Sample records for barred olivine chondrules

  1. Dynamic crystallization study of barred olivine chondrules

    NASA Technical Reports Server (NTRS)

    Lofgren, Gary; Lanier, A. B.

    1990-01-01

    The 'classic' barred olivine (BO) texture was defined by Donaldson (1976) as a single-plate dendrite which shares the entire chondrule with the remaining glass or subsequent crystallization products. This paper describes experiments in which BO textures were produced experimentally from two starting compositions: one modeled after the average BO chondrule composition in L-chondrites determined by Weisberg (1987), and the other after an olivine-rich composition (CH-1) studied by Lofgren (1989). It is shown that most of the textural features observed in natural BO chondrules are replicated in the experimentally produced chondrules. Several new constraints on models for the chondrule-forming process are proposed.

  2. Nepheline and sodalite in a barred olivine chondrule from the Allende meteorite

    NASA Technical Reports Server (NTRS)

    Lumpkin, G. R.

    1980-01-01

    The discovery of nepheline and sodalite in association with glass in a barred olivine chondrule from the Allende C3V meteorite is reported, and the possible origin of the minerals is discussed. Scanning electron microscope/energy dispersive analysis indicates that the major minerals of the chondrule are olivine, bronzite and chromite, with olivine bars separated by glass of nearly pure plagioclase composition. The olivine is observed to have a composition richer in Fe than that predicted from olivine-liquid equilibria, indicating, along with the presence of plagioclase glass and small amounts of subcalcic diopside, the nonequilibrium crystallization of the barred olivine chondrule. The textural features of the chondrule are consistent with a liquid origin for nepheline and sodalite from the chondrule-forming liquid under nonequilibrium conditions.

  3. Experimental Reproduction of Olivine rich Type-I Chondrules

    NASA Technical Reports Server (NTRS)

    Smith, Robert K.

    2005-01-01

    Ordinary chondritic meteorites are an abundant type of stony meteorite characterized by the presence of chondrules. Chondrules are small spheres consisting of silicate, metal, and sulfide minerals that experienced melting in the nebula before incorporation into chondritic meteorite parent bodies. Therefore, chondrules record a variety of processes that occurred in the early solar nebula. Two common types of unequilibrated chondrules with porphyritic textures include FeO-poor (type I) and FeO-rich (type II) each subdivided into an A (SiO2-poor) and B (SiO2-rich) series. Type IA chondrules include those with high proportions of olivine phenocrysts (>80% olivine) and type IB chondrules include those with high proportions of pyroxene phenocrysts (<20% olivine). An intermediate composition, type IAB chondrules include those chondrules in which the proportion of olivine phenocrysts is between 20-80%. We conducted high-temperature laboratory experiments (melting at 1550 C) to produce type I chondrules from average unequilibrated ordinary chondrite (UOC) material mixed with small amounts of additional olivine. The experiments were conducted by adding forsteritic rich olivine (San Carlos olivine, Fo 91) to UOC material (GRO 95544) in a 30/70 ratio, respectively. Results of these high temperature experiments suggest that we have replicated type IA chondrule textures and compositions with dynamic crystallization experiments in which a heterogeneous mixture of UOC (GRO 95544) and olivine (San Carlos olivine) were melted at 1550 C for 1 hr. and cooled at 5-1000 C/hr using graphite crucibles in evacuated silica tubes to provide a reducing environment.

  4. Chondrule heritage and thermal histories from trace element and oxygen isotope analyses of chondrules and amoeboid olivine aggregates

    NASA Astrophysics Data System (ADS)

    Jacquet, Emmanuel; Marrocchi, Yves

    2017-12-01

    We report combined oxygen isotope and mineral-scale trace element analyses of amoeboid olivine aggregates (AOA) and chondrules in ungrouped carbonaceous chondrite, Northwest Africa 5958. The trace element geochemistry of olivine in AOA, for the first time measured by LA-ICP-MS, is consistent with a condensation origin, although the shallow slope of its rare earth element (REE) pattern is yet to be physically explained. Ferromagnesian silicates in type I chondrules resemble those in other carbonaceous chondrites both geochemically and isotopically, and we find a correlation between 16O enrichment and many incompatible elements in olivine. The variation in incompatible element concentrations may relate to varying amounts of olivine crystallization during a subisothermal stage of chondrule-forming events, the duration of which may be anticorrelated with the local solid/gas ratio if this was the determinant of oxygen isotopic ratios as proposed recently. While aqueous alteration has depleted many chondrule mesostases in REE, some chondrules show recognizable subdued group II-like patterns supporting the idea that the immediate precursors of chondrules were nebular condensates.

  5. Chemical zoning and homogenization of olivines in ordinary chondrites and implications for thermal histories of chondrules

    NASA Technical Reports Server (NTRS)

    Miyamoto, Masamichi; Mckay, David S.; Mckay, Gordon A.; Duke, Michael B.

    1986-01-01

    The extent and degree of homogenization of chemical zoning of olivines in type 3 ordinary chondrites is studied in order to obtain some constraints on cooling histories of chondrites. Based on Mg-Fe and CaO zoning, olivines in type 3 chondrites are classified into four types. A single chondrule usually contains olivines with the same type of zoning. Microporphyritic olivines show all four zoning types. Barred olivines usually show almost homogenized chemical zoning. The cooling rates or burial depths needed to homogenize the chemical zoning are calculated by solving the diffusion equation, using the zoning profiles as an initial condition. Mg-Fe zoning of olivine may be altered during initial cooling, whereas CaO zoning is hardly changed. Barred olivines may be homogenized during initial cooling because their size is relatively small. To simulated microporphyritic olivine chondrules, cooling from just below the liquidus at moderately high rates is preferable to cooling from above the liquidus at low rates. For postaccumulation metamorphism of type 3 chondrites to keep Mg-Fe zoning unaltered, the maximum metamorphic temperature must be less than about 400 C if cooling rates based on Fe-Ni data are assumed. Calculated cooling rates for both Fa and CaO homogenization are consistent with those by Fe-Ni data for type 4 chondrites. A hot ejecta blanket several tens of meters thick on the surface of a parent body is sufficient to homogenize Mg-Fe zoning if the temperature of the blanket is 600-700 C. Burial depths for petrologic types of ordinary chondrites in a parent body heated by Al-26 are broadly consistent with those previously proposed.

  6. Experimental Replication of Relict "Dusty" Olivine in Type 1B Chondrules

    NASA Technical Reports Server (NTRS)

    Lofgren, Gary E.; Le, L.

    2002-01-01

    Introduction: Relict "dusty" olivine is considered to be a remnants of previous chondrule forming events based on petrographic and chemical evidence. Dynamic crystallization experiments confirm that dusty olivine can be produced by reduction of FeO-rich olivine in Unequilibrated Ordinary Chondrite (UOC) material. The results of these experiments compliment those of who also produced dusty olivine, but from synthetic starting materials. Techniques: Dynamic crystallization experiments were conducted in which UOC material was reduced in presence of graphite. Starting material was coarsely ground GR095554 or WSG95300 that contained olivine of Fo 65-98. Approximately 75 mg. of UOC material was placed in a graphite crucible and sealed in an evacuated silica tube. The tube was suspended in a gas-mixing furnace operated at 1 log unit below the IW buffer. The experiments were as brief as 1.5 hrs up to 121 hrs. Results: Dusty olivine was produced readily in experiments melted at 1400 C for I hr. and cooled between 5 and 100 C/hr or melted at 1300-1400 C for 24 hours. Fe-rich olivine (dusty olivine precursors) that have been partially reduced were common in the experiments melted at 1400 C and cooled at 1000 C/hr or melted at 1200 C for 24 hrs. Relict olivine is absent in experiments melted at 1400 for 24 hrs, melted above 1400 C, or cooled more slowly than 10 C/hr. Relict olivine in the experiments has minimum Fo value of 83 . Thus even in the shortest experiments the most Fe-rich olivine has been altered significantly. The precursor olivine disappears in a few to many hours depending on temperature. The experiments show Fe-rich olivine in all stages of transition to the new dusty form. The olivine is reduced to form dusty olivine in a matter of a few hours at temperatures less than 1400 C and in minutes at higher temperatures. The reduction appears to proceed from the rim of the crystal inward with time. The reduction appears initially rectilinear as if controlled by

  7. Diffusion Modeling of Cooling Rates of Relict Olivine in Semarkona Chondrules

    NASA Astrophysics Data System (ADS)

    Hewins, R. H.; Ganguly, J.; Mariani, E.

    2009-03-01

    Diffusive exchange profiles between relict olivine and melt-grown olivine in Semarkona Type IIA chondrules were oriented by EBSD to correct D. Results for Fe-Mg (D from Dohmen) and Cr (Ito and Ganguly) are concordant at 300°-400°C/hr.

  8. Chondrule Pyroxene Embedded in Cores of Amoeboid Olivine Aggregates from Allende: Evidence of Overlapping Formation Times of AOAs and Chondrules

    NASA Astrophysics Data System (ADS)

    Fagan, T. J.; Komatsu, M.; Nishijima, E.; Fukushima, H.; Yasuda, T.

    2016-08-01

    Coarse low-Ca pyroxene has been identified in two amoeboid olivine aggregates in the CV3 Allende. The pyroxene crystals appear to be relict chondrule phenocrysts. If so, the texture indicates overlapping formation times of AOAs and chondrules.

  9. Relative abundances of chondrule primary textural types in ordinary chondrites and their bearing on conditions of chondrule formation

    NASA Astrophysics Data System (ADS)

    Gooding, J. L.; Keil, K.

    1981-03-01

    A petrographic survey of > 1600 chondrules in thin-sections of 12 different mildly to highly unequilibrated H-, L-, and Li-chondrites, as well as morphological and textural study of 141 whole chondrules separated from 11 of the same chondrites, was used to determine the relative abundances of definable chondrule primary textural types. Percentage abundances of various chondrule types are remarkably similar in all chondrites studied and are ˜47-52 porphyritic olivine-pyroxene (POP), 15-27 porphyritic olivine (P 0), 9-11 porphyritic pyroxene (PP), 34 barred olivine (BO), 7-9 radial pyroxene (RP), 2-5 granular olivine-pyroxene (GOP), 3-5 cryptocrystalline (C), and ≥ 1 metallic (M). Neither chondrule size nor shape is strongly correlated with textural type. Compound and cratered chondrules, which are interpreted as products of collisions between plastic chondrules, comprise ˜2-28% of non-porphyritic (RP, GOP, C) but only ˜2-9% of porphyritic (POP, PO, PP, BO) chondrules, leading to a model-dependent implication that non-porphyritic chondrules evolved at number densities (chondrules per unit volume of space) which were 102 to 104 times greater than those which prevailed during porphyritic chondrule formation (total range of ˜1 to ˜106 m-3. Distinctive "rims" of fine-grained sulfides and/or silicates occur on both porphyritic and non-porphyritic types and appear to post-date chondrule formation. Apparently, either the same process(es) contributed chondrules to all unequilibrated ordinary chondrites or, if genetically different, the various chondrule types were well mixed before incorporation into chondrites. Melting of pre-existing materials is the mechanism favored for chondrule formation.

  10. The retention of dust in protoplanetary disks: Evidence from agglomeratic olivine chondrules from the outer Solar System

    NASA Astrophysics Data System (ADS)

    Schrader, Devin L.; Nagashima, Kazuhide; Waitukaitis, Scott R.; Davidson, Jemma; McCoy, Timothy J.; Connolly, Harold C.; Lauretta, Dante S.

    2018-02-01

    By investigating the in situ chemical and O-isotope compositions of olivine in lightly sintered dust agglomerates from the early Solar System, we constrain their origins and the retention of dust in the protoplanetary disk. The grain sizes of silicates in these agglomeratic olivine (AO) chondrules indicate that the grain sizes of chondrule precursors in the Renazzo-like carbonaceous (CR) chondrites ranged from <1 to 80 μm. We infer this grain size range to be equivalent to the size range for dust in the early Solar System. AO chondrules may contain, but are not solely composed of, recycled fragments of earlier formed chondrules. They also contain 16O-rich olivine related to amoeboid olivine aggregates and represent the best record of chondrule-precursor materials. AO chondrules contain one or more large grains, sometimes similar to FeO-poor (type I) and/or FeO-rich (type II) chondrules, while others contain a type II chondrule core. These morphologies are consistent with particle agglomeration by electrostatic charging of grains during collision, a process that may explain solid agglomeration in the protoplanetary disk in the micrometer size regime. The petrographic, isotopic, and chemical compositions of AO chondrules are consistent with chondrule formation by large-scale shocks, bow shocks, and current sheets. The petrographic, isotopic, and chemical similarities between AO chondrules in CR chondrites and chondrule-like objects from comet 81P/Wild 2 indicate that comets contain AO chondrules. We infer that these AO chondrules likely formed in the inner Solar System and migrated to the comet forming region at least 3 Ma after the formation of the first Solar System solids. Observations made in this study imply that the protoplanetary disk retained a dusty disk at least ∼3.7 Ma after the formation of the first Solar System solids, longer than half of the dusty accretion disks observed around other stars.

  11. Relict grains in chondrules: Evidence for chondrule recycling

    NASA Technical Reports Server (NTRS)

    Jones, R. H.

    1994-01-01

    The presence of relict grains in chondrules, which offers some insight into the degree to which chondrule material was recycled in the chondrule-forming region, is discussed in this report. Relics are grains that clearly did not crystallize in situ in the host chondrule. They represent coarse-grained precursor material that did not melt during chondrule formation, and provide the only tangible record of chondrule precursor grains. Relics are commonly identified by a large difference in size, textural differences, and/or significant compositional differences compared with normal grains in the host chondrule. Two important types of relics are: (1) 'dusty,' metal-bearing grains of olivine and pyroxene; and (2) forsterite (Mg-rich olivine) grains present in FeO-rich chondrules.

  12. Chemical 3D-imaging of glass inclusions from allende (CV3) olivine via SIMS: A new insight on chondrule formation conditions

    NASA Astrophysics Data System (ADS)

    Florentin, L.; Deloule, E.; Faure, F.; Mangin, D.

    2018-06-01

    Natural glass inclusions - hosted in Mg-rich olivines from Allende (CV3) type I chondrules - and synthetic melt inclusions - trapped in forsterite crystallized from CMAS (CaO-MgO-Al2O3-SiO2) melts - were mapped by Secondary Ion Mass Spectrometry (SIMS) for CMAS major oxides. The first ever 3D chemical images of extra-terrestrial glass inclusions were obtained, along with chemical depth profiles for each oxide. Results show similar patterns for both synthetic glass inclusions (trapped in olivine formed by slow crystallization in a magmatic liquid) and natural inclusions from Allende's olivines. No incompatible-rich boundary layer or diffusion pattern was observed in either case. The absence of an incompatible-rich boundary layer suggests that the olivine overgrowth surrounding glass inclusions in Allende's olivines was formed during slow cooling of the host olivine and likely the surrounding chondrule. This provides new constraints on the cooling rates of type I chondrules.

  13. Heterogeneity and O-16-Enrichments in Oxygen Isotope Ratios of Olivine from Chondrules in the Mokoia CV3 Chondrite

    NASA Technical Reports Server (NTRS)

    Jones, R. H.; Leshin, L. A.; Guan, Y.

    2002-01-01

    Two chondrules from Mokoia contain olivine in which oxygen isotopes are extremely heterogeneous, with some grains highly enriched in O-16. These data provide an important link between CAIs and chondrules. Additional information is contained in the original extended abstract.

  14. The Allende multicompound chondrule (ACC)—Chondrule formation in a local super-dense region of the early solar system

    NASA Astrophysics Data System (ADS)

    Bischoff, Addi; Wurm, Gerhard; Chaussidon, Marc; Horstmann, Marian; Metzler, Knut; Weyrauch, Mona; Weinauer, Julia

    2017-05-01

    In Allende, a very complex compound chondrule (Allende compound chondrule; ACC) was found consisting of at least 16 subchondrules (14 siblings and 2 independents). Its overall texture can roughly be described as a barred olivine object (BO). The BO texture is similar in all siblings, but does not exist in the two independents, which appear as relatively compact olivine-rich units. Because of secondary alteration of pristine Allende components and the ACC in particular, only limited predictions can be made concerning the original compositions of the colliding melt droplets. Based on textural and mineralogical characteristics, the siblings must have been formed on a very short time scale in a dense, local environment. This is also supported by oxygen isotope systematics showing similar compositions for all 16 subchondrules. Furthermore, the ACC subchondrules are isotopically distinct from typical Allende chondrules, indicating formation in or reaction with a more 16O-poor reservoir. We modeled constraints on the particle density required at the ACC formation location, using textural, mineral-chemical, and isotopic observations on this multicompound chondrule to define melt droplet collision conditions. In this context, we discuss the possible relationship between the formation of complex chondrules and the formation of macrochondrules and cluster chondrites. While macrochondrules may have formed under similar or related conditions as complex chondrules, cluster chondrites certainly require different formation conditions. Cluster chondrites represent a mixture of viscously deformed, seemingly young chondrules of different chemical and textural types and a population of older chondrules. Concerning the formation of ACC calculations suggest the existence of very local, kilometer-sized, and super-dense chondrule-forming regions with extremely high solid-to-gas mass ratios of 1000 or more.

  15. Oxygen isotope reservoirs in the outer asteroid belt inferred from oxygen isotope systematics of chondrule olivines and isolated forsterite and olivine grains in Tagish Lake-type carbonaceous chondrites, WIS 91600 and MET 00432

    NASA Astrophysics Data System (ADS)

    Yamanobe, Masakuni; Nakamura, Tomoki; Nakashima, Daisuke

    2018-03-01

    To understand oxygen isotope ratios and redox conditions of the chondrule formation environments of the outer rigions of the asteroid belt, we analyzed major element concentrations and oxygen isotope ratios of olivine grains in chondrules, isolated forsterite, and isolated olivine from the WIS 91600 and MET 00432 carbonaceous chondrites, which are thought to have originated from D-type asteroids located in the outer asteroid belt. The oxygen isotope ratios of individual chondrules and isolated grains show a wide variation in δ18O from -9.9‰ to +9.1‰ along the carbonaceous chondrite anhydrous mineral (CCAM) and primitive chondrule mineral (PCM) lines. The Δ17O (= δ17O - 0.52 × δ18O) values of the measured objects increase with decreasing Mg#; i.e., FeO-poor objects (Mg# > 90; type I chondrules and isolated forsterites) mainly have Δ17O values of ca. -6‰, and FeO-rich objects (Mg# < 90; type II chondrules and isolated olivines) have Δ17O values ranging from -3‰ to +2‰. Similar trends are observed for ferromagnesian silicate particles from comet Wild2 and CR chondrite chondrules, particularly in terms of FeO-rich objects with Δ17O values ranging from -3‰ to +2‰. It is suggested that FeO-rich objects formed in the outer regions of the asteroid belt and were transported to the outer solar nebular regions where comet Wild2 formed.

  16. Formation of chondrules in a moderately high dust enriched disk: Evidence from oxygen isotopes of chondrules from the Kaba CV3 chondrite

    NASA Astrophysics Data System (ADS)

    Hertwig, Andreas T.; Defouilloy, Céline; Kita, Noriko T.

    2018-03-01

    Oxygen three-isotope analysis by secondary ion mass spectrometry of chondrule olivine and pyroxene in combination with electron microprobe analysis were carried out to investigate 24 FeO-poor (type I) and 2 FeO-rich (type II) chondrules from the Kaba (CV) chondrite. The Mg#'s of olivine and pyroxene in individual chondrules are uniform, which confirms that Kaba is one of the least thermally metamorphosed CV3 chondrites. The majority of chondrules in Kaba contain olivine and pyroxene that show indistinguishable Δ17O values (= δ17O - 0.52 × δ18O) within analytical uncertainties, as revealed by multiple spot analyses of individual chondrules. One third of chondrules contain olivine relict grains that are either 16O-rich or 16O-poor relative to other indistinguishable olivine and/or pyroxene analyses in the same chondrules. Excluding those isotopically recognized relicts, the mean oxygen isotope ratios (δ18O, δ17O, and Δ17O) of individual chondrules are calculated, which are interpreted to represent those of the final chondrule melt. Most of these isotope ratios plot on or slightly below the primitive chondrule mineral (PCM) line on the oxygen three-isotope diagram, except for the pyroxene-rich type II chondrule that plots above the PCM and on the terrestrial fractionation line. The Δ17O values of type I chondrules range from ∼-8‰ to ∼-4‰; the pyroxene-rich type II chondrule yields ∼0‰, the olivine-rich type II chondrule ∼-2‰. In contrast to the ungrouped carbonaceous chondrite Acfer 094, the Yamato 81020 CO3, and the Allende CV3 chondrite, type I chondrules in Kaba only possess Δ17O values below -3‰ and a pronounced bimodal distribution of Δ17O values, as evident for those other chondrites, was not observed for Kaba. Investigation of the Mg#-Δ17O relationship revealed that Δ17O values tend to increase with decreasing Mg#'s, similar to those observed for CR chondrites though data from Kaba cluster at the high Mg# (>98) and the low Δ17O

  17. The Vaguries of Pyroxene Nucleation and the Resulting Chondrule Textures

    NASA Technical Reports Server (NTRS)

    Lofgren, G. E.; Le, L.

    2004-01-01

    Pyroxene is a major phase in chondrules, but often follows olivine in the crystallization sequence and depending on the melting temperature and time may not nucleate readily upon cooling. Dynamic crystallization experiments based on total or near total melting were used to study PO (porphyritic olivine) and PP (Porphyritic pyroxene) compositions as defined by. The experiments showed that pyroxene nucleated only at subliquidus temperatures in the PP melts and rarely in the PO melts. Porphyritic chondrules with phenocrysts of both olivine and pyroxene (POP chondrules) were not easily produced in the experiments. POP chondrules are common and it is important for deciphering their formation that we understand pyroxene nucleation properties of chondrule melts.

  18. Chromite and olivine in type II chondrules in carbonaceous and ordinary chondrites - Implications for thermal histories and group differences

    NASA Technical Reports Server (NTRS)

    Johnson, Craig A.; Prinz, Martin

    1991-01-01

    Unequilibrated chromite and olivine margin compositions in type II chondrules are noted to differ systematically among three of the chondrite groups, suggesting that type II liquids differed in composition among the groups. These differences may be interpreted as indicators of different chemical compositions of the precursor solids which underwent melting, or, perhaps, as differences in the extent to which immiscible metal sulfide droplets were lost during chondrule formation. Because zinc is detectable only in type II chromites which have undergone reequilibration, the high zinc contents reported for chondritic chromites in other studies probably reflect redistribution during thermal metamorphism.

  19. Timing of Formation of a Wassonite-bearing Chondrule

    NASA Technical Reports Server (NTRS)

    Needham, A. W.; Nakamura-Messenger, K.; Rubin, A. E.; Choi, B.-G.; Messenger, S.

    2014-01-01

    Wassonite, ideally stoichiometric TiS, is a titanium monosulfide recently discovered in the Yamato 691 EH3 enstatite chondrite. Wassonite grains were located within the mesostasis of a single barred olivine chondrule. Such chondrules likely formed in the solar nebula by melting of fine grained precursor dust. The reduced nature of enstatite chondrites, and the wassonite-bearing chondrule in particular, may suggest precursor materials included Ti-bearing troilite, metallic Fe-Ni, and possibly graphite. Under the reducing conditions present in enstatite chondrites S can partition more readily into silicate melt, leading to raised Ti content of the residual Fe-FeS melt. By the time sulfide crystallized from the melt, the Ti concentration was high enough to form small grains of pure TiS - wassonite. As a mineral not previously observed in nature wassonite and its host chondrule may provide additional constraints on physical and chemical conditions in the solar nebula at a specific time and location relevant to planetary formation. Enstatite chondrites and Earth share similar isotopic compositions of Cr, Ni, Ti, O and N. Understanding the formation conditions of enstatite chondrite chondrules may therefore have wider relevance for terrestrial planet accretion and other early inner solar system processes. Here we present preliminary results of an investigation of the Al-Mg systematics of the only known wassonite-bearing chondrule. The goal of this study is to determine whether this chondrule's formation was contemporaneous with other enstatite chondrite chondrules and to establish its place in the broader timeline of solar system events.

  20. Tetrad effects in REE abundance patterns of chondrules from CM meteorites: Implications for aqueous alteration on the CM parent asteroid

    NASA Astrophysics Data System (ADS)

    Inoue, Mutsuo; Nakamura, Noboru; Kimura, Makoto

    2009-09-01

    Lanthanide tetrad effect in bulk chondrules from two moderately altered CM chondrites, Murchison and Yamato-793321 (Y-793321), are reported for the first time. Twenty-three chondrules were petrographically characterized and analyzed for 10 rare earth elements (REE) and other trace and major elements (Ba, Sr, Rb, K, Ca, Mg and Fe) using the precise isotope dilution technique. The results indicate systematic depletion (several times) of alkali and alkaline earths compared to CV and CO chondrules. Most of the porphyritic olivine (8 PO) and olivine-pyroxene (4 POP), porphyritic and radial pyroxene (2 PP, 1 RP), and granular olivine (1 GO) chondrules show a light-REE (L-REE) depleted, heavy-REE (H-REE) smoothly fractionated pattern composed of four (upward convex) segments possessing a relatively large negative Eu anomaly (CI-normalized La/Sm, Lu/Er and Eu/Eu* ratios = 0.3-1: Eu*, normal value). On the other hand, all barred-olivine (5 BO) chondrules, a few PO and POP indicate almost a flat L-REE pattern. In addition, regardless of their textural types, nearly half of the chondrules have a variable degree of Ce and Yb anomalies, and/or L/H-REE discontinuity, which is similar to CV and CO chondrules. The observed L- and H-convex REE patterns accompanied with the negative Eu anomaly is the first known case for chondrules as well as meteoritic materials, but have been previously reported for geological samples such as sedimentary rocks, late stage igneous and metamorphic rocks, and are explained as the lanthanide tetrad effect, which plausibly results from fluid-rock interaction. We suggest that the marked REE fractionations occurred by the selective incorporation of L-, H-REEs and Eu into alteration products in the matrix during alteration processes on the CM parent body, but that the gas/solid REE fractionation characteristics established in the nebula have basically remained unchanged. We suggest that the tetrad effects observed here represent a new index of physico

  1. Amoeboid olivine aggregates with low-Ca pyroxenes: a genetic link between refractory inclusions and chondrules?

    NASA Astrophysics Data System (ADS)

    Krot, Alexander N.; Petaev, Michail I.; Yurimoto, Hisayoshi

    2004-04-01

    Amoeboid olivine aggregates (AOAs) in primitive (unmetamorphosed and unaltered) carbonaceous chondrites are uniformly 16O-enriched (Δ 17O ˜ -20‰) and consist of forsterite (Fa <2), FeNi-metal, and a refractory component (individual CAIs and fine-grained minerals interspersed with forsterite grains) composed of Al-diopside, anorthite, ±spinel, and exceptionally rare melilite (Åk <15); some CAIs in AOAs have compact, igneous textures. Melilite in AOAs is replaced by a fine-grained mixture of spinel, Al-diopside, and anorthite. Spinel is corroded by anorthite or by Al-diopside. In ˜10% of > 500 AOAs studied in the CR, CV, CM, CO, CH, CB, and ungrouped carbonaceous chondrites Acfer 094, Adelaide, and LEW85332, forsterite is replaced to a various degree by low-Ca pyroxene. There are three major textural occurrences of low-Ca pyroxene in AOAs: (i) thin (<10 μm) discontinuous layers around forsterite grains or along forsterite grain boundaries in AOA peripheries; (ii) haloes and subhedral grains around FeNi-metal nodules in AOA peripheries, and (iii) thick (up to 70 μm) continuous layers with abundant tiny inclusions of FeNi-metal grains around AOAs. AOAs with low-Ca pyroxene appear to have experienced melting of various degrees. In the most extensively melted AOA in the CV chondrite Leoville, only spinel grains are relict; forsterite, anorthite and Al-diopside were melted. This AOA has an igneous rim of low-Ca pyroxene with abundant FeNi-metal nodules and is texturally similar to Type I chondrules. Based on these observations and thermodynamic analysis, we conclude that AOAs are aggregates of relatively low temperature solar nebular condensates originated in 16O-rich gaseous reservoir(s), probably CAI-forming region(s). Some of the CAIs were melted before aggregation into AOAs. Many AOAs must have also experienced melting, but of a much smaller degree than chondrules. Before and possibly after aggregation, melilite and spinel reacted with the gaseous SiO and Mg

  2. Petrology and thermal history of type IA chondrules in the Semarkona (LL3.0) chondrite

    NASA Technical Reports Server (NTRS)

    Jones, R. H.; Scott, E. R. D.

    1989-01-01

    Detailed petrologic studies have been made of 15 type IA, Fe-poor, porphyritic olivine chondrules in Semarkona (LL3.0). Major and minor element concentrations in olivines, pyroxenes, and mesostases, and bulk composition so the chondrules are measured along with zoning profiles in the olivine and pyroxene crystals. The mineral compositions and textures are best interpreted in terms of closed system crystallization in which the olivines and pyroxenes crystallized in situ from a melt corresponding to the bulk composition of the chondrule. Relict olivine grains are not found in the chondrules. Crystallization probably occurred at a cooling rate of the order of 1000 C/hr. Precursor materials of the chondrules were composed of two components, one refractory Ca-, Al-, and Ti-rich, and one less refractory Si-, Fe-, Cr-, and Mn-rich. The evidence is consistent with Semarkona being one of the least metamorphosed ordinary chondrites.

  3. Textural evidence bearing on the origin of isolated olivine crystals in C2 carbonaceous chondrites

    NASA Technical Reports Server (NTRS)

    Richardson, S. M.; Mcsween, H. Y., Jr.

    1978-01-01

    In some cases the mechanical competence of chondrules in carbonaceous chondrites has been reduced by alteration of their mesostasis glass to friable phyllosilicate, providing a mechanism by which euhedral olivines can be separated from chondrules. Morphological features of isolate olivine grains found in carbonaceous chondrites are similar to those of olivine phenocrysts in chondrules. These observations suggest that the isolated olivine grains formed in chondrules, by crystallization from a liquid, rather than by condensation from a vapor.

  4. Chondrule formation, metamorphism, brecciation, an important new primary chondrule group, and the classification of chondrules

    NASA Technical Reports Server (NTRS)

    Sears, Derek W. G.; Shaoxiong, Huang; Benoit, Paul H.

    1995-01-01

    The recently proposed compositional classification scheme for meteoritic chondrules divides the chondrules into groups depending on the composition of their two major phases, olivine (or pyroxene) and the mesostasis, both of which are genetically important. The scheme is here applied to discussions of three topics: the petrographic classification of Roosevelt County 075 (the least-metamorphosed H chondrite known), brecciation (an extremely important and ubiquitous process probably experienced by greater than 40% of all unequilibrated ordinary chondrites), and the group A5 chondrules in the least metamorphosed ordinary chondrites which have many similarities to chondrules in the highly metamorphosed 'equilibrated' chondrites. Since composition provides insights into both primary formation properties of the chondruies and the effects of metamorphism on the entire assemblage it is possible to determine the petrographic type of RC075 as 3.1 with unique certainty. Similarly, the near scheme can be applied to individual chondrules without knowledge of the petrographic type of the host chondrite, which makes it especially suitable for studying breccias. Finally, the new scheme has revealed the existence of chondrules not identified by previous techniques and which appear to be extremely important. Like group A1 and A2 chondrules (but unlike group B1 chondrules) the primitive group A5 chondruies did not supercool during formation, but unlike group A1 and A2 chondrules (and like group B1 chondrules) they did not suffer volatile loss and reduction during formation. It is concluded that the compositional classification scheme provides important new insights into the formation and history of chondrules and chondrites which would be overlooked by previous schemes.

  5. Congruent Melting Kinetics: Constraints on Chondrule Formation

    NASA Technical Reports Server (NTRS)

    Greenwood, James P.; Hess, Paul C.

    1995-01-01

    The processes and mechanisms of melting and their applications to chondrule formation are discussed A model for the kinetics of congruent melting is developed and used to place constraints on the duration and maximum temperature experienced by the interiors of relict-bearing chondrules. Specifically, chondrules containing relict forsteritic olivine or enstatitic pyroxene cannot have been heated in excess of 1901 C or 1577 C, respectively, for more than a few seconds.

  6. Young Pb-Isotopic Ages of Chondrules in CB Carbonaceous Chondrites

    NASA Technical Reports Server (NTRS)

    Amelin, Yuri; Krot, Alexander N.

    2005-01-01

    CB (Bencubbin-type) carbonaceous chondrites differ in many ways from more familiar CV and CO carbonaceous chondrites and from ordinary chondrites. CB chondrites are very rich in Fe-Ni metal (50-70 vol%) and contain magnesian silicates mainly as angular to sub-rounded clasts (or chondrules) with barred olivine (BO) or cryptocrystalline (CC) textures. Both metal and silicates appear to have formed by condensation. The sizes of silicate clasts vary greatly between the two subgroups of CB chondrites: large (up to one cm) in CB(sub a) chondrites, and typically to much much less than 1 mm in CB(sub b) chondrites. The compositional and mineralogical differences between these subgroups and between the CB(sub s) and other types of chondrites suggest different environment and possibly different timing of chondrule formation. In order to constrain the timing of chondrule forming processes in CB(sub s) and understand genetic relationship between their subgroups, we have determined Pb-isotopic ages of silicate material from the CB(sub a) chondrite Gujba and CB(sub b) chondrite Hammadah al Hamra 237 (HH237 hereafter).

  7. CM and CO chondrites: A common parent body or asteroidal neighbors? Insights from chondrule silicates

    NASA Astrophysics Data System (ADS)

    Schrader, Devin L.; Davidson, Jemma

    2017-10-01

    By investigating the petrology and chemical composition of type II (FeO-rich) chondrules in the Mighei-like carbonaceous (CM) chondrites we constrain their thermal histories and relationship to the Ornans-like carbonaceous (CO) chondrites. We identified FeO-rich relict grains in type II chondrules by their Fe/Mn ratios; their presence indicates chondrule recycling among type II chondrules. The majority of relict grains in type II chondrules are FeO-poor olivine grains. Consistent with previous studies, chemical similarities between CM and CO chondrite chondrules indicate that they had similar formation conditions and that their parent bodies probably formed in a common region within the protoplanetary disk. However, important differences such as mean chondrule size and the lower abundance of FeO-poor relicts in CM chondrite type II chondrules than in CO chondrites suggest CM and CO chondrules did not form together and they likely originate from distinct parent asteroids. Despite being aqueously altered, many CM chondrites contain pre-accretionary anhydrous minerals (i.e., olivine) that are among the least thermally metamorphosed materials in chondrites according to the Cr2O3 content of their ferroan olivine. The presence of these minimally altered pre-accretionary chondrule silicates suggests that samples to be returned from aqueously altered asteroids by the Hayabusa2 and OSIRIS-REx asteroid sample return missions, even highly hydrated, may contain silicates that can provide information about the pre-accretionary histories and conditions of asteroids Ryugu and Bennu, respectively.

  8. Non-spherical Lobate Chondrules in CO3.0 Y-81020: General Implications for the Formation of Low-FeO Porphyritic Chondrules in CO Chondrites

    NASA Technical Reports Server (NTRS)

    Rubin, Alan E.; Wasson, John T.

    2006-01-01

    Non-spherical chondrules (arbitrarily defined as having aspect ratios greater than or equal to 1.20) in CO3.0 chondrites comprise multi-lobate, distended, and highly irregular objects with rounded margins; they constitute approx. 70% of the type-I (low-FeO) porphyritic chondrules in Y-81020, approx. 75% of such chondrules in ALHA77307, and approx. 60% of those in Colony. Although the proportion of non-spherical type-I chondrules in LL3.0 Semarkona is comparable (approx. 60%), multi-lobate OC porphyritic chondrules (with lobe heights equivalent to a significant fraction of the mean chondrule diameter) are rare. If the non-spherical type-I chondrules in CO chondrites had formed from totally molten droplets, calculations indicate that they would have collapsed into spheres within approx. 10(exp -3) s, too little time for their 20-micrometer-size olivine phenocrysts to have grown from the melt. These olivine grains must therefore be relicts from an earlier chondrule generation; the final heating episode experienced by the non-spherical chondrules involved only minor amounts of melting and crystallization. The immediate precursors of the individual non-spherical chondrules may have been irregularly shaped chondrule fragments whose fracture surfaces were rounded during melting. Because non-spherical chondrules and circular chondrules form a continuum in shape and have similar grain sizes, mineral and mesostasis compositions, and modal abundances of non-opaque phases, they must have formed by related processes. We conclude that a large majority of low-FeO chondrules in CO3 chondrites experienced a late, low-degree melting event. Previous studies have shown that essentially all type-II (high-FeO) porphyritic chondrules in Y-81020 formed by repeated episodes of low-degree melting. It thus appears that the type-I and type-II porphyritic chondrules in Y-81020 (and, presumably, all CO3 chondrites) experienced analogous formation histories. Because these two types constitute

  9. Oxygen isotope systematics of chondrules in the Murchison CM2 chondrite and implications for the CO-CM relationship

    NASA Astrophysics Data System (ADS)

    Chaumard, Noël; Defouilloy, Céline; Kita, Noriko T.

    2018-05-01

    High-precision oxygen three-isotope measurements of olivine and pyroxene were performed on 29 chondrules in the Murchison CM2 chondrite by secondary ion mass spectrometry (SIMS). The oxygen isotope ratios of analyzed chondrules all plot very close to the primitive chondrule minerals (PCM) line. In each of 24 chondrules, the olivine and/or pyroxene grains analyzed show indistinguishable oxygen isotope ratios. Exceptions are minor occurrences of isotopically distinguished relict olivine grains, which were found in nine chondrules. The isotope homogeneity of these phenocrysts is consistent with a co-magmatic crystallization of olivine and pyroxene from the final chondrule melts and a significant oxygen isotope exchange between the ambient gas and the melts. Homogeneous type I chondrules with Mg#'s of 98.9-99.5 have host chondrule Δ17O values ranging from -6.0‰ to -4.1‰, with one exception (Δ17O: -1.2‰; Mg#: 99.6). Homogeneous chondrules with Mg#'s <96, including four type II chondrules (Mg# ∼65-70), have Δ17O values of around -2.5‰. Five type I chondrules (Mg# ≥99) have internally heterogeneous oxygen isotope ratios with Δ17O values ranging from -6.5‰ to -4.0‰, similar to those of host chondrule values. These heterogeneous chondrules have granular or porphyritic textures, convoluted outlines, and contain numerous metal grains dispersed within fine-grained silicates. This is consistent with a low degree of melting of the chondrule precursors, possibly because of a low temperature of the melting event and/or a shorter duration of melting. The Δ17O values of relict olivine grains in nine chondrules range from -17.9‰ to -3.4‰, while most of them overlap the range of the host chondrule values. Similar to those reported from multiple carbonaceous chondrites (Acfer 094, Y-82094, CO, and CV), the Δ17O ∼ -5‰ and high Mg# (≥99) chondrules, which might derive from a reduced reservoir with limited dust enrichments (∼50 × Solar System), dominate

  10. Secondary melting events in Semarkona chondrules revealed by compositional zoning in low-Ca pyroxene

    NASA Astrophysics Data System (ADS)

    Baecker, Bastian; Rubin, Alan E.; Wasson, John T.

    2017-08-01

    It is well established that many chondrules contain relict grains formed in previous generations of chondrules. We here describe evidence that chondrules experienced multiple mesostasis melting events while remaining closed systems. Spheroidal chondrule shapes resulted from surface-tension effects following a primary heating event that caused substantial melting (≳40%) of the precursor assemblages. In some high-FeO chondrules in LL3.00 Semarkona, low-Ca pyroxene phenocrysts show multiple overgrowth layers produced by secondary melting events. We characterized these layers with the electron microprobe in terms of Fe, Ca and Cr in two Semarkona chondrules. The first low-Ca pyroxene overgrowth that forms after a minor heating/melting event has low Ca and Fe; concentrations of these incompatibles gradually increase over the next 8 ± 4 μm until falling temperatures and slowing diffusion caused growth to stop. The next melting event remelts and mixes the local mesostasis; cooling causes growth of a normal igneously zoned layer. In the simplest cases, the Ca concentrations at the minima gradually increase towards the edge of the phenocryst. Heat deposition during heating events varied over a wide range; the weakest events produced recognizable changes in slopes (that we call "inflections" rather than minima). Large fractions of the individual phenocrysts were formed by the process that produced the overgrowth layers. It appears that overgrowth formation stopped when the Ca content of the mesostasis became high enough to make high-Ca pyroxene a liquidus phase. Both Semarkona chondrules include olivine phenocrysts similar in size and modal abundance to the low-Ca pyroxene phenocrysts. Olivine compositional profiles show symmetrical, apparently normal zoning except for asymmetries attributable to the presence of relict grains. Surface compositions of different olivine phenocrysts in the same chondrule are very similar to one another, consistent with growth from

  11. Using the Fe/Mn Ratio of FeO-Rich Olivine In WILD 2, Chondrite Matrix, and Type IIA Chondrules to Disentangle Their Histories

    NASA Technical Reports Server (NTRS)

    Frank, David R.; Le, L.; Zolensky, M. E.

    2012-01-01

    The Stardust Mission returned a large abundance of impactors from Comet 81P/Wild2 in the 5-30 m range. The preliminary examination of just a limited number of these particles showed that the collection captured abundant crystalline grains with a diverse mineralogy [1,2]. Many of these grains resemble those found in chondrite matrix and even contain fragments of chondrules and CAIs [1-3]. In particular, the olivine found in Wild 2 exhibits a wide compositional range (Fa0-97) with minor element abundances similar to the matrix olivine found in many carbonaceous chondrites (CCs) and unequilibrated ordinary chondrites (UOCs). Despite the wide distribution of Fa content, the olivine found in the matrices of CCs, UOCs, and Wild 2 can be roughly lumped into two types based solely on fayalite content. In fact, in some cases, a distinct bi-modal distribution is observed.

  12. Evidence for the presence of planetesimal material among the precursors of magnesian chondrules of nebular origin

    NASA Astrophysics Data System (ADS)

    Libourel, Guy; Krot, Alexander N.

    2007-02-01

    Chondrules are the major high-temperature components of chondritic meteorites, which are conventionally viewed as the samples from the very first generation of undifferentiated planetesimals. Growing evidences from long- and short-lived radionuclide chronologies indicate however that chondrite parent asteroids accreted after or contemporaneously with igneous activities on differentiated asteroids, questioning the pristine nature of chondrites. Here we report a discovery of metal-bearing olivine aggregates with granoblastic textures inside magnesian porphyritic (Type I) chondrules from the CV carbonaceous chondrite Vigarano. Formation of the granoblastic textures requires sintering and prolonged, high-temperature (> 1000 °C) annealing - conditions which are not expected in the solar nebula during chondrule formation, but could have been achieved on parent bodies of olivine-rich differentiated or thermally metamorphosed meteorites. The mineralogy and petrography of the metal-olivine aggregates thus indicate that they are relict, dunite-like lithic fragments which resulted from fragmentation of such bodies. The very old Pb-Pb absolute ages and Al-Mg relative model ages of bulk CV chondrules suggest that such planetesimals may have formed as early as the currently accepted age of the Solar System (4567.2 ± 0.6 Ma).

  13. Chronology of formation of early solar system solids from bulk Mg isotope analyses of CV3 chondrules

    NASA Astrophysics Data System (ADS)

    Chen, Hsin-Wei; Claydon, Jennifer L.; Elliott, Tim; Coath, Christopher D.; Lai, Yi-Jen; Russell, Sara S.

    2018-04-01

    We have analysed the petrography, major element abundances and bulk Al-Mg isotope systematics of 19 ferromagnesian chondrules from the CV3 chondrites Allende, Mokoia, and Vigarano, together with an Al-rich chondrule and refractory olivine from Mokoia. Co-variations of Al/Mg with Na/Mg and Ti/Mg in our bulk chondrules suggest their compositions are dominantly controlled by reworking of different proportions of chondrule components (e.g. mafic minerals and mesostatis); their precursors are thus fragments from prior generations of chondrules. Our samples show a range in fractionation corrected 26Mg/24Mg (Δ‧26Mg) ∼ 60 ppm, relative to precisions <±5 ppm (2se) and these values broadly covary with 27Al/24Mg. The data can be used to calculate model initial 26Al/27Al, or (26Al/27Al)0, of the chondrule precursors. Our resolvably radiogenic chondrules yield model (26Al/27Al)0 ∼ 1-2 × 10-5, equivalent to model "ages" of precursor formation ≦1 Ma post CAI. However, many of our chondrules show near solar Δ‧26Mg and no variability despite a range in 27Al/24Mg. This suggests their derivation either from younger precursor chondrules or open system behaviour once 26Al was effectively extinct ((26Al/27Al)0 < 0.8 × 10-5, given the resolution here). Evidence for the latter explanation is provided by marked rims of orthopyroxene replacing olivine, indicating reaction of chondrules with a surrounding silicate vapour. Concurrent isotopic exchange of Mg with a near chondritic vapour during late reworking could explain their isotopic systematics. One ferromagnesian object is dominated by a high Mg# olivine with elevated Ti and Ca abundances. This refractory olivine has a markedly negative Δ‧26Mg = -16 ± 3 ppm (2se), reflecting its early removal (model age of <0.5 Ma post CAI), from a reservoir with evolving Δ‧26Mg. If representative of the chondrule forming region, this grain defines a minimum interval of radiogenic ingrowth for CV chondrites commensurate with (26Al

  14. The Formation of Chondrules: Petrologic Tests of the Shock Wave Model

    NASA Technical Reports Server (NTRS)

    Connolly, H. C., Jr.; Love, S. G.

    1998-01-01

    Chondrules are mm-sized spheroidal igneous components of chondritic meteorites. They consist of olivine and orthopyroxene set in a glassy mesostasis with varying minor amounts of metals, sulfieds, oxides and carbon phases.

  15. Oxygen isotope characteristics of chondrules from the Yamato-82094 ungrouped carbonaceous chondrite: Further evidence for common O-isotope environments sampled among carbonaceous chondrites

    NASA Astrophysics Data System (ADS)

    Tenner, T. J.; Kimura, M.; Kita, N. T.

    2017-02-01

    High-precision secondary ion mass spectrometry (SIMS) was employed to investigate oxygen three isotopes of phenocrysts in 35 chondrules from the Yamato (Y) 82094 ungrouped 3.2 carbonaceous chondrite. Twenty-one of 21 chondrules have multiple homogeneous pyroxene data (∆17O 3SD analytical uncertainty: 0.7‰); 17 of 17 chondrules have multiple homogeneous pyroxene and plagioclase data. Twenty-one of 25 chondrules have one or more olivine data matching coexisting pyroxene data. Such homogeneous phenocrysts (1) are interpreted to have crystallized from the final chondrule melt, defining host O-isotope ratios; and (2) suggest efficient O-isotope exchange between ambient gas and chondrule melt during formation. Host values plot within 0.7‰ of the primitive chondrule mineral (PCM) line. Seventeen chondrules have relict olivine and/or spinel, with some δ17O and δ18O values approaching -40‰, similar to CAI or AOA-like precursors. Regarding host chondrule data, 22 of 34 have Mg#s of 98.8-99.5 and ∆17O of -3.9‰ to -6.1‰, consistent with most Acfer 094, CO, CR, and CV chondrite chondrules, and suggesting a common reduced O-isotope reservoir devoid of 16O-poor H2O. Six Y-82094 chondrules have ∆17O near -2.5‰, with Mg#s of 64-97, consistent with lower Mg# chondrules from Acfer 094, CO, CR, and CV chondrites; their signatures suggest precursors consisting of those forming Mg# 99, ∆17O: -5‰ ± 1‰ chondrules plus 16O-poor H2O, at high dust enrichments. Three type II chondrules plot slightly above the PCM line, near the terrestrial fractionation line (∆17O: +0.1‰). Their O-isotopes and olivine chemistry are like LL3 type II chondrules, suggesting they sampled ordinary chondrite-like chondrule precursors. Finally, three Mg# >99 chondrules have ∆17O of -6.7‰ to -8.1‰, potentially due to 16O-rich refractory precursor components. The predominance of Mg# 99, ∆17O: -5‰ ± 1‰ chondrules and a high chondrule-to-matrix ratio suggests bulk Y-82094

  16. Relict chondrules in primitive achondrites: Remnants from their precursor parent bodies

    NASA Astrophysics Data System (ADS)

    Schrader, Devin L.; McCoy, Timothy J.; Gardner-Vandy, Kathryn

    2017-05-01

    We studied the petrography, analyzed the chemical compositions, constrained the closure temperatures (via geothermometry), and determined the oxidation states of relict chondrules in Campo del Cielo (IAB iron meteorite), Graves Nunataks (GRA) 98028 (acapulcoite), and Netschaëvo (IIE iron meteorite) to constrain their formation conditions and investigate links to known meteorite groups. Despite having been thermally metamorphosed, mineral phases within relict chondrules retain information about their precursor compositions. The sizes and textures of relict chondrules, and silicate and chromite compositions indicate that Campo del Cielo, GRA 98028, and Netschaëvo had distinct parent bodies that were similar to, but different from, known chondrite groups. To determine the utility of relict chondrule sizes in thermally metamorphosed meteorites, we determined the chondrule size distributions in the LL chondrites Semarkona (LL3.00), Soko-Banja (LL4), Siena (LL5), and Saint-Séverin (LL6), and the H chondrites Clovis (No. 1) (H3.6), Kesen (H4), Arbol Solo (H5), and Estacado (H6). As expected, mean chondrule diameters increase with degree of thermal metamorphism. We find that Campo del Cielo and GRA 98028 were reduced during thermal metamorphism, consistent with previous studies, indicating that their precursors were initially more FeO-rich than their current compositions. In contrast to previous studies, we find no evidence for reduction of silicates in Netschaëvo. Normal zoning of olivine in Netschaëvo is consistent with crystallization and suggests its silicates are near their primary FeO-contents. The presence of elongated chromite grains along olivine grain boundaries in Netschaëvo indicates formation during thermal metamorphism under oxidizing conditions. Due to the absence of reduction and the composition of chromite being distinct from that of metamorphosed H chondrites, we conclude that Netschaëvo, and by extension the IIE iron meteorites, are not from the H

  17. The solar nebula redox state as recorded by the most reduced chondrules of five primitive chondrites

    NASA Technical Reports Server (NTRS)

    Johnson, M. C.

    1986-01-01

    Mafic minerals in the most reduced chondrules of five primitive meteorites were analyzed with an electron microprobe to determine the lower limit on their FeO contents. The accuracy obtained was + or - 0.01 weight percent FeO. The thermodynamic relationship between mole fraction FeSiO3 and pO2 of the ambient nebular gas at the time of mineral equilibration was established, and was used to infer the local O/H ratio of the nebular gas during chondrule formation. The lowest ferrosilite compositions reflected equilibration at 1500 K with a gas 2-18 times more oxidizing than a gas of solar composition. Olivines in low-FeO unequilibrated ordinary chondrites (UOC) chondrules are uniformly more FeO-rich than coexisting pyroxenes. This discrepancy suggests that a significant change in the O/H ratio of the nebular gas occurred between the time of olivine and pyroxene crystallization in the region of the nebula where UOCs formed. Mineral compositions in the chondrules of two C2 chondrites studied suggest they formed in a more homogeneous region of the nebula than the UOCs.

  18. Sulfur and sulfides in chondrules

    NASA Astrophysics Data System (ADS)

    Marrocchi, Yves; Libourel, Guy

    2013-10-01

    suggest the occurrence of an external source of iron, very likely gaseous, during chondrule formation. We therefore propose that enrichments in sulfur (and other volatile and moderately volatile elements) from PO to PP type I bulk chondrule compositions towards chondritic values result from progressive reaction between partially depleted olivine-bearing precursors and a volatile-rich gas phase.

  19. Complex zoning behavior in pyroxene in FeO-rich chondrules in the Semarkona ordinary chondrite

    NASA Technical Reports Server (NTRS)

    Jones, Rhian H.; Papike, J. J.

    1993-01-01

    A detailed understanding of the properties of silicate minerals in chondrules is essential to the interpretation of chondrule formation conditions. This study is further work in a series of petrologic studies of chondrules in the least equilibrated LL chondrite, Semarkona (LL3.0). The objectives of this work are as follows: (1) to understand chondrule formation conditions and nebular processes; and (2) to use the data as a basis for understanding the effects of metamorphism in more equilibrated chondrites. FeO-rich pyroxene in the chondrules described shows complex zoning behavior. Low-Ca clinopyroxene, orthopyroxene, pigeonite, and augite are all observed, in various associations with one another. Coexisting olivine phenocrysts are also FeO-rich and strongly zoned. Compositional and zoning properties are similar to those observed in boninites and are interpreted as resulting from rapid cooling of individual chondrules.

  20. Impact-Induced Chondrule Deformation and Aqueous Alteration of CM2 Murchison

    NASA Technical Reports Server (NTRS)

    Hanna, R. D.; Zolensky, M.; Ketcham, R. A.; Behr, W. M.; Martinez, J. E.

    2014-01-01

    Deformed chondrules in CM2 Murchison have been found to define a prominent foliation [1,2] and lineation [3] in 3D using X-ray computed tomography (XCT). It has been hypothesized that chondrules in foliated chondrites deform by "squeezing" into surrounding pore space [4,5], a process that also likely removes primary porosity [6]. However, shock stage classification based on olivine extinction in Murchison is consistently low (S1-S2) [4-5,7] implying that significant intracrystalline plastic deformation of olivine has not occurred. One objective of our study is therefore to determine the microstructural mechanisms and phases that are accommodating the impact stress and resulting in relative displacements within the chondrules. Another question regarding impact deformation in Murchison is whether it facilitated aqueous alteration as has been proposed for the CMs which generally show a positive correlation between degree of alteration and petrofabric strength [7,2]. As pointed out by [2], CM Murchison represents a unique counterpoint to this correlation: it has a strong petrofabric but a relatively low degree of aqueous alteration. However, Murchison may not represent an inconsistency to the proposed causal relationship between impact and alteration, if it can be established that the incipient aqueous alteration post-dated chondrule deformation. Methods: Two thin sections from Murchison sample USNM 5487 were cut approximately perpendicular to the foliation and parallel to lineation determined by XCT [1,3] and one section was additionally polished for EBSD. Using a combination of optical petrography, SEM, EDS, and EBSD several chondrules were characterized in detail to: determine phases, find microstructures indicative of strain, document the geometric relationships between grain-scale microstructures and the foliation and lineation direction, and look for textural relationships of alteration minerals (tochilinite and Mg-Fe serpentine) that indicate timing of their

  1. A RELICT Spinel Grain in an Allende Ferromagnesian Chondrule

    NASA Astrophysics Data System (ADS)

    Misawa, K.; Fujita, T.; Kitamura, M.; Nakamura, N.; Yurimoto, H.

    1993-07-01

    It is suggested that one of the refractory lithophile precursors in CV-CO chondrules was a hightemperature condensate from the nebular gas and was related to Ca,Al-rich inclusions (CAIs) [1-3]. However, little is known about refractory siderophile precursors in chondrules [4]. Allende barred olivine chondrule R-11 consists mainly of olivine (Fa(sub)7- 18), pyroxene (En(sub)93Fs(sub)1Wo(sub)6, En(sub)66Fs(sub)1Wo(sub)33), plagioclase (An(sub)80), Fe-poor spinel, and alkali-rich glass. The CI- chondrite normalized REE pattern of the chondrule, excluding a spinel grain, are fractionated, HREEdepleted (4.6-7.8 x CI) with a large positive Yb anomaly. The REE abundances are hump-shaped functions of elemental volatility, moderately refractory REE-enriched, suggesting that the refractory lithophile precursor component of R-11 could be a condensate from the nebular gas and related to Group 11 CAIs [1,2]. An interior portion of spinel is almost Fe-free, but in an outer zone (2040 micrometers in width) FeO contents increase rapidly. TiO(sub)2, Cr(sub)2O(sub)3, and V(sub)2O(sub)3 contents in core spinel are less than 0.5%, which is different from the V-rich nature of spinel in fluffy Type A CAIs [5]. The Fe-Mg zoning of spinel may have been generated by diffusional emplacement of Mg and Fe during chondrule-forming events. The spinel contains silicate inclusions and tiny metallic grains. The largest silicate inclusion is composed of Al,Ti-rich pyroxene and Ak 40 melilite. One of the submicrometersized grains was analyzed by SEM-EDS and found to be composed of refractory Pt-group metals with minor amounts of Fe and Ni. This is the first occurrence of refractory Pt-group metal nuggets in a ferromagnesian chondrule from the Allende meteorite. Tungsten, Os, Ir, Mo, and Ru are enriched 2-6 x 10^5 relative to CIs, and abundances of Pt and Rh decrease 2-10 x 10^4 with increasing volatility. In addition, abundances of Fe and Ni in the nugget are equal to or less than that CI chondrites

  2. Chondrules born in plasma? Simulation of gas-grain interaction using plasma arcs with applications to chondrule and cosmic spherule formation

    NASA Astrophysics Data System (ADS)

    Morlok, A.; Sutton, Y. C.; Braithwaite, N. St. J.; Grady, Monica M.

