society of London Special Publication 293 (Coltorti & Gregoire, 2008).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920033271&hterms=ATLA&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DATLA','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920033271&hterms=ATLA&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DATLA"><span>A <span class="hlt">mantle</span> plume model for the Equatorial Highlands of Venus</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kiefer, Walter S.; Hager, Bradford H.</p> <p>1991-01-01</p> <p>The possibility that the Equatorial Highlands are the surface expressions of hot upwelling <span class="hlt">mantle</span> plumes is considered via a series of <span class="hlt">mantle</span> plume models developed using a cylindrical axisymmetric finite element code and depth-dependent Newtonian rheology. The results are scaled by assuming whole <span class="hlt">mantle</span> convection and that Venus and the earth have similar <span class="hlt">mantle</span> heat flows. The best model fits are for Beta and Atla. The common feature of the allowed viscosity models is that they lack a pronounced low-viscosity zone in the upper <span class="hlt">mantle</span>. The shape of Venus's long-wavelength admittance spectrum and the slope of its geoid spectrum are also consistent with the lack of a low-viscosity zone. It is argued that the lack of an asthenosphere on Venus is due to the <span class="hlt">mantle</span> of Venus being drier than the earth's <span class="hlt">mantle</span>. <span class="hlt">Mantle</span> plumes may also have contributed to the formation of some smaller highland swells, such as the Bell and Eistla regions and the Hathor/Innini/Ushas region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.V14B..03T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.V14B..03T"><span>Magnesium isotopic composition of the <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Teng, F.; Li, W.; Ke, S.; Marty, B.; Huang, S.; Dauphas, N.; Wu, F.; Helz, R. L.</p> <p>2009-12-01</p> <p>Studies of Mg isotopic composition of the Earth not only are important for understanding its geochemistry but also can shed light on the accretion history of the Earth as well as the evolution of the Earth-Moon system. However, to date, the Mg isotopic composition of the Earth is still poorly constrained and highly debated. There is uncertainty in the magnitude of Mg isotope fractionation at <span class="hlt">mantle</span> temperatures and whether the Earth has a chondritic Mg isotopic composition or not. To constrain further the Mg isotopic composition of the <span class="hlt">mantle</span> and investigate the behavior of Mg isotopes during igneous <span class="hlt">differentiation</span>, we report >200 high-precision (δ26Mg < 0.1‰, 2SD) analyses of Mg isotopes on 1) global mid-ocean ridge basalts covering major ridge segments of the world and spanning a broad range in latitudes, chemical and radiogenic isotopic compositions; 2) ocean island basalts from Hawaiian (Koolau, Kilauea and Loihi) and French Polynesian volcanoes (Society island and Cook Austral chain); 3) olivine grains from Hawaiian volcanoes (Kilauea, Koolau and Loihi) and 4) peridotite xenoliths from Australia, China, France, Tanzania and USA. Global oceanic basalts and peridotite xenoliths have a limited (<0.2 ‰) variation in Mg isotopic composition, with an average δ26Mg = -0.25 relative to DSM3. Olivines from Hawaiian lavas have δ26Mg ranging from -0.43 to +0.03, with most having compositions identical to basalts and peridotites. Therefore, the mantle’s δ26Mg value is estimated to be ~ -0.25 ± 0.1 (2SD), different from that reported by Wiechert and Halliday (2007; δ26Mg = ~ 0) but similar to more recent studies (δ26Mg = -0.27 to -0.33) (Teng et al. 2007; Handler et al. 2009; Yang et al., 2009). Moreover, we suggest the Earth, as represented by the <span class="hlt">mantle</span>, has a Mg isotopic composition similar to chondrites (δ26Mg = ~-0.33). The need for a model such as that of Wiechert and Halliday (2007) that involves sorting of chondrules and calcium</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70024302','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70024302"><span>Upper-<span class="hlt">mantle</span> origin of the Yellowstone hotspot</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Christiansen, R.L.; Foulger, G.R.; Evans, J.R.</p> <p>2002-01-01</p> <p>Fundamental features of the geology and tectonic setting of the northeast-propagating Yellowstone hotspot are not explained by a simple deep-<span class="hlt">mantle</span> plume hypothesis and, within that framework, must be attributed to coincidence or be explained by auxiliary hypotheses. These features include the persistence of basaltic magmatism along the hotspot track, the origin of the hotspot during a regional middle Miocene tectonic reorganization, a similar and coeval zone of northwestward magmatic propagation, the occurrence of both zones of magmatic propagation along a first-order tectonic boundary, and control of the hotspot track by preexisting structures. Seismic imaging provides no evidence for, and several contraindications of, a vertically extensive plume-like structure beneath Yellowstone or a broad trailing plume head beneath the eastern Snake River Plain. The high helium isotope ratios observed at Yellowstone and other hotspots are commonly assumed to arise from the lower <span class="hlt">mantle</span>, but upper-<span class="hlt">mantle</span> processes can explain the observations. The available evidence thus renders an upper-<span class="hlt">mantle</span> origin for the Yellowstone system the preferred model; there is no evidence that the system extends deeper than ???200 km, and some evidence that it does not. A model whereby the Yellowstone system reflects feedback between upper-<span class="hlt">mantle</span> convection and regional lithospheric tectonics is able to explain the observations better than a deep-<span class="hlt">mantle</span> plume hypothesis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.P44A..06W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.P44A..06W"><span>Volcanism on <span class="hlt">differentiated</span> asteroids (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wilson, L.</p> <p>2013-12-01</p> <p>The Dawn spacecraft's investigation of 4 Vesta, best-preserved of the <span class="hlt">early</span>-forming <span class="hlt">differentiated</span> asteroids, prompts a reappraisal of factors controlling igneous activity on such bodies. Analogy with melt transfer in zones of partial melting on Earth implies that silicate melts moved efficiently within asteroid <span class="hlt">mantles</span> in complex networks of veins and dikes, so that only a few percent of the <span class="hlt">mantle</span> consisted of melt at any one time. Thus even in cases where large amounts of <span class="hlt">mantle</span> melting occurred, the melts did not remain in the <span class="hlt">mantle</span> to form "magma oceans", but instead migrated to shallow depths. The link between magma flow rate and the stresses needed to keep fractures open and allow flow fast enough to avoid excessive cooling implies that only within asteroids with radii more than ~190-250 km would continuous magma flow from <span class="hlt">mantle</span> to surface be possible. In all smaller asteroids (including Vesta) magma must have accumulated in sills at the base of the lithosphere (the conductively controlled ~10 km thick thermal boundary layer) or in crustal magma reservoirs near its base. Magma would then have erupted intermittently to the surface from these steadily replenished reservoirs. The average rates of eruption to the surface (or shallow intrusion) should balance the magma production rate, but since magma could accumulate and erupt intermittently from these reservoirs, the instantaneous eruption rates could be hundreds to thousands of cubic m/s, comparable to historic basaltic eruption rates on Earth and very much greater than the average <span class="hlt">mantle</span> melting rate. The absence of asteroid atmospheres makes explosive eruptions likely even if magmas are volatile-poor. On asteroids with radii less than ~100 km, gases and sub-mm pyroclastic melt droplets would have had speeds exceeding the escape speed assuming a few hundred ppm volatiles, and only cm sized or larger clasts would have been retained. On larger bodies almost all pyroclasts will have returned to the surface</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22364075-vigor-mantle-convection-super-earths','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22364075-vigor-mantle-convection-super-earths"><span>ON THE VIGOR OF <span class="hlt">MANTLE</span> CONVECTION IN SUPER-EARTHS</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Miyagoshi, Takehiro; Tachinami, Chihiro; Kameyama, Masanori</p> <p>2014-01-01</p> <p>Numerical models are presented to clarify how adiabatic compression affects thermal convection in the <span class="hlt">mantle</span> of super-Earths ten times the Earth's mass. The viscosity strongly depends on temperature, and the Rayleigh number is much higher than that of the Earth's <span class="hlt">mantle</span>. The strong effect of adiabatic compression reduces the activity of <span class="hlt">mantle</span> convection; hot plumes ascending from the bottom of the <span class="hlt">mantle</span> lose their thermal buoyancy in the middle of the <span class="hlt">mantle</span> owing to adiabatic decompression, and do not reach the surface. A thick lithosphere, as thick as 0.1 times the depth of the <span class="hlt">mantle</span>, develops along the surface boundary, and themore » efficiency of convective heat transport measured by the Nusselt number is reduced by a factor of about four compared with the Nusselt number for thermal convection of incompressible fluid. The strong effect of adiabatic decompression is likely to inhibit hot spot volcanism on the surface and is also likely to affect the thermal history of the <span class="hlt">mantle</span>, and hence, the generation of magnetic field in super-Earths.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010GeCoA..74.3274D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010GeCoA..74.3274D"><span>Magnesium and iron isotopes in 2.7 Ga Alexo komatiites: <span class="hlt">Mantle</span> signatures, no evidence for Soret diffusion, and identification of diffusive transport in zoned olivine</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dauphas, Nicolas; Teng, Fang-Zhen; Arndt, Nicholas T.</p> <p>2010-06-01</p> <p>Komatiites from Alexo, Canada, are well preserved and represent high-degree partial <span class="hlt">mantle</span> melts (˜50%). They are thus well suited for investigating the Mg and Fe isotopic compositions of the Archean <span class="hlt">mantle</span> and the conditions of magmatic <span class="hlt">differentiation</span> in komatiitic lavas. High precision Mg and Fe isotopic analyses of 22 samples taken along a 15-m depth profile in a komatiite flow are reported. The δ 25Mg and δ 26Mg values of the bulk flow are -0.138 ± 0.021‰ and -0.275 ± 0.042‰, respectively. These values are indistinguishable from those measured in <span class="hlt">mantle</span> peridotites and chondrites, and represent the best estimate of the composition of the silicate Earth from analysis of volcanic rocks. Excluding the samples affected by secondary Fe mobilization, the δ 56Fe and δ 57Fe values of the bulk flow are +0.044 ± 0.030‰, and +0.059 ± 0.044‰, respectively. These values are consistent with a near-chondritic Fe isotopic composition of the silicate Earth and minor fractionation during komatiite magma genesis. In order to explain the <span class="hlt">early</span> crystallization of pigeonite relative to augite in slowly cooled spinifex lavas, it was suggested that magmas trapped in the crystal mush during spinifex growth <span class="hlt">differentiated</span> by Soret effect, which should be associated with large and coupled variations in the isotopic compositions of Mg and Fe. The lack of variations in Mg and Fe isotopic ratios either rules out the Soret effect in the komatiite flow or the effect is effaced as the solidification front migrates downward through the flow crust. Olivine separated from a cumulate sample has light δ 56Fe and slightly heavy δ 26Mg values relative to the bulk flow, which modeling shows can be explained by kinetic isotope fractionation associated with Fe-Mg inter-diffusion in olivine. Such variations can be used to identify diffusive processes involved in the formation of zoned minerals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/993696','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/993696"><span>Receptor units responding to movement in the octopus <span class="hlt">mantle</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Boyle, P R</p> <p>1976-08-01</p> <p>1. A preparation of the <span class="hlt">mantle</span> of Octopus which is inverted over a solid support and which exposes the stellate ganglion and associated nerves is described. 2. Afferent activity can be recorded from stellar nerves following electrical stimulation of the pallial nerve. The latency and frequency of the phasic sensory response is correlated with the contraction of the <span class="hlt">mantle</span> musculature. 3. It is proposed that receptors cells located in the muscle, and their activity following <span class="hlt">mantle</span> contraction, form part of a sensory feedback system in the <span class="hlt">mantle</span>. Large, multipolar nerve cells that were found between the two main layers of circular muscle in the <span class="hlt">mantle</span> could be such receptors.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1610266P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1610266P"><span>The basal part of the Oman ophiolitic <span class="hlt">mantle</span>: a fossil <span class="hlt">Mantle</span> Wedge?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prigent, Cécile; Guillot, Stéphane; Agard, Philippe; Godard, Marguerite; Chauvet, Alain; Dubacq, Benoit; Monié, Patrick; Yamato, Philippe</p> <p>2014-05-01</p> <p>Although the Oman ophiolite is classically regarded as being the direct analog of oceanic lithosphere created at fast spreading ridges, the geodynamic context of its formation is still highly debated. The other alternative end-member model suggests that this ophiolite entirely formed in a supra-subduction zone setting. Fluids involved in the hydration of the oceanic lithosphere and in the presence of a secondary boninitic and andesitic volcanism may provide a way to discriminate between these two interpretations: are they descending near-axis hydrothermal fluxes (first model) or ascending from a subducting slab (second model)? We herein focus on the base of the ophiolitic <span class="hlt">mantle</span> in order to characterize the origin of fluids and decipher hydration processes. Samples were taken along hecto- to kilometre-long sections across the basal banded unit directly overlying the amphibolitic/granulitic metamorphic sole. We carried out a petrological, structural and geochemical study on these rocks and their constitutive minerals. Our results show that, unlike the generally refractory character of Oman harzburgites, all the basal <span class="hlt">mantle</span> rocks display secondary crystallization of clinopyroxene and amphibole through metasomatic processes. The microstructures and the chronology of these secondary mineralizations (clinopyroxene, pargasitic amphibole, antigorite and then lizardite/chrysotile) suggest that these basal rocks have been affected by cooling from <span class="hlt">mantle</span> temperatures (<1200°C) to low-T serpentinisation (<300°C). Furthermore, major elements required to crystallize these minerals and the observed fluid-mobile elements (FMEs) enrichments in the clinopyroxenes and in the amphiboles (B, Pb, Sr), as well as in the serpentines (B, Sr, Rb, Ba, As), are consistent with amphibolite-derived fluids (Ishikawa et al., 2005) and cannot be easily explained by other sources. Based on these observations, we propose a geodynamic model in which intense and continuous metasomatism of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1126236-rolling-hills-core-mantle-boundary','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1126236-rolling-hills-core-mantle-boundary"><span>Rolling hills on the core-<span class="hlt">mantle</span> boundary</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sun, Daoyuan; Helmberger, Don V.; Jackson, Jennifer M.</p> <p>2014-07-17</p> <p>Recent results suggest that an iron-rich oxide may have fractionally crystallized from a primordial magma ocean and settled on the core–<span class="hlt">mantle</span> boundary (CMB). Based on experimental results, the presence of only a few percent of Fe-rich oxide could slow seismic waves down by several percent. This heavy layer can become highly undulating as predicted from dynamic modeling but can remain as a distinct structure with uniform velocity reductions. Here, we use the large USArray seismic network to search for such structures. Strong constraints on D" are provided by the core-phase SKS where it bifurcates, containing a short segment of P-wavemore » diffractions (P d) when crossing the CMB, called SKS d. Synthetics from models with moderate velocity drops (less than 10%) involving a layer with variable thickness, perhaps a composite of sharp small structures, with strong variation in thickness can explain both the observed SKS d waveforms and large scatter in <span class="hlt">differential</span> times between SKKS and SKS. A smooth 3D image is obtained from inverting SKS d waveforms displaying rolling-hills with elongated dome-like structures sitting on the CMB. The most prominent one has an 80-km height, ~8° length, and ~4° width, thus adding still more structural complexity to the lower <span class="hlt">mantle</span>. We suggest that these results can be explained by a dynamically-stabilized material containing small amounts (~5%) iron-rich (Mg,Fe)O providing a self-consistent physical interpretation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P53F..04A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P53F..04A"><span>Thermal Evolution of Earth's <span class="hlt">Mantle</span> During the Accretion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arkani-Hamed, J.; Roberts, J. H.</p> <p>2017-12-01</p> <p>Earth is likely formed by accreting Moon to Mars size embryos. The impact heating by an embryo melts the embryo and the upper <span class="hlt">mantle</span> of the Earth beneath the impact site. The iron core of the embryo sinks and merges with the core of the Earth, while the <span class="hlt">mantle</span> of the embryo mixes with the upper <span class="hlt">mantle</span> of the Earth, producing a buoyant molten/partially molten magma pond. Strong but localized <span class="hlt">mantle</span> dynamics results in fast lithostatic adjustment that pours out a huge amount of molten and partially molten magma which spread on the Earth, and together with impact ejecta creates a globe encircling magma ocean. The lithostatic adjustment diminishes as the magma ocean becomes globe encircling within 104 to 105 yr. The major part of the thermal evolution of Earth's <span class="hlt">mantle</span> after an impact takes place in the presence of a thick and hot magma ocean, which hampers heat loss from the <span class="hlt">mantle</span> and suppresses global <span class="hlt">mantle</span> dynamics. Because the impact velocity of an embryo increases as the Earth grows, a given magma ocean is hotter than the previous ones. We investigated this scenario using 25 Moon to Mars size embryos. Due to random geographic impact sites we considered vertical impacts since no information is available about the impact angles. This may over estimate the impact heating by a factor of 1.4 with respect to the most probable impact angle of 45o. The thermal structure of the Earth at the end of accretion is layered, aside from the localized magma ponds that are distributed randomly due to the random geographic impact sites. We also take into account the impact heating of the solid lower <span class="hlt">mantle</span>, the heating of the lower <span class="hlt">mantle</span> by the gravitational energy released through sinking of an embryo's core. We then follow the thermal evolution of the <span class="hlt">mantle</span> of a growing Earth using a 3D convection model. The Earth grows due to merging of the impactor iron core with the Earth's core, and the accumulating magma ocean on the surface. The growth enhances the lithostatic pressure</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V31A4722G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V31A4722G"><span>Molybdenum Isotopic Composition of the Archean <span class="hlt">Mantle</span> As Inferred from Studies of Komatiites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Greber, N. D.; Puchtel, I. S.; Nagler, T. F.; Mezger, K.</p> <p>2014-12-01</p> <p>Molybdenum isotopic composition has been shown to be a powerful tool in studies of planetary processes, e.g. estimating core formation temperatures [1,2]. However, Mo isotope compositions of terrestrial reservoirs are not well constrained. In order to better constrain the Mo isotopic composition of the <span class="hlt">early</span> Earth's <span class="hlt">mantle</span>, komatiites from four locations were analyzed for their Mo concentrations and isotopic compositions. Komatiites are particularly appropriate for this type of study because they formed by high degrees of partial melting of the <span class="hlt">mantle</span> leading to a complete base metal sulfide removal from the residual <span class="hlt">mantle</span> and the production of sulfur-undersaturated melts and thus a quantitative removal of Mo from the source into the melt. All samples, except for two strongly altered specimens specifically chosen to study the effects of secondary alteration, are very fresh having preserved most of their primary mineralogy. The Mo concentrations in komatiites range from 10 to 120 ng/g. Fresh komatiites have lighter δ98Mo (NIST SRM 3134 = 0.25‰, [3]) than altered samples. The estimated primary Mo isotope compositions of the studied komatiite melts range from 0.02 ± 0.16‰ to 0.19 ± 0.14‰ and are therefore indistinguishable within analytical uncertainty (2SD) from published values for chondritic meteorites (0.09 ± 0.04 ‰; 2SD; [2]) and lighter than the proposed average for Earth's continental crust (0.3 to 0.4‰ [4]). All data combined, although overlapping in errors, show a consistent trend of lighter δ98Mo and lower Mo concentrations in more melt-depleted <span class="hlt">mantle</span> sources, indicating incompatible behaviour of Mo and preferential mobilization of heavy Mo isotopes during <span class="hlt">mantle</span> melting. [1] Hin et al. (2013) EPSL, 379 [2] Burkhardt et al. (2014) EPSL, 391 [3] Nägler, et al. (2014) GGR, 38. [4] Voegelin et al. (2014) Lithos, 190-191.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930000952','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930000952"><span>Asteroids and Archaean crustal evolution: Tests of possible genetic links between major <span class="hlt">mantle</span>/crust melting events and clustered extraterrestrial bombardments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Glikson, A. Y.</p> <p>1992-01-01</p> <p>Since the oldest intact terrestrial rocks of ca. 4.0 Ga and oldest zircon xenocrysts of ca. 4.3 Ga measured to date overlap with the lunar late heavy bombardment, the <span class="hlt">early</span> Precambrian record requires close reexamination vis a vis the effects of megaimpacts. The identification of microtektite-bearing horizons containing spinals of chondritic chemistry and Ir anomalies in 3.5-3.4-Ga greenstone belts provides the first direct evidence for large-scale Archaean impacts. The Archaean crustal record contains evidence for several major greenstone-granite-forming episodes where deep upwelling and adiabatic fusion of the <span class="hlt">mantle</span> was accompanied by contemporaneous crustal anatexis. Isotopic age studies suggest evidence for principal age clusters about 3.5, 3.0, and 2.7 (+/- 0.8) Ga, relics of a ca. 3.8-Ga event, and several less well defined episodes. These peak events were accompanied and followed by protracted thermal fluctuations in intracrustal high-grade metamorphic zones. Interpretations of these events in terms of internal dynamics of the Earth are difficult to reconcile with the thermal behavior of silicate rheologies in a continuously convecting <span class="hlt">mantle</span> regime. A triggering of these episodes by <span class="hlt">mantle</span> rebound response to intermittent extraterrestrial asteroid impacts is supported by (1) identification of major Archaean impacts from microtektite and distal ejecta horizons marked by Ir anomalies; (2) geochemical and experimental evidence for <span class="hlt">mantle</span> upwelling, possibly from levels as deep as the transition zone; and (3) catastrophic adiabatic melting required to generate peridotitic komatites. Episodic <span class="hlt">differentiation</span>/accretion growth of sial consequent on these events is capable of resolving the volume problem that arises from comparisons between modern continental crust and the estimated sial produced by continuous two-stage <span class="hlt">mantle</span> melting processes. The volume problem is exacerbated by projected high accretion rates under Archaean geotherms. It is suggested that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V51A3056H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V51A3056H"><span>Magnesium Isotopic Composition of Kamchatka Sub-Arc <span class="hlt">Mantle</span> Peridotites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hu, Y.; Teng, F. Z.; Ionov, D. A.</p> <p>2016-12-01</p> <p>Subduction of the oceanic slab may add a crustal isotopic signal to the <span class="hlt">mantle</span> wedge. The highly variable Mg isotopic compositions (δ26Mg) of the subducted oceanic crust input[1] and arc lava output[2] imply a distinctive Mg isotopic signature of the <span class="hlt">mantle</span> wedge. Magnesium isotopic data on samples from the sub-arc <span class="hlt">mantle</span> are still limited, however. To characterize the Mg isotopic composition of typical sub-arc <span class="hlt">mantle</span>, 17 large and fresh spinel harzburgite xenoliths from Avacha volcano were analyzed. The harzburgites were formed by 30% melt extraction at ≤ 1 2 GPa and fluid fluxing condition, and underwent possible fluid metasomatism as suggested by distinctively high orthopyroxene mode in some samples, the presence of accessory amphibole and highly variable Ba/La ratios[3]. However, their δ26Mg values display limited variation from -0.32 to -0.21, which are comparable to the <span class="hlt">mantle</span> average at -0.25 ± 0.07[4]. The overall <span class="hlt">mantle</span>-like and homogenous δ26Mg of Avacha sub-arc peridotites are consistent with their similar chemical compositions and high MgO contents (> 44 wt%) relative to likely crustal fluids. Furthermore, clinopyroxene (-0.24 ± 0.10, 2SD, n = 5), a late-stage mineral exsolved from high-temperature, Ca-rich residual orthopyroxene, is in broad Mg isotopic equilibrium with olivine (-0.27 ± 0.04, 2SD, n = 17) and orthopyroxene (-0.22 ± 0.06, 2SD, n = 17). Collectively, this study finds that the Kamchatka <span class="hlt">mantle</span> wedge, as represented by the Avacha peridotites, has a <span class="hlt">mantle</span>-like δ26Mg, and low-degree fluid-<span class="hlt">mantle</span> interaction does not cause significant Mg isotope fractionation in sub-arc <span class="hlt">mantle</span> peridotites. [1] Wang et al., EPSL, 2012 [2] Teng et al., PNAS, 2016 [3] Ionov, J. Petrol., 2010, [4] Teng et al., GCA, 2010.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMGP13A1115F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMGP13A1115F"><span>Eight good reasons why the uppermost <span class="hlt">mantle</span> could be magnetic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferre, E. C.; Friedman, S. A.; Martin Hernandez, F.; Till, J. L.; Ionov, D. A.; Conder, J. A.</p> <p>2012-12-01</p> <p>The launch of Magsat in 1979 prompted a broad magnetic investigation of <span class="hlt">mantle</span> xenoliths (Wasilewski et al., 1979). The study concluded that no magnetic remanence existed in the uppermost <span class="hlt">mantle</span> and that even if present, such sources would be at temperatures too high to contribute to long wavelength magnetic anomalies (LWMA). However, new collections of unaltered <span class="hlt">mantle</span> xenoliths from four different tectonic settings, along with updated views on the sources of LWMA and modern petrologic constraints on fO2 in the <span class="hlt">mantle</span> indicate that the uppermost <span class="hlt">mantle</span> could, in certain cases, contain ferromagnetic minerals. 1. The analysis of some LWMA over areas such as, for example, Bangui in the Central African Craton, the Cascadia subduction zone and serpentinized oceanic lithosphere suggest magnetic sources in the uppermost <span class="hlt">mantle</span>. 2. The most common ferromagnetic phase in the uppermost <span class="hlt">mantle</span> is pure magnetite, which has a pressure-corrected Curie temperature at 10 kbars of 600C instead of the generally used value of 580C. Assuming 30 km-thick continental crust, and crustal and <span class="hlt">mantle</span> geotherms of 15C/km and 5C/km, respectively, the 600C Curie temperature implies the existence of a 30 km-thick layer of <span class="hlt">mantle</span> rocks, whose remanent and induced magnetizations could contribute to LWMA. The thickness of this layer decreases to about 15 km for a 35 km-thick crust. 3. The uppermost <span class="hlt">mantle</span> is cooler than 600C in some tectonic settings, including Archean and Proterozoic shields (>350C), subduction zones (>300C) and old oceanic basins (>250C). 4. Recently investigated sets of unaltered <span class="hlt">mantle</span> xenoliths contain pure SD and PSD magnetite inclusions exsolved in olivine and pyroxene. The fact that these magnetite grains are not associated with any alteration phases, such as serpentine, and exhibit a subhedral shape, demonstrates that they formed in equilibrium with the host silicate. 5. The ascent of <span class="hlt">mantle</span> xenoliths in volcanic conduits through cratons and subduction zones occurs in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011GeCoA..75.5574H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011GeCoA..75.5574H"><span>Osmium mass balance in peridotite and the effects of <span class="hlt">mantle</span>-derived sulphides on basalt petrogenesis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harvey, J.; Dale, C. W.; Gannoun, A.; Burton, K. W.</p> <p>2011-10-01</p> <p>Analyses of enriched <span class="hlt">mantle</span> (EM)-basalts, using lithophile element-based isotope systems, have long provided evidence for discrete <span class="hlt">mantle</span> reservoirs with variable composition. Upon partial melting, the <span class="hlt">mantle</span> reservoir imparts its isotopic fingerprint upon the partial melt produced. However, it has increasingly been recognised that it may not be simple to delimit these previously well-defined <span class="hlt">mantle</span> reservoirs; the "<span class="hlt">mantle</span> zoo" may contain more reservoirs than previously envisaged. Here we demonstrate that a simple model with varying contributions from two populations of compositionally distinct <span class="hlt">mantle</span> sulphides can readily account for the observed heterogeneities in Os isotope systematics of such basalts without additional <span class="hlt">mantle</span> reservoirs. Osmium elemental and isotopic analyses of individual sulphide grains separated from spinel lherzolites from Kilbourne Hole, New Mexico, USA demonstrate that two discrete populations of <span class="hlt">mantle</span> sulphide exist in terms of both Re-Os systematics and textural relationship with co-existing silicates. One population, with a rounded morphology, is preserved in silicate grains and typically possesses high [Os] and low [Re] with unradiogenic, typically sub-chondritic 187Os/ 188Os attributable to long term isolation in a low-Re environment. By contrast, irregular-shaped sulphides, preserved along silicate grain boundaries, possess low [Os], higher [Re] and a wider range of, but generally supra-chondritic 187Os/ 188Os ([Os] typically ⩽ 1-2 ppm, 187Os/ 188Os ⩽ 0.3729; this study). This population is thought to represent metasomatic sulphide. Uncontaminated silicate phases contain negligible Os (<100 ppt) therefore the Os elemental and isotope composition of basalts is dominated by volumetrically insignificant sulphide ([Os] ⩽ 37 ppm; this study). During the <span class="hlt">early</span> stages of partial melting, supra-chondritic interstitial sulphides are mobilised and incorporated into the melt, adding their radiogenic 187Os/ 188Os signature. Only when</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V23B0475A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V23B0475A"><span>Quantifying Textures of Rapakivi Granites and <span class="hlt">Mantle</span> Formation Insights</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ashauer, Z.; Currier, R. M.</p> <p>2017-12-01</p> <p>Rapakivi texture, the <span class="hlt">mantling</span> of plagioclase on alkali feldspar, is a common occurrence in granitoids derived from crustal melting. Presented here, are several textural analyses that quantify <span class="hlt">mantle</span> thickness and the overall distribution of crystal populations. Analyses were performed on outcrops and slabbed samples from the Wolf River Batholith, Wisconsin, USA and the Wiborg Batholith, Finland. Both localities are "classical" rapakivi granites of Proterozoic age associated with incipient rifting of the supercontinent Nuna/Columbia. <span class="hlt">Mantle</span> thickness analysis reveals a relationship between the characteristic size of the <span class="hlt">mantle</span> and the size of the core. The thickest <span class="hlt">mantles</span> tend to be on relatively small cores while relatively large cores display thin <span class="hlt">mantles</span>. This relationship is consistent with a replacement origin as a result of alkali feldspar dissolution with concomitant reprecipitation of plagioclase, due to disequilibrium between crystal and melt. If this is the case then crystal size distributions should be similar between unmantled and <span class="hlt">mantled</span> megacrysts. Preliminary results confirm this supposition: rapakivi <span class="hlt">mantle</span> formation in these classical systems appear to be the result of replacement. These textural analyses immediately call into question the viability of epitaxial growth models. A certain amount of disequilibrium is required to drive the replacement reaction. Two potential mechanisms are 1) mechanical transfer of crystals into a magma of more mafic composition (i.e., magma mixing), and 2) the production of a heterogeneous melt during rapid melting of granitic rock and reaction between unmelted crystals and partial melt. The classical rapakivi granites are associated with prolonged bimodal magmatism, and so there is clear potential to drive either of these <span class="hlt">mantling</span> mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23486061','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23486061"><span>Water and hydrogen are immiscible in Earth's <span class="hlt">mantle</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bali, Enikő; Audétat, Andreas; Keppler, Hans</p> <p>2013-03-14</p> <p>In the deep, chemically reducing parts of Earth's <span class="hlt">mantle</span>, hydrous fluids contain significant amounts of molecular hydrogen (H2). Thermodynamic models of fluids in Earth's <span class="hlt">mantle</span> so far have always assumed that molecular hydrogen and water are completely miscible. Here we show experimental evidence that water and hydrogen can coexist as two separate, immiscible phases. Immiscibility between water and hydrogen may be the cause of the formation of enigmatic, ultra-reducing domains in the <span class="hlt">mantle</span> that contain moissanite (SiC) and other phases indicative of extremely reducing conditions. Moreover, the immiscibility between water and hydrogen may provide a mechanism for the rapid oxidation of Earth's upper <span class="hlt">mantle</span> immediately following core formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27688662','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27688662"><span>Clinicopathological features of alpha-fetoprotein producing <span class="hlt">early</span> gastric cancer with enteroblastic <span class="hlt">differentiation</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Matsumoto, Kohei; Ueyama, Hiroya; Matsumoto, Kenshi; Akazawa, Yoichi; Komori, Hiroyuki; Takeda, Tsutomu; Murakami, Takashi; Asaoka, Daisuke; Hojo, Mariko; Tomita, Natsumi; Nagahara, Akihito; Kajiyama, Yoshiaki; Yao, Takashi; Watanabe, Sumio</p> <p>2016-09-28</p> <p>To investigate clinicopathological features of <span class="hlt">early</span> stage gastric cancer with enteroblastic <span class="hlt">differentiation</span> (GCED). We retrospectively investigated data on 6 cases of <span class="hlt">early</span> stage GCED and 186 cases of <span class="hlt">early</span> stage conventional gastric cancer (CGC: well or moderately <span class="hlt">differentiated</span> adenocarcinoma) who underwent endoscopic submucosal dissection or endoscopic mucosal resection from September 2011 to February 2015 in our hospital. GCED was defined as a tumor having a primitive intestine-like structure composed of cuboidal or columnar cells with clear cytoplasm and immunohistochemical positivity for either alpha-fetoprotein, Glypican 3 or SALL4. The following were compared between GCED and CGC: age, gender, location and size of tumor, macroscopic type, ulceration, depth of invasion, lymphatic and venous invasion, positive horizontal and vertical margin, curative resection rate. Six cases (5 males, 1 female; mean age 75.7 years; 6 lesions) of <span class="hlt">early</span> gastric cancer with a GCED component and 186 cases (139 males, 47 females; mean age 72.7 years; 209 lesions) of <span class="hlt">early</span> stage CGC were investigated. Mean tumor diameters were similar but rates of submucosal invasion, lymphatic invasion, venous invasion, and non-curative resection were higher in GCED than CGC (66.6% vs 11.4%, 33.3% vs 2.3%, 66.6% vs 0.4%, 83.3% vs 11% respectively, P < 0.01). Deep submucosal invasion was not revealed endoscopically or by preoperative biopsy. Histologically, in GCED the superficial mucosal layer was covered with a CGC component. The GCED component tended to exist in the deeper part of the mucosa to the submucosa by lymphatic and/or venous invasion, without severe stromal reaction. In addition, Glypican 3 was the most sensitive marker for GCED (positivity, 83.3%), immunohistochemically. Even in the <span class="hlt">early</span> stage GCED has high malignant potential, and preoperative diagnosis is considered difficult. Endoscopists and pathologists should know the clinicopathological features of this highly malignant type</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T22D..02O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T22D..02O"><span>Geothermal Heat Flux and Upper <span class="hlt">Mantle</span> Viscosity across West Antarctica: Insights from the UKANET and POLENET Seismic Networks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>O'Donnell, J. P.; Dunham, C.; Stuart, G. W.; Brisbourne, A.; Nield, G. A.; Whitehouse, P. L.; Hooper, A. J.; Nyblade, A.; Wiens, D.; Aster, R. C.; Anandakrishnan, S.; Huerta, A. D.; Wilson, T. J.; Winberry, J. P.</p> <p>2017-12-01</p> <p>Quantifying the geothermal heat flux at the base of ice sheets is necessary to understand their dynamics and evolution. The heat flux is a composite function of concentration of upper crustal radiogenic elements and flow of heat from the <span class="hlt">mantle</span> into the crust. Radiogenic element concentration varies with tectonothermal age, while heat flow across the crust-<span class="hlt">mantle</span> boundary depends on crustal and lithospheric thicknesses. Meanwhile, accurately monitoring current ice mass loss via satellite gravimetry or altimetry hinges on knowing the upper <span class="hlt">mantle</span> viscosity structure needed to account for the superimposed glacial isostatic adjustment (GIA) signal in the satellite data. In <span class="hlt">early</span> 2016 the UK Antarctic Network (UKANET) of 10 broadband seismometers was deployed for two years across the southern Antarctic Peninsula and Ellsworth Land. Using UKANET data in conjunction with seismic records from our partner US Polar Earth Observing Network (POLENET) and the Antarctic Seismographic Argentinian Italian Network (ASAIN), we have developed a 3D shear wave velocity model of the West Antarctic crust and uppermost <span class="hlt">mantle</span> based on Rayleigh and Love wave phase velocity dispersion curves extracted from ambient noise cross-correlograms. We combine seismic receiver functions with the shear wave model to help constrain the depth to the crust-<span class="hlt">mantle</span> boundary across West Antarctica and delineate tectonic domains. The shear wave model is subsequently converted to temperature using a database of densities and elastic properties of minerals common in crustal and <span class="hlt">mantle</span> rocks, while the various tectonic domains are assigned upper crustal radiogenic element concentrations based on their inferred tectonothermal ages. We combine this information to map the basal geothermal heat flux variation across West Antarctica. <span class="hlt">Mantle</span> viscosity depends on factors including temperature, grain size, the hydrogen content of olivine and the presence of melt. Using published <span class="hlt">mantle</span> xenolith and magnetotelluric</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.8701X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.8701X"><span>Magmatic plumbing system from lower <span class="hlt">mantle</span> of Hainan plume</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xia, Shaohong; Sun, Jinlong; Xu, Huilong; Huang, Haibo; Cao, Jinghe</p> <p>2017-04-01</p> <p>Intraplate volcanism during Late Cenozoic in the Leiqiong area of southernmost South China, with basaltic lava flows covering a total of more than 7000 km2, has been attributed to an underlying Hainan plume. However, detailed features of Hainan plume, such as morphology of magmatic conduits, depth of magmatic pool in the upper <span class="hlt">mantle</span> and pattern of <span class="hlt">mantle</span> upwelling, are still enigmatic. Here we present seismic tomographic images of the upper 1100 km of the <span class="hlt">mantle</span> beneath the southern South China. Our results show a mushroom-like continuous low-velocity anomaly characterized by a columnar tail with diameter of about 200-300 km that tilts downward to lower <span class="hlt">mantle</span> beneath north of Hainan hotspot and a head that spreads laterally near the <span class="hlt">mantle</span> transition zone, indicating a magmatic pool in the upper <span class="hlt">mantle</span>. Further upward, this head is decomposed into small patches, but when encountering the base of the lithosphere, a pancake-like anomaly is shaped again to feed the Hainan volcanism. Our results challenge the classical model of a fixed thermal plume that rises vertically to the surface, and propose the new layering-style pattern of magmatic upwelling of Hainan plume. This work indicates the spatial complexities and differences of global <span class="hlt">mantle</span> plumes probably due to heterogeneous compositions and changefully thermochemical structures of deep <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950015385&hterms=recycling&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Drecycling','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950015385&hterms=recycling&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Drecycling"><span>Subduction and volatile recycling in Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>King, S. D.; Ita, J. J.; Staudigel, H.</p> <p>1994-01-01</p> <p>The subduction of water and other volatiles into the <span class="hlt">mantle</span> from oceanic sediments and altered oceanic crust is the major source of volatile recycling in the <span class="hlt">mantle</span>. Until now, the geotherms that have been used to estimate the amount of volatiles that are recycled at subduction zones have been produced using the hypothesis that the slab is rigid and undergoes no internal deformation. On the other hand, most fluid dynamical <span class="hlt">mantle</span> flow calculations assume that the slab has no greater strength than the surrounding <span class="hlt">mantle</span>. Both of these views are inconsistent with laboratory work on the deformation of <span class="hlt">mantle</span> minerals at high pressures. We consider the effects of the strength of the slab using two-dimensional calculations of a slab-like thermal downwelling with an endothermic phase change. Because the rheology and composition of subducting slabs are uncertain, we consider a range of Clapeyron slopes which bound current laboratory estimates of the spinel to perovskite plus magnesiowustite phase transition and simple temperature-dependent rheologies based on an Arrhenius law diffusion mechanism. In uniform viscosity convection models, subducted material piles up above the phase change until the pile becomes gravitationally unstable and sinks into the lower <span class="hlt">mantle</span> (the avalanche). Strong slabs moderate the 'catastrophic' effects of the instabilities seen in many constant-viscosity convection calculations; however, even in the strongest slabs we consider, there is some retardation of the slab descent due to the presence of the phase change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.484..363M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.484..363M"><span>Water distribution in the lower <span class="hlt">mantle</span>: Implications for hydrolytic weakening</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Muir, Joshua M. R.; Brodholt, John P.