    2012-12-01

    Abstract-We are investigating <span class="hlt">chondrule</span> formation by nebular shock waves, using hot plasma as an analog of the heated gas produced by a shock wave as it passes through the protoplanetary environment. Precursor material (mainly silicates, plus metal, and sulfide) was dropped through the plasma in a basic experimental set-up designed to simulate gas-grain collisions in an unconstrained spatial environment (i.e., no interaction with furnace walls during formation). These experiments were undertaken in air (at atmospheric pressure), to act as a "proof-of-principle"—could <span class="hlt">chondrules</span>, or <span class="hlt">chondrule</span>-analog objects (CAO), be formed by gas-grain interaction initiated by shock fronts? Our results showed that if accelerating material through a fixed plasma field is a valid simulation of a supersonic shock wave traveling through a cloud of gas and dust, then CAO certainly could be formed by this process. Melting of and mixing between starting materials occurred, indicating temperatures of at least 1266 °C (the <span class="hlt">olivine</span>-feldspar eutectic). The production of CAO with mixed mineralogy from monomineralic starting materials also shows that collisions between particles are an important mechanism within the <span class="hlt">chondrule</span> formation process, such that dust aggregates are not necessarily required as <span class="hlt">chondrule</span> precursors. Not surprisingly, there were significant differences between the synthetic CAO and natural <span class="hlt">chondrules</span>, presumably mainly because of the oxidizing conditions of the experiment. Results also show similarity to features of micrometeorites like cosmic spherules, particularly the dendritic pattern of iron oxide crystallites produced on micrometeorites by oxidation during atmospheric entry and the formation of vesicles by evaporation of sulfides.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.473..256I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.473..256I"><span>An experimental study of <span class="hlt">chondrule</span> formation from chondritic precursors via evaporation and condensation in Knudsen cell: Shock heating model of dust aggregates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Imae, Naoya; Isobe, Hiroshi</p> <p>2017-09-01</p> <p><span class="hlt">Chondrules</span>, igneous objects of ∼1 mm in diameter, formed in the earliest solar system via a transient heating event, are divided into two types: main (type I, FeO-poor) and minor (type II, FeO-rich). Using various chondritic materials for different redox conditions and grain sizes, <span class="hlt">chondrule</span> reproduction experiments were carried out at IW-2 to IW-3.8, with cooling rates mainly ∼100°C/h, with peak temperatures mainly at 1450 °C, and mainly at 100 Pa in a Knudsen cell providing near chemical equilibrium between the charge and the surrounding gas at the peak temperatures. Vapor pressures in the capsule were controlled using solid buffers. After and during the significant evaporation of the iron component from the metallic iron-poor starting materials in near equilibrium, crystallization occurred. This resulted in the formation of a product similar to the type I <span class="hlt">chondrules</span>. Dusty <span class="hlt">olivine</span> grains occurred in charges that had precursor type II <span class="hlt">chondrules</span> containing coarse ferroan <span class="hlt">olivine</span>, but such grains are not common in type I <span class="hlt">chondrules</span>. Therefore fine-grained ferroan matrices rather than type II <span class="hlt">chondrules</span> are main precursor for type I <span class="hlt">chondrules</span>. The type I <span class="hlt">chondrules</span> would have evolved via evaporation and condensation in the similar conditions to the present experimental system. Residual gas, which escaped in experiments, could have condensed to form matrices, leading to complementary compositions. Clusters of matrices and primordial <span class="hlt">chondrules</span> could have been recycled to form main-generation <span class="hlt">chondrules</span> originated from the shock heating.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70068727','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70068727"><span>The lack of potassium-isotopic fractionation in Bishunpur <span class="hlt">chondrules</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>Alexander, C.M. O'D.; Grossman, J.N.; Wang, Jingyuan; Zanda, B.; Bourot-Denise, M.; Hewins, R.H.</p> <p>2000-01-01</p> <p>In a search for evidence of evaporation during <span class="hlt">chondrule</span> formation, the mesostases of 11 Bishunpur <span class="hlt">chondrules</span> and melt inclusions in <span class="hlt">olivine</span> phenocrysts in 7 of them have been analyzed for their alkali element abundances and K-isotopic compositions. Except for six points, all areas of the <span class="hlt">chondrules</span> that were analyzed had δ41K compositions that were normal within error (typically ±3%, 2s̀). The six “anomalous” points are probably all artifacts. Experiments have shown that free evaporation of K leads to large 41K enrichments in the evaporation residues, consistent with Rayleigh fractionation. Under Rayleigh conditions, a 3% enrichment in δ41K is produced by ∼12% loss of K. The range of L-chondrite-normalized K/Al ratios (a measure of the K-elemental fractionation) in the areas analyzed vary by almost three orders of magnitude. If all <span class="hlt">chondrules</span> started out with L-chondrite-like K abundances and the K loss occurred via Rayleigh fractionation, the most K-depleted <span class="hlt">chondrules</span> would have had compositions of up to δ41K ≅ 200%. Clearly, K fractionation did not occur by evaporation under Rayleigh conditions. Yet experiments and modeling indicate that K should have been lost during <span class="hlt">chondrule</span> formation under currently accepted formation conditions (peak temperature, cooling rate, etc.). Invoking precursors with variable alkali abundances to produce the range of K/Al fractionation in <span class="hlt">chondrules</span> does not explain the K-isotopic data because any K that was present should still have experienced sufficient loss during melting for there to have been a measurable isotopic fractionation. If K loss and isotopic fractionation was inevitable during <span class="hlt">chondrule</span> formation, the absence of K-isotopic fractionation in Bishunpur <span class="hlt">chondrules</span> requires that they exchanged K with an isotopically normal reservoir during or after formation. There is evidence for alkali exchange between <span class="hlt">chondrules</span> and rim-matrix in all unequilibrated ordinary chondrites. However, melt inclusions can have</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060049098&hterms=Property+Types&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DProperty%2BTypes','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060049098&hterms=Property+Types&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DProperty%2BTypes"><span>Relationships Among Intrinsic Properties of Ordinary Chondrites: Oxidation State, Bulk Chemistry, Oxygen-isotopic Composition, Petrologic Type, and <span class="hlt">Chondrule</span> Size</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rubin, Alan E.</p> <p>2006-01-01</p> <p>The properties of ordinary chondrites (OC) reflect both nebular and asteroidal processes. OC are modeled here as having acquired nebular water, probably contained within phyllosilicates, during agglomeration. This component had high Ai70 and acted like an oxidizing agent during thermal metamorphism. The nebular origin of this component is consistent with negative correlations in H, L, and LL chondrites between oxidation state (represented by <span class="hlt">olivine</span> Fa) and bulk concentration ratios of elements involved in the metal-silicate fractionation (e.g., NdSi, Ir/Si, Ir/Mn, Ir/Cr, Ir/Mg, Ni/Mg, As/Mg, Ga/Mg). LL chondrites acquired the greatest abundance of phyllosilicates with high (delta)O-17 among OC (and thus became the most oxidized group and the one with the heaviest O isotopes); H chondrites acquired the lowest abundance, becoming the most reduced OC group with the lightest O isotopes. <span class="hlt">Chondrule</span> precursors may have grown larger and more ferroan with time in each OC agglomeration zone. Nebular turbulence may have controlled the sizes of <span class="hlt">chondrule</span> precursors. H-chondrite <span class="hlt">chondrules</span> (which are the smallest among OC) formed from the smallest precursors. In each OC region, low-FeO <span class="hlt">chondrules</span> formed before high-FeO <span class="hlt">chondrules</span> during repeated episodes of <span class="hlt">chondrule</span> formation. During thermal metamorphism, phyllosilicates were dehydrated; the liberated water oxidized metallic Fe-Ni. This caused correlated changes with petrologic type including decreases in the modal abundance of metal, increases in <span class="hlt">olivine</span> Fa and low-Ca pyroxene Fs, increases in the <span class="hlt">olivine</span>/pyroxene ratio, and increases in the kamacite Co and Ni contents. As water (with its heavy 0 isotopes) was lost during metamorphism, inverse correlations between bulk (delta)O-18 and bulk (delta)O-17 with petrologic type were produced. The H5 chondrites that were ejected from their parent body approx.7.5 Ma ago during a major impact event probably had been within a few kilometers of each other since they accreted approx.4</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMGP31A0790H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMGP31A0790H"><span>Suitability of <span class="hlt">chondrules</span> for studying the magnetic field of the early solar system: an examination of synthetically produced dusty <span class="hlt">olivine</span></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.; Feinberg, J. M.; Church, N.; Bromiley, G.; Bowles, J.; Jackson, M.; Moskowitz, B. M.; Harrison, R. J.</p> <p>2008-12-01</p> <p>Chondritic meteorites are rare, yet incredibly valuable windows into the geophysical and geochemical environment of the early solar system. Dusty <span class="hlt">olivine</span> grains containing exsolved nanometer-scale iron-nickel alloy inclusions are present in many chondritic meteorites and their remanent magnetization may give insight into the strength of the solar dynamo at the time of <span class="hlt">chondrule</span> formation. Laboratory methods for determining the paleointensity of these rare materials must be optimized prior to conducting experiments on actual meteorite samples. To this end, we have used high temperature recrystallization techniques to produce synthetic dusty <span class="hlt">olivine</span> samples with textures remarkably similar to those observed in chondritic meteorites. The <span class="hlt">olivine</span> grains used in these annealing experiments are from the 13 kya Haleyjabunga picritic basalt flow in Iceland and have compositions of Fo90, which closely resembles the <span class="hlt">olivine</span> composition observed in chondritic meteorites. Samples were annealed at 1350°C either under vacuum in the presence of graphite or under controlled oxygen fugacity using pure CO gas. The laboratory-produced magnetic mineral assemblages in two sets of samples have been characterized using low and high temperature remanence and susceptibility measurements, hysteresis loops, FORC diagrams, and scanning electron microscopy. The room-temperature remanence properties of these materials have been explored using stepwise IRM and ARM acquisition and alternating field demagnetization. These synthesis techniques allow us to produce a wide rage of iron-nickel grain sizes with correspondingly large variations in coercivity (between 0 and 500 mT). High temperature measurements of saturation magnetization show that both samples reach their Curie temperatures at ~760°C, consistent with kamacite, a low-Ni high-Fe metal alloy. Multiple experiments have shown that care must be taken to rigorously control the atmosphere in which the samples are heated and cooled in order to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...855L..17H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...855L..17H"><span>Thermal History of CBb <span class="hlt">Chondrules</span> and Cooling Rate Distributions of Ejecta Plumes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hewins, R. H.; Condie, C.; Morris, M.; Richardson, M. L. A.; Ouellette, N.; Metcalf, M.</p> <p>2018-03-01</p> <p>It has been proposed that some meteorites, CB and CH chondrites, contain material formed as a result of a protoplanetary collision during accretion. Their melt droplets (<span class="hlt">chondrules</span>) and FeNi metal are proposed to have formed by evaporation and condensation in the resulting impact plume. We observe that the skeletal <span class="hlt">olivine</span> (SO) <span class="hlt">chondrules</span> in CBb chondrites have a blebby texture and an enrichment in refractory elements not found in normal <span class="hlt">chondrules</span>. Because the texture requires complete melting, their maximum liquidus temperature of 1928 K represents a minimum temperature for the putative plume. Dynamic crystallization experiments show that the SO texture can be created only by brief reheating episodes during crystallization, giving a partial dissolution of <span class="hlt">olivine</span>. The ejecta plume formed in a smoothed particle hydrodynamics simulation served as the basis for 3D modeling with the adaptive mesh refinement code FLASH4.3. Tracer particles that move with the fluid cells are used to measure the in situ cooling rates. Their cooling rates are ∼10,000 K hr‑1 briefly at peak temperature and, in the densest regions of the plume, ∼100 K hr‑1 for 1400–1600 K. A small fraction of cells is seen to be heating at any one time, with heating spikes explained by the compression of parcels of gas in a heterogeneous patchy plume. These temperature fluctuations are comparable to those required in crystallization experiments. For the first time, we find an agreement between experiments and models that supports the plume model specifically for the formation of CBb <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920036197&hterms=iodine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Diodine','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920036197&hterms=iodine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Diodine"><span>Iodine-xenon, chemical, and petrographic studies of Semarkona <span class="hlt">chondrules</span> - Evidence for the timing of aqueous alteration</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Swindle, T. D.; Grossman, J. N.; Olinger, C. T.; Garrison, D. H.</p> <p>1991-01-01</p> <p>The relationship of the I-Xe system of the Semarkona meteorite to other measured properties is investigated via INAA, petrographic, and noble-gas analyses on 17 <span class="hlt">chondrules</span> from the meteorite. A range of not less than 10 Ma in apparent I-Xe ages is observed. The three latest apparent ages fall in a cluster, suggesting the possibility of a common event. It is argued that the initial I-129/I-127 ratio (R0) is related to <span class="hlt">chondrule</span> type and/or mineralogy, with nonporphyritic and pyroxene-rich <span class="hlt">chondrules</span> showing evidence for lower R0s than porphyritic and <span class="hlt">olivine</span>-rich <span class="hlt">chondrules</span>. <span class="hlt">Chondrules</span> with sulfides on or near the surface have lower R0s than other <span class="hlt">chondrules</span>. The He-129/Xe-132 ratio in the trapped Xe component anticorrelates with R0, consistent with the evolution of a chronometer in a closed system or in multiple systems. It is concluded that the variations in R0 represent variations in ages, and that later events, possibly aqueous alteration, preferentially affected <span class="hlt">chondrules</span> with nonporphyritic textures and/or sulfide-rich exteriors about 10 Ma after the formation of the <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70014986','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014986"><span>Iodine-xenon, chemical, and petrographie studies of Semarkona <span class="hlt">chondrules</span>: Evidence for the timing of aqueous alteration</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Swindle, T.D.; Grossman, J.N.; Olinger, C.T.; Garrison, D.H.</p> <p>1991-01-01</p> <p>We have performed INAA, petrographie, and noble gas analyses on seventeen <span class="hlt">chondrules</span> from the Semarkona meteorite (LL3.0) primarily to study the relationship of the I-Xe system to other measured properties. We observe a range of ???10 Ma in apparent I-Xe ages. The three latest apparent ages fall in a cluster, suggesting the possibility of a common event. The initial 129I/127I ratio (R0) is apparently related to <span class="hlt">chondrule</span> type and/or mineralogy, with nonporphyritic and pyroxene-rich <span class="hlt">chondrules</span> showing evidence for lower R0'S (later apparent I-Xe ages) than porphyritic and <span class="hlt">olivine</span>-rich <span class="hlt">chondrules</span>. In addition, <span class="hlt">chondrules</span> with sulfides on or near the surface have lower R0S than other <span class="hlt">chondrules</span>. The 129Xe/132Xe ratio in the trapped Xe component anticorrelates with R0, consistent with evolution of a chronometer in a closed system or in multiple similar systems. On the basis of these correlations, we conclude that the variations in R0 represent variations in ages, and that later event(s), possibly aqueous alteration, preferentially affected <span class="hlt">chondrules</span> with nonporphyritic textures and/or sulfide-rich exteriors about 10 Ma after the formation of the <span class="hlt">chondrules</span>. ?? 1991.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70025020','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70025020"><span>Zoned <span class="hlt">chondrules</span> in Semarkona: Evidence for high-and low-temperature processing</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Grossman, J.N.; Alexander, C.M. O'D.; Wang, Jingyuan; Brearley, A.J.</p> <p>2002-01-01</p> <p>At least 15% of the low-FeO <span class="hlt">chondrules</span> in Semarkona (LL3.0) have mesostases that are concentrically zoned in Na, with enrichments near the outer margins. We have studied zoned <span class="hlt">chondrules</span> using electron microprobe methods (x-ray mapping plus quantitative analysis), ion micropobe analysis for trace elements and hydrogen isotopes, cathodoluminescence imaging, and transmission electron microscopy in order to determine what these objects can tell us about the environment in which <span class="hlt">chondrules</span> formed and evolved. Mesostases in these <span class="hlt">chondrules</span> are strongly zoned in all moderately volatile elements and H (interpreted as water). Calcium is depleted in areas of volatile enrichment. Titanium and Cr generally decrease toward the <span class="hlt">chondrule</span> surfaces, whereas Al and Si may either increase or decrease, generally in opposite directions to one another; Mn follows Na in some <span class="hlt">chondrules</span> but not in others; Fe and Mg are unzoned. D/H ratios increase in the water-rich areas of zoned <span class="hlt">chondrules</span>. Mesostasis shows cathodoluminescence zoning in most zoned <span class="hlt">chondrules</span>, with the brightest yellow color near the outside. Mesostasis in zoned <span class="hlt">chondrules</span> appears to be glassy, with no evidence for devitrification. Systematic variations in zoning patterns among pyroxene- and <span class="hlt">olivine</span>-rich <span class="hlt">chondrules</span> may indicate that fractionation of low- and high-Ca pyroxene played some role in Ti, Cr, Mn, Si, Al, and some Ca zoning. But direct condensation of elements into hot <span class="hlt">chondrules</span>, secondary melting of late condensates into the outer portions of <span class="hlt">chondrules</span>, and subsolidus diffusion of elements into warm <span class="hlt">chondrules</span> cannot account for the sub-parallel zoning profiles of many elements, the presence of H2O, or elemental abundance patterns. Zoning of moderately volatile elements and Ca may have been produced by hydration of <span class="hlt">chondrule</span> glass without devitrification during aqueous alteration on the parent asteroid. This could have induced structural changes in the glass allowing rapid diffusion and exchange of elements</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.221..358V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.221..358V"><span>Unraveling the role of liquids during <span class="hlt">chondrule</span> formation processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Varela, Maria Eugenia; Zinner, Ernst</p> <p>2018-01-01</p> <p>The process/es involved in <span class="hlt">chondrule</span> formation cover a wide range of mechanisms whose nature is still unknown. Our attention is focused on solar nebula processes mainly in untangling the origin of the initial liquid droplets that turn into <span class="hlt">chondrules</span>. To do this, we start deciphering the processes under which the chondritic constituents of glass-rich, PO and POP <span class="hlt">chondrules</span> from the Unequilibrated Ordinary Chondrite (UOC) Tieschitz L/H3.6 could have been formed. One constituent is the initial refractory liquid. This chilled liquid, presented as primary glass inclusions in <span class="hlt">olivine</span> or as glass mesostasis, has trace element abundances with unfractionated patterns and lacks the chemical signature that is expected from a geochemical (liquid-crystal) fractionation. The unfractionated crystal-liquid distribution coefficients observed in the glass-rich, PO and POP <span class="hlt">chondrules</span> indicate that formation of these objects was not dominated by an igneous process. In addition, the good correlation of elements with different geochemical and cosmochemical properties (e.g., Yb and La-Ce) that spread around the primordial ratio, indicate that a cosmochemical (condensation) instead of a geochemical process may have been involved in the origin of this refractory liquid. We end up discussing a secondary process: the alkali-Ca exchange reaction that could have taken place within a cooling nebula at sub-solidus temperatures. The extent to which these solid/gas exchange reactions took place will determine the final composition of the <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950042203&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D50%26Ntt%3Dlindstrom','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950042203&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D50%26Ntt%3Dlindstrom"><span>Mn-Cr isotopic systematics of individual Chainpur <span class="hlt">chondrules</span>. [Abstract only</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nyquist, L.; Lindstrom, D.; Wiesmann, H.; Martinez, R.; Bansal, B.; Mittlefehldt, D.; Shih, C.-Y.; Wentworth, S.</p> <p>1994-01-01</p> <p>Twenty-eight <span class="hlt">chondrules</span> separated from Chainpur (LL3.4) were surveyed for abundances of Mn, Cr, Na, Fe, Sc, Hf, Ir, and Zn by Instrumental Neutron Activation Analysis (INAA). Six, weighting 0.6-1.5 mg each, were chosen for Scanning Electron Microscopy (SEM)/Energy Dispersive X-ray (EDX) and high-precision Ce-isotopic studies. LL-chondrite-normalized (Mn/Fe)(sub LL) and (Sc/Fe)(sub LL) were found to be useful in categorizing them. Five <span class="hlt">chondrules</span> (CH-16, -17, -18, -23, and -28) were in the range 0.5 less than (Mn/Fe)(sub LL) less than 1. 4 and 0.5 less than (Sc/Fe)(sub LL) less than 1.4. The sixth (CH-25) had (Mn/Fe)(sub LL) and (Sc/Fe)(sub LL) ratios of 0.40 and 8.1, respectively, and was enriched in the refractory lithophile elements Sc and Hf and the refractory siderophile element Ir by 2.7 and 4.4x LL abundances respectively. SEM/EDX of exterior surfaces of the <span class="hlt">chondrules</span> showed they consisted of varying proportions of low- and high-Ca pyroxenes, <span class="hlt">olivine</span>, glass, kamacite/taenite, and Fe-sulfides. Chromium-53/chromium-52 for the six <span class="hlt">chondrules</span> and bulk Chainpur (WR) are presented. Chromium-54/chromium-52 is close to terrestrial and does not correlate with Mn/Cr. We provisionally ignore the possibility of initial Cr isotopic heterogeneities among the <span class="hlt">chondrules</span>. Omitting both the CH-25 and WR data, a linear regression gives initial (Mn-53/Mn-55)(sub I) = 8 +/- 4 x 10(exp -6), corresponding to <span class="hlt">chondrule</span> formation at Delta(t)(sub LEW) = -9 +/- 4 Ma prior to igneous crystallization of the LEW 86010 angrite. If initial (Mn-53/Mn-55)(sub 0) in the solar system were as high as approximately 4.4 x 10(exp -5) when Allende CAI formed, our data suggest Chainpur <span class="hlt">chondrules</span> formed approximately 9 Ma later, in qualitative agreement with 'late' I-Xe formation ages for most Chainpur <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1409578-olivine-melt-relationships-syneruptive-redox-variations-eruption-bar-lauea-volcano-revealed-xanes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1409578-olivine-melt-relationships-syneruptive-redox-variations-eruption-bar-lauea-volcano-revealed-xanes"><span><span class="hlt">Olivine</span>-melt relationships and syneruptive redox variations in the 1959 eruption of K$$\\<span class="hlt">bar</span>{i}$$lauea Volcano as revealed by XANES</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>Helz, R. T.; Cottrell, E.; Brounce, M. N.</p> <p></p> <p>The 1959 summit eruption of Kmore » $$\\<span class="hlt">bar</span>{i}$$lauea Volcano exhibited high lava fountains of gas-rich, primitive magma, containing <span class="hlt">olivine</span> + chromian spinel in highly vesicular brown glass. Microprobe analysis of these samples shows that euhedral rims on <span class="hlt">olivine</span> phenocrysts, in direct contact with glass, vary significantly in forsterite (Fo) content, at constant major-element melt composition, as do unzoned groundmass <span class="hlt">olivine</span> crystals. Ferric/total iron (Fe+ 3/FeT)ratios for matrix and interstitial glasses, plus <span class="hlt">olivine</span>-hosted glass inclusions in eight 1959 scoria samples have been determined by micro X-ray absorption near-edge structure spectroscopy (μ-XANES). These data show that much of the variation in Fo content reflects variation in oxidation state of iron in the melt, which varies with sulfur concentration in the glass and (locally) with proximity to scoria edges in contact with air. Data for 24 <span class="hlt">olivine</span>-melt pairs in the better-equilibrated samples from later in the eruption show KD averaging 0.280 ± 0.03 for the exchange of Fe and Mg between <span class="hlt">olivine</span> and melt, somewhat displaced from the value of 0.30 ± 0.03 given by Roeder and Emslie (1970). This may reflect the low SiO2 content of the 1959 magmas, which is lower than that in most K$$\\<span class="hlt">bar</span>{i}$$lauea tholeiites. More broadly, we show the potential of μ-XANES and electron microprobe to revisit and refine the value of KD in natural systems.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011cpd..book.....H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011cpd..book.....H"><span><span class="hlt">Chondrules</span> and the Protoplanetary Disk</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hewins, R. H.; Jones, Rhian; Scott, Ed</p> <p>2011-03-01</p> <p>Part I. Introduction: 1. <span class="hlt">Chondrules</span> and the protoplanetary disk: An overview R. H. Hewins; Part. II. Chonrules, Ca-Al-Rich Inclusions and Protoplanetary Disks: 2. Astronomical observations of phenomena in protostellar disks L. Hartmann; 3. Overview of models of the solar nebula: potential <span class="hlt">chondrule</span>-forming environments P. Cassen; 4. Large scale processes in the solar nebula A. P. Boss; 5. Turbulence, <span class="hlt">chondrules</span> and planetisimals J. N. Cuzzi, A. R. Dobrovolskis and R. C. Hogan; 6. <span class="hlt">Chondrule</span> formation: energetics and length scales J. T. Wasson; 7. Unresolved issues in the formation of <span class="hlt">chondrules</span> and chondrites J. A. Wood; 8. Thermal processing in the solar nebula: constraints from refractory inclusions A. M. Davis and G. J. MacPherson; 9. Formation times of <span class="hlt">chondrules</span> and Ca-Al-Rich inclusions: constraints from short-lived radionuclides T. D. Swindle, A. M. Davis, C. M. Hohenberg, G. J. MacPherson and L. E. Nyquist; 10. Formation of <span class="hlt">chondrules</span> and chondrites in the protoplanetary nebula E. R. D. Scott, S. G. Love and A. N. Krot; Part III. <span class="hlt">Chondrule</span> precursors and multiple melting: 11. Origin of refractory precursor components of <span class="hlt">chondrules</span> K. Misawa and N. Nakamura; 12. Mass-independent isotopic effects in chondrites: the role of chemical processes M. H. Thiemens; 13. Agglomeratic <span class="hlt">chondrules</span>: implications for the nature of <span class="hlt">chondrule</span> precursors and formation by incomplete melting M. K. Weisberg and M. Prinz; 14. Constraints on <span class="hlt">chondrule</span> precursors from experimental Data H. C. Connolly Jr. and R. H. Hewins; 15. Nature of matrix in unequilibrated chondrites and its possible relationship to <span class="hlt">chondrules</span> A. J. Brearly; 16. Constraints on chondrite agglomeration from fine-grained <span class="hlt">chondrule</span> Rims K. Metzler and A. Bischoff; 17. Relict grains in <span class="hlt">chondrules</span>: evidence for <span class="hlt">chondrule</span> recycling R. H. Jones; 18. Multiple heating of <span class="hlt">chondrules</span> A. E. Rubin and A. N. Krot; 19. Microchondrule-bearing <span class="hlt">chondrule</span> rims: constraints on <span class="hlt">chondrule</span> formation A. N. Krot and A. E. Rubin; Part IV</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1411211L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1411211L"><span>Rock magnetic properties of dusty <span class="hlt">olivine</span>: a potential carrier of pre-accretionary remanence in unequilibrated ordinary chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lappe, S. C. L. L.; Harrison, R. J.; Feinberg, J. M.</p> <p>2012-04-01</p> <p>The mechanism of <span class="hlt">chondrule</span> formation is an important outstanding question in cosmochemistry. Magnetic signals recorded by Fe-Ni nanoparticles in <span class="hlt">chondrules</span> could carry clues to their origin. Recently, research in this area has focused on 'dusty <span class="hlt">olivine</span>' grains within ordinary chondrites as potential carriers of pre-accretionary remanence. Dusty <span class="hlt">olivine</span> is characterised by the presence of sub-micron Fe-Ni inclusions within the <span class="hlt">olivine</span> host. These metal particles form via subsolidus reduction of the <span class="hlt">olivine</span> during <span class="hlt">chondrule</span> formation and are thought to be protected from subsequent chemical and thermal alteration by the host <span class="hlt">olivine</span>. Three sets of synthetic dusty <span class="hlt">olivines</span> have been produced, using natural <span class="hlt">olivine</span> (average Ni-content of 0.3 wt%), synthetic Ni-containing <span class="hlt">olivine</span> (0.1wt% Ni) and synthetic Ni-free <span class="hlt">olivine</span> as starting materials. The starting materials were ground to powders, packed into a 2-3 mm3 graphite crucible, heated up to 1350 °C under a pure CO gas flow and kept at this temperature for 10 minutes. After this the samples were held in a fixed orientation and quenched into water in a range of known magnetic fields, ranging from 0.2 mT to 1.5 mT. We present here for the first time an analysis of a new FORC-based method of paleointensity determination applied to metallic Fe-bearing samples [1, 2]. The method uses a first-order reversal curve (FORC) diagram to generate a Preisach distribution of coercivities and interaction fields within the sample and then physically models the acquisition of TRM as a function of magnetic field, temperature and time using thermal relaxation theory. The comparison of observed and calculated NRM demagnetisation spectra is adversely effected by a large population of particles in the single-vortex state. Comparison of observed and calculated REM' curves, however, yields much closer agreement in the high-coercivity SD-dominated range. Calculated values of the average REM' ratio show excellent agreement with the experimental</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.208..220M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.208..220M"><span>Nepheline and sodalite in <span class="hlt">chondrules</span> of the Ningqiang carbonaceous chondrite: Implications for a genetic relationship with those in the matrix</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matsumoto, Megumi; Tomeoka, Kazushige; Seto, Yusuke</p> <p>2017-07-01</p> <p>Ningqiang is an ungrouped carbonaceous chondrite that has a chemical and mineralogical affinity to CV3 chondrites. The Ningqiang matrix has distinctly higher abundances of Na, K, and Al than CV3 matrices. A recent study by Matsumoto et al. (2014) revealed that the major proportions of these elements can be attributed to the presence of nepheline and sodalite. Scanning electron microscopy revealed that all of the Ningqiang <span class="hlt">chondrules</span> studied show abundant evidence of extensive Na-Fe metasomatism. Only a small proportion of the <span class="hlt">chondrules</span> contain primary mesostases in their cores, but the mesostases in their mantles were replaced by fine grains of nepheline, sodalite, Fe-rich <span class="hlt">olivine</span>, and hedenbergite. The mesostases in the majority of the <span class="hlt">chondrules</span> were completely replaced by fine grains of the same secondary minerals. Most opaque nodules were also largely replaced by various fine-grained secondary minerals. Nepheline/sodalite form veins penetrating the primary mesostases, providing evidence that aqueous fluids were involved in the alteration reactions. The nepheline/sodalite in the mesostases contain various amounts of inclusions of Fe-rich <span class="hlt">olivine</span>, diopside, hedenbergite, Fe sulfides, and magnetite. The mineralogical features of the nepheline/sodalite in the mesostases are almost identical to those in the meteorite matrix. These results suggest that a significant fraction of the nepheline/sodalite grains in the Ningqiang matrix originated from the nepheline/sodalite produced in <span class="hlt">chondrules</span> and refractory inclusions and that they were disaggregated and mixed into the matrix. These processes can be explained consistently by the model of the dynamic formation of chondrite lithology in a parent body proposed by Tomeoka and Ohnishi (2015). We suggest that after a Ningqiang precursor with a CV3-like lithology was metasomatized, it was fragmented, causing the disaggregation of the fine-grained host matrix and the fine-grained altered mesostases, including nepheline</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140012798','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140012798"><span>Strain Measurements of <span class="hlt">Chondrules</span> and Refraction Inclusion in Allende</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tait, Alastair W.; Fisher, Kent R.; Simon, Justin I.</p> <p>2013-01-01</p> <p>This study uses traditional strain measurement techniques, combined with X-ray computerized tomography (CT), to evaluate petrographic evidence in the Allende CV3 chondrite for preferred orientation and to measure strain in three dimensions. The existence of petrofabrics and lineations was first observed in carbonaceous meteorites in the 1960's. Yet, fifty years later only a few studies have reported that meteorites record such features. Impacts are often cited as the mechanism for this feature, although plastic deformation from overburden and nebular imbrication have also been proposed. Previous work conducted on the Leoville CV3 and the Parnallee LL3 chondrites, exhibited a minimum uniaxial shortening of 33% and 21%, respectively. Petrofabrics in Allende CV3 have been looked at before; previous workers using Electron Back Scatter Diffraction (EBSD) found a major-axis alignment of <span class="hlt">olivine</span> inside dark inclusions and an "augen"-like preferred orientation of <span class="hlt">olivine</span> grains around more competent <span class="hlt">chondrules</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850007297&hterms=physical+dependence&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dphysical%2Bdependence','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850007297&hterms=physical+dependence&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dphysical%2Bdependence"><span>Size dependence of <span class="hlt">chondrule</span> textural types</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Goswami, J. N.</p> <p>1984-01-01</p> <p>Chrondrule textural types were studied for size sorted <span class="hlt">chondrules</span> from the ordinary chondrites Dhajala, Eston and Chainpur and the CM chondrite Murchison. Aliquot samples from size sorted Dhajala <span class="hlt">chondrules</span> were studied for their oxygen isotopic composition and <span class="hlt">chondrules</span> from Weston were studied for their precompaction irradiation records by nuclear track technique. Correlations between <span class="hlt">chondrule</span> textural types and oxygen isotope or track data were identified. A distinct dependence of <span class="hlt">chondrule</span> textural type on <span class="hlt">chondrule</span> size was evident in the data for both Dhajala and Weston <span class="hlt">chondrules</span>. No significant deviation was noticed in the abundance pattern of nonporphyritic <span class="hlt">chondrules</span> within individual size fractions in the 200 to 800 micron size interval. Overabundance is found of nonporphyritic <span class="hlt">chondrules</span> in the 100 to 200 micron size fraction of Murchison <span class="hlt">chondrules</span>, the trend is not as distinct for Chainpur <span class="hlt">chondrules</span>. Two hundred microns is suggested as the cutoff size below which radiative cooling is extremely efficient during the <span class="hlt">chondrule</span> forming process. It is suggested that this offers a possibility for use of physical and chemical characteristics of small <span class="hlt">chondrules</span> to constrain the temperature history during the <span class="hlt">chondrule</span> formation process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.201..275S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.201..275S"><span>Distribution of 26Al in the CR chondrite <span class="hlt">chondrule</span>-forming region of the protoplanetary disk</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schrader, Devin L.; Nagashima, Kazuhide; Krot, Alexander N.; Ogliore, Ryan C.; Yin, Qing-Zhu; Amelin, Yuri; Stirling, Claudine H.; Kaltenbach, Angela</p> <p>2017-03-01</p> <p>We report on the mineralogy, petrography, and in situ measured oxygen- and magnesium-isotope compositions of eight porphyritic <span class="hlt">chondrules</span> (seven FeO-poor and one FeO-rich) from the Renazzo-like carbonaceous (CR) chondrites Graves Nunataks 95229, Grosvenor Mountains 03116, Pecora Escarpment 91082, and Queen Alexandra Range 99177, which experienced minor aqueous alteration and very mild thermal metamorphism. We find no evidence that these processes modified the oxygen- or Al-Mg isotope systematics of <span class="hlt">chondrules</span> in these meteorites. <span class="hlt">Olivine</span>, low-Ca pyroxene, and plagioclase within an individual <span class="hlt">chondrule</span> have similar O-isotope compositions, suggesting crystallization from isotopically uniform melts. The only exceptions are relict grains in two of the <span class="hlt">chondrules</span>; these grains are 16O-enriched relative to phenocrysts of the host <span class="hlt">chondrules</span>. Only the FeO-rich <span class="hlt">chondrule</span> shows a resolvable excesses of 26Mg, corresponding to an inferred initial 26Al/27Al ratio [(26Al/27Al)0] of (2.5 ± 1.6) × 10-6 (±2SE). Combining these results with the previously reported Al-Mg isotope systematics of CR <span class="hlt">chondrules</span> (Nagashima et al., 2014, Geochem. J. 48, 561), 7 of 22 <span class="hlt">chondrules</span> (32%) measured show resolvable excesses of 26Mg; the presence of excess 26Mg does not correlate with the FeO content of <span class="hlt">chondrule</span> silicates. In contrast, virtually all <span class="hlt">chondrules</span> in weakly metamorphosed (petrologic type 3.0-3.1) unequilibrated ordinary chondrites (UOCs), Ornans-like carbonaceous (CO) chondrites, and the ungrouped carbonaceous chondrite Acfer 094 show resolvable excesses of 26Mg. The inferred (26Al/27Al)0 in CR <span class="hlt">chondrules</span> with resolvable excesses of 26Mg range from (1.0 ± 0.4) × 10-6 to (6.3 ± 0.9) × 10-6, which is typically lower than (26Al/27Al)0 in the majority of <span class="hlt">chondrules</span> from UOCs, COs, and Acfer 094. Based on the inferred (26Al/27Al)0, three populations of CR <span class="hlt">chondrules</span> are recognized; the population characterized by low (26Al/27Al)0 (<3 × 10-6) is dominant. There are no noticeable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890039063&hterms=group+differences&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dgroup%2Bdifferences','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890039063&hterms=group+differences&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dgroup%2Bdifferences"><span><span class="hlt">Chondrules</span> in the Sharps H3 chondrite - Evidence for intergroup compositional differences among ordinary chondrite <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rubin, Alan E.; Pernicka, Ernst</p> <p>1989-01-01</p> <p>Bulk compositions of 19 <span class="hlt">chondrules</span> and one matrix-rich sample from H3.4 Sharps were determined by instrumental neutron activation analysis. Samples were characterized petrographically, and mineral compositions were determined by electron microprobe analysis. There is constancy among ordinary chondrite (OC) groups in the compositional interrelationships of different <span class="hlt">chondrule</span> types; e.g., in H3 as well as L3 and LL3 chondrites, porphyritic <span class="hlt">chondrules</span> are more refractory than nonporphyritic <span class="hlt">chondrules</span>. Precursor components of H3 <span class="hlt">chondrules</span> are closely related to those of LL3 <span class="hlt">chondrules</span>. The mean Ir/Ni, Ir/Co, and Ir/Au ratios of H3 <span class="hlt">chondrules</span> differ from the corresponding ratios of LL3 <span class="hlt">chondrules</span> at the 99, 90, and 79 percent confidence levels, respectively. The ratios in H3 <span class="hlt">chondrules</span> exceed those in LL3 <span class="hlt">chondrules</span> by amounts similar to those by which H whole-rocks exceed LL whole-rocks. These data suggest that there are primary systematic differences in bulk composition between H and LL <span class="hlt">chondrules</span>. These differences support the inference that <span class="hlt">chondrule</span> formation occurred after major nebular fractionation events had established the observed bulk compositional differences among OC groups.</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_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_3 --> <div id="page_4" 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_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</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="61"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060049099&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D3.0','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060049099&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D3.0"><span>Oxygen-isotopic Compositions of Low-FeO relicts in High-FeO Host <span class="hlt">Chondrules</span> in Acfer 094, a Type 3.0 Carbonaceous Chondrite Closely Related to CM</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rubin, Alan E.; Kunihiro, Tak; Wasson, John T.</p> <p>2006-01-01</p> <p>With one exception, the low-FeO relict <span class="hlt">olivine</span> grains within high-FeO porphyritic <span class="hlt">chondrules</span> in the type 3.0 Acfer 094 carbonaceous chondrite have DELTA O-17 ( = delta O-17 - 0.52 X delta O-18) values that are substantially more negative than those of the high-FeO <span class="hlt">olivine</span> host materials. These results are similar to observations made earlier on <span class="hlt">chondrules</span> in C03.0 chondrites and are consistent with two independent models: (1) Nebular solids evolved from low-FeO, low-DELTA O-17 compositions towards high-FeO, more positive DELTA O-17 compositions; and (2) the range of compositions resulted from the mixing of two independently formed components. The two models predict different trajectories on a DELTA O-17 vs. log Fe/Mg (<span class="hlt">olivine</span>) diagram, but our sample set has too few values at intermediate Fe/Mg ratios to yield a definitive answer. Published data showing that Acfer 094 has higher volatile contents than CO chondrites suggest a closer link to CM chondrites. This is consistent with the high modal matrix abundance in Acfer 094 (49 vol.%). Acfer 094 may be an unaltered CM chondrite or an exceptionally matrix-rich CO chondrite. <span class="hlt">Chondrules</span> in Acfer 094 and in CO and CM carbonaceous chondrites appear to sample the same population. Textural differences between Acfer 094 and CM chondrites are largely attributable to the high degree of hydrothermal alteration that the CM chondrites experienced in an asteroidal setting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040059902&hterms=nettle+root&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnettle%2Broot','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040059902&hterms=nettle+root&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnettle%2Broot"><span>An Evaluation of Quantitative Methods of Determining the Degree of Melting Experienced by a <span class="hlt">Chondrule</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nettles, J. W.; Lofgren, G. E.; Carlson, W. D.; McSween, H. Y., Jr.</p> <p>2004-01-01</p> <p>Many workers have considered the degree to which partial melting occurred in <span class="hlt">chondrules</span> they have studied, and this has led to attempts to find reliable methods of determining the degree of melting. At least two quantitative methods have been used in the literature: a convolution index (CVI), which is a ratio of the perimeter of the <span class="hlt">chondrule</span> as seen in thin section divided by the perimeter of a circle with the same area as the <span class="hlt">chondrule</span>, and nominal grain size (NGS), which is the inverse square root of the number density of <span class="hlt">olivines</span> and pyroxenes in a <span class="hlt">chondrule</span> (again, as seen in thin section). We have evaluated both nominal grain size and convolution index as melting indicators. Nominal grain size was measured on the results of a set of dynamic crystallization experiments previously described, where aliquots of LEW97008(L3.4) were heated to peak temperatures of 1250, 1350, 1370, and 1450 C, representing varying degrees of partial melting of the starting material. Nominal grain size numbers should correlate with peak temperature (and therefore degree of partial melting) if it is a good melting indicator. The convolution index is not directly testable with these experiments because the experiments do not actually create <span class="hlt">chondrules</span> (and therefore they have no outline on which to measure a CVI). Thus we had no means to directly test how well the CVI predicted different degrees of melting. Therefore, we discuss the use of the CVI measurement and support the discussion with X-ray Computed Tomography (CT) data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMGP51A1306L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMGP51A1306L"><span>Rock magnetic properties of dusty <span class="hlt">olivine</span>: comparison and calibration of non-heating paleointensity methods</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lappe, S. L.; Harrison, R. J.; Feinberg, J. M.</p> <p>2012-12-01</p> <p>The mechanism of <span class="hlt">chondrule</span> formation is an important outstanding question in cosmochemistry. Magnetic signals recorded by Fe-Ni nanoparticles in <span class="hlt">chondrules</span> could carry clues to their origin. Recently, research in this area has focused on 'dusty <span class="hlt">olivine</span>' in ordinary chondrites as potential carriers of pre-accretionary remanence. Dusty <span class="hlt">olivine</span> is characterised by the presence of sub-micron Fe-Ni inclusions within the <span class="hlt">olivine</span> host. These metal particles form via subsolidus reduction of the <span class="hlt">olivine</span> during <span class="hlt">chondrule</span> formation and are thought to be protected from subsequent chemical and thermal alteration by the host <span class="hlt">olivine</span>. Three sets of synthetic dusty <span class="hlt">olivines</span> have been produced, using natural <span class="hlt">olivine</span> (average Ni-content of 0.3 wt%), synthetic Ni-containing <span class="hlt">olivine</span> (0.1wt% Ni) and synthetic Ni-free <span class="hlt">olivine</span> as starting materials. The starting materials were ground to powders, packed into a 8-27 mm3 graphite crucible, heated up to 1350°C under a pure CO gas flow and kept at this temperature for 10 minutes. After this the samples were held in fixed orientation and quenched into water in a range of known magnetic fields from 0.2 mT to 1.5 mT. We present a comparison of all non-heating methods commonly used for paleointensity determination of extraterrestrial material. All samples showed uni-directional, single-component demagnetization behaviour. Saturation REM ratio (NRM/SIRM) and REMc ratio show non-linear behaviour as function of applied field and a saturation value < 1. Using the REM' method the samples showed approximately constant REM' between 100 and 150 mT AF-field. Plotting the average values for this field range again shows non-linear behaviour and a saturation value < 1. Another approach we examined to obtain calibration curves for paleointensity determination is based on ARM measurents. We also present an analysis of a new FORC-based method of paleointensity determination applied to metallic Fe-bearing samples [1, 2]. The method uses a first-order reversal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRE..121.1885C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRE..121.1885C"><span><span class="hlt">Chondrules</span>: The canonical and noncanonical views</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Connolly, Harold C.; Jones, Rhian H.</p> <p>2016-10-01</p> <p>Millimeter-scale rock particles called <span class="hlt">chondrules</span> are the principal components of the most common meteorites, chondrites. Hence, <span class="hlt">chondrules</span> were arguably the most abundant components of the early solar system at the time of planetesimal accretion. Despite their fundamental importance, the existence of <span class="hlt">chondrules</span> would not be predicted from current observations and models of young planetary systems. There are many different models for <span class="hlt">chondrule</span> formation, but no single model satisfies the many constraints determined from their mineralogical and chemical properties and from <span class="hlt">chondrule</span> analog experiments. Significant recent progress has shown that several models can satisfy first-order constraints and successfully reproduce <span class="hlt">chondrule</span> thermal histories. However, second- and third-order constraints such as <span class="hlt">chondrule</span> size ranges, open system behavior, oxidation states, reheating, and chemical diversity have not generally been addressed. <span class="hlt">Chondrule</span> formation models include those based on processes that are known to occur in protoplanetary disk environments, including interactions with the early active Sun, impacts and collisions between planetary bodies, and radiative heating. Other models for <span class="hlt">chondrule</span> heating mechanisms are based on hypothetical processes that are possible but have not been observed, like shock waves, planetesimal bow shocks, and lightning. We examine the evidence for the canonical view of <span class="hlt">chondrule</span> formation, in which <span class="hlt">chondrules</span> were free-floating particles in the protoplanetary disk, and the noncanonical view, in which <span class="hlt">chondrules</span> were the by-products of planetesimal formation. The fundamental difference between these approaches has a bearing on the importance of <span class="hlt">chondrules</span> during planet formation and the relevance of <span class="hlt">chondrules</span> to interpreting the evolution of protoplanetary disks and planetary systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P23A2163U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P23A2163U"><span>Temperature and Time Constraints on Dissolution, Fe-Mg Exchange and Zoning between Relict Forsterite and <span class="hlt">Chondrule</span> Melt - Implications for Thermal History of <span class="hlt">Chondrules</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ustunisik, G. K.; Ebel, D. S. S.; Walker, D.</p> <p>2016-12-01</p> <p>The chemical and textural characteristics of different generations of relict <span class="hlt">olivine</span> grains in <span class="hlt">chondrules</span> record the fact that <span class="hlt">chondrules</span> were re-melted. Mineral dissolution, Fe-Mg exchange, and zoning within the relict crystals constrain the T-t aspects of this re-melting process. Here, we performed isothermal and dynamic cooling experiments at LDEO of Columbia University. For each run, a cubic crystal of known dimensions of Mogok forsterite (Fo99) was placed in synthetic Type IIA <span class="hlt">chondrule</span> mesostasis with 4.92 wt% FeO (TLiq 1315ºC). Pressed pellets of this mixture were hung on Pt-wire loops and inserted in vertical Deltech furnace where CO-CO2 gas mixtures kept fO2 IW-1. For isothermal experiments, each charge was heated to 1428ºC, 1350ºC, 1250ºC, and 1150ºC and was held there from 20 mins to several days (>3 days) before drop-quenching into cold water. The dynamic crystallization experiments were held at 1428ºC for 20 mins, cooled at rates of 75ºC, 722ºC, and 1444ºC/hr to 1000ºC and then water quenched. X-ray-CT and EMPA at AMNH were used to image the partially resorbed/zoned <span class="hlt">olivines</span> in 3-D before and after each run to observe textural evolution of the crystal shapes and volumes and to determine chemical changes. The isothermal experiments at 1150 and 1250ºC for 20 mins, produced no bulk FeO diffusion into the Mogok forsterite. Very minor Fe-Mg exchange at the crystal rims gives slight MgO zoning within the nearby melt. With increasing duration (1 hr and 22 hrs), at 1250ºC, embayments of melt form into the rims of the crystal (amplified at 22 hrs) with significant Fe-Mg exchange. FeO content of Mogok increased with major MgO zonation within nearby melt. At 1150ºC, the same increase in FeO in Mogok and zonation in nearby glass could only be achieved in >3 days experiment. At high Ts (1428ºC) in 20 min run, 75 volume % of Mogok forsterite has been dissolved into the melt. Resorption erodes the Fe-Mg exchange at the rims of the crystal. At longer</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940030965','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940030965"><span><span class="hlt">Chondrule</span> magnetic properties</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wasilewski, P. J.; Obryan, M. V.</p> <p>1994-01-01</p> <p>The topics discussed include the following: <span class="hlt">chondrule</span> magnetic properties; <span class="hlt">chondrules</span> from the same meteorite; and REM values (the ratio for remanence initially measured to saturation remanence in 1 Tesla field). The preliminary field estimates for <span class="hlt">chondrules</span> magnetizing environments range from minimal to a least several mT. These estimates are based on REM values and the characteristics of the remanence initially measured (natural remanence) thermal demagnetization compared to the saturation remanence in 1 Tesla field demagnetization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992Metic..27R.299T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992Metic..27R.299T"><span>A New CV3 Chondrite Find</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Treiman, A. H.; Dehart, J. M.</p> <p>1992-07-01</p> <p>A new meteorite find from West Texas, U.S.A., is a CV3 carbonaceous chondrite. The provisional name of Red Bluff has been proposed to the Nomenclature Committee by R. Farrell. Red Bluff consists of <span class="hlt">chondrules</span> (56.4%), CAIs (8.3%), amoboid <span class="hlt">olivine</span> aggregates (0.6%), mineral fragments (0.8%), and Ca-Al <span class="hlt">chondrules</span> (0.4%) in a fine-grained, clay-rich matrix (33.1%). <span class="hlt">Chondrules</span> in Red Bluff are spherical to irregular in shape, and from 0.25-3.5 mm diameter in thin section; the average diameter is 0.95 mm, with standard deviation of 0.6 mm (69 <span class="hlt">chondrules</span>). Three of the <span class="hlt">chondrules</span> are distinctly larger than the rest; without these three, the average diameter is 0.86 mm (s.d. 0.4 mm). The <span class="hlt">chondrules</span> are almost all of type I (Fe-poor), as shown by cathodoluminescence and chemical analyses; most are also rich in opaques. Compositions of <span class="hlt">chondrule</span> <span class="hlt">olivines</span> average Fa1.9+-1.2 (s.d.); compositions of <span class="hlt">chondrule</span> pyroxenes average Fs3.4+-3.3 (s.d.). <span class="hlt">Chondrule</span> varieties include porphyritic <span class="hlt">olivine</span>, microporphyritic <span class="hlt">olivine</span>, granular <span class="hlt">olivine</span>, macroporphyritic <span class="hlt">olivine</span>, <span class="hlt">barred</span> <span class="hlt">olivine</span>, and rare extracentroradial pyroxene (0.25 mm diam.) [1,2]. Two calcium-aluminum <span class="hlt">chondrules</span> were observed. The largest, 1.5 mm diam., contains spinel, plagioclase, and fassaite, and includes a circular spinel palisade [3]. The other Ca-Al <span class="hlt">chondrule</span> is within a coarse-grained CAI, and could also be a well-developed spinel palisade [3]. Fine- and coarse-grained CAIs are present but have been studied little; most appear to be type B (melilite+pyroxene+plagioclase). Red Bluff's matrix is composed of fine-grained clay, with minor <span class="hlt">olivine</span>, "limonite," troilite, and Fe metal. Alignment of grains and oxide-rich streaks in the matrix mark a planar fabric that wraps around <span class="hlt">chondrules</span> and inclusions. <span class="hlt">Chondrules</span> are commonly surrounded by shells of dark red alteration, darker than the bulk of matrix material. Red Bluff is weathered. It is stained red by oxidized iron minerals, which are most common as veinlets</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830031623&hterms=history+microscopes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhistory%2Bmicroscopes','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830031623&hterms=history+microscopes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhistory%2Bmicroscopes"><span>Microchondrule-bearing clast in the Piancaldoli LL3 meteorite - A new kind of type 3 chondrite and its relevance to the history of <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rubin, A. E.; Scott, E. R. D.; Keil, K.</p> <p>1982-01-01</p> <p>Electron microprobe, scanning electron microscope, and petrographic analyses of the microchondritic clast of the Piancaldoli LL3 chondrite are reported and compared with other type three chondrites. The clast, like other type three chondrites, has a fine-grained Fe-rich opaque silicate matrix, sharply defined <span class="hlt">chondrules</span>, abundant low-Ca clinopyroxene and minor troilite and Si and Cr-bearing metallic Fe, Ni. However, the very high model matrix abundance, unique characteristics of the <span class="hlt">chondrules</span>, and absence of microscopically observable <span class="hlt">olivine</span> indicate that the clast is a new type of type three chondrite. It is concluded that the microchondrules were formed by the same process that formed normal-sized <span class="hlt">chondrules</span> in type three chondrites: melting of preexisting dustballs. It is suggested that dust grains were mineralogically sorted in the nebula before aggregating into dustballs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850044394&hterms=divided+attention&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Ddivided%2Battention','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850044394&hterms=divided+attention&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Ddivided%2Battention"><span>Cosmic setting for <span class="hlt">chondrule</span> formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Taylor, G. J.; Scott, E. R. D.; Keil, K.</p> <p>1983-01-01</p> <p><span class="hlt">Chondrules</span> are igneous-textured, millimeter-sized, spherical to irregularly-shaped silicate objects which constitute the major component of most chondrites. There is agreement that <span class="hlt">chondrules</span> were once molten. Models for <span class="hlt">chondrule</span> origin can be divided into two categories. One involves a 'planetary' setting, which envisages <span class="hlt">chondrules</span> forming on the surfaces of parent bodies. Melting mechanisms include impact and volcanism. The other category is concerned with a cosmic setting in the solar nebula, prior to nebula formation. Aspects regarding the impact on planetary surfaces are considered, taking into account <span class="hlt">chondrule</span> abundances, the abundancy of agglutinates on the moon, comminution, hypervelocity impact pits, questions of age, and <span class="hlt">chondrule</span> compositions. Attention is also given to collisions during accretion, collisions between molten planetesimals, volcanism, and virtues of a nebular setting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010059864','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010059864"><span>Stardust to Planetesimals: A <span class="hlt">Chondrule</span> Connection?</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paque, Julie; Bunch, Ted</p> <p>1997-01-01</p> <p>The unique nature of <span class="hlt">chondrules</span> has been known for nearly two centuries. Modern techniques of analysis have shown that these millimeter sized silicate objects are among the oldest objects in our solar system. Researchers have devised textural and chemical classification systems for <span class="hlt">chondrules</span> in an effort to determine their origins. It is agreed that most <span class="hlt">chondrules</span> were molten at some point in their history, and experimental analogs suggest that the majority of <span class="hlt">chondrules</span> formed from temperatures below 1600 C at cooling rates in the range of hundreds of degrees per hour. Although interstellar grains are present in chondrite matrices, their contribution as precursors to <span class="hlt">chondrule</span> formation is unknown. Models for <span class="hlt">chondrule</span> formation focus on the pre-planetary solar nebula conditions, although planetary impact models have had proponents.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050165548','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050165548"><span><span class="hlt">Chondrule</span> Crystallization Experiments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hweins, R. H.; Connolly, H. C., Jr.; Lofgren, G. E.; Libourel, G.</p> <p>2004-01-01</p> <p>Given the great diversity of <span class="hlt">chondrules</span>, laboratory experiments are invaluable in yielding information on <span class="hlt">chondrule</span> formation process(es) and for deciphering their initial conditions of formation together with their thermal history. In addition, they provide some critical parameters for astrophysical models of the solar system and of nebular disk evolution in particular (partial pressures, temperature, time, opacity, etc). Most of the experiments simulating <span class="hlt">chondrules</span> have assumed formation from an aggregate of solid grains, with total pressure of no importance and with virtually no gain or loss of elements from or to the ambient environment. They used pressed pellets attached to wires and suffered from some losses of alkalis and Fe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19720047640&hterms=CO2+uses&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DCO2%2Buses','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19720047640&hterms=CO2+uses&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DCO2%2Buses"><span>Use of a CO2 laser to prepare <span class="hlt">chondrule</span>-like spherules from supercooled molten oxide and silicate droplets.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nelson, L. S.; Blander, M.; Keil, K.; Skaggs, S. R.</p> <p>1972-01-01</p> <p><span class="hlt">Chondrule</span>-like spherules were formed from individual freely falling subcooled droplets of alumina, enstatite, forsterite, enstatite-albite and forsterite-albite mixtures that had been melted with a focused continuous CO2 laser beam. Their textures (rimmed, excentro-radial, <span class="hlt">barred</span>, glassy) are strikingly similar to those of many meteoritic <span class="hlt">chondrules</span>. It is suggested that the phenomena associated with rapid crystallization from the supercooled melt are responsible for the various textures observed in the artificial spherules as well as in similar meteoritic <span class="hlt">chondrules</span>. It is suggested that the textures observed would also result from rapid crystallization of relatively slowly cooling molten droplets that may have been produced in larger scale events, including condensation from a nebula of solar composition and solidification in an ambient medium of high temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.490...31H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.490...31H"><span>Fe isotope composition of bulk <span class="hlt">chondrules</span> from Murchison (CM2): Constraints for parent body alteration, nebula processes and <span class="hlt">chondrule</span>-matrix complementarity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hezel, Dominik C.; Wilden, Johanna S.; Becker, Daniel; Steinbach, Sonja; Wombacher, Frank; Harak, Markus</p> <p>2018-05-01</p> <p><span class="hlt">Chondrules</span> are a major constituent of primitive meteorites. The formation of <span class="hlt">chondrules</span> is one of the most elusive problems in cosmochemistry. We use Fe isotope compositions of <span class="hlt">chondrules</span> and bulk chondrites to constrain the conditions of <span class="hlt">chondrule</span> formation. Iron isotope compositions of bulk <span class="hlt">chondrules</span> are so far only known from few studies on CV and some ordinary chondrites. We studied 37 <span class="hlt">chondrules</span> from the CM chondrite Murchison. This is particularly challenging, as CM chondrites contain the smallest <span class="hlt">chondrules</span> of all chondrite groups, except for CH chondrites. Bulk <span class="hlt">chondrules</span> have δ56Fe between -0.62 and +0.24‰ relative to the IRMM-014 standard. Bulk Murchison has as all chondrites a δ56Fe of 0.00‰ within error. The δ56Fe distribution of the Murchison <span class="hlt">chondrule</span> population is continuous and close to normal. The width of the δ56Fe distribution is narrower than that of the Allende <span class="hlt">chondrule</span> population. Opaque modal abundances in Murchison <span class="hlt">chondrules</span> is in about 67% of the <span class="hlt">chondrules</span> close to 0 vol.%, and in 33% typically up to 6.5 vol.%. <span class="hlt">Chondrule</span> Al/Mg and Fe/Mg ratios are sub-chondritic, while bulk Murchison has chondritic ratios. We suggest that the variable bulk <span class="hlt">chondrule</span> Fe isotope compositions were established during evaporation and recondensation prior to accretion in the Murchison parent body. This range in isotope composition was likely reduced during aqueous alteration on the parent body. Murchison has a chondritic Fe isotope composition and a number of chondritic element ratios. <span class="hlt">Chondrules</span>, however, have variable Fe isotope compositions and <span class="hlt">chondrules</span> and matrix have complementary Al/Mg and Fe/Mg ratios. In combination, this supports the idea that <span class="hlt">chondrules</span> and matrix formed from a single reservoir and were then accreted in the parent body. The formation in a single region also explains the compositional distribution of the <span class="hlt">chondrule</span> population in Murchison.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...834..125W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...834..125W"><span>Planetesimal Collisions as a <span class="hlt">Chondrule</span> Forming Event</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wakita, Shigeru; Matsumoto, Yuji; Oshino, Shoichi; Hasegawa, Yasuhiro</p> <p>2017-01-01</p> <p>Chondritic meteorites contain unique spherical materials named <span class="hlt">chondrules</span>: sub-mm sized silicate grains once melted in a high temperature condition in the solar nebula. We numerically explore one of the <span class="hlt">chondrule</span> forming processes—planetesimal collisions. Previous studies have found that impact jetting via protoplanet-planetesimal collisions can make <span class="hlt">chondrules</span> with 1% of the impactors’ mass, when the impact velocity exceeds 2.5 km s-1. Based on the mineralogical data of <span class="hlt">chondrules</span>, undifferentiated planetesimals would be more suitable for <span class="hlt">chondrule</span>-forming collisions than potentially differentiated protoplanets. We examine planetesimal-planetesimal collisions using a shock physics code and find two things: one is that planetesimal-planetesimal collisions produce nearly the same amount of <span class="hlt">chondrules</span> as protoplanet-planetesimal collisions (˜1%). The other is that the amount of produced <span class="hlt">chondrules</span> becomes larger as the impact velocity increases when two planetesimals collide with each other. We also find that progenitors of <span class="hlt">chondrules</span> can originate from deeper regions of large targets (planetesimals or protoplanets) than small impactors (planetesimals). The composition of targets is therefore important, to fully account for the mineralogical data of currently sampled <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005psrd.reptE..98T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005psrd.reptE..98T"><span>Little <span class="hlt">Chondrules</span> and Giant Impacts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taylor, G. J.</p> <p>2005-10-01</p> <p>Alexander (Sasha) Krot (University of Hawaii), Yuri Amelin (University of Toronto), Pat Cassen (SETI Institute), and Anders Meibom (Museum National d'Histoire Naturelle, Paris) studied and then extracted frozen droplets of molten silicate (<span class="hlt">chondrules</span>) from unusual meteorites rich in metallic iron-nickel. Called CB (Bencubbin-like) chondrites, these rare but fascinating meteorites contain <span class="hlt">chondrules</span> with different properties than those in other types of chondrites. Most notably, the <span class="hlt">chondrules</span> contain very small concentrations of volatile elements and variable concentrations of refractory elements. (Volatile elements condense from a gas at a relatively low temperature, or are boiled out of solids or liquids at relatively low temperature. Refractory elements are the opposite.) Some of the metal grains in CB chondrites are chemically zoned, indicating that they formed by condensation in a vapor cloud. The most intriguing feature of <span class="hlt">chondrules</span> in CB chondrites is their relatively young age. Lead-lead isotopic dating of <span class="hlt">chondrules</span> separated from two CB chondrites show that they formed 5 million years after formation of the first solids in the solar system (calcium-aluminum-rich inclusions), which is about at least two million years after formation of other <span class="hlt">chondrules</span>, and after energetic events in the solar nebula stopped. Krot and his colleagues suggest that the CB <span class="hlt">chondrules</span> formed as the result of an impact between Moon- to Mars-sized protoplanets. Such impacts were so energetic that huge amounts of material were vaporized and then condensed as <span class="hlt">chondrules</span> or chemically zoned metal grains. This event enriched refractory elements and depleted volatile elements. Such large impacts appear to play important roles in planet formation, including the formation of the Moon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950012911&hterms=Mg+Ca&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DMg%2BCa','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950012911&hterms=Mg+Ca&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DMg%2BCa"><span>Heating during solar nebula formation and Mg isotopic fractionation in precursor grains of CAIs and <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sasaki, S.; Nagahara, H.; Kitagami, K.; Nakagawa, Y.</p> <p>1994-01-01</p> <p>In some Ca-Al-rich inclusion (CAI) grains, mass-dependent isotopic fractionations of Mg, Si, and O are observed and large Mg isotopic fractionation is interpreted to have been produced by cosmochemical processes such as evaporation and condensation. Mass-dependent Mg isotopic fractionation was found in <span class="hlt">olivine</span> <span class="hlt">chondrules</span> of Allende meteorites. Presented is an approximate formula for the temperature of the solar nebula that depends on heliocentric distance and the initial gas distribution. Shock heating during solar nebula formation can cause evaporative fractionation within interstellar grains involved in a gas at the inner zone (a less than 3 AU) of the disk. Alternatively collision of late-accreting gas blobs might cause similar heating if Sigma(sub s) and Sigma are large enough. Since the grain size is small, the solid/gas mass ratio is low and solar (low P(sub O2)), and the ambient gas pressure is low, this heating event could not produce <span class="hlt">chondrules</span> themselves. <span class="hlt">Chondrule</span> formation should proceed around the disk midplane after dust grains would grow and sediment to increase the solid/gas ratio there. The heating source there is uncertain, but transient rapid accretion through the disk could release a large amount of heat, which would be observed as FU Orionis events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950012875&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=19950012875&hterms=recycling&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Drecycling"><span>Producing <span class="hlt">chondrules</span> by recycling and volatile loss</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Alexander, C. M. O.</p> <p>1994-01-01</p> <p>Interelement correlations observed in bulk <span class="hlt">chondrule</span> INAA data, particularly between the refractory lithophiles, have led to the now generally accepted conclusion that the <span class="hlt">chondrule</span> precursors were nebular condensates. However, it has been recently suggested that random sampling of fragments from a previous generation of <span class="hlt">chondrules</span> could reproduce much of the observed range of bulk <span class="hlt">chondrule</span> composition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EM%26P..108..139Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EM%26P..108..139Z"><span>Lavras do Sul: A New Equilibrated Ordinary L5 Chondrite from Rio Grande do Sul, Brazil</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zucolotto, M. E.; Antonello, L. L.; Varela, M. E.; Scorzelli, R. B.; Ludka, Isabel P.; Munayco, P.; dos Santos, E.</p> <p>2012-03-01</p> <p>The new Brazilian chondrite, Lavras do Sul, was found in 1985 at Lavras do Sul, Rio Grande do Sul State-Brazil (33°30'48″S; 53°54'65″W). It consists of a single mass weighing about 1 kg, covered by a black fusion crust with grayish interior. Four polished thin sections were prepared from a slice weighing 67 g on deposit at the Museu Nacional/UFRJ. It consists mostly of <span class="hlt">chondrules</span> and <span class="hlt">chondrule</span> fragments dispersed in a recrystallized matrix. Most <span class="hlt">chondrules</span> are poorly defined and range in size from 300 to 2,000 μm, although some of them show distinct outlines, particularly when viewed under cross-polarized transmitted and reflected light. The texture of <span class="hlt">chondrules</span> varies from non-porphyritic (e.g., <span class="hlt">barred-olivine</span>, radial-pyroxene) to porphyritic ones (e.g., granular <span class="hlt">olivine</span> as well as <span class="hlt">olivine</span>-pyroxene). The meteorite contains mainly <span class="hlt">olivine</span> (Fa24.9), low-Ca pyroxene (Fs22.6) and metal phases, with minor amounts of plagioclase, chromite and magnetite. Mössbauer Spectroscopy studies indicate that the metal phase is kamacite, tetrataenite and antitaenite. Veins of secondary iddingsite crosscut the thin section and some ferromagnesian silicates. The chemical composition indicates that Lavras do Sul is a member of the low iron L chondrite group. The poorly delineated chondritic texture with few well-defined <span class="hlt">chondrules</span>, the occurrence of rare clinopyroxene and plagioclase (and maskelynite) with apparent diameters ranging from 5 to 123 μm led us to classify Lavras do Sul as an equilibrated petrologic type 5. The shock features of some minerals suggest a shock stage S3, and the presence of a small amount of secondary minerals such as iddingsite and goethite, a degree of weathering W1. The meteorite name was approved by the Nomenclature Committee (Nom Com) of the Meteoritical Society (Meteoritic Bulletin Nº99).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPSC...11..145N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPSC...11..145N"><span>Deriving global <span class="hlt">Olivine</span> distribution on Hayabusa's target (25143) Itokawa using Near-Infrared Spectrometer data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nardi, L.; Palomba, E.; Longobardo, A.; Galiano, A.; Dirri, F.</p> <p>2017-09-01</p> <p>In 2005 Hayabusa spacecraft visited asteroid Itokawa, bringing back surface samples to Earth in 2010. Near-Infrared data taken by NIRS and samples analysis confirmed hypothesis made through ground-based observations, in particular the one that sees Itokawa as an LL-chondrite like asteroid processed by space weathering. In this work, we apply spectral indices for <span class="hlt">olivine</span> detection. In particular, we define the <span class="hlt">BAR</span>* and relate it to the <span class="hlt">olivine</span> abundance, by means of calibration on laboratory data. We present the distribution of <span class="hlt">BAR</span>* calculated for nearly 38.000 spectra taken from an altitude of 3.5-7 km, defined as Home Position, which was the longest mission observation phase. In addition, a plot of <span class="hlt">olivine</span> normalized content versus <span class="hlt">BAR</span>* for RELAB compounds is given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70000462','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70000462"><span>The formation conditions of <span class="hlt">chondrules</span> and chondrites</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Alexander, C.M. O'D.; Grossman, Jeffrey N.; Ebel, D.S.; Ciesla, F.J.</p> <p>2008-01-01</p> <p><span class="hlt">Chondrules</span>, which are roughly millimeter-sized silicate-rich spherules, dominate the most primitive meteorites, the chondrites. They formed as molten droplets and, judging from their abundances in chondrites, are the products of one of the most energetic processes that operated in the early inner solar system. The conditions and mechanism of <span class="hlt">chondrule</span> formation remain poorly understood. Here we show that the abundance of the volatile element sodium remained relatively constant during <span class="hlt">chondrule</span> formation. Prevention of the evaporation of sodium requires that <span class="hlt">chondrules</span> formed in regions with much higher solid densities than predicted by known nebular concentration mechanisms. These regions would probably have been self-gravitating. Our model explains many other chemical characteristics of <span class="hlt">chondrules</span> and also implies that <span class="hlt">chondrule</span> and planetesimal formation were linked.</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_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_4 --> <div id="page_5" 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_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</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="81"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22667200-relict-olivines-micrometeorites-precursors-interactions-earths-atmosphere','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22667200-relict-olivines-micrometeorites-precursors-interactions-earths-atmosphere"><span>RELICT <span class="hlt">OLIVINES</span> IN MICROMETEORITES: PRECURSORS AND INTERACTIONS IN THE EARTH’S ATMOSPHERE</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>Rudraswami, N. G.; Prasad, M. Shyam; Dey, S.</p> <p>2016-11-10</p> <p>Antarctica micrometeorites (∼1200) and cosmic spherules (∼5000) from deep sea sediments are studied using electron microscopy to identify Mg-rich <span class="hlt">olivine</span> grains in order to determine the nature of the particle precursors. Mg-rich <span class="hlt">olivine</span> (FeO < 5wt%) in micrometeorites suffers insignificant chemical modification during its history and is a well-preserved phase. We examine 420 forsterite grains enclosed in 162 micrometeorites of different types—unmelted, scoriaceous, and porphyritic—in this study. Forsterites in micrometeorites of different types are crystallized during their formation in solar nebula; their closest analogues are <span class="hlt">chondrule</span> components of CV-type chondrites or volatile rich CM chondrites. The forsteritic <span class="hlt">olivines</span> are suggestedmore » to have originated from a cluster of closely related carbonaceous asteroids that have Mg-rich <span class="hlt">olivines</span> in the narrow range of CaO (0.1–0.3wt%), Al{sub 2}O{sub 3} (0.0–0.3wt%), MnO (0.0–0.3wt%), and Cr{sub 2}O{sub 3} (0.1–0.7wt%). Numerical simulations carried out with the Chemical Ablation Model (CABMOD) enable us to define the physical conditions of atmospheric entry that preserve the original compositions of the Mg-rich <span class="hlt">olivines</span> in these particles. The chemical compositions of relict <span class="hlt">olivines</span> affirm the role of heating at peak temperatures and the cooling rates of the micrometeorites. This modeling approach provides a foundation for understanding the ablation of the particles and the circumstances in which the relict grains tend to survive.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050165557','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050165557"><span>Genetic Relationships Between <span class="hlt">Chondrules</span>, Rims and Matrix</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Huss, G. R.; Alexander, C. M. OD.; Palme, H.; Bland, P. A.; Wasson, J. T.</p> <p>2004-01-01</p> <p>The most primitive chondrites are composed of <span class="hlt">chondrules</span> and <span class="hlt">chondrule</span> fragments, various types of inclusions, discrete mineral grains, metal, sulfides, and fine-grained materials that occur as interchondrule matrix and as <span class="hlt">chondrule</span>/inclusion rims. Understanding how these components are related is essential for understanding how chondrites and their constituents formed and were processed in the solar nebula. For example, were the first generations of <span class="hlt">chondrules</span> formed by melting of matrix or matrix precursors? Did <span class="hlt">chondrule</span> formation result in appreciable transfer of <span class="hlt">chondrule</span> material into the matrix? Here, we consider three types of data: 1) compositional data for bulk chondrites and matrix, 2) mineralogical and textural information, and 3) the abundances and characteristics of presolar materials that reside in the matrix and rims. We use these data to evaluate the roles of evaporation and condensation, <span class="hlt">chondrule</span> formation, mixing of different nebular components, and secondary processing both in the nebula and on the parent bodies. Our goal is to identify the things that are reasonably well established and to point out the areas that need additional work.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JGRE..11612007E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JGRE..11612007E"><span>Magnetic characteristics of CV <span class="hlt">chondrules</span> with paleointensity implications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emmerton, Stacey; Muxworthy, Adrian R.; Hezel, Dominik C.; Bland, Philip A.</p> <p>2011-12-01</p> <p>We have conducted a detailed magnetic study on 45 <span class="hlt">chondrules</span> from two carbonaceous chondrites of the CV type: (1) Mokoia and (2) Allende. Allende has been previously extensively studied and is thought to have a high potential of retaining an extra-terrestrial paleofield. Few paleomagnetic studies of Mokoia have previously been undertaken. We report a range of magnetic measurements including hysteresis, first-order reversal curve analysis (FORCs), demagnetization characteristics, and isothermal remanent (IRM) acquisition behavior on both Mokoia and Allende <span class="hlt">chondrules</span>. The Mokoia <span class="hlt">chondrules</span> displayed more single domain-like behavior than the Allende <span class="hlt">chondrules</span>, suggesting smaller grain sizes and higher magnetic stability. The Mokoia <span class="hlt">chondrules</span> also had higher average concentrations of magnetic minerals and a larger range of magnetic characteristics than the Allende <span class="hlt">chondrules</span>. IRM acquisition analysis found that both sets of <span class="hlt">chondrules</span> have the same dominant magnetic mineral, likely to be a FeNi phase (taenite, kamacite, and/or awaruite) contributing to 48% of the Mokoia <span class="hlt">chondrules</span> and 42% of the Allende <span class="hlt">chondrule</span> characteristics. FORC analysis revealed that generally the Allende <span class="hlt">chondrules</span> displayed low-field coercivity distributions with little interactions, and the Mokoia <span class="hlt">chondrules</span> show clear single-domain like distributions. Paleointensity estimates for the two meteorites using the REMc and Preisach methods yielded estimates between 13 and 60 μT and 3-56 μT, respectively, for Allende and 3-140 μT and 1-110 μT, respectively, for Mokoia. From the data, we suggest that Mokoia <span class="hlt">chondrules</span> carry a non-primary remagnetization, and while Allende is more likely than Mokoia to retain its primary magnetization, it also displays signs of post accretionary magnetization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994Metic..29Q.482K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994Metic..29Q.482K"><span>Distribution of some highly volatile elements in <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, J. S.; Marti, K.</p> <p>1994-07-01</p> <p>As <span class="hlt">chondrule</span> apparently were melted before accretion into chondritic parent bodies, we carried out a N and Xe isotopic study to obtain information on the partitioning of some of the most volatile as well as incompatible elements: noble gases, N, I, REE, and Pu. In separated silicates in Forest Vale, consisting of mostly broken <span class="hlt">chondrules</span>, we observed rather large Xe concentrations, and since noble gases in chondrites are associated with C-rich phases, we decided to study the core portion of a suite of <span class="hlt">chondrules</span> after removing the <span class="hlt">chondrule</span> rim portion and adhering matrix. We selected sets of rounded <span class="hlt">chondrules</span> from four meteorites: Allende (CV3), Dhajala (H3.8), Forest Vale (H4), and Bjurbole (L4). We compare measured N and Xe concentrations and isotopic abundances in cores of <span class="hlt">chondrules</span> to those obtained from unetched <span class="hlt">chondrules</span>. We discuss results obtained from melting steps, because N and Xe in the silicate lattice are mostly released at T greater than 1000 C. All cores of <span class="hlt">chondrules</span> contain less than 1% of the Xe in the respective bulk samples. Moreover, they released much less trapped Xe in the melting step than did untreated bulk chondrites. However, the radiogenic Xer-129 and fissiogenic Xef is not or is only slightly depleted, and spallogenic Xe is a major component, particularly in Forest Vale. We can not deduce the signature of trapped Xe in the <span class="hlt">chondrules</span>. The release systematics are completely different from those observed in primitive achondrites, which contain noble gas in the 'dusty' silicate inclusions. Allende <span class="hlt">chondrules</span> differ from those of ordinary chondrite in the N release pattern. This represents possibly a signature of the local environment during <span class="hlt">chondrule</span> formation, since N may exist in <span class="hlt">chondrule</span> minerals in chemically bound forms. In contrast, all three sets of ordinary chondrite <span class="hlt">chondrules</span> released less than 0.6 ppm N in the melting step, and these signatures reveal substantial components of cosmic-ray-produced N.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUSMMA12A..02W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUSMMA12A..02W"><span>Mineralogy and petrology of the Buzzard Coulee H4 chondrite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Walton, E.; Herd, C.</p> <p>2009-05-01</p> <p>The Buzzard Coulee meteorite was collected as fragments from a fireball witnessed at 17:26.43 MST on November 20, 2008 by thousands of residents across the Canadian prairies. Three samples were made available to this study, weighing 34, 37 and 151.7 g. In hand specimen, the stones are partially to completely covered by black fusion crust. The interior is light grey, with <span class="hlt">chondrules</span> and metal grains readily visible on the broken surface. Prior to sample processing, a NextEngine Desktop 3D laser scanner was used to capture and preserve the meteorite morphology. This method also provides an estimate of the sample volume, which was used to determine a bulk density of 3.5 g/cm3. Microtextures were then characterized using a JEOL 6301F Field Emission SEM at the University of Alberta. Mineral and glass compositions were collected using a Cameca SX- 100 electron microprobe at the same institution. The overall texture is massive, with <span class="hlt">chondrules</span> embedded in a fine-grained matrix with coarser Fe-Ni metals (500 to 800 microns). Major minerals / phases include low-Ca pyroxene (Fs15.8Wo1.0), pigeonite (Fs12.9Wo14.6), <span class="hlt">olivine</span> (Fa17.7), devitrified alkali-rich glass, troilite, kamacite and taenite with minor chromite, merrillite, pentlandite, augite (Fs5.2Wo46.0), and rare spinel (s.s.) and silica glass. The matrix is texturally heterogeneous on a cm-sale; minor recrystallization and small mineral fragments (5 to 15 microns) are typical; dendritic textures of low-Ca pyroxene in glass have also been observed. A variety of <span class="hlt">chondrule</span> types are present in the thin section; <span class="hlt">barred</span> <span class="hlt">olivine</span>, porphyritic <span class="hlt">olivine</span>, porphyritic pyroxene, porphyritic <span class="hlt">olivine</span>-pyroxene, cryptocrystalline pyroxene, radial pyroxene, metal-rich and Al-rich. The Al- rich <span class="hlt">chondrule</span> contains skeletal grains of <span class="hlt">olivine</span> in devitrified alkali-rich glass with euhedral spinel (s.s.) zoned to chromite near the <span class="hlt">chondrule</span> rim. In general, the cryptocrystalline pyroxene <span class="hlt">chondrules</span> are the best preserved with sharply defined</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993Metic..28..466Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993Metic..28..466Z"><span>Metal Precursors and Reduction in Renazzo <span class="hlt">Chondrules</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zanda, B.; Hewins, R. H.; Bourot-Denise, M.</p> <p>1993-07-01</p> <p>The positive Co-Ni correlation and Cr, P contents of metal in CR chondrites have generally been taken to indicate their primitive nature, probably inherited from condensation [1,2]. Si in the metal of primitive chondrites has also been reported and interpreted as a condensation heritage [3,4]. However, Cr, P, and Si (dissolved or in the form of inclusions) in metal of any CR <span class="hlt">chondrule</span> generally fall within a +-10% range, though large interchondrule variations exist [5]. We have shown that Cr and Si in metal are in equilibrium with Fo and En in silicates, due to the reducing conditions that prevailed during <span class="hlt">chondrule</span> formation [6]. In the present paper, we show that the Co-Ni trend was also established during <span class="hlt">chondrule</span> formation out of heterogeneous precursor material with a variable Co/Ni ratio. <span class="hlt">Chondrules</span> in Renazzo are classified as highly molten (HM), in which metal has been expelled to form a mantle outside the <span class="hlt">chondrule</span>, medium molten (MM), with metal inside and at the periphery, and with evidence for grain coalescence, and little melted (LM), in which metal is only present in the form of small blebs dispersed among the silicates. In HM <span class="hlt">chondrules</span>, Ni and Co concentrations are extremely homogeneous, comparatively low and in the cosmic ratio. In LM <span class="hlt">chondrules</span>, quite the opposite: Ni and Co spread over a large range and the amount of scatter increases with decreasing degree of melting of the <span class="hlt">chondrule</span>. In addition, they do not correlate along the cosmic ratio, but show a negative correlation if any. This heterogeneity is present not only from grain to grain in these <span class="hlt">chondrules</span>, but also in individual metal grains. Such a heterogeneity is also exhibited in Cr and P abundances that span a much larger range than the +-10% found in the other <span class="hlt">chondrules</span>. These results indicate that <span class="hlt">chondrule</span> formation is responsible for the homogenization of Co and Ni contents of metal grains through coalescence and mixing. The less melted objects give an idea of the nature of metal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70028854','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70028854"><span>Alkali elemental and potassium isotopic compositions of Semarkona <span class="hlt">chondrules</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>Alexander, C.M. O'D.; Grossman, J.N.</p> <p>2005-01-01</p> <p>We report measurements of K isotope ratios in 28 Semarkona <span class="hlt">chondrules</span> with a wide range of petrologic types and bulk compositions as well as the compositions of CPX-mesostasis pairs in 17 type I Semarkona <span class="hlt">chondrules</span>, including two <span class="hlt">chondrules</span> with radial alkali zonation and 19 type II <span class="hlt">chondrules</span>. Despite the wide range in K/Al ratios, no systematic variations in K isotopic compositions were found. Semarkona <span class="hlt">chondrules</span> do not record a simple history of Rayleigh-type loss of K. Experimentally determined evaporation rates suggest that considerable alkali evaporation would have occurred during <span class="hlt">chondrule</span> formation. Nevertheless, based on Na CPX-mesostasis distribution coefficients, the alkali contents of the cores of most <span class="hlt">chondrules</span> in Semarkona were probably established at the time of final crystallization. However, Na CPX-mesostasis distribution coefficients also show that alkali zonation in type I Semarkona <span class="hlt">chondrules</span> was produced by entry of alkalis after solidification, probably during parent body alteration. This alkali metasomatism may have gone to completion in some <span class="hlt">chondrules</span>. Our preferred explanation for the lack of systematic isotopic enrichments, even in alkali depleted type I <span class="hlt">chondrule</span> cores, is that they exchanged with the ambient gas as they cooled. ?? The Meteoritical Society, 2005.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017M%26PS...52.1991A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017M%26PS...52.1991A"><span>Geochemical and oxygen isotope perspective of a new R chondrite Dhofar 1671: Affinity with ordinary chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ali, Arshad; Nasir, Sobhi J.; Jabeen, Iffat; Al Rawas, Ahmed; Banerjee, Neil R.; Osinski, Gordon R.</p> <p>2017-09-01</p> <p>Dhofar 1671 is a relatively new meteorite that previous studies suggest belongs to the Rumuruti chondrite class. Major and REE compositions are generally in agreement with average values of the R chondrites (RCs). Moderately volatile elements such as Se and Zn abundances are lower than the R chondrite values that are similar to those in ordinary chondrites (OCs). Porphyritic <span class="hlt">olivine</span> pyroxene (POP), radial pyroxene (RP), and <span class="hlt">barred</span> <span class="hlt">olivine</span> (BO) <span class="hlt">chondrules</span> are embedded in a proportionately equal volume of matrix, one of the characteristic features of RCs. Microprobe analyses demonstrate compositional zoning in <span class="hlt">chondrule</span> and matrix <span class="hlt">olivines</span> showing Fa-poor interior and Fa-rich outer zones. Precise oxygen isotope data for <span class="hlt">chondrules</span> and matrix obtained by laser-assisted fluorination show a genetic isotopic relationship between OCs and RCs. On the basis of our data, we propose a strong affinity between these groups and suggest that OC <span class="hlt">chondrule</span> precursors could have interacted with a 17O-rich matrix to form RC <span class="hlt">chondrules</span> (i.e., ∆17O shifts from 1‰ to 3‰). These interactions could have occurred at the same time as "exotic" clasts in brecciated samples formed such as NWA 10214 (LL3-6), Parnallee (LL3), PCA91241 (R3.8-6), and Dhofar 1671 (R3.6). We also infer that the source of the oxidation and 17O enrichment is the matrix, which may have been enriched in 17O-rich water. The abundance of matrix in RCs relative to OCs, ensured that these rocks would be apparently more oxidized and appreciably 17O-enriched. In situ analysis of Dhofar 1671 is recommended to further strengthen the link between OCs and RCs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830012613','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830012613"><span>Conference on <span class="hlt">Chondrules</span> and Their Origins</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hrametz, K.</p> <p>1983-01-01</p> <p><span class="hlt">Chondrule</span> parent materials, <span class="hlt">chondrule</span> formation, and post-formational history are addressed. Contributions involving mineralogy petrology, geochemistry, geochronology, isotopic measurements, physical measurements, experimental studies, and theoretical studies are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V31A4718U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V31A4718U"><span>Experimental Constraints on Alkali Volatilization during <span class="hlt">Chondrule</span> Formation: Implications for Early Solar System Heterogeneity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ustunisik, G. K.; Ebel, D. S.; Nekvasil, H.</p> <p>2014-12-01</p> <p>The chemical variability of <span class="hlt">chondrule</span> volatile element contents provide a wealth of information on the processes that shaped the early solar system and its compositional heterogeneity. An essential observation is that <span class="hlt">chondrule</span> melts contain very low alkalies and other volatile elements (e.g., Cl). The reason for this depletion is the combined effects of cooling rates (10 to 1000K/h), the small size of <span class="hlt">chondrules</span>, and their high melting temperatures (~1700 to 2100 K) resulting in extensive loss of volatiles at canonical pressures (e.g., 10-4<span class="hlt">bar</span>). However, we observe some <span class="hlt">chondrules</span> with significant concentrations of volatiles (Na, Cl), that differ markedly from <span class="hlt">chondrules</span> dominated by refractory elements. Could such heterogeneity arise from loss of alkalis and Cl to a gas phase that itself later condenses, thereby yielding variations in volatile enrichments in <span class="hlt">chondrules</span>? Does Cl enhance volatility of the alkalis to varying extents? Experiments on Cl-bearing and Cl-free melts of equivalent composition for 10 min, 4 h, and 6 h reveal systematic effects of Cl on alkali volatility. Cl-bearing melts lose 48% of initial Na2O, 66% of K2O, 96% of Cl within the first 10 minutes of degassing. Then the amount of alkali loss decreases due to the absence of Cl. Cl-free melts loses only 15% of initial Na2O and 33% K2O. After 4 hours, melts lose 1/3 of initial Na2O and 1/2 of K2O. For both systems, Na2O is more compatible in the melt relative to K2O. Therefore, the vapor given off has a K/Na ratio higher than the melt through time in spite of the much higher initial Na abundance in the melt. Enhanced vaporization of alkalis from Cl-bearing melt suggests that Na and K evaporate more readily as volatile chlorides than as monatomic gases. Cl-free initial melts with normative plagioclase of An50Ab44Or6 evolved into slightly normal zoned ones (An49Ab50Or1) while Cl-bearing initial melts normative to albitic plagioclase (An46Ab50Or4) evolved to reverse zoned ones (An54Ab45Or1). The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.209...24M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.209...24M"><span>Formation of unequilibrated R chondrite <span class="hlt">chondrules</span> and opaque phases</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miller, K. E.; Lauretta, D. S.; Connolly, H. C.; Berger, E. L.; Nagashima, K.; Domanik, K.</p> <p>2017-07-01</p> <p>Sulfide assemblages are commonly found in chondritic meteorites as small inclusions in the matrix or in association with <span class="hlt">chondrules</span>. These assemblages are widely hypothesized to form through pre-accretionary corrosion of metal by H2S gas or through parent body processes. We report here on two unequilibrated R chondrite samples that contain large, <span class="hlt">chondrule</span>-sized sulfide nodules in the matrix. Both samples are from Mount Prestrud (PRE) 95404. Chemical maps and spot and broad-beam electron microprobe analyses (EMPA) were used to assess the distribution, stoichiometry, and bulk composition of sulfide nodules and silicate <span class="hlt">chondrules</span> in the clasts. Oxygen isotope data were collected via secondary ion mass spectrometry (SIMS) to assess the relationship of <span class="hlt">chondrules</span> to other chondrite groups. Scanning electron microscopy (SEM), focused ion beam (FIB), and transmission electron microscopy (TEM) analyses were used to assess fine-scale features and identify crystal structures in sulfide assemblages. Thermodynamic models were used to assess the temperature, sulfur fugacity (fS2), total pressure, dust-to-gas ratio, and oxygen fugacity (fO2) conditions during sulfide nodule and <span class="hlt">chondrule</span> formation. The unequilibrated clasts include a mixture of type I and type II <span class="hlt">chondrules</span>, as well as non-porphyritic <span class="hlt">chondrules</span>. <span class="hlt">Chondrule</span> oxygen isotopes overlap with ordinary-chondrite <span class="hlt">chondrules</span>. Sulfide nodules average 200 μm in diameter, have rounded shapes, and are primarily composed of pyrrhotite, pentlandite, and magnetite. Some are deformed around <span class="hlt">chondrules</span> in a petrologic relationship similar in appearance to compound <span class="hlt">chondrules</span>. Both nodules and sulfides in <span class="hlt">chondrules</span> include phosphate inclusions and Cu-rich lamellae, which suggests a genetic relationship between sulfides in <span class="hlt">chondrules</span> and in the matrix. Ni/Co ratios for matrix and <span class="hlt">chondrule</span> sulfides are solar, while Fe and Ni are non-solar and inversely related. We hypothesize that sulfide nodules formed via pre-accretionary melt</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000E%26PSL.184...57R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000E%26PSL.184...57R"><span>16O enrichments in aluminum-rich <span class="hlt">chondrules</span> from ordinary chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Russell, Sara S.; MacPherson, Glenn J.; Leshin, Laurie A.; McKeegan, Kevin D.</p> <p>2000-12-01</p> <p>The oxygen isotopic compositions of seven Al-rich <span class="hlt">chondrules</span> from four unequilibrated ordinary chondrites were measured in situ using an ion microprobe. On an oxygen three isotope plot, the data are continuous with the ordinary chondrite ferromagnesian <span class="hlt">chondrule</span> field but extend it to more 16O-enriched values along a mixing line of slope=0.83±0.09, with the lightest value recorded at δ18O=-15.7±1.8‰ and δ17O=-13.5±2.6‰. If Al-rich <span class="hlt">chondrules</span> were mixtures of ferromagnesian <span class="hlt">chondrules</span> and CAI material, their bulk chemical compositions would require them to exhibit larger 16O enrichments than we observe. Therefore, Al-rich <span class="hlt">chondrules</span> are not simple mixtures of these two components. Three <span class="hlt">chondrules</span> exhibit significant internal isotopic heterogeneity indicative of partial exchange with a gaseous reservoir. Porphyritic Al-rich <span class="hlt">chondrules</span> are consistently 16O-rich relative to nonporphyritic ones, suggesting that degree of melting is a key factor and pointing to a nebular setting for the isotopic exchange process. Because Al-rich <span class="hlt">chondrules</span> are closely related to ferromagnesian <span class="hlt">chondrules</span>, their radiogenic Mg isotopic abundances can plausibly be applied to help constrain the timing or location of <span class="hlt">chondrule</span> formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940016315&hterms=Mn+complex&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DMn%2Bcomplex','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940016315&hterms=Mn+complex&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DMn%2Bcomplex"><span>Fe/Mn in <span class="hlt">olivine</span> of carbonaceous meteorites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steele, Ian M.</p> <p>1993-01-01</p> <p><span class="hlt">Olivines</span> in primitive meteorites show a range of Fe/Mn both within one grain and among grains suggesting that they have recorded changing conditions during or after growth. Because <span class="hlt">olivine</span> should be an early forming phase, Fe/Mn is used here to infer these earliest conditions. Initial Fe/Mn in cores of isolated, euhedral forsterite in both C2 and C3 meteorites ranges from 25 to 35 but differs at grain edge. Murchison (C2) forsterites show Fe/Mn approaching 1.0 at the grain edge while Ornans Fe/Mn is near 60 at grain edge. These values are lower than the matrix Fe/Mn for both meteorites and the distinct difference in zoning profile indicates different processes operating during and after grain growth. The Fe/Mn of bulk samples from a particular source such as the Moon is nearly constant. Individual samples show variation suggesting that there is some fractionation of Mn from Fe. Minerals have their individual ranges of Fe/Mn which has been used to recognize different types of <span class="hlt">olivine</span> within one meteorite. Extreme values of Fe/Mn below 1.0 occur in forsterite from some IDP's, UOC matrix, and C1 meteorites. There are apparently no detailed studies of Fe/Mn variation within single <span class="hlt">olivine</span> grains. Forsterite grains in C2 and C3 carbonaceous chondrites show complex zoning, and the nearly pure forsterites (Fo greater than approximately 99.5) have high levels of some minor elements including Ti, Al, V, and Sc. There is disagreement on the original source of these grains and both <span class="hlt">chondrule</span> and vapor growth have been proposed. In addition, there is clear evidence that diffusion has affected the outer margins but in some cases the whole grain. Within the cores, the FeO range is limited, and if growing under constant conditions, the Fe/Mn should be near constant as there is little fractionation of Mn from Fe by forsterite. Additionally, there are apparently no co-crystallizing phases as evidenced by a lack of common inclusions in the forsterites. These observations are now</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930028355&hterms=oxygen+planets&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Doxygen%2Bplanets','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930028355&hterms=oxygen+planets&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Doxygen%2Bplanets"><span>The effect of oxygen fugacity on the partitioning of nickel and cobalt between <span class="hlt">olivine</span>, silicate melt, and metal</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ehlers, Karin; Grove, Timothy L.; Sisson, Thomas W.; Recca, Steven I.; Zervas, Deborah A.</p> <p>1992-01-01</p> <p>The effect of oxygen fugacity, f(O2), on the partitioning behavior of Ni and Co between <span class="hlt">olivine</span>, silicate melt, and metal was investigated in the CaO-MgO-Al2O3-SiO2-FeO-Na2O system, an analogue of a <span class="hlt">chondrule</span> composition from an ordinary chondrite. The conditions were 1350 C and 1 atm, with values of f(O2) varying between 10 exp -5.5 and 10 exp -12.6 atm (i.e., the f(O2) range relevant for crystal/liquid processes in terrestrial planets and meteorite parent bodies). Results of chemical analysis showed that the values of the Ni and Co partitioning coefficients begin to decrease at values of f(O2) that are about 3.9 log units below the nickel-nickel oxide and cobalt-cobalt oxide buffers, respectively, near the metal saturation for the <span class="hlt">chondrule</span> analogue composition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950012924&hterms=granovsky&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgranovsky','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950012924&hterms=granovsky&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dgranovsky"><span>Textural variability of ordinary chondrite <span class="hlt">chondrules</span>: Implications of their formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zinovieva, N. G.; Mitreikina, O. B.; Granovsky, L. B.</p> <p>1994-01-01</p> <p>Scanning electron microscopy (SEM) and microprobe examination of the Raguli H3-4, Saratov L3, and Fucbin L5-6 ordinary chondrites and the analysis of preexisted data on other meteorites have shown that the variety of textural types of <span class="hlt">chondrules</span> depends on the chemical composition of the <span class="hlt">chondrules</span>. The comparison of bulk-rock chemistries of the <span class="hlt">chondrules</span> by major components demonstrates that they apparently fall, like basic-ultrabasic rock, into groups of dunitic and pyroxenitic composition. This separation is further validated by the character of zoning in <span class="hlt">chondrules</span> of the intermediate, peridotitic type. The effect is vividly demonstrated by the '<span class="hlt">chondrule-in-chondrule</span>' structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010059877','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010059877"><span>On the Lower Limit of <span class="hlt">Chondrule</span> Cooling Rates: The Significance of Iron Loss in Dynamic Crystallization Experiments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paque, Julie M.; Connolly, Harold C., Jr.; Lofgren, Gary E.</p> <p>1998-01-01</p> <p>It is unlikely that the presence of <span class="hlt">chondrules</span>, and thus their formation, within the protoplanetary nebula would be predicted if it were not for their ubiquitous presence in most chondritic meteorites. The study of these enigmatic, igneous objects has a direct influence on how meteoritic and solar system researchers model the processes operating and the materials present within our protoplanetary nebula. Key to understanding <span class="hlt">chondrule</span> formation is a determination of constraints on their thermal histories. The three important variables in this history are their peak melting temperatures, the duration of their melting at peak temperatures, and the rate at which these object cool. Although these three variables are interdependent, it is cooling rate that provides the most powerful constraint. Cooling rate has a direct affect on the development of both crystal morphology and the elemental distributions within these grains. To date, experiments have indicated that <span class="hlt">chondrule</span> cooling rates are in the range of 10's to 100's of degrees per hour for porphyritic <span class="hlt">chondrules</span> (the most abundant type). The cooling rate for radial and <span class="hlt">barred</span> <span class="hlt">chondrules</span> is thought to be more rapid. To generate these cooling rates (rapid relative to the cooling of the nebula as a whole, but slow compared to simple black body radiation) the environment of <span class="hlt">chondrule</span> formation must have been localized, and the abundance of solid materials must have been greatly enhanced above a gas of solar composition. Thus accurate determinations of <span class="hlt">chondrule</span> cooling rates is critical in understanding both their formation and the nebular environment in which they formed. In a quest to more accurately determine the lower limit on cooling rates and to determine in more detail the effects of Fe loss from a molten sample to Pt wire loops, Weinbruch et al. have explored this issue experimentally and reevaluated the findings of Radomsky and Hewins in light of their new results. The basic conclusions of their paper are an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApJ...752...27M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApJ...752...27M"><span><span class="hlt">Chondrule</span> Formation in Bow Shocks around Eccentric Planetary Embryos</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morris, Melissa A.; Boley, Aaron C.; Desch, Steven J.; Athanassiadou, Themis</p> <p>2012-06-01</p> <p>Recent isotopic studies of Martian meteorites by Dauphas & Pourmand have established that large (~3000 km radius) planetary embryos existed in the solar nebula at the same time that chondrules—millimeter-sized igneous inclusions found in meteorites—were forming. We model the formation of <span class="hlt">chondrules</span> by passage through bow shocks around such a planetary embryo on an eccentric orbit. We numerically model the hydrodynamics of the flow and find that such large bodies retain an atmosphere with Kelvin-Helmholtz instabilities allowing mixing of this atmosphere with the gas and particles flowing past the embryo. We calculate the trajectories of <span class="hlt">chondrules</span> flowing past the body and find that they are not accreted by the protoplanet, but may instead flow through volatiles outgassed from the planet's magma ocean. In contrast, <span class="hlt">chondrules</span> are accreted onto smaller planetesimals. We calculate the thermal histories of <span class="hlt">chondrules</span> passing through the bow shock. We find that peak temperatures and cooling rates are consistent with the formation of the dominant, porphyritic texture of most <span class="hlt">chondrules</span>, assuming a modest enhancement above the likely solar nebula average value of <span class="hlt">chondrule</span> densities (by a factor of 10), attributable to settling of <span class="hlt">chondrule</span> precursors to the midplane of the disk or turbulent concentration. We calculate the rate at which a planetary embryo's eccentricity is damped and conclude that a single planetary embryo scattered into an eccentric orbit can, over ~105 years, produce ~1024 g of <span class="hlt">chondrules</span>. In principle, a small number (1-10) of eccentric planetary embryos can melt the observed mass of <span class="hlt">chondrules</span> in a manner consistent with all known constraints.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950012874','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950012874"><span>Papers presented to the Conference on <span class="hlt">Chondrules</span> and the Protoplanetary Disk</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1994-01-01</p> <p>The following topics are covered in the presented papers: (1) producing <span class="hlt">chondrules</span>; (2) carbons, CAI's, and <span class="hlt">chondrules</span>; (3) large scale processes in the solar nebula; (4) <span class="hlt">chondrule</span>-matrix relationships in chondritic meteorites; (5) overview of nebula models; (6) constraints placed on the nature of <span class="hlt">chondrule</span> precursors; (7) turbulent diffusion and concentration of <span class="hlt">chondrules</span> in the protoplanetary nebula; (8) heating and cooling in the solar nebula; (9) crystallization trends of precursor pyroxene in ordinary chondrites; (10) precipitation induced vertical lightning in the protoplanetary nebula; (11) the role of <span class="hlt">chondrules</span> in nebular fractionations of volatiles and other elements; (12) astronomical observations of phenomena in disks; (13) experimental constraints on models for origins of <span class="hlt">chondrules</span>, and various other topics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050174600','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050174600"><span>Porphyritic <span class="hlt">Olivine</span>-Pyroxene Clast in Kaidun: First Discovery of an Ordinary Chondrite Clast?</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mikouchi, T.; Makishima, J.; Koizumi, E.; Zolensky, M. E.</p> <p>2005-01-01</p> <p>Kaidun is an enigmatic meteorite showing a micro-brecciated texture composed of variable kinds of lithic clasts and mineral fragments. The constituent components range from primitive chondritic materials to differentiated achondritic materials, and thus believed to have originated from a large parent body accumulating materials from many different bodies in the asteroid belt. One of the interesting observations is that no ordinary chondrite component has been found yet, although C and E chondrites components are abundant. In this abstract, we report mineralogy of the clast (Kaidun #15415- 01.3.13a) showing a porphyritic <span class="hlt">olivine</span>-pyroxene <span class="hlt">chondrule</span>-like texture similar to those found in unequilibrated ordinary chondrites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030065978','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030065978"><span>Mineralogy and Petrology of Amoeboid <span class="hlt">Olivine</span> Inclusions in CO3 Chondrites: Relationship to Parent-Body Aqueous Alteration</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chizmadia, Lysa J.; Rubin, Alan E.; Wasson, John T.</p> <p>2003-01-01</p> <p>Petrographic and mineralogic studies of amoeboid <span class="hlt">olivine</span> inclusions (AOIs) in CO3 carbonaceous chondrites reveal that they are sensitive indicators of parent-body aqueous and thermal alteration. As the petrologic subtype increases from 3.0 to 3.8, forsteritic <span class="hlt">olivine</span> (Fa(sub 0-1)) is systematically converted into ferroan <span class="hlt">olivine</span> (Fa(sub 60-75)). We infer that the Fe, Si and O entered the assemblage along grain boundaries, forming ferroan <span class="hlt">olivine</span> that filled fractures and voids. As temperatures increased, Fe(+2) from the new <span class="hlt">olivine</span> exchanged with Mg(+2) from the original AOI to form diffusive haloes around low-FeO cores. Cations of Mn(+2), Ca(+2) and Cr(+3) were also mobilized. The systematic changes in AOI textures and <span class="hlt">olivine</span> compositional distributions can be used to refine the classification of CO3 chondrites into subtypes. In subtype 3.0, <span class="hlt">olivine</span> occurs as small forsterite grains (Fa(sub 0-1)), free of ferroan <span class="hlt">olivine</span>. In petrologic subtype 3.2, narrow veins of FeO-rich <span class="hlt">olivine</span> have formed at forsterite grain boundaries. With increasing alteration, these veins thicken to form zones of ferroan <span class="hlt">olivine</span> at the outside AOI margin and within the AOI interior. By subtype 3.7, there is a fairly broad <span class="hlt">olivine</span> compositional distribution in the range Fa(sub 63-70), and by subtype 3.8, no forsterite remains and the high-Fa peak has narrowed, Fa(sub 64-67). Even at this stage, there is incomplete equilibration in the chondrite as a whole (e.g., data for coarse <span class="hlt">olivine</span> grains in Isna (CO3.8) <span class="hlt">chondrules</span> and lithic clasts show a peak at Fa(sub39)). We infer that the mineral changes in A01 identified in the low petrologic types required aqueous or hydrothermal fluids whereas those in subtypes greater than or equal to 3.3 largely reflect diffusive exchange within and between mineral grains without the aid of fluids.</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_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_5 --> <div id="page_6" 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_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> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="101"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940016300&hterms=Skinner+William&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DSkinner%2BWilliam','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940016300&hterms=Skinner+William&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DSkinner%2BWilliam"><span>Size distributions and aerodynamic equivalence of metal <span class="hlt">chondrules</span> and silicate <span class="hlt">chondrules</span> in Acfer 059</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Skinner, William R.; Leenhouts, James M.</p> <p>1993-01-01</p> <p>The CR2 chondrite Acfer 059 is unusual in that the original droplet shapes of metal <span class="hlt">chondrules</span> are well preserved. We determined separate size distributions for metal <span class="hlt">chondrules</span> and silicate <span class="hlt">chondrules</span>; the two types are well sorted and have similar size distributions about their respective mean diameters of 0.74 mm and 1.44 mm. These mean values are aerodynamically equivalent for the contrasting densities, as shown by calculated terminal settling velocities in a model solar nebula. Aerodynamic equivalence and similarity of size distributions suggest that metal and silicate fractions experienced the same sorting process before they were accreted onto the parent body. These characteristics, together with depletion of iron in Acfer 059 and essentially all other chondrites relative to primitive CI compositions, strongly suggest that sorting in the solar nebula involved a radial aerodynamic component and that sorting and siderophile depletion in chondrites are closely related.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940031660','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940031660"><span>Shape, size, and distribution of magnetic particles in Bjurbole <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nava, David F.</p> <p>1994-01-01</p> <p><span class="hlt">Chondrules</span> from the Bjurbole chondritic meteorite (L4) exhibit saturation remanence magnetization (SIRM) values which vary over three orders of magnitude. REM values (Natural Remanence Magnetization/SIRM) for Allende (C3V) and Chainpur (LL3) are less than 0.01 but in Bjurbole some <span class="hlt">chondrules</span> were found to have REM values greater than 0.1 with several greater than 0.2. REM values greater than 0.1 are abnormal and cannot be acquired during weak field cooling. If exposure to a strong field (whatever the source) during the <span class="hlt">chondrules</span>' history is responsible for the high REM values, was such history associated with a different processing which might have resulted in different shape, size, and distribution of metal particles compared to <span class="hlt">chondrules</span> having REM values of less than 0.01? Furthermore, magnetic hysteresis results show a broad range of magnetic hardness and other intrinsic magnetic properties. These features must be related to (1) size and amount of metal; and (2) properties of, and amount of, tetrataenite in the <span class="hlt">chondrules</span> (all <span class="hlt">chondrules</span> thus far subjected to thermomagnetic analysis show the presence of tetrataenite). A scanning electron microscopy (SEM) study is underway to determine the relationship between the shape, size, and distribution of metal particles within individual <span class="hlt">chondrules</span> and the magnetic properties of these <span class="hlt">chondrules</span>. Results from the SEM study in conjunction with magnetic property data may also help to discern effects from possible lightning strikes in the nebula prior to incorporation of the <span class="hlt">chondrules</span> into the parent body.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770054093&hterms=Theory+constraints&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DTheory%2Bconstraints','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770054093&hterms=Theory+constraints&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DTheory%2Bconstraints"><span>A constraint on impact theories of <span class="hlt">chondrule</span> formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kerridge, J. F.; Kieffer, S. W.</p> <p>1977-01-01</p> <p>The association between agglutinates and <span class="hlt">chondrule</span>-like spherules, which characterizes the assemblage of impact-derived melt products in lunar regolith samples and some gas-rich achondrites, is not found in primitive chondrites. This observation suggests that impacts into a parent-body regolith are unlikely to have produced the <span class="hlt">chondrules</span>. We believe that if <span class="hlt">chondrules</span> were formed from impact melt, it was probably generated by jetting during particle-to-particle collisions, presumably in the nebula.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014Icar..242....1S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014Icar..242....1S"><span>A critical analysis of shock models for <span class="hlt">chondrule</span> formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stammler, Sebastian M.; Dullemond, Cornelis P.</p> <p>2014-11-01</p> <p>In recent years many models of <span class="hlt">chondrule</span> formation have been proposed. One of those models is the processing of dust in shock waves in protoplanetary disks. In this model, the dust and the <span class="hlt">chondrule</span> precursors are overrun by shock waves, which heat them up by frictional heating and thermal exchange with the gas. In this paper we reanalyze the nebular shock model of <span class="hlt">chondrule</span> formation and focus on the downstream boundary condition. We show that for large-scale plane-parallel <span class="hlt">chondrule</span>-melting shocks the postshock equilibrium temperature is too high to avoid volatile loss. Even if we include radiative cooling in lateral directions out of the disk plane into our model (thereby breaking strict plane-parallel geometry) we find that for a realistic vertical extent of the solar nebula disk the temperature decline is not fast enough. On the other hand, if we assume that the shock is entirely optically thin so that particles can radiate freely, the cooling rates are too high to produce the observed <span class="hlt">chondrules</span> textures. Global nebular shocks are therefore problematic as the primary sources of <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApJ...857...96M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApJ...857...96M"><span>Magnetic Fields Recorded by <span class="hlt">Chondrules</span> Formed in Nebular Shocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mai, Chuhong; Desch, Steven J.; Boley, Aaron C.; Weiss, Benjamin P.</p> <p>2018-04-01</p> <p>Recent laboratory efforts have constrained the remanent magnetizations of <span class="hlt">chondrules</span> and the magnetic field strengths to which the <span class="hlt">chondrules</span> were exposed as they cooled below their Curie points. An outstanding question is whether the inferred paleofields represent the background magnetic field of the solar nebula or were unique to the <span class="hlt">chondrule</span>-forming environment. We investigate the amplification of the magnetic field above background values for two proposed <span class="hlt">chondrule</span> formation mechanisms, large-scale nebular shocks and planetary bow shocks. Behind large-scale shocks, the magnetic field parallel to the shock front is amplified by factors of ∼10–30, regardless of the magnetic diffusivity. Therefore, <span class="hlt">chondrules</span> melted in these shocks probably recorded an amplified magnetic field. Behind planetary bow shocks, the field amplification is sensitive to the magnetic diffusivity. We compute the gas properties behind a bow shock around a 3000 km radius planetary embryo, with and without atmospheres, using hydrodynamics models. We calculate the ionization state of the hot, shocked gas, including thermionic emission from dust, thermal ionization of gas-phase potassium atoms, and the magnetic diffusivity due to Ohmic dissipation and ambipolar diffusion. We find that the diffusivity is sufficiently large that magnetic fields have already relaxed to background values in the shock downstream where <span class="hlt">chondrules</span> acquire magnetizations, and that these locations are sufficiently far from the planetary embryos that <span class="hlt">chondrules</span> should not have recorded a significant putative dynamo field generated on these bodies. We conclude that, if melted in planetary bow shocks, <span class="hlt">chondrules</span> probably recorded the background nebular field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9445468','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9445468"><span>The origin of <span class="hlt">chondrules</span> at jovian resonances</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Weidenschilling; Marzari; Hood</p> <p>1998-01-30</p> <p>Isotopic dating indicates that <span class="hlt">chondrules</span> were produced a few million years after the solar nebula formed. This timing is incompatible with dynamical lifetimes of small particles in the nebula and short time scales for the formation of planetesimals. Temporal and dynamical constraints can be reconciled if <span class="hlt">chondrules</span> were produced by heating of debris from disrupted first-generation planetesimals. Jovian resonances can excite planetesimal eccentricities enough to cause collisional disruption and melting of dust by bow shocks in the nebular gas. The ages of <span class="hlt">chondrules</span> may indicate the times of Jupiter's formation and dissipation of gas from the asteroidal region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018P%26SS..151..149R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018P%26SS..151..149R"><span>The Mukundpura meteorite, a new fall of CM chondrite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ray, Dwijesh; Shukla, Anil D.</p> <p>2018-02-01</p> <p>Mukundpura is a new CM chondrite fell near Jaipur, Rajasthan, India on June 6, 2017 at 5:15 IST. The fall was observed by local villager. According to eyewitness, the meteorite was fragmented into several pieces once the object hit the ground. Based on petrography, mineralogy and bulk composition, Mukundpura is classified as CM2 chondrite. The <span class="hlt">chondrules</span> are mainly similar to type I (<span class="hlt">Olivine</span>: Fo99). <span class="hlt">Olivines</span> are often found associated with pyroxene (Wo10-35En62-87Fs2-7) phenocryst. However, occurrences of forsteritic and fayalitic <span class="hlt">olivine</span> (Fa58-71) as isolated mineral clast in matrix are not uncommon. Other types of <span class="hlt">chondrules</span> include porphyritic pyroxene (En86Fs14) and <span class="hlt">barred</span> <span class="hlt">olivine</span> (Fa32.7±0.3) clast. <span class="hlt">Chondrules</span> are commonly rimmed by fine-grained accretionary dust mantles. Phyllosilicates are the most dominant secondary mineral in matrix and largely associated with poorly characterised phases (PCP). FeO/SiO2 and S/SiO2 of PCP are 2.7 and 0.4 respectively. Other phases in matrix generally include calcite (pure CaCO3), Fe-Ni metal and sulphides. Spinel and perovskite occur occasionally as inclusions. The spherical or elliptical shaped metals (within <span class="hlt">chondrule</span> or in isolated grains) are low-Ni type (kamacite <7.5 wt%) and resembles the solar Ni/Co ratio. However, Ni content in metal rarely exceeds 8.5 wt% (up to 23 wt%, taenite). Pyrrhotite (Fe ∼62 wt%; S ∼38 wt%) and pentlandite (Fe ∼31-33 wt%, Ni ∼28-32 wt%, S ∼33 wt%)) are the common sulphides occur as isolated grains within the matrix, however, the former is the most dominant. The bulk chemical composition of Mukundpura is largely similar to other CM type chondrite (e.g. Paris CM). Based on petrography, we infer a modest aqueous alteration stage for Mukundpura while the effect of thermal metamorphism was negligible.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5550225','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5550225"><span>Early formation of planetary building blocks inferred from Pb isotopic ages of <span class="hlt">chondrules</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>Bollard, Jean; Connelly, James N.; Whitehouse, Martin J.; Pringle, Emily A.; Bonal, Lydie; Jørgensen, Jes K.; Nordlund, Åke; Moynier, Frédéric; Bizzarro, Martin</p> <p>2017-01-01</p> <p>The most abundant components of primitive meteorites (chondrites) are millimeter-sized glassy spherical <span class="hlt">chondrules</span> formed by transient melting events in the solar protoplanetary disk. Using Pb-Pb dates of 22 individual <span class="hlt">chondrules</span>, we show that primary production of <span class="hlt">chondrules</span> in the early solar system was restricted to the first million years after the formation of the Sun and that these existing <span class="hlt">chondrules</span> were recycled for the remaining lifetime of the protoplanetary disk. This finding is consistent with a primary <span class="hlt">chondrule</span> formation episode during the early high-mass accretion phase of the protoplanetary disk that transitions into a longer period of <span class="hlt">chondrule</span> reworking. An abundance of <span class="hlt">chondrules</span> at early times provides the precursor material required to drive the efficient and rapid formation of planetary objects via <span class="hlt">chondrule</span> accretion. PMID:28808680</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApJ...826..151H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApJ...826..151H"><span>Partitioning Tungsten between Matrix Precursors and <span class="hlt">Chondrule</span> Precursors through Relative Settling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hubbard, Alexander</p> <p>2016-08-01</p> <p>Recent studies of chondrites have found a tungsten isotopic anomaly between <span class="hlt">chondrules</span> and matrix. Given the refractory nature of tungsten, this implies that W was carried into the solar nebula by at least two distinct families of pre-solar grains. The observed <span class="hlt">chondrule</span>/matrix split requires that the distinct families were kept separate during the dust coagulation process, and that the two families of grain interacted with the <span class="hlt">chondrule</span> formation mechanism differently. We take the co-existence of different families of solids in the same general orbital region at the <span class="hlt">chondrule</span>-precursor size as given, and explore the requirements for them to have interacted with the <span class="hlt">chondrule</span> formation process at significantly different rates. We show that this sorting of families of solids into <span class="hlt">chondrule</span>- and matrix-destined dust had to have been at least as powerful a sorting mechanism as the relative settling of aerodynamically distinct grains at least two scale heights above the midplane. The requirement that the <span class="hlt">chondrule</span> formation mechanism was correlated in some fashion with a dust-grain sorting mechanism argues strongly for spatially localized <span class="hlt">chondrule</span> formation mechanisms such as turbulent dissipation in non-thermally ionized disk surface layers, and argues against volume-filling mechanisms such as planetesimal bow shocks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679621-partitioning-tungsten-between-matrix-precursors-chondrule-precursors-through-relative-settling','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679621-partitioning-tungsten-between-matrix-precursors-chondrule-precursors-through-relative-settling"><span>PARTITIONING TUNGSTEN BETWEEN MATRIX PRECURSORS AND <span class="hlt">CHONDRULE</span> PRECURSORS THROUGH RELATIVE SETTLING</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>Hubbard, Alexander, E-mail: ahubbard@amnh.org</p> <p>2016-08-01</p> <p>Recent studies of chondrites have found a tungsten isotopic anomaly between <span class="hlt">chondrules</span> and matrix. Given the refractory nature of tungsten, this implies that W was carried into the solar nebula by at least two distinct families of pre-solar grains. The observed <span class="hlt">chondrule</span>/matrix split requires that the distinct families were kept separate during the dust coagulation process, and that the two families of grain interacted with the <span class="hlt">chondrule</span> formation mechanism differently. We take the co-existence of different families of solids in the same general orbital region at the <span class="hlt">chondrule</span>-precursor size as given, and explore the requirements for them to have interactedmore » with the <span class="hlt">chondrule</span> formation process at significantly different rates. We show that this sorting of families of solids into <span class="hlt">chondrule</span>- and matrix-destined dust had to have been at least as powerful a sorting mechanism as the relative settling of aerodynamically distinct grains at least two scale heights above the midplane. The requirement that the <span class="hlt">chondrule</span> formation mechanism was correlated in some fashion with a dust-grain sorting mechanism argues strongly for spatially localized <span class="hlt">chondrule</span> formation mechanisms such as turbulent dissipation in non-thermally ionized disk surface layers, and argues against volume-filling mechanisms such as planetesimal bow shocks.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Icar..302...27L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Icar..302...27L"><span>Impact splash <span class="hlt">chondrule</span> formation during planetesimal recycling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lichtenberg, Tim; Golabek, Gregor J.; Dullemond, Cornelis P.; Schönbächler, Maria; Gerya, Taras V.; Meyer, Michael R.</p> <p>2018-03-01</p> <p><span class="hlt">Chondrules</span>, mm-sized igneous-textured spherules, are the dominant bulk silicate constituent of chondritic meteorites and originate from highly energetic, local processes during the first million years after the birth of the Sun. So far, an astrophysically consistent <span class="hlt">chondrule</span> formation scenario explaining major chemical, isotopic and textural features, in particular Fe,Ni metal abundances, bulk Fe/Mg ratios and intra-chondrite chemical and isotopic diversity, remains elusive. Here, we examine the prospect of forming <span class="hlt">chondrules</span> from impact splashes among planetesimals heated by radioactive decay of short-lived radionuclides using thermomechanical models of their interior evolution. We show that intensely melted planetesimals with interior magma oceans became rapidly chemically equilibrated and physically differentiated. Therefore, collisional interactions among such bodies would have resulted in <span class="hlt">chondrule</span>-like but basaltic spherules, which are not observed in the meteoritic record. This inconsistency with the expected dynamical interactions hints at an incomplete understanding of the planetary growth regime during the lifetime of the solar protoplanetary disk. To resolve this conundrum, we examine how the observed chemical and isotopic features of <span class="hlt">chondrules</span> constrain the dynamical environment of accreting chondrite parent bodies by interpreting the meteoritic record as an impact-generated proxy of early solar system planetesimals that underwent repeated collision and reaccretion cycles. Using a coupled evolution-collision model we demonstrate that the vast majority of collisional debris feeding the asteroid main belt must be derived from planetesimals which were partially molten at maximum. Therefore, the precursors of chondrite parent bodies either formed primarily small, from sub-canonical aluminum-26 reservoirs, or collisional destruction mechanisms were efficient enough to shatter planetesimals before they reached the magma ocean phase. Finally, we outline the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11099410','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11099410"><span>The formation of <span class="hlt">chondrules</span> at high gas pressures in the solar nebula.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Galy, A; Young, E D; Ash, R D; O'Nions, R K</p> <p>2000-12-01</p> <p>High-precision magnesium isotope measurements of whole <span class="hlt">chondrules</span> from the Allende carbonaceous chondrite meteorite show that some aluminum-rich Allende <span class="hlt">chondrules</span> formed at or near the time of formation of calcium-aluminum-rich inclusions and that some others formed later and incorporated precursors previously enriched in magnesium-26. <span class="hlt">Chondrule</span> magnesium-25/magnesium-24 correlates with [magnesium]/[aluminum] and size, the aluminum-rich, smaller <span class="hlt">chondrules</span> being the most enriched in the heavy isotopes of magnesium. These relations imply that high gas pressures prevailed during <span class="hlt">chondrule</span> formation in the solar nebula.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4640629','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4640629"><span>Growth of asteroids, planetary embryos, and Kuiper belt objects by <span class="hlt">chondrule</span> accretion</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Johansen, Anders; Low, Mordecai-Mark Mac; Lacerda, Pedro; Bizzarro, Martin</p> <p>2015-01-01</p> <p><span class="hlt">Chondrules</span> are millimeter-sized spherules that dominate primitive meteorites (chondrites) originating from the asteroid belt. The incorporation of <span class="hlt">chondrules</span> into asteroidal bodies must be an important step in planet formation, but the mechanism is not understood. We show that the main growth of asteroids can result from gas drag–assisted accretion of <span class="hlt">chondrules</span>. The largest planetesimals of a population with a characteristic radius of 100 km undergo runaway accretion of <span class="hlt">chondrules</span> within ~3 My, forming planetary embryos up to Mars’s size along with smaller asteroids whose size distribution matches that of main belt asteroids. The aerodynamical accretion leads to size sorting of <span class="hlt">chondrules</span> consistent with chondrites. Accretion of millimeter-sized <span class="hlt">chondrules</span> and ice particles drives the growth of planetesimals beyond the ice line as well, but the growth time increases above the disc lifetime outside of 25 AU. The contribution of direct planetesimal accretion to the growth of both asteroids and Kuiper belt objects is minor. In contrast, planetesimal accretion and <span class="hlt">chondrule</span> accretion play more equal roles in the formation of Moon-sized embryos in the terrestrial planet formation region. These embryos are isolated from each other and accrete planetesimals only at a low rate. However, the continued accretion of <span class="hlt">chondrules</span> destabilizes the oligarchic configuration and leads to the formation of Mars-sized embryos and terrestrial planets by a combination of direct <span class="hlt">chondrule</span> accretion and giant impacts. PMID:26601169</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SciA....1E0109J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SciA....1E0109J"><span>Growth of asteroids, planetary embryos, and Kuiper belt objects by <span class="hlt">chondrule</span> accretion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Johansen, Anders; Mac Low, Mordecai-Mark; Lacerda, Pedro; Bizzarro, Martin</p> <p>2015-04-01</p> <p><span class="hlt">Chondrules</span> are millimeter-sized spherules that dominate primitive meteorites (chondrites) originating from the asteroid belt. The incorporation of <span class="hlt">chondrules</span> into asteroidal bodies must be an important step in planet formation, but the mechanism is not understood. We show that the main growth of asteroids can result from gas drag-assisted accretion of <span class="hlt">chondrules</span>. The largest planetesimals of a population with a characteristic radius of 100 km undergo runaway accretion of <span class="hlt">chondrules</span> within ~3 My, forming planetary embryos up to Mars's size along with smaller asteroids whose size distribution matches that of main belt asteroids. The aerodynamical accretion leads to size sorting of <span class="hlt">chondrules</span> consistent with chondrites. Accretion of millimeter-sized <span class="hlt">chondrules</span> and ice particles drives the growth of planetesimals beyond the ice line as well, but the growth time increases above the disc lifetime outside of 25 AU. The contribution of direct planetesimal accretion to the growth of both asteroids and Kuiper belt objects is minor. In contrast, planetesimal accretion and <span class="hlt">chondrule</span> accretion play more equal roles in the formation of Moon-sized embryos in the terrestrial planet formation region. These embryos are isolated from each other and accrete planetesimals only at a low rate. However, the continued accretion of <span class="hlt">chondrules</span> destabilizes the oligarchic configuration and leads to the formation of Mars-sized embryos and terrestrial planets by a combination of direct <span class="hlt">chondrule</span> accretion and giant impacts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26601169','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26601169"><span>Growth of asteroids, planetary embryos, and Kuiper belt objects by <span class="hlt">chondrule</span> accretion.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Johansen, Anders; Low, Mordecai-Mark Mac; Lacerda, Pedro; Bizzarro, Martin</p> <p>2015-04-01</p> <p><span class="hlt">Chondrules</span> are millimeter-sized spherules that dominate primitive meteorites (chondrites) originating from the asteroid belt. The incorporation of <span class="hlt">chondrules</span> into asteroidal bodies must be an important step in planet formation, but the mechanism is not understood. We show that the main growth of asteroids can result from gas drag-assisted accretion of <span class="hlt">chondrules</span>. The largest planetesimals of a population with a characteristic radius of 100 km undergo runaway accretion of <span class="hlt">chondrules</span> within ~3 My, forming planetary embryos up to Mars's size along with smaller asteroids whose size distribution matches that of main belt asteroids. The aerodynamical accretion leads to size sorting of <span class="hlt">chondrules</span> consistent with chondrites. Accretion of millimeter-sized <span class="hlt">chondrules</span> and ice particles drives the growth of planetesimals beyond the ice line as well, but the growth time increases above the disc lifetime outside of 25 AU. The contribution of direct planetesimal accretion to the growth of both asteroids and Kuiper belt objects is minor. In contrast, planetesimal accretion and <span class="hlt">chondrule</span> accretion play more equal roles in the formation of Moon-sized embryos in the terrestrial planet formation region. These embryos are isolated from each other and accrete planetesimals only at a low rate. However, the continued accretion of <span class="hlt">chondrules</span> destabilizes the oligarchic configuration and leads to the formation of Mars-sized embryos and terrestrial planets by a combination of direct <span class="hlt">chondrule</span> accretion and giant impacts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800060501&hterms=1103&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3D%2526%25231103','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800060501&hterms=1103&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3D%2526%25231103"><span><span class="hlt">Olivines</span> and <span class="hlt">olivine</span> coronas in mesosiderites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nehru, C. E.; Zucker, S. M.; Harlow, G. E.; Prinz, M.</p> <p>1980-01-01</p> <p>The paper presents a study of <span class="hlt">olivines</span> and their surrounding coronas in mesosiderites texturally and compositionally using optical and microprobe methods. <span class="hlt">Olivine</span> composition ranges from Fo(58-92) and shows no consistent pattern of distribution within and between mesosiderites; <span class="hlt">olivine</span> occurs as large single crystals or as partially recrystallized mineral clasts, except for two lithic clasts. These are Emery and Vaca Muerta, and both are shock-modified <span class="hlt">olivine</span> orthopyroxenites. Fine-grained coronas surround <span class="hlt">olivine</span>, except for those in impact-melt group mesosiderites and those without tridymite in their matrices. Coronas consist largely of orthopyroxene, plagioclase, clinopyroxene, chromite, merillite, and ilmenite, and are similar to the matrix, but lack metal and tridymite. Texturally the innermost parts of the corona can be divided into three stages of development: (1) radiating acicular, (2) intermediate, and (3) granular.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.201..185K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.201..185K"><span>Calcium-aluminum-rich inclusions recycled during formation of porphyritic <span class="hlt">chondrules</span> from CH carbonaceous chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krot, Alexander N.; Nagashima, Kazuhide; van Kooten, Elishevah M. M.; Bizzarro, Martin</p> <p>2017-03-01</p> <p>We report on the mineralogy, petrography, and O-isotope compositions of ∼60 Ca, Al-rich inclusions (CAIs) incompletely melted during formation of porphyritic <span class="hlt">chondrules</span> from the CH metal-rich carbonaceous chondrites and Isheyevo (CH/CB). These include (i) relict polymineralic CAIs in porphyritic <span class="hlt">chondrules</span>, (ii) CAIs surrounded by <span class="hlt">chondrule</span>-like igneous rims, (iii) igneous pyroxene-rich and Type C-like CAIs, and (iv) plagioclase-rich <span class="hlt">chondrules</span> with clusters of relict spinel grains. 26Al-26Mg systematics were measured in 10 relict CAIs and 11 CAI-bearing plagioclase-rich <span class="hlt">chondrules</span>. Based on the mineralogy, the CH CAIs incompletely melted during <span class="hlt">chondrule</span> formation can be divided into grossite-rich (n = 13), hibonite-rich (n = 11), spinel ± melilite-rich (n = 33; these include plagioclase-rich <span class="hlt">chondrules</span> with clusters of relict spinel grains) types. Mineralogical observations indicate that these CAIs were mixed with different proportions of ferromagnesian silicates and experienced incomplete melting and gas-melt interaction during <span class="hlt">chondrule</span> formation. These processes resulted in partial or complete destruction of the CAI Wark-Lovering rims, replacement of melilite by Na-bearing plagioclase, and dissolution and overgrowth of nearly end-member spinel by chromium- and iron-bearing spinel. Only two relict CAIs and two CAI-bearing <span class="hlt">chondrules</span> show resolvable excess of radiogenic 26Mg; the inferred initial 26Al/27Al ratios are (1.7 ± 1.3) × 10-6, (3.7 ± 3.1) × 10-7, (1.9 ± 0.9) × 10-6 and (4.9 ± 2.6) × 10-6. There is a large range of Δ17O among the CH CAIs incompletely melted during <span class="hlt">chondrule</span> formation, from ∼-37‰ to ∼-5‰; the unmelted minerals in individual CAIs, however, are isotopically uniform and systematically 16O-enriched relative to the host <span class="hlt">chondrules</span> and <span class="hlt">chondrule</span>-like igneous rims, which have Δ17O ranging from ∼-7‰ to ∼+4‰. Most of the CH CAIs incompletely melted during <span class="hlt">chondrule</span> formation are mineralogically and isotopically</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4942334','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4942334"><span>Early scattering of the solar protoplanetary disk recorded in meteoritic <span class="hlt">chondrules</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>Marrocchi, Yves; Chaussidon, Marc; Piani, Laurette; Libourel, Guy</p> <p>2016-01-01</p> <p>Meteoritic <span class="hlt">chondrules</span> are submillimeter spherules representing the major constituent of nondifferentiated planetesimals formed in the solar protoplanetary disk. The link between the dynamics of the disk and the origin of <span class="hlt">chondrules</span> remains enigmatic. Collisions between planetesimals formed at different heliocentric distances were frequent early in the evolution of the disk. We show that the presence, in some <span class="hlt">chondrules</span>, of previously unrecognized magnetites of magmatic origin implies the formation of these <span class="hlt">chondrules</span> under impact-generated oxidizing conditions. The three oxygen isotopes systematic of magmatic magnetites and silicates can only be explained by invoking an impact between silicate-rich and ice-rich planetesimals. This suggests that these peculiar <span class="hlt">chondrules</span> are by-products of the early mixing in the disk of populations of planetesimals from the inner and outer solar system. PMID:27419237</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830057375&hterms=deutsche+forschungsgemeinschaft&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Ddeutsche%2Bforschungsgemeinschaft','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830057375&hterms=deutsche+forschungsgemeinschaft&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Ddeutsche%2Bforschungsgemeinschaft"><span>Ca-Al-rich <span class="hlt">chondrules</span> and inclusions in ordinary chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bischoff, A.; Keil, K.</p> <p>1983-01-01</p> <p>Ca-Al-rich objects, hitherto mostly found in carbonaceous chondrites, are shown to be widespread, albeit rare, constituents of type 3 ordinary chondrites. Widespread occurrence and textural similarities of Ca-Al-rich <span class="hlt">chondrules</span> to common, Mg-Fe-rich <span class="hlt">chondrules</span> suggest that they formed by related processes. It is suggested in this article that Ca-Al-rich <span class="hlt">chondrules</span> were formed by total melting and crystallization of heterogeneous, submillimeter- to submillimeter-sized dustballs made up of mixtures of high-temperature, Ca-Al-rich and lower-temperature, Na-K-rich components.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUSM.P41C..08H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUSM.P41C..08H"><span>Single <span class="hlt">Chondrule</span> K/Ar ages of Mexican Meteorites Using ID-TIMS.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hernandez, M.; Sole, J.</p> <p>2007-05-01</p> <p>We have determined the K/Ar ages of two H5 ordinary meteorites: Cosina and Nuevo Mercurio, neither dated until this study. We analyzed several single <span class="hlt">chondrules</span> - weighing few milligrams - of each meteorite. Ages were obtained by using very precise K content determined by isotope dilution mass spectrometry. The K content in <span class="hlt">chondrules</span> ranges between 650 and 1400 ppm. The 40Ar was measured by static vacuum noble gas mass spectrometry. Samples were fused with an infrared CO2 laser. <span class="hlt">Chondrule</span> ages vary from 3.66 to 4.59 Ga for Cosina and from 4.20 to 4.87 Ga for Nuevo Mercurio. A comparison between our data and the published K/Ar ages of H and L whole rocks shows that dates obtained from single <span class="hlt">chondrules</span> are older than those obtained from whole rocks and seem to preserve older events not evidenced in the WR ages. This implies that <span class="hlt">chondrules</span> can preserve K/Ar ages very close to U-Pb crystallization ages.</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('https://pubs.er.usgs.gov/publication/70014150','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014150"><span>Compositional evidence regarding the origins of rims on Semarkona <span class="hlt">chondrules</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>Grossman, J.N.; Wasson, J.T.</p> <p>1987-01-01</p> <p>The compositions of the interiors and abraded surfaces of 7 <span class="hlt">chondrules</span> from Semarkona (LL3.0) were measured by neutron activation analysis. For nonvolatile elements, the lithophile and siderophile element abundance patterns in the surfaces are generally similar to those in the corresponding interiors. Siderophile and chalcophile concentrations are much higher in the surfaces, whereas lithophile concentrations are similar in both fractions. Most of the similarities in lithophile patterns and some of the similarities in siderophile patterns between surfaces and interiors may reflect incomplete separation of the fractions in the laboratory, but for 3 or 4 <span class="hlt">chondrules</span> the siderophile resemblance is inherent, implying that the surface and interior metal formed from a single precursor assemblage. Metal and sulfide-rich <span class="hlt">chondrule</span> rims probably formed when droplets of these phases that migrated to the <span class="hlt">chondrule</span> surface during melting were reheated and incorporated into matrix-like material that had accreted onto the surface. The moderately-volatile to volatile elements K, As and Zn tend to be enriched in the surfaces compared with other elements of similar mineral affinity; both enrichments and depletions are observed for other moderately volatile elements. A small fraction of <span class="hlt">chondrules</span> experienced fractional evaporation while they were molten. ?? 1987.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22370448-forming-chondrules-impact-splashes-radiative-cooling-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22370448-forming-chondrules-impact-splashes-radiative-cooling-model"><span>Forming <span class="hlt">chondrules</span> in impact splashes. I. Radiative cooling model</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>Dullemond, Cornelis Petrus; Stammler, Sebastian Markus; Johansen, Anders</p> <p>2014-10-10</p> <p>The formation of <span class="hlt">chondrules</span> is one of the oldest unsolved mysteries in meteoritics and planet formation. Recently an old idea has been revived: the idea that <span class="hlt">chondrules</span> form as a result of collisions between planetesimals in which the ejected molten material forms small droplets that solidify to become <span class="hlt">chondrules</span>. Pre-melting of the planetesimals by radioactive decay of {sup 26}Al would help produce sprays of melt even at relatively low impact velocity. In this paper we study the radiative cooling of a ballistically expanding spherical cloud of <span class="hlt">chondrule</span> droplets ejected from the impact site. We present results from numerical radiative transfermore » models as well as analytic approximate solutions. We find that the temperature after the start of the expansion of the cloud remains constant for a time t {sub cool} and then drops with time t approximately as T ≅ T {sub 0}[(3/5)t/t {sub cool} + 2/5]{sup –5/3} for t > t {sub cool}. The time at which this temperature drop starts t {sub cool} depends via an analytical formula on the mass of the cloud, the expansion velocity, and the size of the <span class="hlt">chondrule</span>. During the early isothermal expansion phase the density is still so high that we expect the vapor of volatile elements to saturate so that no large volatile losses are expected.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140012796','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140012796"><span>Contrasting Size Distributions of <span class="hlt">Chondrules</span> and Inclusions in Allende CV3</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fisher, Kent R.; Tait, Alastair W.; Simon, Jusin I.; Cuzzi, Jeff N.</p> <p>2014-01-01</p> <p>There are several leading theories on the processes that led to the formation of chondrites, e.g., sorting by mass, by X-winds, turbulent concentration, and by photophoresis. The juxtaposition of refractory inclusions (CAIs) and less refractory <span class="hlt">chondrules</span> is central to these theories and there is much to be learned from their relative size distributions. There have been a number of studies into size distributions of particles in chondrites but only on relatively small scales primarily for <span class="hlt">chondrules</span>, and rarely for both Calcium Aluminum-rich Inclusions (CAIs) and <span class="hlt">chondrules</span> in the same sample. We have implemented macro-scale (25 cm diameter sample) and high-resolution microscale sampling of the Allende CV3 chondrite to create a complete data set of size frequencies for CAIs and <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhDT.......173L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhDT.......173L"><span>Magnetic reconnection as a <span class="hlt">chondrule</span> heating mechanism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lazerson, Samuel A.</p> <p>2010-12-01</p> <p>The origin of <span class="hlt">chondrules</span> (sub-millimeter inclusions found in stony meteorites) remains today an open question despite over century of examination. The age of these proto-solar relics shows a well defined cutoff of around 4.5 billion years ago. This places them as the oldest solids in the solar system. Chemical examination indicates that they experienced heating events on the order of 5000 K/hr for periods of around 30 minutes, followed by extending periods of cooling. Additional examination indicates the presence of large magnetic fields during their formation. Most attempts to explain <span class="hlt">chondrule</span> formation in the proto-solar nebula neglect the existence of a plasma environment, with even less mention of dust being a charge carrier (dusty plasma). Simulations of magnetic reconnection in a dusty plasma are forwarded as a mechanism for <span class="hlt">chondrule</span> formation in the proto-solar nebula. Here large dust-neutral relative velocities are found in the reconnection region. These flows are associated with the dynamics of reconnection. The high Knudsen number of the dust particles allows for a direct calculation of frictional heating due to collisions with neutrals (allowing for the neglect of boundary layer formation around the particle). Test particle simulations produce heating equivalent to that recorded in the <span class="hlt">chondrule</span> mineral record. It is shown that magnetic reconnection in a dusty plasma is of fundamental importance to the formation of the most primitive solids in the solar system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006ApJ...639.1227K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006ApJ...639.1227K"><span>Aluminum-Magnesium and Oxygen Isotope Study of Relict Ca-Al-rich Inclusions in <span class="hlt">Chondrules</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krot, Alexander N.; McKeegan, Kevin D.; Huss, Gary R.; Liffman, Kurt; Sahijpal, Sandeep; Hutcheon, Ian D.; Srinivasan, Gopalan; Bischoff, Adolph; Keil, Klaus</p> <p>2006-03-01</p> <p>Relict Ca-Al-rich inclusions (CAIs) in <span class="hlt">chondrules</span> crystallized before their host <span class="hlt">chondrules</span> and were subsequently partly melted together with <span class="hlt">chondrule</span> precursors during <span class="hlt">chondrule</span> formation. Like most CAIs, relict CAIs are 16O enriched (Δ17O<-20‰) compared to their host <span class="hlt">chondrules</span> (Δ17O>-9‰). Hibonite in a relict CAI from the ungrouped carbonaceous chondrite Adelaide has a large excess of radiogenic 26Mg (26Mg*) from the decay of 26Al, corresponding to an initial 26Al/27Al ratio [(26Al/27Al)I] of (3.7+/-0.5)×10-5 in contrast, melilite in this CAI and plagioclase in the host <span class="hlt">chondrule</span> show no evidence for 26Mg* [(26Al/27Al)I of <5×10-6]. Grossite in a relict CAI from the CH carbonaceous chondrite PAT 91546 has little 26Mg*, corresponding to a (26Al/27Al)I of (1.7+/-1.3)×10-6. Three other relict CAIs and their host <span class="hlt">chondrules</span> from the ungrouped carbonaceous chondrite Acfer 094, CH chondrite Acfer 182, and H3.4 ordinary chondrite Sharps do not have detectable 26Mg* [(26Al/27Al)I<1×10-5, <(4-6)×10-6, and <1.3×10-5, respectively]. Isotopic data combined with mineralogical observations suggest that relict CAIs formed in an 16O-rich gaseous reservoir before their host <span class="hlt">chondrules</span>, which originated in an 16O-poor gas. The Adelaide CAI was incorporated into its host <span class="hlt">chondrule</span> after 26Al had mostly decayed, at least 2 Myr after the CAI formed, and this event reset 26Al-26Mg systematics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....6830M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....6830M"><span>Iron isotope signatures within <span class="hlt">chondrules</span> from Allende and Chainpur as indicators of thermal history.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mullane, E.; Russell, S. S.; Gounelle, M.; Mason, T. F. D.</p> <p>2003-04-01</p> <p>Introduction: We have studied the petrography and Fe-isotope composition of seven <span class="hlt">chondrules</span>, four from Allende (CV3) and three from Chainpur (LL3.4). A range of textural-chemical <span class="hlt">chondrule</span> types are represented, allowing us to examine the Fe-isotope signature in material with different thermal histories, with a view to constraing the <span class="hlt">chondrule</span> forming process and elucidating the nature of <span class="hlt">chondrule</span> precursor material. Analytical procedures are detailed elsewhere [1,2,3] Fe-isotope Fractionation: The overall variation in δ56Fe is 1.98 ppm and in δ57Fe is 2.87 ppm. EM-1 (non-porphyritic) is most isotopically heavy and EM-3 (porphyritic) is most isotopically light, with all other <span class="hlt">chondrules</span> falling in a mass fractionation line between these two end-members. This line is defined by the equation δ57Fe = (1.450±0.050)δ56Fe - (0.009±0.016) (R^2 = 0.9995). Discussion: The Fe-fractionation exhibited here is less than would be expected during open system evaporation. This suggests that Rayleigh conditions were not fulfilled during <span class="hlt">chondrule</span> melting. Chainpur <span class="hlt">chondrules</span> exhibit less fractionation than Allende <span class="hlt">chondrules</span>, a total of 0.46 ppm (δ56Fe) in contrast to 1.98 ppm (δ56Fe), respectively, suggesting that Chainpur may be more equilibrated than Allende. Chainpur Fe-isotopes may have been increasingly homogenised by later addition of Fe, either from the nebular reservoir or parent body alteration. Porphyritic and nonporphyritic <span class="hlt">chondrules</span> have differing thermal histories. The former are a product of incomplete melting, whereas the latter derive from almost total/complete melting of precursor material. However, Fe-isotope fractionation does not appear to vary systematically with texture. We conclude that <span class="hlt">chondrule</span> Fe-isotopic signatures represent that of the precursor material, with later equilibration of the Chainpur <span class="hlt">chondrules</span>. Melting history may also influence the Fe-isotopic signature. The isotopically heaviest <span class="hlt">chondrules</span> (e.g. EM-1 &EC-3) may derive from a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850044390&hterms=droplet+beads&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Ddroplet%2Bbeads','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850044390&hterms=droplet+beads&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Ddroplet%2Bbeads"><span>Reduction, partial evaporation, and spattering - Possible chemical and physical processes in fluid drop <span class="hlt">chondrule</span> formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>King, E. A.</p> <p>1983-01-01</p> <p>The major chemical differences between fluid drop <span class="hlt">chondrules</span> and their probable parent materials may have resulted from the loss of volatiles such as S, H2O, Fe, and volatile siderophile elements by partial evaporation during the <span class="hlt">chondrule</span>-forming process. Vertical access solar furnace experiments in vacuum and hydrogen have demonstrated such chemical fractionation trends using standard rock samples. The formation of immiscible iron droplets and spherules by in situ reduction of iron from silicate melt and the subsequent evaporation of the iron have been observed directly. During the time that the main sample bead is molten, many small spatter spherules are thrown off the main bead, thereby producing many additional <span class="hlt">chondrule</span>-like melt spherules that cool rapidly and generate a population of spherules with size frequency distribution characteristics that closely approximate some populations of fluid drop <span class="hlt">chondrules</span> in chondrites. It is possible that spatter-produced fluid drop <span class="hlt">chondrules</span> dominate the meteoritic fluid drop <span class="hlt">chondrule</span> populations. Such meteoritic <span class="hlt">chondrule</span> populations should be chemically related by various relative amounts of iron and other volatile loss by vapor fractionation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995Metic..30R.594W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995Metic..30R.594W"><span>Chondrites: The Compaction of Fine Matrix and Matrix-like <span class="hlt">Chondrule</span> Rims</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wasson, J. T.</p> <p>1995-09-01</p> <p>Primitive chondritic meteorites mainly consist of <span class="hlt">chondrules</span>, sulfide+/-metal, and fine-grained matrix. The most unequilibrated chondrites preserve in their phase compositions and, to a lesser degree, their textures, many details about processes that occurred in the solar nebula. On the other hand, much of the textural evidence records processes that occurred in or on the parent body. I suggest that the low-porosity of <span class="hlt">chondrule</span> matrix and matrix-like rims reflects compaction processes that occurred in asteroid-size bodies, and that neither matrix lumps nor compact matrix-like rims on <span class="hlt">chondrules</span> could have achieved their observed low porosities in the solar nebula. Recent theoretical studies by Donn and Meakin (1) and Chokshi et al. (2) have concluded that grain-grain sticking in the solar nebula mainly produces fluffy structures having very high porosities (probably >>50%). If these structures grow large enough, they can provide an aerogel-like matrix that can trap <span class="hlt">chondrules</span> as well as metal and sulfide grains, and thus form suitable precursors of chondritic meteorites. However, the strength of any such structure formed in the solar nebula must be a trivial fraction of that required to survive passage through the Earth's atmosphere in order to fall as a meteorite. The best evidence of accretionary structures appears to be that reported by Metzler et al. (3). They made SEM images of entire thin sections of CM chondrites, and showed that, in the best preserved chondrites, rims are present on all entitities--on <span class="hlt">chondrules</span>, <span class="hlt">chondrule</span> fragments, refractory inclusions, etc. A study by Krot and Wasson (4) shows a more complex situation in ordinary chondrites. Although matrix is common, a sizable fraction of <span class="hlt">chondrules</span> are not surrounded by matrix-like rims. As summarized by Rubin and Krot (1995), there are reports of small textural and compositional differences between matrix lumps and mean matrix-like <span class="hlt">chondrule</span> rims, but there is so much overlap in properties between</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050173926','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050173926"><span>I-Xe Dating: The Time Line of <span class="hlt">Chondrule</span> Formation and Metamorphism in LL Chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pravdivtseva, O. V.; Hohenberg, C. M.; Meshik, A. P.</p> <p>2005-01-01</p> <p>Refractory inclusions, considered to be the oldest solids formed in the solar nebula. (4567.2 0.6 Ma) [1], are common in many carbonaceous and in some ordinary and enstatite chondrites. High-precision Pb- Pb ages for CAI s and <span class="hlt">chondrules</span> (from different meteorites) suggested that <span class="hlt">chondrule</span> formation appeared to have started about 2 Ma later than that of CAIs [1]. However, recent 26Al/26Mg data suggest simultaneous formation of CAI s and <span class="hlt">chondrules</span> in Allende [2]. The I-Xe ages of CAI s in Allende are about 2 Ma younger than the I-Xe ages of Allende <span class="hlt">chondrules</span> [3] but, like all chronometers, the I-Xe system records closure time of its particular host phase. In the case of Allende CAI s, the major iodine-bearing phase is sodalite, a secondary phase presumably formed by aqueous alteration, so I-Xe reflects the post-formational processes in these objects. In <span class="hlt">chondrules</span> the iodine host phases vary and can reflect formation and/or alteration but, to put <span class="hlt">chondrule</span> ages on a quantative basis, some problems should first be addressed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22667166-forming-chondrules-impact-splashes-ii-volatile-retention','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22667166-forming-chondrules-impact-splashes-ii-volatile-retention"><span>FORMING <span class="hlt">CHONDRULES</span> IN IMPACT SPLASHES. II. VOLATILE RETENTION</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>Dullemond, Cornelis Petrus; Harsono, Daniel; Stammler, Sebastian Markus</p> <p>2016-11-20</p> <p>Solving the mystery of the origin of <span class="hlt">chondrules</span> is one of the most elusive goals in the field of meteoritics. Recently, the idea of planet(esimal) collisions releasing splashes of lava droplets, long considered out of favor, has been reconsidered as a possible origin of <span class="hlt">chondrules</span> by several papers. One of the main problems with this idea is the lack of quantitative and simple models that can be used to test this scenario by directly comparing to the many known observables of <span class="hlt">chondrules</span>. In Paper I of this series, we presented a simple thermal evolution model of a spherically symmetric expandingmore » cloud of molten lava droplets that is assumed to emerge from a collision between two planetesimals. The production of lava could be either because the two planetesimals were already in a largely molten (or almost molten) state due to heating by {sup 26}Al, or due to impact jetting at higher impact velocities. In the present paper, number II of this series, we use this model to calculate whether or not volatile elements such as Na and K will remain abundant in these droplets or whether they will get depleted due to evaporation. The high density of the droplet cloud (e.g., small distance between adjacent droplets) causes the vapor to quickly reach saturation pressure and thus shuts down further evaporation. We show to what extent, and under which conditions, this keeps the abundances of these elements high, as is seen in <span class="hlt">chondrules</span>. We find that for most parameters of our model (cloud mass, expansion velocity, initial temperature) the volatile elements Mg, Si, and Fe remain entirely in the <span class="hlt">chondrules</span>. The Na and K abundances inside the droplets will initially stay mostly at their initial values due to the saturation of the vapor pressure, but at some point start to drop due to the cloud expansion. However, as soon as the temperature starts to decrease, most or all of the vapor recondenses again. At the end, the Na and K elements retain most of their initial abundances</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/10949294','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10949294"><span>Evaporation in the young solar nebula as the origin of 'just-right' melting of <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cohen; Hewins; Yu</p> <p>2000-08-10</p> <p><span class="hlt">Chondrules</span> are millimetre-sized, solidified melt spherules formed in the solar nebula by an early widespread heating event of uncertain nature. They were accreted into chondritic asteroids, which formed about 4.56 billion years ago and have not experienced melting or differentiation since that time. <span class="hlt">Chondrules</span> have diverse chemical compositions, corresponding to liquidus temperatures in the range 1,350-1,800 degrees C. Most <span class="hlt">chondrules</span>, however, show porphyritic textures (consisting of large crystals in a distinctly finer grained or glassy matrix), indicative of melting within the narrow range 0-50 degrees C below the liquidus. This suggests an unusual heating mechanism for <span class="hlt">chondrule</span> precursors, which would raise each individual <span class="hlt">chondrule</span> to just the right temperature (particular to individual bulk composition) in order to form porphyritic textures. Here we report the results of isothermal melting of a chondritic composition at nebular pressures. Our results suggest that evaporation stabilizes porphyritic textures over a wider range of temperatures below the liquidus (about 200 degrees C) than previously believed, thus removing the need for individual <span class="hlt">chondrule</span> temperature buffering. In addition, we show that evaporation explains many <span class="hlt">chondrule</span> bulk and mineral compositions that have hitherto been difficult to understand.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980037669','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980037669"><span>Partitioning of Moderately Siderophile Elements Among <span class="hlt">Olivine</span>, Silicate Melt, and Sulfide Melt: Constraints on Core Formation in the Earth and Mars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gaetani, Glenn A.; Grove, Timothy L.</p> <p>1997-01-01</p> <p>This study investigates the effects of Variations in the fugacities of oxygen and sulfur on the partitioning of first series transition metals (V, Cr, Mn, Fe, Co, Ni. and Cu) and W among coexisting sulfide melt, silicate melt, and <span class="hlt">olivine</span>. Experiments were performed at 1 atm pressure, 1350 C, with the fugacities of oxygen and sulfur controlled by mixing CO2, CO, and SO2 gases. Starting compositions consisted of a CaO-MgO-Al2O3-SiO2-FeO-Na2O analog for a <span class="hlt">barred</span> <span class="hlt">olivine</span> <span class="hlt">chondrule</span> from an ordinary chondrite and a synthetic komatiite. The f(sub O2)/f(sub S2), conditions ranged from log of f(sub O2) = -7.9 to - 10.6, with log of f(sub S2) values ranging from - 1.0 to -2.5. Our experimental results demonstrate that the f(sub O2)/f(sub S2) dependencies of sulfide melt/silicate melt partition coefficients for the first series transition metals arc proportional to their valence states. The f(sub O2)/f(sub S2) dependencies for the partitioning of Fe, Co, Ni, and Cu are weaker than predicted on the basis of their valence states. Variations in conditions have no significant effect on <span class="hlt">olivine</span>/melt partitioning other than those resulting from f(sub O2)-induced changes in the valence state of a given element. The strong f(sub O2)/f(sub S2) dependence for the <span class="hlt">olivine</span>/silicate melt partitioning of V is attributable to a change of valence state, from 4+ to 3+, with decreasing f(sub O2). Our experimentally determined partition coefficients are used to develop models for the segregation of sulfide and metal from the silicate portion of the early Earth and the Shergottite parent body (Mars). We find that the influence of S is not sufficient to explain the overabundance of siderophile and chalcophile elements that remained in the mantle of the Earth following core formation. Important constraints on core formation in Mars are provided by our experimental determination of the partitioning of Cu between silicate and sulfide melts. When combined with existing estimates for siderophile</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeCoA.191..118O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeCoA.191..118O"><span>Magnesium and 54Cr isotope compositions of carbonaceous chondrite <span class="hlt">chondrules</span> - Insights into early disk processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Olsen, Mia B.; Wielandt, Daniel; Schiller, Martin; Van Kooten, Elishevah M. M. E.; Bizzarro, Martin</p> <p>2016-10-01</p> <p>We report on the petrology, magnesium isotopes and mass-independent 54Cr/52Cr compositions (μ54Cr) of 42 <span class="hlt">chondrules</span> from CV (Vigarano and NWA 3118) and CR (NWA 6043, NWA 801 and LAP 02342) chondrites. All sampled <span class="hlt">chondrules</span> are classified as type IA or type IAB, have low 27Al/24Mg ratios (0.04-0.27) and display little or no evidence for secondary alteration processes. The CV and CR <span class="hlt">chondrules</span> show variable 25Mg/24Mg and 26Mg/24Mg values corresponding to a range of mass-dependent fractionation of ∼500 ppm (parts per million) per atomic mass unit. This mass-dependent Mg isotope fractionation is interpreted as reflecting Mg isotope heterogeneity of the <span class="hlt">chondrule</span> precursors and not the result of secondary alteration or volatility-controlled processes during <span class="hlt">chondrule</span> formation. The CV and CR <span class="hlt">chondrule</span> populations studied here are characterized by systematic deficits in the mass-independent component of 26Mg (μ26Mg∗) relative to the solar value defined by CI chondrites, which we interpret as reflecting formation from precursor material with a reduced initial abundance of 26Al compared to the canonical 26Al/27Al of ∼5 × 10-5. Model initial 26Al/27Al values of CV and CR <span class="hlt">chondrules</span> vary from (1.5 ± 4.0) × 10-6 to (2.2 ± 0.4) × 10-5. The CV <span class="hlt">chondrules</span> display significant μ54Cr variability, defining a range of compositions that is comparable to that observed for inner Solar System primitive and differentiated meteorites. In contrast, CR chondrites are characterized by a narrower range of μ54Cr values restricted to compositions typically observed for bulk carbonaceous chondrites. Collectively, these observations suggest that the CV <span class="hlt">chondrules</span> formed from precursors that originated in various regions of the protoplanetary disk and were then transported to the accretion region of the CV parent asteroid whereas CR <span class="hlt">chondrule</span> predominantly formed from precursor with carbonaceous chondrite-like μ54Cr signatures. The observed μ54Cr variability in <span class="hlt">chondrules</span> from CV</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017LPICo1963.2031S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017LPICo1963.2031S"><span>Nucleosynthetic and Mass-Dependent Titanium Isotope Variations in Individual <span class="hlt">Chondrules</span> of Ordinary Chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schönbächler, M.; Bauer, K. K.; Fehr, M. A.; Chaumard, N.; Zanda, B.</p> <p>2017-02-01</p> <p>We present evidence for nucleosynthetic Ti isotope heterogeneity between individual <span class="hlt">chondrules</span> of ordinary chondrites difficult to reconcile with <span class="hlt">chondrule</span> formation from molten planetesimals. Metamorphism resulted in stable Ti isotope fractionation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70022620','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70022620"><span>Bleached <span class="hlt">chondrules</span>: Evidence for widespread aqueous processes on the parent asteroids of ordinary chondrites</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Grossman, J.N.; Alexander, C.M. O'D.; Wang, Jingyuan; Brearley, A.J.</p> <p>2000-01-01</p> <p>We present the first detailed study of a population of texturally distinct <span class="hlt">chondrules</span> previously described by Kurat (1969), Christophe Michel-Levy (1976), and Skinner et al. (1989) that are sharply depleted in alkalis and Al in their outer portions. These 'bleached' <span class="hlt">chondrules</span>, which are exclusively radial pyroxene and cryptocrystalline in texture, have porous outer zones where mesostasis has been lost. Bleached <span class="hlt">chondrules</span> are present in all type 3 ordinary chondrites and are present in lower abundances in types 4-6. They are most abundant in the L and LL groups, apparently less common in H chondrites, and absent in enstatite chondrites. We used x-ray mapping and traditional electron microprobe techniques to characterize bleached <span class="hlt">chondrules</span> in a cross section of ordinary chondrites. We studied bleached <span class="hlt">chondrules</span> from Semarkona by ion microprobe for trace elements and H isotopes, and by transmission electron microscopy. <span class="hlt">Chondrule</span> bleaching was the result of low-temperature alteration by aqueous fluids flowing through fine-grained chondrite matrix prior to thermal metamorphism. During aqueous alteration, interstitial glass dissolved and was partially replaced by phyllosilicates, troilite was altered to pentlandite, but pyroxene was completely unaffected. Calcium-rich zones formed at the inner margins of the bleached zones, either as the result of the early stages of metamorphism or because of fluid-<span class="hlt">chondrule</span> reaction. The mineralogy of bleached <span class="hlt">chondrules</span> is extremely sensitive to thermal metamorphism in type 3 ordinary chondrites, and bleached zones provide a favorable location for the growth of metamorphic minerals in higher petrologic types. The ubiquitous presence of bleached <span class="hlt">chondrules</span> in ordinary chondrites implies that they all experienced aqueous alteration early in their asteroidal histories, but there is no relationship between the degree of alteration and metamorphic grade. A correlation between the oxidation state of chondrite groups and their degree of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840043308&hterms=evolution+inclusions&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Devolution%2Binclusions','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840043308&hterms=evolution+inclusions&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Devolution%2Binclusions"><span>Origin of spinel-rich <span class="hlt">chondrules</span> and inclusions in carbonaceous and ordinary chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kornacki, A. S.; Fegley, B., Jr.</p> <p>1984-01-01</p> <p>The evaluation of three models of the origin of spinel-rich <span class="hlt">chondrules</span> and inclusions presented here includes new calculations of the major-element refractory mineral condensation sequence from a gas of solar composition over a wide pressure interval. Condensation calculations show that spinel-rich <span class="hlt">chondrules</span> did not crystallize from metastable liquid condensates, and that spinel-rich inclusions are not aggregates of refractory nebular condensates. It is proposed that spinel-rich objects are fractionated distillation residues of small aggregates of primitive dust that lost Ca, Si-rich partial melts by evaporation, ablation, or splashing during collisions. This model also explains why spinel-rich <span class="hlt">chondrules</span> and inclusions (1) are usually smaller than melilite-rich <span class="hlt">chondrules</span> and inclusions; (2) often have highly fractionated trace-element compositions; and (3) usually do not contain Pt-metal nuggets even when they are more enriched in the Pt-group metals than nugget-bearing melilite-rich objects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950012885&hterms=role+playing&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Drole%2Bplaying','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950012885&hterms=role+playing&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Drole%2Bplaying"><span>The role of <span class="hlt">chondrules</span> in nebular fractionations of volatiles and other elements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Grossman, J. N.</p> <p>1994-01-01</p> <p>For at least 30 years, cosmochemists have been grappling with the question of how and why groups of geochemically and volatility related elements became fractionated in the major chondrite groups. At least five relatively independent fractionations are known. Virtually everyone who has thought about these facts has been attempted to attribute at least some of the fractionations to the physical separation or mixing of the visible components. By far the most abundant of these components in meteorites is <span class="hlt">chondrules</span>, and indeed <span class="hlt">chondrules</span> have long been suspected of playing a direct role in fractionation of volatile elements. The question addressed here is whether <span class="hlt">chondrules</span> formed before or after chemical components became separated is of fundamental importance to our understanding of the early solar system, as the answer constrains how, when, where, and from what <span class="hlt">chondrules</span> formed, and tells us about how materials were processed in the nebula.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170002376','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170002376"><span>A New Type of Foreign Clast in A Polymict Ureilite: A CAI or AL-Rich <span class="hlt">Chondrule</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Goodrich, C. A.; Ross, D. K.; Treiman, A. H.</p> <p>2017-01-01</p> <p>Introduction: Polymict ureilites are breccias interpreted to represent regolith formed on a ureilitic asteroid [1-3]. They consist of approximately 90-95% clasts of various ureilite types (<span class="hlt">olivine</span>-pyroxene rocks with Fo 75-95), a few % indigenous feldspathic clasts, and a few % foreign clasts [4-20]. The foreign clasts are diverse, including fragments of H, L, LL and R chondrites, angrites, other achondrites, and dark clasts similar to CC [6,7,9-19]. We report a new type of foreign clast in polymict ureilite DaG 999. Methods: Clast 8 in Dar al Gani (DaG) 999/1 (Museum fur Naturkunde) was discovered during a survey of feldspathic clasts in polymict ureilites [19,20]. It was studied by BEI, EMPA, and X-ray mapping on the JEOL 8530F electron microprobe at ARES, JSC. Petrography and Mineral Compositions: Clast 8 is sub-rounded to irregular in shape, approximately 85 micrometers in diameter, and consists of approximately 68% pyroxene and 32% mesostasis (by area). Part of the pyroxene (top half of clast in Fig. 1a and 2) shows a coarse dendritic morphology; the rest appears massive. Mesostasis may be glassy and contains fine needles/grains of pyroxene. The pyroxene has very high CaO (23.5 wt.%) and Al2O3 (19.7 wt.%), with the formula: (Ca(0.91)Mg(0.63)Fe(0.01)Al(sup VI) (0.38)Cr(0.01)Ti(0.05)1.99 Si2O6. The bulk mesostasis also has very high Al2O3 (approximately 26 wt.%). A bulk composition for the clast was obtained by combining modal abundances with phase compositions (Table 1, Fig. 3). Discussion: The pyroxene in clast 8 has a Ca-Al-(Ti)- rich (fassaitic) composition that is clearly distinct from compositions of pyroxenes in main group ureilites [22] or indigenous feldspathic clasts in polymict ureilites [4-8]. It also has significantly higher Al than fassaite in angrites (up to approximately 12 wt.% [23]), which occur as xenoliths in polymict ureilites. Ca-Al-Ti rich pyroxenes are most commonly found in CAIs, Al-rich <span class="hlt">chondrules</span> and other types of refractory</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030110823&hterms=diversity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddiversity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030110823&hterms=diversity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddiversity"><span>Al-rich <span class="hlt">Chondrules</span>: Petrologic Basis for Their Diversity, and Relation to Type C CAIs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>MacPherson, G. J.; Huss, G. R.</p> <p>2003-01-01</p> <p>Al-rich <span class="hlt">chondrules</span> share mineralogical and chemical properties with, and are intermediate in a volatility sense between, CAIs and ferromagnesian <span class="hlt">chondrules</span>. In some way they must be petrogenetic links between the two. A recent upsurge of interest in Al-rich <span class="hlt">chondrules</span> is due to their constituent plagioclase feldspar and Al-rich glass being amenable to successful ion microprobe searches for radiogenic Mg-26, the decay product of Al-26 (t(sub 1/2) = 720,000 y). This has allowed estimates to be made of the time duration between CAI formation and the onset of Al-rich (and possibly, by extension, ferromagnesian) <span class="hlt">chondrule</span> formation, on the order of 1.5-2.5 million years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4993235','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4993235"><span>Magnesium and 54Cr isotope compositions of carbonaceous chondrite <span class="hlt">chondrules</span> – Insights into early disk processes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Olsen, Mia B.; Wielandt, Daniel; Schiller, Martin; Van Kooten, Elishevah M.M.E.; Bizzarro, Martin</p> <p>2016-01-01</p> <p>We report on the petrology, magnesium isotopes and mass-independent 54Cr/52Cr compositions (μ54Cr) of 42 <span class="hlt">chondrules</span> from CV (Vigarano and NWA 3118) and CR (NWA 6043, NWA 801 and LAP 02342) chondrites. All sampled <span class="hlt">chondrules</span> are classified as type IA or type IAB, have low 27Al/24Mg ratios (0.04–0.27) and display little or no evidence for secondary alteration processes. The CV and CR <span class="hlt">chondrules</span> show variable 25Mg/24Mg and 26Mg/24Mg values corresponding to a range of mass-dependent fractionation of ~500 ppm (parts per million) per atomic mass unit. This mass-dependent Mg isotope fractionation is interpreted as reflecting Mg isotope heterogeneity of the <span class="hlt">chondrule</span> precursors and not the result of secondary alteration or volatility-controlled processes during <span class="hlt">chondrule</span> formation. The CV and CR <span class="hlt">chondrule</span> populations studied here are characterized by systematic deficits in the mass-independent component of 26Mg (μ26Mg*) relative to the solar value defined by CI chondrites, which we interpret as reflecting formation from precursor material with a reduced initial abundance of 26Al compared to the canonical 26Al/27Al of ~5 × 10−5. Model initial 26Al/27Al values of CV and CR <span class="hlt">chondrules</span> vary from (1.5 ± 4.0) × 10−6 to (2.2 ± 0.4) × 10−5. The CV <span class="hlt">chondrules</span> display significant μ54Cr variability, defining a range of compositions that is comparable to that observed for inner Solar System primitive and differentiated meteorites. In contrast, CR chondrites are characterized by a narrower range of μ54Cr values restricted to compositions typically observed for bulk carbonaceous chondrites. Collectively, these observations suggest that the CV <span class="hlt">chondrules</span> formed from precursors that originated in various regions of the protoplanetary disk and were then transported to the accretion region of the CV parent asteroid whereas CR <span class="hlt">chondrule</span> predominantly formed from precursor with carbonaceous chondrite-like μ54Cr signatures. The observed μ54Cr variability in <span class="hlt">chondrules</span> from</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('https://pubs.er.usgs.gov/publication/70029459','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70029459"><span>The onset of metamorphism in ordinary and carbonaceous chondrites</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Grossman, J.N.; Brearley, A.J.