</p> <p>2018-02-01</p> <p>The presence of water in lower <span class="hlt">mantle</span> minerals is thought to have substantial effects on the rheological properties of the Earth's lower <span class="hlt">mantle</span> in what is generally known as "hydrolytic weakening". This weakening will have profound effects on global convection, but hydrolytic weakening in lower <span class="hlt">mantle</span> minerals has not been observed experimentally and thus the effect of water on global dynamics remains speculative. In order to constrain the likelihood of hydrolytic weakening being important in the lower <span class="hlt">mantle</span>, we use first principles methods to calculate the partitioning of water (strictly protons) between mineral phases of the lower <span class="hlt">mantle</span> under lower <span class="hlt">mantle</span> conditions. We show that throughout the lower <span class="hlt">mantle</span> water is primarily found either in the minor Ca-perovskite phase or in bridgmanite as an Al3+-H+ pair. Ferropericlase remains dry. However, neither of these methods of water absorption creates additional vacancies in bridgmanite and thus the effect of hydrolytic weakening is likely to be small. We find that water creates significant number of vacancies in bridgmanite only at the deepest part of the lower <span class="hlt">mantle</span> and only for very high water contents (>1000 ppm). We conclude that water is thus likely to have only a limited effect on the rheological properties of the lower <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMDI51A..02T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMDI51A..02T"><span>Supercontinents, Plate Tectonics, Large Igneous Provinces and Deep <span class="hlt">Mantle</span> Heterogeneities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Torsvik, T. H.; Steinberger, B.; Burke, K.; Smethurst, M. A.</p> <p>2008-12-01</p> <p>The formation and break-up of supercontinents is a spectacular demonstration of the Earth's dynamic nature. Pangea, the best-documented supercontinent, formed at the end of the Palaeozoic era (320 Ma) and its dispersal, starting in the <span class="hlt">Early</span> Jurassic (190 Ma), was preceded by and associated with widespread volcanic activity, much of which produced Large Igneous Provinces (LIPs), but whether any of the heat or material involved in the generation of LIP rocks comes from greater depths has remained controversial. Two antipodal Large Low Shear wave Velocity Provinces with centre of mass somewhat south of the equator (African and Pacific LLSVPs), isolated within the faster parts of the deep <span class="hlt">mantle</span> dominate all global shear- wave tomography models. We have tested eight global models and two D" models: They all show that deep- plume sourced hotspots and most reconstructed LIPs for the last 300 million years project radially downwards to the core-<span class="hlt">mantle</span>-boundary near the edges of the LLSVPs showing that the plumes that made those hotspots and LIPS came only from those plume generation zones. This is a robust result because it is observed in multiple reference frames, i.e. fixed/moving hotspot and palaeomagnetic frames, and in the latter case whether the effect of True Polar Wander (TPW) is considered or not. Our observations show that the LLSVPs must have remained essentially stable in their present position for the last 300 million years. LIPs have erupted since the Archean and may all have been derived from the margins of LLSVPs but whether the African and Pacific LLSVPs have remained the same throughout Earth's history is less certain although analogous structures on Mars do indicate long-term stability on that planet. Deep <span class="hlt">mantle</span> heterogeneities and the geoid have remained very stable for the last 300 million years, and the possibility is therefore open for speculating on links to Pangea assembly. In a numerical model, Zhong et al. (2007, EPSL) argued that Pangea</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006GGG.....711013B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006GGG.....711013B"><span><span class="hlt">Mantle</span> transition zone structure and upper <span class="hlt">mantle</span> S velocity variations beneath Ethiopia: Evidence for a broad, deep-seated thermal anomaly</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Benoit, Margaret H.; Nyblade, Andrew A.; Owens, Thomas J.; Stuart, Graham</p> <p>2006-11-01</p> <p>Ethiopia has been subjected to widespread Cenozoic volcanism, rifting, and uplift associated with the Afar hot spot. The hot spot tectonism has been attributed to one or more thermal upwellings in the <span class="hlt">mantle</span>, for example, starting thermal plumes and superplumes. We investigate the origin of the hot spot by imaging the S wave velocity structure of the upper <span class="hlt">mantle</span> beneath Ethiopia using travel time tomography and by examining relief on transition zone discontinuities using receiver function stacks. The tomographic images reveal an elongated low-velocity region that is wide (>500 km) and extends deep into the upper <span class="hlt">mantle</span> (>400 km). The anomaly is aligned with the Afar Depression and Main Ethiopian Rift in the uppermost <span class="hlt">mantle</span>, but its center shifts westward with depth. The 410 km discontinuity is not well imaged, but the 660 km discontinuity is shallower than normal by ˜20-30 km beneath most of Ethiopia, but it is at a normal depth beneath Djibouti and the northwestern edge of the Ethiopian Plateau. The tomographic results combined with a shallow 660 km discontinuity indicate that upper <span class="hlt">mantle</span> temperatures are elevated by ˜300 K and that the thermal anomaly is broad (>500 km wide) and extends to depths ≥660 km. The dimensions of the thermal anomaly are not consistent with a starting thermal plume but are consistent with a flux of excess heat coming from the lower <span class="hlt">mantle</span>. Such a broad thermal upwelling could be part of the African Superplume found in the lower <span class="hlt">mantle</span> beneath southern Africa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMDI21B1960Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMDI21B1960Z"><span>The Evolution of the Earth's <span class="hlt">Mantle</span> Structure and Surface and Core-<span class="hlt">mantle</span> Boundary Heat Flux since the Paleozoic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, N.; Zhong, S.</p> <p>2010-12-01</p> <p>The cause for and time evolution of the seismically observed African and Pacific slow anomalies (i.e., superplumes) are still unclear with two competing proposals. First, the African and Pacific superplumes have remained largely unchanged for at least the last 300 Ma and possibly much longer. Second, the African superplume is formed sometime after the formation of Pangea (i.e., at 330 Ma ago) and the <span class="hlt">mantle</span> in the African hemisphere is predominated by cold downwelling structures before and during the assembly of Pangea, while the Pacific superplume has been stable for the Pangea supercontinent cycle (i.e., globally a degree-1 structure before the Pangea formation). Here, we construct a plate motion history back to 450 Ma and use it as time-dependent surface boundary conditions in 3-dimensional spherical models of thermochemical <span class="hlt">mantle</span> convection to study the evolution of <span class="hlt">mantle</span> structure as well as the surface and core-<span class="hlt">mantle</span> boundary heat flux. Our results for the <span class="hlt">mantle</span> structures suggest that while the <span class="hlt">mantle</span> in the African hemisphere before the assembly of Pangea is predominated by the cold downwelling structure resulting from plate convergence between Gondwana and Laurussia, it is unlikely that the bulk of the African superplume structure can be formed before ~240 Ma (i.e., ~100 Ma after the assembly of Pangea). The evolution of <span class="hlt">mantle</span> structure has implications for heat flux at the surface and core-<span class="hlt">mantle</span> boundary (CMB). Our results show that while the plate motion controls the surface heat flux, the major cold downwellings control the core-<span class="hlt">mantle</span> boundary heat flux. A notable feature in surface heat flux from our models is that the surface heat flux peaks at ~100 Ma ago but decreases for the last 100 Ma due to the breakup of Pangea and its subsequent plate evolution. The CMB heat flux in the equatorial regions shows two minima during period 320-250 Ma and period 120-84 Ma. The first minimum clearly results from the disappearance of a major cold downwelling</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.480...97E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.480...97E"><span>Seismic anisotropy in the Hellenic subduction zone: Effects of slab segmentation and subslab <span class="hlt">mantle</span> flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Evangelidis, C. P.</p> <p>2017-12-01</p> <p>The segmentation and <span class="hlt">differentiation</span> of subducting slabs have considerable effects on <span class="hlt">mantle</span> convection and tectonics. The Hellenic subduction zone is a complex convergent margin with strong curvature and fast slab rollback. The upper <span class="hlt">mantle</span> seismic anisotropy in the region is studied focusing at its western and eastern edges in order to explore the effects of possible slab segmentation on <span class="hlt">mantle</span> flow and fabrics. Complementary to new SKS shear-wave splitting measurements in regions not adequately sampled so far, the source-side splitting technique is applied to constrain the depth of anisotropy and to densify measurements. In the western Hellenic arc, a trench-normal subslab anisotropy is observed near the trench. In the forearc domain, source-side and SKS measurements reveal a trench-parallel pattern. This indicates subslab trench-parallel <span class="hlt">mantle</span> flow, associated with return flow due to the fast slab rollback. The passage from continental to oceanic subduction in the western Hellenic zone is illustrated by a forearc transitional anisotropy pattern. This indicates subslab <span class="hlt">mantle</span> flow parallel to a NE-SW smooth ramp that possibly connects the two subducted slabs. A young tear fault initiated at the Kefalonia Transform Fault is likely not entirely developed, as this trench-parallel anisotropy pattern is observed along the entire western Hellenic subduction system, even following this horizontal offset between the two slabs. At the eastern side of the Hellenic subduction zone, subslab source-side anisotropy measurements show a general trench-normal pattern. These are associated with <span class="hlt">mantle</span> flow through a possible ongoing tearing of the oceanic lithosphere in the area. Although the exact geometry of this slab tear is relatively unknown, SKS trench-parallel measurements imply that the tear has not reached the surface yet. Further exploration of the Hellenic subduction system is necessary; denser seismic networks should be deployed at both its edges in order to achieve</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.lymphoma.org/aboutlymphoma/nhl/mcl/','NIH-MEDLINEPLUS'); return false;" href="https://www.lymphoma.org/aboutlymphoma/nhl/mcl/"><span><span class="hlt">Mantle</span> Cell Lymphoma</span></a></p> <p><a target="_blank" href="http://medlineplus.gov/">MedlinePlus</a></p> <p></p> <p></p> <p>... Cell Lymphoma <span class="hlt">Mantle</span> Cell lymphoma is typically an aggressive Lymphomas that are fast growing and generally need ... LDH suggest that the lymphoma may be more aggressive. and beta-2 microglobulin. Measuring these and other ...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.9229B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.9229B"><span><span class="hlt">Mantle</span> xenoliths from Marosticano area (Northern Italy): a comparison with Veneto Volcanic Province lithospheric <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brombin, Valentina; Bonadiman, Costanza; Coltorti, Massimo</p> <p>2016-04-01</p> <p>The Tertiary Magmatic Province of Veneto, known as Veneto Volcanic Province (VVP), in the North-East of Italy, represents the most important volcanic distric of Adria Plate. It is composed by five volcanic bodies: Val d'Adige, Marosticano, Mts. Lessini, Berici Hills and Euganean Hills. Most of the volcanic products are relatively undifferentiated lavas and range in composition from nephelinites to tholeiites. Often VVP nephelinites and basanites carry <span class="hlt">mantle</span> xenoliths (mainly harzburgites and lherzolite). This study reports petrological comparison between Marosticano xenoliths (new outcrop) and xenoliths from the Lessinean and Val d'Adige areas already studied by many Authors (Siena & Coltorti 1989; Beccaluva et al., 2001, Gasperini et al., 2006). Mineral major elements analyses show that the Marosticano lherzolites and harzburgites reflect "more restitic" composition than the <span class="hlt">mantle</span> domain beneath the other VVP districts (Lessini Mts. and Val d'Adige). In fact, olivine and pyroxene of Marosticano xenoliths have the highest mg# values of the entire district (Marosticano→90-93; literature→86-92). At comparable mg# (45-85 wt%) Marosticano spinels tend to be higher in Cr2O3 (23-44 wt%) contents with respect to the other VVP sp (7-25 wt%). It is worth noting that, Ni contents of Marosticano olivines in both harzburgites and lherzolites are higher (2650-3620 ppm) than those of the Lessinean xenoliths (1500- 3450 ppm), and similar to that of Val d'Adige lherzolites (3000-3500 ppm), approaching the contents of Archean cratonic <span class="hlt">mantle</span> (Kelemen, 1998). In turn, Lessinean olivines properly fall in the Ni-mg# Phanerozoic field. At fixed pressure of 15 kbar, the equilibration temperature of Marosticano xenoliths are similar (Brey & Köhler: 920-1120°C) to those of Lessini (O'Neill & Wall: 990-1110°C; Beccaluva et al., 2007), but higher than those of Val d'Adige (Wells: 909-956°C; Gasperini et al., 2006). Finally, Marosticano <span class="hlt">mantle</span> fragment show similar relatively high</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T13F..06C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T13F..06C"><span><span class="hlt">Mantle</span> Serpentinization near the Central Mariana Trench Constrained by Ocean Bottom Surface Wave Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cai, C.; Wiens, D. A.; Lizarralde, D.; Eimer, M. O.; Shen, W.</p> <p>2017-12-01</p> <p>We investigate the crustal and uppermost <span class="hlt">mantle</span> seismic structure across the Mariana trench by jointly inverting Rayleigh wave phase and group velocities from ambient noise and longer period phase velocities from Helmholtz tomography of teleseismic waveforms. We use data from a temporary deployment in 2012-2013, consisting of 7 island-based stations and 20 broadband ocean bottom seismographs, as well as data from the USGS Northern Mariana Islands Seismograph Network. To avoid any potential bias from the starting model, we use a Bayesian Monte-Carlo algorithm to invert for the azimuthally-averaged SV-wave velocity at each node. This method also allows us to apply prior constraints on crustal thickness and other parameters in a systematic way, and to derive formal estimates of velocity uncertainty. The results show the development of a low velocity zone within the incoming plate beginning about 80 km seaward of the trench axis, consistent with the onset of bending faults from bathymetry and earthquake locations. The maximum depth of the velocity anomaly increases towards the trench, and extends to about 30 km below the seafloor. The low velocities persist after the plate is subducted, as a 20-30 km thick low velocity layer with a somewhat smaller velocity reduction is imaged along the top of the slab beneath the forearc. An extremely low velocity zone is observed beneath the serpentine seamounts in the outer forearc, consistent with 40% serpentinization in the forearc <span class="hlt">mantle</span> wedge. Azimuthal anisotropy results show trench parallel fast axis within the incoming plate at uppermost <span class="hlt">mantle</span> depth (2%-4% anisotropy). All these observations suggest the velocity reduction in the incoming plate prior to subduction results from both serpentinized normal faults and water-filled cracks. Water is expelled from the cracks <span class="hlt">early</span> in subduction, causing a modest increase in the velocity of the subducting <span class="hlt">mantle</span>, and moves upward and causes serpentinization of the outer forearc</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PEPI..183....1S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PEPI..183....1S"><span>Preface: Deep Slab and <span class="hlt">Mantle</span> Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suetsugu, Daisuke; Bina, Craig R.; Inoue, Toru; Wiens, Douglas A.</p> <p>2010-11-01</p> <p>We are pleased to publish this special issue of the journal Physics of the Earth and Planetary Interiors entitled "Deep Slab and <span class="hlt">Mantle</span> Dynamics". This issue is an outgrowth of the international symposium "Deep Slab and <span class="hlt">Mantle</span> Dynamics", which was held on February 25-27, 2009, in Kyoto, Japan. This symposium was organized by the "Stagnant Slab Project" (SSP) research group to present the results of the 5-year project and to facilitate intensive discussion with well-known international researchers in related fields. The SSP and the symposium were supported by a Grant-in-Aid for Scientific Research (16075101) from the Ministry of Education, Culture, Sports, Science and Technology of the Japanese Government. In the symposium, key issues discussed by participants included: transportation of water into the deep <span class="hlt">mantle</span> and its role in slab-related dynamics; observational and experimental constraints on deep slab properties and the slab environment; modeling of slab stagnation to constrain its mechanisms in comparison with observational and experimental data; observational, experimental and modeling constraints on the fate of stagnant slabs; eventual accumulation of stagnant slabs on the core-<span class="hlt">mantle</span> boundary and its geodynamic implications. This special issue is a collection of papers presented in the symposium and other papers related to the subject of the symposium. The collected papers provide an overview of the wide range of multidisciplinary studies of <span class="hlt">mantle</span> dynamics, particularly in the context of subduction, stagnation, and the fate of deep slabs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CoMP..172...51U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CoMP..172...51U"><span>Fluorine and chlorine in <span class="hlt">mantle</span> minerals and the halogen budget of the Earth's <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Urann, B. M.; Le Roux, V.; Hammond, K.; Marschall, H. R.; Lee, C.-T. A.; Monteleone, B. D.</p> <p>2017-07-01</p> <p>The fluorine (F) and chlorine (Cl) contents of arc magmas have been used to track the composition of subducted components, and the F and Cl contents of MORB have been used to estimate the halogen content of depleted MORB <span class="hlt">mantle</span> (DMM). Yet, the F and Cl budget of the Earth's upper <span class="hlt">mantle</span> and their distribution in peridotite minerals remain to be constrained. Here, we developed a method to measure low concentrations of halogens (≥0.4 µg/g F and ≥0.3 µg/g Cl) in minerals by secondary ion mass spectroscopy. We present a comprehensive study of F and Cl in co-existing natural olivine, orthopyroxene, clinopyroxene, and amphibole in seventeen samples from different tectonic settings. We support the hypothesis that F in olivine is controlled by melt polymerization, and that F in pyroxene is controlled by their Na and Al contents, with some effect of melt polymerization. We infer that Cl compatibility ranks as follows: amphibole > clinopyroxene > olivine orthopyroxene, while F compatibility ranks as follows: amphibole > clinopyroxene > orthopyroxene ≥ olivine, depending on the tectonic context. In addition, we show that F, Cl, Be and B are correlated in pyroxenes and amphibole. F and Cl variations suggest that interaction with slab melts and fluids can significantly alter the halogen content of <span class="hlt">mantle</span> minerals. In particular, F in oceanic peridotites is mostly hosted in pyroxenes, and proportionally increases in olivine in subduction-related peridotites. The <span class="hlt">mantle</span> wedge is likely enriched in F compared to un-metasomatized <span class="hlt">mantle</span>, while Cl is always low (<1 µg/g) in all tectonic settings studied here. The bulk anhydrous peridotite <span class="hlt">mantle</span> contains 1.4-31 µg/g F and 0.14-0.38 µg/g Cl. The bulk F content of oceanic-like peridotites (2.1-9.4 µg/g) is lower than DMM estimates, consistent with F-rich eclogite in the source of MORB. Furthermore, the bulk Cl budget of all anhydrous peridotites studied here is lower than previous DMM estimates. Our results indicate that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70029340','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70029340"><span>Subduction-zone magnetic anomalies and implications for hydrated forearc <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Blakely, R.J.; Brocher, T.M.; Wells, R.E.</p> <p>2005-01-01</p> <p>Continental <span class="hlt">mantle</span> in subduction zones is hydrated by release of water from the underlying oceanic plate. Magnetite is a significant byproduct of <span class="hlt">mantle</span> hydration, and forearc <span class="hlt">mantle</span>, cooled by subduction, should contribute to long-wavelength magnetic anomalies above subduction zones. We test this hypothesis with a quantitative model of the Cascadia convergent margin, based on gravity and aeromagnetic anomalies and constrained by seismic velocities, and find that hydrated <span class="hlt">mantle</span> explains an important disparity in potential-field anomalies of Cascadia. A comparison with aeromagnetic data, thermal models, and earthquakes of Cascadia, Japan, and southern Alaska suggests that magnetic <span class="hlt">mantle</span> may be common in forearc settings and thus magnetic anomalies may be useful in mapping hydrated <span class="hlt">mantle</span> in convergent margins worldwide. ?? 2005 Geological Society of America.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR52A..04M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR52A..04M"><span>The rheological effect of water on lower <span class="hlt">mantle</span> minerals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Muir, J.; Brodholt, J. P.</p> <p>2017-12-01</p> <p>The presence of water in many upper <span class="hlt">mantle</span> minerals has been shown to have a large effect on their rheology in what is generally known as "hydrolytic weakening". A growing number of studies are finding that incorporating a water dependent rheology into global <span class="hlt">mantle</span> convection models has a strong effect on global dynamics. However, while there is an abundance of experimental evidence showing that upper <span class="hlt">mantle</span> minerals deformed under hydrous conditions are significantly weaker than when dry, there is no such experimental evidence for lower <span class="hlt">mantle</span> minerals. In this study we use DFT methods to calculate the partitioning of water between different sites in lower <span class="hlt">mantle</span> minerals (bridgmanite, cubic and tetragonal calcium perovskite, ferropericlase and phase H) which allows us to speculate on the effects of water on the rheology and phase stability of lower <span class="hlt">mantle</span> minerals under various conditions. The effect of water on lower <span class="hlt">mantle</span> minerals is found to depend strongly upon both water content and temperature. Under typical lower <span class="hlt">mantle</span> conditions and with reasonable water concentrations (<1000 ppm), water partitions preferentially into bridgmanite but with a mechanism that does not increase the concentration of Mg or Si vacancies in bridgmanite and thus is unlikely to affect its rheology. In cooler conditions, such as in a descending slab, water partitions into calcium perovskite or forms water rich aluminous phases. The presence of water in calcium perovskite has large effects on the preferred phase and can induce multiple phase transitions at varying depths of the <span class="hlt">mantle</span> depending upon both water content and slab temperature. These transitions are likely to be seismically anomalous and could cause large and characteristic seismic heterogeneity in descending slabs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V33A3072H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V33A3072H"><span>Testing Models for the Origin of the Earth-Moon System with 142Nd/144Nd Measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hyung, E.; Jacobsen, S. B.; Zeng, L.