</p> <p>2005-01-01</p> <p>Ordinary and carbonaceous chondrites of the lowest petrologic types were surveyed by X-ray mapping techniques. A variety of metamorphic effects were noted and subjected to detailed analysis using electron microprobe, scanning electron microscopy (SEM), transmission electron microscopy (TEM), and cathodoluminescence (CL) methods. The distribution of Cr in FeO-rich <span class="hlt">olivine</span> systematically changes as metamorphism increases between type 3.0 and type 3.2. Igneous zoning patterns are replaced by complex ones and Cr-rich coatings develop on all grains. Cr distributions in <span class="hlt">olivine</span> are controlled by the exsolution of a Cr-rich phase, probably chromite. Cr in <span class="hlt">olivine</span> may have been partly present as tetrahedrally coordinated Cr3+. Separation of chromite is nearly complete by petrologic type 3.2. The abundance of <span class="hlt">chondrules</span> showing an inhomogeneous distribution of alkalis in mesostasis also increases with petrologic type. TEM shows this to be the result of crystallization of albite. Residual glass compositions systematically change during metamorphism, becoming increasingly rich in K. Glass in type I <span class="hlt">chondrules</span> also gains alkalis during metamorphism. Both types of <span class="hlt">chondrules</span> were open to an exchange of alkalis with opaque matrix and other <span class="hlt">chondrules</span>. The matrix in the least metamorphosed chondrites is rich in S and Na. The S is lost from the matrix at the earliest stages of metamorphism due to coalescence of minute grains. Progressive heating also results in the loss of sulfides from <span class="hlt">chondrule</span> rims and increases sulfide abundances in coarse matrix assemblages as well as inside <span class="hlt">chondrules</span>. Alkalis initially leave the matrix and enter <span class="hlt">chondrules</span> during early metamorphism. Feldspar subsequently nucleates in the matrix and Na re-enters from <span class="hlt">chondrules</span>. These metamorphic trends can be used to refine classification schemes for chondrites. Cr distributions in <span class="hlt">olivine</span> are a highly effective tool for assigning petrologic types to the most primitive meteorites and can be used to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170002226','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170002226"><span>Spinel-Bearing, Al-Rich Chrondrules in the Unequilibrated Ordinary Chondrite NWA7402</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ross, D. K.; Simon, J. I.; Cato, M. J.</p> <p>2017-01-01</p> <p>Several Al-rich <span class="hlt">chondrules</span> (ARCs) have been discovered in the unequilibrated ordinary chondrite NWA7402. Two of these three ARCs are spinel-bearing. Here we have characterized these unusual <span class="hlt">chondrules</span> with respect to their mineralogy and bulk compositions. These objects will be targets for future O and Mg isotope analysis. NWA7402 is clearly unequilibrated, with wide ranges of <span class="hlt">olivine</span> compositions in <span class="hlt">chondrules</span> (Fo99-Fo70, excluding rims). Chromium-oxide contents in <span class="hlt">olivine</span>, and Raman organic spectral parameters support the classification of this meteorite as petrologic type 3.1 [1]. NWA7402 is similar to, and could be paired with NWA5717, in that they both possess light and dark lithologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DPS....4831802M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DPS....4831802M"><span>Evolution of the Magnetic Field during <span class="hlt">Chondrule</span> Formation in Planetary Bow Shocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mai, Chuhong; Desch, Steven; Boley, Aaron C.</p> <p>2016-10-01</p> <p>Recent laboratory efforts (Fu et al., 2014, 2015) have constrained the remanent magnetizations of <span class="hlt">chondrules</span> and the magnetic field strengths they were exposed to as they cooled below their Curie points. An outstanding question is whether these fields represent the background magnetic field of the solar nebula or were unique to the <span class="hlt">chondrule</span>-forming environment. We investigate the amplification of the magnetic field above background values in a planetary bow shock, which is one proposed mechanism for <span class="hlt">chondrule</span> formation. We use a hydrodynamic code to model the temperature and pressure around a 3000 km-radius planetary embryo as it moves supersonically through the nebula gas. We calculate the ionization of hot, shocked gas considering thermionic emission of electrons and ions from grains and thermal ionization of potassium. We calculate the magnetic diffusion rate, including Ohmic dissipation and ambipolar diffusion (assuming a magnetic field strength comparable to 0.5 G). We compute the steady-state magnetic field around in the bow shock and find that behind the planet the field is amplified, but everywhere else it quickly diffuses out of the shocked region and recovers the background value. We consider the trajectories taken by <span class="hlt">chondrules</span> behind the shock and present likely values of the magnetic field amplification experienced by <span class="hlt">chondrules</span> as they cool after melting in the shock.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740005450','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740005450"><span>Artificial meteor ablation studies: <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Blanchard, M. B.; Cunningham, G. G.</p> <p>1973-01-01</p> <p>Artificial meteor ablation was performed on a Mg-rich <span class="hlt">olivine</span> sample using an arc-heated plasma of ionized air. Experimental conditions simulated a meteor traveling about 12 km/sec at an altitude of 70 km. The mineral content of the original <span class="hlt">olivine</span> sample was 98% <span class="hlt">olivine</span> (including traces of <span class="hlt">olivine</span> alteration products) and 2% chromite. Forsterite content of the original <span class="hlt">olivine</span> was Fo-89. After ablation, the forsterite content had increased to Fo-94 in the recrystallized <span class="hlt">olivine</span>. In addition, lamella-like intergrowths of magnetite were prevalent constituents. Wherever magnetite occurred, there was an increase in Mg and a corresponding decrease in Fe for the recrystallized <span class="hlt">olivine</span>. The Allende fusion crust consisted of a recrystallized <span class="hlt">olivine</span>, which was more Mg-rich and Fe-deficient than the original meteorite's <span class="hlt">olivine</span>, and abundant magnetite grains. Although troilite and pentlandite were the common opaque mineral constituents in this meteorite, magnetite was the principal opaque mineral found in the fusion crust.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008ApJ...685.1193B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008ApJ...685.1193B"><span>Gravitational Instabilities, <span class="hlt">Chondrule</span> Formation, and the FU Orionis Phenomenon</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boley, Aaron C.; Durisen, Richard H.</p> <p>2008-10-01</p> <p>Using analytic arguments and numerical simulations, we examine whether <span class="hlt">chondrule</span> formation and the FU Orionis phenomenon can be caused by the burstlike onset of gravitational instabilities (GIs) in dead zones. At least two scenarios for bursting dead zones can work, in principle. If the disk is on the verge of fragmentation, GI activation near r ~ 4-5 AU can produce <span class="hlt">chondrule</span>-forming shocks, at least under extreme conditions. Mass fluxes are also high enough during the onset of GIs to suggest that the outburst is related to an FU Orionis phenomenon. This situation is demonstrated by numerical simulations. In contrast, as supported by analytic arguments, if the burst takes place close to r ~ 1 AU, then even low pitch angle spiral waves can create <span class="hlt">chondrule</span>-producing shocks and outbursts. We also study the stability of the massive disks in our simulations against fragmentation and find that although disk evolution is sensitive to changes in opacity, the disks we study do not fragment, even at high resolution and even for extreme assumptions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070003472','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070003472"><span>Turbulent Size Selection and Concentration of <span class="hlt">Chondrule</span>-Sized Objects: Reynolds Number Invariance and Implications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cuzzi, J. N.; Hogan, R.; Dobrovolskis, A.; Paque, J.</p> <p>2006-01-01</p> <p>It is generally agreed that individual <span class="hlt">chondrules</span> formed as entities in a gaseous nebula prior to being accumulated into a meteorite parent body, within which they incur various forms of modification before arriving in our labs. While there are major unanswered questions about the properties of the nebula environment in which <span class="hlt">chondrules</span> formed, the process by which the most primitive meteorites are formed overwhelmingly from <span class="hlt">chondrules</span> must then be an aspect of "nebula processing". Textures in certain fragments of primitive meteorites might be summarized as being primarily <span class="hlt">chondrules</span> and clastic, <span class="hlt">chondrule</span>-sized, fragments of other minerals, each covered with a rim of fine dust with physical and chemical properties which are essentially independent of the composition and mineralogy of the underlying <span class="hlt">chondrule</span>. This (unfortunately rather rare) texture was called "primary accretionary texture" to reflect their belief that it precedes subsequent stages in which fragmentation, comminution, mixing, heating, and other forms of alteration occur on the parent body(-ies). The size distribution of these <span class="hlt">chondrules</span> and fragments, and the properties of their dusty rims, are key clues regarding the primary nebula accretion process. Even in the much more abundant meteorites which have clearly suffered internal mixing, abrasion, grinding, and even mineralogical alteration or replacement (due presumably to the collisional growth and heating process itself), key <span class="hlt">chondrule</span> properties such as mean size and density remain relatively well defined, and well defined rims persist in many cases. It has been our goal to infer the key nebula processes indirectly from the properties of these very earliest primitive meteorites by making use of a theoretical framework in which the nebula possesses a plausible level of isotropic turbulence. We have shown that turbulence has the property of concentrating one particular particle size by orders of magnitude, where the preferentially concentrated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-PIA16218.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-PIA16218.html"><span><span class="hlt">Olivine</span> on Earth</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2012-10-30</p> <p>The semi-precious gem peridot is a variety of <span class="hlt">olivine</span>. NASA Curiosity rover shows the diffraction signature, or fingerprint, of the mineral <span class="hlt">olivine</span>, shown here on Earth in the form of tumbled crystals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.201..303N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.201..303N"><span>26Al-26Mg systematics in <span class="hlt">chondrules</span> from Kaba and Yamato 980145 CV3 carbonaceous chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagashima, Kazuhide; Krot, Alexander N.; Komatsu, Mutsumi</p> <p>2017-03-01</p> <p>We report the mineralogy, petrography, and in situ measured 26Al-26Mg systematics in <span class="hlt">chondrules</span> from the least metamorphosed CV3 (Vigarano-type) chondrites, Kaba and Yamato (Y) 980145. Two Y 980145 <span class="hlt">chondrules</span> measured show no resolvable excesses in 26Mg (26Mg∗), a decay product of a short-lived (t1/2 ∼0.7 Ma) radionuclide 26Al. Plagioclase in one of the <span class="hlt">chondrules</span> is replaced by nepheline, indicative of thermal metamorphism. The lack of 26Mg∗ in the Y 980145 <span class="hlt">chondrules</span> is most likely due to disturbance of their 26Al-26Mg systematics during the metamorphism. Although Kaba experienced extensive metasomatic alteration (<300 °C), it largely avoided subsequent thermal metamorphism, and the 26Al-26Mg systematics of its <span class="hlt">chondrules</span> appear to be undisturbed. All eight Kaba <span class="hlt">chondrules</span> measured show 26Mg∗, corresponding to the initial 26Al/27Al ratios [(26Al/27Al)0] ranging from (2.9 ± 1.7) × 10-6 to (6.3 ± 2.7) × 10-6. If CV parent asteroid accreted rapidly after <span class="hlt">chondrule</span> formation, the inferred (26Al/27Al)0 ratios in Kaba <span class="hlt">chondrules</span> provide an upper limit on 26Al available in this asteroid at the time of its accretion. The estimated initial abundance of 26Al in the CV asteroid is too low to melt it and contradicts the existence of a molten core in this body suggested from the paleomagnetic records of Allende [Carporzen et al. (2011) Magnetic evidence for a partially differentiated carbonaceous chondrite parent body. Proc. Natl. Acad. Sci. USA108, 6386-6389] and Kaba [Gattacceca et al. (2013) More evidence for a partially differentiated CV parent body from the meteorite Kaba. Lunar Planet. Sci.44, abstract#1721].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654469-mixing-transport-dust-early-solar-nebula-inferred-from-titanium-isotope-variations-among-chondrules','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654469-mixing-transport-dust-early-solar-nebula-inferred-from-titanium-isotope-variations-among-chondrules"><span>Mixing and Transport of Dust in the Early Solar Nebula as Inferred from Titanium Isotope Variations among <span class="hlt">Chondrules</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>Gerber, Simone; Burkhardt, Christoph; Budde, Gerrit</p> <p>2017-05-20</p> <p><span class="hlt">Chondrules</span> formed by the melting of dust aggregates in the solar protoplanetary disk and as such provide unique insights into how solid material was transported and mixed within the disk. Here, we show that <span class="hlt">chondrules</span> from enstatite and ordinary chondrites show only small {sup 50}Ti variations and scatter closely around the {sup 50}Ti composition of their host chondrites. By contrast, <span class="hlt">chondrules</span> from carbonaceous chondrites have highly variable {sup 50}Ti compositions, which, relative to the terrestrial standard, range from the small {sup 50}Ti deficits measured for enstatite and ordinary chondrite <span class="hlt">chondrules</span> to the large {sup 50}Ti excesses known from Ca–Al-rich inclusionsmore » (CAIs). These {sup 50}Ti variations can be attributed to the addition of isotopically heterogeneous CAI-like material to enstatite and ordinary chondrite-like <span class="hlt">chondrule</span> precursors. The new Ti isotopic data demonstrate that isotopic variations among carbonaceous chondrite <span class="hlt">chondrules</span> do not require formation over a wide range of orbital distances, but can instead be fully accounted for by the incorporation of isotopically anomalous “nuggets” into <span class="hlt">chondrule</span> precursors. As such, these data obviate the need for disk-wide transport of <span class="hlt">chondrules</span> prior to chondrite parent body accretion and are consistent with formation of <span class="hlt">chondrules</span> from a given chondrite group in localized regions of the disk. Finally, the ubiquitous presence of {sup 50}Ti-enriched material in carbonaceous chondrites and the lack of this material in the non-carbonaceous chondrites support the idea that these two meteorite groups derive from areas of the disk that remained isolated from each other, probably through the formation of Jupiter.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70030455','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70030455"><span>Cotectic proportions of <span class="hlt">olivine</span> and spinel in <span class="hlt">olivine</span>-tholeiitic basalt and evaluation of pre-eruptive processes</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Roeder, Peter; Gofton, Emma; Thornber, Carl</p> <p>2006-01-01</p> <p>The volume %, distribution, texture and composition of coexisting <span class="hlt">olivine</span>, Cr-spinel and glass has been determined in quenched lava samples from Hawaii, Iceland and mid-oceanic ridges. The volume ratio of <span class="hlt">olivine</span> to spinel varies from 60 to 2800 and samples with >0·02% spinel have a volume ratio of <span class="hlt">olivine</span> to spinel of approximately 100. A plot of wt % MgO vs ppm Cr for natural and experimental basaltic glasses suggests that the general trend of the glasses can be explained by the crystallization of a cotectic ratio of <span class="hlt">olivine</span> to spinel of about 100. One group of samples has an <span class="hlt">olivine</span> to spinel ratio of approximately 100, with skeletal <span class="hlt">olivine</span> phenocrysts and small (<50 μm) spinel crystals that tend to be spatially associated with the <span class="hlt">olivine</span> phenocrysts. The large number of spinel crystals included within <span class="hlt">olivine</span> phenocrysts is thought to be due to skeletal <span class="hlt">olivine</span> phenocrysts coming into physical contact with spinel by synneusis during the chaotic conditions of ascent and extrusion. A second group of samples tend to have large <span class="hlt">olivine</span> phenocrysts relatively free of included spinel, a few large (>100 μm) spinel crystals that show evidence of two stages of growth, and a volume ratio of <span class="hlt">olivine</span> to spinel of 100 to well over 1000. The <span class="hlt">olivine</span> and spinel in this group have crystallized more slowly with little physical interaction, and show evidence that they have accumulated in a magma chamber.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008Icar..197..269M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008Icar..197..269M"><span>Origin of three-dimensional shapes of <span class="hlt">chondrules</span>. I. Hydrodynamics simulations of rotating droplet exposed to high-velocity rarefied gas flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miura, Hitoshi; Nakamoto, Taishi; Doi, Masao</p> <p>2008-09-01</p> <p>The origin of three-dimensional shapes of <span class="hlt">chondrules</span> is an important information to identify their formation mechanism in the early solar nebula. The measurement of their shapes by using X-ray computed topography suggested that they are usually close to perfect spheres, however, some of them have rugby-ball-like (prolate) shapes [Tsuchiyama, A., Shigeyoshi, R., Kawabata, T., Nakano, T., Uesugi, K., Shirono, S., 2003. Lunar Planet. Sci. 34, 1271-1272]. We considered that the prolate shapes reflect the deformations of <span class="hlt">chondrule</span> precursor dust particles when they are heated and melted in the high velocity gas flow. In order to reveal the origin of <span class="hlt">chondrule</span> shapes, we carried out the three-dimensional hydrodynamics simulations of a rotating molten <span class="hlt">chondrule</span> exposed to the gas flow in the framework of the shock-wave heating model for <span class="hlt">chondrule</span> formation. We adopted the gas ram pressure acting on the <span class="hlt">chondrule</span> surface of p=10 dyncm in a typical shock wave. Considering that the <span class="hlt">chondrule</span> precursor dust particle has an irregular shape before melting, the ram pressure causes a net torque to rotate the particle. The estimated angular velocity is ω=140 rads for the precursor radius of r=1 mm, though it has a different value depending on the irregularity of the shape. In addition, the rotation axis is likely to be perpendicular to the direction of the gas flow. Our calculations showed that the rotating molten <span class="hlt">chondrule</span> elongates along the rotation axis, in contrast, shrinks perpendicularly to it. It is a prolate shape. The reason why the molten <span class="hlt">chondrule</span> is deformed to a prolate shape was clearly discussed. Our study gives a complementary constraint for <span class="hlt">chondrule</span> formation mechanisms, comparing with conventional chemical analyses and dynamic crystallization experiments that have mainly constrained the thermal evolutions of <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930041163&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D60%26Ntt%3Dlindstrom','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930041163&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D60%26Ntt%3Dlindstrom"><span>Mineralogy, petrology and geochemistry of carbonaceous chondritic clasts in the LEW 85300 polymict eucrite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zolensky, M. E.; Hewins, R. H.; Mittlefehldt, D. W.; Lindstrom, M. M.; Xiao, X.; Lipschutz, M. E.</p> <p>1992-01-01</p> <p>We have performed a detailed petrologic and mineralogic study of two chondritic clasts from the polymict eucrite Lewis Cliff (LEW) 85300, and performed chemical analyses by INAA and RNAA on one of these. Petrologically, the clasts are identified and are composed of dispersed aggregates, <span class="hlt">chondrules</span>, and <span class="hlt">chondrule</span> fragments supported by matrix. The aggregates and <span class="hlt">chondrules</span> are composed of <span class="hlt">olivine</span>, orthopyroxene, plus some diopside. The matrix consists of fine-grained <span class="hlt">olivine</span>, and lesser orthopyroxene and augite. Fine-grained saponite is common in the matrix. The bulk major composition of the clast studied by INAA and RNAA shows unusual abundance patterns for lithophile, siderophile and chalcophile elements but is basically chondritic. The INAA/RNAA data preclude assignment of the LEW 85300,15 clast to any commonly accepted group of carbonaceous chondrite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V23B0484H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V23B0484H"><span>Internal Stratigraphy of the Palisades Sill <span class="hlt">Olivine</span> Zone: An <span class="hlt">Olivine</span> Slurry Emplaced in a Hot Sill</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haddad, J. R.; Naslund, H. R.</p> <p>2017-12-01</p> <p>The Palisades Sill is a 300 m thick Jurassic-Triassic sill-like sheet formed from a quartz-normative tholeiitic magma. Three geochemical reversals within the sill are the result of magma chamber recharges. This study focuses on the reversal at 10 m height, widely considered to be the result of the emplacement of an <span class="hlt">olivine</span>-rich slurry (Husch 1990, Gorring 1995). Major and trace elements were determined for 35 samples from the <span class="hlt">olivine</span> layer and adjacent sill spanning 10 m of stratigraphic height. Samples were collected from outcrops near the Ross Dock Picnic Area in Fort Lee, NJ. Mineral compositions were determined for 21 thin sections using an electron microprobe (EMP). Bulk rock chemistry shows that the base of the <span class="hlt">olivine</span> layer is between 2.5 and 3.25 m above the base of sampling. This is indicated by a marked reversal in Mg#, which jumped from 64.2 to 68.6; Al2O3, Co, Ni, Sc, Cs, Dy, and La also show clear reversals at the same interval. This is further collaborated by the formation of a ledge in the outcrop. Bulk chemistry and <span class="hlt">olivine</span> composition show no systematic changes within the <span class="hlt">olivine</span> layer. EMP analyses of augites reveals that below the 2.5 m height, crystals are typically strongly zoned, average rim Mg#= 67, core Mg#= 82. Above the 2.5 m layer, core Mg# are similar, but average rim Mg#=75. The plagioclase/augite ratio remains relatively constant through the <span class="hlt">olivine</span> layer, but the ratio of <span class="hlt">olivine</span> to plagioclase+augite is quite variable, suggesting that the <span class="hlt">olivine</span>-slurry was emplaced as an inhomogeneous mixture of <span class="hlt">olivine</span> + magma. Similar tholeiitic sills on Victoria Island, Canada, contain <span class="hlt">olivine</span>-rich basal layers in which the <span class="hlt">olivine</span> to plagioclase+augite ratio systematically increases, and the <span class="hlt">olivine</span> composition becomes systematically more Fe-rich, from the base to the top of the layer. Comparisons between these otherwise similar basal <span class="hlt">olivine</span>-rich layers, suggests that sills like the Palisades, which represents the injection of an <span class="hlt">olivine</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16107841','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16107841"><span>Young <span class="hlt">chondrules</span> in CB chondrites from a giant impact in the early Solar System.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Krot, Alexander N; Amelin, Yuri; Cassen, Patrick; Meibom, Anders</p> <p>2005-08-18</p> <p><span class="hlt">Chondrules</span>, which are the major constituent of chondritic meteorites, are believed to have formed during brief, localized, repetitive melting of dust (probably caused by shock waves) in the protoplanetary disk around the early Sun. The ages of primitive <span class="hlt">chondrules</span> in chondritic meteorites indicate that their formation started shortly after that of the calcium-aluminium-rich inclusions (4,567.2 +/- 0.7 Myr ago) and lasted for about 3 Myr, which is consistent with the dissipation timescale for protoplanetary disks around young solar-mass stars. Here we report the 207Pb-206Pb ages of <span class="hlt">chondrules</span> in the metal-rich CB (Bencubbin-like) carbonaceous chondrites Gujba (4,562.7 +/- 0.5 Myr) and Hammadah al Hamra 237 (4,562.8 +/- 0.9 Myr), which formed during a single-stage, highly energetic event. Both the relatively young ages and the single-stage formation of the CB <span class="hlt">chondrules</span> are inconsistent with formation during a nebular shock wave. We conclude that <span class="hlt">chondrules</span> and metal grains in the CB chondrites formed from a vapour-melt plume produced by a giant impact between planetary embryos after dust in the protoplanetary disk had largely dissipated. These findings therefore provide evidence for planet-sized objects in the earliest asteroid belt, as required by current numerical simulations of planet formation in the inner Solar System.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950055059&hterms=chromatic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dchromatic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950055059&hterms=chromatic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dchromatic"><span>The origin of chromitic <span class="hlt">chondrules</span> and the volatility of Cr under a range of nebular conditions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Krot, Alexander; Ivanova, Marina A.; Wasson, John T.</p> <p>1993-01-01</p> <p>We characterize ten chromatic <span class="hlt">chondrules</span>, two spinelian <span class="hlt">chondrules</span> andd one spinel-bearing <span class="hlt">chondrule</span> and summarize data for 120 chromitic inclusions discovered in an extensive survey of ordinary chondrites. Compositional and petrographic evidence suggests that chromitic <span class="hlt">chondrules</span> and inclusions are closely related. The Cr/(Cr + Al) ratios in the spinal of these objects range from 0.5 to 0.9 and bulk Al2O3 contents are uniformly high (greater than 10 wt%, except for one with 8 wt%). No other elements having comparable solar abundances are so stongly enriched, and alkali feldspar and merrillite are more common than in normal <span class="hlt">chondrules</span>. The Cr/Mg ratios in chromitic <span class="hlt">chondrules</span> are 180-750 times the ratios in the bulk chondrite. With the possible exception of magnetic clumping of chromite in the presolar cloud, mechanical processes cannot account for this enrichment. Examination of nebular equilibrium processes shows that 50%-condensation temperatures of Cr at pH2/pH2O of 1500 are several tens of degrees below those of Mg as Mg2SiO4; the condensation of Cr is primarily as MgCr2O4 dissolved in MgAl2O4 at nebular pressures of 10(exp -4) atm or below. At pH2 = 10(exp -3) atm condesation as Cr in Fe-Ni is favored. Making the nebula much more oxidizing reduces the difference in condensation temperatures but Mg remains more refractory. We conclude that nebular equilibrium processes are not responsible for the enhanced Cr/Mg ratios. We propose that both Cr and Al became enriched in residues formed by incomplete evaporation of presolar lumps. We suggest that spinals remained as solid phases when the bulk of the silicates were incorporated into the evaporating melt; vaporization of Al and Cr were inhibited by the slow kinetics of diffusion. Subsequent melting and crystallization of these residues fractionated Cr from Al. The resulting materials constituted major components in the precursors of chromitic <span class="hlt">chondrules</span>. Our model implies that chromitic <span class="hlt">chondrules</span> and inclusions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950012905&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D50%26Ntt%3Dlindstrom','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950012905&hterms=lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D50%26Ntt%3Dlindstrom"><span>Mn-Cr isotopic systematics of Chainpur <span class="hlt">chondrules</span> and bulk ordinary chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nyquist, L.; Lindstrom, D.; Wiesmann, H.; Bansal, B.; Shih, C.-Y.; Mittlefehldt, D.; Martinez, R.; Wentworth, S.</p> <p>1994-01-01</p> <p>We report on ongoing study of the Mn-Cr systematics of individual Chainpur (LL3.4) <span class="hlt">chondrules</span> and compare the results to those for bulk ordinary chondrites. Twenty-eight <span class="hlt">chondrules</span> were surveyed for abundances of Mn, Cr, Na, Fe, Sc, Hf, Ir, and Zn by INAA. Twelve were chosen for SEM/EDX and high-precision Cr-isotopic studies on the basis of LL-chondrite-normalized Mn(LL), Sc(LL), (Mn/Fe)(LL), and (Sc/Fe)(LL) as well as their Mn/Cr ratios. Classification into textural types follows from SEM/EDX examination of interior surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050162284','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050162284"><span>Petrographic Evidence for Rapid Heating and Cooling During Chrondrule Formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wasson, J. T.</p> <p>2004-01-01</p> <p>The <span class="hlt">chondrule</span> cooling rates used in most <span class="hlt">chondrule</span>-formation models appear to be too low. Recent petrographic evidence indicates that the amount of crystal (especially <span class="hlt">olivine</span>) growth that occurred after the last melting event was about 30 smaller than the grain sizes simulated in order to estimate cooling rates. The smaller amount of growth leads to an upwards revision of cooling rates by about a factor of 1000. Most <span class="hlt">chondrules</span> are porphyritic. They consist of large and small crystals of <span class="hlt">olivine</span> and, less commonly, pyroxene immersed in a mesostasis having a plagioclase-rich composition. In the most primitive chondrites the mesostasis is often vitreous. Because the large majority of <span class="hlt">chondrules</span> contain FeS, it is clear that the nebula had cooled below the FeS condensation temperature (ca. 650 K) before <span class="hlt">chondrule</span> formation occurred. The high FeO/(FeO+MgO) ratios of some <span class="hlt">chondrules</span> require still lower nebular temperatures (less than 500 K). The traditional view has been that porphyritic <span class="hlt">chondrules</span> formed in a single heating/cooling event and many laboratory experiments have been carried out in various kinds of kinds of furnaces to try to simulate the formation of <span class="hlt">chondrules</span> textures in a single heating/cooling cycle. These furnace experiments have been used to infer the cooling rates of <span class="hlt">chondrules</span> during the temperature range at which <span class="hlt">olivine</span> crystallized from the melt. Most of these inferred values are in the range 0.01-1 K per second. These low cooling rates are problematical because there is no long-term nebular environment that yields such values. In transparent regions <span class="hlt">chondrules</span> would cool at rates orders of magnitude higher, whereas in an opaque nebular disk the cooling rates would be many orders of magnitude lower. And these latter conditions are not suitable locations for <span class="hlt">chondrule</span> formation because such high temperatures would cause the complete evaporation of <span class="hlt">chondrules</span> (which have melting temperatures about 600 K higher than their evaporation temperatures</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.469...75A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.469...75A"><span>Testing the <span class="hlt">chondrule</span>-rich accretion model for planetary embryos using calcium isotopes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Amsellem, Elsa; Moynier, Frédéric; Pringle, Emily A.; Bouvier, Audrey; Chen, Heng; Day, James M. D.</p> <p>2017-07-01</p> <p>Understanding the composition of raw materials that formed the Earth is a crucial step towards understanding the formation of terrestrial planets and their bulk composition. Calcium is the fifth most abundant element in terrestrial planets and, therefore, is a key element with which to trace planetary composition. However, in order to use Ca isotopes as a tracer of Earth's accretion history, it is first necessary to understand the isotopic behavior of Ca during the earliest stages of planetary formation. Chondrites are some of the oldest materials of the Solar System, and the study of their isotopic composition enables understanding of how and in what conditions the Solar System formed. Here we present Ca isotope data for a suite of bulk chondrites as well as Allende (CV) <span class="hlt">chondrules</span>. We show that most groups of carbonaceous chondrites (CV, CI, CR and CM) are significantly enriched in the lighter Ca isotopes (δ 44 / 40 Ca = + 0.1 to + 0.93 ‰) compared with bulk silicate Earth (δ 44 / 40 Ca = + 1.05 ± 0.04 ‰, Huang et al., 2010) or Mars, while enstatite chondrites are indistinguishable from Earth in Ca isotope composition (δ 44 / 40 Ca = + 0.91 to + 1.06 ‰). <span class="hlt">Chondrules</span> from Allende are enriched in the heavier isotopes of Ca compared to the bulk and the matrix of the meteorite (δ 44 / 40 Ca = + 1.00 to + 1.21 ‰). This implies that Earth and Mars have Ca isotope compositions that are distinct from most carbonaceous chondrites but that may be like <span class="hlt">chondrules</span>. This Ca isotopic similarity between Earth, Mars, and <span class="hlt">chondrules</span> is permissive of recent dynamical models of planetary formation that propose a <span class="hlt">chondrule</span>-rich accretion model for planetary embryos.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910046580&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=19910046580&hterms=iodine&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Diodine"><span>Iodine-xenon studies of petrographically and chemically characterized Chainpur <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Swindle, T. D.; Caffee, M. W.; Hohenberg, C. M.; Lindstrom, M. M.; Taylor, G. J.</p> <p>1991-01-01</p> <p>INAA, noble gas, and petrographic studies conducted on samples of 18 <span class="hlt">chondrules</span> and matric material from the Chainpur (LL3) indicate that the I-129/I-127 ratio, R(0), varies by a factor of more than 10 among the <span class="hlt">chondrules</span>. This corresponds to a greater-than-50 Ma span in apparent I-Xe ages. Models which invoke either gas-dust mixing or nebular heterogeneity cannot satisfactorily explain these data, any more than can hypotheses which attribute the variations to differences in formation age, metamorphic rate, or time of aqueous alteration. It is alternatively suggested that the variations represent periods of low-grade shock events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015A%26A...579A..43C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015A%26A...579A..43C"><span>How to form planetesimals from mm-sized <span class="hlt">chondrules</span> and <span class="hlt">chondrule</span> aggregates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carrera, Daniel; Johansen, Anders; Davies, Melvyn B.</p> <p>2015-07-01</p> <p>The size distribution of asteroids and Kuiper belt objects in the solar system is difficult to reconcile with a bottom-up formation scenario due to the observed scarcity of objects smaller than ~100 km in size. Instead, planetesimals appear to form top-down, with large 100-1000 km bodies forming from the rapid gravitational collapse of dense clumps of small solid particles. In this paper we investigate the conditions under which solid particles can form dense clumps in a protoplanetary disk. We used a hydrodynamic code to model the interaction between solid particles and the gas inside a shearing box inside the disk, considering particle sizes from submillimeter-sized <span class="hlt">chondrules</span> to meter-sized rocks. We found that particles down to millimeter sizes can form dense particle clouds through the run-away convergence of radial drift known as the streaming instability. We made a map of the range of conditions (strength of turbulence, particle mass-loading, disk mass, and distance to the star) that are prone to producing dense particle clumps. Finally, we estimate the distribution of collision speeds between mm-sized particles. We calculated the rate of sticking collisions and obtain a robust upper limit on the particle growth timescale of ~105 years. This means that mm-sized <span class="hlt">chondrule</span> aggregates can grow on a timescale much smaller than the disk accretion timescale (~106-107 years). Our results suggest a pathway from the mm-sized grains found in primitive meteorites to fully formed asteroids. We speculate that asteroids may form from a positive feedback loop in which coagualation leads to particle clumping driven by the streaming instability. This clumping, in turn, reduces collision speeds and enhances coagulation. Future simulations should model coagulation and the streaming instability together to explore this feedback loop further. Appendices are available in electronic form at http://www.aanda.org</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://ntrs.nasa.gov/search.jsp?R=20020046273&hterms=reproduction&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dreproduction','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020046273&hterms=reproduction&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dreproduction"><span>Experimental Reproduction of Type 1B <span class="hlt">Chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lofgren, G. E.; Le, L.</p> <p>2002-01-01</p> <p>We have replicated type 1B <span class="hlt">chondrule</span> textures and compositions with crystallization experiments in which UOC material was melted at 1400 deg.C and cooled at 5-1000 deg.C/hr using graphite crucibles in evacuated silica tubes to provide a reducing environment. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.479..108X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.479..108X"><span>Disequilibrium growth of <span class="hlt">olivine</span> in mafic magmas revealed by phosphorus zoning patterns of <span class="hlt">olivine</span> from mafic-ultramafic intrusions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xing, Chang-Ming; Wang, Christina Yan; Tan, Wei</p> <p>2017-12-01</p> <p><span class="hlt">Olivine</span> from mafic-ultramafic intrusions rarely displays growth zoning in major and some minor elements, such as Fe, Mg and Ni, due to fast diffusion of these elements at high temperatures. These elements in <span class="hlt">olivine</span> are thus not useful in deciphering magma chamber processes, such as magma convection, multiple injection and mixing. High-resolution X-ray elemental intensity mapping reveals distinct P zoning patterns of <span class="hlt">olivine</span> from two mafic-ultramafic intrusions in SW China. Polyhedral <span class="hlt">olivine</span> grains from lherzolite and dunite of the Abulangdang intrusion show P-rich dendrites similar to those observed in volcanic rocks. Rounded <span class="hlt">olivine</span> grains from net-textured Fe-Ti oxide ores of the Baima layered intrusion have irregular P-rich patches/bands crosscut and interlocked by P-poor <span class="hlt">olivine</span> domains. P-rich patches/bands contain 250 to 612 ppm P, much higher than P-poor <span class="hlt">olivine</span> domains with 123 to 230 ppm P. In electron backscattered diffraction (EBSD) maps, P-rich patches/bands within a single <span class="hlt">olivine</span> grain have the same crystallographic orientation, indicating that they were remnants of the same crystal. Thus, both P-rich patches/bands and P-poor <span class="hlt">olivine</span> domains in the same grain show a disequilibrium texture and clearly record two-stage growth. The P-rich patches/bands are likely the remnants of a polyhedral <span class="hlt">olivine</span> crystal that formed in the first stage, whereas the P-poor <span class="hlt">olivine</span> domains containing rounded Ti-rich magnetite and Fe-rich melt inclusions may have formed from an Fe-rich ambient melt in the second stage. The complex P zoning of <span class="hlt">olivine</span> can be attributed to the dissolution of early polyhedral <span class="hlt">olivine</span> and re-precipitation from the Fe-rich ambient melt. The early polyhedral <span class="hlt">olivine</span> was in chemical disequilibrium with the ambient melt that may have been developed by silicate liquid immiscibility in a crystal mush. Our study implies that <span class="hlt">olivine</span> crystals in igneous cumulates with an equilibrium appearance may have experienced disequilibrium growth processes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.213..618R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.213..618R"><span>Cosmogenic He and Ne in <span class="hlt">chondrules</span> from clastic matrix and a lithic clast of Murchison: No pre-irradiation by the early sun</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Riebe, My E. I.; Huber, Liliane; Metzler, Knut; Busemann, Henner; Luginbuehl, Stefanie M.; Meier, Matthias M. M.; Maden, Colin; Wieler, Rainer</p> <p>2017-09-01</p> <p>Whether or not some meteorites retain a record of irradiation by a large flux of energetic particles from the early sun in the form of excesses of cosmic-ray produced noble gases in individual crystals or single <span class="hlt">chondrules</span> is a topic of ongoing debate. Here, we present He and Ne isotopic data for individual <span class="hlt">chondrules</span> in Murchison, a chondritic regolith breccia of the CM group. We separated 27 <span class="hlt">chondrules</span> from a clastic matrix portion and 26 <span class="hlt">chondrules</span> from an adjacent single so-called "primary accretionary rock" (Metzler et al., 1992). All <span class="hlt">chondrules</span> from the primary rock fragment are expected to share a common irradiation history, whereas <span class="hlt">chondrules</span> from the clastic matrix were stirred in the regolith independently of each other. All "primary rock <span class="hlt">chondrules</span>" and 23 of the "matrix <span class="hlt">chondrules</span>" have very similar concentrations of cosmogenic 3He and 21Ne, corresponding to a cosmic-ray exposure age to galactic cosmic rays (GCR) of ∼1.3-1.9 Ma, in the range of Murchison's meteoroid exposure age determined with cosmogenic radionuclides. Four clastic matrix <span class="hlt">chondrules</span> contain excesses of cosmogenic 3He and 21Ne, corresponding to nominal 4π exposure ages of ∼4-∼29 Ma, with a Ne isotopic composition as expected for production by GCR. If the fraction of excess cosmogenic gas bearing <span class="hlt">chondrules</span> in the primary rock and clastic matrix were the same, we would expect this result with a statistical probability of only 0.5 - 2.7%. Therefore, the exposure age distributions for Murchison <span class="hlt">chondrules</span> in primary rock and clastic matrix are very likely different. Such a difference is expected if the excess cosmogenic gas was acquired by some of the matrix <span class="hlt">chondrules</span> in the regolith, but not if <span class="hlt">chondrules</span> were irradiated in the solar nebula by the early sun before they accreted on the Murchison parent body. Therefore, Murchison does not provide evidence for irradiation by a high fluence of energetic particles from the early sun. By inference, this statement likely holds for the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940016235&hterms=ccc&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dccc','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940016235&hterms=ccc&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dccc"><span>Oxygen isotopic relationships between the LEW85332 carbonaceous chondrite and CR chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Prinz, M.; Weisberg, M. K.; Clayton, R. N.; Mayeda, T. K.</p> <p>1993-01-01</p> <p>LEW85332, originally described as a unique C3 chondrite, was shown to be a C2 chondrite with important linkages to the CR clan. An important petrologic aspect of LEW85332 is that it contains anhydrous <span class="hlt">chondrules</span> and hydrated matrix, and new oxygen isotopic data on <span class="hlt">chondrules</span>, matrix and whole rock are consistent with the petrology. <span class="hlt">Chondrules</span> fall on the equilibrated chondrite line (ECL), with a slope near 1, which goes through ordinary chondrite <span class="hlt">chondrules</span>. This contrasts with the CR <span class="hlt">chondrule</span> line which has a lower slope due to hydrated components. LEW85332 <span class="hlt">chondrules</span> define a new carbonaceous chondrite <span class="hlt">chondrule</span> line, parallel to the anhydrous CV <span class="hlt">chondrule</span> line (CCC), consistent with the well-established concept of two oxygen isotopic reservoirs. Matrix and whole rock fall on the CR line. The whole rock composition indicates that the chondrite is dominated by <span class="hlt">chondrules</span>, and that most of them contain light oxygen similar to that of anhydrous <span class="hlt">olivine</span> and pyroxene separates in the Renazzo and Al Rais CR chondrites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950060235&hterms=corona+discharge&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcorona%2Bdischarge','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950060235&hterms=corona+discharge&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dcorona%2Bdischarge"><span>Electrical discharge heating of <span class="hlt">chondrules</span> in the solar nebula</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Love, Stanley G.; Keil, Klaus; Scott, Edward R. D.</p> <p>1995-01-01</p> <p>We present a rudimentary theoretical assessment of electrical discharge heating as a candidate mechanism for the formation of <span class="hlt">chondrules</span> in the solar nebula. The discharge model combines estimates of the properties of the nebula, a mechanism for terrestrial thunderstorm electrification, and some fundamental electrical properties of gases. Large uncertainties in the model inputs limit these calculations to order-or-magnitude accuracy. Despite the uncertainty, it is possible to estimate an upper limit to the efficiency of nebular discharges at melting millimeter-sized stony objects. We find that electrical arcs analogous to terrestrial lightning could have occurred in the nebula, but that under most conditions these discharges probably could not have melted <span class="hlt">chondrules</span>. Despite our difficulties, we believe the topic worthy of further investigation and suggest some experiments which could improve our understanding of nebular discharges.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005occ..book.....S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005occ..book.....S"><span>The Origin of <span class="hlt">Chondrules</span> and Chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sears, Derek W. G.</p> <p>2005-01-01</p> <p>Drawing on research from the various scientific disciplines involved, this text summarizes the origin and history of <span class="hlt">chondrules</span> and chondrites. Including citations to every published paper on the topic, it forms a comprehensive bibliography of the latest research. In addition, extensive illustrations provide a clear visual representation of the scientific theories. The text will be a valuable reference for graduate students and researchers in planetary science, geology and astronomy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V43C0545S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V43C0545S"><span>Raman and FTIR spectroscopy of methane in <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, A.; Oze, C.; Rossman, G. R.; Celestian, A. J.</p> <p>2017-12-01</p> <p><span class="hlt">Olivine</span> has been proposed to be a direct source of methane (CH4) in serpentinization systems and experiments. Here, Raman and Fourier Transform Infrared (FTIR) spectroscopy were used to verify the presence and abundance of CH4 in <span class="hlt">olivine</span> samples from nine localities, including the San Carlos <span class="hlt">olivine</span>. Raman analyses did not identify any methane in the <span class="hlt">olivine</span> samples. As <span class="hlt">olivine</span> is orthorhombic, three polarized FTIR spectra were obtained for the <span class="hlt">olivine</span> samples. No methane was detected in any of the <span class="hlt">olivine</span> samples using FTIR. Overall, <span class="hlt">olivine</span> investigated in this study does not appear to be a primary source of methane.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150001926','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150001926"><span>Mineralogical Comparison of <span class="hlt">Olivine</span> in Shergottites and A Shocked L Chondrite: Implications for Shock Histories of Brown <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Takenouchi, A.; Mikouchi, T.; Yamaguchi, A.; Zolensky, M. E.</p> <p>2015-01-01</p> <p>Most Martian meteorites are heavily shocked, exhibiting numerous shock features, for example undulatory extinction of <span class="hlt">olivine</span> and pyroxene, the presence of diaplectic glass ("maskelynite") and the formation of shock melt. Among these shock features, <span class="hlt">olivine</span> darkening ("brown" <span class="hlt">olivine</span>) is unique in Martian meteorites because no other meteorite group shows such a feature. Although the presence of brown <span class="hlt">olivine</span> in shergottites was reported thirty years ago, detailed observation by TEM has not been performed until the NWA 2737 chassignite was discovered, whose <span class="hlt">olivine</span> is darkened, being completely black in hand specimen. Fe metal nano-particles were found in NWA 2737 <span class="hlt">olivine</span> which are considered to have been formed by <span class="hlt">olivine</span> reduction during heavy shock. Subsequently, magnetite nano-particles were also found in other Martian meteorites and the coexistence of Fe metal and magnetite nano-particles was reported in the NWA 1950 shergottite and some Fe metal nano-particles were mantled by magnetite. Therefore, the formation process of nano-particles seems to be complex. Because "brown" <span class="hlt">olivine</span> is unique to Martian meteorites, they have a potential to constrain their shock conditions. In order to better understand the shock history of Martian meteorites, we compared <span class="hlt">olivine</span> in several shergottites with that in a highly-shocked L chondrite which contains ringwoodite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015E%26PSL.424..119B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015E%26PSL.424..119B"><span>The ascent of kimberlite: Insights from <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brett, R. C.; Russell, J. K.; Andrews, G. D. M.; Jones, T. J.</p> <p>2015-08-01</p> <p><span class="hlt">Olivine</span> xenocrysts are ubiquitous in kimberlite deposits worldwide and derive from the disaggregation of mantle-derived peridotitic xenoliths. Here, we provide descriptions of textural features in xenocrystic <span class="hlt">olivine</span> from kimberlite deposits at the Diavik Diamond Mine, Canada and at Igwisi Hills volcano, Tanzania. We establish a relative sequence of textural events recorded by <span class="hlt">olivine</span> during magma ascent through the cratonic mantle lithosphere, including: xenolith disaggregation, decompression fracturing expressed as mineral- and fluid-inclusion-rich sealed and healed cracks, grain size and shape modification by chemical dissolution and abrasion, late-stage crystallization of overgrowths on <span class="hlt">olivine</span> xenocrysts, and lastly, mechanical milling and rounding of the <span class="hlt">olivine</span> cargo prior to emplacement. Ascent through the lithosphere operates as a "kimberlite factory" wherein progressive upward dyke propagation of the initial carbonatitic melt fractures the overlying mantle to entrain and disaggregate mantle xenoliths. Preferential assimilation of orthopyroxene (Opx) xenocrysts by the silica-undersaturated carbonatitic melt leads to deep-seated exsolution of CO2-rich fluid generating buoyancy and supporting rapid ascent. Concomitant dissolution of <span class="hlt">olivine</span> produces irregular-shaped relict grains preserved as cores to most kimberlitic <span class="hlt">olivine</span>. Multiple generations of decompression cracks in <span class="hlt">olivine</span> provide evidence for a progression in ambient fluid compositions (e.g., from carbonatitic to silicic) during ascent. Numerical modelling predicts tensile failure of xenoliths (disaggregation) and <span class="hlt">olivine</span> (cracks) over ascent distances of 2-7 km and 15-25 km, respectively, at velocities of 0.1 to >4 m s-1. Efficient assimilation of Opx during ascent results in a silica-enriched, <span class="hlt">olivine</span>-saturated kimberlitic melt (i.e. SiO2 >20 wt.%) that crystallizes overgrowths on partially digested and abraded <span class="hlt">olivine</span> xenocrysts. <span class="hlt">Olivine</span> saturation is constrained to occur at pressures <1 GPa; an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014M%26PS...49.1440E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014M%26PS...49.1440E"><span>Crystallization kinetics of <span class="hlt">olivine</span>-phyric shergottites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ennis, Megan E.; McSween, Harry Y.</p> <p>2014-08-01</p> <p>Crystal size distribution (CSD) and spatial distribution pattern (SDP) analyses are applied to the early crystallizing phases, <span class="hlt">olivine</span> and pyroxene, in <span class="hlt">olivine</span>-phyric shergottites (Elephant moraine [EET] 79001A, Dar al Gani [DaG] 476, and dhofar [Dho] 019) from each sampling locality inferred from Mars ejection ages. Trace element zonation patterns (P and Cr) in <span class="hlt">olivine</span> are also used to characterize the crystallization history of these Martian basalts. Previously reported 2-D CSDs for these meteorites are re-evaluated using a newer stereographically corrected methodology. Kinks in the <span class="hlt">olivine</span> CSD plots suggest several populations that crystallized under different conditions. CSDs for pyroxene in DaG 476 and EET 79001A reveal single populations that grew under steady-state conditions; pyroxenes in Dho 019 were too intergrown for CSD analysis. Magma chamber residence times of several days for small grains to several months for <span class="hlt">olivine</span> megacrysts are calculated using the CSD slopes and growth rates inferred from previous experimental data. Phosphorus imaging in <span class="hlt">olivines</span> in DaG 476 and Dho 019 indicate rapid growth of skeletal, sector-zoned, or patchy cores, probably in response to delayed nucleation, followed by slow growth, and finally rapid dendritic growth with back-filling to form oscillatory zoning in rims. SPD analyses indicate that <span class="hlt">olivine</span> and pyroxene crystals grew or accumulated in clusters rather than as randomly distributed grains. These data reveal complex solidification histories for Martian basalts, and are generally consistent with the formation at depth of <span class="hlt">olivine</span> megacryst cores, which were entrained in ascending magmas that crystallized pyroxenes, small <span class="hlt">olivines</span>, and oscillatory rims on megacrysts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014LPICo1800.5005P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014LPICo1800.5005P"><span>2D Size Distribution of <span class="hlt">Chondrules</span> and Chondritic Fragments of an Ordinary Chondrite from Lut Desert (Iran)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pourkhorsandi, H.; Mirnejad, H.</p> <p>2014-09-01</p> <p>2D size measurement of <span class="hlt">chondrules</span> and chondiritic fragments of a meteorite from Lut desert of Iran is conducted. <span class="hlt">Chondrules</span> exhibit a size range of 55-1800 µm (average 437 µm). Chondiritic fragments show a size range of 46-1220 µm (average 261 µm).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22521549-planetary-embryo-bow-shocks-mechanism-chondrule-formation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22521549-planetary-embryo-bow-shocks-mechanism-chondrule-formation"><span>PLANETARY EMBRYO BOW SHOCKS AS A MECHANISM FOR <span class="hlt">CHONDRULE</span> FORMATION</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>Mann, Christopher R.; Boley, Aaron C.; Morris, Melissa A.</p> <p>2016-02-20</p> <p>We use radiation hydrodynamics with direct particle integration to explore the feasibility of <span class="hlt">chondrule</span> formation in planetary embryo bow shocks. The calculations presented here are used to explore the consequences of a Mars-size planetary embryo traveling on a moderately excited orbit through the dusty, early environment of the solar system. The embryo’s eccentric orbit produces a range of supersonic relative velocities between the embryo and the circularly orbiting gas and dust, prompting the formation of bow shocks. Temporary atmospheres around these embryos, which can be created via volatile outgassing and gas capture from the surrounding nebula, can non-trivially affect thermalmore » profiles of solids entering the shock. We explore the thermal environment of solids that traverse the bow shock at different impact radii, the effects that planetoid atmospheres have on shock morphologies, and the stripping efficiency of planetoidal atmospheres in the presence of high relative winds. Simulations are run using adiabatic and radiative conditions, with multiple treatments for the local opacities. Shock speeds of 5, 6, and 7 km s{sup −1} are explored. We find that a high-mass atmosphere and inefficient radiative conditions can produce peak temperatures and cooling rates that are consistent with the constraints set by <span class="hlt">chondrule</span> furnace studies. For most conditions, the derived cooling rates are potentially too high to be consistent with <span class="hlt">chondrule</span> formation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ASPC..341..839B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ASPC..341..839B"><span>The Three-Dimensionality of Spiral Shocks: Did <span class="hlt">Chondrules</span> Catch a Breaking Wave?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boley, A. C.; Durisen, R. H.; Pickett, M. K.</p> <p>2005-12-01</p> <p>Spiral shocks in vertically stratified disks lead to hydraulic/shock-jumps (hs-jumps) that stimulate large scale (tenths of an AU or more) radial and vertical motions, breaking surface waves, high-altitude shocks, and vortical flows. These effects are demonstrated by three-dimensional hydrodynamics simulations in Solar Nebula models. Trajectories of fluid elements, along with their thermal histories, suggest that hs-jumps mix the nebular gas and provide diverse pre-shock conditions, some of which are conducive to <span class="hlt">chondrule</span> formation. In addition, hs-jumps may provide an energy source for driving nebular turbulence to size-sort <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70014409','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014409"><span>ALH85085: a unique volatile-poor carbonaceous chondrite with possible implications for nebular fractionation processes</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Grossman, J.N.; Rubin, A.E.; MacPherson, G.J.</p> <p>1988-01-01</p> <p>Allan Hills 85085 is a unique chondrite with affinities to the Al Rais-Renazzo clan of carbonaceous chondrites. Its constituents are less than 50 ??m in mean size. <span class="hlt">Chondrules</span> and microchondrules of all textures are present; nonporphyritic <span class="hlt">chondrules</span> are unusually abundant. The mean compositions of porphyritic, nonporphyritic and <span class="hlt">barred</span> <span class="hlt">olivine</span> <span class="hlt">chondrules</span> resemble those in ordinary chondrites except that they are depleted in volatile elements. Ca-, Al-rich inclusions are abundant and largely free of nebular alteration; they comprise types similar to those in CM and CO chondrites, as well as unique types. Calcium dialuminate occurs in several inclusions. Metal, silicate and sulfide compositions are close to those in CM-CO chondrites and Al Rais and Renazzo. C1-chondrite clasts and metal-rich "reduced" clasts are present, but opaque matrix is absent. Siderophile abundances in ALH85085 are extremely high (e.g., Fe Si = 1.7 ?? solar), and volatiles are depleted (e.g., Na Si = 0.25 ?? solar, S Si = 0.03 ?? solar). Nonvolatile lithophile abundances are similar to those in Al Rais, Renazzo, and CM and CO chondrites. ALH85085 agglomerated when temperatures in the nebula were near 1000 K, in the same region where Renazzo, Al Rais and the CI chondrites formed. Agglomeration of high-temperature material may thus be a mechanism by which the fractionation of refractory lithophiles occurred in the nebula. <span class="hlt">Chondrule</span> formation must have occurred at high temperatures when clumps of precursors were small. After agglomeration, ALH85085 was annealed and lightly shocked. C1 and other clasts were subsequently incorporated during late-stage brecciation. ?? 1988.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020046214&hterms=Sulfur&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DSulfur','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020046214&hterms=Sulfur&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DSulfur"><span>Sulfur Isotope Composition of Putative Primary Troilite in <span class="hlt">Chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tachibana, Shogo; Huss, Gary R.</p> <p>2002-01-01</p> <p>Sulfur isotope compositions of putative primary troilites in <span class="hlt">chondrules</span> from Bishunpur were measured by ion probe. These primary troilites have the same S isotope compositions as matrix troilites and thus appear to be isotopically unfractionated. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993Metic..28R.378K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993Metic..28R.378K"><span>Aqueous Alteration of the Grosnaja CV3 Carbonaceous Chondrite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Keller, L. P.; McKay, D. S.</p> <p>1993-07-01</p> <p>Previous petrographic studies have shown that aqueous alteration products are locally well developed in some of the CV3 falls [e.g., 1-3]. In this abstract, we describe our transmission electron microscope (TEM) study of the extent of aqueous alteration in matrix and in <span class="hlt">chondrules</span> in the Grosnaja CV3 carbonaceous chondrite. Grosnaja is an observed fall and belongs to the oxidized subgroup of the CV chondrites [4]. We obtained fragments of Grosnaja from the Naturhistorisches Museum in Vienna. Regions of interest were extracted from polished thin sections and prepared for TEM observation by ion milling. Quantitative energy-dispersive X-ray (EDX) analyses were obtained using a JEOL 2000FX TEM equipped with a LINK thin- window EDX detector. Grosnaja has undergone aqueous alteration, which has resulted in the formation of phyllosilicates in matrix and in <span class="hlt">chondrules</span>. The suprising result from Grosnaja is that three different types of phyllosilicates are intimately intergrown. Serpentine is the most abundant phyllosilicate in matrix and occurs as fine-grained packets along grain boundaries and as fracture-fillings and veinlets that cross cut <span class="hlt">olivine</span> and pyroxene grains. Mixed with the serpentine are packets of fine-grained phyllosilicates with a distinct 1.4-nm basal spacing that is probably a chlorite group mineral. Rare packets of smectite occur as epitaxial intergrowths with <span class="hlt">olivine</span>, but are not interstratified with serpentine as observed in the CI chondrites. Phyllosilicates in Grosnaja matrix occur with Mg-rich carbonates, fine-grained magnetite, chromite and pentlandite, and poorly-crystalline FeNi- oxide/hydroxides, which stain the matrix a brownish-red color. Some of the rust may be of terrestrial origin (Grosnaja fell in 1861). Although the matrix phyllosilicates are too small to obtain single-phase chemical analyses in the TEM, quantitative EDX analyses suggest that the serpentine contains significant Fe (Mg/Mg + Fe ~0.5). The serpentine/chlorite forms as an</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130010925','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130010925"><span>A New Spinel-<span class="hlt">Olivine</span> Oxybarometer: Near-Liquidus Partitioning of V between <span class="hlt">Olivine</span>-Melt, Spinel-Melt, and Spinel-<span class="hlt">Olivine</span> in Martian Basalt Composition Y980459 as a Function of Oxygen Fugacity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Papike, J. J.; Le, L.; Burger, P. V.; Shearer, C. K.; Bell, A. S.; Jones, J.</p> <p>2013-01-01</p> <p>Our research on valence state partitioning began in 2005 with a review of Cr, Fe, Ti, and V partitioning among crystallographic sites in <span class="hlt">olivine</span>, pyroxene, and spinel [1]. That paper was followed by several on QUE94201 melt composition and specifically on Cr, V, and Eu partitioning between pyroxene and melt [2-5]. This paper represents the continuation of our examination of the partitioning of multivalent V between <span class="hlt">olivine</span>, spinel, and melt in martian <span class="hlt">olivine</span>-phyric basalts of Y980459 composition [6, 7]. Here we introduce a new, potentially powerful oxybarometer, V partitioning between spinel and <span class="hlt">olivine</span>, which can be used when no melt is preserved in the meteorite. The bulk composition of QUE94201 was ideal for our study of martian pyroxene-phyric basalts and specifically the partitioning between pyroxene-melt for Cr, V, and Eu. Likewise, bulk composition Y980459 is ideal for the study of martian <span class="hlt">olivine</span>-phyric basalts and specifically for <span class="hlt">olivine</span>-melt, spinel-melt, and spinel-<span class="hlt">olivine</span> partitioning of V as a function of oxygen fugacity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150001936','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150001936"><span>Early Size Distributions of <span class="hlt">Chondrule</span> Subgroups Overprinted by the Final Accumulation Process of Particle Components in Allende</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McCain, K. A.; Simon, J. I.; Cuzzi, J. N</p> <p>2015-01-01</p> <p>Populations of compositionally distinct particles are fundamental components of undifferentiated chondritic meteorites. Many theories explain the formation of chondrites, one class of which includes mechanisms for sorting the component particles in the solar nebula prior to their accretion. Mechanisms include sorting by mass, turbulent concentration, X-winds, and photophoresis, which will produce characteristic distributions of observable properties such as particle size. Distinguishing processes that occur in specific astrophysical environments requires characterization of particle types, which include refractory Ca-Al-rich Inclusions (CAIs) and less-refractory <span class="hlt">chondrules</span>. Previous investigations of modal abundances of CAIs and <span class="hlt">chondrules</span> exist, but differences within and between these two groups, both of which are made up of diverse subgroups with different thermal histories and chemical compositions, remain mostly unstudied. The presence of rims, a significant event occurring after the formation of at least some <span class="hlt">chondrules</span>, have also yet to be considered with respect to sorting. Here we present the sizes of CAIs and <span class="hlt">chondrules</span> in Allende with attention to the smallest sizes, subgroups, and particle rims.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR42A..04F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR42A..04F"><span>Site-specific hydration and dehydration of San Carlos <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferriss, E.; Plank, T. A.; Walker, D.</p> <p>2016-12-01</p> <p>Hydrogen incorporation and diffusion in <span class="hlt">olivine</span> is critical to understanding fundamental Earth processes such as mantle rheology, plate tectonics, melt generation and magma ascent. Interpreting measured H profiles in <span class="hlt">olivine</span> requires a more comprehensive understanding of H point defect reactions than currently exists because H diffusivity (D) ranges over 6 orders of magnitude, from slow diffusing H incorporated as (4H+)Si­ [1] to rapid `proton-polaron' bulk H diffusion [2]. Here we present the first experiments on H diffusing into and then out of Fe-bearing <span class="hlt">olivine</span> using the whole-block method [3], which allows a finely-resolved time series of H profiles in 3 crystallographic directions using the same sample for all dehydration steps. A piece of nearly-dry, oriented San Carlos <span class="hlt">olivine</span> was hydrated in a piston cylinder apparatus using H2O and solid buffers of Ni/NiO and San Carlos <span class="hlt">olivine</span> and enstatite at 800 °C and 10 kbar for 17.5 hours, just long enough to saturate the `proton-polaron' mechanism. The sample was then dehydrated in a CO/CO2 gas-mixing furnace at 800°C and 10-14 <span class="hlt">bar</span> fO2 for total heating times of 1, 3, 7, 13, 19, 43, and 68 hrs, at which point most, but not all, of the H had left the crystal. FTIR profiles at 1, 3, and 7 hours show bulk H profiles consistent with `proton-polaron' diffusion. Later the pace of dehydration slowed, and in several cases the bulk H profile shape differed from what would be expected during simple diffusive loss. The small peak at 3600 cm-1, (4H+)Si, remained essentially unchanged throughout all experiments. The peak at 3573 cm-1, (Ti4+)Mg(2H+)Mg, was initially present but tiny, grew to become the largest peak after hydration, and then during dehydration returned to its initial height. The apparent diffusivity of this peak during hydration and the initial stages of dehydration is 4 orders of magnitude faster than the same peak in synthetic forsterite [2]. Peaks at 3542, 3525, 3489, and 3480 cm-1 were not present</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1114889-water-carbon-dioxide-adsorption-olivine-surfaces','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1114889-water-carbon-dioxide-adsorption-olivine-surfaces"><span>Water and Carbon Dioxide Adsorption at <span class="hlt">Olivine</span> Surfaces</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>Kerisit, Sebastien N.; Bylaska, Eric J.; Felmy, Andrew R.</p> <p>2013-11-14</p> <p>Plane-wave density functional theory (DFT) calculations were performed to simulate water and carbon dioxide adsorption at the (010) surface of five <span class="hlt">olivine</span> minerals, namely, forsterite (Mg2SiO4), calcio-<span class="hlt">olivine</span> (Ca2SiO4), tephroite (Mn2SiO4), fayalite (Fe2SiO4), and Co-<span class="hlt">olivine</span> (Co2SiO4). Adsorption energies per water molecule obtained from energy minimizations varied from -78 kJ mol-1 for fayalite to -128 kJ mol-1 for calcio-<span class="hlt">olivine</span> at sub-monolayer coverage and became less exothermic as coverage increased. In contrast, carbon dioxide adsorption energies at sub-monolayer coverage ranged from -20 kJ mol-1 for fayalite to -59 kJ mol-1 for calcio-<span class="hlt">olivine</span>. Therefore, the DFT calculations show a strong driving force for carbonmore » dioxide displacement by water at the surface of all <span class="hlt">olivine</span> minerals in a competitive adsorption scenario. Additionally, adsorption energies for both water and carbon dioxide were found to be more exothermic for the alkaline-earth (AE) <span class="hlt">olivines</span> than for the transition-metal (TM) <span class="hlt">olivines</span> and to not correlate with the solvation enthalpies of the corresponding divalent cations. However, a correlation was obtained with the charge of the surface divalent cation indicating that the more ionic character of the AE cations in the <span class="hlt">olivine</span> structure relative to the TM cations leads to greater interactions with adsorbed water and carbon dioxide molecules at the surface and thus more exothermic adsorption energies for the AE <span class="hlt">olivines</span>. For calcio-<span class="hlt">olivine</span>, which exhibits the highest divalent cation charge of the five <span class="hlt">olivines</span>, ab initio molecular dynamics simulations showed that this effect leads both water and carbon dioxide to react with the surface and form hydroxyl groups and a carbonate-like species, respectively.« less</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('https://pubs.er.usgs.gov/publication/70011043','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70011043"><span>Geobarometry of ultramafic xenoliths from Loihi Seamount, Hawaii, on the basis of CO2 inclusions in <span class="hlt">olivine</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>Roedder, E.</p> <p>1983-01-01</p> <p>Abundant fluid inclusions in <span class="hlt">olivine</span> of dunite xenoliths (???1-3 cm) in basalt dredged from the young Loihi Seamount, 30 km southeast of Hawaii, are evidence for three coexisting immiscible fluid phases-silicate melt (now glass), sulfide melt (now solid), and dense supercritical CO2 (now liquid + gas)-during growth and later fracturing of some of these <span class="hlt">olivine</span> crystals. Some <span class="hlt">olivine</span> xenocrysts, probably from disaggregation of xenoliths, contain similar inclusions. Most of the inclusions (2-10 ??m) are on secondary planes, trapped during healing of fractures after the original crystal growth. Some such planes end abruptly within single crystals and are termed pseudosecondary, because they formed during the growth of the host <span class="hlt">olivine</span> crystals. The "vapor" bubble in a few large (20-60 ??m), isolated, and hence primary, silicate melt inclusions is too large to be the result of simple differential shrinkage. Under correct viewing conditions, these bubbles are seen to consist of CO2 liquid and gas, with an aggregate ??{variant} = ??? 0.5-0.75 g cm-3, and represent trapped globules of dense supercritical CO2 (i.e., incipient "vesiculation" at depth). Some spinel crystals enclosed within <span class="hlt">olivine</span> have attached CO2 blebs. Spherical sulfide blebs having widely variable volume ratios to CO2 and silicate glass are found in both primary and pseudosecondary inclusions, demonstrating that an immiscible sulfide melt was also present. Assuming <span class="hlt">olivine</span> growth at ??? 1200??C and hydrostatic pressure from a liquid lava column, extrapolation of CO2 P-V-T data indicates that the primary inclusions were trapped at ??? 220-470 MPa (2200-4700 <span class="hlt">bars</span>), or ??? 8-17 km depth in basalt magma of ??{variant} = 2.7 g cm-3. Because the temperature cannot change much during the rise to eruption, the range of CO2 densities reveals the change in pressure from that during original <span class="hlt">olivine</span> growth to later deformation and rise to eruption on the sea floor. The presence of numerous decrepitated inclusions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1430963-hf-chronology-cr-chondrites-implications-timescales-chondrule-formation-distribution-solar-nebula','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1430963-hf-chronology-cr-chondrites-implications-timescales-chondrule-formation-distribution-solar-nebula"><span>Hf-W chronology of CR chondrites: Implications for the timescales of <span class="hlt">chondrule</span> formation and the distribution of 26Al in the solar nebula</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>Budde, Gerrit; Kruijer, Thomas S.; Kleine, Thorsten</p> <p></p> <p>The CR chondrites are distinct from most other chondrites in having younger <span class="hlt">chondrule</span> 26Al- 26Mg ages, but the significance of these ages and whether they reflect true formation times or a heterogeneous distribution of 26Al are not well understood. To better determine the timescales of CR <span class="hlt">chondrule</span> formation and CR chondrite parent body accretion, we obtained Hf-W isotopic data for metal, silicate, and <span class="hlt">chondrule</span> separates from four CR chondrites. We also obtained Mo isotopic data for the same samples, to assess potential genetic links among the components of CR chondrites, and between these components and bulk chondrites. The isotopic datamore » demonstrate that metal and silicate in CR chondrites exhibit distinct nucleosynthetic W and Mo isotope anomalies, caused by the heterogeneous distribution of a single presolar s-process carrier. These isotope signatures are akin to the complementary anomalies found previously for <span class="hlt">chondrules</span> and matrix in CV chondrites and indicate that the major components of CR chondrites are genetically linked and formed from a common reservoir of solar nebula dust. The obtained Hf-W age of 3.6±0.6 million years (Ma) after the formation of Ca-Al-rich inclusions (CAIs) most likely dates metal-silicate separation during <span class="hlt">chondrule</span> formation and is consistent with Al-Mg and Pb-Pb ages for CR <span class="hlt">chondrules</span>, indicating that CR <span class="hlt">chondrules</span> formed ~1–2 Ma later than <span class="hlt">chondrules</span> from most other chondrite groups. Moreover, chemical, isotopic, and chronological data imply close temporal link between <span class="hlt">chondrule</span> formation and chondrite accretion, making the CR chondrite parent body one of the youngest meteorite parent bodies. Such a late accretion at ~3.6 Ma after CAIs is consistent with isotopic composition of CR chondrites (e.g., 15N/ 14N) that is indicative of a formation at a larger heliocentric distance, probably beyond the orbit of Jupiter. As such, the accretion age of the CR parent body provides the earliest possible time at which Jupiter could</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1430963-hf-chronology-cr-chondrites-implications-timescales-chondrule-formation-distribution-solar-nebula','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1430963-hf-chronology-cr-chondrites-implications-timescales-chondrule-formation-distribution-solar-nebula"><span>Hf-W chronology of CR chondrites: Implications for the timescales of <span class="hlt">chondrule</span> formation and the distribution of 26Al in the solar nebula</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Budde, Gerrit; Kruijer, Thomas S.; Kleine, Thorsten</p> <p>2017-10-24</p> <p>The CR chondrites are distinct from most other chondrites in having younger <span class="hlt">chondrule</span> 26Al- 26Mg ages, but the significance of these ages and whether they reflect true formation times or a heterogeneous distribution of 26Al are not well understood. To better determine the timescales of CR <span class="hlt">chondrule</span> formation and CR chondrite parent body accretion, we obtained Hf-W isotopic data for metal, silicate, and <span class="hlt">chondrule</span> separates from four CR chondrites. We also obtained Mo isotopic data for the same samples, to assess potential genetic links among the components of CR chondrites, and between these components and bulk chondrites. The isotopic datamore » demonstrate that metal and silicate in CR chondrites exhibit distinct nucleosynthetic W and Mo isotope anomalies, caused by the heterogeneous distribution of a single presolar s-process carrier. These isotope signatures are akin to the complementary anomalies found previously for <span class="hlt">chondrules</span> and matrix in CV chondrites and indicate that the major components of CR chondrites are genetically linked and formed from a common reservoir of solar nebula dust. The obtained Hf-W age of 3.6±0.6 million years (Ma) after the formation of Ca-Al-rich inclusions (CAIs) most likely dates metal-silicate separation during <span class="hlt">chondrule</span> formation and is consistent with Al-Mg and Pb-Pb ages for CR <span class="hlt">chondrules</span>, indicating that CR <span class="hlt">chondrules</span> formed ~1–2 Ma later than <span class="hlt">chondrules</span> from most other chondrite groups. Moreover, chemical, isotopic, and chronological data imply close temporal link between <span class="hlt">chondrule</span> formation and chondrite accretion, making the CR chondrite parent body one of the youngest meteorite parent bodies. Such a late accretion at ~3.6 Ma after CAIs is consistent with isotopic composition of CR chondrites (e.g., 15N/ 14N) that is indicative of a formation at a larger heliocentric distance, probably beyond the orbit of Jupiter. As such, the accretion age of the CR parent body provides the earliest possible time at which Jupiter could</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810810G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810810G"><span><span class="hlt">Olivine</span> and spinel fabric development in lineated peridotites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>German, Lindsey; Newman, Julie; Chatzaras, Vasileios; Kruckenberg, Seth; Stewart, Eric; Tikoff, Basil</p> <p>2016-04-01</p> <p>Investigation of <span class="hlt">olivine</span> and spinel fabrics in lineated harzburgites from the Red Hills peridotite massif, New Zealand, reveals that the spinel grain population records the same orientation of the principal finite strain axes as <span class="hlt">olivine</span> grains, however, <span class="hlt">olivine</span> grains generally record stronger fabric anisotropy. Further, <span class="hlt">olivine</span> crystallographic preferred orientation (CPO) reflects the constrictional kinematic context of these rocks. In these harzburgites, deformed at ~1200 °C and >6 kbar, spinel grains are variably oriented and display weak to no CPO. Shape fabric in spinels, determined using X-ray computed tomography (XRCT) indicates a range of geometries (L>S, L=S and L<S ellipsoids), with the shape factor ranging from -0.30 (prolate fabric) to +0.55 (oblate fabric). <span class="hlt">Olivine</span> grains (mean diameter: 0.13 - 0.27 mm) exhibit evidence for dislocation creep, including subgrains, undulose extinction and a strong shape preferred orientation, with long axes parallel or subparallel to the mean spinel long axis orientation derived from XRCT. <span class="hlt">Olivine</span> fabric analyses, carried out using Image SXM on grain traces from optical photomicrographs of two mutually perpendicular thin sections from each sample, yield moderately to strongly prolate fabrics (L>S tectonites) for <span class="hlt">olivine</span> in all samples. CPO, plotted with respect to lineation and foliation as defined by XRCT analyses of spinel grains, is characterized by [100] maxima parallel or subparallel to the lineation; [010] and [001] form girdles perpendicular to the lineation, consistent with the D-type CPO for <span class="hlt">olivine</span>. <span class="hlt">Olivine</span> CPO is typically interpreted in the context of deformation conditions (e.g., temperature, stress) based on experimental studies. However, the D-type CPO for <span class="hlt">olivine</span> is generally associated with deformation at relatively lower temperatures than suggested by the mineral compositions in these rocks. Our data suggest that <span class="hlt">olivine</span> CPO may not only respond to deformation conditions, but may be controlled by the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910025734&hterms=hanford&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dhanford','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910025734&hterms=hanford&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dhanford"><span><span class="hlt">Chondrule</span>-like objects and brown glasses in howardites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Olsen, Edward J.; Fredriksson, Kurt; Rajan, Sundar; Noonan, Albert</p> <p>1990-01-01</p> <p>Chondrulelike objects and brown glasses were analyzed in the howardites, Bununu, Malvern, Monticello, Pavlovka, and Yamato 7308. The objects are very similar to <span class="hlt">chondrules</span> in ordinary and carbonaceous chondrites. Like the brown glasses, the chondrulelike objects could have been produced by impact melting that left some crystalline nuclei, followed by a slower cooling rate than for the glasses. Alternatively, these objects are <span class="hlt">chondrules</span> implanted from chondrite impactors. They are, however, without rims or any adhering matrix. The brown glasses appear to represent melting of average regolithic surface material, except for Monticello and Y7308, both of which have some siliceous glasses. The siliceous glasses could not have been produced by vapor fractionation but by melting of differentiated lithologies such as fayalitic granites. Impact mechanics indicates that howardites with abundant brown glasses came from an asteroid larger than Vesta (greater than 400 km radius), upon which impacts occurred at relative velocities of up to 5 km/s. Howardites with little or no brown glasses came from a smaller parent body. It is concluded that at least two parent bodies are likely sources for the basaltic achondrites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Litho.260..356K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Litho.260..356K"><span>The fate of <span class="hlt">olivine</span> in the lower crust: Pseudomorphs after <span class="hlt">olivine</span> in coronitic metagabbro from the Grenville Orogen, Ontario</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kendrick, J. L.; Jamieson, R. A.</p> <p>2016-09-01</p> <p>Orthopyroxene-oxide symplectites after <span class="hlt">olivine</span> are among the most enigmatic features of corona assemblages in metagabbros. Two coronitic metagabbro bodies from the Algonquin suite in the Grenville Orogen, Ontario, contain exceptionally well preserved orthopyroxene + Fe-Ti oxide symplectite formed during prograde Ottawan (ca. 1060 Ma) granulite-facies metamorphism. Based on textural evidence, we propose a new hypothesis for the formation of these symplectites. Under oxidising conditions associated with fluid infiltration, magmatic <span class="hlt">olivine</span> and ilmenite underwent a coupled reaction whereby magnetite produced by oxidation of <span class="hlt">olivine</span> replaced adjacent igneous ilmenite. Ilmenite was re-precipitated as a fine-grained intergrowth with orthopyroxene and some magnetite in the former <span class="hlt">olivine</span> sites. This hypothesis is supported by textural evidence showing partial replacement of magmatic ilmenite by magnetite and a close spatial association between magmatic oxides and orthopyroxene + Fe-Ti oxide symplectite, which locally radiates from ilmenite into <span class="hlt">olivine</span>. Measured orthopyroxene/oxide ratios in the symplectite (20-35% oxides) agree with the ratio predicted from the proposed reaction (ca. 30%). Coronas and pseudomorphs formed during high-grade metamorphism, with increasing fO2 interpreted to result from fluid infiltration at near-peak conditions of ca. 13 kbar, 800 °C. The same samples contain red-brown fine-grained aggregates interpreted as iddingsite pseudomorphs after <span class="hlt">olivine</span>. Raman spectroscopy suggests that the iddingsite consists largely of amorphous silica and Fe-hydroxide; textural evidence indicates that it formed by late-stage oxidation and hydration of <span class="hlt">olivine</span> that survived earlier metamorphism. The unusual co-occurrence of granulite-facies pseudomorphs after <span class="hlt">olivine</span> with an alteration product formed at near-surface conditions indicates that some <span class="hlt">olivine</span> may survive protracted high-grade metamorphism in environments where fluid access is limited.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016LPICo1921.6503B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016LPICo1921.6503B"><span>Titanium and Oxygen Isotope Compositions of Individual <span class="hlt">Chondrules</span> from Ordinary Chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bauer, K. K.; Schönbächler, M.; Fehr, M. A.; Vennemann, T.; Chaumard, N.; Zanda, B.</p> <p>2016-08-01</p> <p>We measured Ti and triple-O isotope compositions of individual <span class="hlt">chondrules</span> (characterized by CT scanning) from ordinary chondrites. We will discuss correlations between Ti and ∆17O and their implication for the origin of nucleosynthetic anomalies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110005555','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110005555"><span>High Precision Oxygen Three Isotope Analysis of Wild-2 Particles and Anhydrous Chondritic Interplanetary Dust Particles</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nakashima, D.; Ushikubo, T.; Zolensky, Michael E.; Weisberg, M. K.; Joswiak, D. J.; Brownlee, D. E.; Matrajt, G.; Kita, N. T.</p> <p>2011-01-01</p> <p>One of the most important discoveries from comet Wild-2 samples was observation of crystalline silicate particles that resemble <span class="hlt">chondrules</span> and CAIs in carbonaceous chondrites. Previous oxygen isotope analyses of crystalline silicate terminal particles showed heterogeneous oxygen isotope ratios with delta(sup 18)O to approx. delta(sup 17)O down to -50% in the CAI-like particle Inti, a relict <span class="hlt">olivine</span> grain in Gozen-sama, and an <span class="hlt">olivine</span> particle. However, many Wild-2 particles as well as ferromagnesian silicates in anhydrous interplanetary dust particles (IDPs) showed Delta(sup 17)O values that cluster around -2%. In carbonaceous chondrites, <span class="hlt">chondrules</span> seem to show two major isotope reservoirs with Delta(sup 17)O values at -5% and -2%. It was suggested that the Delta(sup 17)O = -2% is the common oxygen isotope reservoir for carbonaceous chondrite <span class="hlt">chondrules</span> and cometary dust, from the outer asteroid belt to the Kuiper belt region. However, a larger dataset with high precision isotope analyses (+/-1-2%) is still needed to resolve the similarities or distinctions among Wild-2 particles, IDPs and <span class="hlt">chondrules</span> in meteorites. We have made signifi-cant efforts to establish routine analyses of small particles (< or =10micronsm) at 1-2% precision using IMS-1280 at WiscSIMS laboratory. Here we report new results of high precision oxygen isotope analyses of Wild-2 particles and anhydrous chondritic IDPs, and discuss the relationship between the cometary dust and carbonaceous chondrite <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4946626','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4946626"><span>Pb-Pb dating of individual <span class="hlt">chondrules</span> from the CBa chondrite Gujba: Assessment of the impact plume formation model</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bollard, Jean; Connelly, James N.; Bizzarro, Martin</p> <p>2016-01-01</p> <p>The CB chondrites are metal-rich meteorites with characteristics that sharply distinguish them from other chondrite groups. Their unusual chemical and petrologic features and a young formation age of bulk <span class="hlt">chondrules</span> dated from the CBa chondrite Gujba are interpreted to reflect a single-stage impact origin. Here, we report high-precision internal isochrons for four individual <span class="hlt">chondrules</span> of the Gujba chondrite to probe the formation history of CB chondrites and evaluate the concordancy of relevant short-lived radionuclide chronometers. All four <span class="hlt">chondrules</span> define a brief formation interval with a weighted mean age of 4562.49 ± 0.21 Myr, consistent with its origin from the vapor-melt impact plume generated by colliding planetesimals. Formation in a debris disk mostly devoid of nebular gas and dust sets an upper limit for the solar protoplanetary disk lifetime at 4.8 ± 0.3 Myr. Finally, given the well-behaved Pb-Pb systematics of all four <span class="hlt">chondrules</span>, a precise formation age and the concordancy of the Mn-Cr, Hf-W, and I-Xe short-lived radionuclide relative chronometers, we propose that Gujba may serve as a suitable time anchor for these systems. PMID:27429545</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160003881','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160003881"><span>An Amoeboid <span class="hlt">Olivine</span> Aggregate in LEW 85300</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Komatsu, M. D.; Yamaguchi, A.; Fagan, T. J.; Zolensky, M. E.; Shiran, N.; Mikouchi, T.</p> <p>2016-01-01</p> <p>Amoeboid <span class="hlt">Olivine</span> aggregates (AOAs) are irregularly shaped objects commonly observed in carbonaceous chondrites. Because they are composed of fine-grained <span class="hlt">olivine</span> and Ca-Al-rich minerals, they are sensitive indicators for nebular process and parent body alteration of their parent bodies. Recently an AOA was found in a carbonaceous clast in polymict eucrite LEW 85300. The bulk major element composition of the clast matrix in LEW 85300 suggests a relation to CM, CO and CV chondrites, whereas bulk clast trace and major element compositions do not match any carbonaceous chondrite, suggesting they have a unique origin. Here we characterize the mineralogy of AOA in LEW 85300 and discuss the origin of the carbonaceous clasts. Results and Discussion: The AOA is located in an impact melt vein. Half of the aggregate shows recrystallization textures (euhedral pyroxene and molten metal/FeS) due to impact melting, but the remaining part preserves the original texture. The AOA is composed of <span class="hlt">olivine</span>, FeS and Mg,Al-phyllosilicate. Individual <span class="hlt">olivine</span> grains measure 1-8 microns, with Fe-rich rims, probably due to impact heating. <span class="hlt">Olivines</span> in the AOA are highly forsteritic (Fo95-99), indicating that the AOA escaped thermal metamorphism [4]. Although no LIME (Low-Fe, Mn-Enriched) <span class="hlt">olivine</span> is observed, forsterite composition and the coexistence of Mg,Al-phyllosilicate suggest that the AOA is similar to those in the Bali-type oxidized CV (CVoxB) and CR chondrites. However, it should be noted that fayalitic <span class="hlt">olivine</span>, which commonly occurs in CVoxB AOA, is not observed in this AOA. Also, the smaller grain size (<8 microns) of <span class="hlt">olivine</span> suggests they may be related to CM or CO chondrites. Therefore, we cannot exclude the possibility that the AOA originated from a unique carbonaceous chondrite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930068398&hterms=Israel+humanity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DIsrael%2Bhumanity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930068398&hterms=Israel+humanity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DIsrael%2Bhumanity"><span>Secondary processing of <span class="hlt">chondrules</span> and refractory inclusions (CAIs) by gasdynamic heating</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Podolak, M.; Prialnik, D.; Bunch, T. E.; Cassen, P.; Reynolds, R.</p> <p>1993-01-01</p> <p>Results of calculations performed to determine the conditions necessary for producing the opaque rims on <span class="hlt">chondrules</span> and CAI rims by high-speed entry into the transient atmosphere of an accreting meteorite parent body are presented. The sensitivity of these results to variations in critical parameters is investigated. The range of entry velocities which can produce such rims is shown to depend on the size, melting temperature, and thermal conductivity of the particles. For particles greater than 2 mm in radius, with thermal conductivities of 20,000 ergs/sm s K or lower, entry velocities of about 3 km/s suffice. For particle sizes less than 1 mm in radius, the range of encounter velocities that can produce rims is narrow or vanishing, regardless of the thermal conductivity, unless the melting temperature in the outer part of the <span class="hlt">chondrule</span> has been reduced by compositional heterogeneity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040056060&hterms=oxygen+planets&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Doxygen%2Bplanets','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040056060&hterms=oxygen+planets&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Doxygen%2Bplanets"><span>Lunar and Planetary Science XXXV: Special Session: Oxygen in the Solar System, II</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2004-01-01</p> <p>The Special Session: Oxygen in the Solar System, II, included the following reports:Evolution of Oxygen Isotopes in the Solar Nebula; Disequilibrium Melting of Refractory Inclusions: A Mechanism for High-Temperature Oxygen; Isotope Exchange in the Solar Nebula; Oxygen Isotopic Compositions of the Al-rich <span class="hlt">Chondrules</span> in the CR Carbonaceous Chondrites: Evidence for a Genetic Link to Ca-Al-rich Inclusions and for Oxygen Isotope Exchange During <span class="hlt">Chondrule</span> Melting; Nebular Formation of Fayalitic <span class="hlt">Olivine</span>: Ineffectiveness of Dust Enrichment; Water in Terrestrial Planets: Always an Oxidant?; Oxygen Barometry of Basaltic Glasses Based on Vanadium Valence Determination Using Synchrotron MicroXANES; A New Oxygen Barometer for Solar System Basaltic Glasses Based on Vanadium Valence; The Relationship Between Clinopyroxene Fe3+ Content and Oxygen Fugacity ; and <span class="hlt">Olivine</span>-Silicate Melt Partitioning of Iridium.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EGSGA..27.4166N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EGSGA..27.4166N"><span>Texture and Elastic Anisotropy of Mantle <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nikitin, A. N.; Ivankina, T. I.; Bourilitchev, D. E.; Klima, K.; Locajicek, T.; Pros, Z.</p> <p></p> <p>Eight <span class="hlt">olivine</span> rock samples from different European regions were collected for neu- tron texture analyses and for P-wave velocity measurements by means of ultrasonic sounding at various confining pressures. The orientation distribution functions (ODFs) of <span class="hlt">olivine</span> were determined and pole figures of the main crystallographic planes were calculated. The spatial P-wave velocity distributions were determined at confining pressures from 0.1 to 400 MPa and modelled from the <span class="hlt">olivine</span> textures. In dependence upon the type of rock (xenolith or dunite) different behavior of both the P-wave veloc- ity distributions and the anisotropy coefficients with various confining pressures was observed. In order to explain the interdependence of elastic anisotropy and hydrostatic pressure, a model for polycrystalline <span class="hlt">olivine</span> rocks was suggested, which considers the influence of the crystallographic and the mechanical textures on the elastic behaviour of the polycrystal. Since the <span class="hlt">olivine</span> texture depends upon the active slip systems and the deformation temperature, neutron texture analyses enable us to estimate depth and thermodynamical conditions during texture formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060049100&hterms=trigo&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtrigo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060049100&hterms=trigo&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtrigo"><span>Carbon-rich Chondritic Clast PV1 from the Plainview H-chondrite Regolith Formation from H3 Chondrite Material by Possible Cometary Impact</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rubin, Alan E.; Trigo-Rodriguez, Josep M.; Kunihiro, Takuya; Kallemeyn, Gregory W.; Wasson, John T.</p> <p>2006-01-01</p> <p>Chondritic clast PV1 from the Plainview H-chondrite regolith breccia is a subrounded, 5-mm diameter unequilibrated chondritic fragment that contains 13 wt% C occurring mainly within irregularly shaped 30-400-micron-size opaque patches. The clast formed from H3 chondrite material as indicated by the mean apparent <span class="hlt">chondrule</span> diameter (310 micron vs. approximately 300 micron in H3 chondrites), the mean Mg-normalized refractory lithophile abundance ratio (1.00 +/- 0.09 XH), the previously determined 0-isotopic composition (Delta O-17 = 0.66% vs. 0.68 +/- 0.04%0 in H3 chondrites and 0.73 +/- 0.09% in H4-6 chondrites), the heterogeneous <span class="hlt">olivine</span> compositions in grain cores (with a minimum range of Fal-19), and the presence of glass in some <span class="hlt">chondrules</span>. Although the clast lacks the fine-grained, ferroan silicate matrix material present in type 3 ordinary chondrites, PV1 contains objects that appear to be recrystallized clumps of matrix material. Similarly, the apparent dearth of radial pyroxene and cryptocrystalline <span class="hlt">chondrules</span> in PV1 is accounted for by the presence of some recrystallized fragments of these <span class="hlt">chondrule</span> textural types. All of the <span class="hlt">chondrules</span> in PV1 are interfused indicating that temperatures must have briefly reached approximately 1100C (the approximate solidus temperature of H-chondrite silicate). The most likely source of this heating was by an impact. Some metal was lost during impact heating as indicated by the moderately low abundance of metallic Fe-Ni in PV1 (approximately 14 wt%) compared to that in mean H chondrites (approximately 18 wt%). The carbon enrichment of the clast may have resulted from a second impact event, one involving a cometary projectile, possibly a Jupiter-family comet. As the clast cooled, it experienced hydrothermal alteration at low water/rock ratios as evidenced by the thick rims of ferroan <span class="hlt">olivine</span> around low-FeO <span class="hlt">olivine</span> cores. The C-rich chondritic clast was later incorporated into the H-chondrite parent-body regolith and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V34A..02X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V34A..02X"><span>Change in Frictional Behavior during <span class="hlt">Olivine</span> Serpentinization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xing, T.; Zhu, W.; French, M. E.; Belzer, B.</p> <p>2017-12-01</p> <p>Hydration of mantle peridotites (serpentinization) is pervasive at plate boundaries. It is widely accepted that serpentinization is intrinsically linked to hydromechanical processes within the sub-seafloor, where the interplay between cracking, fluid supply and chemical reactions is responsible for a spectrum of fault slip, from earthquake swarms at the transform faults, to slow slip events at the subduction zone. Previous studies demonstrate that serpentine minerals can either promote slip or creep depend on many factors that include sliding velocity, temperature, pressure, interstitial fluids, etc. One missing link from the experimental investigation of serpentine to observations of tectonic faults is the extent of alteration necessary for changing the frictional behaviors. We quantify changes in frictional behavior due to serpentinization by conducting experiments after in-situ serpentinization of <span class="hlt">olivine</span> gouge. In the sample configuration a layer of powder is sandwiched between porous sandstone blocks with 35° saw-cut surface. The starting material of fine-grained (63 120 µm) <span class="hlt">olivine</span> powder is reacted with deionized water for 72 hours at 150°C before loading starts. Under the conventional triaxial configuration, the sample is stressed until sliding occurs within the gouge. A series of velocity-steps is then performed to measure the response of friction coefficient to variations of sliding velocity from which the rate-and-state parameters are deduced. For comparison, we measured the frictional behavior of unaltered <span class="hlt">olivine</span> and pure serpentine gouges.Our results confirm that serpentinization causes reduced frictional strength and velocity weakening. In unaltered <span class="hlt">olivine</span> gouge, an increase in frictional resistance with increasing sliding velocity is observed, whereas the serpentinized <span class="hlt">olivine</span> and serpentine gouges favor velocity weakening behaviors at the same conditions. Furthermore, we observed that high pore pressures cause velocity weakening in <span class="hlt">olivine</span> but</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850047880&hterms=copernicus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dcopernicus','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850047880&hterms=copernicus&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dcopernicus"><span>Origin of <span class="hlt">olivine</span> at Copernicus</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pieters, C. M.; Wilhelms, D. E.</p> <p>1985-01-01</p> <p>The central peaks of Copernicus are among the few lunar areas where near-infrared telescopic reflectance spectra indicate extensive exposures of <span class="hlt">olivine</span>. Other parts of Copernicus crater and ejecta, which were derived from highland units in the upper parts of the target site, contain only low-Ca pyroxene as a mafic mineral. The exposure of compositionally distinct layers including the presence of extensive <span class="hlt">olivine</span> may result from penetration to an anomalously deep layer of the crust or to the lunar mantle. It is suggested that the Procellarum basin and the younger, superposed Insularum basin have provided access to these normally deep-seated crustal or mantle materials by thinning the upper crustal material early in lunar history. The occurrences of <span class="hlt">olivine</span> in portions of the compositionally heterogeneous Aristarchus Region, in a related geologic setting, may be due to the same sequence of early events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26PSL.454..293B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26PSL.454..293B"><span>Molybdenum isotopic evidence for the origin of <span class="hlt">chondrules</span> and a distinct genetic heritage of carbonaceous and non-carbonaceous meteorites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Budde, Gerrit; Burkhardt, Christoph; Brennecka, Gregory A.; Fischer-Gödde, Mario; Kruijer, Thomas S.; Kleine, Thorsten</p> <p>2016-11-01</p> <p>Nucleosynthetic isotope anomalies are powerful tracers to determine the provenance of meteorites and their components, and to identify genetic links between these materials. Here we show that <span class="hlt">chondrules</span> and matrix separated from the Allende CV3 chondrite have complementary nucleosynthetic Mo isotope anomalies. These anomalies result from the enrichment of a presolar carrier enriched in s-process Mo into the matrix, and the corresponding depletion of this carrier in the <span class="hlt">chondrules</span>. This carrier most likely is a metal and so the uneven distribution of presolar material probably results from metal-silicate fractionation during <span class="hlt">chondrule</span> formation. The Mo isotope anomalies correlate with those reported for W isotopes on the same samples in an earlier study, suggesting that the isotope variations for both Mo and W are caused by the heterogeneous distribution of the same carrier. The isotopic complementary of <span class="hlt">chondrules</span> and matrix indicates that both components are genetically linked and formed together from one common reservoir of solar nebula dust. As such, the isotopic data require that most <span class="hlt">chondrules</span> formed in the solar nebula and are not a product of protoplanetary impacts. Allende <span class="hlt">chondrules</span> and matrix together with bulk carbonaceous chondrites and some iron meteorites (groups IID, IIIF, and IVB) show uniform excesses in 92Mo, 95Mo, and 97Mo that result from the addition of supernova material to the solar nebula region in which these carbonaceous meteorites formed. Non-carbonaceous meteorites (enstatite and ordinary chondrites as well as most iron meteorites) do not contain this material, demonstrating that two distinct Mo isotope reservoirs co-existed in the early solar nebula that remained spatially separated for several million years. This separation was most likely achieved through the formation of the gas giants, which cleared the disk between the inner and outer solar system regions parental to the non-carbonaceous and carbonaceous meteorites. The Mo isotope</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940007634&hterms=chemistry+elements&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dchemistry%2Belements','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940007634&hterms=chemistry+elements&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dchemistry%2Belements"><span>SXRF determination of trace elements in <span class="hlt">chondrule</span> rims in the unequilibrated CO3 chondrite, ALH A77307</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brearley, Adrian J.; Bajt, Sasa; Sutton, Steve R.; Papike, J. J.</p> <p>1993-01-01</p> <p>The concentrations of Ni, Cu, Zn, Ga, Ge, and Se in five <span class="hlt">chondrule</span> rims in the CO3 chondrite ALH A77307 (3.0) using the synchrotron x-ray fluorescence (SXRF) microprobe at Brookhaven National Laboratory were determined. The data show that the trace element chemistry of rims on different <span class="hlt">chondrules</span> is remarkably similar, consistent with data obtained for the major elements by electron microprobe. These results support the idea that rims are not genetically related to individual <span class="hlt">chondrules</span>, but all sampled the same reservoir of homogeneously mixed dust. Of the trace elements analyzed Zn and Ga show depletions relative to CI chondrite values, but in comparison with bulk CO chondrites all the elements are enriched by approximately 1.5 to 3.5 x CO. The high concentrations of the highly volatile elements Se and Ga and moderately volatile Zn (1.5 to 2 x CO) in rims show that matrix is the major reservoir of volatile elements in ALH A77307.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.222..284B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.222..284B"><span>Hf-W chronology of CR chondrites: Implications for the timescales of <span class="hlt">chondrule</span> formation and the distribution of 26Al in the solar nebula</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Budde, Gerrit; Kruijer, Thomas S.; Kleine, Thorsten</p> <p>2018-02-01</p> <p>Renazzo-type carbonaceous (CR) chondrites are distinct from most other chondrites in having younger <span class="hlt">chondrule</span> 26Al-26Mg ages, but the significance of these ages and whether they reflect true formation times or spatial variations of the 26Al/27Al ratio within the solar protoplanetary disk are a matter of debate. To address these issues and to determine the timescales of metal-silicate fractionation and <span class="hlt">chondrule</span> formation in CR chondrites, we applied the short-lived 182Hf-182W chronometer to metal, silicate, and <span class="hlt">chondrule</span> separates from four CR chondrites. We also obtained Mo isotope data for the same samples to assess potential genetic links among the components of CR chondrites, and between these components and bulk chondrites. All investigated samples plot on a single Hf-W isochron and constrain the time of metal-silicate fractionation in CR chondrites to 3.6 ± 0.6 million years (Ma) after the formation of Ca-Al-rich inclusions (CAIs). This age is indistinguishable from a ∼3.7 Ma Al-Mg age for CR <span class="hlt">chondrules</span>, suggesting not only that metal-silicate fractionation and <span class="hlt">chondrule</span> formation were coeval, but also that these two processes were linked to each other. The good agreement of the Hf-W and Al-Mg ages, combined with concordant Hf-W and Al-Mg ages for angrites and CV <span class="hlt">chondrules</span>, provides strong evidence for a disk-wide, homogeneous distribution of 26Al in the early solar system. As such, the young Al-Mg ages for CR <span class="hlt">chondrules</span> do not reflect spatial 26Al/27Al heterogeneities but indicate that CR <span class="hlt">chondrules</span> formed ∼1-2 Ma later than <span class="hlt">chondrules</span> from most other chondrite groups. Metal and silicate in CR chondrites exhibit distinct nucleosynthetic Mo and W isotope anomalies, which are caused by the heterogeneous distribution of the same presolar s-process carrier. These data suggest that the major components of CR chondrites are genetically linked and therefore formed from a single reservoir of nebular dust, most likely by localized melting events within the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017M%26PS...52.2166R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017M%26PS...52.2166R"><span>Protracted storage of CR <span class="hlt">chondrules</span> in a region of the disk transparent to galactic cosmic rays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roth, Antoine S. G.; Metzler, Knut; Baumgartner, Lukas P.; Hofmann, Beda A.; Leya, Ingo</p> <p>2017-10-01</p> <p>Renazzo-type carbonaceous (CR) chondrites are accretionary breccias that formed last. As such they are ideal samples to study precompaction exposures to cosmic rays. Here, we present noble gas data for 24 <span class="hlt">chondrules</span> and 3 dark inclusion samples (DIs) from Shişr 033 (CR2). The meteorite was selected based on the absence of implanted solar wind noble gases and an anomalous oxygen isotopic composition of the DIs; the oxygen isotopes match those in CV3 and CO3 chondrites. Our samples contain variable mixtures of galactic cosmic ray (GCR)-produced cosmogenic noble gases and trapped noble gases of presolar origin. Remarkably, all <span class="hlt">chondrules</span> have cosmogenic 3He and 21Ne concentrations up to 4.3 and 7.1 times higher than the DIs, respectively. We derived an average 3He-21Ne cosmic ray exposure (CRE) age for Shişr 033 of 2.03 ± 0.20 Ma (2 SD) and excesses in cosmogenic 3He and 21Ne in <span class="hlt">chondrules</span> (relative to the DIs) in the range (in 10-8 cm3STP/g) 3.99-7.76 and 0.94-1.71, respectively. Assuming present-day GCR flux density, the excesses translate into average precompaction 3He-21Ne CRE ages of 3.1-27.3 Ma depending on the exposure geometry. The data can be interpreted assuming a protracted storage of a single <span class="hlt">chondrule</span> generation prior to the final assembly of the Shişr 033 parent body in a region of the disk transparent to GCRs.</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('https://ntrs.nasa.gov/search.jsp?R=19860058985&hterms=History+Genetics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DHistory%2BGenetics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860058985&hterms=History+Genetics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DHistory%2BGenetics"><span>Mineralogy of interplanetary dust particles from the '<span class="hlt">olivine</span>' infrared class</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Christoffersen, R.; Buseck, P. R.</p> <p>1986-01-01</p> <p>Analytical electron microscopy observations establish that <span class="hlt">olivine</span> is abundant and the predominant silicate phase in three interplanetary dust particles (IDPs) from the '<span class="hlt">olivine</span>' infrared spectra category. Two of the particles have microstructures resembling those of most nonhydrous chondritic IDPs, consisting of micron to submicron grains together with a matrix composed of amorphous carbonaceous material and sub-500 A grains. In addition to <span class="hlt">olivine</span> these particles respectively contain enstatite and magnetite, and pentlandite plus Ca-rich clinopyroxene. The third IDP consists mostly of <span class="hlt">olivine</span> and pyrrhotite with little or no matrix material. <span class="hlt">Olivine</span> grains in this particle contain prominent solar-flare ion tracks with densities corresponding to a space-exposure age between 1000 to 100,000 years. Although the three particles have <span class="hlt">olivine</span>-rich mineralogies in common, other aspects of their mineralogies and microstructures suggest that they experienced different formation histories. The differences between the particles indicate that the <span class="hlt">olivine</span> infrared spectral category is a diverse collection of IDPs that probably incorporates several genetic groups.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120002880','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120002880"><span>Search for <span class="hlt">Olivine</span> Spectral Signatures on the Surface of Vesta</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Palomba, E.; De Sanctis, M. C.; Ammannito, E.; Capaccioni, F.; Capria, M. T.; Farina, M.; Frigeri, A.; Longobardo, A.; Tosi, F.; Zambon, F.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20120002880'); toggleEditAbsImage('author_20120002880_show'); toggleEditAbsImage('author_20120002880_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20120002880_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20120002880_hide"></p> <p>2012-01-01</p> <p>The occurrence of <span class="hlt">olivines</span> on Vesta were first postulated from traditional petrogenetic models which suggest the formation of <span class="hlt">olivine</span> as lower crustal cumulates. An indirect confirmation is given by their presence as a minor component in some samples of diogenite meteorites, the harzburgitic diogenites and the dunitic diogenites, and as <span class="hlt">olivine</span> mineral clasts in howardites. Another indication for this mineral was given by interpretations of groundbased and Hubble Space Telescope observations that suggested the presence of local <span class="hlt">olivine</span>-bearing units on the surface of Vesta. The VIR instrument onboard the DAWN mission has been mapping Vesta since July 2011. VIR acquired hyperspectral images of Vesta s surface in the wavelength range from 0.25 to 5.1 m during Approach, Survey and High Altitude Mapping (HAMO) orbits that allowed a 2/3 of the entire asteroid surface to be mapped. The VIR operative spectral interval, resolution and coverage is suitable for the detection and mapping of any <span class="hlt">olivine</span> rich regions that may occur on the Vesta surface. The abundance of <span class="hlt">olivine</span> in diogenites is typically lower than 10% but some samples richer in <span class="hlt">olivine</span> are known. However, we do not expect to have extensive exposures of <span class="hlt">olivine</span>-rich material on Vesta. Moreover, the partial overlap of <span class="hlt">olivine</span> and pyroxene spectral signatures will make <span class="hlt">olivine</span> difficult to detect. Different spectral parameters have been used to map <span class="hlt">olivine</span> on extraterrestrial bodies, and here we discuss the different approaches used, and develop new ones specifically for Vesta. Our new methods are based on combinations of the spectral parameters relative to the 1 and 2 micron bands (the most prominent spectral features of Vesta surface in the visible and the infrared), such as band center locations, band depths, band areas, band area ratios. Before the direct application to the VIR data, the efficiency of each approach is evaluated by means of analysis of laboratory spectra of HED meteorites, pyroxenes, <span class="hlt">olivines</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009M%26PS...44..763W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009M%26PS...44..763W"><span>Petrology and mineralogy of the Ningqiang carbonaceous chondrite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Y.; Hsu, W.</p> <p>2009-07-01</p> <p>We report detailed chemical, petrological, and mineralogical studies on the Ningqiang carbonaceous chondrite. Ningqiang is a unique ungrouped type 3 carbonaceous chondrite. Its bulk composition is similar to that of CV and CK chondrites, but refractory lithophile elements (1.01 × CI) are distinctly depleted relative to CV (1.29 × CI) and CK (1.20 × CI) chondrites. Ningqiang consists of 47.5 vol% <span class="hlt">chondrules</span>, 2.0 vol% Ca,Al-rich inclusions (CAIs), 4.5 vol% amoeboid <span class="hlt">olivine</span> aggregates (AOAs), and 46.0 vol% matrix. Most <span class="hlt">chondrules</span> (95%) in Ningqiang are Mgrich. The abundances of Fe-rich and Al-rich <span class="hlt">chondrules</span> are very low. Al-rich <span class="hlt">chondrules</span> (ARCs) in Ningqiang are composed mainly of <span class="hlt">olivine</span>, plagioclase, spinel, and pyroxenes. In ARCs, spinel and plagioclase are enriched in moderately volatile elements (Cr, Mn, and Na), and low-Ca pyroxenes are enriched in refractory elements (Al and Ti). The petrology and mineralogy of ARCs in Ningqiang indicate that they were formed from hybrid precursors of ferromagnesian <span class="hlt">chondrules</span> mixed with refractory materials during <span class="hlt">chondrule</span> formation processes. We found 294 CAIs (55.0% type A, 39.5% spinel-pyroxene-rich, 4.4% hibonite-rich, and several type C and anorthite-spinelrich inclusions) and 73 AOAs in 15 Ningqiang sections (equivalent to 20 cm2 surface area). This is the first report of hibonite-rich inclusions in Ningqiang. They are texturally similar to those in CM, CH, and CB chondrites, and exhibit three textural forms: aggregates of euhedral hibonite single crystals, fine-grained aggregates of subhedral hibonite with minor spinel, and hibonite ± Al,Ti-diopside ± spinel spherules. Evidence of secondary alteration is ubiquitous in Ningqiang. Opaque assemblages, formed by secondary alteration of pre-existing alloys on the parent body, are widespread in <span class="hlt">chondrules</span> and matrix. On the other hand, nepheline and sodalite, existing in all chondritic components, formed by alkali-halogen metasomatism in the solar nebula.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19750028094&hterms=history+microscopes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhistory%2Bmicroscopes','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19750028094&hterms=history+microscopes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhistory%2Bmicroscopes"><span>A scanning electron microscope study of <span class="hlt">olivine</span> crystal surfaces</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Olsen, E. J.; Grossman, L.</p> <p>1974-01-01</p> <p>SEM photographs were taken of euhedral <span class="hlt">olivine</span> grains from the Murchison C2 chondrite and several terrestrial and lunar occurrences. In general, the crystal faces of the meteorite grains are rough and uneven, with irregular growth patterns. They are very similar to crystal faces on terrestrial <span class="hlt">olivine</span> grains that formed by sublimation from a vapor phase. They are very different from the relatively smooth and featureless surfaces of magmatic <span class="hlt">olivine</span> crystals that precipitated from igneous melts. Qualitatively, the surface morphology of the crystal supports the contention that many euhedral crystals of <span class="hlt">olivine</span> in C2 meteorites condensed from a gas phase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160002410','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160002410"><span><span class="hlt">Chondrules</span> and Opaque Phases in Unequilibrated R Chondrites: A Comprehensive Assessment of Their Formation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miller, K. E.; Lauretta, D. S.; Connolly, H. C., Jr.; Berger, E. L.; Domanik, K.</p> <p>2016-01-01</p> <p>Equilibrated Rumuruti (R) chondrites record an oxygen fugacity between 0 and 3.5 log units below the fayalite-magnetite-quartz buffer, and a sulfur fugacity (fS2) 2 log units above the iron-troilite buffer. They are more than an order of magnitude more oxidized than the ordinary chondrites [1], and orders of magnitude more sulfidized than solar values. Although the R chondrites have the highest (delta)O-17 value of any meteorites, analyses of unequilibrated R chondrites indicate <span class="hlt">chondrule</span> formation in an oxygen isotope reservoir similar to that of the ordinary chondrite <span class="hlt">chondrules</span>. We present the relationship of the R chondrite parent body to pre-accretionary volatiles O and S based on our analyses of unequilibrated R chondrite material in two thin sections from the meteorite Mount Prestrud (PRE) 95404.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000081089&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D50%26Ntt%3DRussell','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000081089&hterms=Russell&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26Nf%3DPublication-Date%257CBTWN%2B20000101%2B20001231%26N%3D0%26No%3D50%26Ntt%3DRussell"><span><span class="hlt">Chondrules</span> of the Very First Generation in Bencubbin/CH-like Meteorites QUE94411 and Hammadah Al Hamra 237: Condensation Origin at High Ambient Nebular Temperatures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Krot, Alexander N.; Meibom, Anders; Russell, Sara S.; Young, Edward; Alexander, Conel M.; McKeegan, Kevin D.; Lofgren, Gary; Cuzzi, Jeff; Zipfel, Jutta; Keil, Klaus</p> <p>2000-01-01</p> <p><span class="hlt">Chondrules</span> in QUE94411 and HH 237 formed at high ambient T prior to condensation of Fe,Ni-metal following a large scale thermal event that resulted in complete vaporization of a solar nebula region. These <span class="hlt">chondrules</span> escaped subsequent remelting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150002321','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150002321"><span>Vaporization Studies of <span class="hlt">Olivine</span> via Knudsen Effusion Mass Spectrometry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Costa, G. C. C.; Jacobson, N. S.</p> <p>2014-01-01</p> <p><span class="hlt">Olivine</span> is the major mineral in the Earth's upper mantle occurring predominantly in igneous rocks and has been identified in meteorites, asteroids, the Moon and Mars. Among many other important applications in planetary and materials sciences, the thermodynamic properties of vapor species from <span class="hlt">olivine</span> are crucial as input parameters in computational modelling of the atmospheres of hot, rocky exoplanets (lava planets). There are several weight loss studies of <span class="hlt">olivine</span> vaporization in the literature and one Knudsen Effusion Mass Spectrometry (KEMS) study. In this study, we examine a forsterite-rich <span class="hlt">olivine</span> (93% forsterite and 7% fayalite, Fo93Fa7) with KEMS to further understand its vaporization and thermodynamic properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017LPICo1963.2012J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017LPICo1963.2012J"><span>Harvesting the Decay Energy of 26-Al to Drive Lightning Discharge and <span class="hlt">Chondrule</span> Formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Johansen, A.; Okuzumi, S.</p> <p>2017-02-01</p> <p>We demonstrate that positrons released in the decay of 26-Al cause large-scale charging of dense pebble regions. The charge separation is neutralized by lightning discharge and this can lead to the formation of <span class="hlt">chondrules</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.5127F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.5127F"><span>Chemical profiles along <span class="hlt">olivine</span> crystallographic axes: a record of the melt-rock interaction sequence forming Hole U1309D <span class="hlt">Olivine</span>-rich troctolites (Atlantis Massif, MAR, 30°N)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferrando, Carlotta; Godard, Marguerite; Ildefonse, Benoit; Rampone, Elisabetta</p> <p>2017-04-01</p> <p>The gabbroic section drilled at IODP Hole U1309D (Mid-Atlantic Ridge, IODP Expeditions 304, 305) comprises a whole range of modes from primitive <span class="hlt">olivine</span>-rich troctolites to evolved gabbros. These series occur as discrete alternating intervals of variable composition and thickness at different depths. High MgO contents and a relatively large proportion of <span class="hlt">olivine</span>-rich lithologies (up to 90% modal <span class="hlt">olivine</span>) characterize this gabbroic section. Contacts between <span class="hlt">olivine</span>-rich troctolites and neighboring coarse grained <span class="hlt">olivine</span> gabbros are sharp, with the exception of the contacts between <span class="hlt">olivine</span>-rich intervals and cross-cutting gabbroic veins, which are diffuse and characterized by progressive variations in plagioclase content. <span class="hlt">Olivine</span>-rich troctolites are heterogeneously distributed along the borehole and show variable modal composition: centimeter to decimeter scale dunitic (90% <span class="hlt">olivine</span>), troctolitic (enriched in plagioclase) and wehrlitic (enriched in clinopyroxene) domains were identified. Previous in-situ trace element geochemistry and crystallographic preferred orientation measurements of <span class="hlt">olivine</span>-rich troctolites indicated that they record extensive melt impregnation of pre-existing <span class="hlt">olivine</span>-rich material, either mantle rocks or dunitic cumulate. We performed a detailed multi-scale petro-structural and geochemical study on selected samples of well-preserved <span class="hlt">olivine</span>-rich troctolites with the aim to unravel the sequence of re-equilibration processes and better constrain the local conditions driving the formation of these rocks. Processed EBSD maps show variable textures at single sample scale. All identified domains are characterized by coarse grained and deformed <span class="hlt">olivines</span>, and small rounded undeformed <span class="hlt">olivines</span>. Coarse grained and small rounded <span class="hlt">olivines</span> have the same major and trace element compositions. Small <span class="hlt">olivines</span> are interpreted as relicts after dissolution of coarse grained <span class="hlt">olivines</span>. Clinopyroxene, plagioclase, and minor orthopyroxene are present as interstitial</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFMMR43A0980L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFMMR43A0980L"><span><span class="hlt">Olivine</span> Instability: An Experimental View of Mechanism of Deep Earthquakes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Long, H.; Weidner, D.; Li, L.; Chen, J.; Wang, L.</p> <p>2007-12-01</p> <p><span class="hlt">Olivine</span> (¦Á-(Mg,Fe)2SiO4) is the major constituent of the upper mantle and the ocean lithosphere. In subduction zone, where the earthquakes happen, the rheology of slab is mainly controlled by that of <span class="hlt">olivine</span>. Several different mechanisms for deep focus earthquakes have been suggested, which include <span class="hlt">olivine</span> instability (Bridgman, 1936; Orowan, 1960; Post, 1977; Ogawa, 1987; Hobbs and Ord, 1988; Kao and Chen, 1995), shear-induced melting (Griggs, 1954, 1972; Griggs and Handin, 1960; Griggs and Baker, 1969), phase transformation (Bridgman, 1945; Benioff, 1963; Meade and Jeanloz, 1989), dehydration of hydrous specimens (Meade and Jeanloz, 1991), and <span class="hlt">olivine</span> metastability-induced anticrack (Green and Houston, 1995). Since the low temperature of the ¡°cold¡± slab, which can be as low as 600¡ãC in transition zone, <span class="hlt">olivine</span> may still exist there and thus its shear instability may still be the possible mechanism for the deep-focus earthquakes. In our experimental study on deformation of San Carlos <span class="hlt">olivine</span> at subduction zone conditions carried out on a D-DIA apparatus, Sam85 at X17B2, NSLS, we observed that the transitional temperature between regimes of insensitive to temperature and sensitive to temperature can be as high as 900¡ãC or even higher for the annealed polycrystal <span class="hlt">olivine</span> sample, while that for unannealed sample can be as low as 450¡ãC. Our results for the unannealed sample are consistent to the result of Raterron et al (2004), which is concluded from the relaxation experiments. The annealed and unannealed <span class="hlt">olivine</span> can be present the natural <span class="hlt">olivine</span> in non-fault systems and that in pre-existing fault systems in subduction zone, respectively. We therefore propose a new <span class="hlt">olivine</span> instability model with a ¡°sandwich¡± formation for the deep focus earthquakes: In this model the pre-existing fault system is surrounded by the no-fault systems. When the slab dives down, the <span class="hlt">olivine</span> in both systems undergoes a stress- build-up process and can hold very high</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008CryRp..53..404G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008CryRp..53..404G"><span>Calcio-<span class="hlt">olivine</span> γ-Ca2SiO4: I. Rietveld refinement of the crystal structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gobechiya, E. R.; Yamnova, N. A.; Zadov, A. E.; Gazeev, V. M.</p> <p>2008-05-01</p> <p>The structure of the natural mineral calcio-<span class="hlt">olivine</span> (γ-Ca2SiO4) found in skarn xenoliths in the region of the Lakargi Mountain (North Caucasus, Kabardino-Balkaria, Russia) is refined by the Rietveld method [ a = 5.07389(7) Å, b = 11.21128(14) Å, c = 6.75340(9) Å, V = 384.170(5) Å3, Z = 4, ρcalcd = 2.98 g/cm3, space group Pbnm]. The X-ray diffraction pattern of a powdered sample is recorded on a STOE STADI MP diffractometer [λCu K α1; Ge(111) primary monochromator; 6.00° < 2θ < 100.88°; step width, 2.5° in 2θ; number of reflections, 224]. All calculations are performed with the WYRIET (version 3.3) software package. The structural model is refined in the anisotropic approximation to R p = 6.44, R wp = 8.52, R exp = 5.85, R B = 4.98, R F = 6.90, and s = 1.46. It is shown that the sample under investigation is a mixture of several mineral phases, among which calcio-<span class="hlt">olivine</span> (the natural analogue of the γ-Ca2SiO4 compound) (83%), hillebrandite (13%), and wadalite (4%) are dominant. Only the scale factors and the unit cell parameters are refined for hillebrandite Ca2SiO3(OH)2 [ a = 3.63472(16) Å, b = 16.4140(10) Å, c = 11.7914(8) Å, space group Cmc21, Z = 6] and wadalite Ca6Al5Si2O16Cl3 ( a = 12.0088 Å, space group, I <span class="hlt">bar</span> 4 3 d Z = 4). The results of the structure refinement of the main component of the sample confirm that the mineral calcio-<span class="hlt">olivine</span> is isostructural to the synthetic compound γ-Ca2SiO4. The structure of this compound is formed by the heteropolyhedral framework composed of Ca octahedra joined together into <span class="hlt">olivine</span>-like ribbons and isolated Si tetrahedra.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150002979','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150002979"><span>Na, K-Rich Rim Around a <span class="hlt">Chondrule</span> in Unequilibrated Ordinary Chondrite Lew 86018 (L3.1)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mishra, R. K.; Simon, J. I.; Ross, D. K.; Needham, A. W.; Messenger, S.; Keller, L. P.; Han, J.; Marhas, K. K.</p> <p>2015-01-01</p> <p>Ordinary chondrites represent the most abundant early Solar system extra-terrestrial (approximately 85% abundance) material available for laboratory studies and expectedly record the most extensive range of alterations effects from unmetamorphosed chondritic material to the highest temperatures of thermal metamorphism. The least metamorphosed chondrites belonging to petrologic type 3, the so called unequili-brated ordinary chondrites (UOCs), provide insights into alteration that happened during the primeval, ear-liest stage of Solar system formation. The higher grade petrologic types 4-6 ordinary chondrites on the other hand document up to near textural equilibrium (in type 6) extensive thermal metamorphism consisting of minerals and phases providing evidence of equilibration of heterogeneous mineral composition, solid-state recrystallization. Despite being the most abundant, the effect of alteration is less explicitly understood in ordinary chondrites (even less in UOCs) compared to other groups (e.g. CV, CO, CR). Additionally, the relationship between metasomatism (also referred as aqueous alteration or fluid-assisted metamorphism) and metamorphism (primarily thermal driven) has not been studied and alterations in the ordinary chondrites have been considered to have occurred in absence of fluids in general. Despite this conventional view, UOCs of lowest grades (3.0-3.2) show some evidence of low temperature (approximately 200 C), fluid assisted metamorphism in the form of the presence of phyllosilicates, ferroan <span class="hlt">olivine</span>, and magnetites in their matrices and occasionally in <span class="hlt">chondrules</span>. Here, we present petrographic and mineralogical studies of UOC, Lewis Hills (LEW) 86018 to further our understanding of the extent and relative importance of metasomatism and/or metamorphism in UOCs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70037122','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70037122"><span>Extraction of in situ cosmogenic 14C from <span class="hlt">olivine</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>Pigati, J.S.; Lifton, N.A.; Timothy, Jull A.J.; Quade, Jay</p> <p>2010-01-01</p> <p>Chemical pretreatment and extraction techniques have been developed previously to extract in situ cosmogenic radiocarbon (in situ 14C) from quartz and carbonate. These minerals can be found in most environments on Earth, but are usually absent from mafic terrains. To fill this gap, we conducted numerous experiments aimed at extracting in situ 14C from <span class="hlt">olivine</span> ((Fe,Mg)2SiO4). We were able to extract a stable and reproducible in situ 14C component from <span class="hlt">olivine</span> using stepped heating and a lithium metaborate (LiBO2) flux, following treatment with dilute HNO3 over a variety of experimental conditions. However, measured concentrations for samples from the Tabernacle Hill basalt flow (17.3 ?? 0.3 ka4) in central Utah and the McCarty's basalt flow (3.0 ?? 0.2 ka) in western New Mexico were significantly lower than expected based on exposure of <span class="hlt">olivine</span> in our samples to cosmic rays at each site. The source of the discrepancy is not clear. We speculate that in situ 14C atoms may not have been released from Mg-rich crystal lattices (the <span class="hlt">olivine</span> composition at both sites was ~Fo65Fa35). Alternatively, a portion of the 14C atoms released from the <span class="hlt">olivine</span> grains may have become trapped in synthetic spinel-like minerals that were created in the <span class="hlt">olivine</span>-flux mixture during the extraction process, or were simply retained in the mixture itself. Regardless, the magnitude of the discrepancy appears to be inversely proportional to the Fe/(Fe+Mg) ratio of the <span class="hlt">olivine</span> separates. If we apply a simple correction factor based on the chemical composition of the separates, then corrected in situ 14C concentrations are similar to theoretical values at both sites. At this time, we do not know if this agreement is fortuitous or real. Future research should include measurement of in situ 14C concentrations in <span class="hlt">olivine</span> from known-age basalt flows with different chemical compositions (i.e. more Fe-rich) to determine if this correction is robust for all <span class="hlt">olivine</span>-bearing rocks. ?? 2010 by the Arizona</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1982tcsc.meet..142G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1982tcsc.meet..142G"><span>Evaluation of <span class="hlt">olivine</span> refractories for TES</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gay, B. M.; Cochrane, R. L.; Palmour, H., III; Paisley, M. J.</p> <p>1982-02-01</p> <p>The principal objectives of this program are to (1) experimentally determine the degree of improvement in thermal and mechanical performance that can be obtained with an <span class="hlt">olivine</span> thermal storage brick made of domestic materials using advanced processing techniques compared with state-of-the-art as represented by commercial European bricks, (2) conduct an assessment of existing German ceramic process technology and determine its adaptability to domestic raw materials and manufacturing practices, and (3) investigate, on a limited basis, method for further improvement of domestic-<span class="hlt">olivine</span> brick. To date, accomplishments include (1) installation of improved, computer-based instrumentation, (2) the use of this system to determine performance characteristics of a set of heat storage refractories under cyclic use conditions, (3) acquisition of the services of a knowledgeable European consultant, (4) continued lab-scale process/property optimization studies, and (5) comparative testing of <span class="hlt">olivine</span>-based and magnesite-based heat storage refractories in the calorimetric test facility at Purdue University.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFM.V61A1349R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFM.V61A1349R"><span>A Re-appraisal of <span class="hlt">Olivine</span> Sorting and Accumulation in Hawaiian Magmas.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rhodes, J. M.</p> <p>2002-12-01</p> <p>Bowen never used the m-words (magma mixing) in his highly influential book "The Origin of the Igneous Rocks". Yet, in the past 20-30 years, magma mixing has been proposed as an important, almost ubiquitous, process at volcanoes in all tectonic environments ranging from oceanic basalts to large silicic magma bodies, and as the possible trigger of eruptions. Bowen regarded Hawaiian <span class="hlt">olivine</span> basalts and picrites as the result of <span class="hlt">olivine</span> accumulation in a lower MgO magma that was crystallizing and fractionating <span class="hlt">olivine</span>. This, with variants, has been the party line ever since, the only debate being over the MgO content of the proposed parental magmas. Although magma mixing has been recognized as an important process in differentiated, low-MgO (below 7 percent), Hawaiian magmas, the wide range in MgO (7-30 percent) in Hawaiian <span class="hlt">olivine</span> tholeiites and picrites is invariably attributed to <span class="hlt">olivine</span> crystallization, fractionation and accumulation. In this paper I will re-evaluate this hypothesis using well-documented examples from Kilauea, Mauna Kea and Mauna Loa that exhibit well-defined, coherent linear trends of major oxides and trace elements with MgO . If <span class="hlt">olivine</span> control is the only factor responsible for these trends, then the intersection of the regression lines for each trend should intersect <span class="hlt">olivine</span> compositions at a common forsterite composition, corresponding to the average accumulated <span class="hlt">olivine</span> in each of the magmas. In some cases (the ongoing Puu Oo eruption) this simple test holds and <span class="hlt">olivine</span> fractionation and accumulation can clearly be shown to be the dominant process. In other examples from Mauna Kea and Mauna Loa (1852, 1868, 1950 eruptions, and Mauna Loa in general) the test does not hold, and a more complicated process is required. Additionally, for those magmas that fail the test, CaO/Al2O3 invariably decreases with decreasing MgO content. This should not happen if only <span class="hlt">olivine</span> fractionation and accumulation are involved. The explanation for these linear</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR24B..02Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR24B..02Y"><span>Diffusional creep of fine-grained <span class="hlt">olivine</span> aggregates: Chemical and melt effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yabe, K.; Hiraga, T.</p> <p>2017-12-01</p> <p>Since <span class="hlt">olivine</span> is the major constituent mineral of the earth's upper mantle, flow properties of the upper mantle are often estimated based on flow laws of <span class="hlt">olivine</span> aggregate which are determined by high-temperature creep experiments. Recently, Miyazaki et al. (2013) showed that crystallographic preferred orientation (CPO) which has been interpreted as the main cause for seismic wave anisotropy in mantle asthenosphere could be formed in diffusional creep regime. The detail of diffusional creep of <span class="hlt">olivine</span> aggregates is not clear yet. The strength of <span class="hlt">olivine</span> aggregates synthesized using sol-gel method (Faul and Jackson 2007) was more than one order of magnitude harder in viscosity than those synthesized from natural mantle rocks (Hirth and Kohlstedt 1995, Hansen et al. 2011) even at the same experimental conditions. This discrepancy can be interpreted by a presence of melt and/or impurity. The purpose of this study is to examine the effects of chemical composition and presence of the melt phase on the creep properties of <span class="hlt">olivine</span> aggregates. At first, Fe-bearing <span class="hlt">olivine</span> aggregates were prepared by vacuum sintering of nano-sized <span class="hlt">olivine</span> powder synthesized from highly pure and fine-grained (<100 nm) source powders. Samples with and without dopants of Al2O3 and CaO were prepared. Then uniaxial compression tests at 1 atm were conducted. Deformation experiments showed that all the samples were deformed by diffusional creep mechanism. Both doped and non-doped samples exhibited sample strength at low temperature (=1150˚C), while the doped sample became significantly weaker with showing higher temperature sensitivity compared to non-doped samples at higher temperature. The temperature sensitivity of doped samples didn't change below and above solidus, which indicate the weakening due to chemical effect, not by the melting. Non-doped samples exhibits essentially the same strength as <span class="hlt">olivine</span> aggregates synthesized from sol-gel method (Faul and Jackson 2007), while doped sample is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930049219&hterms=negative+effects+oxygen&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnegative%2Beffects%2Boxygen','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930049219&hterms=negative+effects+oxygen&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dnegative%2Beffects%2Boxygen"><span>The Mn-Fe negative correlation in <span class="hlt">olivines</span> in ALHA 77257 ureilite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miyamoto, M.; Furuta, T.; Fujii, N.; Mckay, D. S.; Lofgren, G. E.; Duke, M. B.</p> <p>1993-01-01</p> <p>An electron probe microanalyzer is used to measure the Mn, Fe, and oxygen zoning profiles of <span class="hlt">olivines</span> in the ALHA 77257 ureilite. This is done to study the effects of reduction on the Mn-Fe value, as ureilite <span class="hlt">olivines</span> exhibit thin reduced rims. Since the Mn content gradually increases toward the rim of ureilite <span class="hlt">olivines</span>, while the Fa (= 100 x Fe/(Mg + Fe), mol percent) component decreases, the Mn-Fe content of <span class="hlt">olivine</span> is likely related to redox conditions. The results of melting experiments suggest that the Mn-Fe positive correlation is related to temperature and that the negative correlation of Mn-Fe in <span class="hlt">olivine</span> and low-Ca pyroxene is related to reduction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.222..305D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.222..305D"><span>Experimentally determined subsolidus metal-<span class="hlt">olivine</span> element partitioning with applications to pallasites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Donohue, Patrick H.; Hill, Eddy; Huss, Gary R.</p> <p>2018-02-01</p> <p>Pallasite meteorites, which consist primarily of <span class="hlt">olivine</span> and metal, may be remnants of disrupted core-mantle boundaries of differentiated asteroids or planetesimals. The early thermal histories of pallasites are potentially recorded by minor- and trace-element zonation in <span class="hlt">olivine</span>. However, constraining this history requires knowledge of element behavior under the conditions of pallasite formation, which is lacking for many of the main elements of interest (e.g., Co, Cr, Mn). In this study, we experimentally determined metal/<span class="hlt">olivine</span> partition coefficients for Fe, Ni, Co, Cr, and Mn in a pallasite analogue at subsolidus temperatures. Metal/<span class="hlt">olivine</span> partition coefficients (KM) increase in the order KMn < KCr < 1 < KFe < KCo < KNi, with five orders of magnitude separating KMn from KNi. Transition metals also become more siderophile with increasing experimental temperature (900-1550 °C). The experiments incidentally produced diffusion profiles in <span class="hlt">olivine</span> for these elements; our results suggest they diffuse through <span class="hlt">olivine</span> at similar rates. Core compositions of pallasite <span class="hlt">olivines</span> are consistent with high-temperature equilibration with FeNi-metal. <span class="hlt">Olivine</span> zonation toward crystal rims varies significantly for the investigated transition metals. We suggest rim zonation results from partial re-equilibration during late stage crystallization of minor phases (e.g., chromite, phosphates). This re-equilibration occurred over short timescales relative to overall pallasite cooling, likely tied to initial cooling rates on the order of 100-300 °C/Myr.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Icar..258..467N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Icar..258..467N"><span>Exogenic <span class="hlt">olivine</span> on Vesta from Dawn Framing Camera color data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nathues, Andreas; Hoffmann, Martin; Schäfer, Michael; Thangjam, Guneshwar; Le Corre, Lucille; Reddy, Vishnu; Christensen, Ulrich; Mengel, Kurt; Sierks, Holger; Vincent, Jean-Baptist; Cloutis, Edward A.; Russell, Christopher T.; Schäfer, Tanja; Gutierrez-Marques, Pablo; Hall, Ian; Ripken, Joachim; Büttner, Irene</p> <p>2015-09-01</p> <p>In this paper we present the results of a global survey of <span class="hlt">olivine</span>-rich lithologies on (4) Vesta. We investigated Dawn Framing Camera (FC) High Altitude Mapping Orbit (HAMO) color cubes (∼60 m/pixel resolution) by using a method described in Thangjam et al. (Thangjam, G., Nathues, A., Mengel, K., Hoffmann, M., Schäfer, M., Reddy, V., Cloutis, E.A., Christensen, U., Sierks, H., Le Corre, L., Vincent, J.-B, Russell, C.T. [2014b]. Meteorit. Planet. Sci. arXiv:1408.4687 [astro-ph.EP]). In total we identified 15 impact craters exhibiting <span class="hlt">olivine</span>-rich (>40 wt.% ol) outcrops on their inner walls, some showing <span class="hlt">olivine</span>-rich material also in their ejecta and floors. <span class="hlt">Olivine</span>-rich sites are concentrated in the Bellicia, Arruntia and Pomponia region on Vesta's northern hemisphere. From our multi-color and stratigraphic analysis, we conclude that most, if not all, of the <span class="hlt">olivine</span>-rich material identified is of exogenic origin, i.e. remnants of A- or/and S-type projectiles. The <span class="hlt">olivine</span>-rich lithologies in the north are possibly ejecta of the ∼90 km diameter Albana crater. We cannot draw a final conclusion on their relative stratigraphic succession, but it seems that the dark material (Nathues, A., Hoffmann, M., Cloutis, E.A., Schäfer, M., Reddy, V., Christensen, U., Sierks, H., Thangjam, G.S., Le Corre, L., Mengel, K., Vincent, J.-B., Russell, C.T., Prettyman, T., Schmedemann, N., Kneissl, T., Raymond, C., Gutierrez-Marques, P., Hall, I. Büttner, I. [2014b]. Icarus (239, 222-237)) and the <span class="hlt">olivine</span>-rich lithologies are of a similar age. The origin of some potential <span class="hlt">olivine</span>-rich sites in the Rheasilvia basin and at crater Portia are ambiguous, i.e. these are either of endogenic or exogenic origin. However, the small number and size of these sites led us to conclude that <span class="hlt">olivine</span>-rich mantle material, containing more than 40 wt.% of <span class="hlt">olivine</span>, is basically absent on the present surface of Vesta. In combination with recent impact models of Veneneia and Rheasilvia (Clenet, H., Jutzi</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.V43D..02C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.V43D..02C"><span>Helium Diffusion in <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cherniak, D. J.; Watson, E. B.</p> <p>2011-12-01</p> <p>Diffusion of helium has been characterized in natural Fe-bearing <span class="hlt">olivine</span> (~Fo90) and synthetic forsterite. Polished, oriented slabs of <span class="hlt">olivine</span> were implanted with 3He, at 100 keV at a dose of 5x1015/cm2 or at 3.0 MeV at a dose of 1x1016/cm2. A set of experiments on the implanted <span class="hlt">olivine</span> were run in 1-atm furnaces. In addition to the one-atm experiments, experiments on implanted samples were also run at higher pressures (2.6 and 2.7 GPa) to assess the potential effects of pressure on He diffusion and the applicability of the measured diffusivities in describing He transport in the mantle. The high-pressure experiments were conducted in a piston-cylinder apparatus using an "ultra-soft" pressure cell, with the diffusion sample directly surrounded by AgCl. 3He distributions following experiments were measured with Nuclear Reaction Analysis using the reaction 3He(d,p)4He. This direct profiling method permits us to evaluate anisotropy of diffusion, which cannot be easily assessed using bulk-release methods. For diffusion in forsterite parallel to c we obtain the following Arrhenius relation over the temperatures 250-950°C: D = 3.91x10-6exp(-159 ± 4 kJ mol-1/RT) m2/sec. The data define a single Arrhenius line spanning more than 7 orders of magnitude in D and 700°C in temperature. Diffusion parallel to a appears slightly slower, yielding an activation energy for diffusion of 135 kJ/mol and a pre-exponential factor of 3.73x10-8 m2/sec. Diffusion parallel to b is slower than diffusion parallel to a (by about two-thirds of a log unit); for this orientation an activation energy of 138 kJ/mol and a pre-exponential factor of 1.34x10-8 m2/sec are obtained. This anisotropy is broadly consistent with observations for diffusion of Ni and Fe-Mg in <span class="hlt">olivine</span>. Diffusion in Fe-bearing <span class="hlt">olivine</span> (transport parallel to b) agrees within uncertainty with findings for He diffusion in forsterite. The higher-pressure experiments yield diffusivities in agreement with those from the 1-atm</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('https://ntrs.nasa.gov/search.jsp?R=19930055821&hterms=GMT&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DGMT','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930055821&hterms=GMT&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DGMT"><span>Magombedze - A new H-chondrite with light-dark structure</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Macpherson, Glenn J.; Jarosewich, Eugene; Lowenstein, Peter</p> <p>1993-01-01</p> <p>Magombedze is a light-dark structured H-chondrite breccia that fell in Zimbabwe on July 2, 1990 at 15:30 GMT. White clasts are moderately shocked and have equilibrated mafic silicates (pyroxene Fs(16-18), <span class="hlt">olivine</span> Fa(18-19)) together with clear optically-recognizable plagioclase of variable composition (An(9-13) found); <span class="hlt">chondrules</span> are distinct but contain no trace of preserved glass. The darker surrounding material contains a higher proportion of fine-grained metal and sulfide than the white clasts, and many of its constituent grains show little evidence of shock. Mafic silicates in the dark lithology are distinctly less-equilibrated (pyroxene Fs(5-21), <span class="hlt">olivine</span> Fa(11-20)) than those in the white clasts, and many <span class="hlt">chondrules</span> preserve brown devitrified glass; some metamorphic plagioclase of variable composition (An(11-22) found) is present. Some monoclinic pyroxene occurs in both fractions, but it is relatively common in the dark fraction. The white clasts are classified as H5, and the enclosing dark material is H3-5.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990091993&hterms=boo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dboo','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990091993&hterms=boo&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dboo"><span>Thermal Emission Spectroscopy of 1 Ceres: Evidence for <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Witteborn, F. C.; Roush, T. L.; Cohen, M.</p> <p>1999-01-01</p> <p>Thermal emission spectra of the largest asteroid 1 Ceres obtained from the Kuiper Airborne Observatory display features that may provide information on its surface mineralogy. A plot of the Ceres spectrum (calibrated using alpha Boo as a standard) divided by a standard thermal model (STM) is shown. Also shown is the emissivity spectrum deduced from reflectivity measurements for <span class="hlt">olivine</span> grains <5 microns in diameter. The general shape of the Ceres and the <span class="hlt">olivine</span> curves agree in essential details, such as the maxima from 8 to 12 microns, the minimum between 12 and 14 microns, the broad peak near 17.5 micron, and the slope beyond 22 micron. (Use of the 10 to 15-micron grain reflectivities provides a better match to the 12- to 14-micron dip. We used a value of unity for beta, the beaming factor associated with small-scale surface roughness in our STM. Adjustment of beta to a lower value raises the long-wavelength side of the Ceres spectrum, providing an even better match to the <span class="hlt">olivine</span> curve.) The emissivity behavior roughly matches the emission coefficients which were calculated for <span class="hlt">olivine</span> particles with a particle radius of 3 microns. Their calculations show not only the negative slope from 23 to 25 pm, but a continued decrease past 30 micron. The Ceres emissivity is thus similar to that of small <span class="hlt">olivine</span> grains from 8 to 30 micron, but <span class="hlt">olivine</span>'s emissivity is lower from 5 to 8 pm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.6629S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.6629S"><span>Phosphorus as indicator of magmatic <span class="hlt">olivine</span> residence time, morphology and growth rate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sobolev, Alexander; Batanova, Valentina</p> <p>2015-04-01</p> <p>Phosphorus is among of slowest elements by diffusion rate in silicate melts and crystals (e.g. Spandler et al, 2007). In the same time it is moderately incompatible to compatible with <span class="hlt">olivine</span> (Brunet & Chazot, 2001; Grant & Kohn, 2013). This makes phosphorus valuable tracer of <span class="hlt">olivine</span> crystallization in natural conditions. Indeed, it is shown that natural magmatic <span class="hlt">olivine</span> crystals commonly posses strong and complicated zoning in phosphorus (Milman-Barris et al, 2008; Welsch et al, 2014). In this paper we intend to review phosphorus behavior in <span class="hlt">olivine</span> in published experimental and natural <span class="hlt">olivine</span> studies and present large set of new EPMA data on phosphorus zoning in <span class="hlt">olivine</span> phenocrysts from MORBs, OIBs, komatiites and kimberlites. We will show that sharp <span class="hlt">olivine</span> zones enriched in phosphorus by a factor of 10-20 over prediction by equilibrium partition may be due to formation of P-rich boundary layer on the interface of fast growing <span class="hlt">olivine</span>. This is proved by finding of small-size (normally 10 mkm or less) exceptionally P-rich melt inclusions in <span class="hlt">olivine</span>, which are otherwise similar in composition to typical melt. These observations could provide potential <span class="hlt">olivine</span> growth speedometer. We will also demonstrate, that sharp zoning in phosphorus may provide valuable information on the residence time of <span class="hlt">olivine</span> crystals in different environments: magma chambers and conduits as well as mantle sources. This study has been founded by Russian Science Foundation grant 14-17-00491. References: Spandler, et al, 2007, Nature, v. 447, p. 303-306; Brunet & Chazot, 2001, Chemical Geology, v. 176, p. 51-72; Grant & Kohn, 2013, American Mineralogist, v. 98, p. 1860-1869; Milman-Barris et al, 2008, Contr. Min. Petrol. v. 155, p.739-765; Welsch et al, 2014, Geology, v. 42, p.867-870.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29731517','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29731517"><span>Experimentally Determined Subsolidus Metal-<span class="hlt">Olivine</span> Element Partitioning with Applications to Pallasites.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Donohue, Patrick H; Hill, Eddy; Huss, Gary R</p> <p>2018-02-01</p> <p>Pallasite meteorites, which consist primarily of <span class="hlt">olivine</span> and metal, may be remnants of disrupted core-mantle boundaries of differentiated asteroids or planetesimals. The early thermal histories of pallasites are potentially recorded by minor- and trace-element zonation in <span class="hlt">olivine</span>. However, constraining this history requires knowledge of element behavior under the conditions of pallasite formation, which is lacking for many of the main elements of interest (e.g., Co, Cr, Mn). In this study, we experimentally determined metal/<span class="hlt">olivine</span> partition coefficients for Fe, Ni, Co, Cr, and Mn in a pallasite analogue at subsolidus temperatures. Metal/<span class="hlt">olivine</span> partition coefficients ( K M ) increase in the order K Mn < K Cr < 1 < K Fe < K Co < K Ni , with five orders of magnitude separating K Mn from K Ni . Transition metals also become more siderophile with increasing experimental temperature (900 to 1550°C). The experiments incidentally produced diffusion profiles in <span class="hlt">olivine</span> for these elements; Our results suggest they diffuse through <span class="hlt">olivine</span> at similar rates. Core compositions of pallasite <span class="hlt">olivines</span> are consistent with high-temperature equilibration with FeNi-metal. <span class="hlt">Olivine</span> zonation toward crystal rims varies significantly for the investigated transition metals. We suggest rim zonation results from partial re-equilibration during late stage crystallization of minor phases (e.g., chromite, phosphates). This re- equilibration occurred over short timescales relative to overall pallasite cooling, likely tied to initial cooling rates on the order of 100-300°C/Myr.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1422289-synthesis-nanometer-sized-fayalite-magnesium-iron-ii-mixture-olivines','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1422289-synthesis-nanometer-sized-fayalite-magnesium-iron-ii-mixture-olivines"><span>Synthesis of nanometer-sized fayalite and magnesium-iron(II) mixture <span class="hlt">olivines</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>Qafoku, Odeta; Ilton, Eugene S.; Bowden, Mark E.</p> <p></p> <p><span class="hlt">Olivines</span> are divalent orthosilicates with important geologic, biological, and industrial significance and are typically comprised of mixtures of Mg2+ and Fe2+ ranging from forsterite (Mg2SiO4) to fayalite (Fe2SiO4). Investigating the role of Fe(II) in <span class="hlt">olivine</span> reactivity requires the ability to synthesize <span class="hlt">olivines</span> that are nanometer-sized, have different percentages of Mg2+ and Fe2+, and have good bulk and surface purity. This article demonstrates a new method for synthesizing nanosized fayalite and Mg-Fe mixture <span class="hlt">olivines</span>. First, carbonaceous precursors are generated from sucrose, PVA, colloidal silica, Mg2+, and Fe3+. Second, these precursors are calcined in air to burn carbon and create mixtures ofmore » Fe(III)-oxides, forsterite, and SiO2. Finally, calcination in reducing CO-CO2 gas buffer leads to Fe(II)-rich <span class="hlt">olivines</span>. XRD, Mössbauer, and IR analyses verify good bulk purity and composition. XPS indicates that surface iron is in its reduced Fe(II) form, and surface Si is consistent with <span class="hlt">olivine</span>. SEM shows particle sizes predominately between 50 and 450 nm, and BET surface areas are 2.8-4.2 m2/g. STEM HAADF analysis demonstrates even distributions of Mg and Fe among the available M1 and M2 sites of the <span class="hlt">olivine</span> crystals. These nanosized Fe(II)-rich <span class="hlt">olivines</span> are suitable for laboratory studies with in situ probes that require mineral samples with high reactivity at short timescales.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22521780-redistribution-alkaline-elements-association-aqueous-activity-early-solar-system','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22521780-redistribution-alkaline-elements-association-aqueous-activity-early-solar-system"><span>REDISTRIBUTION OF ALKALINE ELEMENTS IN ASSOCIATION WITH AQUEOUS ACTIVITY IN THE EARLY SOLAR SYSTEM</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>Hidaka, Hiroshi; Higuchi, Takuya; Yoneda, Shigekazu, E-mail: hidaka@hiroshima-u.ac.jp, E-mail: s-yoneda@kahaku.go.jp</p> <p>2015-12-10</p> <p>It is known that the Sayama meteorite (CM2) shows an extensive signature for aqueous alteration on the meteorite parent body, and that most of the primary minerals in the <span class="hlt">chondrules</span> are replaced with phyllosilicates as the result of the aqueous alteration. In this paper, it is confirmed from the observation of two-dimensional Raman spectra that a part of <span class="hlt">olivine</span> in a <span class="hlt">chondrule</span> collected from the Sayama chondrite is serperntinized. Ion microprobe analysis of the <span class="hlt">chondrule</span> showed that alkaline elements such as Rb and Cs are heterogeneously redistributed in the <span class="hlt">chondrule</span>. The result of higher Rb and Cs contents in serpentinizedmore » phases in the <span class="hlt">chondrule</span> rather than in other parts suggested the selective adsorption of alkaline elements into the serpentine in association with early aqueous activity on the meteorite parent body. Furthermore Ba isotopic analysis provided variations of {sup 135}Ba/{sup 138}Ba and {sup 137}Ba/{sup 138}Ba in the <span class="hlt">chondrule</span>. This result was consistent with our previous isotopic data suggesting isotopic evidence for the existence of the presently extinct nuclide {sup 135}Cs in the Sayama meteorite, but the abundance of {sup 135}Cs in the solar system remains unclear because of large analytical uncertainties.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950012918&hterms=fine+dust&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dfine%2Bdust','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950012918&hterms=fine+dust&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dfine%2Bdust"><span>The fine nebula dust component: A key to <span class="hlt">chondrule</span> formation by lightning</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wasson, J. T.; Rasmussen, K. L.</p> <p>1994-01-01</p> <p>Our assessment indicates that <span class="hlt">chondrule</span> formation by lightning is indeed possible in the solar nebula. Previously the overriding objection to the lightning process of <span class="hlt">chondrule</span> formation has been that low nebula pressures prevented the buildup of large potential differences. The breakdown potential is controlled by the mean free live distance of an electron. We calculate the mean free live distance in pure H2 gas at 2 AU to be approximately 500 m. A fine dust load constituting 4 wt% of the dust in the dusty midplane region leads to a reduced mean free live distance of only 7 m. Very conservatively we estimate the breakdown potential to be at least 10, 1.8, and 0.7 V/cm at 1, 2, and 3 AU respectively. We set the radius of the lightning bolt equal to the kinetic mean free path of the gas. Our calculations based on electron drift velocities in a fully ionized H2 gas show that first strike durations are 0.96, 3.4, and 7.0 ms at 1, 2, and 3 AU respectively, in much better accordance with the meteoritic evidence than previous estimates of 10-100 s.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100008965','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100008965"><span><span class="hlt">Olivine</span> in Almahata Sitta - Curiouser and Curiouser</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zolensky, M. E.; Herrin, J.; Mikouchi, T.; Satake, W.; Kurihara, T.; Sandford, S. A.; Milam, S. N.; Hagiya, K.; Ohsumi, K.; Friedrich, J. M.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20100008965'); toggleEditAbsImage('author_20100008965_show'); toggleEditAbsImage('author_20100008965_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20100008965_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20100008965_hide"></p> <p>2010-01-01</p> <p>Almahata Sitta (hereafter Alma) is an anomalous, polymict ureilite. Anomalous features include low abundance of <span class="hlt">olivine</span>, large compositional range of silicates, high abundance and large size of pores, crystalline pore wall linings, and overall finegrained texture. Tomography suggests the presence of foliation, which is known from other ureilites. Alma pyroxenes and their interpretation are discussed in two companion abstracts. In this abstract we discuss the composition of <span class="hlt">olivine</span> in Alma, which is indicative of the complexity of this meteorite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005ApJ...621L.137B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005ApJ...621L.137B"><span><span class="hlt">Chondrule</span>-forming Shock Fronts in the Solar Nebula: A Possible Unified Scenario for Planet and Chondrite Formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boss, A. P.; Durisen, R. H.</p> <p>2005-03-01</p> <p><span class="hlt">Chondrules</span> are millimeter-sized spherules found throughout primitive chondritic meteorites. Flash heating by a shock front is the leading explanation of their formation. However, identifying a mechanism for creating shock fronts inside the solar nebula has been difficult. In a gaseous disk capable of forming Jupiter, the disk must have been marginally gravitationally unstable at and beyond Jupiter's orbit. We show that this instability can drive inward spiral shock fronts with shock speeds of up to ~10 km s-1 at asteroidal orbits, sufficient to account for <span class="hlt">chondrule</span> formation. The mixing and transport of solids in such a disk, combined with the planet-forming tendencies of gravitational instabilities, results in a unified scenario linking chondrite production with gas giant planet formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780062717&hterms=trivalent+chromium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtrivalent%2Bchromium','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780062717&hterms=trivalent+chromium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dtrivalent%2Bchromium"><span>Minor elements in lunar <span class="hlt">olivine</span> as a petrologic indicator</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steele, I. M.; Smith, J. V.</p> <p>1975-01-01</p> <p>Accurate electron microprobe analyses (approximately 50 ppm) were made for Al, Ca, Ti, Cr, Mn, and Ni in Mg-rich <span class="hlt">olivines</span> which may derive from early lunar crust or deeper environments. Low-Ca contents consistently occur only in <span class="hlt">olivines</span> from dunitic and troctolitic breccia: spinel troctolite and other rock types have high-Ca <span class="hlt">olivines</span> suggesting derivation by near-surface processes. Rock 15445 has <span class="hlt">olivine</span> with distinctly low CaO (approximately 0.01 wt.%). Chromium ranges to higher values (max.0.2 oxide wt.%) than for terrestrial harzburgites and lherzolites but is similar to the range in terrestrial komatiites. Divalent chromium may be indicated over trivalent Cr because <span class="hlt">olivines</span> lack sufficient other elements for charge balance of the latter. NiO values in lunar specimens range from 0.00 to 0.07 wt.% and a weak anticorrelation with Cr2O3 suggests an oxidation state effect. Al2O3 values are mostly below 0.04-wt.% and show no obvious correlation with fragment type. TiO2 values lie below 0.13-wt.% and seem to correlate best with crystallization rate and plagioclase content of the host rock. High values of Al2O3 and TiO2 reported by other workers have not been confirmed, and are probably wrong.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/588524-elastic-constants-san-carlos-olivine-gpa','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/588524-elastic-constants-san-carlos-olivine-gpa"><span>The elastic constants of San Carlos <span class="hlt">olivine</span> to 17 GPa</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>Abramson, E.H.; Brown, J.M.; Slutsky, L.J.</p> <p>1997-06-01</p> <p>All elastic constants, the average bulk and shear moduli, and the lattice parameters of San Carlos <span class="hlt">olivine</span> (Fo{sub 90}) (initial density 3.355gm/cm{sup 3}) have been determined to a pressure of 12 GPa at room temperature. Measurements of c{sub 11}, c{sub 33}, c{sub 13}, and c{sub 55} have been extended to 17 GPa. The pressure dependence of the adiabatic, isotropic (Hashin-Shtrikman bounds) bulk modulus, and shear modulus may be expressed as K{sub HS}=129.4+4.29P and by G{sub HS}=78+1.71P{minus}0.027P{sup 2}, where both the pressure and the moduli are in gigapascals. The isothermal compression of <span class="hlt">olivine</span> is described by a bulk modulus given asmore » K{sub T}=126.3+4.28P. Elastic constants other than c{sub 55} can be adequately represented by a linear relationship in pressure. In the order (c{sub 11},c{sub 12},c{sub 13},c{sub 22},c{sub 23},c{sub 33},c{sub 44},c{sub 55},c{sub 66}) the 1 <span class="hlt">bar</span> intercepts (gigapascal units) are (320.5, 68.1, 71.6, 196.5, 76.8, 233.5, 64.0, 77.0, 78.7). The first derivatives are (6.54, 3.86, 3.57, 5.38, 3.37, 5.51, 1.67, 1.81, 1.93). The second derivative for c{sub 55} is {minus}0.070GPa{sup {minus}1}. Incompressibilities for the three axes may also be expressed as linear relationships with pressure. In the order of {bold a, b}, and {bold c} axes the intercepts in gigapascals are (547.8, 285.8, 381.8) and the first derivatives are (20.1, 12.3, 14.0).{copyright} 1997 American Geophysical Union« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70017600','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70017600"><span>Role of <span class="hlt">olivine</span> cumulates in destabilizing the flanks of Hawaiian volcanoes</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Clague, D.A.; Denlinger, R.P.</p> <p>1994-01-01</p> <p>The south flank of Kilauea Volcano is unstable and has the structure of a huge landslide; it is one of at least 17 enormous catastrophic landslides shed from the Hawaiian Islands. Mechanisms previously proposed for movement of the south flank invoke slip of the volcanic pile over seafloor sediments. Slip on a low friction de??collement alone cannot explain why the thickest and widest sector of the flank moves more rapidly than the rest, or why this section contains a 300 km3 aseismic volume above the seismically defined de??collement. It is proposed that this aseismic volume, adjacent to the caldera in the direction of flank slip, consists of <span class="hlt">olivine</span> cumulates that creep outward, pushing the south flank seawards. Average primary Kilauea tholeiitic magma contains about 16.5 wt.% MgO compared with an average 10 wt.% MgO for erupted subaerial and submarine basalts. This difference requires fractionation of 17 wt.% (14 vol.%) <span class="hlt">olivine</span> phenocrysts that accumulate near the base of the magma reservoir where they form cumulates. Submarine-erupted Kilauea lavas contain abundant deformed <span class="hlt">olivine</span> xenocrysts derived from these cumulates. Deformed dunite formed during the tholeiitic shield stage is also erupted as xenoliths in subsequent alkalic lavas. The deformation structures in <span class="hlt">olivine</span> xenocrysts suggest that the cumulus <span class="hlt">olivine</span> was densely packed, probably with as little as 5-10 vol.% intercumulus liquid, before entrainment of the xenocrysts. The <span class="hlt">olivine</span> cumulates were at magmatic temperatures (>1100??C) when the xenocrysts were entrained. <span class="hlt">Olivine</span> at 1100??C has a rheology similar to ice, and the <span class="hlt">olivine</span> cumulates should flow down and away from the summit of the volcano. Flow of the <span class="hlt">olivine</span> cumulates places constant pressure on the unbuttressed seaward flank, leading to an extensional region that localizes deep intrusions behind the flank; these intrusions add to the seaward push. This mechanism ties the source of gravitational instability to the caldera complex and deep</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987eprs.nasaR....B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987eprs.nasaR....B"><span>Experimental constraints on the origin of <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boynton, W. V.; Drake; Hildebrand; Jones; Lewis; Treiman; Wark</p> <p>1987-11-01</p> <p>Chrondule formation was an important (perhaps ubiguitous) process in the early solar system, yet their origins remain elusive. Some points, however, are clear. The precursor material of chondules (dust) was rapidly heated at rates of perhaps thousands of degrees per second and was cooled more slowly. It was proposed to investigate <span class="hlt">chondrule</span> formation in the Space Station environment via a dust-box (a chamber in which dust can be suspended, heated, and cooled. A microgravity environment is conducive to this kind of experiment because of the significant retardation of settling rates compared with a terrestrial laboratory environment. These long-duration experiments might require the development of technologies to counteract even the small, but finite and permanent gravitation field of the Space Station. Simple, but interesting experiments on dust suspensions immediately present themselves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012GeCoA..95..169S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012GeCoA..95..169S"><span>Inherited Pb isotopic records in <span class="hlt">olivine</span> antecryst-hosted melt inclusions from Hawaiian lavas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sakyi, Patrick Asamoah; Tanaka, Ryoji; Kobayashi, Katsura; Nakamura, Eizo</p> <p>2012-10-01</p> <p>Dislocation textures of <span class="hlt">olivine</span> grains and Pb isotopic compositions (207Pb/206Pb and 208Pb/206Pb) of <span class="hlt">olivine</span>-hosted melt inclusions in basaltic lavas from three Hawaiian volcanoes (Kilauea, Mauna Loa, and Koolau) were examined. More than 70% of the blocky <span class="hlt">olivine</span> grains in the studied samples have a regular-shaped dislocation texture with their dislocation densities exceeding 106 cm-2, and can be considered as deformed <span class="hlt">olivine</span>. The size distribution of blocky <span class="hlt">olivine</span> grains shows that more than 99% of blocky <span class="hlt">olivines</span> coarser than 1.2 mm are identified as deformed <span class="hlt">olivine</span>. These deformed <span class="hlt">olivine</span> grains are identified as antecrysts, which originally crystallized from previous stages of magmatism in the same shield, followed by plastic deformation prior to entrainment in the erupted host magmas. This study revealed that entrainment of mantle-derived crystallization products by younger batches of magma is an important part of the evolution of magnesium-rich Hawaiian magma. Lead isotopic compositions of melt inclusions hosted in the <span class="hlt">olivine</span> antecrysts provide information of the evolutionary history of Hawaiian volcanoes which could not have been accessed if only whole rock analyses were carried out. Antecryst-hosted melt inclusions in Kilauea and Koolau lavas demonstrate that the source components in the melting region changed during shield formation. In particular, evidence of interaction of plume-derived melts and upper mantle was observed in the earliest stage of Koolau magmatism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014GeCoA.142...27U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014GeCoA.142...27U"><span>Experimental investigation of condensation predictions for dust-enriched systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ustunisik, Gokce; Ebel, Denton S.; Walker, David; Boesenberg, Joseph S.</p> <p>2014-10-01</p> <p>Condensation models describe the equilibrium distribution of elements between coexisting phases (mineral solid solutions, silicate liquid, and vapor) in a closed chemical system, where the vapor phase is always present, using equations of state of the phases involved at a fixed total pressure (<1 <span class="hlt">bar</span>) and temperature (T). The VAPORS code uses a CaO-MgO-Al2O3-SiO2 (CMAS) liquid model at T above the stability field of <span class="hlt">olivine</span>, and the MELTS thermodynamics algorithm at lower T. Quenched high-T crystal + liquid assemblages are preserved in meteorites as Type B Ca-, Al-rich inclusions (CAIs), and <span class="hlt">olivine</span>-rich ferromagnesian <span class="hlt">chondrules</span>. Experimental tests of compositional regions within 100 K of the predicted T of <span class="hlt">olivine</span> stability may clarify the nature of the phases present, the phase boundaries, and the partition of trace elements among these phases. Twenty-three Pt-loop equilibrium experiments in seven phase fields on twelve bulk compositions at specific T and dust enrichment factors tested the predicted stability fields of forsteritic <span class="hlt">olivine</span> (Mg2SiO4), enstatite (MgSiO3), Cr-bearing spinel (MgAl2O4), perovskite (CaTiO3), melilite (Ca2Al2SiO7-Ca2Mg2Si2O7) and/or grossite (CaAl4O7) crystallizing from liquid. Experimental results for forsterite, enstatite, and grossite are in very good agreement with predictions, both in chemistry and phase abundances. On the other hand the stability of spinel with <span class="hlt">olivine</span>, and stability of perovskite and gehlenite are quite different from predictions. Perovskite is absent in all experiments. Even at low oxygen fugacity (IW-3.4), the most TiO2-rich experiments do not crystallize Al-, Ti-bearing calcic pyroxene. The stability of spinel and <span class="hlt">olivine</span> together is limited to a smaller phase field than is predicted. The melilite stability field is much larger than predicted, indicating a deficiency of current liquid or melilite activity models. In that respect, these experiments contribute to improving the data for calibrating thermodynamic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.468...62P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.468...62P"><span>The origin of volatile element depletion in early solar system material: Clues from Zn isotopes in <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pringle, Emily A.; Moynier, Frédéric; Beck, Pierre; Paniello, Randal; Hezel, Dominik C.</p> <p>2017-06-01</p> <p>Volatile lithophile elements are depleted in the different planetary materials to various degrees, but the origin of these depletions is still debated. Stable isotopes of moderately volatile elements such as Zn can be used to understand the origin of volatile element depletions. Samples with significant volatile element depletions, including the Moon and terrestrial tektites, display heavy Zn isotope compositions (i.e. enrichment of 66Zn vs. 64Zn), consistent with kinetic Zn isotope fractionation during evaporation. However, Luck et al. (2005) found a negative correlation between δ66Zn and 1/[Zn] between CI, CM, CO, and CV chondrites, opposite to what would be expected if evaporation caused the Zn abundance variations among chondrite groups. We have analyzed the Zn isotope composition of multiple samples of the major carbonaceous chondrite classes: CI (1), CM (4), CV (2), CO (4), CB (2), CH (2), CK (4), and CK/CR (1). The bulk chondrites define a negative correlation in a plot of δ66Zn vs 1/[Zn], confirming earlier results that Zn abundance variations among carbonaceous chondrites cannot be explained by evaporation. Exceptions are CB and CH chondrites, which display Zn systematics consistent with a collisional formation mechanism that created enrichment in heavy Zn isotopes relative to the trend defined by CI-CK. We further report Zn isotope analyses of chondrite components, including <span class="hlt">chondrules</span> from Allende (CV3) and Mokoia (CV3), as well as an aliquot of Allende matrix. All <span class="hlt">chondrules</span> are enriched in light Zn isotopes (∼500 ppm on 66Zn/64Zn) relative to the bulk, contrary to what would be expected if Zn were depleted during evaporation, on the other hand the matrix has a complementary heavy isotope composition. We report sequential leaching experiments in un-equilibrated ordinary chondrites, which show sulfides are isotopically heavy compared to silicates and the bulk meteorite by ca. +0.65 per mil on 66Zn/64Zn. We suggest isotopically heavy sulfides were</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910018789','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910018789"><span>Moessbauer spectroscopy and scanning electron microscopy of the Murchison meteorite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brown, Christopher L.; Oliver, Frederick W.; Hammond, Ernest C., Jr.</p> <p>1989-01-01</p> <p>Meteorites provide a wealth of information about the solar system's formation, since they have similar building blocks as the Earth's crust but have been virtually unaltered since their formation. Some stony meteorites contain minerals and silicate inclusions, called <span class="hlt">chondrules</span>, in the matrix. Utilizing Moessbauer spectroscopy, we identified minerals in the Murchison meteorite, a carbonaceous chondritic meteorite, by the gamma ray resonance lines observed. Absorption patterns of the spectra were found due to the minerals <span class="hlt">olivine</span> and phyllosilicate. We used a scanning electron microscope to describe the structure of the <span class="hlt">chondrules</span> in the Murchison meteorite. The <span class="hlt">chondrules</span> were found to be deformed due to weathering of the meteorite. Diameters varied in size from 0.2 to 0.5 mm. Further enhancement of the microscopic imagery using a digital image processor was used to describe the physical characteristics of the inclusions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995GeCoA..59.2291B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995GeCoA..59.2291B"><span>Aqueous alteration and brecciation in Bells, an unusual, saponite-bearing, CM chondrite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brearley, Adrian J.</p> <p>1995-06-01</p> <p>The petrological and mineralogical characteristics of the unusual CM2 chondrite, Bells, have been investigated in detail by scanning electron microscopy (SEM), electron microprobe analysis (EPMA), and transmission electron microscopy (TEM). Bells is a highly brecciated chondrite which contains few intact <span class="hlt">chondrules</span>, a very low abundance of refractory inclusions, and is notable in having an unusually high abundance of magnetite, which is disseminated throughout the fine-grained matrix. Fragmental <span class="hlt">olivines</span> and pyroxenes are common and, based on compositional data, appear to have been derived from <span class="hlt">chondrules</span> as a result of extensive brecciation. The fine-grained mineralogy of matrix in Bells differs considerably from other CM chondrites and has closer affinities to matrix in CI chondrites. The dominant phases are fine-grained saponite interlayered with serpentine, and phases such as tochilinite and cronstedtite, which are typical of CM chondrite matrices, are entirely absent. Pentlandite, pyrrhotite, magnetite, anhydrite, calcite, and rare Ti-oxides also occur as accessory phases. Based on its oxygen and noble gas isotopic compositions (Zadnik, 1985; Rowe et al., 1994), Bells can be considered to be a CM2 chondrite, although its bulk composition shows some departures from the typical range exhibited by this group. However, these variations in bulk chemistry are entirely consistent with the observed mineralogy of Bells. The unusual fine-grained mineralogy of Bells matrix can be reasonably attributed to the combined effects of aqueous alteration and advanced brecciation in a parent body environment. Extensive brecciation has assisted aqueous alteration by reducing <span class="hlt">chondrules</span> and mineral grains into progressively smaller grains with high surface areas, which are more susceptible to dissolution reactions involving aqueous fluids. This has resulted in the preferential dissolution of Fe-rich <span class="hlt">chondrule</span> <span class="hlt">olivines</span>, which are now completely absent in Bells although present in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120007401','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120007401"><span>Trace Element Compositions of Pallasite <span class="hlt">Olivine</span> Grains and Pallasite Origin</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mittlefehldt, David W.; Herrin, J. S.</p> <p>2010-01-01</p> <p>Pallasites are mixtures of metal with magnesian <span class="hlt">olivine</span>. Most have similar metal compositions and <span class="hlt">olivine</span> oxygen isotopic compositions; these are the main-group pallasites (PMG). The Eagle Station grouplet of pallasites (PES) have distinctive metal and <span class="hlt">olivine</span> compositions and oxygen isotopic compositions. Pallasites are thought to have formed at the core-mantle boundary of their parent asteroids by mixing molten metal with solid <span class="hlt">olivine</span> of either cumulatic or restitic origin. We have continued our investigation of pallasite <span class="hlt">olivines</span> by doing in situ trace element analyses in order to further constrain their origin. We determined Al, P, Ca, Ga and first row transition element contents of <span class="hlt">olivine</span> grains from suite of PMG and PES by LA-ICP-MS at JSC. Included in the PMG suite are some that have anomalous metal compositions (PMG-am) and atypically ferroan <span class="hlt">olivines</span> (PMG-as). Our EMPA work has shown that there are unanticipated variations in <span class="hlt">olivine</span> Fe/Mn, even within those PMG that have uni-form Fe/Mg. Manganese is homologous with Fe2+, and thus can be used the same way to investigate magmatic fractionation processes. It has an advantage for pallasite studies in that it is unaffected by redox exchange with the metal. PMG can be divided into three clusters on the basis of Mn/Mg; low, medium and high that can be thought of as less, typically and more fractionated in an igneous sense. The majority of PMG have medium Mn/Mg ratios. PMG-am occur in all three clusters; there does not seem to be any relationship between putative <span class="hlt">olivine</span> igneous fractionation and metal composition. The PMG-as and one PMG-am make up the high Mn/Mg cluster; no PMG are in this cluster. The high Mn/Mg cluster ought to be the most fractionated (equivalent to the most Fe-rich in igneous suites), yet they have among the lowest contents of incompatible lithophile elements Al and Ti and the two PMG-as in this cluster also have low Ca and Sc contents. This is inconsistent with simple igneous</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.483...90N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.483...90N"><span>Mantle-derived trace element variability in <span class="hlt">olivines</span> and their melt inclusions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Neave, David A.; Shorttle, Oliver; Oeser, Martin; Weyer, Stefan; Kobayashi, Katsura</p> <p>2018-02-01</p> <p>Trace element variability in oceanic basalts is commonly used to constrain the physics of mantle melting and the chemistry of Earth's deep interior. However, the geochemical properties of mantle melts are often overprinted by mixing and crystallisation processes during ascent and storage. Studying primitive melt inclusions offers one solution to this problem, but the fidelity of the melt-inclusion archive to bulk magma chemistry has been repeatedly questioned. To provide a novel check of the melt inclusion record, we present new major and trace element analyses from <span class="hlt">olivine</span> macrocrysts in the products of two geographically proximal, yet compositionally distinct, primitive eruptions from the Reykjanes Peninsula of Iceland. By combining these macrocryst analyses with new and published melt inclusion analyses we demonstrate that <span class="hlt">olivines</span> have similar patterns of incompatible trace element (ITE) variability to the inclusions they host, capturing chemical systematics on intra- and inter-eruption scales. ITE variability (element concentrations, ratios, variances and variance ratios) in <span class="hlt">olivines</span> from the ITE-enriched Stapafell eruption is best accounted for by <span class="hlt">olivine</span>-dominated fractional crystallisation. In contrast, ITE variability in <span class="hlt">olivines</span> and inclusions from the ITE-depleted Háleyjabunga eruption cannot be explained by crystallisation alone, and must have originated in the mantle. Compatible trace element (CTE) variability is best described by crystallisation processes in both eruptions. Modest correlations between host and inclusion ITE contents in samples from Háleyjabunga suggest that melt inclusions can be faithful archives of melting and magmatic processes. It also indicates that degrees of ITE enrichment can be estimated from <span class="hlt">olivines</span> directly when melt inclusion and matrix glass records of geochemical variability are poor or absent. Inter-eruption differences in <span class="hlt">olivine</span> ITE systematics between Stapafell and Háleyjabunga mirror differences in 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_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=20050165543&hterms=coagulation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dcoagulation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050165543&hterms=coagulation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dcoagulation"><span>Chondrites and the Protoplanetary Disk, Part 2</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2004-01-01</p> <p>Contents include the following: On the Dynamical Evolution of a Nebula and Its Effect on Dust Coagulation and the Formation of Centimeter-sized Particles. The Mineralogy and Grain Properties of the Disk Surfaces in Three Herbig Ae/Be Stars. Astrophysical Observations of Disk Evolution Around Solar Mass Stars. The Systematic Petrology of Chondrites: A Consistent Approach to Assist Classification and Interpretation. Understanding Our Origins: Formation of Sun-like Stars in H II Region Environments. <span class="hlt">Chondrule</span> Crystallization Experiments. Formation of SiO2-rich <span class="hlt">Chondrules</span> by Fractional Condensation. Refractory Forsterites from Murchison (CM2) and Yamato 81020 (CO3.0) Chondrites: Cathodoluminescence, Chemical Compositions and Oxygen Isotopes. Apparent I-Xe Cooling Rates of <span class="hlt">Chondrules</span> Compared with Silicates from the Colomera Iron Meteorite. <span class="hlt">Chondrule</span> Formation in Planetesimal Bow Shocks: Physical Processes in the Near Vicinity of the Planetesimal. Genetic Relationships Between <span class="hlt">Chondrules</span>, Rims and Matrix. Chondrite Fractionation was Cosmochemical; <span class="hlt">Chondrule</span> Fractionation was Geochemical. <span class="hlt">Chondrule</span> Formation and Accretion of Chondrite Parent Bodies: Environmental Constraints. Amoeboid <span class="hlt">Olivine</span> Aggregates from the Semarkona LL3.0 Chondrite. The Evolution of Solids in Proto-Planetary Disks. New Nickel Vapor Pressure Measurements: Possible Implications for Nebular Condensates. Chemical, Mineralogical and Isotopic Properties of <span class="hlt">Chondrules</span>: Clues to Their Origin. Maximal Size of <span class="hlt">Chondrules</span> in Shock-Wave Heating Model: Stripping of Liquid Surface in Hypersonic Rarefied Gas Flow. The Nature and Origin of Interplanetary Dust: High Temperature Components. Refractory Relic Components in <span class="hlt">Chondrules</span> from Ordinary Chondrites. Constraints on the Origin of <span class="hlt">Chondrules</span> and CAIs from Short-lived and Long-lived Radionuclides. The Genetic Relationship Between Refractory Inclusions and <span class="hlt">Chondrules</span>. Contemporaneous <span class="hlt">Chondrule</span> Formation Between Ordinary and Carbonaceous Chondrites. <span class="hlt">Chondrules</span> and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998CoMP..132..139T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998CoMP..132..139T"><span>High pressure breakdown of antigorite to spinifex-textured <span class="hlt">olivine</span> and orthopyroxene, SE Spain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Trommsdorff, V.; Sánchez-Vizcaíno, V. López; Gómez-Pugnaire, M. T.; Müntener, O.</p> <p></p> <p>The prograde, high pressure, transition from antigorite serpentinite to enstatite-<span class="hlt">olivine</span> rock occurs along a tectonically undisturbed profile at Cerro del Almirez, SE Spain. The reactant assemblage is antigorite + <span class="hlt">olivine</span> with tremolite rimming precursor diopside. The product assemblage of tremolite + chlorite + enstatite + <span class="hlt">olivine</span> has a spinifex-like texture with arborescent or radiating <span class="hlt">olivine</span> elongated parallel to [001] and with radially grown enstatite. Product enstatite is very poor in Al2O3. Due to numerous oriented submicroscopic inclusions of chromian magnetite, product <span class="hlt">olivine</span> has a brownish pleochroism and a bulk chromium content similar to precursor antigorite. Titanian clinohumite with a fluorine content of 0.45-0.50 wt% persisted beyond the breakdown of antigorite. The partitioning of iron and magnesium amongst the silicate phases is almost identical to that at lower pressures. Average Kd values Mn/Mg and Ni/Mg are 0.17 and 0.70 for antigorite-<span class="hlt">olivine</span> pairs and 1.83 and 0.22 for orthopyroxene-<span class="hlt">olivine</span> pairs, respectively. These data are useful in discriminating generations of <span class="hlt">olivine</span> grown on each other. From the field data a phase diagram topology for a portion of the system CaO-MgO-SiO2-H2O is derived. This topology forms the basis for extrapolations into inaccessible P-T regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110005444','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110005444"><span>Effect of Sulfur on Siderophile Element Partitioning Between <span class="hlt">Olivine</span> and Martian Primary Melt</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Usui, T.; Shearer, C. K.; Righter, K.; Jones, J. H.