</p> <p>2015-12-01</p> <p>The Sm-Nd system is widely used for tracking the <span class="hlt">differentiation</span> and evolution of planetary silicate reservoirs, due to the well understood, strong Sm-Nd fractionation between melt and <span class="hlt">mantle</span> minerals. The short-lived 146Sm-142Nd system with a half-life of 103 Ma or 68 Ma has been used to constrain <span class="hlt">early</span> planetary <span class="hlt">differentiation</span> events based on <span class="hlt">early</span> Archean terrestrial rocks, lunar rocks and meteorites. <span class="hlt">Early</span> Archean terrestrial rocks show significant variations in 142Nd/144Nd of about 30 ppm, demonstrating very <span class="hlt">early</span> <span class="hlt">differentiation</span> of the Earth's <span class="hlt">mantle</span> and crust. In contrast, present day 142Nd/144Nd ratios of <span class="hlt">mantle</span>-derived ocean island basalts and MORBs show almost no variation at the reported analytical precision level (2σ = ± 6 ppm), suggesting that such <span class="hlt">early</span> variations have been erased with time due to crustal recycling and <span class="hlt">mantle</span> mixing. The 142Nd/144Nd ratio of the lunar <span class="hlt">mantle</span> has been reported to be offset from terrestrial standards by about -5 ppm, barely resolvable with the reported analytical uncertainties. Differences in the 142Nd/144Nd ratios between the bulk Earth and Moon may suggest <span class="hlt">early</span> large scale silicate <span class="hlt">differentiation</span> events on the Earth that predate the Giant Moon forming impact. To address this problem, we carry out new 142Nd/144Nd measurements of terrestrial rocks, and lunar rocks and meteorites with a TIMS (Isoprobe T) equipped with new Xact Faraday amplifiers provided by Isotopx. We find that the Xact amplifiers provide lower noise than the earlier generation preamplifiers and operate close to the theoretical thermodynamic noise limit calculated from the Johnson equation. So far we have been able to improve multidynamic measurements to be reproducible to within ± 2 ppm at the 2σ level, and with this precision we find no variations in a few young terrestrial rocks. Our next step is measurements of lunar rocks and E-chondrites. If these turn out to be identical to the modern Earth, then the Nd isotope system may tell the same</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.V52A..07I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.V52A..07I"><span>Osmium isotope variations in the Pacific <span class="hlt">mantle</span>: implications for the distribution of heterogeneity in the convecting <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ishikawa, A.; Senda, R.; Suzuki, K.; Tani, K.; Ishii, T.</p> <p>2015-12-01</p> <p>Recent accumulation of Os isotope data obtained either from abyssal peridotites or from ocean island peridotite xenoliths has clearly demonstrated that the modern convecting <span class="hlt">mantle</span> is substantially heterogeneous in Os-isotope composition. Unlike other radiogenic isotope heterogeneities observed in oceanic basalts, largely controlled by incorporation of recycled crustal materials, it seems likely that the observed range of Os-isotope compositions in oceanic peridotites directly reflect varying degrees of ancient melt extraction from peridotitic <span class="hlt">mantle</span>. Hence, global variations of Os-isotope compositions in oceanic peridotites may provide an important piece of information in unraveling the geochemical and geodynamic evolution of the convecting <span class="hlt">mantle</span>. Here we present the Os-isotope variations in peridotite-serpentinite recovered from the Pacific area because the number of data available is yet scarce when compared with data from other oceans (Atlantic, Arctic and Indian Ocean). Our primary purpose is to test whether <span class="hlt">mantle</span> domains underlying four major oceans are distinct in terms of Os isotope variations, reflecting the pattern of <span class="hlt">mantle</span> convection or mixing efficiency. We examined 187Os/188Os ratios and highly siderophile element concentrations in serpentinized harzburgite recovered from Hess Deep in the East Pacific Rise, a <span class="hlt">mantle</span> section in the Taitao ophiolite, Chile (Schulte et al., 2009), serpentinized harzburgite bodies in the Izu-Ogasawara and Tonga forearc (Parkinson et al., 1998), peridotite xenoliths from the Pali-Kaau vent in O'ahu island, Hawaii (Bizimis et al., 2007), and low-temperature type peridotite xenoliths from Malaita, Solomon Islands (Ishikawa et al., 2011). The results demonstrate that samples from each area display very similar Os-isotope variations with a pronounced peak in 187Os/188Os = 0.125-0.128. Moreover, the relatively larger datasets obtained from Hess Deep, Taitao and Malaita clearly exhibit the presence of secondary peak in 187Os</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008Litho.102..279F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008Litho.102..279F"><span><span class="hlt">Mantle</span> source volumes and the origin of the mid-Tertiary ignimbrite flare-up in the southern Rocky Mountains, western U.S.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Farmer, G. Lang; Bailley, Treasure; Elkins-Tanton, Linda T.</p> <p>2008-04-01</p> <p>Voluminous intermediate to silicic composition volcanic rocks were generated throughout the southern Rocky Mountains, western U.S., during the mid-Tertiary "ignimbrite flare-up", principally at the San Juan and Mogollon-Datil volcanic fields. At both volcanic centers, radiogenic isotope data have been interpreted as evidence that 50% or more of the volcanic rocks (by mass) were derived from <span class="hlt">mantle</span>-derived, mafic parental magmas, but no consensus exists as to whether melting was largely of lithospheric or sub-lithospheric <span class="hlt">mantle</span>. Recent xenolith studies, however, have revealed that thick (> 100 km), fertile, and hydrated continental lithosphere was present beneath at least portions of the southern Rocky Mountains during the mid-Tertiary. The presence of such thick <span class="hlt">mantle</span> lithosphere, combined with an apparent lack of syn-magmatic extension, leaves conductive heating of lithospheric <span class="hlt">mantle</span> as a plausible method of generating the mafic magmas that fueled the ignimbrite flare-up in this inland region. To further assess this possibility, we estimated the minimum volume of <span class="hlt">mantle</span> needed to generate the mafic magmas parental to the preserved mid-Tertiary igneous rocks. Conservative estimates of the <span class="hlt">mantle</span> source volumes that supplied the Mogollon-Datil and San Juan volcanic fields are ˜ 2 M km 3 and ˜ 7 M km 3, respectively. These volumes could have comprised only lithospheric <span class="hlt">mantle</span> if at least the lower ˜ 20 km of the <span class="hlt">mantle</span> lithosphere beneath the entire southern Rocky Mountains region underwent partial melting during the mid-Tertiary and if the resulting mafic magmas were drawn laterally for distances of up to ˜ 300 km into each center. Such widespread melting of lithospheric <span class="hlt">mantle</span> requires that the lithospheric <span class="hlt">mantle</span> have been uniformly fertile and primed for melting in the mid-Tertiary, a possibility if the lithospheric <span class="hlt">mantle</span> had experienced widespread hydration and refrigeration during <span class="hlt">early</span> Tertiary low angle subduction. Exposure of the <span class="hlt">mantle</span> lithosphere</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI41A0328N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI41A0328N"><span>Monte Carlo Models to Constrain Temperature Variation in the Lowermost <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nowacki, A.; Walker, A.; Davies, C. J.</p> <p>2017-12-01</p> <p>The three dimensional temperature variation in the lowermost <span class="hlt">mantle</span> is diagnostic of the pattern of <span class="hlt">mantle</span> convection and controls the extraction of heat from the outer core. Direct measurement of <span class="hlt">mantle</span> temperature is impossible and the temperature in the lowermost <span class="hlt">mantle</span> is poorly constrained. However, since temperature variations indirectly impact many geophysical observables, it is possible to isolate the thermal signal if <span class="hlt">mantle</span> composition and the physical properties of <span class="hlt">mantle</span> minerals are known. Here we describe a scheme that allows seismic, geodynamic, and thermal properties of the core and <span class="hlt">mantle</span> to be calculated given an assumed temperature (T) and mineralogical (X) distribution in the <span class="hlt">mantle</span> while making use of a self consistent parameterisation of the thermoelastic properties of <span class="hlt">mantle</span> minerals. For a given T and X, this scheme allows us to determine the misfit between our model and observations for the long-wavelength surface geoid, core-<span class="hlt">mantle</span> boundary topography, inner-core radius, total surface heat-flux and p- and s-wave tomography. The comparison is quick, taking much less than a second, and can accommodate uncertainty in the mineralogical parameterisation. This makes the scheme well-suited to use in a Monte Carlo approach to the determination of the long-wavelength temperature and composition of the lowermost <span class="hlt">mantle</span>. We present some initial results from our model, which include the robust generation of a thermal boundary layer in the one-dimensional thermal structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11834831','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11834831"><span>The <span class="hlt">mantle</span> flow field beneath western North America.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Silver, P G; Holt, W E</p> <p>2002-02-08</p> <p>Although motions at the surface of tectonic plates are well determined, the accompanying horizontal <span class="hlt">mantle</span> flow is not. We have combined observations of surface deformation and upper <span class="hlt">mantle</span> seismic anisotropy to estimate this flow field for western North America. We find that the <span class="hlt">mantle</span> velocity is 5.5 +/- 1.5 centimeters per year due east in a hot spot reference frame, nearly opposite to the direction of North American plate motion (west-southwest). The flow is only weakly coupled to the motion of the surface plate, producing a small drag force. This flow field is probably due to heterogeneity in <span class="hlt">mantle</span> density associated with the former Farallon oceanic plate beneath North America.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1812781P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1812781P"><span><span class="hlt">Mantle</span> xenoliths from Central Vietnam: evidence for at least Meso-Proterozoic formation of the lithospheric <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Proßegger, Peter; Ntaflos, Theodoros; Ackerman, Lukáš; Hauzenberger, Christoph; Tran, Tuan Anh</p> <p>2016-04-01</p> <p>Intraplate Cenozoic basalts that are widely dispersed along the continental margin of East Asia belong to the Western Pacific "diffuse" igneous province. They consist mainly of alkali basalts, basanites,rarely nephelinites, which are <span class="hlt">mantle</span> xenolith-bearing, potassic rocks and quartz tholeiites. The volcanism in this area has been attributed to the continental extension caused by the collision of India with Asia and by the subduction of the Pacific Ocean below Asia. We studied a suite of 24 <span class="hlt">mantle</span> xenoliths from La Bang Lake, Dak Doa district and Bien Ho, Pleiku city in the Gia Province, Central Vietnam. They are predominantly spinel lherzolites (19) but spinel harburgites (3) and two garnet pyroxenites are present as well. The sizes of the xenoliths range from 5 to 40 cm in diameter with medium to coarse-grained protogranular textures. Whole rock major and trace element analyses display a wide range of compositions. The MgO concentration varies from 36.0 to 45.8 wt% whereas Al2O3 and CaO range from 0.63 to 4.36 wt% and from 0.52 to 4.21 wt% (with one sample having CaO of 6.63 wt%) respectively. Both CaO and Al2O3 positively correlate with MgO most likely indicating that the sampled rocks were derived from a common <span class="hlt">mantle</span> source experienced variable degrees of partial melting. Mineral analyses show that the rock forming minerals are chemically homogeneous. The Fo contents of olivine vary between 89.2 and 91.2 and the Mg# of orthopyroxene and clinopyroxene range from 89 to 92 and 89 to 94 respectively. The range of Cr# for spinel is 0.06-0.26. Model calculations in both whole rock and clinopyroxenes show that lithospheric <span class="hlt">mantle</span> underneath Central Vietnam experienced melt extractions that vary between 2-7, 12-15 and 20-30%. The majority of the primitive <span class="hlt">mantle</span>-normalized whole rock and clinopyroxene REE patterns are parallel to each other indicating that clinopyroxene is the main repository of the trace elements. Clinopyroxenes are divided into two groups: group A</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI33A..01L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI33A..01L"><span>Preservation of Primordial <span class="hlt">Mantle</span> in the Aftermath of a Giant Impact</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lock, S. J.; Stewart, S. T.; Mukhopadhyay, S.</p> <p>2016-12-01</p> <p>Terrestrial planets experience a number of giant impacts in the final stages of accretion. These highly energetic events force planets into hot, partially vaporized, and occasionally rapidly-rotating states. However, recent measurements of Xe and W isotopes in <span class="hlt">mantle</span> plume-derived basalts imply that the terrestrial <span class="hlt">mantle</span> was not homogenized during this violent stage of Earth's accretion. Understanding the physical structure of post-impact states is key for interpreting these primitive <span class="hlt">mantle</span> signatures. Post-impact states are highly thermally stratified: the lowermost <span class="hlt">mantle</span> has lower entropy than the rest of the <span class="hlt">mantle</span>. Usually, the lowermost <span class="hlt">mantle</span> is near the solidus or partially molten. The high-entropy portion of the <span class="hlt">mantle</span> is super-liquidus, smoothly grading to a silicate vapor atmosphere. Here, we consider the competing processes acting on these distinct layers as the <span class="hlt">mantle</span> establishes a single thermal gradient. If the whole <span class="hlt">mantle</span> chemically mixed during cooling, then any pre-impact chemical signature would be erased. Previous work has neglected the critical time period between the highly vaporized post-impact state and a fully-condensed silicate body, i.e., a separated magma ocean and atmosphere. The post-impact structure cools rapidly by radiation from the photosphere, causing contraction of the body and redistribution of mass and angular momentum. One consequence of contraction is that the pressure in the <span class="hlt">mantle</span> increases significantly (on the order of several to 10s GPa at the core <span class="hlt">mantle</span> boundary) over 10s-1000s years. The increased pressure causes part of the <span class="hlt">mantle</span> to solidify. Significantly, the timescale for pressure-induced freezing is shorter than the timescale for thermal equilibration between the low and high entropy <span class="hlt">mantle</span> layers and the timescale for melt percolation (both >100s yrs). Therefore, pressure-induced freezing in the aftermath of a giant impact may be an important factor in preserving primordial Xe and W signatures in the lower</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18288192','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18288192"><span>Evidence of lower-<span class="hlt">mantle</span> slab penetration phases in plate motions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Goes, Saskia; Capitanio, Fabio A; Morra, Gabriele</p> <p>2008-02-21</p> <p>It is well accepted that subduction of the cold lithosphere is a crucial component of the Earth's plate tectonic style of <span class="hlt">mantle</span> convection. But whether and how subducting plates penetrate into the lower <span class="hlt">mantle</span> is the subject of continuing debate, which has substantial implications for the chemical and thermal evolution of the <span class="hlt">mantle</span>. Here we identify lower-<span class="hlt">mantle</span> slab penetration events by comparing Cenozoic plate motions at the Earth's main subduction zones with motions predicted by fully dynamic models of the upper-<span class="hlt">mantle</span> phase of subduction, driven solely by downgoing plate density. Whereas subduction of older, intrinsically denser, lithosphere occurs at rates consistent with the model, younger lithosphere (of ages less than about 60 Myr) often subducts up to two times faster, while trench motions are very low. We conclude that the most likely explanation is that older lithosphere, subducting under significant trench retreat, tends to lie down flat above the transition to the high-viscosity lower <span class="hlt">mantle</span>, whereas younger lithosphere, which is less able to drive trench retreat and deforms more readily, buckles and thickens. Slab thickening enhances buoyancy (volume times density) and thereby Stokes sinking velocity, thus facilitating fast lower-<span class="hlt">mantle</span> penetration. Such an interpretation is consistent with seismic images of the distribution of subducted material in upper and lower <span class="hlt">mantle</span>. Thus we identify a direct expression of time-dependent flow between the upper and lower <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V32A..03B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V32A..03B"><span>The paradox of a wet (high H2O) and dry (low H2O/Ce) <span class="hlt">mantle</span>: High water concentrations in <span class="hlt">mantle</span> garnet pyroxenites from Hawaii</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bizimis, M.; Peslier, A. H.</p> <p>2013-12-01</p> <p>Water dissolved as trace amounts in anhydrous minerals has a large influence on the melting behavior and physical properties of the <span class="hlt">mantle</span>. The water concentration of the oceanic <span class="hlt">mantle</span> is inferred from the analyses of MORB and OIB [1], but there is little data from actual <span class="hlt">mantle</span> samples. Moreover, enriched mineralogies (pyroxenites, eclogites) are thought as important sources of heterogeneity in the <span class="hlt">mantle</span>, but their water concentrations and their effect on the water budget and cycling in the <span class="hlt">mantle</span> are virtually unknown. We analyzed by FTIR water concentrations in garnet clinopyroxenite xenoliths from Salt Lake Crater, Oahu, Hawaii. These pyroxenites are high-pressure (>20kb) crystal fractionates from alkalic melts. The clinopyroxenes (cpx) have 260 to 576 ppm wt. H2O, with the least <span class="hlt">differentiated</span> samples (Mg#>0.8) in the 400-500 ppm range. Orthopyroxene (opx) contain 117-265 ppm H2O, about half of that of cpx, consistent with other natural sample studies, but lower than experimental cpx/opx equilibrium data. These pyroxenite cpx and opx water concentrations are at the high-end of on-and off-craton peridotite xenolith concentrations and megacrysts from kimberites [2] and those of Hawaiian spinel peridotites. In contrast, garnet has extremely low water contents (<5ppm H2O). There is no correlation between water in cpx and lithophile element concentrations. Phlogopite is present in some samples, and its modal abundance shows a positive correlation in Mg# with cpx, implying equilibrium. However, there is no correlation between water concentrations and the presence of phlogopite. These data imply that cpx and opx water concentrations may be buffered by phlogopite crystallization. Reconstructed bulk rock pyroxenite water concentrations (not including phlogopite, i.e. minimum) range from 200-460 ppm (average 331× 75 ppm), significantly higher than water estimates for the MORB source (50-200 ppm), but in the range of E-MORB, OIB and the source of rejuvenated Hawaiian</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMDI13D2456M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMDI13D2456M"><span>Circulation of carbon dioxide in the <span class="hlt">mantle</span>: multiscale modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morra, G.; Yuen, D. A.; Lee, S.</p> <p>2012-12-01</p> <p>Much speculation has been put forward on the quantity and nature of carbon reservoirs in the deep Earth, because of its involvement in the evolution of life at the surface and inside planetary interiors. Carbon penetrates into the Earth's <span class="hlt">mantle</span> mostly during subduction of oceanic crust, which contains carbonate deposits [1], however the form that it assumes at lower <span class="hlt">mantle</span> depths is scarcely understood [2], hampering our ability to estimate the amount of carbon in the entire <span class="hlt">mantle</span> by orders of magnitude. We present simulations of spontaneous degassing of supercritical CO2 using in-house developed novel implementations of the Fast-Multipole Boundary Element Method suitable for modeling two-phase flow (here <span class="hlt">mantle</span> mineral and free CO2 fluid) through disordered materials such as porous rocks. Because the mutual interaction of droplets immersed either in a fluid or a solid matrix and their weakening effect to the host rock alters the strength of the <span class="hlt">mantle</span> rocks, at the large scale the fluid phases in the <span class="hlt">mantle</span> may control the creeping of <span class="hlt">mantle</span> rocks [3]. In particular our study focuses on the percolation of supercritical CO2, estimated through the solution of the Laplace equation in a porous system, stochastically generated through a series of random Karhunen-Loeve decomposition. The model outcome is employed to extract the transmissivity of supercritical fluids in the <span class="hlt">mantle</span> from the lowest scale up to the <span class="hlt">mantle</span> scale and in combination with the creeping flow of the convecting <span class="hlt">mantle</span>. The emerging scenarios on the global carbon cycle are finally discussed. [1] Boulard, E., et al., New host for carbon in the deep Earth. Proceedings of the National Academy of Sciences, 2011. 108(13): p. 5184-5187. [2] Walter, M.J., et al., Deep <span class="hlt">Mantle</span> Cycling of Oceanic Crust: Evidence from Diamonds and Their Mineral Inclusions. Science, 2011. 334(6052): p. 54-57. [3] Morra, G., et al., Ascent of Bubbles in Magma Conduits Using Boundary Elements and Particles. Procedia Computer</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Litho.282..326G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Litho.282..326G"><span>Age and evolution of the lithospheric <span class="hlt">mantle</span> beneath the Khanka Massif: Geochemical and Re-Os isotopic evidence from Sviyagino <span class="hlt">mantle</span> xenoliths</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Peng; Xu, Wen-Liang; Wang, Chun-Guang; Wang, Feng; Ge, Wen-Chun; Sorokin, A. A.; Wang, Zhi-Wei</p> <p>2017-06-01</p> <p>New geochemical and Re-Os isotopic data of <span class="hlt">mantle</span> xenoliths entrained in Cenozoic Sviyagino alkali basalts from the Russian Far East provide insights into the age and evolution of the sub-continental lithospheric <span class="hlt">mantle</span> (SCLM) beneath the Khanka Massif, within the Central Asian Orogenic Belt (CAOB). These <span class="hlt">mantle</span> xenoliths are predominantly spinel lherzolites with minor spinel harzburgite. The lherzolites contain high whole-rock concentrations of Al2O3 and CaO, with low forsterite content in olivine (Fo = 89.5-90.3%) and low Cr# in spinel (0.09-0.11). By contrast, the harzburgite is more refractory, containing lower whole rock Al2O3 and CaO contents, with higher Fo (91.3%) and spinel Cr# (0.28). Their whole rock and mineral compositions suggest that the lherzolites experienced low-degree (1-4%) batch melting and negligible metasomatism, whereas the harzburgite underwent a higher degree (10%) of fractional melting, and experienced minor post-melting silicate metasomatism. Two-pyroxene rare earth element (REE)-based thermometry (TREE) yields predominant equilibrium temperatures of 884-1043 °C, similar to values obtained from two-pyroxene major element-based thermometry (TBKN = 942-1054 °C). Two lherzolite samples yield high TREE relative to TBKN (TREE - TBKN ≥ 71 °C), suggesting that they cooled rapidly as a result of the upwelling of hot asthenospheric <span class="hlt">mantle</span> material that underplated a cold ancient lithosphere. The harzburgite with a low Re/Os value has an 187Os/188Os ratio of 0.11458, yielding an Os model age (TMA) relative to the primitive upper <span class="hlt">mantle</span> (PUM) of 2.09 Ga, and a Re depletion ages (TRD) of 1.91 Ga; both of which record ancient melt depletion during the Paleoproterozoic ( 2.0 Ga). The 187Os/188Os values of lherzolites (0.12411-0.12924) correlate well with bulk Al2O3 concentrations and record the physical mixing of ancient <span class="hlt">mantle</span> domains and PUM-like ambient <span class="hlt">mantle</span> material within the asthenosphere. This indicates that the SCLM beneath the Khanka</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.V41F..07V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.V41F..07V"><span>Archean Pb Isotope Evolution: Implications for the <span class="hlt">Early</span> Earth.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vervoort, J. D.; Thorpe, R.; Albarede, F.; Blichert-Toft, J.</p> <p>2008-12-01</p> <p>.728 Ga (Normetal) to 2.70 Ga (Noranda). The Pb isotopic compositions from these galenas, when normalized to a common age of 2.7 Ga, define a highly linear array in 207Pb/204Pb vs. 206Pb/204Pb. This array is nearly coincident with the 2.7 Ga geochron with a slope that corresponds to an age of ~4.4 Ga and with an extraordinary large range of 207Pb/204Pb, about the same magnitude as modern MORB. These data have important implications for the evolution of the Archean <span class="hlt">mantle</span>. First, the slope of the Abitibi Pb-Pb array and its coincidence with the 2.7 Ga geochron suggests widespread U-Pb <span class="hlt">differentiation</span> within the first hundred million years of Earth's history. This may have been due to either core formation or silicate/melt <span class="hlt">differentiation</span> due to widespread melting of the <span class="hlt">mantle</span> (e.g., formation of a magma ocean). Second, variations in μ in the Abitibi <span class="hlt">mantle</span> and the subsequent Pb isotopic heterogeneities, whatever their cause, have not been significantly changed from 4.4 until 2.7 Ga. This implies that changes in μ in the Abitibi <span class="hlt">mantle</span> source between 4.4 and 2.7 Ga, such as would be caused by crust extraction or recycling of older crust into this region of the <span class="hlt">mantle</span>, were insufficient to destroy the original μ variations created at 4.4 Ga. Therefore, it appears that this portion of the <span class="hlt">mantle</span> had essentially remained isolated and undisturbed from the <span class="hlt">early</span> Hadean until the late Archean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI11A2339M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI11A2339M"><span>Recycling Seamounts: Implications for <span class="hlt">Mantle</span> Source Heterogeneities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Madrigal, P.; Gazel, E.</p> <p>2016-12-01</p> <p>Isolated seamounts formed away from plate boundaries and/or known hotspot tracks are widely distributed in the Earth's oceanic plates. Despite their pervasiveness, the origin and composition of the magmatic sources that create these seamounts are still unknown. Moreover, as the seamount provinces travel along with the oceanic plate towards subduction trenches these volcanic edifices become subducted materials that are later recycled into the <span class="hlt">mantle</span>. Using radiogenic isotopes (Sr-Nd-Pb) from present-day non-plume ocean island basalts (OIB) sampled by drilling and dredging as well as by normal processes of accretion to subduction margins, we modeled the isotopic evolution of these enriched reservoirs to assess their role as discrete components contributing to upper <span class="hlt">mantle</span> heterogeneity. Our evidence suggests that a highly enriched <span class="hlt">mantle</span> reservoir can originate from OIB-type subducted material that gets incorporated and stirred throughout the upper <span class="hlt">mantle</span> in a shorter time period ( 200 Ma-500 Ma) than other highly enriched components like ancient subducted oceanic crust (>1 Ga), thought to be the forming agent of the HIMU <span class="hlt">mantle</span> reservoir endmember. Enriched signatures from intraplate volcanism can be described by mixing of a depleted component like DMM and an enriched reservoir like non-plume related seamounts. Our data suggests that the isotopic evolution in time of a seamount-province type of reservoir can acquire sufficiently enriched compositions to resemble some of the most enriched magmas on Earth. This "fast-forming" (between 200 and 500 Ma) enriched reservoir could also explain some of the enriched signatures commonly present in intraplate and EMORB magmas unrelated to deep <span class="hlt">mantle</span> plume upwellings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.V23E0689A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.V23E0689A"><span>Isotopic Evidence For Chaotic Imprint In The Upper <span class="hlt">Mantle</span> Heterogeneity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Armienti, P.; Gasperini, D.</p> <p>2006-12-01</p> <p>Heterogeneities of the asthenospheric <span class="hlt">mantle</span> along mid-ocean ridges have been documented as the ultimate effect of complex processes dominated by temperature, pressure and composition of the shallow <span class="hlt">mantle</span>, in a convective regime that involves mass transfer from the deep <span class="hlt">mantle</span>, occasionally disturbed by the occurrence of hot spots (e.g. Graham et al., 2001; Agranier et al., 2005; Debaille et al., 2006). Alternatively, upper <span class="hlt">mantle</span> heterogeneity is seen as the natural result of basically athermal processes that are intrinsic to plate tectonics, such as delamination and recycling of continental crust and of subducted aseismic ridges (Meibom and Anderson, 2003; Anderson, 2006). Here we discuss whether the theory of chaotic dynamical systems applied to isotopic space series along the Mid-Atlantic Ridge (MAR) and the East Pacific Rise (EPR) can delimit the length-scale of upper <span class="hlt">mantle</span> heterogeneities, then if the model of marble-cake <span class="hlt">mantle</span> (Allègre and Turcotte, 1986) is consistent with a fractal distribution of such heterogeneity. The correlations between the isotopic (Sr, Nd, Hf, Pb) composition of MORB were parameterized as a function of the ridge length. We found that the distribution of isotopic heterogenity along both the MAR and EPR is self- similar in the range of 7000-9000 km. Self-similarity is the imprint of chaotic <span class="hlt">mantle</span> processes. The existence of strange attractors in the distribution of isotopic composition of the asthenosphere sampled at ridge crests reveals recursion of the same <span class="hlt">mantle</span> process(es), endured over long periods of time, up to a stationary state. The occurrence of the same fractal dimension for both the MAR and EPR implies independency of contingent events, suggesting common <span class="hlt">mantle</span> processes, on a planetary scale. We envisage the cyclic route of "melting, melt extraction and recycling" as the main <span class="hlt">mantle</span> process which could be able to induce scale invariance. It should have happened for a significant number of times over the Earth</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150003055','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150003055"><span>Water Distribution in the Continental and Oceanic Upper <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peslier, Anne H.</p> <p>2015-01-01</p> <p>Nominally anhydrous minerals such as olivine, pyroxene and garnet can accommodate tens to hundreds of ppm H2O in the form of hydrogen bonded to structural oxygen in lattice defects. Although in seemingly small amounts, this water can significantly alter chemical and physical properties of the minerals and rocks. Water in particular can modify their rheological properties and its distribution in the <span class="hlt">mantle</span> derives from melting and metasomatic processes and lithology repartition (pyroxenite vs peridotite). These effects will be examined here using Fourier transform infrared spectrometry (FTIR) water analyses on minerals from <span class="hlt">mantle</span> xenoliths from cratons, plume-influenced cratons and oceanic settings. In particular, our results on xenoliths from three different cratons will be compared. Each craton has a different water distribution and only the <span class="hlt">mantle</span> root of Kaapvaal has evidence for dry olivine at its base. This challenges the link between olivine water content and survival of Archean cratonic <span class="hlt">mantle</span>, and questions whether xenoliths are representative of the whole cratonic <span class="hlt">mantle</span>. We will also present our latest data on Hawaii and Tanzanian craton xenoliths which both suggest the intriguing result that <span class="hlt">mantle</span> lithosphere is not enriched in water when it interacts with melts from deep <span class="hlt">mantle</span> upwellings (plumes).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI11A2336R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI11A2336R"><span><span class="hlt">Mantle</span> mixing and thermal evolution during Pangaea assembly and breakup</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rudolph, M. L.; Li, M.; Zhong, S.; Manga, M.</p> <p>2016-12-01</p> <p>Continents insulate the underlying <span class="hlt">mantle</span>, and it has been suggested that the arrangement of the continents can have a significant effect on sub-continental <span class="hlt">mantle</span> temperatures. Additionally, the dispersal or agglomeration of continents may affect the efficacy of continental insulation, with some studies suggesting warming of 100K beneath supercontinents. During the most recent supercontinent cycle, Pangaea was encircled by subduction, potentially creating a `curtain' of subducted material that may have prevented mixing of the sub-Pangaea <span class="hlt">mantle</span> with the sub-Panthalassa <span class="hlt">mantle</span>. Using 3D spherical shell geometry <span class="hlt">mantle</span> convection simulations, we quantify the effect of insulation by continents and supercontinents. We explore the differences in model predictions for purely thermal vs. thermochemical convection, and we use tracers to quantify the exchange of material between the sub-oceanic to the sub-continental <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T41A0588H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T41A0588H"><span><span class="hlt">Mantle</span> Flow Induced by Subduction Beneath Taurides Mountains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hui, H.; Sandvol, E. A.; Rey, P. F.; Brocard, G. Y.</p> <p>2017-12-01</p> <p>GPS data of Anatolian Plateau shows westward plate motion with respect to the Eurasian plate at a rate of approximately 20 mm/yr, however, the fast direction of shear-wave splitting data in Anatolian Plateau is dominantly northeast-southwest, with significant variations around the central Taurides Mountains. To address the decoupling between the deformation in the crust and in the <span class="hlt">mantle</span>, we explore the <span class="hlt">mantle</span> strain pattern beneath Anatoian Plateau. Numerical models of the African plate subducting beneath the Taurides have been constructed with the open source code Underworld by Louis Moresi and the Lithospheric Modeling Recipe by EarthByte Group. We have constructed a 2-D model with dimension of 400km × 480km with 60km thick plate subducting into the <span class="hlt">mantle</span>. In our numerical model, we observe a poloidal component of the <span class="hlt">mantle</span> flow around the edge of the subducting plate, which could be explained by straight-forward corner flow. The horizontal component of <span class="hlt">mantle</span> flow above the subducting plate may explain the shear-wave splitting pattern that is nearly perpendicular to the trench at Anatolia. We are also working on 3-D models with dimension of 400km×400km×480km with the subducting plate width 100km. The asthenospheric <span class="hlt">mantle</span> below the subducting plate exhibits a flow parallel to the trench, then rotates around the edge of the plate and becomes perpendicular to the trench. This <span class="hlt">mantle</span> flow pattern may explain the shear-wave splitting directions in central Anatolia.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4570G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4570G"><span>Reconstructing <span class="hlt">mantle</span> heterogeneity with data assimilation based on the back-and-forth nudging method: Implications for <span class="hlt">mantle</span>-dynamic fitting of past plate motions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Glišović, Petar; Forte, Alessandro</p> <p>2016-04-01</p> <p>The paleo-distribution of density variations throughout the <span class="hlt">mantle</span> is unknown. To address this question, we reconstruct 3-D <span class="hlt">mantle</span> structure over the Cenozoic era using a data assimilation method that implements a new back-and-forth nudging algorithm. For this purpose, we employ convection models for a compressible and self-gravitating <span class="hlt">mantle</span> that employ 3-D <span class="hlt">mantle</span> structure derived from joint seismic-geodynamic tomography as a starting condition. These convection models are then integrated backwards in time and are required to match geologic estimates of past plate motions derived from marine magnetic data. Our implementation of the nudging algorithm limits the difference between a reconstruction (backward-in-time solution) and a prediction (forward-in-time solution) on over a sequence of 5-million-year time windows that span the Cenozoic. We find that forward integration of reconstructed <span class="hlt">mantle</span> heterogeneity that is constrained to match past plate motions delivers relatively poor fits to the seismic-tomographic inference of present-day <span class="hlt">mantle</span> heterogeneity in the upper <span class="hlt">mantle</span>. We suggest that uncertainties in the past plate motions, related for example to plate reorganization episodes, could partly contribute to the poor match between predicted and observed present-day heterogeneity. We propose that convection models that allow tectonic plates to evolve freely in accord with the buoyancy forces and rheological structure in the <span class="hlt">mantle</span> could provide additional constraints on geologic estimates of paleo-configurations of the major tectonic plates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR31A0435T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR31A0435T"><span>Development of Capabilities for New Experimental Studies on the Elasticity and Rheology of Lower <span class="hlt">Mantle</span> Minerals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Triplett, R.; Weidner, D.; Whitaker, M. L.; Chen, H.; Li, L.</p> <p>2017-12-01</p> <p>Key mineralogical components of the mid-<span class="hlt">mantle</span> of the Earth have historically been difficult to obtain elasticity data on because they either cannot be recovered to ambient conditions (e.g. calcium silicate perovskite) or back-transform during experimental preparation (e.g. magnesium silicate perovskite). Recently the conditions of the mid-<span class="hlt">mantle</span> (14+ GPa, 1500+ K) and even of the lower <span class="hlt">mantle</span> (24+ GPa, 1800+ K) have become reachable using multi-anvil apparatuses (MAA) with in-situ synchrotron x-ray capabilities, but the capabilities of these facilities have not yet fully matured. Examples include that reaching such pressures typically results in samples that are too small for ultrasonics, the few ultrasonics experiments done at these conditions have extremely limited x-ray visibility, and rheological experiments that apply <span class="hlt">differential</span> stress have not been done at these conditions on large volume samples. The pressure reachable in a Large Volume Press (LVP) is limited by the properties of available ultra-hard (UH) materials such as tungsten carbide (WC) and x-ray transparent polycrystalline diamond (PCD) and cubic boron nitride (cBN). A key factor is the interaction of 1st stage anvils and anvils of UH materials; obtaining WC anvils of larger size is prohibitive in both capability and cost, and anvils of hardened steel are limited in the tonnage that can be applied before damage occurs. Other complications include the difference in compressibility between WC and PCD/cBN anvils and the availability of WC with simultaneous high compressive strength (pressure gain per tonnage) and high transverse rupture strength (lower chance of blowout and reusability). The DT25 press to be used at the new NSLS-II beamline XPD-D is a Kawaii-style LVP MAA which accepts 25 mm UH 2nd-stage anvils and has the capability to apply a <span class="hlt">differential</span> load while at extreme conditions. We report on our development of techniques to do new and expanded experiments at lower <span class="hlt">mantle</span> conditions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890004472','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890004472"><span>Driving forces: Slab subduction and <span class="hlt">mantle</span> convection</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hager, Bradford H.</p> <p>1988-01-01</p> <p><span class="hlt">Mantle</span> convection is the mechanism ultimately responsible for most geological activity at Earth's surface. To zeroth order, the lithosphere is the cold outer thermal boundary layer of the convecting <span class="hlt">mantle</span>. Subduction of cold dense lithosphere provides tha major source of negative buoyancy driving <span class="hlt">mantle</span> convection and, hence, surface tectonics. There are, however, importnat differences between plate tectonics and the more familiar convecting systems observed in the laboratory. Most important, the temperature dependence of the effective viscosity of <span class="hlt">mantle</span> rocks makes the thermal boundary layer mechanically strong, leading to nearly rigid plates. This strength stabilizes the cold boundary layer against small amplitude perturbations and allows it to store substantial gravitational potential energy. Paradoxically, through going faults at subduction zones make the lithosphere there locally weak, allowing rapid convergence, unlike what is observed in laboratory experiments using fluids with temperature dependent viscosities. This bimodal strength distribution of the lithosphere distinguishes plate tectonics from simple convection experiments. In addition, Earth has a buoyant, relatively weak layer (the crust) occupying the upper part of the thermal boundary layer. Phase changes lead to extra sources of heat and bouyancy. These phenomena lead to observed richness of behavior of the plate tectonic style of <span class="hlt">mantle</span> convection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1911542M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1911542M"><span>Understanding how the shape and spatial distribution of ULVZs provides insight into their cause and to the nature of global-scale <span class="hlt">mantle</span> convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McNamara, Allen; Li, Mingming; Garnero, Ed; Marin, Nicole</p> <p>2017-04-01</p> <p>Seismic observations of the lower <span class="hlt">mantle</span> infer multiple scales of compositional heterogeneity. The largest-scale heterogeneity, observed in seismic tomography models, is in the form of large, nearly antipodal regions referred to as the Large Low Shear Velocity Provinces (LLSVPs). In contrast, diffracted wave and core-reflection precursor seismic studies reveal small-scale Ultra Low Velocity Zones (ULVZs) at the base of the <span class="hlt">mantle</span> that are almost two orders of magnitude smaller than the LLSVPs. We hypothesize that ULVZs provide insight into the nature of LLSVPs, and the LLSVPs, in turn, provide clues to the nature of global-scale <span class="hlt">mantle</span> convection and compositional state. However, both LLSVPs and ULVZs are observations, and it remains unclear what is causing them. Here, we examine several related questions to aid in understanding their cause and the dynamical processes associated with them. Can we use seismic observations of ULVZ locations to <span class="hlt">differentiate</span> whether they are caused by compositional heterogeneity or simply partial melting in otherwise normal <span class="hlt">mantle</span>? Can we use the map-view shape of ULVZs to tell us about lowermost <span class="hlt">mantle</span> flow directions and the temporal stability of these flow directions? Can the cross-sectional morphology of ULVZs tell us something about the viscosity difference between LLSVPs and background <span class="hlt">mantle</span>? We performed geodynamical experiments to help answer these questions. We find that ULVZs caused by compositional heterogeneity preferentially form patch-like shapes along the margins of LLSVPs. Rounded patches indicate regions with long-lived stable <span class="hlt">mantle</span> flow patterns, and linear patches indicate changing <span class="hlt">mantle</span> flow patterns. Typically, these ULVZ patches have an asymmetrical cross-sectional shape; however, if LLSVPs have a larger grain-size than background <span class="hlt">mantle</span>, their increased diffusion creep viscosity will act to make them more symmetrical. Alternatively, ULVZs caused simply