</p> <p>2011-01-01</p> <p>Since <span class="hlt">olivine</span> is a common early crystallizing phase in basaltic magmas that have produced planetary and asteroidal crusts, a number of experimental studies have investigated elemental partitioning between <span class="hlt">olivine</span> and silicate melt [e.g., 1, 2, 3]. In particular, <span class="hlt">olivine</span>/melt partition coefficients of Ni and Co (DNi and DCo) have been intensively studied because these elements are preferentially partitioned into <span class="hlt">olivine</span> and thus provide a uniquely useful insight into the basalt petrogenesis [e.g., 4, 5]. However, none of these experimental studies are consistent with incompatible signatures of Co [e.g., 6, 7, 8] and Ni [7] in <span class="hlt">olivines</span> from Martian meteorites. Chemical analyses of undegassed MORB samples suggest that S dissolved in silicate melts can reduce DNi up to 50 % compared to S-free experimental systems [9]. High S solubility (up to 4000 ppm) for primitive shergottite melts [10] implies that S might have significantly influenced the Ni and Co partitioning into shergottite <span class="hlt">olivines</span>. This study conducts melting experiments on Martian magmatic conditions to investigate the effect of S on the partitioning of siderophile elements between <span class="hlt">olivine</span> and Martian primary melt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMMR22A..05F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMMR22A..05F"><span>Water Retention and Rheology of Ti-doped, Synthetic <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faul, U.; Jackson, I.; Fitz Gerald, J. D.</p> <p>2012-12-01</p> <p>Upper mantle flow laws are currently based almost entirely on experiments with <span class="hlt">olivine</span> from San Carlos in Arizona. Synthetically produced <span class="hlt">olivine</span> enables the exploration of the effects of trace elements on the rheology. We have conducted a range of experiments in a gas medium apparatus with solution-gelation derived <span class="hlt">olivine</span> that show that titanium is the most effective in binding water in the <span class="hlt">olivine</span> structure. The FTIR signature of this structurally bound water is most similar to that of water-undersaturated natural <span class="hlt">olivine</span> with absorption bands at 3575 and 3525 cm-1. Water added, titanium-free solgel contains little water after hotpressing and shows adsorption bands at wavenumbers near 3200 cm-1. Noble metal capsules such as Pt or AuPd, providing more oxidizing conditions, are more effective in retaining water. Experiments with NiFe-lined welded Pt capsules retain no more water than NiFe lined samples without Pt capsule. Water retention is, however, again dependent on trace element content, with Ti doped samples containing tens of ppm after hotpressing. By comparison undoped samples run under the same conditions contain little water, again with different FTIR spectra to Ti-doped samples. Our experiments suggest that Ti by itself, or with water contents at the FTIR detection limit enhances diffusion creep rates relative to undoped, dry solgel <span class="hlt">olivine</span>. Water contents around 10 ppm in NiFe wrapped samples show an enhancement of strain rates of more than one order of magnitude. The addition of Ti, together with the presence of water, also enhances grain growth. For more coarse-grained samples in the dislocation creep regime the enhancement of the stain rate as a function of water content is approximately consistent with the flow laws of Hirth and Kohlstedt (2003).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010044721&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DXxxii','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010044721&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DXxxii"><span>A Parent Magma for the Nakhla Martian Meteorite: Reconciliation of Estimates from 1-<span class="hlt">Bar</span> Experiments, Magmatic Inclusions in <span class="hlt">Olivine</span>, and Magmatic Inclusions in Augite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Treiman, Allan H.; Goodrich, Cyrena Anne</p> <p>2001-01-01</p> <p>The composition of the parent magma for the Nakhla (martian) meteorite has been estimated from mineral-melt partitioning and from magmatic inclusions in <span class="hlt">olivine</span> and in augite. These independent lines of evidence have converged on small range of likely compositions. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940011778','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940011778"><span>Gas-grain energy transfer in solar nebula shock waves: Implications for the origin of <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hood, L. L.; Horanyi, M.</p> <p>1993-01-01</p> <p>Meteoritic <span class="hlt">chondrules</span> provide evidence for the occurrence of rapid transient heating events in the protoplanetary nebula. Astronomical evidence suggests that gas dynamic shock waves are likely to be excited in protostellar accretion disks by processes such as protosolar mass ejections, nonaxisymmetric structures in an evolving disk, and impact on the nebula surface of infalling 'clumps' of circumstellar gas. Previous detailed calculations of gas-grain energy and momentum transfer have supported the possibility that such shock waves could have melted pre-existing <span class="hlt">chondrule</span>-sized grains. The main requirement for grains to reach melting temperatures in shock waves with plausibly low Mach numbers is that grains existed in dust-rich zones (optical depth greater than 1) where radiative cooling of a given grain can be nearly balanced by radiation from surrounding grains. Localized dust-rich zones also provide a means of explaining the apparent small spatial scale of heating events. For example, the scale size of at least some optically thick dust-rich zones must have been relatively small (less than 10 kilometers) to be consistent with petrologic evidence for accretion of hot material onto cold <span class="hlt">chondrules</span>. The implied number density of mm-sized grains for these zones would be greater than 30 m(exp -3). In this paper, we make several improvements of our earlier calculations to include radiation self-consistently in the shock jump conditions, and we include heating of grains due to radiation from the shocked gas. In addition, we estimate the importance of momentum feedback of dust concentrations onto the shocked gas which would tend to reduce the efficiency of gas dynamic heating of grains in the center of the dust cloud.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060020744','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060020744"><span>Geochemistry of Pallasite <span class="hlt">Olivines</span> and the Origin of Main-Group Pallasites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mittlefehldt, D. W.; Rumble, D., III</p> <p>2006-01-01</p> <p>Main-group pallasites (PMG) are mixtures of iron-nickel metal and magnesian <span class="hlt">olivine</span> thought to have been formed at the core-mantle boundary of an asteroid [1]. Some have anomalous metal compositions (PMG-am) and a few have atypically ferroan <span class="hlt">olivines</span> (PMG-as) [2]. PMG metal is consistent with an origin as a late fractionate of the IIIAB iron core [2]. Most PMG <span class="hlt">olivines</span> have very similar Fe/Mg ratios, likely due to subsolidus redox reaction with the metal [3]. In contrast, minor and trace elements show substantial variation, which may be explained by either: (i) PMG were formed at a range of depths in the parent asteroid; the element variations reflect variations in igneous evolution with depth, (ii) the pallasite parent asteroid was chemically heterogeneous; the heterogeneity partially survived igneous processing, or (iii) PMG represent the core-mantle boundaries of several distinct parent asteroids [4, 5]. We have continued doing major, minor and trace elements by EMPA and INAA on a wider suite of PMG <span class="hlt">olivines</span>, and have begun doing precise oxygen isotope analyses to test these hypotheses. Manganese is homologous with Fe(2+), and can be used to distinguish between magmatic and redox processes as causes for Fe/Mg variations. PMG <span class="hlt">olivines</span> have a range in molar 1000*Mn/Mg of 2.3-4.6 indicating substantial igneous fractionation in <span class="hlt">olivines</span> with very similar Fe/Mg (0.138-0.148). The Mg-Mn-Fe distributions can be explained by a fractional crystallization-reduction model; higher Mn/Mg ratios reflect more evolved <span class="hlt">olivines</span> while Fe/Mg is buffered by redox reactions with the metal. There is a positive association between Mn/Mg and Sc content that is consistent with igneous fractionation. However, most PMG <span class="hlt">olivines</span> fall within a narrow Mn/Mg range (3.0-3.6), but these show a substantial range in Sc (1.00-2.29 micro-g/g). Assuming fractional crystallization, this Sc range could have resulted from approx.65% crystallization of an ultramafic magma. This is inconsistent with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V31A3060G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V31A3060G"><span>A Calcium-in-<span class="hlt">Olivine</span> Geohygrometer and its Application to Subduction Zone Magmatism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gavrilenko, M.; Herzberg, C. T.; Vidito, C. A.; Carr, M. J.; Tenner, T.; Ozerov, A.</p> <p>2016-12-01</p> <p>Calcium contents of subduction zone <span class="hlt">olivines</span> are lower than those for <span class="hlt">olivines</span> from modern MORB, Archean komatiites, and Hawaii (Fig. 1). A role for magmatic H2O is likely for subduction zone <span class="hlt">olivines</span>, and we have explored the suggestion by [1] that H2O has affected the partitioning of CaO between <span class="hlt">olivine</span> and silicate melt. We provide a provisional calibration of DCaOOl/L as a function of magmatic MgO and H2O, based on nominally anhydrous experiments (Fig. 2) and minimally degassed H2O contents of <span class="hlt">olivine</span>-hosted melt inclusions (Fig. 3). The low diffusivity of Ca in <span class="hlt">olivine</span> [2], when compared to that of H+ [3, 4, 5, 6], might help to retain the memory of magmatic water that is otherwise lost by diffusion and degassing. Application of our geohygrometer (Fig. 4) typically yields 3 to 4 wt. % magmatic H2O at the Kamchatka and Central American arcs for <span class="hlt">olivines</span> having 1000 ppm Ca, which agrees with H2O maxima from melt inclusion studies [7]; Cerro Negro and Shiveluch volcanoes are exceptions, with about 6% H2O. Our geohygrometer is by no means a replacement for more accurate methods of H2O analysis, but it has the advantage of applicability in cases where <span class="hlt">olivine</span>-hosted melt inclusions do not exist (or in case when melt inclusions are partly or completely degassed). Additionally, application of the geohygrometer to core-rim <span class="hlt">olivine</span> Ca analyses has the potential to reveal changes in magmatic H2O, as revealed by Klyuchevskoy and Shiveluch volcanoes. High precision EMPA analyses with 10-20 µm spatial resolution on some <span class="hlt">olivine</span> grains from Klyuchevskoy and Shiveluch show a decrease in Ca content from core centers to the rim contacts. Our geohygrometer indicates the <span class="hlt">olivine</span> grains may record changing magmatic H2O. Furthermore, high Mg numbers and Ni contents indicate these are mantle <span class="hlt">olivines</span>, and the inferred H2O may be recording entry from the slab to the mantle wedge, a prediction that will be tested by SIMS analyses. References: [1] Feig et al. (2006) CMP, 152</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.208..160G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.208..160G"><span>The storage capacity of fluorine in <span class="hlt">olivine</span> and pyroxene under upper mantle conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grützner, Tobias; Kohn, Simon C.; Bromiley, David W.; Rohrbach, Arno; Berndt, Jasper; Klemme, Stephan</p> <p>2017-07-01</p> <p>We present new experimental results on the fluorine storage capacity of <span class="hlt">olivine</span> and orthopyroxene in the Earth's mantle. Experiments were performed in the system MgO-SiO2 + MgF2 at temperatures between 1350 °C and 1700 °C and pressures up to 17 GPa. Electron microprobe measurements show that fluorine concentrations in <span class="hlt">olivine</span> reach up to 5100 μg/g. The storage capacity of fluorine in <span class="hlt">olivine</span> shows only a small pressure dependence but a strong temperature dependence with a positive correlation between increasing temperature and fluorine storage capacity. Fluorine concentrations found in enstatite are one order of magnitude smaller and reach up to 670 μg/g. Our data show that concentrations of fluorine in fluorine-saturated <span class="hlt">olivine</span> are in the same range as water concentrations in <span class="hlt">olivine</span>. Nevertheless, fluorine and water solubility in <span class="hlt">olivine</span> show opposing behavior with increasing pressure and temperature. The fluorine solubility in <span class="hlt">olivine</span> increases with increasing temperature but is not much affected by pressure. In contrast, water solubility in <span class="hlt">olivine</span> has previously been shown to decrease with increasing temperature and increase with increasing pressure. Our experiments show that nominally fluorine-free minerals like forsterite and enstatite are capable of storing the entire fluorine budget of the upper mantle, without the need to invoke accessory phases such as apatite or amphibole.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930052989&hterms=1586&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3D%2526%25231586','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930052989&hterms=1586&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3D%2526%25231586"><span>The CR (Renazzo-type) carbonaceous chondrite group and its implications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weisberg, Michael K.; Prinz, Martin; Clayton, Robert N.; Mayeda, Toshiko K.</p> <p>1993-01-01</p> <p>A petrologic, geochemical, and oxygen isotropic study of the CR chondrites including Renazzo, Al Rais, El Djouf 001 and the paired Acfer meteorites, EET87770 and the paired samples, MAC87320, Y790112, Y793495, and Y791498 is presented. It is concluded that the CR group is characterized by abundant large multilayered, Fe, Ni metal-rich, type I <span class="hlt">chondrules</span>; abundant matrix and dark inclusions; unique assemblages of serpentine and chlorite-rich phyllosilicates and Ca-carbonates; Ca-carbonate rims on <span class="hlt">chondrules</span>; abundant Fe, Ni metal with a positive Ni vs. Co trend and a solar Ni:Co ratio; and amoeboid <span class="hlt">olivine</span> aggregates with Mn-rich and Mn-poor forsterite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JGRE..113.6004P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JGRE..113.6004P"><span>Martian dunite NWA 2737: Integrated spectroscopic analyses of brown <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pieters, Carle M.; Klima, Rachel L.; Hiroi, Takahiro; Dyar, M. Darby; Lane, Melissa D.; Treiman, Allan H.; Noble, Sarah K.; Sunshine, Jessica M.; Bishop, Janice L.</p> <p>2008-06-01</p> <p>A second Martian meteorite has been identified that is composed primarily of heavily shocked dunite, Northwest Africa (NWA) 2737. This meteorite has several similarities to the Chassigny dunite cumulate, but the <span class="hlt">olivine</span> is more Mg rich and, most notably, is very dark and visually brown. Carefully coordinated analyses of NWA 2737 whole-rock and <span class="hlt">olivine</span> separates were undertaken using visible and near-infrared reflectance, midinfrared emission and reflectance, and Mössbauer spectroscopic studies of the same samples along with detailed petrography, chemistry, scanning electron microscopy, and transmission electron microscopy analyses. Midinfrared spectra of this sample indicate that the <span class="hlt">olivine</span> is fully crystalline and that its molecular structure remains intact. The unusual color and spectral properties that extend from the visible through the near-infrared part of the spectrum are shown to be due to nanophase metallic iron particles dispersed throughout the <span class="hlt">olivine</span> during a major shock event on Mars. Although a minor amount of Fe3+ is present, it cannot account for the well-documented unusual optical properties of Martian meteorite NWA 2737. Perhaps unique to the Martian environment, this ``brown'' <span class="hlt">olivine</span> exhibits spectral properties that can potentially be used to remotely explore the pressure-temperature history of surface geology as well as assess surface composition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI51C0327M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI51C0327M"><span>Deformation of <span class="hlt">olivine</span> during phase transformation to wadsleyite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mohiuddin, A.; Girard, J.; Karato, S. I.</p> <p>2017-12-01</p> <p>The strength of subducting slabs in the transition zone is critical in controlling the style of mantle convection. However, rheological properties of a subducted slab are elusive: low temperatures of a slab would make slabs strong, but in many regions there is evidence of intense deformation of slabs in the transition zone. One potential cause of intense deformation of subducting slabs is grain size reduction and accompanied microstructural changes during phase transformation of <span class="hlt">olivine</span> to its higher-pressure polymorphs. There have been no experimental studies to quantify the influence of grain-size evolution. In addition to grain size reduction, distribution of small grains during phase transformation governs the degree of weakening during phase transformation (for e.g. load bearing framework vs. inter-connected layered framework). We conducted laboratory studies on the size and spatial distribution of new grains of wadsleyite after the transformation from <span class="hlt">olivine</span>. Our results under static conditions show that an interconnected microstructure develops during the initial stage of phase transformation and that the grain size of the interconnected phase (wadsleyite) depends on the temperature at which the phase transformation occurs (smaller grains at lower temperatures). Development of an interconnected microstructure may lead to strain localization in the weaker phase, i.e. the fine-grained interconnected network accommodates most of the strain and therefore weakening of the entire composite. We will test this model through a series of two synchrotron in-situ deformation experiments: (i) <span class="hlt">Olivine</span> aggregate will be deformed during slow pressure increase from deep upper mantle pressure ( 10 GPa) to transition zone pressure ( 15 GPa) at a given temperature simulating the deformation of a slab penetrating into the transition zone (ii) <span class="hlt">olivine</span> is partially transformed to wadsleyite in a multi anvil apparatus at Yale and will be deformed within the stability field where</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V32A..02P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V32A..02P"><span>Dehydration Rate of <span class="hlt">Olivines</span> with Application to Magma Ascent Rate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Plank, T. A.; Ferriss, E.; Walker, D.; Newcombe, M. E.</p> <p>2017-12-01</p> <p>The physics of magma transport and eruption are highly sensitive to the decompression rate, for which few measurements exist. There is great promise, however, in being able to use <span class="hlt">olivine</span> dehydration to clock the ascent of magmas and xenoliths prior to eruption. Every <span class="hlt">olivine</span> phenocryst we have measured is zoned in water (H) as a consequence of decompression-driven-degassing and diffusion through the <span class="hlt">olivine</span>. A major impediment to exploiting this crystal clock, however, is the appropriate diffusivity to use. Published laboratory measurements vary by > 5 orders of magnitude. In order to better define the dehydration rates operating in natural <span class="hlt">olivines</span>, we conducted laboratory experiments using the whole-block method [1], which allows a finely-resolved time series of H profiles in 3 crystallographic directions using the same sample for all dehydration steps. Starting materials consisted of an untreated <span class="hlt">olivine</span> from the 1959 Kilauea Iki eruption, and a San Carlos <span class="hlt">olivine</span> first hydrated in a piston cylinder at NNO, 800°C and 1 GPa for 17.5 hours, just enough to saturate the proton-polaron (p-p) mechanism [2]. Samples were dehydrated at 1 atm, NNO-2.6 and 1000 and 800°C in 6-7 time steps over 8-68 total hours. Both samples show rapid movement of different FTIR absorption bands during the first few hours at 800°C, at the p-p rate. Water loss then converges to a rate intermediate between p-p and proton-Mg-vacancy (p-v) rates for both crystals. In San Carlos, water loss from the 3600 cm-1 band (Si-vacancy defect) speeds up after 20 hours, while the 3525 cm-1 band (Ti-clinohumite defect) slows down, until both are dehydroxylating at a rate of 20% p-p:80% p-v. The apparent diffusivity of these bands is > 4 orders of magnitude faster than the same bands in synthetic forsterite [3]. The Iki <span class="hlt">olivine</span> dehydrates at a constant rate from 3-8 hrs at 1000°C, at 12% p-p: 88% p-v. Both crystals show very similar diffusivity along [100] at 1000°C (logD -10.5 m2/s). This study thus</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.minsocam.org/MSA/AmMin/TOC/2004/MJ04.html','USGSPUBS'); return false;" href="http://www.minsocam.org/MSA/AmMin/TOC/2004/MJ04.html"><span>Reaction rim growth on <span class="hlt">olivine</span> in silicic melts: Implications for magma mixing</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Coombs, Michelle L.; Gardner, James E.</p> <p>2004-01-01</p> <p>Finely crystalline amphibole or pyroxene rims that form during reaction between silicic host melt and cognate <span class="hlt">olivine</span> xenocrysts, newly introduced during magma mixing events, can provide information about the timing between mixing and volcanic eruptions. We investigated rim growth experimentally by placing forsteritic <span class="hlt">olivine</span> in rhyolitic and rhyodacitic melts for times between 25 and 622 h at 50 and 150 MPa, H2O-saturated, at the Ni-NiO buffer. Rims of orthopyroxene microlites formed from high-silica rhyolite and rhyodacite melts at 885°C and 50 MPa, and in the rhyolite at 150 MPa and 885°C. Rims of amphibole with lesser orthopyroxene formed in the rhyolite at 150 MPa and 800°C and in the rhyodacite at 150 MPa and 885°C. Irregular, convolute <span class="hlt">olivine</span> edges and mass balance between <span class="hlt">olivine</span>, melt, and rim phases show that <span class="hlt">olivine</span> partly dissolved at all conditions. Iron-rich zones at the exteriors of <span class="hlt">olivines</span>, which increased in width parabolically with time, show that Fe-Mg interdiffusion occurring in <span class="hlt">olivines</span> was not outpaced by <span class="hlt">olivine</span> dissolution. Linear increases of the square of rim widths with time suggest that diffusion within the melt is the rate-controlling process for <span class="hlt">olivine</span> dissolution and rim growth. Rims grew one-half to one order-of-magnitude faster when melt water contents were doubled, unless conditions were far above the liquidus. Rim growth rate in rhyolite increases from 0.055 ± 0.01 µm2/h at 885°C and 50 MPa to 0.64 ± 0.13 µm2/h at 800°C and 150 MPa. Melt composition has a lesser effect on rim growth rates, with growth rate increasing as melt SiO2 content decreases. Pyroxene rims on <span class="hlt">olivines</span> in andesite erupted from Arenal volcano (Costa Rica) grew at a rate of 3.0 ± 0.2 µm2/h over an eleven-year period. This rate is faster than those of the experiments due to lower melt viscosity and higher temperatures, and suggests that a magma mixing event preceded the start of the eruption by days.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19191538','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19191538"><span>Short- and long-term <span class="hlt">olivine</span> weathering in Svalbard: implications for Mars.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hausrath, E M; Treiman, A H; Vicenzi, E; Bish, D L; Blake, D; Sarrazin, P; Hoehler, T; Midtkandal, I; Steele, A; Brantley, S L</p> <p>2008-12-01</p> <p>Liquid water is essential to life as we know it on Earth; therefore, the search for water on Mars is a critical component of the search for life. <span class="hlt">Olivine</span>, a mineral identified as present on Mars, has been proposed as an indicator of the duration and characteristics of water because it dissolves quickly, particularly under low-pH conditions. The duration of <span class="hlt">olivine</span> persistence relative to glass under conditions of aqueous alteration reflects the pH and temperature of the reacting fluids. In this paper, we investigate the utility of 3 methodologies to detect silicate weathering in a Mars analog environment (Sverrefjell volcano, Svalbard). CheMin, a miniature X-ray diffraction instrument developed for flight on NASA's upcoming Mars Science Laboratory, was deployed on Svalbard and was successful in detecting <span class="hlt">olivine</span> and weathering products. The persistence of <span class="hlt">olivine</span> and glass in Svalbard rocks was also investigated via laboratory observations of weathered hand samples as well as an in situ burial experiment. Observations of hand samples are consistent with the inference that <span class="hlt">olivine</span> persists longer than glass at near-zero temperatures in the presence of solutions at pH approximately 7-9 on Svalbard, whereas in hydrothermally altered zones, glass has persisted longer than <span class="hlt">olivine</span> in the presence of fluids at similar pH at approximately 50 degrees C. Analysis of the surfaces of <span class="hlt">olivine</span> and glass samples, which were buried on Sverrefjell for 1 year and then retrieved, documented only minor incipient weathering, though these results suggest the importance of biological impacts. The 3 types of observations (CheMin, laboratory observations of hand samples, burial experiments) of weathering of <span class="hlt">olivine</span> and glass at Svalbard show promise for interpretation of weathering on Mars. Furthermore, the weathering relationships observed on Svalbard are consistent with laboratory-measured dissolution rates, which suggests that relative mineral dissolution rates in the laboratory, in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820048211&hterms=sem&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsem','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820048211&hterms=sem&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsem"><span>SEM, optical, and Moessbauer studies of submicrometer chromite in Allende</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Housley, R. M.</p> <p>1982-01-01</p> <p>New scanning electron and optical microscope results are presented showing that sub-micrometer chromite is abundant along healed cracks and grain boundaries in Allende <span class="hlt">chondrule</span> <span class="hlt">olivine</span>. Some wider healed cracks also contain pentlandite and euhedral Ni3Fe grains. Also reported are Moessbauer measurements on Allende HF-HCl residues confirming a high Fe(+++)/Fe(++) ratio.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992Metic..27S.236H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992Metic..27S.236H"><span>New Evidence for the Origin of White Matrix in Tieschitz</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hutchison, R.</p> <p>1992-07-01</p> <p>In Tieschitz, an unequilibrated ordinary chondrite, <span class="hlt">chondrules</span>, and inclusions have rims of fine-grained, opaque matrix. Between the larger objects, channels <~20 micrometers wide may be filled with Na- and Al-rich, nepheline-normative white matrix. Christophe Michel-Levy (1976) suggested that white matrix was formed by the partial solution and redeposition of <span class="hlt">chondrule</span> mesostases, but this was disputed by Hutchison et al. (1979), because silica undersaturated white matrix commonly abuts low-Ca pyroxene, with no sign of reaction. Such materials should be incompatible at low pressure and elevated temperature. Alexander et al. (1989) found material resembling white matrix in two Sharps <span class="hlt">chondrules</span>, but did not find it elsewhere. Furthermore, the major minerals of white matrix are still unidentified. In a thick polished section, the analytical scanning electron microscope revealed several porphyritic <span class="hlt">chondrules</span> with mesostases composed of two types of material with different electron back-scattering properties. One type lacks internal boundaries and appears brighter than the other, which is blocky on a 5-micrometer scale; the latter resembles white matrix. Bright mesostasis has higher SiO2, TiO2, FeO, MgO, and CaO compared with the dark, blocky material, which is richer in Al2O3 and the alkalis (Table 1, cf nos. 3 and 5). A porphyritic <span class="hlt">olivine</span> (PO) <span class="hlt">chondrule</span> 1 mm in diameter has zoned phenocrysts of Fo(sub)90-75 (Table 1 ) and mesostasis containing Ca-pyroxene dendrites of uniform composition close to Wo(sub)38En(sub)42 and with a high MnO/FeO ratio of ~0.07. Both types of mesostasis are present and in contact. Pyroxene dendrites extend across contacts without structural or compositional change. Furthermore, at its contact with a 0.6-mm <span class="hlt">barred</span> pyroxene <span class="hlt">chondrule</span>, the PO <span class="hlt">chondrule</span> is slightly indented and needles of Ca-pyroxene radiate from the point of contact into bright mesostasis. The evidence indicates that in the PO <span class="hlt">chondrule</span> a single generation of dendritic Ca</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V33D0556L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V33D0556L"><span>V/Sc in <span class="hlt">olivine</span> as a proxy for magma redox conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Locmelis, M.; Arevalo, R. D., Jr.; Puchtel, I. S.; Fiorentini, M. L.</p> <p>2017-12-01</p> <p>Although <span class="hlt">olivine</span> is the most abundant mineral in the upper mantle and a major constituent of most mantle-derived rocks, studies on its trace element chemistry are underrepresented. This is especially the case for komatiites, an ultramafic, <span class="hlt">olivine</span>-dominated rock type that formed via high degrees of partial melting (up to 50%) of the mantle. Komatiites were mostly emplaced in the Archean and therefore provide a unique perspective on the composition and evolution of the early Earth's mantle. Here, we present the V/Sc compositions of <span class="hlt">olivines</span> from a global set of Paleo- (3.5-3.3 Ga) and Neo-Archean (2.7 Ga) komatiites analyzed via laser ablation ICP-MS. Vanadium and Sc behave similar during partial melting, but V is redox-sensitive (V2+-V5+) and most compatible in <span class="hlt">olivine</span> as V2+. Scandium is monovalent (Sc3+) and its compatibility in <span class="hlt">olivine</span> is not affected by the oxygen fugacity (fO2) of the komatiite lava. Therefore, V/Sc ratios in <span class="hlt">olivines</span> are potentially indicative of the fO2 of the magma they crystallized from. Our data show that V/Sc ratios measured in Neo-Archean <span class="hlt">olivines</span> (V/Scmean = 1.0 ± 0.1; 2σm) are significantly lower than in their Paleo-Archean counterparts (V/Scmean = 2.1 ± 0.1; 2σm). Geochemical models show that the elevated V/Sc ratios captured by the Paleo-Archean <span class="hlt">olivines</span> reflect crystallization from magmas that were 1.6 log units (relative to QFM) more reduced than their Neo-Archean counterparts, and thus contained a higher proportion of V2+. Because assimilation of sedimentary bedrocks can alter the composition of komatiites upon emplacement, it may be argued that the redox states recorded by the <span class="hlt">olivines</span> do not reflect mantle fO2, but the assimilation of crustal material. However, such an effect is not visible in our data as V/Sc ratios in <span class="hlt">olivines</span> from localities that show evidence of crustal assimilation do not differ from komatiites that did not assimilate significant amounts of crustal rocks. Rather than a crustal signature, the V</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014DPS....4650601B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014DPS....4650601B"><span>Space Weathering in <span class="hlt">Olivine</span> and the Mineralogy of (Some) M-Class Asteroids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Britt, Daniel; Kohout, Tomas; Schelling, Patrick; Consolmagno, Guy J.</p> <p>2014-11-01</p> <p>One aspect of space weathering of airless bodies is the production of nanophase iron (npFe0) from Fe bearing silicate minerals. The combined effects of low oxygen fugacity and solar-wind implanted H tend to result in strongly-reduced surfaces that can be chemically activated by heating due to micrometeorite impacts. The mineral kinetics of <span class="hlt">olivine</span> makes it particularly vulnerable to reduction, decomposition, and npFe0 production. Kohout et al. has recently developed a new method of controlled npFe0 production on <span class="hlt">olivine</span> powder grains that mimics the essential features of this weathering process and was developed to quantitatively evaluate spectral changes related to space weathering and presence of npFe0. Compared to fresh <span class="hlt">olivine</span> the treated samples exhibit spectral characteristics of space weathering including spectral darkening, shallowing and attenuation of 1 µm <span class="hlt">olivine</span> absorption band, and reddening. The attenuation of the 1 µm band significantly shrinks the band FWHM and shifts the much reduced band center to shorter wavelengths around 0.95 µm. These spectral changes are related to increasing amounts of npFe0 and the disruption of the crystal structure of the parent <span class="hlt">olivine</span>. Significantly, the darkened, reddened, and band attenuated <span class="hlt">olivine</span> spectra are a close match to a number of M-class asteroids. What is particularly interesting is the match with the weak absorption band near 0.95 µm seen in many M-class asteroids (i.e. 16 Psyche, 22 Kalliope, 55 Pandora to name a few). One of the major issues in asteroid science is the relative scarcity of <span class="hlt">olivine</span> asteroids (the ”Great Dunite Shortage” coined by Bell et al in Asteroids II). One possibility worth further study is that asteroidal <span class="hlt">olivine</span> may be hidden by the relative ease with which it weathers. The surface chemical and micrometeorite environment in the asteroid belt may produce over time a spectrum for an <span class="hlt">olivine</span>-rich surface that is remarkably similar to that of an M-class asteroid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016M%26PS...51..372R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016M%26PS...51..372R"><span>First finding of impact melt in the IIE Netschaëvo meteorite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roosbroek, N.; Pittarello, L.; Greshake, A.; Debaille, V.; Claeys, P.</p> <p>2016-02-01</p> <p>About half of the IIE nonmagmatic iron meteorites contain silicate inclusions with a primitive to differentiated nature. The presence of preserved <span class="hlt">chondrules</span> has been reported for two IIE meteorites so far, Netschaëvo and Mont Dieu, which represent the most primitive silicate material within this group. In this study, silicate inclusions from two samples of Netschaëvo were examined. Both silicate inclusions are characterized by a porphyritic texture dominated by clusters of coarse-grained <span class="hlt">olivine</span> and pyroxene, set in a fine-grained groundmass that consists of new crystals of <span class="hlt">olivine</span> and a glassy appearing matrix. This texture does not correspond to the description of the previously examined pieces of Netschaëvo, which consist of primitive <span class="hlt">chondrule</span>-bearing angular clasts. Detailed petrographic observations and geochemical analyses suggest that the investigated samples of Netschaëvo consist of quenched impact melt. This implies that Netschaëvo is a breccia containing metamorphosed and impact-melt rock (IMR) clasts and that collisions played a major role in the formation of the IIE group.</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://pubs.er.usgs.gov/publication/70009984','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70009984"><span>Shock-produced <span class="hlt">olivine</span> glass: First observation</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Jeanloz, R.; Ahrens, T.J.; Lally, J.S.; Nord, G.L.; Christie, J.M.; Heuer, A.H.</p> <p>1977-01-01</p> <p>Transmission electron microscope (TEM) observations of an experimentally shock-deformed single crystal of natural peridot, (Mg0.88Fe 0.12SiO4 recovered from peak pressures of about 56 ?? 109 pascals revealed the presence of amorphous zones located within crystalline regions with a high density of tangled dislocations. This is the first reported observation ofolivine glass. The shocked sample exhibits a wide variation in the degree of shock deformation on a small scale, and the glass appears to be intimately associated with the highest density of dislocations. This study suggests that <span class="hlt">olivine</span> glass may be formed as a result of shock at pressures above about 50 to 55 ?? 109 pascals and that further TEM observations of naturally shocked <span class="hlt">olivines</span> may demonstrate the presence of glass.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020046564&hterms=dating&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Ddating','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020046564&hterms=dating&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Ddating"><span>I-Xe Dating: Comparison of I-Xe and Pb-Pb Ages of Richardton <span class="hlt">Chondrules</span> and Separated Mineral Phases</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pravdivtseva, O. V.; Amelin, Y.; Hohenberg, C. M.; Meshik, A. P.</p> <p>2002-01-01</p> <p>I-Xe and Pb-Pb ages of individual Richardton <span class="hlt">chondrules</span> and different mineral phases were compared in order to test the absolute I-Xe age normalization. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22050979-calcio-olivine-gamma-ca-sub-sio-sub-rietveld-refinement-crystal-structure','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22050979-calcio-olivine-gamma-ca-sub-sio-sub-rietveld-refinement-crystal-structure"><span>Calcio-<span class="hlt">olivine</span> {gamma}-Ca{sub 2}SiO{sub 4}: I. Rietveld refinement of the crystal structure</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>Gobechiya, E. R., E-mail: elgob@mail.ru; Yamnova, N. A.; Zadov, A. E.</p> <p>2008-05-15</p> <p>The structure of the natural mineral calcio-<span class="hlt">olivine</span> ({gamma}-Ca{sub 2}SiO{sub 4}) found in skarn xenoliths in the region of the Lakargi Mountain (North Caucasus, Kabardino-Balkaria, Russia) is refined by the Rietveld method [a = 5.07389(7) A, b = 11.21128(14) A, c = 6.75340(9) A, V = 384.170(5) A{sup 3}, Z = 4, {rho}{sub calcd} = 2.98 g/cm{sup 3}, space group Pbnm]. The X-ray diffraction pattern of a powdered sample is recorded on a STOE STADI MP diffractometer [{lambda}CuK{sub {alpha}1}; Ge(111) primary monochromator; 6.00{sup o} < 2{theta} < 100.88{sup o}; step width, 2.5{sup o} in 2{theta}; number of reflections, 224]. All calculationsmore » are performed with the WYRIET (version 3.3) software package. The structural model is refined in the anisotropic approximation to R{sub p} = 6.44, R{sub wp} = 8.52, R{sub exp} = 5.85, R{sub B} = 4.98, R{sub F} = 6.90, and s = 1.46. It is shown that the sample under investigation is a mixture of several mineral phases, among which calcio-<span class="hlt">olivine</span> (the natural analogue of the {gamma}-Ca{sub 2}SiO{sub 4} compound) (83%), hillebrandite (13%), and wadalite (4%) are dominant. Only the scale factors and the unit cell parameters are refined for hillebrandite Ca{sub 2}SiO{sub 3}(OH){sub 2} [a = 3.63472(16) A, b = 16.4140(10) A, c = 11.7914(8) A, space group Cmc2{sub 1}, Z = 6] and wadalite Ca{sub 6}Al{sub 5}Si{sub 2}O{sub 16}Cl{sub 3} (a = 12.0088 A, space group, I 4 <span class="hlt">bar</span> 3d, Z = 4). The results of the structure refinement of the main component of the sample confirm that the mineral calcio-<span class="hlt">olivine</span> is isostructural to the synthetic compound {gamma}-Ca{sub 2}SiO{sub 4}. The structure of this compound is formed by the heteropolyhedral framework composed of Ca octahedra joined together into <span class="hlt">olivine</span>-like ribbons and isolated Si tetrahedra.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000PCM....27..480D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000PCM....27..480D"><span>Evidence for stable grain boundary melt films in experimentally deformed <span class="hlt">olivine</span>-orthopyroxene rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Kloe, R.; Drury, M. R.; van Roermund, H. L. M.</p> <p></p> <p>The microstructure of <span class="hlt">olivine-olivine</span> grain boundaries has been studied in experimentally deformed (1200-1227°C, 300MPa) partially molten <span class="hlt">olivine</span> and <span class="hlt">olivine</span>-orthopyroxene rocks. In-situ melting produced 1vol% melt in all samples studied. Grain boundary analyses were carried out using a number of transmission electron microscopy techniques. The grain boundary chemistry in undeformed <span class="hlt">olivine</span>-orthopyroxene starting material showed evidence for the presence of an intergranular phase along some, but not all, of the <span class="hlt">olivine-olivine</span> boundaries. In the deformed samples, ultrathin Si-rich, Al- and Ca-bearing amorphous films have been observed along all investigated <span class="hlt">olivine-olivine</span> grain boundaries. The chemistry of the grain boundaries, which is considered to be indicative for the presence of a thin film, was measured with energy-dispersive X-ray spectroscopy (EDX) and energy-filtering imaging. The amorphous nature of the films was confirmed with diffuse dark field imaging, Fresnel fringe imaging, and high-resolution electron microscopy. The films range in thickness from 0.6 to 3.0nm, and EDX analyses show that the presence of Al and Ca is restricted to this ultrathin film along the grain boundaries. Because thin melt films have been observed in all the samples, they are thought to be stable features of the melt microstructure in deformed partially molten rocks. The transition from the occasional presence of films in the undeformed starting material to the general occurrence of the films in deformed materials suggests that deformation promotes the formation and distribution of the films. Alternatively, hot-pressing may be too short for films to develop along all grain boundaries. A difference in creep strength between the studied samples could not be attributed to grain boundary melt films, as these have been found in all deformed samples. However, a weakening effect of grain boundary melt films on <span class="hlt">olivine</span> rheology could not be ruled out due to the lack of confirmed melt</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920003695','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920003695"><span>Low temperature annealing and cathodoluminescence studies of type 1 <span class="hlt">chondrule</span> compositions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dehart, John M.; Lofgren, Gary E.</p> <p>1991-01-01</p> <p>Preliminary results indicate that the yellow luminescing mesostases in type I <span class="hlt">chondrules</span> can be altered by the effects of the low level thermal metamorphism. Although heat alone was insufficient to alter the CL, reheating for geologically relevant periods could have the same results as we obtained in a second series of experiments with water present. It is known that both water and solutions of sodium metasilicate greatly accelerate the devitrification of glasses. The results of the experiments that will be repeated should further clarify how the CL changes with increased thermal alteration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030018906','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030018906"><span>Blowing in the Wind: I. Velocities of <span class="hlt">Chondrule</span>-sized Particles in a Turbulent Protoplanetary Nebula</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cuzzi, Jeffrey N.; Hogan, Robert C.; Fonda, Mark (Technical Monitor)</p> <p>2003-01-01</p> <p>Small but macroscopic particles - <span class="hlt">chondrules</span>, higher temperature mineral inclusions, metal grains, and their like - dominate the fabric of primitive meteorites. The properties of these constituents, and their relationship to the fine dust grains which surround them, suggest that they led an extended existence in a gaseous protoplanetary nebula prior to their incorporation into their parent primitive bodies. In this paper we explore in some detail the velocities acquired by such particles in a turbulent nebula. We treat velocities in inertial space (relevant to diffusion), velocities relative to the gas and entrained microscopic dust (relevant to accretion of dust rims), and velocities relative to each other (relevant to collisions). We extend previous work by presenting explicit, closed-form solutions for the magnitude and size dependence of these velocities in this important particle size regime, and compare these expressions with new numerical calculations. The magnitude and size dependence of these velocities have immediate applications to <span class="hlt">chondrule</span> and CAI rimming by fine dust, and to their diffusion in the nebula, which we explore separately.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790049939&hterms=1603&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D%2526%25231603','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790049939&hterms=1603&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3D%2526%25231603"><span>Optical absorption and radiative heat transport in <span class="hlt">olivine</span> at high temperature</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shankland, T. J.; Nitsan, U.; Duba, A. G.</p> <p>1979-01-01</p> <p>Results are presented of measurements of the optical absorption spectra (300-8000 nm) of <span class="hlt">olivine</span> as a function of temperature (300-1700 K) under conditions of controlled and known oxygen fugacity within the stability field of the samples. The absorption spectra are used to calculate the temperature-dependent radiative transfer coefficient of <span class="hlt">olivine</span> and to numerically study the accuracy of the method. The present absorption measurements in <span class="hlt">olivine</span> under oxidizing conditions known to be within the <span class="hlt">olivine</span> stability field indicate that the effective radiative conductivity K(R) is lower than that obtained in previous studies under different experimental conditions. The lower value of K(R) makes it more likely that some of the earth's internal heat is removed by convection and less likely that thermal models involving conduction and radiation alone will satisfactorily explain thermal conditions in the earth's mantle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70031054','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70031054"><span>Characterization and petrologic interpretation of <span class="hlt">olivine</span>-rich basalts at Gusev Crater, Mars</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McSween, H.Y.; Wyatt, M.B.; Gellert, Ralf; Bell, J.F.; Morris, R.V.; Herkenhoff, K. E.; Crumpler, L.S.; Milam, K.A.; Stockstill, K.R.; Tornabene, L.L.; Arvidson, R. E.; Bartlett, P.; Blaney, D.; Cabrol, N.A.; Christensen, P.R.; Clark, B. C.; Crisp, J.A.; Des Marais, D.J.; Economou, T.; Farmer, J.D.; Farrand, W.; Ghosh, A.; Golombek, M.; Gorevan, S.; Greeley, R.; Hamilton, V.E.; Johnson, J. R.; Joliff, B.L.; Klingelhofer, G.; Knudson, A.T.; McLennan, S.; Ming, D.; Moersch, J.E.; Rieder, R.; Ruff, S.W.; Schrorder, C.; de Souza, P.A.; Squyres, S. W.; Wanke, H.; Wang, A.; Yen, A.; Zipfel, J.</p> <p>2006-01-01</p> <p>Rocks on the floor of Gusev crater are basalts of uniform composition and mineralogy. <span class="hlt">Olivine</span>, the only mineral to have been identified or inferred from data by all instruments on the Spirit rover, is especially abundant in these rocks. These picritic basalts are similar in many respects to certain Martian meteorites (<span class="hlt">olivine</span>-phyric shergottites). The <span class="hlt">olivine</span> megacrysts in both have intermediate compositions, with modal abundances ranging up to 20-30%. Associated minerals in both include low-calcium and high-calcium pyroxenes, plagioclase of intermediate composition, iron-titanium-chromium oxides, and phosphate. These rocks also share minor element trends, reflected in their nickel-magnesium and chromium-magnesium ratios. Gusev basalts and shergottites appear to have formed from primitive magmas produced by melting an undepleted mantle at depth and erupted without significant fractionation. However, apparent differences between Gusev rocks and shergottites in their ages, plagioclase abundances, and volatile contents preclude direct correlation. Orbital determinations of global <span class="hlt">olivine</span> distribution and compositions by thermal emission spectroscopy suggest that <span class="hlt">olivine</span>-rich rocks may be widespread. Because weathering under acidic conditions preferentially attacks <span class="hlt">olivine</span> and disguises such rocks beneath alteration rinds, picritic basalts formed from primitive magmas may even be a common component of the Martian crust formed during ancient and recent times. Copyright 2006 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080026098','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080026098"><span>Characterization and Petrologic Interpretation of <span class="hlt">Olivine</span>-Rich Basalts at Gusev Crater, Mars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>McSween, H. Y.; Wyatt, M. B.; Gellert, R.; Bell, J. F., III; Morris, R. V.; Herkenhoff, K. E.; Crumpler, L. S.; Milam, K. A.; Stockstill, K. R.; Tornabene, L. L.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20080026098'); toggleEditAbsImage('author_20080026098_show'); toggleEditAbsImage('author_20080026098_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20080026098_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20080026098_hide"></p> <p>2006-01-01</p> <p>Rocks on the floor of Gusev crater are basalts of uniform composition and mineralogy. <span class="hlt">Olivine</span>, the only mineral to have been identified or inferred from data by all instruments on the Spirit rover, is especially abundant in these rocks. These picritic basalts are similar in many respects to certain Martian meteorites (<span class="hlt">olivine</span>-phyric shergottites). The <span class="hlt">olivine</span> megacrysts in both have intermediate compositions, with modal abundances ranging up to 20-30%. Associated minerals in both include low-calcium and high-calcium pyroxenes, plagioclase of intermediate composition, iron-titanium-chromium oxides, and phosphate. These rocks also share minor element trends, reflected in their nickel-magnesium and chromium-magnesium ratios. Gusev basalts and shergottites appear to have formed from primitive magmas produced by melting an undepleted mantle at depth and erupted without significant fractionation. However, apparent differences between Gusev rocks and shergottites in their ages, plagioclase abundances, and volatile contents preclude direct correlation. Orbital determinations of global <span class="hlt">olivine</span> distribution and compositions by thermal emission spectroscopy suggest that <span class="hlt">olivine</span>-rich rocks may be widespread. Because weathering under acidic conditions preferentially attacks <span class="hlt">olivine</span> and disguises such rocks beneath alteration rinds, picritic basalts formed from primitive magmas may even be a common component of the Martian crust formed during ancient and recent times.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940031655','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940031655"><span>Cr, Mn, and Ca distributions for <span class="hlt">olivine</span> in angritic systems: Constraints on the origins of Cr-rich and Ca-poor core <span class="hlt">olivine</span> in angrite LEW87051</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mikouchi, T.; Mckay, G.; Le, L.</p> <p>1994-01-01</p> <p>Angrite meteorites are a type of basaltic achondrites that are noted for their very old cyrstallization ages (4.55 b.y.) and unusual chemical and mineralogical properties. In spite of great interest, only four angrites have been found. LEW87051 is the smallest one which weighs 0.6 g. It is a porphyritic rock with coarse subhedral to euhedral <span class="hlt">olivines</span> set in a fine-grained groundmass which clearly represents a crystallized melt. The largest uncertainty about the petrogenesis of LEW87051 is the relationship between the large <span class="hlt">olivine</span> crystals and the groundmass. Prinz et al. suggests that <span class="hlt">olivines</span> are xenocrysts, while McKay et al. proposed a fractional cyrstallization model based on experimental studies. However, the crystals have Cr-rich and Ca-poor cores which do not match experimental <span class="hlt">olivines</span>. Although Jurewicz and McKay tried to explaine the zoning of the rim by diffusion, some features are not explained. There also exists a definite composition boundary of Fe(2+) and MnO between the core and the rim. To clarify the origin of these <span class="hlt">olivines</span>, we have performed experiments using LEW87051 analogs to measure the effects of oxygen fugacity on distribution coefficients of various elements in an angritic system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMGC41B0537K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMGC41B0537K"><span>Solar Radiation Management and <span class="hlt">Olivine</span> Dissolution Methods in Climate Engineering</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kone, S.</p> <p>2014-12-01</p> <p>An overview of solar radiation management and <span class="hlt">olivine</span> dissolution methods allows to discuss, comparatively, the benefits and consequences of these two geoengineering techniques. The combination of those two techniques allows to concomitantly act on the two main agents intervening in global warming: solar radiation and carbon dioxide. The earth surface temperature increases due mainly to carbon dioxide (a greenhouse gas) that keeps the solar radiation and causes the global warming. Two complementary methods to mitigate climate change are overviewed: SRM method, which uses injected aerosols, aims to reduce the amount of the inbound solar radiation in atmosphere; and <span class="hlt">olivine</span> dissolution in water, a key chemical reaction envisaged in climate engineering , aiming to reduce the amount of the carbon dioxide in extracting it from atmosphere. The SRM method works on scenarios of solar radiation decrease and the <span class="hlt">olivine</span> dissolution method works as a carbon dioxide sequestration method. <span class="hlt">Olivine</span> dissolution in water impacts negatively on the pH of rivers but positively in counteracting ocean acidification and in transporting the silica in ocean, which has benefits for diatom shell formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1393479-stabilization-lithium-transition-metal-silicates-olivine-structure','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1393479-stabilization-lithium-transition-metal-silicates-olivine-structure"><span>Stabilization of Lithium Transition Metal Silicates in the <span class="hlt">Olivine</span> Structure</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sun, Xiaoqi; Tripathi, Rajesh; Popov, Guerman; ...</p> <p>2017-07-28</p> <p>While <span class="hlt">olivine</span> LiFePO 4 shows amongst the best electrochemical properties of Li-ion positive electrodes with respect to rate behavior owing to facile Li + migration pathways in the framework, replacing the [PO 4] 3- polyanion with a silicate [SO 4] 4- moitie in <span class="hlt">olivine</span> is desirable. This would allow additional balancing alkali content and hence electron transfer, and increase the capacity. We demonstrate the first stabilization of a lithium transition-metal silicate (as a pure silicate) in the <span class="hlt">olivine</span> structure type. Using LiInSiO 4 and LiScSiO 4 as the parent materials, transition metal (Mn, Fe, Co) substitutions on the In/Sc sitemore » were investigated by computational modelling via atomic scale simulation. Transition metal substitution was found to be only favourable for Co, a finding confirmed by the successful solid state synthesis of <span class="hlt">olivine</span> LixInyCo 2-x-ySiO 4. Finally, the stabilization of the structure was achieved by entropy provided by cation disorder.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V32A..03N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V32A..03N"><span>Water-in-<span class="hlt">Olivine</span> Magma Ascent Chronometry: Every Crystal is a Clock</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Newcombe, M. E.; Asimow, P. D.; Ferriss, E.; Barth, A.; Lloyd, A. S.; Hauri, E.; Plank, T. A.</p> <p>2017-12-01</p> <p>The syneruptive decompression rate of basaltic magma in volcanic conduits is thought to be a critical control on eruptive vigor. Recent efforts have constrained decompression rates using models of diffusive water loss from melt embayments (Lloyd et al. 2014; Ferguson et al. 2016), <span class="hlt">olivine</span>-hosted melt inclusions (Chen et al. 2013; Le Voyer et al. 2014), and clinopyroxene phenocrysts (Lloyd et al. 2016). However, these techniques are difficult to apply because of the rarity of melt embayments and clinopyroxene phenocrysts suitable for analysis and the complexities associated with modeling water loss from melt inclusions. We are developing a new magma ascent chronometer based on syneruptive diffusive water loss from <span class="hlt">olivine</span> phenocrysts. We have found water zonation in every <span class="hlt">olivine</span> phenocryst we have measured, from explosive eruptions of Pavlof, Seguam, Fuego, Cerro Negro and Kilauea volcanoes. Phenocrysts were polished to expose a central plane normal to the crystallographic `b' axis and volatile concentration profiles were measured along `a' and `c' axes by SIMS or nanoSIMS. Profiles are compared to 1D and 3D finite-element models of diffusive water loss from <span class="hlt">olivine</span>, with or without melt inclusions, whose boundaries are in equilibrium with a melt undergoing closed-system degassing. In every case, we observe faster water diffusion along the `a' axis, consistent with the diffusion anisotropy observed by Kohlstedt and Mackwell (1998) for the so-called `proton-polaron' mechanism of H-transport. Water concentration gradients along `a' match the 1D diffusion model with a diffusivity of 10-10 m2/s (see Plank et al., this meeting), <span class="hlt">olivine</span>-melt partition coefficient of 0.0007­-0.002 (based on melt inclusion-<span class="hlt">olivine</span> pairs), and decompression rates equal to the best-fit values from melt embayment studies (Lloyd et al. 2014; Ferguson et al. 2016). Agreement between the melt embayment and water-in-<span class="hlt">olivine</span> ascent chronometers at Fuego, Seguam, and Kilauea Iki demonstrates the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V34C..08P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V34C..08P"><span>Diffusion of Water through <span class="hlt">Olivine</span> and Clinopyroxene: Implications for Melt Inclusion Fidelity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Plank, T. A.; Lloyd, A. S.; Ferriss, E.</p> <p>2016-12-01</p> <p>The maximum H2O concentrations measured in <span class="hlt">olivine</span>-hosted melt inclusions (MIs) from arc tephra fall within a narrow range of 3-5 wt%. A major question is whether this reflects parental water concentrations or diffusive exchange through the host crystal during storage and ascent. Laboratory experiments have shown that water can diffuse through 500 micron <span class="hlt">olivine</span> in minutes to days at 1100°C. We have tested these predictions with a natural experiment using volatile (H2O, CO2, S) diffusion along melt embayments to constrain ascent rates during the 1974 eruption of Volcan Fuego to 5-8 minutes from 7 km depth [1]. Thus, <span class="hlt">olivine</span>-hosted MIs may move from their storage region to the surface during some eruptions rapidly enough to retain almost all of their original water. Only the smallest MIs (< 30 microns) will lose any water during such fast ascent, even for the fastest diffusion mechanism through <span class="hlt">olivine</span>. We have also assessed the potential for clinopyroxene (cpx) to retain water (as H+) during magma ascent. In the same 1974 Fuego deposits, cpx crystals show H-loss on their rims and even from their interiors. Such diffusive loss in 5-8 minutes requires rapid diffusion of H in cpx, comparable to <span class="hlt">olivine</span> and melt, and consistent with our recent laboratory experiments dehydrating Fe-bearing cpx [2]. Although H-diffusion is dependent on the site occupancy, all sites may lose H rapidly in cpx with Mg# < 92.5. While cpx and <span class="hlt">olivine</span> may lose H during ascent and degassing, <span class="hlt">olivine</span>-hosted MIs stand a better chance of retaining water due to the very low partitioning of water in <span class="hlt">olivine</span> (D 0.001). The most favorable conditions for faithful retention of parental water concentrations involve a) rapid ascent (< hr.) from H2O-undersaturated reservoirs (prior to major water degassing), b) minerals with low partition coefficients for water, c) large crystals (>500 microns) and large melt inclusions (>50 microns), and 4) rapid post-eruptive cooling (< 1min, clast sizes < 1 cm). The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010000326','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010000326"><span>Thermal Emission Spectroscopy of 1 Ceres: Evidence for <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Witteborn, Fred. C.; Roush, Ted L.; Cohen, Martin</p> <p>1999-01-01</p> <p>Thermal emission spectra of the largest asteroid, 1 Ceres, obtained from the Kuiper Airborne Observatory display features that may provide information about its surface mineralogy. The emissivity, obtained by dividing the spectra by a standard thermal model, is compared with emissivity spectra of <span class="hlt">olivines</span> and phyllosilicates deduced via Kirchoff's law from reflectivity measurements. The spectra provide a fairly good match to fine grained <span class="hlt">olivines</span> (0 to 5 micrometer size range). The smoothness of the spectrum beyond 18 micrometers is an indication of particles smaller than 50 micrometers. While the abrupt rise in emissivity near 8 micrometers matches many silicates, the distinct emissivity minimum centered near 12.8 micrometers is consistant with iron-poor <span class="hlt">olivines</span>, but not with phyllosilicates. It suggests the presence of opaques and does not exclude a mixture with organics and fine-grained phyllosilicates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.P51A2558C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.P51A2558C"><span>Exploring <span class="hlt">Chondrule</span> and CAI Rims Using Micro- and Nano-Scale Petrological and Compositional Analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cartwright, J. A.; Perez-Huerta, A.; Leitner, J.; Vollmer, C.</p> <p>2017-12-01</p> <p>As the major components within chondrites, <span class="hlt">chondrules</span> (mm-sized droplets of quenched silicate melt) and calcium-aluminum-rich inclusions (CAI, refractory) represent the most abundant and the earliest materials that solidified from the solar nebula. However, the exact formation mechanisms of these clasts, and whether these processes are related, remains unconstrained, despite extensive petrological and compositional study. By taking advantage of recent advances in nano-scale tomographical techniques, we have undertaken a combined micro- and nano-scale study of CAI and <span class="hlt">chondrule</span> rim morphologies, to investigate their formation mechanisms. The target lithologies for this research are Wark-Lovering rims (WLR), and fine-grained rims (FGR) around CAIs and <span class="hlt">chondrules</span> respectively, present within many chondrites. The FGRs, which are up to 100 µm thick, are of particular interest as recent studies have identified presolar grains within them. These grains predate the formation of our Solar System, suggesting FGR formation under nebular conditions. By contrast, WLRs are 10-20 µm thick, made of different compositional layers, and likely formed by flash-heating shortly after CAI formation, thus recording nebular conditions. A detailed multi-scale study of these respective rims will enable us to better understand their formation histories and determine the potential for commonality between these two phases, despite reports of an observed formation age difference of up to 2-3 Myr. We are using a combination of complimentary techniques on our selected target areas: 1) Micro-scale characterization using standard microscopic and compositional techniques (SEM-EBSD, EMPA); 2) Nano-scale characterization of structures using transmission electron microscopy (TEM) and elemental, isotopic and tomographic analysis with NanoSIMS and atom probe tomography (APT). Preliminary nano-scale APT analysis of FGR morphologies within the Allende carbonaceous chondrite has successfully discerned</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034899','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034899"><span>Remote compositional analysis of lunar <span class="hlt">olivine</span>-rich lithologies with Moon Mineralogy Mapper (M3) spectra</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Isaacson, P.J.; Pieters, C.M.; Besse, S.; Clark, R.N.; Head, J.W.; Klima, R.L.; Mustard, J.F.; Petro, N.E.; Staid, M.I.; Sunshine, J.M.; Taylor, L.A.; Thaisen, K.G.; Tompkins, S.</p> <p>2011-01-01</p> <p>A systematic approach for deconvolving remotely sensed lunar <span class="hlt">olivine</span>-rich visible to near-infrared (VNIR) reflectance spectra with the Modified Gaussian Model (MGM) is evaluated with Chandrayaan-1 Moon Mineralogy Mapper (M 3) spectra. Whereas earlier studies of laboratory reflectance spectra focused only on complications due to chromite inclusions in lunar <span class="hlt">olivines</span>, we develop a systematic approach for addressing (through continuum removal) the prominent continuum slopes common to remotely sensed reflectance spectra of planetary surfaces. We have validated our continuum removal on a suite of laboratory reflectance spectra. Suites of <span class="hlt">olivine</span>-dominated reflectance spectra from a small crater near Mare Moscoviense, the Copernicus central peak, Aristarchus, and the crater Marius in the Marius Hills were analyzed. Spectral diversity was detected in visual evaluation of the spectra and was quantified using the MGM. The MGM-derived band positions are used to estimate the <span class="hlt">olivine</span>'s composition in a relative sense. Spectra of <span class="hlt">olivines</span> from Moscoviense exhibit diversity in their absorption features, and this diversity suggests some variation in <span class="hlt">olivine</span> Fe/Mg content. <span class="hlt">Olivines</span> from Copernicus are observed to be spectrally homogeneous and thus are predicted to be more compositionally homogeneous than those at Moscoviense but are of broadly similar composition to the Moscoviense <span class="hlt">olivines</span>. <span class="hlt">Olivines</span> from Aristarchus and Marius exhibit clear spectral differences from those at Moscoviense and Copernicus but also exhibit features that suggest contributions from other phases. If the various precautions discussed here are weighed carefully, the methods presented here can be used to make general predictions of absolute <span class="hlt">olivine</span> composition (Fe/Mg content). Copyright ?? 2011 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRB..121.7193C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRB..121.7193C"><span>Load relaxation of <span class="hlt">olivine</span> single crystals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cooper, Reid F.; Stone, Donald S.; Plookphol, Thawatchai</p> <p>2016-10-01</p> <p>Single crystals of ferromagnesian <span class="hlt">olivine</span> (San Carlos, AZ, peridot; Fo88-90) have been deformed in both uniaxial creep and load relaxation under conditions of ambient pressure, T = 1500°C and pO2 = 10-10 atm; creep stresses were in the range 40 ≤ σ1 (MPa) ≤ 220. The crystals were oriented such that the applied stress was parallel to [011]c, which promotes single slip on the slowest slip system in <span class="hlt">olivine</span>, (010)[001]. The creep rates at steady state match well the results of earlier investigators, as does the stress sensitivity (a power law exponent of n = 3.6). Dislocation microstructures, including spatial distribution of low-angle (subgrain) boundaries, additionally confirm previous investigations. Inverted primary creep (an accelerating strain rate with an increase in stress) was observed. Load relaxation, however, produced a singular response—a single hardness curve—regardless of the magnitude of creep stress or total accumulated strain preceding relaxation. The log stress versus log strain rate data from load-relaxation and creep experiments overlap to within experimental error. The load-relaxation behavior is distinctly different than that described for other crystalline solids, where the flow stress is affected strongly by work hardening such that a family of distinct hardness curves is generated, which are related by a scaling function. The response of <span class="hlt">olivine</span> for the conditions studied, we argue, indicates flow that is rate limited by dislocation glide, reflecting specifically a high intrinsic lattice resistance (Peierls stress).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR32A..07C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR32A..07C"><span>Load Relaxation of <span class="hlt">Olivine</span> Single Crystals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cooper, R. F.; Stone, D. S.; Plookphol, T.</p> <p>2016-12-01</p> <p>Single crystals of ferromagnesian <span class="hlt">olivine</span> (San Carlos, AZ, peridot; Fo90-92) have been deformed in both uniaxial creep and load relaxation under conditions of ambient pressure, T = 1500ºC and pO2 = 10-10 atm; creep stresses were in the range 40 ≤ σ1 (MPa) ≤ 220. The crystals were oriented such that the applied stress was parallel to [011]c, which promotes single slip on the slowest slip system in <span class="hlt">olivine</span>, (010)[001]. The creep rates at steady state match well the results of earlier investigators, as does the stress sensitivity (a power-law exponent of n = 3.6). Dislocation microstructures, including spatial distribution of low-angle (subgrain) boundaries, additionally confirm previous investigations. Inverted primary creep (an accelerating strain rate with an increase in stress) was observed. Load-relaxation, however, produced a singular response—a single hardness curve—regardless of the magnitude of creep stress or total accumulated strain preceding relaxation. The log-stress v. log-strain rate data from load-relaxation and creep experiments overlap to within experimental error. The load-relaxation behavior is distinctly different that that described for other crystalline solids, where the flow stress is affected strongly by work hardening such that a family of distinct hardness curves is generated, which are related by a scaling function. The response of <span class="hlt">olivine</span> for the conditions studied, thus, indicates flow that is rate-limited by dislocation glide, reflecting specifically a high intrinsic lattice resistance (Peierls stress).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060049097&hterms=inclusion&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dinclusion','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060049097&hterms=inclusion&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dinclusion"><span>Non-nebular Origin of Dark Mantles Around <span class="hlt">Chondrules</span> and Inclusions in CM Chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Trigo-Rodriquez, Josep M.; Rubin, Alan E.; Wasson, John T.</p> <p>2006-01-01</p> <p>Our examination of nine CM chondrites that span the aqueous alteration sequence leads us to conclude that compact dark fine mantles surrounding <span class="hlt">chondrules</span> and inclusions in CM chondrites are not discrete fine-grained rims acquired in the solar nebula as modeled by Metzler et al. [Accretionary dust mantles in CM chondrites: evidence for solar nebula processes. Geochim. Cosmochim. Acta 56, 1992, 2873-28971. Nebular processes that lead to agglomeration produce materials with porosities far higher than those in the dark mantles. We infer that the mantles were produced from porous nebular materials on the CM parent asteroid by impact-compaction (a process that produces the lowest porosity adjacent to <span class="hlt">chondrules</span> and inclusions). Compaction was followed by aqueous alteration that formed tochilinite, serpentine, Ni-bearing sulfide, and other secondary products in voids in the interchondrule regions. Metzler et al. reported a correlation between mantle thickness and the radius of the enclosed object. In Yamato 791 198 we find no correlation when all sizes of central objects and dark lumps are included but a significant correlation (r(sup 2) = 0.44) if we limit consideration to central objects with radii >35 microns; a moderate correlation is also found in QUE 97990. We suggest that impact-induced shear of a plum-pudding-like precursor produced the observed "mantles"; these were shielded from comminution during impact events by the adjacent stronger <span class="hlt">chondrules</span> and inclusions. Some mantles in CM chondrites with low degrees of alteration show distinct layers that may largely reflect differences in porosity. Typically, a gray, uniform inner layer is surrounded by an outer layer consisting of darker silicates with BSE-bright speckles. The CM-chondrite objects characterized as "primary accretionary rocks" by Metzler et al. did not form in the nebula, but rather on the parent body. The absence of solar-flare particle tracks and solar-wind-implanted rare gases in these clasts</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/2017GeCoA.202..231B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.202..231B"><span>Petrography and geochemistry of distal spherules from the K-Pg boundary in the Umbria-Marche region (Italy) and their origin as fractional condensates and melts in the Chicxulub impact plume</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belza, J.; Goderis, S.; Montanari, A.; Vanhaecke, F.; Claeys, P.</p> <p>2017-04-01</p> <p>The impact spherules from the distal K-Pg boundary sections are considered to represent silicate droplets condensed and solidified from a laterally expanding, cooling vapor plume formed upon hypervelocity impact. In the present-day Cretaceous-Paleogene boundary (K-Pg) spherule population of the Umbria-Marche region in Italy, three texturally and compositionally distinct types of impact spherules can be identified that are dominantly composed of (1) goethite, (2) K-feldspar or (3) glauconite. Although these phases represent the products of diagenetic alteration, the remnant textural characteristics of the spherules and the type of alteration product are indicative of the spherules' original compositions, which are important to constrain the physicochemical conditions prevalent throughout the impact vapor plume. The presence of relict ghost crystals and the identification of 'iddingsite' indicate that goethite likely represents pseudomorphic replacement after <span class="hlt">olivine</span>. Goethite spherules contain numerous dendritic, euhedral and skeletal spinel crystals variably dispersed in the groundmass. In terms of textures, five types of goethite spherules can be distinguished, showing striking similarities to <span class="hlt">chondrules</span>: (I) skeletal, (II) <span class="hlt">barred</span>, (III) radial/<span class="hlt">barred</span>, (IV) porphyritic and (V) relict/granular. The morphology of both spinel and <span class="hlt">olivine</span> (pseudomorphs) is consistent with established formation conditions (peak temperature Tmax, degree of supercooling ΔT, cooling rate, presence of nucleation sites) for different <span class="hlt">chondrule</span> textural types. As goethite spherules are anomalously enriched in moderately to highly refractory lithophile (Sc, V, Y, Zr, Nb, REE, Hf, Ta, Th) and siderophile (Cr, Co, Ni, W, Ir, Pt) elements, they are interpreted to represent (diagenetically altered) refractory (high-T) condensation products from a well-homogenized plume consisting of both vaporized target and projectile matter. Different from goethite spherules, K-feldspar spherules exhibit</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017M%26PS...52.2491T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017M%26PS...52.2491T"><span>Mineralogical study of brown <span class="hlt">olivine</span> in Northwest Africa 1950 shergottite and implications for the formation mechanism of iron nanoparticles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takenouchi, Atsushi; Mikouchi, Takashi; Kogure, Toshihiro</p> <p>2017-12-01</p> <p>Martian meteorites, in particular shergottites, contain darkened <span class="hlt">olivine</span> (so-called "brown <span class="hlt">olivine</span>") whose color is induced by iron nanoparticles formed in <span class="hlt">olivine</span> during a shock event. The formation process and conditions of brown <span class="hlt">olivine</span> have been discussed in the Northwest Africa 2737 (NWA 2737) chassignite. However, formation conditions of brown <span class="hlt">olivine</span> in NWA 2737 cannot be applied to shergottites because NWA 2737 has a different shock history from that of shergottites. Therefore, this study observed brown <span class="hlt">olivine</span> in the NWA 1950 shergottite and discusses the general formation process and conditions of brown <span class="hlt">olivine</span> in shergottites. Our observation of NWA 1950 revealed that <span class="hlt">olivine</span> is heterogeneously darkened between and within grains different from brown <span class="hlt">olivine</span> in NWA 2737. XANES analysis showed that brown <span class="hlt">olivine</span> contains small amounts of Fe3+ and TEM/STEM observation revealed that there is no SiO-rich phase around iron metal nanoparticles. These observations indicate that iron nanoparticles were formed by a disproportionation reaction of <span class="hlt">olivine</span> (3Fe2+<span class="hlt">olivine</span> → Fe0metal + 2Fe3+<span class="hlt">olivine</span> + Volivine, where Volivine means a vacancy in <span class="hlt">olivine</span>). Some parts of brown <span class="hlt">olivine</span> show lamellar textures in SEM observation and Raman peaks in addition to those expected for <span class="hlt">olivine</span>, implying that brown <span class="hlt">olivine</span> experienced a phase transition (to e.g., ringwoodite). In order to induce heterogeneous darkening, heterogeneous high temperature of about 1500-1700 K and shock duration of at least 90 ms are required. This heterogeneous high temperature resulted in high postshock temperature (>900 K) inducing back-transformation of most high-pressure phases. Therefore, in spite of lack of high-pressure phases, NWA 1950 (= Martian meteorites with brown <span class="hlt">olivine</span>) experienced higher pressure and temperature compared to other highly shocked meteorite groups.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140011875','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140011875"><span>H Diffusion in <span class="hlt">Olivine</span> and Pyroxene from Peridotite Xenoliths and a Hawaiian Magma Speedometer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Peslier, A. H.; Bizimis, M.</p> <p>2014-01-01</p> <p>Hydrogen is present as a trace element in <span class="hlt">olivine</span> and pyroxene and its content distribution in the mantle results from melting and metasomatic processes. Here we examine how these H contents can be disturbed during decompression. Hydrogen was analyzed by FTIR in <span class="hlt">olivine</span> and pyroxene of spinel peridotite xenoliths from Salt Lake Crater (SLC) nephelinites which are part of the rejuvenated volcanism at Oahu (Hawaii) [1,2]. H mobility in pyroxene resulting from spinel exsolution during mantle upwelling Most pyroxenes in SLC peridotites exhibit exsolutions, characterized by spinel inclusions. Pyroxene edges where no exsolution are present have less H then their core near the spinel. Given that H does not enter spinel [3], subsolidus requilibration may have concentrated H in the pyroxene adjacent to the spinel exsolution during mantle upwelling. H diffusion in <span class="hlt">olivine</span> during xenolith transport by its host magma and host magma ascent rates <span class="hlt">Olivines</span> have lower water contents at the edge and near fractures compared to at their core, while the concentrations of all other chemical elements appear homogeneous. This suggests that some of the initial water has diffused out of the <span class="hlt">olivine</span>. Water loss from the <span class="hlt">olivine</span> is thought to occur during host-magma ascent and xenolith transport to the surface [4-6]. Diffusion modeling matches best the data when the initial water content used is that measured at the core of the <span class="hlt">olivines</span>, implying that mantle water contents are preserved at the core of the <span class="hlt">olivines</span>. The 3225 cm(sup -1) OH band at times varies independantly of other OH bands, suggesting uneven H distribution in <span class="hlt">olivine</span> defects likely acquired during mantle metasomatism just prior to eruption and unequilibrated. Diffusion times (1-48 hrs) combined with depths of peridotite equilibration or of magma start of degassing allow to calculate ascent rates for the host nephelinite of 0.1 to 27 m/s.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.......103L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.......103L"><span>Compositional Zoning in Kilauea <span class="hlt">Olivine</span>: A Geochemical Tool for Investigating Magmatic Processes at Hawaiian Volcanoes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lynn, Kendra J.</p> <p></p> <p><span class="hlt">Olivine</span> compositions and zoning patterns have been widely used to investigate the evolution of magmas from their source to the Earthfs surface. Modeling the formation of compositional zoning in <span class="hlt">olivine</span> crystals has been used to retrieve timescales of magma residence, mixing, and transit. This dissertation is composed of three projects that apply diffusion chronometry principles to investigate how zoned <span class="hlt">olivine</span> phenocrysts record magmatic processes at Hawaiian volcanoes. <span class="hlt">Olivine</span> phenocrysts from K.lauea, the most active and thoroughly studied volcano in Hawaiei, are used to develop a better understanding of how Hawaiian <span class="hlt">olivine</span> crystals record magmatic histories. This work begins by examining how crustal processes such as magma mixing and diffusive reequilibration can modify <span class="hlt">olivine</span> compositions inherited from growth in parental magmas (Chapter 2). Diffusive re-equilibration of Fe-Mg, Mn, and Ni in <span class="hlt">olivine</span> crystals overprints the chemical relationships inherited during growth, which strongly impacts interpretations about mantle processes and source components. These issues are further complicated by sectioning effects, where small (400 ƒEm along the c-axis) <span class="hlt">olivine</span> crystals are more susceptible to overprinting compared to large (800 ƒEm) crystals. <span class="hlt">Olivine</span> compositions and zoning patterns are then used to show that magmas during K.laueafs explosive Keanak.koei Tephra period (1500-1823 C.E.) were mixed and stored in crustal reservoirs for weeks to months prior to eruption (Chapter 3). Fe-Mg disequilibrium between <span class="hlt">olivine</span> rims and their surrounding glasses show that a late-stage mixing event likely occurred hours to days prior to eruption, but the exact timescale is difficult to quantify using Fe-Mg and Ni diffusion. Lithium, a rapidly diffusing trace element in <span class="hlt">olivine</span>, is modeled for the first time in a natural volcanic system to quantify this late-stage, short-duration mixing event (Chapter 4). Lithium zoning in <span class="hlt">olivine</span> records both growth and diffusion processes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70001175','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70001175"><span>Serpentinization and alteration in an <span class="hlt">olivine</span> cumulate from the Stillwater Complex, Southwestern Montana</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Page, N.J.</p> <p>1976-01-01</p> <p>Some of the <span class="hlt">olivine</span> cumulates of the Ultramafic zone of the Stillwater Complex, Montana, are progressively altered to serpentine minerals and thompsonite. Lizardite and chrysotile developed in the cumulus <span class="hlt">olivine</span> and postcumulus pyroxenes; thompsonite developed in postcumulus plagioclase. The detailed mineralogy, petrology, and chemistry indicate that <span class="hlt">olivine</span> and plagioclase react to form the alteration products, except for H2O, without changes in the bulk composition of the rocks. ?? 1976 Springer-Verlag.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017DokES.475..919K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017DokES.475..919K"><span>Experimental testing of <span class="hlt">olivine</span>-melt equilibrium models at high temperatures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krasheninnikov, S. P.; Sobolev, A. V.; Batanova, V. G.; Kargaltsev, A. A.; Borisov, A. A.</p> <p>2017-08-01</p> <p>Data are presented on the equilibrium compositions of <span class="hlt">olivine</span> and melts in the products of 101 experiments performed at 1300-1600°C, atmospheric pressure, and controlled oxygen fugacity by means of new equipment at the Vernadsky Institute. It was shown that the available models of the <span class="hlt">olivine</span>-melt equilibrium describe with insufficient adequacy the natural systems at temperatures over 1400°C. The most adequate is the model by Ford et al. (1983). However, this model overestimates systematically the equilibrium temperature with underestimating by 20-40°C at 1450-1600°C. These data point to the need for developing a new, improved quantitative model of the <span class="hlt">olivine</span>-melt equilibrium for high-temperature magnesian melts, as well as to the possibility of these studies on the basis of the equipment presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050175986','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050175986"><span>Temperature Dependence and Recoil-free Fraction Effects in <span class="hlt">Olivines</span> Across the Mg-Fe Solid Solution</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sklute, E. C.; Rothstein, Y.; Dyar, M. D.; Schaefer, M. W.; Menzies, O. N.; Bland, P. A.; Berry, F. J.</p> <p>2005-01-01</p> <p><span class="hlt">Olivine</span> and pyroxene are the major ferromagnesian minerals in most meteorite types and in mafic igneous rocks that are dominant at the surface of the Earth. It is probable that they are the major mineralogical components at the surface of any planetary body that has undergone differentiation processes. In situ mineralogical studies of the rocks and soils on Mars suggest that <span class="hlt">olivine</span> is a widespread mineral on that planet s surface (particularly at the Gusev site) and that it has been relatively unaffected by alteration. Thus an understanding of the characteristics of Mossbauer spectra of <span class="hlt">olivine</span> is of great importance in interpreting MER results. However, variable temperature Mossbauer spectra of <span class="hlt">olivine</span>, which are needed to quantify recoil-free fraction effects and to understand the temperature dependence of <span class="hlt">olivine</span> spectra, are lacking in the literature. Thus, we present here a study of the temperature dependence and recoil-free fraction of a series of synthetic <span class="hlt">olivines</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.B33I..02D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.B33I..02D"><span>Effect of the Hydrothermal Fluid Composition on the Serpentinization of <span class="hlt">Olivine</span> and Pyroxene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Daniel, I.; Andreani, M.</p> <p>2016-12-01</p> <p>The hydrothermal alteration of ultramafic rocks leads to the serpentinization reaction that mainly forms serpentine and variable amounts of talc, brucite and magnetite, as well as hydrogen and magnesite when carbonate is present in the fluid. The serpentinization kinetics of pyroxene under hydrothermal conditions has been very little studied in comparison with <span class="hlt">olivine</span>, and both have been evaluated experimentally only in simple aqueous fluids. Here, we have evaluated the effect of the fluid chemistry - aluminum, carbonate and pH on the serpentinization rate of <span class="hlt">olivine</span> and orthopyroxene at 200 °C, 340 °C and 200 MPa to simulate natural hydrothermal conditions. We used low-pressure diamond-anvil cells (lp-DAC) and time-resolved X-ray diffraction to monitor in situ the progress of serpentinization in twelve experiments. We also performed several complementary long-lasting experiments of several days in particular with orthopyroxene, for which in situ monitoring was not possible. At 340 °C in presence of Al and/or carbonate and at high pH, <span class="hlt">olivine</span> conversion into lizardite is extremely fast with a half-time reaction t1/2 = 2 hrs only, while orthopyroxene did not react much even after 6 days (11%). In contrast to <span class="hlt">olivine</span>, orthopyroxene conversion to serpentine was faster without Al (48 % in 6 days). Magnetite was also observed to form in the runs with <span class="hlt">olivine</span> at 340 °C and moderate pH. In experiments run with orthopyroxene only, we observed the exclusive formation of proto-serpentine instead of lizardite. We propose that the contrasted effect of Al on the serpentinization rate of <span class="hlt">olivine</span> and orthopyroxene results from the complexation of Al in the solution that reacts differently with the mineral surfaces during their dissolution. The positively charged <span class="hlt">olivine</span> surface allows the adsorption of the dominant negatively charged Al(OH)4- complex, while the neutral surface of orthopyroxene does not. This adsorption process could facilitate both the dissolution of <span class="hlt">olivine</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910057730&hterms=redox+reaction&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dredox%2Breaction','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910057730&hterms=redox+reaction&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dredox%2Breaction"><span>Moessbauer spectra of <span class="hlt">olivine</span>-rich achondrites - Evidence for preterrestrial redox reactions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Burns, R. G.; Martinez, S. L.</p> <p>1991-01-01</p> <p>Moessbauer spectral measurements at 4.2 K were made on several ureilites and the two shergottites found in Antarctica, as well as two ureilite falls, three SNC meteorite falls, and two finds in order to distinguish products of preterrestrial redox reactions from phases formed during oxidative weathering on the earth. The spectra indicated that several ureilites contain major proportions of metallic iron, much of which resulted from preterrestrial carbon-induced reduction of ferrous iron in the outermost 10-100 microns of <span class="hlt">olivine</span> grains in contact with carbonaceous material in the ureilites. The cryptocrystalline nature of these Fe inclusions in <span class="hlt">olivine</span> renders the metal extremely vulnerable to aerial oxidation, even in ureilites collected as falls. It is inferred that the nanophase ferric oxides or oxyhydroxides identified in Brachina and Lafayette were produced by terrestrial weather of <span class="hlt">olivines</span> before the meteorites were found. The absence of goethite in two <span class="hlt">olivine</span>-bearing Antarctic shergottites suggests that the 2 percent ferric iron determined in their Moessbauer spectra also originated from oxidation on Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.477.2786P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.477.2786P"><span><span class="hlt">Olivine</span>-rich asteroids in the near-Earth space</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Popescu, Marcel; Perna, D.; Barucci, M. A.; Fornasier, S.; Doressoundiram, A.; Lantz, C.; Merlin, F.; Belskaya, I. N.; Fulchignoni, M.</p> <p>2018-06-01</p> <p>In the framework of a 30-night spectroscopic survey of small near-Earth asteroids (NEAs), we present new results regarding the identification of <span class="hlt">olivine</span>-rich objects. The following NEAs were classified as A-type using visible spectra obtained with 3.6-m New Technology Telescope: (293726) 2007 RQ17, (444584) 2006 UK, 2012 NP, 2014 YS34, 2015 HB117, 2015 LH, 2015 TB179, 2015 TW144. We determined a relative abundance of 5.4 per cent (8 out of 147 observed targets) A-types at a 100-m size range of NEA population. The ratio is at least five times larger compared with the previously known A-types, which represent less than ˜ 1 per cent of NEAs taxonomically classified. By taking into account that part of our targets may not be confirmed as <span class="hlt">olivine</span>-rich asteroids by their near-infrared spectra, or they can have a nebular origin, our result provides an upper-limit estimation of mantle fragments at size ranges below 300 m. Our findings are compared with the `battered-to-bits' scenario, claiming that at small sizes the <span class="hlt">olivine</span>-rich objects should be more abundant when compared with basaltic and iron ones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017A%26A...597A..50Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017A%26A...597A..50Y"><span>Optical spectroscopic characterizations of laser irradiated <span class="hlt">olivine</span> grains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Yazhou; Zhang, Hao; Wang, Ziwei; Yuan, Ye; Li, Shaolin; Hsu, Weibiao; Liu, Chujian</p> <p>2017-01-01</p> <p>Context. Visible and near-infrared spectra of asteroids are known to be susceptible to nanophase irons produced by space weathering processes, thus making mineral identifications difficult. Mid-infrared spectroscopy may retain more mineral features owing to its lattice vibrational nature. Aims: We investigate the structure and reflectance spectral feature changes of <span class="hlt">olivine</span> grains before and after simulated space weathering. Methods: We irradiate <span class="hlt">olivine</span> grains by using pulsed laser to simulate varying degrees of micrometeorite bombardments. Reflectance measurements from 0.5 to 25 μm and radiative transfer calculations were carried out in order to compare them with each other. Results: Both the experimental simulations and modeling results indicate that the mid-infrared spectral features of <span class="hlt">olivine</span> grains can survive the intense irradiations. Although the Christansen Feature is slightly shifted to longer wavelength, major vibrational bands remain essentially unchanged, because the lattice structure is quite immune to even the strongest irradiations, as revealed by both the X-ray diffraction and Raman scattering measurements. Conclusions: Mid-infrared spectroscopy is much more immune to productions of nanophase irons and amorphous materials and thus may be used more reliably in remote detections of minerals on asteroid surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013300','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013300"><span>Space Weathering of <span class="hlt">Olivine</span> in Lunar Soils: A Comparison to Itokawa Regolith Samples</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Keller, L. P.; Berger, E. L.</p> <p>2014-01-01</p> <p>Regolith particles from airless bodies preserve a record of the space weathering processes that occurred during their surface exposure history. These processes have major implications for interpreting remote-sensing data from airless bodies. Solar wind irradiation effects occur in the rims of exposed grains, and impact processes result in the accumulation of vapordeposited elements and other surface-adhering materials. The grains returned from the surface of Itokawa by the Hayabusa mission allow the space weathering "style" of a chondritic, asteroidal "soil" to be compared to the lunar case. Here, we present new studies of space-weathered <span class="hlt">olivine</span> grains from lunar soils, and compare these results to <span class="hlt">olivine</span> grains from Itokawa. Samples and Methods: We analyzed microtome thin sections of <span class="hlt">olivine</span> grains from the 20-45 micron fractions of three lunar soils: 71061, 71501 and 10084 (immature, submature and mature, respectively). Imaging and analytical data were obtained using a JEOL 2500SE 200kV field-emission scanning-transmission electron microscope equipped with a thin-window energy-dispersive x-ray spectrometer. Similar analyses were obtained from three Hayabusa <span class="hlt">olivine</span> grains. Results and Discussion: We observed lunar grains showing a range of solar flare track densities (from <10(exp 9) to approx.10(exp 12)/sq cm). The lunar <span class="hlt">olivines</span> all show disordered, highly strained, nanocrystalline rims up to 150-nm thick. The disordered rim thickness is positively correlated with solar flare track density. All of the disordered rims are overlain by a Si-rich amorphous layer, ranging up to 50-nm thick, enriched in elements that are not derived from the host <span class="hlt">olivine</span> (e.g., Ca, Al, and Ti). The outmost layer represents impact-generated vapor deposits typically observed on other lunar soil grains. The Hayabusa <span class="hlt">olivine</span> grains show track densities <10(exp 10)/sq cm and display disordered rims 50- to 100-nm thick. The track densities are intermediate to those observed in <span class="hlt">olivines</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.T33D..02C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.T33D..02C"><span>New Insights on the Rheology of <span class="hlt">Olivine</span> Deformed under Lithospheric Temperature Conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cordier, P.; Demouchy, S. A.; Mussi, A.; Tommasi, A.</p> <p>2014-12-01</p> <p>Rheology of mantle rocks at lithospheric temperatures remains poorly constrained, since most experimental studies on creep mechanisms of <span class="hlt">olivine</span> single crystals ((MgFe)2SiO4, Pbnm) and polycrystalline <span class="hlt">olivine</span> aggregates were performed at high-temperatures (T >> 1200oC). In this study, we report results from deformation experiments on oriented single crystals of San Carlos <span class="hlt">olivine</span> and polycrystalline <span class="hlt">olivine</span> aggregate at temperatures relevant of the uppermost mantle (ranging from 800o to 1090oC) in tri-axial compression. The experiments were carried out at a confining pressure of 300 MPa in a high-resolution gas-medium mechanical testing apparatus at various constant strain rates (from 7 x 10-6 s-1 to 1 x 10-4 s-1). Mechanical tests show that mantle lithosphere is actually weaker than previously inferred from the extrapolation of high-temperature experiments. In this study, we present characterization of dislocation microstructures based on transmission electron microscopy and electron tomography. It is shown that below 1000°C, dislocation activity is restricted to [001] glide with a strong predominance of {110} as glide planes. We observe recovery mechanisms which suggest that the mechanical properties observed in laboratory experiments represent an upper bound for the actual behavior of <span class="hlt">olivine</span> under lithospheric mantle conditions. Moreover, the drastic reduction in slip system activity observed questions the ability of deforming <span class="hlt">olivine</span> aggregates in the ductile regime at such temperatures. We show that ductility is preserved thanks to the activation of alternative deformation mechanisms in grain boundaries involving disclinations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V23B0485S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V23B0485S"><span>Meeting the Continental Crust: the Hidden <span class="hlt">Olivine</span> Trauma in Subduction Settings</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salas Reyes, P.; Ruprecht, P.; Rabbia, O. M.; Hernandez, L.</p> <p>2017-12-01</p> <p>In a conventional framework, <span class="hlt">olivine</span> zonation represents concentric growth from an evolving liquid. Alternatively, it has been suggested (e.g. Welsch et al. 2014) that <span class="hlt">olivine</span> develop dendritic textures and compositional discontinuities due to rapid growth and boundary layer effects, respectively, where any complex zoning is quickly erased through diffusive re-equilibration in the high temperature magmatic environment. In particular, <span class="hlt">olivine</span> crystals from large volcanic centers in convergent margins rarely preserve such dendritic textures and complex zoning due prolonged magma residence. Small volume, mafic monogenetic vents may bypass such crustal re-equilibration and potentially record the otherwise elusive early <span class="hlt">olivine</span> growth history. We selected tephra deposits from Los Hornitos, in the Andean arc of Central Chile (35.5˚S), that represents primitive magmas ( 15 wt.% MgO) and contain magnesian <span class="hlt">olivines</span> (Fo>88) hosting quenched melt inclusions. We obtained detailed quantitative EPMA zoning profiles and measured volatile contents (H, C, S, Cl) in the co-existing melt inclusions. Furthermore, we analyzed mineral morphologies connecting compositional zoning with growth textures. We find that 40% of the <span class="hlt">olivine</span> crystals retain dendritic shapes while the others are polyhedral with trapped melt inclusions and cavities. The polyhedral crystals are normally zoned (Fo92 to Fo88; Ni 4000 ppm to 1000 ppm), however an oscillatory zonation depicted by concentric -coupled Fo and Ni- enriched layers exist and therefore even those crystals still preserve also a more complete growth history. The related melt inclusions yield values of up to 6000 ppm of S. Such zonation may imply sudden growth during elevated degrees of undercooling (-ΔT > 60°C) as the magmas transit from the hot mantle to the cooler conditions in the crust. Moreover, the preservation of such Fo and Ni zonation requires limited time between crystal growth and eruption. The elevated S content in melt inclusions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T41A0616L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T41A0616L"><span>Low temperature dissolution creep induced B-type <span class="hlt">olivine</span> fabric during serpentinization and deformation in mantle wedge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, W.; Zhang, J.</p> <p>2017-12-01</p> <p>The B-type <span class="hlt">olivine</span> fabric (i.e., the [010]ol axes subnormal to foliation and the [001]ol axes subparallel to the lineation) has been regarded as an important <span class="hlt">olivine</span> fabric for interpreting global trench-parallel S-wave polarization in fore-arc regions. However, strong serpentinization and cold temperature environment in the mantle wedge should inhibit development of the B-type <span class="hlt">olivine</span> fabric that requires high temperature to activate solid-state plastic deformation. Here we report fabrics of <span class="hlt">olivine</span> and antigorite generated at low temperatures (300-370 oC) during serpentinization in a fossil mantle wedge of the Val Malenco area, Central Alps. <span class="hlt">Olivine</span> in the serpentine matrix develops a pronounced B-type fabric, while antigorite in the same matrix displays a strong crystallographic orientation (CPO) with the (001) and the [010] subparallel to foliation and lineation, respectively. The following evidence leads to the conclusion that the B-type <span class="hlt">olivine</span> fabric is resulted from dissolution creep assisted by grain boundaries sliding (GBS) and grain rotation, rather than solid-state plastic deformation: (1) serpentinization took place at low temperatures and a fluid-enriched environment, ideal for dissolution-precipitation creep; (2) the voids and zigzag boundaries along the interface between antigorite and <span class="hlt">olivine</span> suggest a fluid dissolution reaction; (3) the primary coarse <span class="hlt">olivine</span> develops a nearly random fabric, indicating the B-type fabrics in the fine-grained <span class="hlt">olivine</span> can't be inherited fabrics. These results document for the first time the B-type <span class="hlt">olivine</span> CPO formed by dissolution creep at low temperatures during serpentinization and provide a mechanism to reconcile petrofabric observations with geophysical observations of trench parallel fast S-wave seismic anisotropy in fore-arc mantle wedge regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.222..146C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.222..146C"><span>New constraints on Xe incorporation mechanisms in <span class="hlt">olivine</span> from first-principles calculations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Crépisson, Céline; Blanchard, Marc; Lazzeri, Michele; Balan, Etienne; Sanloup, Chrystèle</p> <p>2018-02-01</p> <p>Storage of Xe at depth in silicate minerals has recently been proposed to explain the low Xe abundance in the Earth's and Mars' atmospheres compared to other noble gases (the so-called 'Missing Xenon' issue). Evidences for incorporation, and thus reactivity of Xe in <span class="hlt">olivine</span> at high pressure and high temperature are based on variations in cell parameters and the appearance of a new Raman band. To constrain the, so far only hypothetical, Xe incorporation mechanism in <span class="hlt">olivine</span>, we theoretically investigated models of Xe-bearing <span class="hlt">olivine</span> using density functional theory. Three types of incorporation mechanisms are tested: Xe for Si and Xe for Mg substitutions, and interstitial Xe. Xe for Si substitution, implying an oxidation of Xe, is found to be the only mechanism consistent with experimental observations, leading to an increase of cell parameter a and the appearance of a new Raman band around 720-750 cm-1 associated with Xesbnd O stretching vibrations. Raman spectroscopy makes it possible to identify Xe incorporation site, even at low Xe content, due to high Xe polarizability. An estimation of Xe content in <span class="hlt">olivine</span>, based on present work and previous in situ experimental results, shows that up to 0.4 at.% Xe could be stored in <span class="hlt">olivine</span> at depth.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.V13B0690L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.V13B0690L"><span>NiO and Fe/Mn in Fo-rich <span class="hlt">olivines</span> from OIB, MORB, and mantle peridotites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, H.; Baker, M.; Hofmann, A. E.; Clague, D.; Stolper, E.</p> <p>2006-12-01</p> <p><span class="hlt">Olivines</span> from mantle peridotites have a narrow range of NiO (0.36±0.03 [1σ] wt%), but NiO of <span class="hlt">olivines</span> in basalts suggest NiO in mantle <span class="hlt">olivines</span> is actually more variable: e.g., Hawaiian phenocrysts (Fo>90) have NiO >0.55%, and <span class="hlt">olivines</span> from continental flood basalts can have >0.5% NiO. At the other end of the spectrum, some basaltic suites (e.g., Iceland, MORBs) have Fo>90 <span class="hlt">olivines</span> with NiO >0.2%. Partial melting calculations on peridotites show it is difficult to generate liquids that crystallize Fo>90 <span class="hlt">olivines</span> with >0.4% NiO without resorting to complex processes. Hypotheses to explain the variability of NiO in mantle-derived <span class="hlt">olivines</span> include (1) reaction of peridotite with silica-rich melts of eclogite results in decreasing modal abundance of <span class="hlt">olivine</span> and increasing NiO in <span class="hlt">olivine</span> [1,2]; (2) magmas with NiO-rich <span class="hlt">olivines</span> come from sources enriched in NiO due to a core-derived component [3]. [4] proposed that high Fe/Mn of Hawaiian vs. Icelandic and MORB lavas reflect a core-derived component in their sources. Possible core incorporation is poorly constrained but FeO and NiO are expected to increase by such processes, leading to correlations between NiO and Fe/Mn in mantle rocks with significant core-derived components. We present high-precision analyses of Fo-rich <span class="hlt">olivines</span> from OIBs, MORBs, komatiites, and mantle peridotites, focusing on NiO contents and Fe/Mn ratios. Our goal is to test hypotheses to explain elevated NiO of Fo-rich <span class="hlt">olivines</span> in basalts. <span class="hlt">Olivines</span> are Fo85.1-93.4; more were analyzed, but we focused on this range to avoid complications due to decreasing NiO in <span class="hlt">olivine</span> with crystallization. Errors (1σ) are 0.01 wt% in NiO and 1.5 in Fe/Mn (wt). Our data show several features: (1) NiO contents and Fe/Mn ratios of Fo>88 <span class="hlt">olivines</span> are positively correlated, with the low end of the trend (NiO ~0.23%, Fe/Mn ~61) defined by MORB and Iceland and the high end of the trend (NiO ~0.55%, Fe/Mn ~80) by Reunion and Hawaii. Between these end points, there is a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18..688L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18..688L"><span><span class="hlt">Bar</span> dimensions and <span class="hlt">bar</span> shapes in estuaries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Leuven, Jasper; Kleinhans, Maarten; Weisscher, Steven; van der Vegt, Maarten</p> <p>2016-04-01</p> <p>Estuaries cause fascinating patterns of dynamic channels and shoals. Intertidal sandbars are valuable habitats, whilst channels provide access to harbors. We still lack a full explanation and classification scheme for the shapes and dimensions of <span class="hlt">bar</span> patterns in natural estuaries, in contrast with <span class="hlt">bars</span> in rivers. Analytical physics-based models suggest that <span class="hlt">bar</span> length in estuaries increases with flow velocity, tidal excursion length or estuary width, depending on which model. However, these hypotheses were never validated for lack of data and experiments. We present a large dataset and determine the controls on <span class="hlt">bar</span> shape and dimensions in estuaries, spanning <span class="hlt">bar</span> lengths from centimeters (experiments) to 10s of kilometers length. First, we visually identified and classified 190 <span class="hlt">bars</span>, measured their dimensions (width, length, height) and local braiding index. Data on estuarine geometry and tidal characteristics were obtained from governmental databases and literature on case studies. We found that many complex <span class="hlt">bars</span> can be seen as simple elongated <span class="hlt">bars</span> partly cut by mutually evasive ebb- and flood-dominated channels. Data analysis shows that <span class="hlt">bar</span> dimensions scale with estuary dimensions, in particular estuary width. Breaking up the complex <span class="hlt">bars</span> in simple <span class="hlt">bars</span> greatly reduced scatter. Analytical <span class="hlt">bar</span> theory overpredicts <span class="hlt">bar</span> dimensions by an order of magnitude in case of small estuarine systems. Likewise, braiding index depends on local width-to-depth ratio, as was previously found for river systems. Our results suggest that estuary dimensions determine the order of magnitude of <span class="hlt">bar</span> dimensions, while tidal characteristics modify this. We will continue to model <span class="hlt">bars</span> numerically and experimentally. Our dataset on tidal <span class="hlt">bars</span> enables future studies on the sedimentary architecture of geologically complex tidal deposits and enables studying effects of man-induced perturbations such as dredging and dumping on <span class="hlt">bar</span> and channel patterns and habitats.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V51D0383Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V51D0383Y"><span><span class="hlt">Olivine</span>-Rich Troctolite from the Southwest Indian Ridge: Constrains on Melt-Rock Reaction beneath Mid-Ocean Ridges</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, A. Y.</p> <p>2017-12-01</p> <p>The origin of <span class="hlt">olivine</span>-rich troctolite, which have been recovered in the plutonic sample suites from the fast-spreading East Pacific Rise, and slow-spreading Mid-Atlantic Ridge and Central Indian Ridge, has been highly debated. They can form either by fractionation of primitive mid-ocean ridge basalt (MORB) melts or by melt migrating through pre-existing (possibly mantle) <span class="hlt">olivine</span> matrix, thus recording valuable information of magmatic process at mantle-crust transition. This study presents in situ major and trace element study on the <span class="hlt">olivine</span>-rich troctolite first reported from the ultraslow-spreading Southwest Indian Ridge (SWIR), together with a series of samples from peridotite, gabbro to basalt from an amagmatic segment at 53°E during Dayangyihao Cruises, to investigate the magmatic processes occurred at mantle-crust transition and origin of <span class="hlt">olivine</span>-rich troctolite. The <span class="hlt">olivine</span> in the troctolite shows cumulate textures with interstitial clinopyroxene, plagioclase and minor spinel, which is cross-cut by an <span class="hlt">olivine</span> gabbro vein. <span class="hlt">Olivine</span> in the troctolite show only mildly decreasing NiO contents (from 0.31-0.25 wt.%) with decreasing Fo (from 86 to 81), and even <span class="hlt">olivine</span> in the gabbro have NiO up to 0.24 wt.% with Fo of 75. The Fo vs. Ni correlation of <span class="hlt">olivine</span> is shifted to uniquely higher NiO at a certain Fo compared to the trends defined by either <span class="hlt">olivine</span> from other lower oceanic crust (LOC) cumulates worldwide or <span class="hlt">olivine</span> compositions from classic fractionation model for primitive MORB magma. Interstitial clinopyroxene in the troctolite have high Mg# (88-90), Cr2O3 (up to 1.51 wt.%) and TiO2 contents (up to 1.01 wt.%) with Eu/Eu* from 0.4-0.6. Such high-Ti-Cr-Mg# clinopyroxene is rare among global LOC cumulates, and cannot result from simple fractionation of MORB magma. The mineral compositions in the <span class="hlt">olivine</span>-rich troctolite could be modeled by reaction between a primitive <span class="hlt">olivine</span> matrix and a highly evolved melt (with 2.4 wt.% TiO2), and such a melt composition is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030111398&hterms=equilibrium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dequilibrium','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030111398&hterms=equilibrium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dequilibrium"><span><span class="hlt">Olivine</span>-Orthopyroxene Equilibrium in Metal-rich Systems: Applications to Achondrites and Equilibrated Chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lauretta, D. S.; Benedix, G. K.; McCoy, T. J.</p> <p>2003-01-01</p> <p><span class="hlt">Olivine</span> and orthopyroxene are major minerals in every type of stony meteorite. The majority of achondritic meteorites and silicate-bearing iron meteorites have experienced high temperatures. If these temperatures persisted for an extended period of time then the iron contents of <span class="hlt">olivine</span> and orthopyroxene should be in equilibrium. In their study of ungrouped clasts and chondritic meteorites, suggested that the equilibrium compositions of <span class="hlt">olivine</span> and orthopyroxene should fall on a mixing line between LL chondrites and aubrites. Here we show that this is not necessarily the case and that a range of FeO contents in <span class="hlt">olivine</span> and orthopyroxene can be in equilibrium with each other. The key parameters that determine the equilibrium Fe content in these minerals are temperature, oxygen fugacity (fO2), and silica activity (aSiO2).</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('http://adsabs.harvard.edu/abs/2010EGUGA..12.1418F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.1418F"><span>Phosphorus zoning in <span class="hlt">olivine</span> of Kilauea Iki lava lake, Hawaii</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fabbrizio, Alessandro; Beckett, John R.; Baker, Michael B.; Stolper, Edward M.</p> <p>2010-05-01</p> <p>Kilauea Iki lava lake was formed when the lavas of the 1959 summit eruption of Kilauea volcano ponded in Kilauea Iki pit crater, as described by [1]. The main chamber of this lake has been drilled repeatedly from 1960 to 1981 as the lake has cooled and crystallized and partial descriptions of core can be found in [2-7]. The bulk of the core consists of a gray, <span class="hlt">olivine</span>-phyric basalt matrix [3]. Rapid diffusion of divalent cations through <span class="hlt">olivine</span> at magmatic temperatures can delete information on early-formed zoning and thus information on early magmatic history, recorded in <span class="hlt">olivine</span> during its growth, is often largely lost [8-11]. In the last years many studies [8-11] have shown that natural <span class="hlt">olivine</span>, terrestrial and extraterrestrial, from several localities and rock types can preserve a complex zoning in P (sometimes associated with Cr and Al). Simple crystallization experiments conducted by [10] and [11] were able to replicate these features (i.e., sector and oscillatory zoning). Here, we describe P, Cr and Al zoning in <span class="hlt">olivine</span> from the 1981 drilling of Kilauea Iki lava lake hole #1 (KI81-1) [6]. Kα X-ray intensity maps and major and minor element quantitative analyses were obtained using the Caltech JEOL JXA-8200 electron microprobe. We acquired P, Cr, Al, Fe and Ti X-ray maps simultaneously at 15 kV and 400 nA, a beam diameter of 1 μm, pixel spacing of 1-2 μm, and count times of 420-1500 msec/step were used depending on the dimension of the crystal. 15 kV and 40 nA with a beam diameter of 1 μm were used to collect quantitative analyses. P2O5 contents of the Iki <span class="hlt">olivines</span> range from below detection limit to 0.30 wt%. Zoning in phosphorus, based on X-ray intensity maps, was observed in all <span class="hlt">olivines</span> we examined. The P zoning patterns of the <span class="hlt">olivines</span> display several styles. P shows oscillatory zoning comparable to that seen in terrestrial and extraterrestrial igneous <span class="hlt">olivines</span> and in experimentally grown <span class="hlt">olivine</span> [8-11]; high P regions, inside the crystals, outline</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010LPI....41.2239H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010LPI....41.2239H"><span>Correlations Between <span class="hlt">Olivine</span> Abundance and Thermal Inertia: Implications for Global Weathering and/or Alteration 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>Hamilton, V. E.; McDowell, M. L.; Koeppen, W. C.</p> <p>2010-03-01</p> <p>TES data show no global trend between thermal inertia and <span class="hlt">olivine</span> abundance. But it is premature to conclude that all dark surfaces were once more mafic OR that <span class="hlt">olivine</span> is not preferentially removed from <span class="hlt">olivine</span>-enriched outcrops as they erode.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.481..372C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.481..372C"><span>Old formation ages of igneous clasts on the L chondrite parent body reflect an early generation of planetesimals or <span class="hlt">chondrule</span> formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Crowther, Sarah A.; Filtness, Michal J.; Jones, Rhian H.; Gilmour, Jamie D.</p> <p>2018-01-01</p> <p>The Barwell meteorite contains large, abundant clasts that are igneous in nature. We report iodine-xenon ages of five clasts and one sample of host chondrite material. The fragment of host chondrite material yielded the oldest age determined: 4567.8 ± 1.2 Ma. Two clasts produced old, well defined ages of 4564.96 ± 0.33 Ma and 4565.60 ± 0.33 Ma. These, and a third clast having a less precise old age of 4566.0 ± 3.2 Ma, are interpreted as recording the timing of crystallisation of the samples. They were incorporated into the Barwell parent body before it underwent thermal metamorphism, but the I-Xe ages survived secondary processing on the parent body and were not reset by metamorphism, metasomatism or shock. Two further clasts record younger ages of 4560.96 ± 0.45 Ma and 4554.22 ± 0.38 Ma. These samples contain a high abundance of albitic mesostasis, and the most likely explanation of the ages is that they record the timing of metasomatism on the parent body. We also analysed four host chondrite samples that do not give I-Xe ages: in these samples, the system appears to have been disturbed by shock. It has been suggested previously that the igneous clasts are derived from an early generation of partially melted asteroids. We do not have direct evidence that the clasts we examined were necessarily derived from a partially differentiated body, only that they were derived from cooling of a silicate melt; the clasts could thus be the products of any one of several proposed models for <span class="hlt">chondrule</span> formation. Our results indicate that processes akin to <span class="hlt">chondrule</span> formation, in that they involve rapid cooling of a silicate melt, were ongoing at the same time as CAI formation, lending support to the suggestion that Al-Mg <span class="hlt">chondrule</span> ages indicate either heterogeneous distribution of 26Al or resetting of the Al-Mg system after <span class="hlt">chondrule</span> formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770051870&hterms=Recrystallization&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DRecrystallization','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770051870&hterms=Recrystallization&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DRecrystallization"><span>Shock-induced fine-grained recrystallization of <span class="hlt">olivine</span> - Evidence against subsolidus reduction of Fe/2+/</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ahrens, T. J.; Tsay, F.-D.; Live, D. H.</p> <p>1976-01-01</p> <p>Electron spin resonance (ESR) studies have been carried out on three single grains of terrestrial <span class="hlt">olivine</span> (Fo90) shock loaded along the 010 line to peak pressures of 280, 330, and 440 kbar. The results indicate that neither metallic Fe similar to that observed in returned lunar soils nor paramagnetic Fe(3+) caused by oxidation of Fe(2+) has been produced in these shock experiments. Trace amounts of Mn (2+) have been detected in both shocked and unshocked <span class="hlt">olivine</span>. The ESR signals of Mn(2+) show spectral features which are found to correlate with the degree of shock-induced recrystallization observed petrographically. The increasing mass fraction of recrystallized <span class="hlt">olivine</span> correlates with increasing shock pressures. This phenomenon is modelled assuming it results from the progressive effect of the shock-induced transformation of the <span class="hlt">olivine</span> to a yet unknown high-pressure phase and its subsequent reversion to the low-pressure <span class="hlt">olivine</span> phase. The mass fraction of recrystallized material is predicted to be nearly linear with shock pressure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.219..124R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.219..124R"><span>Lithium isotope fractionation by diffusion in minerals Part 2: <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Richter, Frank; Chaussidon, Marc; Bruce Watson, E.; Mendybaev, Ruslan; Homolova, Veronika</p> <p>2017-12-01</p> <p>Recent experiments have shown that lithium isotopes can be significantly fractionated by diffusion in silicate liquids and in augite. Here we report new laboratory experiments that document similarly large lithium isotopic fractionation by diffusion in <span class="hlt">olivine</span>. Two types of experiments were used. A powder-source method where lithium from finely ground spodumene (LiAlSi2O6) diffused into oriented San Carlos <span class="hlt">olivine</span>, and piston cylinder annealing experiments where Kunlun clinopyroxene (∼30 ppm lithium) and oriented San Carlos <span class="hlt">olivine</span> (∼2 ppm lithium) were juxtaposed. The lithium concentration along traverses across the run products was measured using both laser ablation as a source for a Varian 820-MS quadrupole mass spectrometer and a CAMECA 1270 secondary ion mass spectrometer. The CAMECA 1270 was also used to measure the lithium isotopic fractionation across <span class="hlt">olivine</span> grains recovered from the experiments. The lithium isotopes were found to be fractionationed by many tens of permil in the diffusion boundary layer at the grain edges as a result of 6Li diffusing significantly faster than 7Li. The lithium concentration and isotopic fractionation data across the <span class="hlt">olivine</span> recovered from the different experiments were modeled using calculations in which lithium was assumed to be of two distinct types - one being fast diffusing interstitial lithium, the other much less mobile lithium on a metal site. The two-site diffusion model involves a large number of independent parameters and we found that different choices of the parameters can produce very comparable fits to the lithium concentration profiles and associated isotopic fractionation. Because of this nonuniqueness we are able to determine only a range for the relative diffusivity of 6Li compared to 7Li. When the mass dependence of lithium diffusion is parameterized as D6Li /D7Li =(7 / 6) β , the isotope fractionation for diffusion along the a and c crystallographic direction of <span class="hlt">olivine</span> can be fit by β = 0.4 ± 0</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017M%26PS...52..937L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017M%26PS...52..937L"><span>Petrology, mineralogy, porosity, and cosmic-ray exposure history of Huaxi ordinary chondrite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Shijie; Wang, Shijie; Leya, Ingo; Li, Yang; Li, Xiongyao; Smith, Thomas</p> <p>2017-05-01</p> <p>A meteorite fall was heard and collected on July 13, 2010 at about 18:00 (local time) in the Shibanjing village of the Huaxi district of Guiyang, Guizhou province, China. The total mass of the fall is estimated to be at least 1.6 kg; some fragments are missing. The meteorite consists mainly of <span class="hlt">olivine</span>, low-Ca pyroxene, high-Ca pyroxene, plagioclase, kamacite, taenite, and troilite. Minor phases include chromite and apatite. Various textural types of <span class="hlt">chondrules</span> exist in this meteorite: most <span class="hlt">chondrule</span> textures can be easily defined. The grain sizes of secondary plagioclase in this meteorite range from 2 to 50 μm. The chemical composition of <span class="hlt">olivine</span> and low-Ca pyroxene are uniform; Fa in <span class="hlt">olivine</span> and Fs in low-Ca pyroxene are, respectively, 19.6 ± 0.2 and 17.0 ± 0.3 (mole%). Huaxi has been classified as an H5 ordinary chondrite, with a shock grade S2, and weathering W0. The weak shock features, rare fractures, and the high porosity (17.6%) indicates that Huaxi is a less compacted meteorite. The preatmospheric radius of Huaxi is 11 cm, corresponding to 21 kg. The meteorite experienced a relatively short cosmic-ray exposure of about 1.6 ± 0.1 Ma. The 4He and 40Ar retention ages are older than 4.6 Ga implying that Huaxi did not degas after thermal metamorphism on its parent body.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoRL..43.9611Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoRL..43.9611Z"><span>Sound velocities of <span class="hlt">olivine</span> at high pressures and temperatures and the composition of Earth's upper mantle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Jin S.; Bass, Jay D.</p> <p>2016-09-01</p> <p>We present the elastic properties of San Carlos <span class="hlt">olivine</span> up to P = 12.8(8) GPa and T = 1300(200) K using Brillouin spectroscopy with CO2 laser heating. A comparison of our results with the global seismic model AK135 yields average <span class="hlt">olivine</span> content near 410 km depth of about 37% and 43% in a dry and wet (1.9 wt % H2O) upper mantle, respectively. These <span class="hlt">olivine</span> contents are far less than in the pyrolite model. However, comparisons of our results with regional seismic models lead to very different conclusions. High <span class="hlt">olivine</span> contents of up to 87% are implied by seismic models of the western U.S. and eastern Pacific regions. In contrast, we infer less than 35% <span class="hlt">olivine</span> under the central Pacific. Strong variations of <span class="hlt">olivine</span> content and upper mantle lithologies near the 410 km discontinuity are suggested by regional seismic models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017M%26PS...52.2412D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017M%26PS...52.2412D"><span>Reclassification of Hart and Northwest Africa 6047: Criteria for distinguishing between CV and CK3 chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dunn, Tasha L.; Gross, Juliane</p> <p>2017-11-01</p> <p>The single parent body model for the CV and CK chondrites (Greenwood et al.) was challenged by Dunn et al., who argued that magnetite compositions could not be reconciled by a single metamorphic sequence (i.e., CV3 → CK3 → CK4-6). Cr isotopic compositions, which are distinguishable between the CV and CK chondrites, also support two different parent bodies (Yin et al.). Despite this, there are many petrographic and mineralogical similarities between the unequilibrated (petrologic type 3) CK chondrites and the CV chondrites (also type 3), which may result in misclassification of samples. Hart and Northwest Africa 6047 (NWA 6047) are an excellent example of this. In this study, we revisit the classification of Hart and NWA 6047 using magnetite compositions, petrography, and compositions of <span class="hlt">olivine</span>, the most ubiquitous mineral in both CV and CK chondrites. Not only do our results suggest that NWA 6047 and Hart were misclassified, but our assessment of CV and CK3 chondrites has also led to the development of criteria that can be used to distinguish between CV and CK3 chondrites. These criteria include: abundances of Cr2O3, TiO2, NiO, and Al2O3 in magnetite; Fa content and NiO abundance of matrix <span class="hlt">olivine</span>; FeO content of <span class="hlt">chondrules</span>; and the <span class="hlt">chondrule</span>:matrix ratio. Classification as a CV chondrite is also supported by the presence of igneous <span class="hlt">chondrule</span> rims, calcium-aluminum-rich inclusions, and an elongated petrofabric. However, none of these petrographic characteristics can be used conclusively to distinguish between CV and CK3 chondrites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930040728&hterms=trivalent+chromium&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtrivalent%2Bchromium','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930040728&hterms=trivalent+chromium&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtrivalent%2Bchromium"><span>Reduced chromium in <span class="hlt">olivine</span> grains from lunar basalt 15555 - X-ray Absorption Near Edge Structure (XANES)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sutton, S. R.; Jones, K. W.; Gordon, B.; Rivers, M. L.; Bajt, S.; Smith, J. V.</p> <p>1993-01-01</p> <p>The oxidation state of Cr in 200-micron regions within individual lunar <span class="hlt">olivine</span> and pyroxene grains from lunar basalt 15555 was inferred using X-ray Absorption Near Edge Structure (XANES). Reference materials had previously been studied by optical absorption spectroscopy and included Cr-bearing borosilicate glasses synthesized under controlled oxygen fugacity and Cr-doped <span class="hlt">olivines</span>. The energy dependence of XANES spectral features defined by these reference materials indicated that Cr is predominantly divalent in the lunar <span class="hlt">olivine</span> and trivalent in the pyroxene. These results, coupled with the apparent f(02)-independence of partitioning coefficients for Cr into <span class="hlt">olivine</span>, imply that the source magma was dominated by divalent Cr at the time of <span class="hlt">olivine</span> crystallization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PEPI..260....1D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PEPI..260....1D"><span>Diffusivity of hydrogen in iron-bearing <span class="hlt">olivine</span> at 3 GPa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Demouchy, Sylvie; Thoraval, Catherine; Bolfan-Casanova, Nathalie; Manthilake, Geeth</p> <p>2016-11-01</p> <p>The kinetics of hydrogenation of dry iron-bearing <span class="hlt">olivine</span> single crystals was determined by performing hydration experiments under hydrothermal conditions at high pressure. The experiments were performed in a multi-anvil press at 3 GPa, for a temperature range between 900 and 1200 °C and for various durations. The oxygen fugacity was buffered along Ni-NiO joint. Polarized Fourier transform infrared spectroscopy and recent empirical calibration were used to quantify the hydroxyl distributions in the samples along crystallographic axes after the experiments. The chemical diffusion coefficients are similar (barely slower) than in <span class="hlt">olivine</span> hydrated at lower pressure (0.2 and 0.3 GPa) for the same diffusion mechanism. Under the given experimental conditions, the anisotropy of diffusion is the same as for proton-vacancy mechanism, with diffusion along the [0 0 1] axis faster than along the [1 0 0]. However, the anisotropy at 3 GPa is weaker compared to measurements at lower pressures and the analysis of concentration profiles using 3D models shows that an isotropic solution could also be relevant. Fits of the diffusion data to an Arrhenius law yield activation energies for the slightly faster [0 0 1] axis of the crystallographic axes around 198 ± 5 kJ mol-1, a value only slightly lower than the results from previous experimental studies for natural iron-bearing <span class="hlt">olivine</span> hydrogenated at lower confining pressure. At 3 GPa, hydrogenation can be well approximated by a single mechanism controlled by coupled diffusion of protons and octahedral vacancies (di- and tri-valent ions). The diffusion rates are fast enough to alter hydrogen concentration within <span class="hlt">olivine</span> in xenoliths ascending from the mantle or experiencing hydrogen-rich metasomatism events, but too slow to permit complete homogenization of hydrogen in <span class="hlt">olivine</span>-rich rocks at kilometer scale in less than one My.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017LPICo1963.2009K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017LPICo1963.2009K"><span>Multiple Mechanisms of Transient Heating Events in the Protoplanetary Disk: Evidence from Precursors of <span class="hlt">Chondrules</span> and Igneous Ca,Al-Rich Inclusions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krot, A. N.; Nagashima, K.; Libourel, G.; Miller, K. E.</p> <p>2017-02-01</p> <p>Here we review the mineralogy, petrography, O-isotope compositions, and trace element abundances of precursors of <span class="hlt">chondrules</span> and igneous CAIs which provide important constraints on the mechanisms of transient heating events in the protoplanetary disk.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014E%26PSL.387...67N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014E%26PSL.387...67N"><span>Dehydration breakdown of antigorite and the formation of B-type <span class="hlt">olivine</span> CPO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nagaya, Takayoshi; Wallis, Simon R.; Kobayashi, Hiroaki; Michibayashi, Katsuyoshi; Mizukami, Tomoyuki; Seto, Yusuke; Miyake, Akira; Matsumoto, Megumi</p> <p>2014-02-01</p> <p>Peridotite formed by contact metamorphism and dehydration breakdown of an antigorite schist from the Happo area, central Japan shows a strong <span class="hlt">olivine</span> crystallographic preferred orientation (Ol CPO). The lack of mesoscale deformation structures associated with the intrusion and the lack of microstructural evidence for plastic deformation of neoblastic grains suggest that <span class="hlt">olivine</span> CPO in this area did not form as a result of solid-state deformation. Instead, the good correspondence between the original antigorite orientation and the orientation of the newly formed <span class="hlt">olivine</span> implies the CPO formed by topotactic growth of the <span class="hlt">olivine</span> after antigorite. Ol CPO is likely to develop by a similar process in subduction zone environments where foliated serpentinite is dragged down to depths where antigorite is no longer stable. The Happo Ol CPO has a strong a-axis concentration perpendicular to the lineation and within the foliation-commonly referred to as B-type Ol CPO. Seismic fast directions parallel to the ocean trench are observed in many convergent margins and are consistent with the presence of B-type Ol CPO in the mantle wedge of these regions. Experimental work has shown that B-type CPO can form by dislocation creep under hydrous conditions at relatively high stresses. There are, however, several discrepancies between the characteristics of natural and laboratory samples with B-type Ol CPO. (1) The formation conditions (stress and temperature) of some natural examples with B-type CPO fall outside those predicted by experiments. (2) In deformation experiments, slip in the crystallographic c-axis direction is important but has not been observed in natural examples of B-type CPO. (3) Experimental work suggests the presence of H2O and either high shear stress or relatively low temperatures are essential for the formation of B-type CPO. These conditions are most likely to be achieved close to subduction boundaries, but these regions are also associated with serpentinization</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70014210','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70014210"><span>Relation of the spectroscopic reflectance of <span class="hlt">olivine</span> to mineral chemistry and some remote sensing implications.</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>King, T.V.V.; Ridley, W.I.</p> <p>1987-01-01</p> <p>Using high-resolution visible and near-infrared diffuse spectral reflectance, systematically investigates apparent wavelength shifts as a function of mineral chemistry in the Fe/Mg <span class="hlt">olivine</span> series from Fo11 to Fo91. The study also shows that trace amounts of nickel can be spectrally detected in the <span class="hlt">olivine</span> structure. Significant spectral variation as a function of grain size is also demonstrated, adding a further complication to the interpretation of remotely sensed data from <span class="hlt">olivine</span>-rich surfaces. Some permutations of Fe-Mg-Ni relations in <span class="hlt">olivines</span> are discussed as they apply to the interpretation of asteroid surfaces and other extraterrestrial bodies. -from Authors</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990JGR....95.5079M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990JGR....95.5079M"><span>Diffusion of hydrogen in <span class="hlt">olivine</span>: Implications for water in the mantle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mackwell, Stephen J.; Kohlstedt, David L.</p> <p>1990-04-01</p> <p>To investigate the kinetics of diffusion of hydrogen in <span class="hlt">olivine</span>, single crystals from San Carlos in Arizona have been annealed at temperatures between 800° and 1000°C under hydrothermal conditions at a confining pressure of 300 MPa. The hydrogen diffusivities were determined for the [100], [010], and [001] directions from concentration profiles for hydroxyl in the samples. These profiles were obtained from infrared spectra taken at 100-μm intervals across a thin slice which was cut from the central portion of each annealed crystal. The rate of diffusion is anisotropic, with fastest transport along the [100] axis and slowest along the [010] axis. The fit of the data to an Arrhenius law for diffusion parallel to [100] yields an activation enthalpy of 130±30 kJ/mol with a preexponential term of (6±3)×10-5 m2 s-1. For diffusion parallel to [001], as there are insufficient data to calculate the activation enthalpy for diffusion, we used the same value as that for diffusion parallel to [100] and determined a preexponential term of (5±4)×10-6 m2 s-1. The diffusion rate parallel to [010] is about 1 order of magnitude slower than along [001]. The measured diffusivities are large enough that the hydrogen content of <span class="hlt">olivine</span> grains which are millimeters in diameter will adjust to changing environmental conditions in time scales of hours at temperatures as low as 800°C. As xenoliths ascending from the mantle remain at high temperatures (i.e., >1000°C) but experience a rapid decrease in pressure, and hence hydrogen fugacity, <span class="hlt">olivine</span> grains may dehydrate during ascent. By comparison, slow rates of carbon diffusion (Tingle et al., 1988) suggest that carbon will not be lost from <span class="hlt">olivine</span> during ascent. Thus, low hydrogen contents within <span class="hlt">olivine</span> and within fluid inclusions in <span class="hlt">olivine</span> cannot be taken as support for low water contents in the mantle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810946C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810946C"><span>Development of <span class="hlt">olivine</span> crystallographic preferred orientation in response to strain-induced fabric geometry</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, Jr.; Withers, Anthony C.; Bagley, Brian</p> <p>2016-04-01</p> <p>The effect of finite strain ellipsoid geometry on crystallographic preferred orientation (CPO) is well known for crustal minerals (e.g., quartz, calcite, biotite, and hornblende). In the upper mantle, however, it remains poorly constrained how strain and fabric may affect <span class="hlt">olivine</span> CPO. We present data from a suite of 40 spinel peridotite xenoliths from Marie Byrd Land (west Antarctica), which support an interpretation that fabric geometry rather than deformation conditions control the development of <span class="hlt">olivine</span> CPO. We use X-ray computed tomography (XRCT) to quantitatively determine spinel fabric (orientation and geometry). <span class="hlt">Olivine</span> CPOs, determined by Electron Backscattered Diffraction (EBSD), are plotted with respect to the XRCT-derived spinel foliation and lineation; this approach allows for the accurate, and unbiased, identification of CPO symmetries and types in mantle xenoliths. The combined XRCT and EBSD data show that the xenoliths are characterized by a range of fabric geometries (from oblate to prolate) and <span class="hlt">olivine</span> CPO patterns; we recognize the A-type, axial-[010], axial-[100], and B-type patterns. The mantle xenoliths equilibrated at temperatures 779-1198 oC, as determined by 2-Px geothermometry. Using a geotherm consistent with the stability of spinel in all xenoliths, the range of equilibration temperatures occurs at depths between 39 and 72 km. <span class="hlt">Olivine</span> recrystallized grain size piezometry reveals differential stresses ranging 2-60 MPa. Analysis of low-angle misorientation axes show a wide range in the distribution of rotation axes, with dominant {0kl}[100] slip. We use Fourier Transform Infrared (FTIR) spectroscopy to estimate the water content in the xenolith with the B-type CPO pattern. FTIR analysis shows that the equilibrium H concentration in <span class="hlt">olivine</span> is low (4-13 ppm H2O). Combining these data, we observe that <span class="hlt">olivine</span> CPO symmetry is controlled neither by the deformation conditions (stress, temperature, pressure, water content) for the range of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMMR41A2337B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMMR41A2337B"><span>Comparing <span class="hlt">olivine</span> single crystal and polycrystal rheology: evidence for supplementary accommodation mechanisms at grain boundaries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bollinger, C.; Merkel, S.; Raterron, P.; Castelnau, O.; Detrez, F.</p> <p>2013-12-01</p> <p>Rheology in the Earth's upper-mantle is mostly constrained by the plastic properties of <span class="hlt">olivine</span>. Over recent years, several groups have been carrying out deformation experiments on single crystals and polycrystals of <span class="hlt">olivine</span> at upper mantle pressure (P) and temperature (T). Yet, the rheology of <span class="hlt">olivine</span> at mantle conditions is still not well constrained. We carried out deformation experiments on San Carlos <span class="hlt">olivine</span> polycrystals, at P and T ranging from 3 to 8 GPa and 1373 to 1673 K, respectively, and at strain rates ranging from 10-6 to 10-4 s-1, using the D-DIA apparatus installed at the NSLS X17B2 beamline (NY, USA). The deformation rates of the polycrystals are compared to those of single crystals oriented along the soft orientations [110]c, [011]c, [101]c which activate the easiest slip systems (Raterron et al., 2012). This comparison suggests that, in <span class="hlt">olivine</span> polycrystals deforming in the dislocation creep regime, other relaxation mechanisms need to be considered to account for the observed polycrystal strain rates. This highlights the importance of supplementary mechanisms, such as those occurring at grain boundaries, to properly model <span class="hlt">olivine</span> aggregates plasticity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5382570','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5382570"><span><span class="hlt">Olivine</span> Dissolution in Seawater: Implications for CO2 Sequestration through Enhanced Weathering in Coastal Environments</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>2017-01-01</p> <p>Enhanced weathering of (ultra)basic silicate rocks such as <span class="hlt">olivine</span>-rich dunite has been proposed as a large-scale climate engineering approach. When implemented in coastal environments, <span class="hlt">olivine</span> weathering is expected to increase seawater alkalinity, thus resulting in additional CO2 uptake from the atmosphere. However, the mechanisms of marine <span class="hlt">olivine</span> weathering and its effect on seawater–carbonate chemistry remain poorly understood. Here, we present results from batch reaction experiments, in which forsteritic <span class="hlt">olivine</span> was subjected to rotational agitation in different seawater media for periods of days to months. <span class="hlt">Olivine</span> dissolution caused a significant increase in alkalinity of the seawater with a consequent DIC increase due to CO2 invasion, thus confirming viability of the basic concept of enhanced silicate weathering. However, our experiments also identified several important challenges with respect to the detailed quantification of the CO2 sequestration efficiency under field conditions, which include nonstoichiometric dissolution, potential pore water saturation in the seabed, and the potential occurrence of secondary reactions. Before enhanced weathering of <span class="hlt">olivine</span> in coastal environments can be considered an option for realizing negative CO2 emissions for climate mitigation purposes, these aspects need further experimental assessment. PMID:28281750</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Tectp.722....1L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Tectp.722....1L"><span>B-type <span class="hlt">olivine</span> fabric induced by low temperature dissolution creep during serpentinization and deformation in mantle wedge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Wenlong; Zhang, Junfeng; Barou, Fabrice</p> <p>2018-01-01</p> <p>The B-type <span class="hlt">olivine</span> fabric (i.e., the [010] axes subnormal to foliation and the [001] axes subparallel to the lineation) has been regarded as an important <span class="hlt">olivine</span> fabric for interpreting global trench-parallel S-wave polarization in fore-arc regions. However, strong serpentinization and cold temperature environment in the mantle wedge should inhibit development of the B-type <span class="hlt">olivine</span> fabric that requires high temperature to activate solid-state plastic deformation. Here we report fabrics of <span class="hlt">olivine</span> and antigorite generated at low temperatures (300-370 °C) during serpentinization in a fossil mantle wedge of the Val Malenco area, Central Alps. <span class="hlt">Olivine</span> in the serpentine matrix develops a pronounced B-type fabric, while antigorite in the same matrix displays a strong crystallographic preferred orientation (CPO) with the (001) planes and the [010] axes subparallel to foliation and lineation, respectively. The following evidence leads to the conclusion that the B-type <span class="hlt">olivine</span> fabric results from dissolution creep assisted by grain boundary sliding (GBS) and grain rotation, rather than solid-state plastic deformation: (1) serpentinization took place at low temperatures and a fluid-enriched environment, ideal for dissolution-precipitation creep; (2) the voids and zigzag boundaries along the interface between antigorite and <span class="hlt">olivine</span> suggest a fluid dissolution reaction; (3) the primary coarse <span class="hlt">olivine</span> develops a nearly random fabric, indicating the B-type fabrics in the fine-grained <span class="hlt">olivine</span> may not be inherited fabrics. These results document for the first time the B-type <span class="hlt">olivine</span> CPO formed by dissolution creep at low temperatures during serpentinization and provide a mechanism to reconcile petrofabric observations with geophysical observations of trench parallel fast S-wave seismic anisotropy in fore-arc mantle wedge regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780029863&hterms=Glasses+SiO2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DGlasses%2BSiO2','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19780029863&hterms=Glasses+SiO2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DGlasses%2BSiO2"><span>High-silica glass inclusions in <span class="hlt">olivine</span> of Luna-24 samples</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Roedder, E.; Weiblen, P. W.</p> <p>1977-01-01</p> <p>Optical examination of nine polished grain mounts of Luna-24 drill-core material (0.09-0.50 mm size) revealed melt inclusions in <span class="hlt">olivine</span> crystals. Two inclusions consist of clear glass with exceptionally high Si, yet contain no visible daughter minerals and have had no reaction effects with the <span class="hlt">olivine</span> walls. Their compositions (one has SiO2 93.8, Al2O3 1.51, FeO 2.32, MgO 1.61, CaO 0.06, Na2O less than 0.05, K2O 0.11, total 99.41%; the other is similar) are unique and quite unlike the high-Si high-K melt of granitic composition that is found as inclusions in late-stage minerals of these (and the Apollo) samples, from silicate liquid immiscibility. The host <span class="hlt">olivines</span> are Fo73 and Fo51. The origin of the melt in the inclusions and the lack of reaction effects are perplexing unsolved problems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26PSL.452..133F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26PSL.452..133F"><span>Hidden secrets of deformation: Impact-induced compaction within a CV chondrite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Forman, L. V.; Bland, P. A.; Timms, N. E.; Collins, G. S.; Davison, T. M.; Ciesla, F. J.; Benedix, G. K.; Daly, L.; Trimby, P. W.; Yang, L.; Ringer, S. P.</p> <p>2016-10-01</p> <p>The CV3 Allende is one of the most extensively studied meteorites in worldwide collections. It is currently classified as S1-essentially unshocked-using the classification scheme of Stöffler et al. (1991), however recent modelling suggests the low porosity observed in Allende indicates the body should have undergone compaction-related deformation. In this study, we detail previously undetected evidence of impact through use of Electron Backscatter Diffraction mapping to identify deformation microstructures in <span class="hlt">chondrules</span>, AOAs and matrix grains. Our results demonstrate that forsterite-rich <span class="hlt">chondrules</span> commonly preserve crystal-plastic microstructures (particularly at their margins); that low-angle boundaries in deformed matrix grains of <span class="hlt">olivine</span> have a preferred orientation; and that disparities in deformation occur between <span class="hlt">chondrules</span>, surrounding and non-adjacent matrix grains. We find heterogeneous compaction effects present throughout the matrix, consistent with a highly porous initial material. Given the spatial distribution of these crystal-plastic deformation microstructures, we suggest that this is evidence that Allende has undergone impact-induced compaction from an initially heterogeneous and porous parent body. We suggest that current shock classifications (Stöffler et al., 1991) relying upon data from <span class="hlt">chondrule</span> interiors do not constrain the complete shock history of a sample.</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/2015LPICo1856.5250C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015LPICo1856.5250C"><span>A <span class="hlt">Chondrule</span> from the Mokoia (CV3) Chondrite with Anomalously Low 26Mg*: Evidence for a Multi-Stage History-</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Claydon, J. L.; Elliott, T.; Coath, C. D.; Chen, H. W.; Taylor, C. A.; Russell, S. S.</p> <p>2015-07-01</p> <p>MC-ICP-MS measurements of Mg isotopes in <span class="hlt">chondrule</span> MOK13B reveal that it may have formed from low-Al/Mg material that underwent chemical fractionation to increase Al/Mg after decay of 26-Al, or it may sample a region with anomalous Al or Mg isotopes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.V51B0526N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.V51B0526N"><span>Limitations on the Estimation of Parental Magma Temperature Using <span class="hlt">Olivine</span>-melt Equilibria: Hotspots Not So Hot</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Natland, J. H.</p> <p>2004-12-01</p> <p>Estimates of temperatures of magmas parental to picritic tholeiites using <span class="hlt">olivine</span>-melt equilibria and FeO-MgO relationships depend strongly on the assumption that a liquid composition, usually a glass, is related to the most magnesian <span class="hlt">olivine</span> in the rock, or to an <span class="hlt">olivine</span> composition in equilibrium with mantle peridotite, along an <span class="hlt">olivine</span>-controlled liquid line of descent. The liquid Fe2+/Fe3+ also has to be known; where data exist, average values from wet chemical determinations are used. Crystallization histories of tholeiitic picrites from islands, spreading ridges, and large igneous provinces, however, usually reveal them to be hybrid rocks that are assembled by two types of magma mixing: 1) between a) differentiated magmas that are on <span class="hlt">olivine</span>-plagioclase or <span class="hlt">olivine</span>-plagioclase-clinopyroxene cotectics and b) crystal sludges with abundant <span class="hlt">olivine</span> that may have accumulated from liquids crystallizing <span class="hlt">olivine</span> alone; and 2) between primitive magma strains in which <span class="hlt">olivine</span> crystallized either alone or with other silicate minerals at elevated pressure on separate liquid lines of descent. Many picrites give evidence that both types of mixing have occurred. If either type has occurred, the assumption of <span class="hlt">olivine</span>-control linking a glass and an <span class="hlt">olivine</span> composition can only circumstantially be correct. Oxidation state can also be underestimated and therefore FeO contents overestimated if basalts have degassed S, as at Hawaii. In Case 1, hybrid host glass compositions often have higher FeO at given MgO content than liquids which produced many <span class="hlt">olivine</span> crystals in the rock. In Case 2, the separate parental melt strains are revealed by diversity of compositions of both melt inclusions and Cr-spinel and are most often interpreted to mean local heterogeneity of the mantle source. The inclusions do not always affirm an <span class="hlt">olivine</span>-controlled liquid line of descent. Instead, inclusions with <13% Al2O3 are increasingly interpreted from both major oxides and trace elements to be derived</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V31A2674S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V31A2674S"><span>A Tale of Two <span class="hlt">Olivines</span>: Magma Ascent in the Auckland Volcanic Field, New Zealand</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smid, E. R.; McGee, L. E.; Smith, I. E.; Lindsay, J. M.</p> <p>2013-12-01</p> <p>The Auckland Volcanic Field (AVF) is a nephelinitic to subalkali basaltic monogenetic field centered on the city of Auckland, New Zealand. Lavas are <span class="hlt">olivine</span>-phyric, and the deposits of several volcanoes in the field contain <span class="hlt">olivine</span> crystals with chrome spinel (Cr-spinel) inclusions. Microprobe analyses show at least two populations of <span class="hlt">olivine</span>, categorised by their Mg# and their spinel inclusion compositions: the first has <span class="hlt">olivines</span> that are euhedral, have compositions slightly less forsteritic than expected for whole rock Mg#, and have Cr-spinel inclusions with relatively low Cr2O3 contents of ~20%. These are interpreted as antecrysts inherited from the mantle source that yielded their host magma. The second population is characterised by <span class="hlt">olivines</span> that are sub- to euhedral, are significantly more forsteritic than expected from their host whole rock Mg#, and have Cr-spinel inclusons with relatively high Cr2O3 contents of ~50%. These are interpreted as xenocrysts. The composition of these high Cr2O3 spinels very closely resembles the composition of spinels within <span class="hlt">olivines</span> in dunite sampled from the Dun Mountain Ophiolite on the South Island of New Zealand. The northward extension of the Dun Mountain complex beneath the North Island is defined by the Junction Magnetic Anomaly, marking a crustal terrane boundary that underlies the Auckland Volcanic Field. These data indicate that the magmas that have risen to produce the volcanoes of the Auckland Volcanic Field have carried crystals from an underlying ultramafic crust as well as from their asthenospheric source. Euhedral <span class="hlt">olivine</span> crystals which do not contain Cr-spinel are also present in AVF lavas and these are interpreted as true phenocrysts that crystallised directly from their host magmas. The lack of reaction textures at crystal margins suggests rapid ascent rates. A crustal origin for the xenocrysts not only has large implications for ascent rate modelling of <span class="hlt">olivines</span>, but also for the crustal structure of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMDI13B..07S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMDI13B..07S"><span>The Effect of Trace H2O on the Mechanisms of the <span class="hlt">Olivine</span>-Ringwoodite Transformation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sharp, T. G.; Rieck, K. D.; Hu, J.; Du Frane, W. L.</p> <p>2011-12-01</p> <p>The existence of metastable <span class="hlt">olivine</span> has been inferred as a possible trigger of deep focus earthquakes. Because hydrogen increases <span class="hlt">olivine</span>-ringwoodite transformation rates, the existence of metastable <span class="hlt">olivine</span> in the transition would require the subduction of very dry <span class="hlt">olivine</span>. Our previous work has shown that for San Carlos <span class="hlt">olivine</span> spheres, hydrated in a piston cylinder with 75 ppm H2O and 300 ppm D2O, ringwoodite-rim growth rates are greatly enhanced relative to anhydrous samples (Du Frane2010 and Diedrich et al, 2009). In anhydrous samples, rim-growth rates decrease with time as elastic strain builds up in the system, eventually stopping the reaction. As strain increases, wadsleyite forms, rather than or in addition to ringwoodite. In hydrous samples, hydrogen partitions to the ringwoodite growth rim, hydrolytically weakening it, and preventing the build up of elastic strain energy. Eventually, elastic strain energy may build up in slightly hydrous samples if the hydrogen content of the rim decreases sufficiently. Here we investigate the transformation mechanisms in the same San Carlos <span class="hlt">olivine</span> samples, hydrated to 75 and 300 ppm H2O and D2O and transformed at 18 GPa. A 75-ppm-H2O sample run at 1100°C for 40 minutes shows a complex mixture of reaction textures. Optical microscopy and Raman spectroscopy show that the ringwoodite rims are nearly pure ringwoodite with minor amounts of wadsleyite. Scanning electron microscopy and transmission electron microscopy on a Focused Ion Beam slices of this sample show that the outermost rim is uniform, relatively course grained and defect free ringwoodite. This suggests limited nucleation at the sample-capsule interface and fairly rapid incoherent growth. The inner rim consists of a complex mixture of <span class="hlt">olivine</span> and ringwoodite in which most of the ringwoodite has no crystallographic relationship to the host <span class="hlt">olivine</span> and therefore represents incoherent nucleation and growth. Coherent ringwoodite lamellae are also present in the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19990010760&hterms=cellular+solids&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dcellular%2Bsolids','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19990010760&hterms=cellular+solids&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dcellular%2Bsolids"><span>Cellular Precipitates Of Iron Oxide in <span class="hlt">Olivine</span> in a Stratospheric Interplanetary Dust Particle</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rietmeijer, Frans J. M.</p> <p>1996-01-01</p> <p>The petrology of a massive <span class="hlt">olivine</span>-sulphide interplanetary dust particle shows melting of Fe,Ni-sulphide plus complete loss of sulphur and subsequent quenching to a mixture of iron-oxides and Fe,Ni-metal. Oxidation of the fayalite component in <span class="hlt">olivine</span> produced maghemite discs and cellular intergrowths with <span class="hlt">olivine</span> and rare andradite-rich garnet. Cellular reactions require no long-range solid-state diffusion and are kinetically favourable during pyrometamorphic oxidation. Local melting of the cellular intergrowths resulted in three dimensional symplectic textures. Dynamic pyrometamorphism of this asteroidal particle occurred at approx. 1100 C during atmospheric entry flash (5-15 s) heating.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.475..143H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.475..143H"><span>Discriminating between pyroxenite and peridotite sources for continental flood basalts (CFB) in southern Africa using <span class="hlt">olivine</span> chemistry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Howarth, Geoffrey H.; Harris, Chris</p> <p>2017-10-01</p> <p>Continental Flood Basalts (CFB) result from voluminous outpourings of magma that often precede continental break-up. Notwithstanding the petrogenetic importance of CFBs, the nature of the mantle source for such magmas is contentious, particularly with regard to picrites with Ni-rich <span class="hlt">olivine</span> phenocrysts. Previous studies have suggested that Ni-rich <span class="hlt">olivines</span> associated with plume volcanism in regions of thickened (>90 km) lithosphere are related to either source mineralogy differences (peridotite versus pyroxenite) or change in <span class="hlt">olivine</span>-melt partitioning due to pressure increase. In order to evaluate these two hypotheses, we present trace element data for <span class="hlt">olivines</span> from the Karoo CFB Tuli and Mwenezi picrites and the Etendeka CFB Horingbaai/LTZ-L type picrites, all of which erupted in regions of thickened (>90 km) lithosphere in southern Africa. Karoo picrite <span class="hlt">olivines</span> are Ni-rich, Ca- and Mn-poor, and have low (<1.4) 100*Mn/Fe. These compositions are consistent with a pyroxenitic source. Etendeka Horingbaai/LTZ-L picrite <span class="hlt">olivines</span> do not show Ni-enrichment, but are characterized by high Al and Cr, and high (>1.4) 100*Mn/Fe, which is more consistent with high temperature melting of a dominantly peridotitic source. We also show that the Karoo and Etendeka <span class="hlt">olivines</span> are characterized by distinct Mn/Zn ratios of <13 and >15, respectively. In addition, bulk rock geochemical data compilations and previously reported <span class="hlt">olivine</span> δ18O for Karoo and Etendeka CFBs are discussed in order to further constrain source components based on previously described pyroxenite melt geochemical indices such as MgO-CaO systematics, FeO/MnO, Zn/Fe, and FC3MS (FeO/CaO-3*MgO/SiO2). These geochemical indices suggest a pyroxenite-dominated source for Karoo CFBs as well as for Etendeka ferropicrites whereas a peridotite-dominated source is indicated for Etendeka Horingbaai/LTZ-L type picrites analyzed in this study. Based on our data, Ni-enrichment of <span class="hlt">olivine</span> in plume-related magmas in regions of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRB..121.7137H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRB..121.7137H"><span>Viscous anisotropy of textured <span class="hlt">olivine</span> aggregates: 2. Micromechanical model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, Lars N.; Conrad, Clinton P.; Boneh, Yuval; Skemer, Philip; Warren, Jessica M.; Kohlstedt, David L.</p> <p>2016-10-01</p> <p>The significant viscous anisotropy that results from crystallographic alignment (texture) of <span class="hlt">olivine</span> grains in deformed upper mantle rocks strongly influences a large variety of geodynamic processes. Our ability to explore the effects of anisotropic viscosity in simulations of these processes requires a mechanical model that can predict the magnitude of anisotropy and its evolution. Unfortunately, existing models of <span class="hlt">olivine</span> textural evolution and viscous anisotropy are calibrated for relatively small deformations and simple strain paths, making them less general than desired for many large-scale geodynamic scenarios. Here we develop a new set of micromechanical models to describe the mechanical behavior and textural evolution of <span class="hlt">olivine</span> through a large range of strains and complex strain histories. For the mechanical behavior, we explore two extreme scenarios, one in which each grain experiences the same stress tensor (Sachs model) and one in which each grain undergoes a strain rate as close as possible to the macroscopic strain rate (pseudo-Taylor model). For the textural evolution, we develop a new model in which the director method is used to control the rate of grain rotation and the available slip systems in <span class="hlt">olivine</span> are used to control the axis of rotation. Only recently has enough laboratory data on the deformation of <span class="hlt">olivine</span> become available to calibrate these models. We use these new data to conduct inversions for the best parameters to characterize both the mechanical and textural evolution models. These inversions demonstrate that the calibrated pseudo-Taylor model best reproduces the mechanical observations. Additionally, the pseudo-Taylor textural evolution model can reasonably reproduce the observed texture strength, shape, and orientation after large and complex deformations. A quantitative comparison between our calibrated models and previously published models reveals that our new models excel in predicting the magnitude of viscous anisotropy and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR51A2680C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR51A2680C"><span>Water sensitivity of the seismic properties of polycrystalline <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cline, C. J., II; Jackson, I.; Faul, U.; Berry, A.</p> <p>2016-12-01</p> <p>Fully synthetic solgel-derived Fo90 <span class="hlt">olivine</span> specimens have been fabricated with varying concentrations of hydroxyl, chemically bound as doubly protonated Si vacancies associated with nearby Ti/Mg substitution (the `Ti-clinohumite' defect). The `water' contents of three such specimens hot-pressed within welded Pt capsules are controlled by the amount of added TiO2-dopant and ranged between 176 and 802 ppm Ti/Si, providing concentrations of bound hydrogen ranging between 330 and 1150 ppm H/Si respectively. These sol-gel derived specimens, along with another natural Ti-bearing specimen hot-pressed from powder produced by grinding hand-picked single crystals of San Carlos <span class="hlt">olivine</span>, were then each subsequently wrapped in Pt and interrogated under water-undersaturated conditions via forced torsional oscillation. Testing was conducted at seismic periods of 1 - 1000 s and 200 MPa confining pressure during slow staged cooling from 1200 to 25 °C. All Ti-doped hydrous specimens tested, including the San Carlos <span class="hlt">olivine</span> specimen, show high temperature background behavior, involving monotonically increasing levels of dissipation and decreasing values of shear modulus with increasing oscillation period and increasing temperature. Comparison of the mechanical behavior observed in these water-undersaturated specimens to that for a similarly fabricated dry Ti-bearing <span class="hlt">olivine</span> specimen shows a striking contrast, with much more dissipation and lower modulus observed in the hydrous specimens, but with limited sensitivity of seismic properties to the total water content among the hydrous specimens in the series. Further experiments in progress on Pt-sleeved, dry, undoped Fo90 are designed to clarify further the sensitivity of the seismic properties to water content and possibly oxygen fugacity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5597306','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5597306"><span>Size effects resolve discrepancies in 40 years of work on low-temperature plasticity in <span class="hlt">olivine</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>Kumamoto, Kathryn M.; Thom, Christopher A.; Wallis, David; Hansen, Lars N.; Armstrong, David E. J.; Warren, Jessica M.; Goldsby, David L.; Wilkinson, Angus J.</p> <p>2017-01-01</p> <p>The strength of <span class="hlt">olivine</span> at low temperatures and high stresses in Earth’s lithospheric mantle exerts a critical control on many geodynamic processes, including lithospheric flexure and the formation of plate boundaries. Unfortunately, laboratory-derived values of the strength of <span class="hlt">olivine</span> at lithospheric conditions are highly variable and significantly disagree with those inferred from geophysical observations. We demonstrate via nanoindentation that the strength of <span class="hlt">olivine</span> depends on the length scale of deformation, with experiments on smaller volumes of material exhibiting larger yield stresses. This “size effect” resolves discrepancies among previous measurements of <span class="hlt">olivine</span> strength using other techniques. It also corroborates the most recent flow law for <span class="hlt">olivine</span>, which proposes a much weaker lithospheric mantle than previously estimated, thus bringing experimental measurements into closer alignment with geophysical constraints. Further implications include an increased difficulty of activating plasticity in cold, fine-grained shear zones and an impact on the evolution of fault surface roughness due to the size-dependent deformation of nanometer- to micrometer-sized asperities. PMID:28924611</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030110932&hterms=smectite&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsmectite','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030110932&hterms=smectite&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsmectite"><span>A Study of <span class="hlt">Olivine</span> Alteration to Iddingsite Using Raman Spectroscopy</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kuebler, K. E.; Wang, Alian; Haskin, L. A.; Jolliff, B. L.</p> <p>2003-01-01</p> <p>A crucial task of Mars surface science is to determine past environmental conditions, especially aqueous environments and their nature. Identification of mineral alteration by water is one way to do this. Recent work interprets TES spectra as indicating altered basalt on Mars. <span class="hlt">Olivine</span>, a primary basaltic mineral, is easily altered by aqueous solutions. Alteration assemblages of <span class="hlt">olivine</span> may be specific to deuteric, hydrothermal, surface water, or metamorphic environments. Raman spectra are produced by molecular vibrations and provide direct means for studying and identifying alteration products. Here, we present a combined study of changes in the chemical composition and Raman spectra of an <span class="hlt">olivine</span> as it alters to iddingsite. Iddingsite is found in some SNC meteorites and is presumably present on Mars. The term 'iddingsite' has been used as a catch-all term to describe reddish alteration products of <span class="hlt">olivine</span>, although some authors ascribe a narrower definition: an angstrom-scale intergrowth of goethite and smectite (presumably saponite) formed in an oxidizing and fluid-rich environment. Alteration conserves Fe (albeit oxidized) but requires addition of Al and H2O and removal of Mg and Si. The smectite that forms may be removed by continued alteration. Dehydration of the goethite forms hematite. Our purpose is to study the mineral assemblage, determine the structural and chemical variability of the components with respect to the degree of alteration, and to find spectral indicators of alteration that will be useful during in-situ analyses on Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760023652','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760023652"><span>Pyroxenes and <span class="hlt">olivines</span>: Structural implications of shock-wave data for high pressure phases</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jeanloz, R.; Ahrens, T. J.</p> <p>1975-01-01</p> <p>The nature of the shock-induced, high-pressure phases of <span class="hlt">olivine</span> and pyroxene rocks is examined in the light of data for the densities of a new class of perovskite-related silicate structures. Also examined are some new Hugoniot and release adiabat data for bronzite. Reexamining available shock data for magnesian pyroxenes and <span class="hlt">olivines</span> leads to the conclusion that they define a mixed phase (or disequilibrium) region to about the 100 GPa range, related to the kinetics of phase transformation in these silicates. By recognizing this point, certain discrepancies in previous interpretations of shock data can be explained. A set of theoretical Hugonoits for pyroxene and <span class="hlt">olivine</span> stoichiometry, perovskite-bearing assemblages was constructed based on their properties deduced from high-pressure work, showing that the shock data is compatible with transformations to perovskites in the 45-7GPa region. Finally, the shock data indicate very similar properties for <span class="hlt">olivine</span> and pyroxene at high pressures making them both equally likely candidates for the lower mantle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013GeCoA.122..280G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013GeCoA.122..280G"><span>Chromium valences in ureilite <span class="hlt">olivine</span> and implications for ureilite petrogenesis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goodrich, C. A.; Sutton, S. R.; Wirick, S.; Jercinovic, M. J.</p> <p>2013-12-01</p> <p>Ureilites are a group of ultramafic achondrites commonly thought to be residues of partial melting on a carbon-rich asteroid. They show a large variation in FeO content (<span class="hlt">olivine</span> Fo values ranging from ∼74 to 95) that cannot be due to igneous fractionation and suggests instead variation in oxidation state. The presence of chromite in only a few of the most ferroan (Fo 75-76) samples appears to support such a model. MicroXANES analyses were used in this study to determine the valence states of Cr (previously unknown) in <span class="hlt">olivine</span> cores of 11 main group ureilites. The goal of this work was to use a method that is independent of Fo to determine the oxidation conditions under which ureilites formed, in order to evaluate whether the ureilite FeO-variation is correlated with oxidation state, and whether it is nebular or planetary in origin. Two of the analyzed samples, LEW 88774 (Fo 74.2) and NWA 766 (Fo 76.7) contain primary chromite; two others, LAP 03587 (Fo 74.4) and CMS 04048 (Fo 76.2) contain sub-micrometer-sized exsolutions of chromite + Ca-rich pyroxene in <span class="hlt">olivine</span>; and one, EET 96328 (Fo 85.2) contains an unusual chromite grain of uncertain origin. No chromite has been observed in the remaining six samples (Fo 77.4-92.3). Chromium in <span class="hlt">olivine</span> in all eleven samples was found to be dominated by the divalent species, with valences ranging from 2.10 ± 0.02 (1σ) to 2.46 ± 0.04. The non-chromite-bearing ureilites have the most reduced Cr, with a weighted mean valence of 2.12 ± 0.01, i.e., Cr2+/Cr3+ = 7.33. All low-Fo chromite-bearing ureilites have more oxidized Cr, with valences ranging from 2.22 ± 0.03 to 2.46 ± 0.04. EET 96328, whose chromite grain we interpret as a late-crystallizing phase, yielded a reduced Cr valence of 2.15 ± 0.07, similar to the non-chromite-bearing samples. Based on the measured Cr valences, magmatic (1200-1300 °C) oxygen fugacities (fO2) of the non-chromite-bearing samples were estimated to be in the range IW-1.9 to IW-2.8 (assuming</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940016334&hterms=chromium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dchromium','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940016334&hterms=chromium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dchromium"><span>The x ray microprobe determination of chromium oxidation state in <span class="hlt">olivine</span> from lunar basalt and kimberlitic diamonds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sutton, S. R.; Bajt, S.; Rivers, M. L.; Smith, J. V.</p> <p>1993-01-01</p> <p>The synchrotron x-ray microprobe is being used to obtain oxidation state information on planetary materials with high spatial resolution. Initial results on chromium in <span class="hlt">olivine</span> from various sources including laboratory experiments, lunar basalt, and kimberlitic diamonds are reported. The lunar <span class="hlt">olivine</span> was dominated by Cr(2+) whereas the diamond inclusions had Cr(2+/Cr(3+) ratios up to about 0.3. The simpliest interpretation is that the terrestrial <span class="hlt">olivine</span> crystallized in a more oxidizing environment than the lunar <span class="hlt">olivine</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70011459','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70011459"><span>Origin of biotite-hornblende-garnet coronas between oxides and plagioclase in <span class="hlt">olivine</span> metagabbros, Adirondack region, New York</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Whitney, P.R.; McLelland, J.M.</p> <p>1982-01-01</p> <p>Complex multivariant reactions involving Fe-Ti oxide minerals, plagioclase and <span class="hlt">olivine</span> have produced coronas of biotite, hornblende and garnet between ilmenite and plagioclase in Adirondack <span class="hlt">olivine</span> metagabbros. Both the biotite (6-10% TiO2) and the hornblende (3-6% TiO2) are exceptionally Titanium-rich. The garnet is nearly identical in composition to the garnet in coronas around <span class="hlt">olivine</span> in the same rocks. The coronas form in two stages: (a) Plagioclase+Fe-Ti Oxides+<span class="hlt">Olivine</span>+water =Hornblende+Spinel+Orthopyroxene??Biotite +more-sodic Plagioclase (b) Hornblende+Orthopyroxene??Spinel+Plagioclase =Garnet+Clinopyroxene+more-sodic Plagioclase The Orthopyroxene and part of the clinopyroxene form adjacent to <span class="hlt">olivine</span>. Both reactions are linked by exchange of Mg2+ and Fe2+ with the reactions forming pyroxene and garnet coronas around <span class="hlt">olivine</span> in the same rocks. The reactions occur under granulite fades metamorphic conditions, either during isobaric cooling or with increasing pressure at high temperature. ?? 1983 Springer-Verlag.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EM%26P..109...43Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EM%26P..109...43Z"><span>Varre-Sai: The Recent Brazilian Fall</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zucolotto, M. E.; Antonello, L. L.; Varela, M. E.; Scorzelli, R. B.; Munayco, P.; dos Santos, E.; Ludka, Isabel P.</p> <p>2012-12-01</p> <p>Varre-Sai, the most recent Brazilian meteorite fall, on June 19th, 2010 at Varre-Sai, in Rio de Janeiro State, Brazil (20°51'41″S; 41°44'.80″W). At least eight masses (total ~3.5 kg) were recovered. Most are totally covered by fusion crust. The exposed interior is of light-grey colour with a few dark shock veins. Five thin polished and etched sections were prepared from a slice weighing 35 g on deposit at the National Museum/UFRJ. It consists mostly of <span class="hlt">chondrules</span> ranging in size from 0.35 to ~2.2 mm, and <span class="hlt">chondrule</span> fragments enclosed in a crystalline matrix. The matrix consists of tiny isolated subhedral and anhedral crystals and opaque minerals that are intergrown with broken <span class="hlt">chondrules</span>. The chondritic texture is poorly defined with <span class="hlt">chondrule</span> textures that vary from non-porphyritic to porphyritic ones. The essential minerals are <span class="hlt">olivine</span> (Fa25±0.2) and low-Ca pyroxene (Fa21.66±0.2Wo1.4). Accessory minerals are plagioclase, apatite, Fe-Ni metal phases, troilite, chromite and magnetite. Mössbauer spectroscopy analysis confirms that the mineral phases are <span class="hlt">olivine</span>, pyroxene, troilite and kamacite/taenite. Chemical data indicate that Varre-Sai is a member of the low iron L chondrite group. The observed texture and mineral phases led us to classify Varre-Sai as an equilibrated petrologic type 5. The shock features of the minerals (undulatory extinction, planar structure and numerous cracks), as well as plagioclase partial or totally transformed to maskelynite, suggest a shock stage S4. Also, some post-impact metamorphic processes could be inferred from the meta-sulfide conjoint grains that show complex mixtures of kamacite-taenite-tetrataenite and troilite. The occurrence of veins crosscutting the studied sections indicates that Varre-Sai was affected by a late fracturing event. Sealing of these fractures must have been a fast process, as shown by troilite globule textures pointing towards rapid solidification. The meteorite name was approved by the Nomenclature</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70012593','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70012593"><span>Dislocation substructure of mantle-derived <span class="hlt">olivine</span> as revealed by selective chemical etching and transmission electron microscopy</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Kirby, S.H.; Wegner, M.W.</p> <p>1978-01-01</p> <p>Cleaved and mechanically polished surfaces of <span class="hlt">olivine</span> from peridotite xenoliths from San Carlos, Arizona, were chemically etched using the techniques of Wegner and Christie (1974). Dislocation etch pits are produced on all surface orientations and they tend to be preferentially aligned along the traces of subgrain boundaries, which are approximately parallel to (100), (010), and (001). Shallow channels were also produced on (010) surfaces and represent dislocations near the surface that are etched out along their lengths. The dislocation etch channel loops are often concentric, and emanate from (100) subgrain boundaries, which suggests that dislocation sources are in the boundaries. Data on subgrain misorientation and dislocation line orientation and arguments based on subgrain boundary energy minimization are used to characterize the dislocation structures of the subgrain boundaries. (010) subgrain boundaries are of the twist type, composed of networks of [100] and [001] screw dislocations. Both (100) and (001) subgrain boundaries are tilt walls composed of arrays of edge dislocation with Burgers vectors b=[100] and [001], respectively. The inferred slip systems are {001} ???100???, {100} ???001???, and {010} ???100??? in order of diminishing importance. Exploratory transmission electron microscopy is in accord with these identifications. The flow stresses associated with the development of the subgrain structure are estimated from the densities of free dislocations and from the subgrain dimensions. Inferred stresses range from 35 to 75 <span class="hlt">bars</span> using the free dislocation densities and 20 to 100 <span class="hlt">bars</span> using the subgrain sizes. ?? 1978 Springer-Verlag.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20180002142','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20180002142"><span>Aqueous Alteration and Shock Metamorphism of Antarctic CR Chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Komatsu, M.; Fagan, T. J.; Yamaguchi, A.; Mikouchi, T.; Yasutake, M.; Zolensky, M. E.</p> <p>2018-01-01</p> <p>CR chondrites are the group of carbonaceous chondrites that best preserve records of formation of their components in the solar nebula. Although they are affected by aqueous alteration, many <span class="hlt">chondrules</span> and CAIs are well-preserved, suggesting they have experienced little thermal metamorphism. We have been investigating the petrologic variations among the CR chondrites in the NIPR Antarctic meteorite collection. We focused particular attention on the petrology of amoeboid <span class="hlt">olivine</span> aggregates (AOAs) in order to understand secondary alteration on the CR chondrite parent body. AOAs are composed of fine-grained forsteritic <span class="hlt">olivine</span> and refractory minerals formed by condensation in the solar nebula, and can be used as sensitive indicators of secondary alteration processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.V42B..07L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.V42B..07L"><span>Recycled Crust in the Mantle: Is High-Ni <span class="hlt">Olivine</span> the Smoking Gun or a Red Herring?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, C.; Ripley, E. M.</p> <p>2008-12-01</p> <p>It is widely accepted that small amounts of recycled crustal components are present in some mantle-derived mafic and ultramafic magmas. This concept is supported by many isotopic and trace element studies of basalts, picrites and komatiites in the last 30 years. Recently Sobolev et al. [1,2] used <span class="hlt">olivine</span> compositions such as Ni content and Mn/Fe ratio to demonstrate that the amounts of the recycled crustal component (i.e. pyroxenite) in these mantle-derived melts are much larger than previously appreciated. Their calculations show that the pyroxenite-derived component varies mostly between 40 and 80% for Hawaiian shield basalts and Siberian flood basalts, and mostly between 10 and 40% for mid-ocean ridge basalts and Archean komatiities. However, a critical test using <span class="hlt">olivine</span>-liquid Mg-Fe equilibrium that was overlooked by Sobolev et al. [1,2] reveals that mixing of the two end-members (pyroxenite-derived and peridotite-derived melts) that were used in their models cannot generate the parental melts for the above natural samples. Such a discrepancy prompts us to reexamine the conventional view of a peridotite-dominant source for the Hawaiian shield basalts. This hypothesis has been criticized recently by many people because the contents of Ni in <span class="hlt">olivine</span> phenocrysts in the basalts are significantly higher than mantle <span class="hlt">olivines</span> in associated peridotite xenoliths and because total pressure has little effect on <span class="hlt">olivine</span>-liquid Ni partition coefficient (DNi). What has not been generally considered is that the depth of <span class="hlt">olivine</span> crystallization/equilibration has a negative effect on <span class="hlt">olivine</span> Ni content because DNi is negatively correlated with melt temperature which decreases during adiabatic ascent. To evaluate such an effect quantitatively we have used all available experimental results of Ni partitioning between <span class="hlt">olivine</span> and liquid to construct a robust empirical equation for DNi based on melt composition and temperature. The results of our calculations indicate that the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.V11C..06S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.V11C..06S"><span>Potential Temperatures of Sources of MORB, OIB and LIPs Based on AL Partitioning Between <span class="hlt">Olivine</span> and Spinel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sobolev, A. V.; Batanova, V. G.; Krasheninnikov, S.; Borisov, A.; Arndt, N.; Kuzmin, D.; Krivolutskaya, N.; Sushevskaya, N.</p> <p>2013-12-01</p> <p>Knowledge of potential temperatures of convecting mantle is required for the understanding the global processes on the Earth [1]. The common way to estimate these is the reconstruction of primary melt compositions and liquidus temperatures based on the Fe-Mg partitioning between <span class="hlt">olivine</span> and melt. This approach requires knowledge of the compositions of primitive melts in equilibrium with <span class="hlt">olivine</span> alone as well as composition of <span class="hlt">olivine</span> equilibrium with primary melts. This information is in most cases unavailable or of questionable quality. Here we report a new approach to obtain crystallization temperatures of primary melts based on the <span class="hlt">olivine</span>-spinel Al-Cr geothermometer [2]. The advantages of this approach are: (1) low rate of diffusion of Al in the <span class="hlt">olivine</span>, which promises to preserve high magmatic temperatures and (2) common presence of spinel in assemblage with high-Mg <span class="hlt">olivine</span>. In order to decipher influence of elevated Ti concentrations in spinel we have run several experiments at high temperatures (1400-1200 degree C), atmospheric pressure and controled oxygen fugacity. We also analysed over two thousand spinel inclusions and high-Mg host <span class="hlt">olivines</span> from different MORB, OIB, LIP and Archean komatiites on the JXA-8230 EPMA at ISTerre, Grenoble, France. Concentrations of Al, Ti, Na, P, Zn, Cr, Mn, Ca, Co, Ni were determined with a precision of 10 ppm (2 standard errors) using a newly developed protocol [3]. When available, we also analysed matrix glass and glass inclusions in <span class="hlt">olivine</span> and found that temperature estimations from <span class="hlt">olivine</span>-spinel (Al-Cr) and <span class="hlt">olivine</span>-melt (Fe-Mg) [4] equilibrium match within (+/-30 degree C). The results show contrasting crystallization temperatures of Mg-rich <span class="hlt">olivine</span> of the same Fo content from different types of mantle-derived magmas, from the lowest (down to 1220 degree C) for MORB to the highest (up to 1550 degree C) for komatiites and Siberian meimechites. These results match predictions from Fe-Mg <span class="hlt">olivine</span>-melt equilibrium and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI51A0290M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI51A0290M"><span>The effects of pressure, temperature and composition on <span class="hlt">olivine</span>-liquid exchange coefficients</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matzen, A. K.; Wood, B. J.</p> <p>2017-12-01</p> <p>It has recently been observed that there is a correlation between trace element (Ni and Mn) concentrations in <span class="hlt">olivine</span> (ol) phenocrysts and thickness of the lithosphere on which they were erupted [1]. There are a number of potential explanations for this observation: the mantle may have interacted with the Ni-rich core; the trace element concentrations reflect presence of recycled crust in the mantle; or it arises from melting of peridotite at different temperatures (T) and pressures (P). Discriminating between these hypotheses requires accurate models of <span class="hlt">olivine</span>-silicate liquid (liq) partitioning. The three variables that control the observed variations in experimentally-derived ol-liq partition coefficients are T, P, and the composition of the silicate liquid (and to a lesser extent the <span class="hlt">olivine</span> composition). However, experiments cannot unambiguously disentangle the effects of these variables. For <span class="hlt">olivine</span>-saturated liquids at constant P, any change in T results in the crystallization or dissolution of <span class="hlt">olivine</span> and thus a change in liquid composition, resulting in a correlation between T and silicate liquid composition (note that changing the bulk composition such that <span class="hlt">olivine</span> saturation occurs at a different T also results in a correlation with composition and T). Alternatively, P and T can be varied in concert such that liquid and <span class="hlt">olivine</span> compositions remain approximately constant [e.g., 2], resulting in a correlation between T and P. In an attempt to resolve the conflation of T, P and compositional effects we turned to metal (met)-liq partitioning studies. Experiments show that, unlike most other elements, P has a strong effect on the partitioning of Ni between Fe-rich metal and silicate melt. Assuming that the pressure dependence of K_{D, Ni-Fe}^{met-liq} (0-25 GPa) [3] is driven primarily by the changing activities in the silicate melt, we can approximate the effect that pressure will have on K_{D, Ni-Fe}^{ol-liq} as measured by [2], using Kress and Carmichael</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://adsabs.harvard.edu/abs/2009AGUFM.V21A1965H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.V21A1965H"><span>Amphibole-bearing multiphase solid inclusions in <span class="hlt">olivine</span>, the Murotomisaki Gabbro, Southwest Japan: An evidence of hydrous flux melting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hoshide, T.; Obata, M.</p> <p>2009-12-01</p> <p>The Murotomisaki Gabbro is a sill-like layered intrusion of up to 220m thickness exposed near Cape Muroto, Southwest Japan. Despite the small size of the intrusion, it contains well-developed centimeter- to meter-scale layered structures of modal variation of <span class="hlt">olivine</span>, plagioclase and augite. Hoshide et al (2006a, b) identified the ’crystal accumulation zone’ (40m from the bottom) that was formed by gravitational settling of <span class="hlt">olivine</span> crystals and the ’crystal growth zone’ (40-100m from the bottom), in which <span class="hlt">olivine</span> crystals grew significantly. The fine-scale compositional layering is best developed in the ’crystal growth zone’. Amphibole-bearing multiphase solid inclusions (called ‘the amphibole-clot inclusions’) are common in <span class="hlt">olivine</span> crystals from both the crystal accumulation- and the crystal growth zones. The amphibole clot inclusions show spherical or convex-polygonal shapes and are composed of pargasitic amphibole, biotite and orthopyroxene, with minor amounts of augite, apatite and opaque minerals. Plagioclase rarely occurs in the amphibole clot inclusions. Bulk chemical compositions of the inclusions, obtained from mineral microprobe analyses and modal composition, are characteristically high in MgO content (16-23 wt %) and they roughly lie between presumable fractionated melt compositions and <span class="hlt">olivine</span> compositions. From observations above, it is likely that amphibole clot inclusions are of melt origin, which had formed from some hydrous melts probably entrapped in growing <span class="hlt">olivine</span> crystals. However, it may be difficult to explain both the very magnesian nature of the inclusion and absence of plagioclase in the inclusion by the crystallization of the normal hydrous basaltic melt. The difficulty may be resolved if we suppose, for a trapped melt composition, a more magnesian (i.e., picritic) composition. The highly magnesian nature of the amphibole clot inclusions may suggest that significant amount of <span class="hlt">olivine</span> component had been added to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFM.V62A1386L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFM.V62A1386L"><span>Rocks Whose Compositions are Determined by Flow Differentiation of <span class="hlt">Olivine</span>- and Sulfide Droplet-Laden Magma: the Jinchuan Story</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, C.; Ripley, E. M.; de Waal, S. A.; Xu, Z.