by partial melting of normal <span class="hlt">mantle</span> are preferentially</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Tectp.737....1P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Tectp.737....1P"><span>Petrology and geochemistry of the Tasse <span class="hlt">mantle</span> xenoliths of the Canadian Cordillera: A record of Archean to Quaternary <span class="hlt">mantle</span> growth, metasomatism, removal, and melting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Polat, Ali; Frei, Robert; Longstaffe, Fred J.; Thorkelson, Derek J.; Friedman, Eyal</p> <p>2018-07-01</p> <p><span class="hlt">Mantle</span> xenoliths hosted by the Quaternary Tasse alkaline basalts in the Canadian Cordillera, southeastern British Columbia, are mostly spinel lherzolite originating from subcontinental lithospheric <span class="hlt">mantle</span>. The xenoliths contain abundant feldspar veins, melt pockets and spongy clinopyroxene, recording extensive alkaline metasomatism and partial melting. Feldspar occurs as veins and interstitial crystal in melt pockets. Melt pockets occur mainly at triple junctions, along grain boundaries, and consist mainly of olivine, cpx, opx and spinel surrounded by interstitial feldspar. The Nd, Sr and Pb isotopic compositions of the xenoliths indicate that their sources are characterized by variable mixtures of depleted MORB <span class="hlt">mantle</span> and EM1 and EM2 <span class="hlt">mantle</span> components. Large variations in εNd values (-8.2 to +9.6) and Nd depleted <span class="hlt">mantle</span> model ages (TDM = 66 to 3380 Ma) are consistent with multiple sources and melt extraction events, and long-term (>3300 Ma) isolation of some source regions from the convecting <span class="hlt">mantle</span>. Samples with Archean and Paleoproterozoic Nd model ages are interpreted as either have been derived from relict Laurentian <span class="hlt">mantle</span> pieces beneath the Cordillera or have been eroded from the root of the Laurentian craton to the east and transported to the base of the Cordilleran lithosphere by edge-driven convection currents. The oxygen isotope compositions of the xenoliths (average δ18O = +5.1 ± 0.5‰) are similar to those of depleted <span class="hlt">mantle</span>. The average δ18O values of olivine (+5.0 ± 0.2‰), opx (+5.9 ± 0.6‰), cpx (+6.0 ± 0.6‰) and spinel (+4.5 ± 0.2‰) are similar to <span class="hlt">mantle</span> values. Large fractionations for olivine-opx, olivine-cpx and opx-cpx pairs, however, reflect disequilibrium stemming from metasomatism and partial melting. Whole-rock trace element, Nd, Sr, Pb and O isotope compositions of the xenoliths and host alkaline basalts indicate different <span class="hlt">mantle</span> sources for these two suites of rocks. The xenoliths were derived from shallow lithospheric</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010090463&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearths%2Bouter%2Bcore','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010090463&hterms=earths+outer+core&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dearths%2Bouter%2Bcore"><span>Geodynamo Modeling of Core-<span class="hlt">Mantle</span> Interactions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuang, Wei-Jia; Chao, Benjamin F.; Smith, David E. (Technical Monitor)</p> <p>2001-01-01</p> <p>Angular momentum exchange between the Earth's <span class="hlt">mantle</span> and core influences the Earth's rotation on time scales of decades and longer, in particular in the length of day (LOD) which have been measured with progressively increasing accuracy for the last two centuries. There are four possible coupling mechanisms for transferring the axial angular momentum across the core-<span class="hlt">mantle</span> boundary (CMB): viscous, magnetic, topography, and gravitational torques. Here we use our scalable, modularized, fully dynamic geodynamo model for the core to assess the importance of these torques. This numerical model, as an extension of the Kuang-Bloxham model that has successfully simulated the generation of the Earth's magnetic field, is used to obtain numerical results in various physical conditions in terms of specific parameterization consistent with the dynamical processes in the fluid outer core. The results show that depending on the electrical conductivity of the lower <span class="hlt">mantle</span> and the amplitude of the boundary topography at CMB, both magnetic and topographic couplings can contribute significantly to the angular momentum exchange. This implies that the core-<span class="hlt">mantle</span> interactions are far more complex than has been assumed and that there is unlikely a single dominant coupling mechanism for the observed decadal LOD variation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140007370','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140007370"><span>Core-<span class="hlt">Mantle</span> Partitioning of Volatile Elements and the Origin of Volatile Elements in Earth and Moon</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Righter, K.; Pando, K.; Danielson, L.; Nickodem, K.</p> <p>2014-01-01</p> <p>Depletions of siderophile elements in <span class="hlt">mantles</span> have placed constraints on the conditions on core segregation and <span class="hlt">differentiation</span> in bodies such as Earth, Earth's Moon, Mars, and asteroid 4 Vesta. Among the siderophile elements there are a sub-set that are also volatile (volatile siderophile elements or VSE; Ga, Ge, In, As, Sb, Sn, Bi, Zn, Cu, Cd), and thus can help to constrain the origin of volatile elements in these bodies, and in particular the Earth and Moon. One of the fundamental observations of the geochemistry of the Moon is the overall depletion of volatile elements relative to the Earth, but a satisfactory explanation has remained elusive. Hypotheses for Earth include addition during accretion and core formation and mobilized into the metallic core, multiple stage origin, or addition after the core formed. Any explanation for volatile elements in the Earth's <span class="hlt">mantle</span> must also be linked to an explanation of these elements in the lunar <span class="hlt">mantle</span>. New metal-silicate partitioning data will be applied to the origin of volatile elements in both the Earth and Moon, and will evaluate theories for exogenous versus endogenous origin of volatile elements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMDI21A4272D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMDI21A4272D"><span>The Fate of Sulfur during Decompression Melting of Peridotite and Crystallization of Basalts - Implications for Sulfur Geochemistry of MORB and the Earth's Upper <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ding, S.; Dasgupta, R.</p> <p>2014-12-01</p> <p>Magmatism in mid-ocean ridges is the main pathway of sulfur (S) from the Earth's <span class="hlt">mantle</span> to the surficial reservoir. MORB is generally considered sulfide saturated due to the positive correlation between S and FeOT concentration (e.g., [1]). However, most MORBs are <span class="hlt">differentiated</span>, and both S content and sulfur concentration at sulfide saturation (SCSS) change with P, T, and magma composition (e.g., [2]). Therefore, it remains uncertain, from the MORB chemistry alone, whether <span class="hlt">mantle</span> melts parental to MORB are sulfide saturated. In this study, we modeled the behavior of S during isentropic partial melting of a fertile peridotite using pMELTS [3] and an SCSS parameterization [4]. Our results show that during decompression melting, at a fixed <span class="hlt">mantle</span> potential temperature, TP (e.g., 1300 °C), SCSS of aggregate melt first slightly increases then decreases at shallower depth with total variation <200 ppm. However, an increase of TP results in a significant increase of SCSS of primitive melts. Our model shows that at 15% melting (F), sulfide in the residue is exhausted for a <span class="hlt">mantle</span> with <200 ppm S. The resulted sulfide-undersaturated partial melts contain <1000 ppm S and are 4-6 times enriched in Cu compared to the source. In order to compare our modeled results directly to the <span class="hlt">differentiated</span> basalts, isobaric crystallization calculation was performed on 5, 10, and 15% aggregate melts. SCSS changes along liquid line of descent with a decrease in T and increase in FeOT. Comparison of S contents between the model results and MORB glasses [5] reveals that many MORBs derive from sulfide undersaturated melts. Further, for a TP of 1300-1350 °C and F of 10-15 wt.%, reproduction of self-consistent S, and Cu budget of many MORB glasses requires that S of their <span class="hlt">mantle</span> source be ~25-200 ppm. We will discuss the interplay of TP, average F, and the conditions of <span class="hlt">differentiation</span> to bracket the S geochemistry of MORB and MORB source <span class="hlt">mantle</span> and develop similar systematics for OIBs and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011GeoRL..3820306B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011GeoRL..3820306B"><span>Vertical coherence in <span class="hlt">mantle</span> heterogeneity from global seismic data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boschi, L.; Becker, T. W.</p> <p>2011-10-01</p> <p>The vertical coherence of <span class="hlt">mantle</span> structure is of importance for a range of dynamic issues including convective mass transport and the geochemical evolution of Earth. Here, we use seismic data to infer the most likely depth ranges of strong, global changes in the horizontal pattern of <span class="hlt">mantle</span> heterogeneity. We apply our algorithm to a comprehensive set of measurements, including various shear- and compressional-wave delay times and Love- and Rayleigh-wave fundamental mode and overtone dispersion, so that tomography resolution is as high as possible at all <span class="hlt">mantle</span> depths. We find that vertical coherence is minimum at ∼100 km and ∼800 km depths, corresponding to the base of the lithosphere and the transition between upper and lower <span class="hlt">mantle</span>, respectively. The D″ layer is visible, but not as prominent as the shallower features. The rest of the lower <span class="hlt">mantle</span> is, essentially, vertically coherent. These findings are consistent with slab stagnation at depths around, and perhaps below, the 660-km phase transition, and inconsistent with global, chemically distinct, mid-<span class="hlt">mantle</span> layering.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5493751','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5493751"><span>Clustering of arc volcanoes caused by temperature perturbations in the back-arc <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lee, Changyeol; Wada, Ikuko</p> <p>2017-01-01</p> <p>Clustering of arc volcanoes in subduction zones indicates along-arc variation in the physical condition of the underlying <span class="hlt">mantle</span> where majority of arc magmas are generated. The sub-arc <span class="hlt">mantle</span> is brought in from the back-arc largely by slab-driven <span class="hlt">mantle</span> wedge flow. Dynamic processes in the back-arc, such as small-scale <span class="hlt">mantle</span> convection, are likely to cause lateral variations in the back-arc <span class="hlt">mantle</span> temperature. Here we use a simple three-dimensional numerical model to quantify the effects of back-arc temperature perturbations on the <span class="hlt">mantle</span> wedge flow pattern and sub-arc <span class="hlt">mantle</span> temperature. Our model calculations show that relatively small temperature perturbations in the back-arc result in vigorous inflow of hotter <span class="hlt">mantle</span> and subdued inflow of colder <span class="hlt">mantle</span> beneath the arc due to the temperature dependence of the <span class="hlt">mantle</span> viscosity. This causes a three-dimensional <span class="hlt">mantle</span> flow pattern that amplifies the along-arc variations in the sub-arc <span class="hlt">mantle</span> temperature, providing a simple mechanism for volcano clustering. PMID:28660880</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28660880','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28660880"><span>Clustering of arc volcanoes caused by temperature perturbations in the back-arc <span class="hlt">mantle</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Changyeol; Wada, Ikuko</p> <p>2017-06-29</p> <p>Clustering of arc volcanoes in subduction zones indicates along-arc variation in the physical condition of the underlying <span class="hlt">mantle</span> where majority of arc magmas are generated. The sub-arc <span class="hlt">mantle</span> is brought in from the back-arc largely by slab-driven <span class="hlt">mantle</span> wedge flow. Dynamic processes in the back-arc, such as small-scale <span class="hlt">mantle</span> convection, are likely to cause lateral variations in the back-arc <span class="hlt">mantle</span> temperature. Here we use a simple three-dimensional numerical model to quantify the effects of back-arc temperature perturbations on the <span class="hlt">mantle</span> wedge flow pattern and sub-arc <span class="hlt">mantle</span> temperature. Our model calculations show that relatively small temperature perturbations in the back-arc result in vigorous inflow of hotter <span class="hlt">mantle</span> and subdued inflow of colder <span class="hlt">mantle</span> beneath the arc due to the temperature dependence of the <span class="hlt">mantle</span> viscosity. This causes a three-dimensional <span class="hlt">mantle</span> flow pattern that amplifies the along-arc variations in the sub-arc <span class="hlt">mantle</span> temperature, providing a simple mechanism for volcano clustering.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V24A..03J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V24A..03J"><span>Phase behavior and reactive transport of partial melt in heterogeneous <span class="hlt">mantle</span> model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jordan, J.; Hesse, M. A.</p> <p>2013-12-01</p> <p>The reactive transport of partial melt is the key process that leads to the chemical and physical <span class="hlt">differentiation</span> of terrestrial planets and smaller celestial bodies. The essential role of the lithological heterogeneities during partial melting of the <span class="hlt">mantle</span> is increasingly recognized. How far can enriched melts propagate while interacting with the ambient <span class="hlt">mantle</span>? Can the melt flow emanating from a fertile heterogeneity be localized through a reactive infiltration feedback in a model without exogenous factors or contrived initial conditions? A full understanding of the role of heterogeneities requires reactive melt transport models that account for the phase behavior of major elements. Previous work on reactive transport in the <span class="hlt">mantle</span> focuses on trace element partitioning; we present the first nonlinear chromatographic analysis of reactive melt transport in systems with binary solid solution. Our analysis shows that reactive melt transport in systems with binary solid solution leads to the formation of two separate reaction fronts: a slow melting/freezing front along which enthalpy change is dominant and a fast dissolution/precipitation front along which compositional changes are dominated by an ion-exchange process over enthalpy change. An intermediate state forms between these two fronts with a bulk-rock composition and enthalpy that are not necessarily bounded by the bulk-rock composition and enthalpy of either the enriched heterogeneity or the depleted ambient <span class="hlt">mantle</span>. The formation of this intermediate state makes it difficult to anticipate the porosity changes and hence the stability of reaction fronts. Therefore, we develop a graphical representation for the solution that allows identification of the intermediate state by inspection, for all possible bulk-rock compositions and enthalpies of the heterogeneity and the ambient <span class="hlt">mantle</span>. We apply the analysis to the partial melting of an enriched heterogeneity. This leads to the formation of moving precipitation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27689814','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27689814"><span>Heparan sulfates and the decrease of N-glycans promote <span class="hlt">early</span> adipogenic <span class="hlt">differentiation</span> rather than myogenesis of murine myogenic progenitor cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grassot, Vincent; Bouchatal, Amel; Da Silva, Anne; Chantepie, Sandrine; Papy-Garcia, Dulce; Maftah, Abderrahman; Gallet, Paul-François; Petit, Jean-Michel</p> <p></p> <p>In vitro, extracted muscle satellite cells, called myogenic progenitor cells, can <span class="hlt">differentiate</span> either in myotubes or preadipocytes, depending on environmental factors and the medium. Transcriptomic analyses on glycosylation genes during satellite cells <span class="hlt">differentiation</span> into myotubes showed that 31 genes present a significant variation of expression at the <span class="hlt">early</span> stages of murine myogenic progenitor cells (MPC) <span class="hlt">differentiation</span>. In the present study, we analyzed the expression of 383 glycosylation related genes during murine MPC <span class="hlt">differentiation</span> into preadipocytes and compared the data to those previously obtained during their <span class="hlt">differentiation</span> into myotubes. Fifty-six glycosylation related genes are specifically modified in their expression during <span class="hlt">early</span> adipogenesis. The variations correspond mainly to: a decrease of N-glycans, and of alpha (2,3) and (2,6) linked sialic acids, and to a high level of heparan sulfates. A high amount of TGF-β1 in extracellular media during <span class="hlt">early</span> adipogenesis was also observed. It seems that the increases of heparan sulfates and TGF-β1 favor pre-adipogenic differentition of MPC and possibly prevent their myogenic <span class="hlt">differentiation</span>. Copyright © 2016 International Society of <span class="hlt">Differentiation</span>. Published by Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMDI53A1699I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMDI53A1699I"><span>Quantitative Restoration of the Evolution of <span class="hlt">Mantle</span> Structures Using Data Assimilation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ismail-Zadeh, A.; Schubert, G.; Tsepelev, I.</p> <p>2008-12-01</p> <p>Rapid progress in imaging deep Earth structures and in studies of physical and chemical properties of <span class="hlt">mantle</span> rocks facilitates research in assimilation of data related to <span class="hlt">mantle</span> dynamics. We present a quantitative approach to assimilation of geophysical and geodetic data, which allows for incorporating observations and unknown initial conditions for <span class="hlt">mantle</span> temperature and flow into a three-dimensional dynamic model in order to determine the initial conditions in the geological past. Once the conditions are determined the evolution of <span class="hlt">mantle</span> structures can be restore backward in time. We apply data assimilation techniques to model the evolution of <span class="hlt">mantle</span> plumes and lithospheric slabs. We show that the geometry of the <span class="hlt">mantle</span> structures changes with time diminishing the degree of surface curvature of the structures, because the heat conduction smoothes the complex thermal surfaces of <span class="hlt">mantle</span> bodies with time. Present seismic tomography images of <span class="hlt">mantle</span> structures do not allow definition of the sharp shapes of these structures. Assimilation of <span class="hlt">mantle</span> temperature and flow to the geological past instead provides a quantitative tool to restore thermal shapes of prominent structures in the past from their diffusive shapes at present.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70017117','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70017117"><span>A sharp and flat section of the core-<span class="hlt">mantle</span> boundary</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Vidale, J.E.; Benz, H.M.</p> <p>1992-01-01</p> <p>THE transition zone between the Earth's core and <span class="hlt">mantle</span> plays an important role as a boundary layer for <span class="hlt">mantle</span> and core convection1. This zone conducts a large amount of heat from the core to the <span class="hlt">mantle</span>, and contains at least one thermal boundary layer2,3; the proximity of reactive silicates and molten iron leads to the possibility of zones of intermediate composition4. Here we investigate one region of the core-<span class="hlt">mantle</span> boundary using seismic waves that are converted from shear to compressional waves by reflection at the boundary. The use of this phase (known as ScP), the large number of receiving stations, and the large aperture of our array all provide higher resolution than has previously been possible5-7. For the 350-km-long section of the core-<span class="hlt">mantle</span> boundary under the northeast Pacific sampled by the reflections, the local boundary topography has an amplitude of less than 500 m, no sharp radial gradients exist in the 400 km above the boundary, and the <span class="hlt">mantle</span>-lo-core transition occurs over less than 1 km. The simplicity of the structure near and above the core-<span class="hlt">mantle</span> boundary argues against chemical heterogeneity at the base of the <span class="hlt">mantle</span> in this location.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI52A..01C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI52A..01C"><span>Radial Anisotropy in the <span class="hlt">Mantle</span> Transition Zone and Its Implications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chang, S. J.; Ferreira, A. M.</p> <p>2016-12-01</p> <p>Seismic anisotropy is a useful tool to investigate <span class="hlt">mantle</span> flow, <span class="hlt">mantle</span> convection, and the presence of melts in <span class="hlt">mantle</span>, since it provides information on the direction of <span class="hlt">mantle</span> flow or the orientation of melts by combining it with laboratory results in mineral physics. Although the uppermost and lowermost <span class="hlt">mantle</span> with strong anisotropy have been well studied, anisotropic properties of the <span class="hlt">mantle</span> transition zone is still enigmatic. We use a recent global radially anisotropic model, SGLOBE-rani, to examine the patterns of radial anisotropy in the <span class="hlt">mantle</span> transition zone. Strong faster SV velocity anomalies are found in the upper transition zone beneath subduction zones in the western Pacific, which decrease with depth, thereby nearly isotropic in the lower transition zone. This may imply that the origin for the anisotropy is the lattice-preferred orientation of wadsleyite, the dominant anisotropic mineral in the upper transition zone. The water content in the upper transition zone may be inferred from radial anisotropy because of the report that anisotropic intensity depends on the water content in wadsleyite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17731881','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17731881"><span>Three-Dimensional Spherical Models of Convection in the Earth's <span class="hlt">Mantle</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bercovici, D; Schubert, G; Glatzmaier, G A</p> <p>1989-05-26</p> <p>Three-dimensional, spherical models of <span class="hlt">mantle</span> convection in the earth reveal that upwelling cylindrical plumes and downwelling planar sheets are the primary features of <span class="hlt">mantle</span> circulation. Thus, subduction zones and descending sheetlike slabs in the <span class="hlt">mantle</span> are fundamental characteristics of thermal convection in a spherical shell and are not merely the consequences of the rigidity of the slabs, which are cooler than the surrounding <span class="hlt">mantle</span>. Cylindrical <span class="hlt">mantle</span> plumes that cause hotspots such as Hawaii are probably the only form of active upwelling and are therefore not just secondary convective currents separate from the large-scale <span class="hlt">mantle</span> circulation. Active sheetlike upwellings that could be associated with mid-ocean ridges did not develop in the model simulations, a result that is in agreement with evidence suggesting that ridges are passive phenomena resulting from the tearing of surface plates by the pull of descending slabs.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.213...16C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.213...16C"><span>Tectonic predictions with <span class="hlt">mantle</span> convection models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coltice, Nicolas; Shephard, Grace E.</p> <p>2018-04-01</p> <p>Over the past 15 yr, numerical models of convection in Earth's <span class="hlt">mantle</span> have made a leap forward: they can now produce self-consistent plate-like behaviour at the surface together with deep <span class="hlt">mantle</span> circulation. These digital tools provide a new window into the intimate connections between plate tectonics and <span class="hlt">mantle</span> dynamics, and can therefore be used for tectonic predictions, in principle. This contribution explores this assumption. First, initial conditions at 30, 20, 10 and 0 Ma are generated by driving a convective flow with imposed plate velocities at the surface. We then compute instantaneous <span class="hlt">mantle</span> flows in response to the guessed temperature fields without imposing any boundary conditions. Plate boundaries self-consistently emerge at correct locations with respect to reconstructions, except for small plates close to subduction zones. As already observed for other types of instantaneous flow calculations, the structure of the top boundary layer and upper-<span class="hlt">mantle</span> slab is the dominant character that leads to accurate predictions of surface velocities. Perturbations of the rheological parameters have little impact on the resulting surface velocities. We then compute fully dynamic model evolution from 30 and 10 to 0 Ma, without imposing plate boundaries or plate velocities. Contrary to instantaneous calculations, errors in kinematic predictions are substantial, although the plate layout and kinematics in several areas remain consistent with the expectations for the Earth. For these calculations, varying the rheological parameters makes a difference for plate boundary evolution. Also, identified errors in initial conditions contribute to first-order kinematic errors. This experiment shows that the tectonic predictions of dynamic models over 10 My are highly sensitive to uncertainties of rheological parameters and initial temperature field in comparison to instantaneous flow calculations. Indeed, the initial conditions and the rheological parameters can be good enough</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.8441M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.8441M"><span>Iron spin transitions in the lower <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McCammon, C.; Dubrovinsky, L.; Potapkin, V.; Glazyrin, K.; Kantor, A.; Kupenko, I.; Prescher, C.; Sinmyo, R.; Smirnov, G.; Chumakov, A.; Rüffer, R.</p> <p>2012-04-01</p> <p>Iron has the ability to adopt different electronic configurations (spin states), which can significantly influence <span class="hlt">mantle</span> properties and dynamics. It is now generally accepted as a result of studies over the past decade that ferrous iron in (Mg,Fe)O undergoes a high-spin to low-spin transition in the mid-part of the lower <span class="hlt">mantle</span>; however results on (Mg,Fe)(Si,Al)O3 perovskite, the dominant phase of the lower <span class="hlt">mantle</span>, remain controversial. Identifying spin transitions in (Mg,Fe)(Si,Al)O3 perovskite presents a significant challenge. X-ray emission spectroscopy provides information on the bulk spin number, but cannot separate individual contributions. Nuclear forward scattering measures hyperfine interactions, but is not well suited to complex materials due to the non-uniqueness of fitting models. Energy-domain Mössbauer spectroscopy generally enables an unambiguous resolution of all hyperfine parameters which can be used to infer spin states; however high pressure measurements using conventional radioactive point sources require extremely long counting times. To solve this problem, we have developed an energy-domain synchrotron Mössbauer source that enables rapid measurement of spectra under extreme conditions (both high pressure and high temperature) with a quality generally sufficient to unambiguously deconvolute even highly complex spectra. We have used the newly developed method to measure high quality Mössbauer spectra of different compositions of (Mg,Fe)O and (Mg,Fe)(Si,Al)O3 perovskite at pressures up to 122 GPa and temperatures up to 2400 K. Experiments were carried out at the European Synchrotron Radiation Facility on the nuclear resonance beamline ID18 equipped with a portable laser heating system for diamond anvil cells. Our results confirm previous observations for (Mg,Fe)O that show a broad spin crossover region at high pressures and high temperatures, and show unambiguously that ferric iron in (Mg,Fe)(Si,Al)O3 perovskite remains in the high-spin state</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMDI53A1698D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMDI53A1698D"><span>Thermally-Driven <span class="hlt">Mantle</span> Plumes Reconcile Hot-spot Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davies, D.; Davies, J.</p> <p>2008-12-01</p> <p>Hot-spots are anomalous regions of magmatism that cannot be directly associated with plate tectonic processes (e.g. Morgan, 1972). They are widely regarded as the surface expression of upwelling <span class="hlt">mantle</span> plumes. Hot-spots exhibit variable life-spans, magmatic productivity and fixity (e.g. Ito and van Keken, 2007). This suggests that a wide-range of upwelling structures coexist within Earth's <span class="hlt">mantle</span>, a view supported by geochemical and seismic evidence, but, thus far, not reproduced by numerical models. Here, results from a new, global, 3-D spherical, <span class="hlt">mantle</span> convection model are presented, which better reconcile hot-spot observations, the key modification from previous models being increased convective vigor. Model upwellings show broad-ranging dynamics; some drift slowly, while others are more mobile, displaying variable life-spans, intensities and migration velocities. Such behavior is consistent with hot-spot observations, indicating that the <span class="hlt">mantle</span> must be simulated at the correct vigor and in the appropriate geometry to reproduce Earth-like dynamics. Thermally-driven <span class="hlt">mantle</span> plumes can explain the principal features of hot-spot volcanism on Earth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR43A0461S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR43A0461S"><span>Mineralogy of the Hydrous Lower <span class="hlt">Mantle</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shim, S. H.; Chen, H.; Leinenweber, K. D.; Kunz, M.; Prakapenka, V.; Bechtel, H.; Liu, Z.</p> <p>2017-12-01</p> <p>The hydrous ringwoodite inclusions found in diamonds suggest water storage in the <span class="hlt">mantle</span> transition zone. However, water storage in the lower <span class="hlt">mantle</span> remains unclear. Bridgmanite and magnesiowustite appear to have very little storage capacity for water. Here, we report experimental results indicating significant changes in the lower-<span class="hlt">mantle</span> mineralogy under the presence of water. We have synthesized Mg2SiO4 ringwoodite with 2 wt% water in multi-anvil press at 20 GPa and 1573 K at ASU. The hydrous ringwoodite sample was then loaded to diamond anvil cells with Ar or Ne as a pressure medium. We heated the pure hydrous ringwoodite samples at lower-<span class="hlt">mantle</span> pressure using a CO2 laser heating system at ASU. We measured X-ray diffraction patterns at the GSECARS sector of the Advanced Photon Source (APS) and 12.2.2 sector of the Advanced Light Source (ALS). For the separate Pt-mixed samples, we have conducted in situ heating at the beamlines using near IR laser heating systems. We measured the infrared spectra of the heated samples at high pressure and after pressure quench at 1.4.4 sector of ALS. In the in situ experiments with hydrous ringwoodite + Pt mixture as a starting material, we found formation of stishovite together with bridgmanite and periclase during heating with a near IR laser beams at 1300-2500 K and 35-66 GPa. However, some hydrous ringwoodite still remains even after a total of 45 min of heating. In contrast, the hydrous ringwoodite samples heated without Pt by CO2 laser beams are transformed completely to bridgmanite, periclase and stishovite at 31-55 GPa and 1600-1900 K. We have detected IR active OH mode of stishovite from the samples heated at lower-<span class="hlt">mantle</span> pressures. The unit-cell volume of stishovite measured after pressure quench is greater than that of dry stishovite by 0.3-0.6%, supporting 0.5-1 wt% of H2O in stishovite in these samples. Stishovite is a thermodynamically forbidden phase in the dry lower <span class="hlt">mantle</span> because of the existence of periclase and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17813909','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17813909"><span><span class="hlt">Mantle</span> convection with plates and mobile, faulted plate margins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhong, S; Gurnis, M</p> <p>1995-02-10</p> <p>A finite-element formulation of faults has been incorporated into time-dependent models of <span class="hlt">mantle</span> convection with realistic rheology, continents, and phase changes. Realistic tectonic plates naturally form with self-consistent coupling between plate and <span class="hlt">mantle</span> dynamics. After the initiation of subduction, trenches rapidly roll back with subducted slabs temporarily laid out along the base of the transition zone. After the slabs have penetrated into the lower <span class="hlt">mantle</span>, the velocity of trench migration decreases markedly. The inhibition of slab penetration into the lower <span class="hlt">mantle</span> by the 670-kilometer phase change is greatly reduced in these models as compared to models without tectonic plates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5065123-concentration-behavior-storage-sub-suboceanic-upper-mantle-implications-mantle-metasomatism','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5065123-concentration-behavior-storage-sub-suboceanic-upper-mantle-implications-mantle-metasomatism"><span>Concentration, behavior and storage of H/sub 2/O in the suboceanic upper <span class="hlt">mantle</span>: implications for <span class="hlt">mantle</span> metasomatism</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Michael, P.J.</p> <p>1988-02-01</p> <p>Mid-ocean ridge basalt glasses from the Pacific-Nazca Ridge and the northern Juan de Fuca Ridge were analyzed for H/sub 2/O by gas chromatography. Incompatible element enriched (IEE) glasses have higher H/sub 2/O contents than depleted (IED) glasses. H/sub 2/O increases systematically with decreasing Mg/Mg + Fe/sup 2 +/ within each group. Near-primary IED MORBs have an average of about 800 ppm H/sub 2/O, while near-primary IEE MORBs (with chondrite normalized Nb/Zr or La/Sm approx. 2) have about 2100 ppm H/sub 2/O. If these basalts formed by 10-20% partial melting then the IED <span class="hlt">mantle</span> source had 100-180 ppm H/sub 2/O, whilemore » the IEE source had 250-450 ppm H/sub 2/O. The ratio H/sub 2/O/(Ce + Nd) is fairly constant at 95 +/- 30 for all oceanic basalts from the Pacific. During trace element fractionation in the suboceanic upper <span class="hlt">mantle</span>, H/sub 2/O behaves more compatibly than K, Rb, Nb, and Cl, but less compatibly than Sm, Zr and Ti. H/sub 2/O is contained mostly in amphibole in the shallow upper <span class="hlt">mantle</span>. At pressures greater than the amphibole stability limit, it is likely that a significant proportion of H/sub 2/O is contained in a <span class="hlt">mantle</span> phase which is more refractory than phlogopite at these pressures. The role of H/sub 2/O in <span class="hlt">mantle</span> enrichment processes is examined by assuming that an enriched component was added. The modeled concentrations of K, Na, Ti and incompatible trace elements in this component are high relative to H/sub 2/O, indicating that suboceanic <span class="hlt">mantle</span> enrichment is caused by silicate melts such as basanites and not by aqueous fluids.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.3250F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.3250F"><span><span class="hlt">Mantle</span> dynamics in the Mediterranean</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faccenna, Claudio; Becker, Thorsten W.</p> <p>2016-04-01</p> <p>The Mediterranean offers a unique avenue to study the driving forces of tectonic deformation within a complex mobile belt. Lithospheric dynamics are affected by slab rollback and collision of two large, slowly moving plates, forcing fragments of continental and oceanic lithosphere to interact. Here, we review the rich and growing set of constraints from geological reconstructions, geodetic data, and crustal and upper <span class="hlt">mantle</span> heterogeneity imaged by structural seismology. We discuss a conceptual and quantitative framework for the causes of surface deformations. Exploring existing and newly developed tectonic and numerical geodynamic models, we illustrate the role of <span class="hlt">mantle</span> convection on surface geology. A coherent picture emerges which can be outlined by two, almost symmetric, upper <span class="hlt">mantle</span> convection cells. The down-wellings are found in the centre of the Mediterranean, and are associated with the descent of the Tyrrhenian and the Hellenic slabs. During plate convergence, these slabs migrated, driving return flow of the asthenosphere from the backarc regions. These currents can be found at large distance from the subduction zones, and are at present expressed in two upwellings beneath Anatolia and eastern Iberia. This convection system provides an explanation for the general pattern of seismic anisotropy in the Mediterranean, the first-order Anatolia and Adria microplate kinematics, and the positive dynamic topography of Anatolia and Eastern Iberia. More generally, it is an illustration of upper <span class="hlt">mantle</span>, small-scale convection leading to intraplate deformation and complex plate boundary reconfiguration at the westernmost terminus of the Tethyan collision.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4416816','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4416816"><span>Overlapping DNA Methylation Dynamics in Mouse Intestinal Cell <span class="hlt">Differentiation</span> and <span class="hlt">Early</span> Stages of Malignant Progression</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Forn, Marta; Díez-Villanueva, Anna; Merlos-Suárez, Anna; Muñoz, Mar; Lois, Sergi; Carriò, Elvira; Jordà, Mireia; Bigas, Anna; Batlle, Eduard; Peinado, Miguel A.</p> <p>2015-01-01</p> <p>Mouse models of intestinal crypt cell <span class="hlt">differentiation</span> and tumorigenesis have been used to characterize the molecular mechanisms underlying both processes. DNA methylation is a key epigenetic mark and plays an important role in cell identity and <span class="hlt">differentiation</span> programs and cancer. To get insights into the dynamics of cell <span class="hlt">differentiation</span> and malignant transformation we have compared the DNA methylation profiles along the mouse small intestine crypt and <span class="hlt">early</span> stages of tumorigenesis. Genome-scale analysis of DNA methylation together with microarray gene expression have been applied to compare intestinal crypt stem cells (EphB2high), <span class="hlt">differentiated</span> cells (EphB2negative), ApcMin/+ adenomas and the corresponding non-tumor adjacent tissue, together with small and large intestine samples and the colon cancer cell line CT26. Compared with late stages, small intestine crypt <span class="hlt">differentiation</span> and <span class="hlt">early</span> stages of tumorigenesis display few and relatively small changes in DNA methylation. Hypermethylated loci are largely shared by the two processes and affect the proximities of promoter and enhancer regions, with enrichment in genes associated with the intestinal stem cell signature and the PRC2 complex. The hypermethylation is progressive, with minute levels in <span class="hlt">differentiated</span> cells, as compared with intestinal stem cells, and reaching full methylation in advanced stages. Hypomethylation shows different signatures in <span class="hlt">differentiation</span> and cancer and is already present in the non-tumor tissue adjacent to the adenomas in ApcMin/+ mice, but at lower levels than advanced cancers. This study provides a reference framework to decipher the mechanisms driving mouse intestinal tumorigenesis and also the human counterpart. PMID:25933092</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.T51F2994P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.T51F2994P"><span>Nature of the uppermost <span class="hlt">mantle</span> below the Porcupine Basin, offshore Ireland: new insights from seismic refraction and gravity data modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prada, M.; Watremez, L.; Chen, C.; O'Reilly, B.; Minshull, T. A.; Reston, T. J.; Wagner, G.; Gaw, V.; Klaeschen, D.; Shannon, P.</p> <p>2015-12-01</p> <p>The Porcupine Basin is a tongue-shaped basin SW of Ireland formed during the opening of the North Atlantic Ocean. Its history of sedimentation reveals several rifting and subsidence phases during the Late Paleozoic and Cenozoic, with a particular major rift phase occurring in Late Jurassic-<span class="hlt">Early</span> Cretaceous times. Previous work, focused on seismic and gravity data, suggest the presence of major crustal faulting and uppermost <span class="hlt">mantle</span> serpentinization in the basin. Serpentinization is a key factor in lithospheric extension since it reduces the strength of <span class="hlt">mantle</span> rocks, and hence, influences the tectonics of the lithosphere. Besides reducing the seismic velocity of the rock, serpentinization decreases <span class="hlt">mantle</span> rock density favoring isostatic rebound and basin uplift, thus affecting the tectonic and thermal evolution of the basin. Here we characterize the deep structure of the Porcupine Basin from wide-angle seismic (WAS) and gravity data, with especial emphasis on the nature of the underlying <span class="hlt">mantle</span>. The WAS data used were acquired along a 300 km long transect across the northern region of the basin. We used a travel time inversion method to model the data and obtain a P-wave velocity (Vp) model of the crust and uppermost <span class="hlt">mantle</span>, together with the geometry of the main geological interfaces. The crustal structure along the model reveals a maximum stretching factor of ~5-6. These values are well within the range of crustal extension at which the crust becomes entirely brittle allowing the formation of major crustal faulting and serpentinization of the <span class="hlt">mantle</span>. To further constrain the seismic structure and hence the nature of the <span class="hlt">mantle</span> we assess the Vp uncertainty of the model by means of a Monte Carlo analysis and perform gravity modeling to test different interpretations regarding <span class="hlt">mantle</span> rock nature. This project is funded by the Irish Shelf Petroleum Studies Group (ISPSG) of the Irish Petroleum Infrastructure Programme Group 4.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFMDI41B1801Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFMDI41B1801Y"><span>Whole-<span class="hlt">mantle</span> P-wave velocity structure and azimuthal anisotropy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yamamoto, Y.; Zhao, D.</p> <p>2009-12-01</p> <p>There are some hotspot volcanoes on Earth, such as Hawaii and Iceland. The <span class="hlt">mantle</span> plume hypothesis was proposed forty years ago to explain hotspot volcanoes (e.g., Wilson, 1963; Morgan, 1971). Seismic tomography is a powerful technique to detect <span class="hlt">mantle</span> plumes and determine their detailed structures. We determined a new whole-<span class="hlt">mantle</span> 3-D P-wave velocity model (Tohoku model) using a global tomography method (Zhao, 2004, 2009). A flexible-grid approach with a grid interval of ~200 km is adopted to conduct the tomographic inversion. Our model shows that low-velocity (low-V) anomalies with diameters of several hundreds of kilometers are visible from the core-<span class="hlt">mantle</span> boundary (CMB) to the surface under the major hotspot regions. Under South Pacific where several hotspots including Tahiti exist, there is a huge low-V anomaly from the CMB to the surface. This feature is consistent with the previous models. We conducted extensive resolution tests in order to understand whether this low-V anomaly shows a single superplume or a plume cluster. Unfortunately this problem is still not resolved because the ray path coverage in the <span class="hlt">mantle</span> under South Pacific is not good enough. A network of ocean bottom seismometers is necessary to solve this problem. To better understand the whole-<span class="hlt">mantle</span> structure and dynamics, we also conducted P-wave tomographic inversions for the 3-D velocity structure and azimuthal anisotropy. At each grid node there are three unknown parameters: one represents the isotropic velocity, the other two represent the azimuthal anisotropy. Our results show that in the shallow part of the <span class="hlt">mantle</span> (< ~200 km depth) the fast velocity direction (FVD) is almost the same as the plate motion direction. For example, the FVD in the western Pacific is NWW-SEE, which is normal to the Japan trench axis. In the Tonga subduction zone, the FVD is also perpendicular to the trench axis. Under the Tibetan region the FVD is NE-SW, which is parallel to the direction of the India</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1612819C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1612819C"><span>Understanding the nature of <span class="hlt">mantle</span> upwelling beneath East-Africa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Civiero, Chiara; Hammond, James; Goes, Saskia; Ahmed, Abdulhakim; Ayele, Atalay; Doubre, Cecile; Goitom, Berhe; Keir, Derek; Kendall, Mike; Leroy, Sylvie; Ogubazghi, Ghebrebrhan; Rumpker, Georg; Stuart, Graham</p> <p>2014-05-01</p> <p>The concept of hot upwelling material - otherwise known as <span class="hlt">mantle</span> plumes - has long been accepted as a possible mechanism to explain hotspots occurring at Earth's surface and it is recognized as a way of removing heat from the deep Earth. Nevertheless, this theory remains controversial since no one has definitively imaged a plume and over the last decades several other potential mechanisms that do not require a deep <span class="hlt">mantle</span> source have been invoked to explain this phenomenon, for example small-scale convection at rifted margins, meteorite impacts or lithospheric delamination. One of the best locations to study the potential connection between hotspot volcanism at the surface and deep <span class="hlt">mantle</span> plumes on land is the East African Rift (EAR). We image seismic velocity structure of the <span class="hlt">mantle</span> below EAR with higher resolution than has been available to date by including seismic data recorded by stations from many regional networks ranging from Saudi Arabia to Tanzania. We use relative travel-time tomography to produce P- velocity models from the surface down into the lower <span class="hlt">mantle</span> incorporating 9250 ray-paths in our model from 495 events and 402 stations. We add smaller earthquakes (4.5 < mb < 5.5) from poorly sampled regions in order to have a more uniform data coverage. The tomographic results allow us to image structures of ~ 100-km length scales to ~ 1000 km depth beneath the northern East-Africa rift (Ethiopia, Eritrea, Djibouti, Yemen) with good resolution also in the transition zone and uppermost lower <span class="hlt">mantle</span>. Our observations provide evidence that the shallow <span class="hlt">mantle</span> slow seismic velocities continue trough the transition zone and into the lower <span class="hlt">mantle</span>. In particular, the relatively slow velocity anomaly beneath the Afar Depression extends up to depths of at least 1000 km depth while another low-velocity anomaly beneath the Main Ethiopian Rift seems to be present in the upper <span class="hlt">mantle</span> only. These features in the lower <span class="hlt">mantle</span> are isolated with a diameter of about 400 km</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGeo..100..198F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGeo..100..198F"><span><span class="hlt">Early</span> Earth plume-lid tectonics: A high-resolution 3D numerical modelling approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fischer, R.; Gerya, T.</p> <p>2016-10-01</p> <p>Geological-geochemical evidence point towards higher <span class="hlt">mantle</span> potential temperature and a different type of tectonics (global plume-lid tectonics) in the <span class="hlt">early</span> Earth (>3.2 Ga) compared to the present day (global plate tectonics). In order to investigate tectono-magmatic processes associated with plume-lid tectonics and crustal growth under hotter <span class="hlt">mantle</span> temperature conditions, we conduct a series of 3D high-resolution magmatic-thermomechanical models with the finite-difference code I3ELVIS. No external plate tectonic forces are applied to isolate 3D effects of various plume-lithosphere and crust-<span class="hlt">mantle</span> interactions. Results of the numerical experiments show two distinct phases in coupled crust-<span class="hlt">mantle</span> evolution: (1) a longer (80-100 Myr) and relatively quiet 'growth phase' which is marked by growth of crust and lithosphere, followed by (2) a short (∼20 Myr) and catastrophic 'removal phase', where unstable parts of the crust and <span class="hlt">mantle</span> lithosphere are removed by eclogitic dripping and later delamination. This modelling suggests that the <span class="hlt">early</span> Earth plume-lid tectonic regime followed a pattern of episodic growth and removal also called episodic overturn with a periodicity of ∼100 Myr.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994JGR....99.2053H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994JGR....99.2053H"><span>Episodic large-scale overturn of two-layer <span class="hlt">mantles</span> in terrestrial planets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Herrick, D. L.; Parmentier, E. M.</p> <p>1994-01-01</p> <p>It is usually assumed that the upper and lower <span class="hlt">mantles</span> of a chemically stratified planet are arranged so that the upper <span class="hlt">mantle</span> is chemically less dense and that these layers convect separately. Possible buoyant overturn of the two <span class="hlt">mantle</span> layers has not previously been considered. Such overturn would initially occur when thermal expansion of a chemically denser lower <span class="hlt">mantle</span> more than offsets the compositional density difference between the layers, reversing the relative sense of buoyancy. Once overturn has occurred, the chemically denser, but thermally less dense upper <span class="hlt">mantle</span> cools more efficiently than the lower <span class="hlt">mantle</span> and loses its relative thermal buoyancy. If mixing is slow, this leads to repeated overturns that result in thermal histories that differ radically from those obtained without this large-scale overturning. Thermal evolution calculations, for a two-layer <span class="hlt">mantle</span> over a wide range of parameter space, show that large-scale overturn occurs cyclically with a well-defined period. This period depends most strongly on the viscosity of the lower <span class="hlt">mantle</span>, to which it is approximately proportional. Geologically interesting overturn periods on the order of 107 to 109 years result for lower <span class="hlt">mantle</span> viscosities of 1022 to 1024 Pa s for the Earth and Venus, and 1021 to 1023 Pa s for Mars. The <span class="hlt">mantles</span> of Mercury and the Moon are too thin to permit two-layer convection, and therefore the model is not appropriate for them. Overturn cannot occur on Earth or Venus if the compositional density difference between the layers exceeds about 4%, or on Mars if it exceeds about 2%. Large-scale <span class="hlt">mantle</span> overturn could have significant tectonic consequences such as the initiation of a new plate tectonic cycle on the Earth or a major resurfacing event on Mars or Venus. Such episodic events in the evolution of a planet are not easily explained by whole <span class="hlt">mantle</span> thermal convection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70024147','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70024147"><span>Processes of lithosphere evolution: New evidence on the structure of the continental crust and uppermost <span class="hlt">mantle</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Artemieva, I.M.; Mooney, W.D.; Perchuc, E.; Thybo, H.</p> <p>2002-01-01</p> <p>We discuss the structure of the continental lithosphere, its physical properties, and the mechanisms that formed and modified it since the <span class="hlt">early</span> Archean. The structure of the upper <span class="hlt">mantle</span> and the crust is derived primarily from global and regional seismic tomography studies of Eurasia and from global and regional data on seismic anisotropy. These data as documented in the papers of this special issue of Tectonophysics are used to illustrate the role of different tectonic processes in the lithospheric evolution since Archean to present. These include, but are not limited to, cratonization, terrane accretion and collision, continental rifting (both passive and active), subduction, and lithospheric basal erosion due to a relative motion of cratonic keels and the convective <span class="hlt">mantle</span>. ?? 2002 Elsevier Science B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.T44C..02S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.T44C..02S"><span>Lithology and temperature: How key <span class="hlt">mantle</span> variables control rift volcanism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shorttle, O.; Hoggard, M.; Matthews, S.; Maclennan, J.</p> <p>2015-12-01</p> <p>Continental rifting is often associated with extensive magmatic activity, emplacing millions of cubic kilometres of basalt and triggering environmental change. The lasting geological record of this volcanic catastrophism are the large igneous provinces found at the margins of many continents and abrupt extinctions in the fossil record, most strikingly that found at the Permo-Triassic boundary. Rather than being considered purely a passive plate tectonic phenomenon, these episodes are frequently explained by the involvement of <span class="hlt">mantle</span> plumes, upwellings of <span class="hlt">mantle</span> rock made buoyant by their high temperatures. However, there has been debate over the relative role of the <span class="hlt">mantle</span>'s temperature and composition in generating the large volumes of magma involved in rift and intra-plate volcanism, and even when the <span class="hlt">mantle</span> is inferred to be hot, this has been variously attributed to <span class="hlt">mantle</span> plumes or continental insulation effects. To help resolve these uncertainties we have combined geochemical, geophysical and modelling results in a two stage approach: Firstly, we have investigated how <span class="hlt">mantle</span> composition and temperature contribute to melting beneath Iceland, the present day manifestation of the <span class="hlt">mantle</span> plume implicated in the 54Ma break up of the North Atlantic. By considering both the igneous crustal production on Iceland and the chemistry of its basalts we have been able to place stringent constraints on the viable temperature and lithology of the Icelandic <span class="hlt">mantle</span>. Although a >100°C excess temperature is required to generate Iceland's thick igneous crust, geochemistry also indicates that pyroxenite comprises 10% of its source. Therefore, the dynamics of rifting on Iceland are modulated both by thermal and compositional <span class="hlt">mantle</span> anomalies. Secondly, we have performed a global assessment of the <span class="hlt">mantle</span>'s post break-up thermal history to determine the amplitude and longevity of continental insulation in driving excess volcanism. Using seismically constrained igneous crustal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70013666','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70013666"><span>The role of <span class="hlt">mantle</span> CO2 in volcanism</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Barnes, I.; Evans, William C.; White, L.D.</p> <p>1988-01-01</p> <p>Carbon dioxide is the propellant gas in volcanic eruptions and is also found in <span class="hlt">mantle</span> xenoliths. It is speculated that CO2 occurs as a free gas phase in the <span class="hlt">mantle</span> because there is no reason to expect CO2 to be so universally associated with volcanic rocks unless the CO2 comes from the same source as the volcanic rocks and their xenoliths. If correct, the presence of a free gas in the <span class="hlt">mantle</span> would lead to physical instability, with excess gas pressure providing the cause of both buoyancy of volcanic melts and seismicity in volcanic regions. Convection in the <span class="hlt">mantle</span> and episodic volcanic eruptions are likely necessary consequences. This suggestion has considerable implications for those responsible for providing warnings of impending disasters resulting from volcanic eruptions and earthquakes in volcanic regions. ?? 1988.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013140','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013140"><span>Constraining the Composition of the Subcontinental Lithospheric <span class="hlt">Mantle</span> Beneath the East African Rift: FTIR Analysis of Water in Spinel Peridotite <span class="hlt">Mantle</span> Xenoliths</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Erickson, Stephanie Gwen; Nelson, Wendy R.; Peslier, Anne H.; Snow, Jonathan E.</p> <p>2014-01-01</p> <p>The East African Rift System was initiated by the impingement of the Afar <span class="hlt">mantle</span> plume on the base of the non-cratonic continental lithosphere (assembled during the Pan-African Orogeny), producing over 300,000 kmof continental flood basalts approx.30 Ma ago. The contribution of the subcontinental lithospheric <span class="hlt">mantle</span> (SCLM) to this voluminous period of volcanism is implied based on basaltic geochemical and isotopic data. However, the role of percolating melts on the SCLM composition is less clear. Metasomatism is capable of hybridizing or overprinting the geochemical signature of the SCLM. In addition, models suggest that adding fluids to lithospheric <span class="hlt">mantle</span> affects its stability. We investigated the nature of the SCLM using Fourier transform infrared spectrometry (FTIR) to measure water content in <span class="hlt">mantle</span> xenoliths entrained in young (1 Ma) basaltic lavas from the Ethiopian volcanic province. The <span class="hlt">mantle</span> xenoliths consist dominantly of spinel lherzolites and are composed of nominally anhydrous minerals, which can contain trace water as H in mineral defects. Eleven <span class="hlt">mantle</span> xenoliths come from the Injibara-Gojam region and two from the Mega-Sidamo region. Water abundances of olivines in six samples are 1-5ppm H2O while the rest are below the limit of detection (<0.5 ppm H2O); orthopyroxene and clinopyroxene contain 80-238 and 111-340 ppm wt H2O, respectively. Two xenoliths have higher water contents - a websterite (470 ppm) and dunite (229 ppm), consistent with involvement of ascending melts. The low water content of the upper SCLM beneath Ethiopia is as dry as the oceanic <span class="hlt">mantle</span> except for small domains represented by percolating melts. Consequently, rifting of the East African lithosphere may not have been facilitated by a hydrated upper <span class="hlt">mantle</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.6175A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.6175A"><span>Iron speciation and redox state of <span class="hlt">mantle</span> eclogites: Implications for ancient volatile cycles during <span class="hlt">mantle</span> melting and oceanic crust subduction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aulbach, Sonja; Woodand, Alan; Vasilyev, Prokopiy; Viljoen, Fanus</p> <p>2017-04-01</p> <p>Kimberlite-borne <span class="hlt">mantle</span> eclogite xenoliths of Archaean and Palaeoproterozoic age are commonly interpreted as representing former oceanic crust. As such, they may retain a memory of the redox state of the ancient convecting <span class="hlt">mantle</span> sources that gave rise to their magmatic protoliths and which controls the speciation of volatiles in planetary interiors. <span class="hlt">Mantle</span> eclogite suites commonly include both cumulate and variably evolved extrusive varieties [1], which may be characterised by initial differences in Fe3+/Fetotal. Recent Fe-based oxybarometry shows <span class="hlt">mantle</span> eclogites to have fO2 relative to the fayalite-magnetite-quartz buffer (ΔFMQ) of -3 to 0, whereby low fO2 relative to modern MORB may relate to subduction of more reducing Archaean oceanic crust or loss of ferric Fe during partial melt loss [2]. Indeed, using V/Sc as a redox proxy, it was recently shown that Archaean <span class="hlt">mantle</span> eclogites are more reduced than modern MORB (ΔFMQ-1.3 vs. ΔFMQ -0.4) [3]. However, in the warmer ancient <span class="hlt">mantle</span>, they were also subject to modification due to partial melt loss upon recycling and, after capture in the cratonic <span class="hlt">mantle</span> lithosphere, may be overprinted by interaction with metasomatic melts and fluids. In order to help further constrain the redox state of <span class="hlt">mantle</span> eclogites and unravel the effect of primary and secondary processes, we measured Fe3+/Fetotal by Mössbauer in garnet from <span class="hlt">mantle</span> eclogites from the Lace kimberlite (Kaapvaal craton), comprising samples with melt- and cumulate-like oceanic crustal protoliths as well as metasomatised samples. Fe3+/ΣFe in garnet shows a strong negative correlation with jadeite content and bulk-rock Li and Cu abundances, suggesting increased partitioning of Fe3+ into jadeite in the presence of monovalent cations with which it can form coupled substitutions. Broad negative correlation with whole-rock Al2O3/TiO2 and positive correlation with ΣREE are interpreted as incompatible behaviour of Fe3+ during olivine-plagioclase accumulation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930005144','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930005144"><span>Venus tectonic styles and crustal <span class="hlt">differentiation</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kaula, W. M.; Lenardic, A.</p> <p>1992-01-01</p> <p>Two of the most important constraints are known from Pioneer Venus data: the lack of a system of spreading rises, indicating distributed deformation rather than plate tectonics; and the high gravity/topography ratio, indicating the absence of an asthenosphere. In addition, the high depth/diameter ratios of craters on Venus indicate that Venus probably has no more crust than Earth. The problems of the character of tectonics and crustal formation and recycling are closely coupled. Venus appears to lack a recycling mechanism as effective as subduction, but may also have a low rate of crustal <span class="hlt">differentiation</span> because of a <span class="hlt">mantle</span> convection pattern that is more distributed, less concentrated, than Earth's. Distributed convection, coupled with the nonlinear dependence of volcanism on heat flow, would lead to much less magmatism, despite only moderately less heat flow, compared to Earth. The plausible reason for this difference in convective style is the absence of water in the upper <span class="hlt">mantle</span> of Venus. We have applied finite element modeling to problems of the interaction of <span class="hlt">mantle</span> convection and crust on Venus. The main emphasis has been on the tectonic evolution of Ishtar Terra, as the consequence of convergent <span class="hlt">mantle</span> flow. The <span class="hlt">early</span> stage evolution is primarily mechanical, with crust being piled up on the down-stream side. Then the downflow migrates away from the center. In the later stages, after more than 100 m.y., thermal effects develop due to the insulating influence of the thickened crust. An important feature of this modeling is the entrainment of some crustal material in downflows. An important general theme in both convergent and divergent flows is that of mixing vs. stratification. Models of multicomponent solid-state flow obtain that lower-density crustal material can be entrained and recycled, provided that the ration of low-density to high-density material is small enough (as in subducted slabs on Earth). The same considerations should apply in upflows; a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI14A..08L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI14A..08L"><span>Flow in the Deep <span class="hlt">Mantle</span> from Seisimc Anisotropy: Progress and Prospects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Long, M. D.</p> <p>2017-12-01</p> <p>Observations of seismic anisotropy, or the directional dependence of seismic wavespeeds, provide one some of the most direct constraints on the pattern of flow in the Earth's <span class="hlt">mantle</span>. In particular, as our understanding of crystallographic preferred orientation (CPO) of olivine aggregates under a range of deformation conditions has improved, our ability to exploit observations of upper <span class="hlt">mantle</span> anisotropy has led to fundamental discoveries about the patterns of flow in the upper <span class="hlt">mantle</span> and the drivers of that flow. It has been a challenge, however, to develop a similar framework for understanding flow in the deep <span class="hlt">mantle</span> (transition zone, uppermost lower <span class="hlt">mantle</span>, and lowermost <span class="hlt">mantle</span>), even though there is convincing observational evidence for seismic anisotropy at these depths. Recent progress on the observational front has allowed for an increasingly detailed view of mid-<span class="hlt">mantle</span> anisotropy (transition zone and uppermost lower <span class="hlt">mantle</span>), particularly in subduction systems, which may eventually lead to a better understanding of mid-<span class="hlt">mantle</span> deformation and the dynamics of slab interaction with the surrounding mid-<span class="hlt">mantle</span>. New approaches to the observation and modeling of lowermost <span class="hlt">mantle</span> anisotropy, in combination with constraints from mineral physics, are progressing towards interpretive frameworks that allow for the discrimination of different <span class="hlt">mantle</span> flow geometries in different regions of D". In particular, observational strategies that involve the use of multiple types of body wave phases sampled over a range of propagation azimuths enable detailed forward modeling approaches that can discriminate between different mechanisms for D" anisotropy (e.g., CPO of post-perovskite, bridgmanite, or ferropericlase, or shape preferred orientation of partial melt) and identify plausible anisotropic orientations. We have recently begun to move towards a full waveform modeling approach in this work, which allows for a more accurate simulation for seismic wave propagation. Ongoing</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. Their policies may differ from this site.</div> </div><!-- container --> <footer><a id="backToTop" href="#top"> </a><nav><a id="backToTop" href="#top"> </a><ul class="links"><a id="backToTop" href="#top"> </a><li><a id="backToTop" href="#top"></a><a href="/sitemap.html">Site Map</a></li> <li><a href="/members/index.html">Members Only</a></li> <li><a href="/website-policies.html">Website Policies</a></li> <li><a href="https://doe.responsibledisclosure.com/hc/en-us" target="_blank">Vulnerability Disclosure Program</a></li> <li><a href="/contact.html">Contact Us</a></li> </ul> <div class="small">Science.gov is maintained by the U.S. Department of Energy's <a href="https://www.osti.gov/" target="_blank">Office of Scientific and Technical Information</a>, in partnership with <a href="https://www.cendi.gov/" target="_blank">CENDI</a>.</div> </nav> </footer> <script type="text/javascript"><!-- // var lastDiv = ""; function showDiv(divName) { // hide last div if (lastDiv) { document.getElementById(lastDiv).className = "hiddenDiv"; } //if value of the box is not nothing and an object with that name exists, then change the class if (divName && document.getElementById(divName)) { document.getElementById(divName).className = "visibleDiv"; lastDiv = divName; } } //--> </script> <script> /** * Function that tracks a click on an outbound link in Google Analytics. * This function takes a valid URL string as an argument, and uses that URL string * as the event label. */ var trackOutboundLink = function(url,collectionCode) { try { h = window.open(url); setTimeout(function() { ga('send', 'event', 'topic-page-click-through', collectionCode, url); }, 1000); } catch(err){} }; </script> <!-- Google Analytics --> <script> (function(i,s,o,g,r,a,m){i['GoogleAnalyticsObject']=r;i[r]=i[r]||function(){ (i[r].q=i[r].q||[]).push(arguments)},i[r].l=1*new Date();a=s.createElement(o), m=s.getElementsByTagName(o)[0];a.async=1;a.src=g;m.parentNode.insertBefore(a,m) })(window,document,'script','//www.google-analytics.com/analytics.js','ga'); ga('create', 'UA-1122789-34', 'auto'); ga('send', 'pageview'); </script> <!-- End Google Analytics --> <script> showDiv('page_1') </script> </body> </html>