</p> <p>2002-12-01</p> <p>The Jinchuan intrusion in western China is an elongated, deeply-dipping dyke-like body of dominantly <span class="hlt">olivine</span>-rich ultramafic rocks of high magnesium basaltic magma. It hosts the second largest Ni-Cu sulfide deposit in the world. More than 500 million tones of sulfide ore grading 1.2 percent Ni and 0.7 percent Cu occur mostly as next-textured and disseminated sulfide (pyrrhotite, pentlendite and chalcopyrite) with cumulus <span class="hlt">olivine</span> in about half of the rocks of the intrusion. Based on different petrological zonations, the Jinchuan intrusion is further divided into three segments: eastern, central and western segments. The central segment is characterized by concentric enrichments of cumulus <span class="hlt">olivine</span> and sulfide, whereas the eastern and western segments are characterized by the increase of both cumulus <span class="hlt">olivine</span> and sulfide toward the footwall. The forsterite contents of fresh <span class="hlt">olivine</span> from different segments are similar and vary between 82 and 86 mole percent. The small range of <span class="hlt">olivine</span> compositional variation corresponds to less than 6 percent of fractional crystallization. Mass balance calculations based on sulfide solubility in basaltic magma indicate that the volume of the parental magma of the sulfide is many times larger than that which is currently represented in the intrusion. Large amounts of cumulus <span class="hlt">olivine</span> (more than 40 weight percent) in the marginal samples and high concentrations of sulfide in the intrusion are consistent with an interpretation that the Jinchuan intrusion was formed by <span class="hlt">olivine</span>- and sulfide droplet-laden magma ascending through a subvertical conduit to a higher level. Differentiation processes of the <span class="hlt">olivine</span>- and sulfide droplet-laden magma varied in different parts of the conduit. Sub-vertical flow differentiation controlled the central segment of the conduit, resulting in further enrichment of <span class="hlt">olivine</span> crystals and sulfide droplets in the conduit center. In contrast, sub-lateral flow and gravitational differentiation dominated in the eastern</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..204a2008M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..204a2008M"><span>Production and Application of <span class="hlt">Olivine</span> Nano-Silica in Concrete</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mardiana, Oesman; Haryadi</p> <p>2017-05-01</p> <p>The aim of this research was to produce nano silica by synthesis of nano silica through extraction and dissolution of ground <span class="hlt">olivine</span> rock, and applied the nano silica in the design concrete mix. The producing process of amorphous silica used sulfuric acid as the dissolution reagent. The separation of ground <span class="hlt">olivine</span> rock occurred when the rock was heated in a batch reactor containing sulfuric acid. The results showed that the optimum mole ratio of <span class="hlt">olivine</span>- acid was 1: 8 wherein the weight ratio of the highest nano silica generated. The heating temperature and acid concentration influenced the mass of silica produced, that was at temperature of 90 °C and 3 M acid giving the highest yield of 44.90%. Characterization using Fourier Transform Infrared (FTIR ) concluded that amorphous silica at a wavenumber of 1089 cm-1 indicated the presence of siloxane, Si-O-Si, stretching bond. Characterization using Scanning Electron Microscope - Energy Dispersive Spectroscopy (SEM-EDS) showed the surface and the size of the silica particles. The average size of silica particles was between 1-10 μm due to the rapid aggregation of the growing particles of nano silica into microparticles, caused of the pH control was not fully achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.1562J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.1562J"><span>Biosygnatures on <span class="hlt">olivines</span> in search of past life 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>Jakus, Natalia; Manecki, Maciej; Faehnrich, Karol; Młynarska, Maria; Słupski, Paweł</p> <p>2017-04-01</p> <p>Biosignatures indicate past and present activity of living organisms. Only inorganic biosignatures, e.g. results of interactions between the minerals and the microorganisms in Martian soils could resist harsh environmental conditions on Mars. However, it may be difficult to distinguish the traces of the organism activities from the effects of "natural" chemical and physical processes. In this study, an acidiophilic, chemoautotrophic, iron-oxidizing bacteria Acidithiobacillus ferrooxidans were incubated with magnesium-iron silicate (<span class="hlt">olivine</span>) crystals to identify the potential development of biogenic textures on the surface. The Mg-rich <span class="hlt">olivines</span> were separated from the gabbro rock (Trodos, Cyprus). The isometric crystals were up to 2 mm in size. All the grains were cleaned in ultrasonic bath and fixed on the epoxy stubs. This enabled the observation of the very same surfaces before and after the experiments allowing inspection of natural etch pits and weathering patterns present before inoculation as well as the forms resulting from the experiments. The stubs with the <span class="hlt">olivines</span> were sterilized with ethanol prior to the experiments. Bacteria were isolated from old pyrite mine in Klucze near Olkusz (Southern Poland). A liquid media K9 was used through the experiments (Silverman and Ludgren, 1959). The experiments were run in triplicates. <span class="hlt">Olivine</span> grains were placed in the inoculated medium and incubated for 7 days at 28 C. An abiotic experiment was run as control. Additionally, the experiments in modified (iron deficient) medium were designed to stimulate potential active scavenging for Fe by bacteria-mediated dissolution. In the Fe-deficient medium, the negligible amount of iron was present only to initiate the bacteria growth: the only source of Fe was the <span class="hlt">olivine</span> grain throughout the experiment. After 7 days of incubation the <span class="hlt">olivine</span> grains were removed and air-dried. The alterations of the crystals by both, purely inorganic and biologically mediated dissolution were</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160003501','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160003501"><span>Constraints on Mantle Plume Melting Conditions in the Martian Mantle Based on Improved Melting Phase Relationships of <span class="hlt">Olivine</span>-Phyric Shergottite Yamato 980459</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.; Rapp, Jennifer F.; Usui, Tomohiro; Draper, David S.; Filiberto, Justin</p> <p>2016-01-01</p> <p>Martian meteorite Yamato 980459 (hereafter Y98) is an <span class="hlt">olivine</span>-phyric shergottite that has been interpreted as closely approximating a martian mantle melt [1-4], making it an important constraint on adiabatic decompression melting models. It has long been recognized that low pressure melting of the Y98 composition occurs at extremely high temperatures relative to martian basalts (1430 degC at 1 <span class="hlt">bar</span>), which caused great difficulties in a previous attempt to explain Y98 magma generation via a mantle plume model [2]. However, previous studies of the phase diagram were limited to pressures of 2 GPa and less [2, 5], whereas decompression melting in the present-day martian mantle occurs at pressures of 3-7 GPa, with the shallow boundary of the melt production zone occurring just below the base of the thermal lithosphere [6]. Recent experimental work has now extended our knowledge of the Y98 melting phase relationships to 8 GPa. In light of this improved petrological knowledge, we are therefore reassessing the constraints that Y98 imposes on melting conditions in martian mantle plumes. Two recently discovered <span class="hlt">olivine</span>- phyric shergottites, Northwest Africa (NWA) 5789 and NWA 6234, may also be primary melts from the martian mantle [7, 8]. However, these latter meteorites have not been the subject of detailed experimental petrology studies, so we focus here on Y98.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001A%26A...368L..38D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001A%26A...368L..38D"><span>Structural and chemical alteration of crystalline <span class="hlt">olivine</span> under low energy He+ irradiation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Demyk, K.; Carrez, Ph.; Leroux, H.; Cordier, P.; Jones, A. P.; Borg, J.; Quirico, E.; Raynal, P. I.; d'Hendecourt, L.</p> <p>2001-03-01</p> <p>We present the results of irradiation experiments on crystalline <span class="hlt">olivine</span> with He+ ions at energies of 4 and 10 keV and fluences varying from 5 1016 to 1018 ions/cm2. The aim of these experiments is to simulate ion implantation into interstellar grains in shocks in the ISM. Irradiated samples were analysed by transmission electron microscopy (TEM). The irradiation causes the amorphization of the <span class="hlt">olivine</span>, at all He+ fluences considered. The thickness of the amorphized region is 40 +/- 15 nm and 90 +/- 10 nm for the 4 keV and 10 keV experiments, respectively. The amorphization of the <span class="hlt">olivine</span> occurs in conjunction with an increase in the porosity of the material due to the formation of bubbles. In addition, the amorphized layer is deficient in oxygen and magnesium. We find that the O/Si and Mg/Si ratios decrease as the He+ fluence increases. These experiments show that the irradiation of dust in supernova shocks can efficiently alter the dust structure and composition. Our result are consistent with the lack of crystalline silicates in the interstellar medium and also with the compositional evolution observed from <span class="hlt">olivine</span>-type silicates around evolved stars to pyroxene-type silicates around protostars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeCoA.221..379H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeCoA.221..379H"><span>Presolar silicates in the matrix and fine-grained rims around <span class="hlt">chondrules</span> in primitive CO3.0 chondrites: Evidence for pre-accretionary aqueous alteration of the rims in the solar nebula</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haenecour, Pierre; Floss, Christine; Zega, Thomas J.; Croat, Thomas K.; Wang, Alian; Jolliff, Bradley L.; Carpenter, Paul</p> <p>2018-01-01</p> <p>To investigate the origin of fine-grained rims around <span class="hlt">chondrules</span> (FGRs), we compared presolar grain abundances, elemental compositions and mineralogies in fine-grained interstitial matrix material and individual FGRs in the primitive CO3.0 chondrites Allan Hills A77307, LaPaz Icefield 031117 and Dominion Range 08006. The observation of similar overall O-anomalous (∼155 ppm) and C-anomalous grain abundances (∼40 ppm) in all three CO3.0 chondrites suggests that they all accreted from a nebular reservoir with similar presolar grain abundances. The presence of presolar silicate grains in FGRs combined with the observation of similar estimated porosity between interstitial matrix regions and FGRs in LAP 031117 and ALHA77307, as well as the identification of a composite FGR (a small rimmed <span class="hlt">chondrule</span> within a larger <span class="hlt">chondrule</span> rim) in ALHA77307, all provide evidence for a formation of FGRs by accretion of dust grains onto freely-floating <span class="hlt">chondrules</span> in the solar nebula before their aggregation into their parent body asteroids. Our study also shows systematically lower abundances of presolar silicate grains in the FGRs than in the matrix regions of CO3 chondrites, while the abundances of SiC grains are the same in all areas, within errors. This trend differs from CR2 chondrites in which the presolar silicate abundances are higher in the FGRs than in the matrix, but similar to each other within 2σ errors. This observation combined with the identification of localized (micrometer-scaled) aqueous alteration in a FGR of LAP 031117 suggests that the lower abundance of presolar silicates in FGRs reflects pre-accretionary aqueous alteration of the fine-grained material in the FGRs. This pre-accretionary alteration could be due to either hydration and heating of freely floating rimmed <span class="hlt">chondrules</span> in icy regions of the solar nebula or melted water ice associated with 26Al-related heating inside precursor planetesimals, followed by aggregation of FGRs into the CO chondrite parent-body.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Litho.272..301B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Litho.272..301B"><span>The aluminum-in-<span class="hlt">olivine</span> thermometer for mantle peridotites - Experimental versus empirical calibration and potential applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bussweiler, Y.; Brey, G. P.; Pearson, D. G.; Stachel, T.; Stern, R. A.; Hardman, M. F.; Kjarsgaard, B. A.; Jackson, S. E.</p> <p>2017-02-01</p> <p>This study provides an experimental calibration of the empirical Al-in-<span class="hlt">olivine</span> thermometer for mantle peridotites proposed by De Hoog et al. (2010). We report Al concentrations measured by secondary ion mass spectrometry (SIMS) in <span class="hlt">olivines</span> produced in the original high-pressure, high-temperature, four-phase lherzolite experiments by Brey et al. (1990). These reversed experiments were used for the calibration of the two-pyroxene thermometer and Al-in-orthopyroxene barometer by Brey and Köhler (1990). The experimental conditions of the runs investigated here range from 28 to 60 kbar and 1000 to 1300 °C. <span class="hlt">Olivine</span> compositions from this range of experiments have Al concentrations that are consistent, within analytical uncertainties, with those predicted by the empirical calibration of the Al-in-<span class="hlt">olivine</span> thermometer for mantle peridotites. Fitting the experimental data to a thermometer equation, using the least squares method, results in the expression: This version of the Al-in-<span class="hlt">olivine</span> thermometer appears to be applicable to garnet peridotites (lherzolites and harzburgites) well outside the range of experimental conditions investigated here. However, the thermometer is not applicable to spinel-bearing peridotites. We provide new trace element criteria to distinguish between <span class="hlt">olivine</span> from garnet-, garnet-spinel-, and spinel-facies peridotites. The estimated accuracy of the thermometer is ± 20 °C. Thus, the thermometer could serve as a useful tool in settings where two-pyroxene thermometry cannot be applied, such as garnet harzburgites and single inclusions in diamond.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940030905','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940030905"><span>Alteration and formation of rims on the CM parent body</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Browning, Lauren B.; Mcsween, Harry Y., Jr.; Zolensky, Michael</p> <p>1994-01-01</p> <p>All types of coarse-grained components in CM chondrites are surrounded by fine-grained dust coatings, but the origin of these rims is not yet clear. Although a strictly nebular origin seems likely for rims in the relatively unaltered type 3 chondrites, the rims in CM chondrites are dominated by secondary alteration phases. It has been argued that either the coarse-grained cores accreted altered rim materials while still in the nebula or that alteration of primary rim phases occurred on the CM parent body. To constrain the origin of alteration phases in rim material, we have analyzed the textures and mineral associations from 10 CM chondritic falls by optical and scanning electron microscopy. Our results indicate that the secondary phases in CM chondritic rims were produced by parent body fluid-rock interactions which redefined some primary rim textures and may have produced, in some cases, both coarse-grained components and the rims that surround them. Textural features demonstrate the interactive exchange of alteration fluids between rims, matrix, and <span class="hlt">chondrules</span> on the CM parent body. For example, most matrix-rim contacts are gradational, suggesting the synchronous alteration of both components. Several observations suggest the possibility of in situ rim production. For example, tochilinite and phyllosilicates commonly form rims around matrix carbonates, which are generally believed to have precipitated from alteration fluids on the CM parent body. This suggests that the rims surrounding matrix carbonates may also have been produced by alteration processes. Partially replaced <span class="hlt">chondrule</span> <span class="hlt">olivines</span> bear a striking resemblance to many rimmed <span class="hlt">olivines</span> in the matrix which suggests, by analogy, that site-specific precipitation of S-bearing phases may also be responsible for the occurrence of many tochilinite-rich rims around isolated matrix <span class="hlt">olivines</span>. Non-silicate rims precipitate around <span class="hlt">olivines</span> of any composition, but the process is most effective for fayalitic <span class="hlt">olivines</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EP%26S...69..128T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EP%26S...69..128T"><span>Sintering polycrystalline <span class="hlt">olivine</span> and polycrystalline clinopyroxene containing trace amount of graphite from natural crystals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsubokawa, Yumiko; Ishikawa, Masahiro</p> <p>2017-09-01</p> <p>Graphite-bearing polycrystalline <span class="hlt">olivine</span> and polycrystalline clinopyroxene with submicron to micron grain size were successfully sintered from a single crystal of naturally occurring <span class="hlt">olivine</span> (Fo88-92Fa12-8: Mg1.76-1.84Fe0.16-0.24SiO4) and a single crystal of naturally occurring clinopyroxene (Di99Hed1: Ca0.92Na0.07Mn0.01Mg0.93Fe0.01Al0.06Si2O6). The milled powders of both these crystals were sintered under argon gas flow at temperatures ranging from 1130 to 1350 °C for 2 h. As the sintering temperature increased, the average grain size of <span class="hlt">olivine</span> increased from 0.2 to 1.4 µm and that of clinopyroxene increased from 0.1 to 2.4 µm. The porosity of sintered samples remained at an almost-constant volume of 2-5% for <span class="hlt">olivine</span> and 3-4% for clinopyroxene. The samples sintered from powders milled with ethanol exhibited trace amount of graphite, identified via Raman spectroscopy analysis. As the sintering temperature increased, the intensity of the graphite Raman peak decreased, compared with both <span class="hlt">olivine</span> and clinopyroxene peaks. The carbon content of the sintered samples was estimated to be a few hundred ppm. The in-plane size ( L a ) of graphite in the sintered <span class="hlt">olivine</span> was estimated to be <15 nm. Our experiments demonstrate new possibilities for preparing graphite-bearing silicate-mantle mineral rocks, and this method might be useful in understanding the influence of the physical properties of graphite on grain-size-sensitive rheology or the seismic velocity of the Earth's mantle.[Figure not available: see fulltext.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034531','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034531"><span>Diffusion-driven magnesium and iron isotope fractionation in Hawaiian <span class="hlt">olivine</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>Teng, F.-Z.; Dauphas, N.; Helz, R.T.; Gao, S.; Huang, S.</p> <p>2011-01-01</p> <p>Diffusion plays an important role in Earth sciences to estimate the timescales of geological processes such as erosion, sediment burial, and magma cooling. In igneous systems, these diffusive processes are recorded in the form of crystal zoning. However, meaningful interpretation of these signatures is often hampered by the fact that they cannot be unambiguously ascribed to a single process (e.g., magmatic fractionation, diffusion limited transport in the crystal or in the liquid). Here we show that Mg and Fe isotope fractionations in <span class="hlt">olivine</span> crystals can be used to trace diffusive processes in magmatic systems. Over sixty <span class="hlt">olivine</span> fragments from Hawaiian basalts show isotopically fractionated Mg and Fe relative to basalts worldwide, with up to 0.4??? variation in 26Mg/24Mg ratios and 1.6??? variation in 56Fe/54Fe ratios. The linearly and negatively correlated Mg and Fe isotopic compositions [i.e., ??56Fe=(??3.3??0.3)????26Mg], co-variations of Mg and Fe isotopic compositions with Fe/Mg ratios of <span class="hlt">olivine</span> fragments, and modeling results based on Mg and Fe elemental profiles demonstrate the coupled Mg and Fe isotope fractionation to be a manifestation of Mg-Fe inter-diffusion in zoned <span class="hlt">olivines</span> during magmatic differentiation. This characteristic can be used to constrain the nature of mineral zoning in igneous and metamorphic rocks, and hence determine the residence times of crystals in magmas, the composition of primary melts, and the duration of metamorphic events. With improvements in methodology, in situ isotope mapping will become an essential tool of petrology to identify diffusion in crystals. ?? 2011 Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1614790G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1614790G"><span>The Standard Hydrous <span class="hlt">Olivine</span> (SHO) conductivity model: A new tool for probing water in the upper mantle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gardés, Emmanuel; Gaillard, Fabrice; Tarits, Pascal</p> <p>2014-05-01</p> <p>It has long been assumed that the incorporation of water in <span class="hlt">olivine</span> has dramatic effects on the physical properties of the mantle, affecting large scale geodynamic processesand triggering most electrical conductivity anomalies in the mantle. But the conductivity models for hydrous <span class="hlt">olivine</span> based on experimental measurements predict contrasting effects of water (e.g. Wang et al. 2006; Yoshino et al. 2009), precluding any unequivocal interpretation of electrical conductivities in the mantle. Our thesis is that the uncertainties and biases in the water contents of the <span class="hlt">olivines</span> used for experiments were inappropriately appreciated, resulting in apparent incompatibilities when analysing the different datasets and in significant biases in the models outside of their range of calibration. Here, we analyse all published experimental work and provide a new model, SHO, that settles these major inconstancies. SHO is calibrated on the largest database of raw conductivity measurements on oriented single crystals and polycrystals of hydrous <span class="hlt">olivine</span>, with water concentrations and temperatures spreading over 0-2220 wt. ppm and 200-1440° C. Our model provides both oriented conductivities, allowing for calculating conductivity anisotropy, and isotropic conductivity, relevant for <span class="hlt">olivine</span> aggregates without preferential orientation. SHO isotropic conductivity (S/m) is given by 2.93 - 157000 -1.54 - 87000-1820C1/H32O σ = 10 e RT + 10 CH2Oe RT , where CH2O is the water concentration in <span class="hlt">olivine</span> (wt. ppm), T the temperature (K) and R = 8.314 J/K/mol. In the normally hot mantle, our model predicts a moderate effect of water on the conductivity of <span class="hlt">olivine</span>. High conductivities (~ 0.1 S/m) are obtained at great depths and elevated water concentrations only (> 350 km and > 400 wt. ppm). The strongest effects are therefore expected in the coldest regions of the mantle, like cratonic lithospheres or subduction zones, where higher incorporation of water in <span class="hlt">olivine</span> is allowed. Wang, D</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110022525','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110022525"><span><span class="hlt">Olivine</span> Composition of the Mars Trojan 5261 Eureka: Spitzer IRS Data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lim, L. F.; Burt, B. J.; Emery, J. P.; Mueller, M.; Rivkin, A. S.; Trilling, D.</p> <p>2011-01-01</p> <p>The largest Mars trojan, 5261 Eureka, is one of two prototype "Sa" asteroids in the Bus-Demeo taxonomy. Analysis of its visible/near-IR spectrum led to the conclusion that it might represent either an angritic analog or an <span class="hlt">olivine</span>-rich composition such as an R chondrite. Spitzer IRS data (5-30 micrometers) have enabled us to resolve this ambiguity. The thermal-IR spectrum exhibits strong <span class="hlt">olivine</span> reststrahlen features consistent with a composition of approximately equals Fo60-70. Laboratory spectra of R chondrites, brachinites, and chassignites are dominated by similar features.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940016276&hterms=hamlet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhamlet','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940016276&hterms=hamlet&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhamlet"><span>Post-metamorphic brecciation in type 3 ordinary chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Scott, E. R. D.; Mccoy, T. J.; Keil, K.</p> <p>1993-01-01</p> <p>Type 3.1-3.9 ordinary chondrites can be divided into two kinds: those in which the compositions of <span class="hlt">chondrule</span> silicates are entirely consistent with metamorphism of type 3.0 material, and those in which the computational heterogeneity appears to be too extreme for in situ metamorphism. We present petrologic data for three LL3 chondrites of the second kind--Ngawi, ALH A77278 (both type 3.6), and Hamlet (type 3.9)--and compare these data with results for the first kind of LL3-4 chondrites. Given that <span class="hlt">chondrules</span> form in the nebula and that metamorphic equilibration occurs in asteroids, our new data imply that Ngawi, A77278, Hamlet, and many other type 3 ordinary chondrites are post-metamorphic breccias containing materials with diverse metamorphic histories; they are not metamorphic rocks or special kinds of 'primitive breccias.' We infer also that metamorphism to type 3.1-3.9 levels produces very friable material that is easily remixed into breccias and lithified by mild shock. Thus, petrologic types and subtypes of chondrites indicate the mean metamorphic history of the ingredients, not the thermal history of the rock. The metamorphic history of individual type 1 or 2 porphyritic <span class="hlt">chondrules</span> in type 3 breccias is best derived from <span class="hlt">olivine</span> and pyroxene analyses and the data of McCoy et al. for unbrecciated chondrites. The new <span class="hlt">chondrule</span> classification schemes of Sears, DeHart et al., appears to provide less information about the original state and metamorphic history of individual porphyritic <span class="hlt">chondrules</span> and should not replace existing classification schemes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993LPI....24.1267S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993LPI....24.1267S"><span>Post-metamorphic brecciation in type 3 ordinary chondrites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scott, E. R. D.; McCoy, T. J.; Keil, K.</p> <p>1993-03-01</p> <p>Type 3.1-3.9 ordinary chondrites can be divided into two kinds: those in which the compositions of <span class="hlt">chondrule</span> silicates are entirely consistent with metamorphism of type 3.0 material, and those in which the computational heterogeneity appears to be too extreme for in situ metamorphism. We present petrologic data for three LL3 chondrites of the second kind--Ngawi, ALH A77278 (both type 3.6), and Hamlet (type 3.9)--and compare these data with results for the first kind of LL3-4 chondrites. Given that <span class="hlt">chondrules</span> form in the nebula and that metamorphic equilibration occurs in asteroids, our new data imply that Ngawi, A77278, Hamlet, and many other type 3 ordinary chondrites are post-metamorphic breccias containing materials with diverse metamorphic histories; they are not metamorphic rocks or special kinds of 'primitive breccias.' We infer also that metamorphism to type 3.1-3.9 levels produces very friable material that is easily remixed into breccias and lithified by mild shock. Thus, petrologic types and subtypes of chondrites indicate the mean metamorphic history of the ingredients, not the thermal history of the rock. The metamorphic history of individual type 1 or 2 porphyritic <span class="hlt">chondrules</span> in type 3 breccias is best derived from <span class="hlt">olivine</span> and pyroxene analyses and the data of McCoy et al. for unbrecciated chondrites. The new <span class="hlt">chondrule</span> classification schemes of Sears, DeHart et al., appears to provide less information about the original state and metamorphic history of individual porphyritic <span class="hlt">chondrules</span> and should not replace existing classification schemes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.5743D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.5743D"><span>Deciphering the dynamics of <span class="hlt">olivine</span> nucleation and growth during antigorite breakdown</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dilissen, Nicole; Kahl, Wolf-Achim; Garrido, Carlos J.; López Sánchez-Vizcaíno, Vicente; Hidas, Károly</p> <p>2016-04-01</p> <p>Subduction zones are dynamic convergent plate boundaries associated with arc volcanism and earthquakes, which are believed to be controlled by fluids released during devolatilization reactions from the downgoing slab. The high-pressure breakdown of antigorite-serpentinite to prograde chlorite-harzburgite is considered to be the most significant source of water in subduction zones. The Cerro del Almirez ultramafic massif (Betic Cordillera, SE Spain) is a unique exhumed subduction terrane that preserves this dehydration reaction as a sharp front. A key to the understanding of the metamorphic conditions prevailing during serpentinite dehydration is to study the two prominent textures, granofels and spinifex-like chlorite harzburgite, which are the reaction products of antigorite breakdown. The textural study of these two types of Chl-harzburgite can provide insights into the kinetic of serpentinite dehydration reaction and the key factors controlling the overstepping of the reaction. Detailed mapping of textural variations in chlorite-harzburgite unveiled a network of granofels and spinifex-like lenses in the Almirez massif. In this work, we focus in the detailed textural variations across a well-exposed lens of spinifex-like chlorite-harzburgite, surrounded by granofels chlorite-harzburgite. This outcrop allowed us to make a very detailed oriented sampling (every 0.1-0.5 m across the 6 m thick lens) from the granofels into spinifex textures. The petrological study shows a developing transition of the <span class="hlt">olivine</span> crystal shape, with premature mm-sized spinifex-like <span class="hlt">olivine</span> crystals at the lens rims and well developed cm-sized spinifex-like grains in the core of the lens. The micro-CT study of oriented cores, together with EBSD study of thin sections from the same cores, allows the 3D reconstruction of <span class="hlt">olivine</span> shapes and their lattice preferred orientation (LPO), constraining how <span class="hlt">olivine</span> shapes and LPO differ from one texture to the other. This study provides valuable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890052751&hterms=lime&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dlime','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890052751&hterms=lime&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dlime"><span>Unusual <span class="hlt">olivine</span> and pyroxene composition in interplanetary dust and unequilibrated ordinary chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klock, W.; Mckay, D. S.; Thomas, K. L.; Palme, H.</p> <p>1989-01-01</p> <p>The presence, in both a number of interplanetary dust particles (IDPs) and in meteorite matrices, of <span class="hlt">olivine</span> and orthopyroxene grains, low in FeO but containing up to 5 wt pct MnO, is reported. The majority of <span class="hlt">olivines</span> and pyroxenes in meteorites contain less than 0.5 wt pct MnO. The presence of these low-iron, manganese-enriched (LIME) <span class="hlt">olivines</span> and pyroxenes in IDPs and meteorites may indicate a link between the origin and history of IDPs and the matrix material of primitive meteorites. The origin of the LIME silicates could be explained by condensation from a gas of solar composition. Forsterite is the first major silicate phase to condense from a solar nebula gas, and Mn, which is not stable as a metal under solar nebula conditions, would condense at about 1100 K as Mn2SiO4 in solid solution with forsterite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26998522','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26998522"><span>Low-temperature plasticity of <span class="hlt">olivine</span> revisited with in situ TEM nanomechanical testing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Idrissi, Hosni; Bollinger, Caroline; Boioli, Francesca; Schryvers, Dominique; Cordier, Patrick</p> <p>2016-03-01</p> <p>The rheology of the lithospheric mantle is fundamental to understanding how mantle convection couples with plate tectonics. However, <span class="hlt">olivine</span> rheology at lithospheric conditions is still poorly understood because experiments are difficult in this temperature range where rocks and mineral become very brittle. We combine techniques of quantitative in situ tensile testing in a transmission electron microscope and numerical modeling of dislocation dynamics to constrain the low-temperature rheology of <span class="hlt">olivine</span>. We find that the intrinsic ductility of <span class="hlt">olivine</span> at low temperature is significantly lower than previously reported values, which were obtained under strain-hardened conditions. Using this method, we can anchor rheological laws determined at higher temperature and can provide a better constraint on intermediate temperatures relevant for the lithosphere. More generally, we demonstrate the possibility of characterizing the mechanical properties of specimens, which can be available in the form of submillimeter-sized particles only.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.3327M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.3327M"><span>Origin of spinel lamella and/or inclusions in <span class="hlt">olivine</span> of harzburgite form the Pauza ultramafic rocks from the Kurdistan region, northeastern Iraq</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mohammad, Y.; Maekawa, H.; Karim, K.</p> <p>2009-04-01</p> <p>Exsolution lamellae and octahedral inclusions of chromian spinel occur in <span class="hlt">olivine</span> of harzburgite of the Pauza ultramafic rocks, Kurdistan region, northeastern Iraq. The lamella is up to 80μm long and up to 50 μm wide. The lamellae and octahedral inclusions of chromian spinel are distributed heterogeneously in the host <span class="hlt">olivine</span> crystal. They are depleted in Al2O3 relative to the subhedral spinel grains in the matrix and spinel lamella in orthopyroxene. <span class="hlt">Olivine</span> (Fo92 - 93) with spinel lamellae occurs as fine-grained crystals around orthopyroxene, whereas <span class="hlt">olivine</span> (Fo90-91) free from spinel is found in matrix. Based on back-scattered images analyses, enrichments of both Cr # and Fe+3 in the chromian spinel lamella in <span class="hlt">olivine</span> (replacive <span class="hlt">olivine</span>) relative to that in adjacent orthopyroxene. As well as the compositions of chromian spinel lamellae host <span class="hlt">olivine</span> are more Mg-rich than the matrix <span class="hlt">olivine</span>. Furthermore the restriction of <span class="hlt">olivine</span> with spinel lamellae and octahedral inclusions on around orthopyroxene, and the similarity of spinel lamella orientations in both <span class="hlt">olivine</span> and adjacent orthopyroxene. This study concludes that the spinel inclusions in <span class="hlt">olivine</span> are remnant (inherited from former orthopyroxene) spinel exsolution lamella in orthopyroxene, that has been formed in upper mantle conditions ( T = 1200 °C, P = 2.5 GPa ). Replacive <span class="hlt">olivine</span> are formed by reaction of ascending silica poor melt and orthopyroxene in harzburgite as pressure decrease the solubility of silica-rich phase (orthopyroxene) in the system increase, therefore ascending melt dissolve pyroxene with spinel exsolution lamella and precipitate replacive <span class="hlt">olivine</span> with spinel inclusions. We can conclude that the <span class="hlt">olivines</span> with spinel lamella are not necessary to be original and presenting ultrahigh-pressure and/or ultra deep-mantle conditions as previously concluded. It has been formed by melting of orthopyroxene (orthopyroxene with spinel exsolution lamella = <span class="hlt">olivine</span> with spinel lamellae and octahedral</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26601281','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26601281"><span>Dislocation-accommodated grain boundary sliding as the major deformation mechanism of <span class="hlt">olivine</span> in the Earth's upper mantle.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ohuchi, Tomohiro; Kawazoe, Takaaki; Higo, Yuji; Funakoshi, Ken-Ichi; Suzuki, Akio; Kikegawa, Takumi; Irifune, Tetsuo</p> <p>2015-10-01</p> <p>Understanding the deformation mechanisms of <span class="hlt">olivine</span> is important for addressing the dynamic processes in Earth's upper mantle. It has been thought that dislocation creep is the dominant mechanism because of extrapolated laboratory data on the plasticity of <span class="hlt">olivine</span> at pressures below 0.5 GPa. However, we found that dislocation-accommodated grain boundary sliding (DisGBS), rather than dislocation creep, dominates the deformation of <span class="hlt">olivine</span> under middle and deep upper mantle conditions. We used a deformation-DIA apparatus combined with synchrotron in situ x-ray observations to study the plasticity of <span class="hlt">olivine</span> aggregates at pressures up to 6.7 GPa (that is, ~200-km depth) and at temperatures between 1273 and 1473 K, which is equivalent to the conditions in the middle region of the upper mantle. The creep strength of <span class="hlt">olivine</span> deforming by DisGBS is apparently less sensitive to pressure because of the competing pressure-hardening effect of the activation volume and pressure-softening effect of water fugacity. The estimated viscosity of <span class="hlt">olivine</span> controlled by DisGBS is independent of depth and ranges from 10(19.6) to 10(20.7) Pa·s throughout the asthenospheric upper mantle with a representative water content (50 to 1000 parts per million H/Si), which is consistent with geophysical viscosity profiles. Because DisGBS is a grain size-sensitive creep mechanism, the evolution of the grain size of <span class="hlt">olivine</span> is an important process controlling the dynamics of the upper mantle.</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('http://adsabs.harvard.edu/abs/2017EGUGA..19..335S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19..335S"><span>Phenocrysts and megacrysts of <span class="hlt">olivines</span> from ultramafic lamprophyres of the Chadobets and Il'bokich uplifts, Southwestern Siberia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smirnova, Maria; Sazonova, Lyudmila; Nosova, Anna; Kargin, Alexey; Shcherbakov, Vasiliy</p> <p>2017-04-01</p> <p>The study of composition and zoning of <span class="hlt">olivines</span> from ultramafic lamprophyres of the SW Siberian craton allowed us to distinguish their main types (phenocrysts and megacrysts) and to estimate the possible P-T conditions of phenocryst crystallization. The studied rocks occur as sills and dikes in the Chadobets and Il'bokich uplifts of the Irkeneeva-Chadobets trough. The ultramafic lamprophyres of these uplifts are spaced around 80 km apart and differ in age by more than 150 Ma. The rocks of the Il'bokich Uplift are dated at Devonian, while the age of the Chadobets Complex is restricted to the Triassic. The episodes of these complexes formation were separated by the large flood basalt event. According to classification (Tappe et al., 2005), the studied rocks are aillikite and damtjernite. <span class="hlt">Olivine</span> phenocrysts from the rocks of the Il'bokich and Chadobets complexes are represented by sub- and euhedral grains. They are composed of core, transitional zone, and rim. <span class="hlt">Olivine</span> cores in the aillikites of the Il'bokich Complex are characterized by Mg# 89; CaO - 0.13-0.14 wt %; TiO2 around 0.03 wt %, Al - 200-380 ppm, and Cr - 130-340 ppm. The cores of phenocrysts from the Chadobets lamprophyres have Mg# 85-87, CaO varying within 0.1-0.2 wt %, and TiO2 - 0.02-0.05 wt %. The megacrysts differ from the phenocrysts of these rocks in the lower Mg# 83-84 and CaO - 0.08-0.14 wt % at higher TiO2 - 0.04-0.05 wt %. Al - 100-700 ppm, Cr - 20-65 ppm. The most striking difference between <span class="hlt">olivines</span> of the two complexes is observed between their Mg#-Ni relations. The cores of <span class="hlt">olivine</span> phenocrysts from the Il'bokich lamprophyres are characterized by the high Mg number (Mg# = 89) and Ni content (2800-3000 ppm), whereas <span class="hlt">olivine</span> cores of the Chadobets aillikites have higher contents of Ni (3000-3500 ppm) at lowered (Mg# = 86-88). These characteristics reflect the compositions of their protolith. The temperature was estimated using monomineral <span class="hlt">olivine</span> thermometer based on the contents of Cr and Al</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22270785-high-temperature-processing-solids-through-solar-nebular-bow-shocks-radiation-hydrodynamics-simulations-particles','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22270785-high-temperature-processing-solids-through-solar-nebular-bow-shocks-radiation-hydrodynamics-simulations-particles"><span>HIGH-TEMPERATURE PROCESSING OF SOLIDS THROUGH SOLAR NEBULAR BOW SHOCKS: 3D RADIATION HYDRODYNAMICS SIMULATIONS WITH PARTICLES</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>Boley, A. C.; Morris, M. A.; Desch, S. J.</p> <p>2013-10-20</p> <p>A fundamental, unsolved problem in solar system formation is explaining the melting and crystallization of <span class="hlt">chondrules</span> found in chondritic meteorites. Theoretical models of <span class="hlt">chondrule</span> melting in nebular shocks have been shown to be consistent with many aspects of thermal histories inferred for <span class="hlt">chondrules</span> from laboratory experiments; but, the mechanism driving these shocks is unknown. Planetesimals and planetary embryos on eccentric orbits can produce bow shocks as they move supersonically through the disk gas, and are one possible source of <span class="hlt">chondrule</span>-melting shocks. We investigate <span class="hlt">chondrule</span> formation in bow shocks around planetoids through three-dimensional radiation hydrodynamics simulations. A new radiation transport algorithmmore » that combines elements of flux-limited diffusion and Monte Carlo methods is used to capture the complexity of radiative transport around bow shocks. An equation of state that includes the rotational, vibrational, and dissociation modes of H{sub 2} is also used. Solids are followed directly in the simulations and their thermal histories are recorded. Adiabatic expansion creates rapid cooling of the gas, and tail shocks behind the embryo can cause secondary heating events. Radiative transport is efficient, and bow shocks around planetoids can have luminosities ∼few× 10{sup –8} L{sub ☉}. While <span class="hlt">barred</span> and radial <span class="hlt">chondrule</span> textures could be produced in the radiative shocks explored here, porphyritic <span class="hlt">chondrules</span> may only be possible in the adiabatic limit. We present a series of predicted cooling curves that merit investigation in laboratory experiments to determine whether the solids produced by bow shocks are represented in the meteoritic record by <span class="hlt">chondrules</span> or other solids.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V11B0345B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V11B0345B"><span>Chemical signature of a migrating grain boundaries in polycrystalline <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boneh, Y.; Marquardt, K.; Skemer, P. A.</p> <p>2017-12-01</p> <p><span class="hlt">Olivine</span> is the most abundant phase and influences strongly the physical and chemical properties of the upper mantle. The structure and chemistry of <span class="hlt">olivine</span> grain-boundaries is important to understand, as these interfaces provide a reservoir for incompatible elements and partial melt, and serve as a fast pathway for chemical diffusion. This project investigates the chemical characteristics of grain boundaries in an <span class="hlt">olivine</span>-rich aggregate. The sample is composed of Fo50 <span class="hlt">olivine</span> crystals with minor amounts of enstatite. It was previously deformed (Hansen et al., 2016) and then annealed (Boneh et al., 2017) to investigate the microstructural changes during recrystallization. This transient microstructure has a bimodal grain size distribution and includes grains that experienced abnormal grain-growth, (porphyroblasts) and highly strained grains with no significant recrystallization or growth (matrix). Using high-resolution transmission electron microscopy (HR-TEM) with energy dispersive X-ray (EDX) at the Bayerisches Geoinstitut (BGI), we characterized boundaries between pairs of porphyroblasts, pairs of matrix grains, and mixed boundaries between porphyroblast and matrix grains. It was found that the boundary between porphyroblasts is enriched in Al and Ca and depleted in Mg, in comparison to grain interiors. However, matrix-matrix boundaries show less chemical segregation of these elements. The relatively high level of chemical segregation to porphyroblast grain boundaries offers different possible interpretations: 1) During grain boundary migration incompatible elements are swept up by the migrating grain boundary. 2) Large angle grain boundaries provide a large density of energetically favorable storage sites for incompatible elements. 3) Diffusion along low angle grain boundaries is too slow to allow for fast chemical equilibration between the different grain boundaries. 4) Dislocations cores serve as an important transport media for impurities (i.e., Cottrell</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11834830','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11834830"><span>Existence of an 16O-rich gaseous reservoir in the solar nebula.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Krot, Alexander N; McKeegan, Kevin D; Leshin, Laurie A; MacPherson, Glenn J; Scott, Edward R D</p> <p>2002-02-08</p> <p>Carbonaceous chondrite condensate <span class="hlt">olivine</span> grains from two distinct petrographic settings, calcium-aluminum-rich inclusion (CAI) accretionary rims and amoeboid <span class="hlt">olivine</span> aggregates (AOAs), are oxygen-16 (16O) enriched at the level previously observed inside CAIs. This requires that the gas in the nebular region where these grains condensed was 16O-rich. This contrasts with an 16O-poor gas present during the formation of <span class="hlt">chondrules</span>, suggesting that CAIs and AOAs formed in a spatially restricted region of the solar nebula containing 16O-rich gas. The 16O-rich gas composition may have resulted either from mass-independent isotopic chemistry or from evaporation of regions with enhanced dust/gas ratios, possibly in an X-wind environment near the young Sun.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28377520','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28377520"><span>Hydration-reduced lattice thermal conductivity of <span class="hlt">olivine</span> in Earth's upper mantle.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chang, Yun-Yuan; Hsieh, Wen-Pin; Tan, Eh; Chen, Jiuhua</p> <p>2017-04-18</p> <p>Earth's water cycle enables the incorporation of water (hydration) in mantle minerals that can influence the physical properties of the mantle. Lattice thermal conductivity of mantle minerals is critical for controlling the temperature profile and dynamics of the mantle and subducting slabs. However, the effect of hydration on lattice thermal conductivity remains poorly understood and has often been assumed to be negligible. Here we have precisely measured the lattice thermal conductivity of hydrous San Carlos <span class="hlt">olivine</span> (Mg 0.9 Fe 0.1 ) 2 SiO 4 (Fo90) up to 15 gigapascals using an ultrafast optical pump-probe technique. The thermal conductivity of hydrous Fo90 with ∼7,000 wt ppm water is significantly suppressed at pressures above ∼5 gigapascals, and is approximately 2 times smaller than the nominally anhydrous Fo90 at mantle transition zone pressures, demonstrating the critical influence of hydration on the lattice thermal conductivity of <span class="hlt">olivine</span> in this region. Modeling the thermal structure of a subducting slab with our results shows that the hydration-reduced thermal conductivity in hydrated oceanic crust further decreases the temperature at the cold, dry center of the subducting slab. Therefore, the <span class="hlt">olivine</span>-wadsleyite transformation rate in the slab with hydrated oceanic crust is much slower than that with dry oceanic crust after the slab sinks into the transition zone, extending the metastable <span class="hlt">olivine</span> to a greater depth. The hydration-reduced thermal conductivity could enable hydrous minerals to survive in deeper mantle and enhance water transportation to the transition zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010044526&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DXxxii','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010044526&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DXxxii"><span>Thermo-Reflectance Spectra of Eros: Unambiguous Detection of <span class="hlt">Olivine</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lucey, P. G.; Hinrichs, J. L.; Urquhart-Kelly, M.; Wellnitz, D.; Bell, J. F., III; Clark, B. E.</p> <p>2001-01-01</p> <p><span class="hlt">Olivine</span> is readily detected on 433 Eros using the new thermo-reflectance spectral technique applied to near-IR spectra obtained at Eros by the NEAR spacecraft. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Litho.265...31J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Litho.265...31J"><span><span class="hlt">Olivine</span> inclusions in Siberian diamonds and mantle xenoliths: Contrasting water and trace-element contents</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jean, M. M.; Taylor, L. A.; Howarth, G. H.; Peslier, A. H.; Fedele, L.; Bodnar, R. J.; Guan, Y.; Doucet, L. S.; Ionov, D. A.; Logvinova, A. M.; Golovin, A. V.; Sobolev, N. V.</p> <p>2016-11-01</p> <p>A subject of continuing debate is how the Earth's lithospheric portion of the upper mantle has remained the thickest (> 200 km) and oldest (> 3 Gy) beneath cratons and is yet surrounded by a vigorously convecting asthenosphere. It is generally admitted that water is a key parameter in the strength and longevity of cratonic roots, because <span class="hlt">olivine</span>, the main phase of the lithospheric mantle, becomes stronger if its water content decreases. Expanding upon the work presented in Novella et al. (2015) and Taylor et al. (2016), we report new water contents for additional <span class="hlt">olivine</span> inclusions in diamonds together with the trace-element composition for all <span class="hlt">olivine</span> inclusions, as well as for mantle xenoliths from various kimberlite pipes located on the Siberian craton. The <span class="hlt">olivine</span> diamond inclusions from this study have systematically low-water contents (< 50 ppmw H2O), moderate to high forsterite (e.g., Fo91-94) contents and low Ni, Co, and Zn ppm contents (e.g., < 2848, < 108, and < 47 ppm, respectively). In contrast, <span class="hlt">olivines</span> from Siberian craton mantle xenoliths have a wide range of water contents (6-323 ppmw H2O) and extend to lower-Fo (91-92), Ni, Co, and Zn-rich compositions, compared to the diamond inclusions. Depleted incompatible trace-element concentrations in <span class="hlt">olivine</span> (0.1-0.001 × Primitive Mantle) advance our hypothesis for the protogenetic origins for the majority of Siberian diamond inclusions. These observations are consistent with the peridotite xenoliths as representing a part of the cratonic lithosphere that has experienced melt re-fertilization, which has also transported water. The <span class="hlt">olivine</span> diamond inclusions, on the other hand, preserve "micro-samples" of an initial, dry cratonic lithosphere, mostly resulting from melting events. These inclusions are likely sourced from the initial cratonic mantle lithosphere, which thereby, resisted delamination over time, due to its buoyancy and strength, imparted from melt and water depletion, respectively. And thus, our</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900046410&hterms=small+data+lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsmall%2Bdata%2Blindstrom','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900046410&hterms=small+data+lindstrom&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsmall%2Bdata%2Blindstrom"><span>Chemical differences between small subsamples of Apollo 15 <span class="hlt">olivine</span>-normative basalts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shervais, J. W.; Vetter, S. K.; Lindstrom, M. M.</p> <p>1990-01-01</p> <p>Results are presented on the chemical and petrological characterization of nine samples of an Apollo 15 mare basalt suite. The results show that all nine samples are low-silica <span class="hlt">olivine</span> normative basalts (ONBs) similar to those described earlier for low-silica ONBs from Apollo 15 site. The samples were found to vary in texture and grain size, from fine-grained intergranular or subophitic basalts to coarse-grained granular 'microgabbros'. Several displayed macroscopic heterogeneity. Variation diagrams show that the overall trend of the data is consistent with the fractionation of <span class="hlt">olivine</span> (plus minor Cr-spinel) from a high-MgO parent magma.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880029590&hterms=body+chemistry&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dbody%2Bchemistry','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880029590&hterms=body+chemistry&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dbody%2Bchemistry"><span>Relation of the spectroscopic reflectance of <span class="hlt">olivine</span> to mineral chemistry and some remote sensing implications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>King, Trude V. V.; Ridley, W. Ian</p> <p>1987-01-01</p> <p>High-resolution visible and near-IR diffuse spectral reflectance are used to systematically investigate apparent wavelength shifts as a function of mineral chemistry in the Fe/Mg <span class="hlt">olivine</span> series from Fo(11) to Fo(91). The study also shows that trace amounts of nickel can be spectrally detected in the <span class="hlt">olivine</span> structure. Significant compositional information can only be extracted at relatively high resolution, because the overall spectral characteristics of the <span class="hlt">olivines</span> change only subtly as a function of the Fe/Mg ratio. This laboratory study is expected to aid in the interpretation of remotely sensed data from both terrestrial and extraterrestrial bodies. Terrestrial applications may include the recognition of ultramafic, ultrabasic, and basaltic terrains which in themselves may have mineral potential. Among extraterrestrial applications, the asteroids are obvious candidates for further examination. Some permutations of Fe-Mg-Ni relations in <span class="hlt">olivines</span> are discussed as they apply to the interpretation of asteroid surfaces and other extraterrestrial bodies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29563498','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29563498"><span>The oldest magnetic record in our solar system identified using nanometric imaging and numerical modeling.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shah, Jay; Williams, Wyn; Almeida, Trevor P; Nagy, Lesleis; Muxworthy, Adrian R; Kovács, András; Valdez-Grijalva, Miguel A; Fabian, Karl; Russell, Sara S; Genge, Matthew J; Dunin-Borkowski, Rafal E</p> <p>2018-03-21</p> <p>Recordings of magnetic fields, thought to be crucial to our solar system's rapid accretion, are potentially retained in unaltered nanometric low-Ni kamacite (~ metallic Fe) grains encased within dusty <span class="hlt">olivine</span> crystals, found in the <span class="hlt">chondrules</span> of unequilibrated chondrites. However, most of these kamacite grains are magnetically non-uniform, so their ability to retain four-billion-year-old magnetic recordings cannot be estimated by previous theories, which assume only uniform magnetization. Here, we demonstrate that non-uniformly magnetized nanometric kamacite grains are stable over solar system timescales and likely the primary carrier of remanence in dusty <span class="hlt">olivine</span>. By performing in-situ temperature-dependent nanometric magnetic measurements using off-axis electron holography, we demonstrate the thermal stability of multi-vortex kamacite grains from the chondritic Bishunpur meteorite. Combined with numerical micromagnetic modeling, we determine the stability of the magnetization of these grains. Our study shows that dusty <span class="hlt">olivine</span> kamacite grains are capable of retaining magnetic recordings from the accreting solar system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EM%26P..110....1M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EM%26P..110....1M"><span>The New Peruvian Meteorite Carancas: Mössbauer Spectroscopy and X-Ray Diffraction Studies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Munayco, P.; Munayco, J.; Varela, M. E.; Scorzelli, R. B.</p> <p>2013-02-01</p> <p>The Carancas meteorite fell on 15 September 2007 approximately 10 km south of Desaguadero, near Lake Titicaca, Peru, producing bright lights, clouds of dust in the sky and intense detonations. The Carancas meteorite is classified as a H4-5 ordinary chondrite with shock stage S3 and a degree of weathering W0. The Carancas meteorite is characterized by well defined <span class="hlt">chondrules</span> composed either of <span class="hlt">olivine</span> or pyroxene. The Mössbauer spectra show an overlapping of paramagnetic and magnetic phases. The spectra show two quadrupole doublets associated to <span class="hlt">olivine</span> and pyroxene; and two magnetic sextets, associated with the primary phases kamacite/taenite and Troilite (Fe2+). Metal particles were extracted from the bulk powdered samples exhibit only kamacite and small amounts of the intergrowth tetrataenite/antitaenite. X-Ray diffractogram shows the primary phases <span class="hlt">olivine</span>, pyroxene, troilite, kamacite, diopside and albite. Iron oxides has not been detected by Mössbauer spectroscopy or XRD as can be expected for a meteorite immediately recovered after its fall.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Icar..289...42C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Icar..289...42C"><span>Vaporization and thermodynamics of forsterite-rich <span class="hlt">olivine</span> and some implications for silicate atmospheres of hot rocky exoplanets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Costa, Gustavo C. C.; Jacobson, Nathan S.; Fegley, Bruce, Jr.</p> <p>2017-06-01</p> <p>We describe an experimental and theoretical study of <span class="hlt">olivine</span> [Mg2SiO4 (Fo)-Fe2SiO4 (Fa)] vaporization. The vaporization behavior and thermodynamic properties of a fosterite-rich <span class="hlt">olivine</span> (Fo95Fa5) have been explored by high-temperature Knudsen effusion mass spectrometry (KEMS) from 1750 to 2250 K. The gases observed (in order of decreasing partial pressure) are Fe, SiO, Mg, O2 and O. We measured the solidus temperature (∼2050 K), partial pressures of individual gases, the total vapor pressure, and thermodynamic activities and partial molar enthalpies of MgO, 'FeO', and SiO2 for the Fo95Fa5 <span class="hlt">olivine</span>. The results are compared to other measurements and models of the <span class="hlt">olivine</span> system. Our experimental data show <span class="hlt">olivine</span> vaporizes incongruently. We discuss this system both as a psuedo-binary of Fo-Fa and a psuedo-ternary of MgO-'FeO'-SiO2. Iron/magnesium molar ratios in the sample before (∼0.05) and after (∼0.04) vaporization are consistent with the small positive deviations from ideality of fayalite (γ ∼ 1.17) in <span class="hlt">olivine</span> of the composition studied (e.g., Nafziger and Muan, 1967). Our data for <span class="hlt">olivine</span> + melt confirm prior theoretical models predicting fractional vaporization of Fe relative to Mg from molten silicates (Fegley and Cameron, 1987; Schaefer and Fegley, 2009; Ito et al., 2015). If loss of silicate atmospheres occurs from hot rocky exoplanets with magma oceans the residual planet may be enriched in magnesium relative to iron.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010045242&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DXxxii','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010045242&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DXxxii"><span><span class="hlt">Olivine</span> Weathering: Abiotic Versus Biotic Processes as Possible Biosignatures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Longazo, T. G.; Wentworth, S. J.; McKay, D. S.; Southam, G.; Clemett, S. J.</p> <p>2001-01-01</p> <p>A preliminary study to determine how abiotic versus biotic processes affect the weathering of <span class="hlt">olivine</span> crystals. Perhaps the differences between these weathering processes could be used as biosignatures. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR33A2672S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR33A2672S"><span>Discovery of composite diopside-magnetite lamellae in discrete <span class="hlt">olivine</span> crytals from Colorado Plateau diatremes: indication of former hydrous ringwoodite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sakamaki, K.; Sato, Y.; Marshall, E. W., IV; Ogasawara, Y.</p> <p>2016-12-01</p> <p>We investigate composite diopside (Di) + magnetite (Mt) lamellae in <span class="hlt">olivine</span> crystals from Oligocene diatremes of serpentinized ultramafic microbreccia located at Buell Park (AZ) and Green Knobs (NM) in the Colorado Plateau, and propose their genesis as breakdown products of precursor hydrous ringwoodite (γ-<span class="hlt">olivine</span>) lamellae coexisting with α-<span class="hlt">olivine</span> host. Among a hundred <span class="hlt">olivines</span> (2-5 mm across, Fo89-93 in mol%) from both localities, the Di + Mt composite lamellae are recognized in only 15 of relatively Fe-rich grains (Fo89-91.5). The <span class="hlt">olivine</span> host contains minor amounts of Ca (< 0.01 wt% CaO), Mn, Ni, and Co. Lamellar Di (Di95) contains minor amounts of Al, Na, Cr, Mn, and Ni. Lamellar Mt contains Cr (5.0-43.0 wt% Cr2O3) with minor amounts of Si, Ti, Al, Mn, Ni, and Co. The area fractions of <span class="hlt">olivine</span> host and the lamellae in a typical grain (sample no. BP02-3) were measured at 98.8 % of the host and 1.2 % of the lamellae that are composed of Di:Mt = 85:15 to 53:47, average 66:34. The estimated average CaO content in a lamella reaches 17 wt% and the reintegrated CaO in the host and the lamellae is 0.22 wt%.We propose that Fe3+ in lamellar Mt was produced by dehydration of hydrous precursor phase via the reaction, Fe2+ + OH- = Fe3+ + O2- + 1/2H2. Converting Fe3+ into Fe2+ in the precursor phase based on this reaction, the composition satisfies the stoichiometry of <span class="hlt">olivine</span> (X2TO4). Thus, the pre-existing phase certainly is of hydrous and contains Ca and other components with <span class="hlt">olivine</span> stoichiometry. The most likely phase is lamellar hydrous ringwoodite. The precursor phase, hydrous ringwoodite, might have occurred as lamellae with α-<span class="hlt">olivine</span> host and have probably decomposed by the following reaction, (1+X+Y+Z) hydrous ringwoodite → α-<span class="hlt">olivine</span> + X Di + Y Mt + Z H2 (where X:Y:Z=2:1:1). The composite Di-Mt lamellae after hydrous ringwoodite lamellae in α-<span class="hlt">olivine</span> host certainly suggest the materials originated from a deep mantle setting at least 300 km.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AGUFM.T41C0231B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AGUFM.T41C0231B"><span><span class="hlt">Olivine</span> Friction at the Base of the Seismogenic Zone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boettcher, M. S.; Hirth, G.; Evans, B.</p> <p>2003-12-01</p> <p>The frictional properties at the base of the seismogenic zone in oceanic lithosphere are fundamental to our understanding of oceanic earthquake processes. While the composition of the oceanic lithosphere is probably the simplest and most well constrained of any seismogenic region on Earth, few data on its frictional properties exist. We are investigating the strength and sliding stability of <span class="hlt">olivine</span> aggregates at temperature and effective pressure conditions close to those at the base of the seismogenic zone on a typical transform fault. We have conducted triaxial compression tests on dry <span class="hlt">olivine</span> powder (38-60 \\ μ m particles) at effective pressures of P{eff} = P{c} - P{f} = 50, \\ 200, \\ & \\ 300 MPa using argon as a pore fluid medium, temperatures of T = 800o{C} \\ & \\ 1000o{C}, and strain rates of ˙ {ɛ } = 3 x 10-5 \\ & \\ 3 x 10-4. For all experiments, strain became localized on faults and strain-rate steps showed velocity-weakening behavior. Stick-slip events were observed at all temperatures up to 1000oC, with a greater tendency towards instability (i.e. more stick-slip events) at the higher strain rate. By contrast, previous laboratory work by Stesky et al. (1974) found stable sliding for <span class="hlt">olivine</span> at temperatures above 200oC. Our experiments are consistent with seismic data, which find that earthquake hypocenters regularly occur to temperatures well above 200oC, regularly to near the 600oC isotherm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MinPe.111..909Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MinPe.111..909Y"><span>Genetic relationship between deformation and low-Ca content in <span class="hlt">olivine</span> from magmatic systems: evidence from the Poyi ultramafic intrusion, NW China</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yao, Zhuo-sen; Qin, Ke-zhang; Xue, Sheng-chao</p> <p>2017-12-01</p> <p>The deformation features (e.g., undulose extinction and subgrain boundaries) and low Ca content (<1000 ppm) of high-Fo <span class="hlt">olivine</span> have been widely used as indictors for the mantle origin of <span class="hlt">olivine</span> in the past. However, grains with these characteristics are also found in some crustal intrusions, e.g., Duke Island and Bushveld complexes. Here, we study this type of <span class="hlt">olivine</span> in the Poyi ultramafic intrusion, NW China, to trace the formation of these unusual features in magmatic systems. As a result of the possible Ca-depleted parental melt and low Ca <span class="hlt">olivine</span>/melt partition coefficient, <span class="hlt">olivine</span> from the Poyi intrusion is extremely depleted in Ca. On the other hand, it has been confirmed that trace elements with large ionic radii (e.g., Ca2+ and Al3+) are chemically segregated at the grain boundary of <span class="hlt">olivine</span>, exerting a dragging influence on grain boundary processes (named as solute drag effect). In this regard, the low Ca content in <span class="hlt">olivine</span> weakens the solute drag effect, and in doing so it enhances the rate and strength of grain deformation, which occurs to accommodate the stress derived by fast compaction of the crystal mush in Poyi intrusion. Therefore, there is a genetic relationship between the plastic deformation and low Ca content in <span class="hlt">olivines</span> from magmatic cumulates, and this link is one of the reasons causing the widespread deformation observed in Ca-depleted <span class="hlt">olivine</span> from Poyi and other intrusions. What is more important, this work fills the gaps in the interpretation of this type of <span class="hlt">olivine</span> in volcanic rocks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NIMPA.876..202F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NIMPA.876..202F"><span>Performance simulation of Ba<span class="hlt">Bar</span> DIRC <span class="hlt">bar</span> boxes in TORCH</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Föhl, K.; Brook, N.; Castillo García, L.; Cussans, D.; Forty, R.; Frei, C.; Gao, R.; Gys, T.; Harnew, N.; Piedigrossi, D.; Rademacker, J.; Ros García, A.; van Dijk, M.</p> <p>2017-12-01</p> <p>TORCH is a large-area precision time-of-flight detector based on the DIRC principle. The DIRC <span class="hlt">bar</span> boxes of the Ba<span class="hlt">Bar</span> experiment at SLAC could possibly be reused to form a part of the TORCH detector time-of-flight wall area, proposed to provide positive particle identification of low momentum kaons in the LHCb experiment at CERN. For a potential integration of Ba<span class="hlt">Bar</span> <span class="hlt">bar</span> boxes into TORCH, new imaging readout optics are required. From the several designs of readout optics that have been considered, two are used in this paper to study the effect of Ba<span class="hlt">Bar</span> <span class="hlt">bar</span> optical imperfections on the detector reconstruction performance. The kaon-pion separation powers obtained from analysing simulated photon hit patterns show the performance reduction for a Ba<span class="hlt">Bar</span> <span class="hlt">bar</span> of non-square geometry compared to a perfectly rectangular cross section.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013IJMPA..2850153B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013IJMPA..2850153B"><span>PREDICTIONS FOR $B \\to \\tau \\<span class="hlt">bar</span>{\\mu} + \\mu \\<span class="hlt">bar</span>{\\tau}$</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Boubaa, Dris; Datta, Alakabha; Duraisamy, Murugeswaran; Khalil, Shaaban</p> <p>2013-12-01</p> <p>The observation of B -> τ \\<span class="hlt">bar</span> {μ } + μ \\<span class="hlt">bar</span> {τ } at present experiments would be a clear sign of new physics. In this paper, we calculate this process in an extended Higgs sector framework where the decay is mediated by the exchange of spin zero particle with flavor changing neutral current couplings. If we identify the scalar with the newly discovered state at LHC with a mass 125 GeV then we find that, after imposing all experimental constraints, the BR(Bs -> τ \\<span class="hlt">bar</span> {μ } + μ \\<span class="hlt">bar</span> {τ }) can be as high as 10-6 and BR (Bd -> τ \\<span class="hlt">bar</span> {μ } + μ \\<span class="hlt">bar</span> {τ }) can be as high as 10-7. We also calculate this process in the minimal supersymmetric standard model and find the BR(Bs ->τ \\<span class="hlt">bar</span> {μ } + μ \\<span class="hlt">bar</span> {τ }) is typically of the order 10-8.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4646795','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4646795"><span>Dislocation-accommodated grain boundary sliding as the major deformation mechanism of <span class="hlt">olivine</span> in the Earth’s upper mantle</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ohuchi, Tomohiro; Kawazoe, Takaaki; Higo, Yuji; Funakoshi, Ken-ichi; Suzuki, Akio; Kikegawa, Takumi; Irifune, Tetsuo</p> <p>2015-01-01</p> <p>Understanding the deformation mechanisms of <span class="hlt">olivine</span> is important for addressing the dynamic processes in Earth’s upper mantle. It has been thought that dislocation creep is the dominant mechanism because of extrapolated laboratory data on the plasticity of <span class="hlt">olivine</span> at pressures below 0.5 GPa. However, we found that dislocation-accommodated grain boundary sliding (DisGBS), rather than dislocation creep, dominates the deformation of <span class="hlt">olivine</span> under middle and deep upper mantle conditions. We used a deformation-DIA apparatus combined with synchrotron in situ x-ray observations to study the plasticity of <span class="hlt">olivine</span> aggregates at pressures up to 6.7 GPa (that is, ~200-km depth) and at temperatures between 1273 and 1473 K, which is equivalent to the conditions in the middle region of the upper mantle. The creep strength of <span class="hlt">olivine</span> deforming by DisGBS is apparently less sensitive to pressure because of the competing pressure-hardening effect of the activation volume and pressure-softening effect of water fugacity. The estimated viscosity of <span class="hlt">olivine</span> controlled by DisGBS is independent of depth and ranges from 1019.6 to 1020.7 Pa·s throughout the asthenospheric upper mantle with a representative water content (50 to 1000 parts per million H/Si), which is consistent with geophysical viscosity profiles. Because DisGBS is a grain size–sensitive creep mechanism, the evolution of the grain size of <span class="hlt">olivine</span> is an important process controlling the dynamics of the upper mantle. PMID:26601281</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR41E..03K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR41E..03K"><span>Investigation of <span class="hlt">olivine</span> and orthopyroxene grain boundaries by atom probe tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krawczynski, M.; Skemer, P. A.; Bachhav, M.; Dong, Y.; Marquis, E. A.</p> <p>2016-12-01</p> <p>Accurate chemical analysis at grain boundaries is challenging by traditional microscopic techniques, especially for poor conducting geological samples. Atom probe tomography (APT) is a unique technique that can elucidate chemistry and 3-D distribution of elements within a sample volume at the sub-nanometer length scale. With advances in laser and sample preparation techniques in the last decade, APT is now successfully applied to a wide range of poor conducting materials like metal oxides, ceramics, and biological minerals. In this study, we apply the APT technique to investigate the grain boundary chemistry of orthopyroxene (opx) and <span class="hlt">olivine</span>. These minerals are the most abundant in the upper mantle and their grain boundaries may be important geochemical reservoirs in Earth. Moreover, physical properties such as grain boundary diffusivity, conductivity, and mobility, are likely influenced by the presence or absence of impurities. Single crystals of opx and <span class="hlt">olivine</span> grains, separated from a San Carlos xenolith, were deformed at 1 GPa and 1500 K. Plastic deformation promoted dynamic recrystallization, creating new grain boundaries within a chemically homogeneous medium. Needle shaped specimens of opx-opx and <span class="hlt">olivine-olivine</span> grain boundaries were prepared using standard lift out techniques and a dual beam focused ion beam (FIB). APT analyses were performed in laser mode with laser energy of 50 pJ/pulse, repetition rate of 200 kHz, and detection rate of 1%. A 3-D distribution of elements was reconstructed and 1-D profiles across the grain boundary have been calculated. Fe, Al, and Ca show enrichments at the grain boundaries for both phases, consistent with previous studies that used STEM/EDX or EPMA techniques. Although qualitatively similar, the spatial resolution of the APT method is significantly better than other methods, and our data show that the grain-boundary enrichment of minor elements in both <span class="hlt">olivine</span> and pyroxene compositions is limited to a region no greater</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://hdl.handle.net/2060/20050162228','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050162228"><span>The Iodine-Xenon System in Outer and Inner Portions of <span class="hlt">Chondrules</span> from the Unnamed Antarctic LL3 Chondrite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Meshik, A. P.; Pravdivtseva, O. V.; Hohenberg, C. M.; Amelin, Y.</p> <p>2004-01-01</p> <p>Alteration processes may affect I-Xe system in unequilibrated ordinary chondrites. It was shown that at the edges, where a contribution is made by matrix material around the rim, *Xe-129/Xe-128 values are generally lower (later apparent ages) than in the main <span class="hlt">chondrule</span> mass. In this work we attempted to investigate whether thermal metamorphism can affect the I-Xe system in LL3 chondrites which did not experienced aqueous alteration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.V23D2870K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.V23D2870K"><span>Calculation Of Clinopyroxene And <span class="hlt">Olivine</span> Growth Rates Using Plagioclase Residence Time</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kilinc, A. I.; Borell, A.; Leu, A.</p> <p>2012-12-01</p> <p>According to the Crystal Size Distribution theory (CSD) in a plot of logarithm of number of crystals of a given size range per unit volume [ln(n)], against crystal size [L] shows a straight line. Slope of that line is given by where is the crystal residence time and G is the crystal growth rate. Therefore if is known then G can be calculated. We used thin sections of the Kilauea basalt from Hawaii where <span class="hlt">olivine</span>, clinopyroxene and plagioclase crystallized within a small temperature range, and the crystal growth rate of plagioclase is known. Assuming that crystal residence times of these three minerals are the same, we plotted ln(n) against L and using the slope and the known crystal growth rate of plagioclase we calculated the crystal growth rates of clinopyroxene and <span class="hlt">olivine</span>. For the clinopyroxene growth rate we report 10-10.9cm/sec, which is in good agreement with Congdon's data of 10-10 cm/sec. We also calculated the growth rate of <span class="hlt">olivine</span> is a basaltic melt as 10-8.5 cm/sec which is comparable to < 10-10 to 10-7 cm/sec given by Donaldson and Jambon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.1917G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.1917G"><span>Melting mode and source lithology inferred from trace element systematic in historical <span class="hlt">olivine</span> from Lanzarote, Canary Islands</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gómez-Ulla, Alejandra; Sigmarsson, Olgeir; Guðfinnsson, Guðmundur H.</p> <p>2017-04-01</p> <p>Trace element concentrations and ratios in <span class="hlt">olivine</span> phenocrysts, such as fractionation-corrected Ni x (FeO/MgO) and Fe/Mn, have been shown useful as probes of pyroxenite derived component in mixtures of primary mantle melts (e.g. Sobolev et al., 2007). For instance, higher Ni and lower Mn and Ca contents are expected in partial melts of pyroxenite compared to those of lherzolite. We have measured trace element concentrations in <span class="hlt">olivine</span> from 1730-1736 AD (Timanfaya) and 1824 AD eruptions in Lanzarote (Canary Islands), which erupted mafic and mantle nodule bearing magmas, ranging in composition from highly silica-undersaturated basanite through alkali basalt to tholeiite. The early basanite exhibit the largest <span class="hlt">olivine</span> trace element variation covering the range of those from MORB and OIB worldwide, whereas later erupted tholeiite have values typical from pyroxenite derived melts. The Fo value decreased systematically with time during the 1730-36 eruption and the proportion of silica-saturated primary melt increased in the parental magma mixture with time. At the end of the eruption, tholeiite magmas crystallized <span class="hlt">olivine</span> with, increasing concentrations of Mn and Ca and higher Ca/Al at relatively uniform Ni x (FeO/MgO) and Fe/Mn, all of which is readily explained by increased decompression melting at lower temperature. The basanite from the eruption that took place in 1824 AD has <span class="hlt">olivine</span> with even higher Fo value and trace element variability similar those of the Timanfaya basanite. The fact that the Lanzarote basanite contain <span class="hlt">olivine</span> with trace element systematic spanning that of MORB and pyroxenite melt can be explained by CO2-flux melting of a lithologically heterogeneous source, generating the diverse compositions. Initial reactive porous flow through depleted oceanic lithosphere and equilibration with dunitic restite of percolating pyroxenite melt may have amplified the observed Ni depletion in <span class="hlt">olivine</span> of the earliest basanite. The fact that <span class="hlt">olivine</span> compositions and</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 <span class="hlt">olivine</span> crystallographic preferred orientations: The effect of strain geometry on mantle 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 mantle. Specifically, the relationship between shape preferred orientation (SPO) and CPO in mantle 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 <span class="hlt">olivine</span> 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), differential stresses (2-60 MPa), and water content (up to 500 H/106Si) of the xenolith suite, variations in <span class="hlt">olivine</span> CPO do not correlate with changes in deformation conditions. Here we establish for the first time in naturally deformed mantle rocks that finite strain geometry controls the development of axial-type <span class="hlt">olivine</span> CPOs; axial-[010] and axial-[100] CPOs form in relation to oblate and prolate fabric ellipsoids, respectively. Girdling of <span class="hlt">olivine</span> crystal axes results from intracrystalline slip with activation of multiple slip systems and grain boundary sliding. Our results demonstrate that mantle deformation may deviate from simple shear. <span class="hlt">Olivine</span> texture in field studies and seismic anisotropy in geophysical investigations can provide critical constraints for the 3-D strain in the upper mantle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.V41C2506G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.V41C2506G"><span>Serpentinization of <span class="hlt">Olivine</span> by Seawater: A Flow-Through Experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gouze, P.; Luquot, L.; Andreani, M.; Godard, M.; Gibert, B.</p> <p>2011-12-01</p> <p>The mantle exposed at slow spreading ridges is pervasively serpentinized, down to ca. 5km according to geophysical data. The onset and durability of this hydration process require efficient penetration and renewal of fluids at the mineral-fluid interface. However, the mechanisms of fluid penetration are still poorly understood. Moreover, serpentinization is exovolumic, if a mass-conservative system is assumed, or chemical elements are leached out to conserve rock volume. Thus, the extent of serpentinization depends of the system capacity to create space and/or to drive mass transfers. In order to investigate these hydrodynamic and chemical mechanisms, we did a laboratory experiment during which seawater was injected in a sintered San Carlos <span class="hlt">olivine</span> sample at conditions representative of low temperature ultramafic hydrothermal systems. The percolation-reaction experiment was carried out at 19 MPa and 190°C; the initial water flow was set at 0.2 mL/h then decreased down to 0.06 mL/h after 8 days. During the experiment (23 days), permeability decreased continuously. The composition of the outlet fluid varied strongly during the first 24h of the experiment, then reached equilibrium values. The high Si concentrations in outlet fluids indicated steady <span class="hlt">olivine</span> dissolution, while their low Fe and Mg concentrations suggested precipitation of Fe- and Mg-rich mineral phases. The reacted sample acquired a reddish brown color, indicating oxidation reactions occurred. Optical observation and SEM imaging revealed the presence of a soft white material filling the pores of the reacted sample. It was identified as a poorly crystallized serpentine type material by AEM/TEM analyses. This proto-serpentine is intimately associated to <100 nm Fe-oxide patches (probably hematite) growing on the <span class="hlt">olivine</span> surface. We interpret the precipitation of this proto-serpentine together with Fe-oxides throughout the sample as marking the early stages of serpentinization. The fluid composition not</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CoMP..173...19Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CoMP..173...19Z"><span>An experimental study of Fe-Ni exchange between sulfide melt and <span class="hlt">olivine</span> at upper mantle conditions: implications for mantle sulfide compositions and phase equilibria</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zhou; von der Handt, Anette; Hirschmann, Marc M.</p> <p>2018-03-01</p> <p>The behavior of nickel in the Earth's mantle is controlled by sulfide melt-<span class="hlt">olivine</span> reaction. Prior to this study, experiments were carried out at low pressures with narrow range of Ni/Fe in sulfide melt. As the mantle becomes more reduced with depth, experiments at comparable conditions provide an assessment of the effect of pressure at low-oxygen fugacity conditions. In this study, we constrain the Fe-Ni composition of molten sulfide in the Earth's upper mantle via sulfide melt-<span class="hlt">olivine</span> reaction experiments at 2 GPa, 1200 and 1400 °C, with sulfide melt X_{{{Ni}}}^{{{Sulfide}}}={{Ni}}/{{Ni+{Fe}}} (atomic ratio) ranging from 0 to 0.94. To verify the approach to equilibrium and to explore the effect of {f_{{{O}2}}} on Fe-Ni exchange between phases, four different suites of experiments were conducted, varying in their experimental geometry and initial composition. Effects of Ni secondary fluorescence on <span class="hlt">olivine</span> analyses were corrected using the PENELOPE algorithm (<span class="hlt">Bar</span>ó et al., Nucl Instrum Methods Phys Res B 100:31-46, 1995), "zero time" experiments, and measurements before and after dissolution of surrounding sulfides. Oxygen fugacities in the experiments, estimated from the measured O contents of sulfide melts and from the compositions of coexisting <span class="hlt">olivines</span>, were 3.0 ± 1.0 log units more reduced than the fayalite-magnetite-quartz (FMQ) buffer (suite 1, 2 and 3), and FMQ - 1 or more oxidized (suite 4). For the reduced (suites 1-3) experiments, Fe-Ni distribution coefficients K_{{D}}{}={(X_{{{Ni}}}^{{{sulfide}}}/X_{{{Fe}}}^{{{sulfide}}})}/{(X_{{{Ni}}^{{{<span class="hlt">olivine}}}/X_{{{Fe}}}^{{{olivine</span>}}})}} are small, averaging 10.0 ± 5.7, with little variation as a function of total Ni content. More oxidized experiments (suite 4) give larger values of K D (21.1-25.2). Compared to previous determinations at 100 kPa, values of K D from this study are chiefly lower, in large part owing to the more reduced conditions of the experiments. The observed difference does not seem</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010044720&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DXxxii','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010044720&hterms=Xxxii&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DXxxii"><span>Systematics of Ni, Co, Cr and V in <span class="hlt">Olivine</span> from Planetary Melt Systems: Martian Basalts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Herd, C. D. K.; Jones, J. H.; Shearer, C. K.; Papike, J. J.</p> <p>2001-01-01</p> <p>Secondary Ion Mass Spectrometry (SIMS) data for Ni, Co, Cr, and V in <span class="hlt">olivine</span> in martian basalts is compared to data from lunar and terrestrial basalts. We use experimentally-derived and published D values to calculate as-yet unsampled, <span class="hlt">olivine</span>-bearing, non-cumulus melt compositions. Additional information is contained in the original extended abstract.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeCoA.154..130O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeCoA.154..130O"><span>Processes and time scales of magmatic evolution as revealed by Fe-Mg chemical and isotopic zoning in natural <span class="hlt">olivines</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oeser, Martin; Dohmen, Ralf; Horn, Ingo; Schuth, Stephan; Weyer, Stefan</p> <p>2015-04-01</p> <p>In this study, we applied high-precision in situ Fe and Mg isotope analyses by femtosecond laser ablation (fs-LA) MC-ICP-MS on chemically zoned <span class="hlt">olivine</span> xeno- and phenocrysts from intra-plate volcanic regions in order to investigate the magnitude of Fe and Mg isotope fractionation and its suitability to gain information on magma evolution. Our results show that chemical zoning (i.e., Mg#) in magmatic <span class="hlt">olivines</span> is commonly associated with significant zoning in δ56Fe and δ26Mg (up to 1.7‰ and 0.7‰, respectively). We explored different cases of kinetic fractionation of Fe and Mg isotopes by modeling diffusion in the melt or <span class="hlt">olivine</span> and simultaneous growth or dissolution. Combining the information of chemical and isotopic zoning in <span class="hlt">olivine</span> allows to distinguish between various processes that may occur during magma evolution, namely diffusive Fe-Mg exchange between <span class="hlt">olivine</span> and melt, rapid crystal growth, and Fe-Mg inter-diffusion simultaneous to crystal dissolution or growth. Chemical diffusion in <span class="hlt">olivine</span> appears to be the dominant process that drives isotope fractionation in magmatic <span class="hlt">olivine</span>. Simplified modeling of Fe and Mg diffusion is suitable to reproduce both the chemical and the isotopic zoning in most of the investigated <span class="hlt">olivines</span> and, additionally, provides time information about magmatic processes. For the Massif Central (France), modeling of diffusive re-equilibration of mantle <span class="hlt">olivines</span> in basanites revealed a short time span (<2 years) between the entrainment of a mantle xenolith in an intra-plate basaltic magma and the eruption of the magma. Furthermore, we determined high cooling rates (on the order of a few tens to hundreds of °C per year) for basanite samples from a single large outcrop in the Massif Central, which probably reflects the cooling of a massive lava flow after eruption. Results from the modeling of Fe and Mg isotope fractionation in <span class="hlt">olivine</span> point to a systematic difference between βFe and βMg (i.e., βFe/βMg ≈ 2), implying that the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20150006011','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20150006011"><span>Evidence of Metasomatism in the Lowest Petrographic Types Inferred from A Na(-), K, Rich Rim Around A LEW 86018 (L3.1) <span class="hlt">Chondrule</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mishra, Ritesh Kumar; Marhas, Kuljeet Kaur; Simon, Justin I.; Ross, Daniel Kent</p> <p>2015-01-01</p> <p>Ordinary chondrites (OCs) represent the most abundant extraterrestrial materials and also record the widest range of alteration of primary, pristine minerals of early Solar system material available for study. Relatively few investigations, however, address: (1) the role of fluid alteration, and (2) the relationship between thermal metamorphism and metasomatism in OCs, issues that have been extensively studied in many other meteorite groups e.g., CV, CO, CR, and enstatite chondrites. Detailed elemental abundances profiles across individual <span class="hlt">chondrules</span>, and mineralogical studies of Lewis Hills (LEW) 86018 (L3.1), an unequilibrated ordinary chondrite (UOC) of low petrographic type of 3.1 returned from Antarctica, provide evidence of extensive alteration of primary minerals. Some <span class="hlt">chondrules</span> have Na(-), K(-), rich rims surrounded by nepheline, albite, and sodalite-like Na(-), Cl(-), Al-rich secondary minerals in the near vicinity within the matrices. Although, limited evidences of low temperature (approximately 250 C) fluid-assisted alteration of primary minerals to phyllosilicates, ferroanolivine, magnetite, and scapolite have been reported in the lowest grades (less than 3.2) Semarkona (LL3.00) and Bishunpur (LL3.10), alkali-rich secondary mineralization has previously only been seen in higher grade greater than 3.4 UOCs. This preliminary result suggests highly localized metamorphism in UOCs and widens the range of alteration in UOCs and complicates classification of petrographic type and extent of thermal metamorphism or metasomatism. The work in progress will document the micro-textures, geochemistry (Ba, Ca, REE), and isotopic composition (oxygen, Al(-)- 26 Mg-26) of mineral phases in <span class="hlt">chondrules</span> and adjoining objects to help us understand the formation scenario and delineate possible modes of metamorphism in UOCs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013135','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013135"><span>Surviving High-temperature Components in CI Chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zolensky, M.; Frank, D.</p> <p>2014-01-01</p> <p>The CI1 chondrites, while having the most solar-like compo-sition of any astromaterial available for laboratory analysis, have also been considerably altered by asteroidal processes including aqueous alteration. It is of fundamental importance to determine their pre-alteration mineralogy, so that the state of matter in the early Solar System can be better determined. In the course of a re-examination of the compositional range of <span class="hlt">olivine</span> and low-Ca pyroxene in CI chondrites Orgueil, Ivuna and Alais [1] we found the first reported complete CAI, as already reported [2], with at-tached rock consisting mainly of <span class="hlt">olivine</span> and low-Ca pyroxene. The range of residual <span class="hlt">olivine</span> major element compositions we have determined in the CIs (Fig. 1) may now be directly com-pared with those of other astromaterials, including Wild 2 grains. The abundance of <span class="hlt">olivine</span> and low-Ca pyroxene in CIs is higher than is generally appreciated, and in fact much higher than for some CMs [1]. We also noted numerous rounded objects varying in shape from spheres to oblate spheroids, and ranging up to 100µm in size (Fig. 2), which have been previously noted [3] but have not been well documented or appreciated. We characterized the mineralogy by transmission electron microscopy and found that they consist mainly of rather fine-grained, flaky single phase to intergrown serpentine and saponite. These two materials in fact dominate the bulk of the host CI1 chondrites. With the exception of sparse spinels, the rounded phyllosilicate objects are remarka-bly free of other minerals, suggesting that the precursor from which the phyllosilicates were derived was a homogeneous mate-rial. We suggest that these round phyllosilicates aggregates in CI1 chondrites were cryptocrystalline to glassy microchondrules. If so then CI chondrites cannot be considered <span class="hlt">chondrule</span>-free. Small though they are, the abundance of these putative microchondrules is the same as that of <span class="hlt">chondrules</span> in the Tagish Lake meteorite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800065203&hterms=L37&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DL37','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800065203&hterms=L37&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DL37"><span>Chemical energy in cold-cloud aggregates - The origin of meteoritic <span class="hlt">chondrules</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Clayton, D. D.</p> <p>1980-01-01</p> <p>If interstellar particles and molecules accumulate into larger particles during the collapse of a cold cloud, the resulting aggregates contain a large store of internal chemical energy. It is here proposed that subsequent warming of these accumulates leads to a thermal runaway when exothermic chemical reactions begin within the aggregate. These, after cooling, are the crystalline <span class="hlt">chondrules</span> found so abundantly within chondritic meteorites. Chemical energy can also heat meteoritic parent bodies of any size, and both thermal metamorphism and certain molten meteorites are proposed to have occurred in this way. If this new theory is correct, (1) the model of chemical condensation in a hot gaseous solar system is eliminated, and (2) a new way of studying the chemical evolution of the interstellar medium has been found. A simple dust experiment on a comet flyby is proposed to test some features of this controversy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.4520P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.4520P"><span>Evidence of phase nucleation during <span class="hlt">olivine</span> diffusion creep: a new perspective for mantle strain localisation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Précigout, Jacques; Stünitz, Holger</p> <p>2017-04-01</p> <p>Mantle strain localisation is of great importance for lithosphere dynamics, but the cause for this phenomenon remains very elusive, particularly in conditions of the strong and ductile uppermost mantle. In these latter, grain size reduction leading to diffusion creep in <span class="hlt">olivine</span> is believed to be one of the best candidates to account for strain localisation. However, the mechanisms of grain size reduction in this regime are still poorly understood. Here we show the results of Griggs-type experiments that document grain size reduction and material weakening during wet <span class="hlt">olivine</span> diffusion creep at 900 °C and 1.2 GPa. While occurring for both, mono-phase and two-phase aggregates, grain size reduction is coeval with strain localisation and local phase mixing in <span class="hlt">olivine</span>-pyroxene aggregates. Based on evidence of fluid inclusions and cracks filled with a fine-grained phase mixture, we conclude that grain size reduces as a result of fluid-assisted nucleation. Cavitation induced by grain boundary sliding (creep cavitation) can be inferred, and may play a critical role for <span class="hlt">olivine</span> grain size reduction. Amongst their implications for rock rheology in general, our findings highlight a key process for strain localisation in the ductile uppermost mantle. This study has been published under the reference: "Précigout, J., and Stünitz, H. (2016) Evidence of phase nucleation during <span class="hlt">olivine</span> diffusion creep: a new perspective for mantle strain localisation. Earth and Planetary Science Letters 455: 94-105, doi:101016/j.epsl.2016.09.029".</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006GeCoA..70..206F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006GeCoA..70..206F"><span>Vapor pressures and evaporation coefficients for melts of ferromagnesian <span class="hlt">chondrule</span>-like compositions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fedkin, A. V.; Grossman, L.; Ghiorso, M. S.</p> <p>2006-01-01</p> <p>To determine evaporation coefficients for the major gaseous species that evaporate from silicate melts, the Hertz-Knudsen equation was used to model the compositions of residues of <span class="hlt">chondrule</span> analogs produced by evaporation in vacuum by Hashimoto [Hashimoto A. (1983) Evaporation metamorphism in the early solar nebula-evaporation experiments on the melt FeO-MgO-SiO 2-CaO-Al 2O 3 and chemical fractionations of primitive materials. Geochem. J. 17, 111-145] and Wang et al. [Wang J., Davis A. M., Clayton R. N., Mayeda T. K., Hashimoto A. (2001) Chemical and isotopic fractionation during the evaporation of the FeO-MgO-SiO 2-CaO-Al 2O 3-TiO 2 rare earth element melt system. Geochim. Cosmochim. Acta 65, 479-494], in vacuum and in H 2 by Yu et al. [Yu Y., Hewins R. H., Alexander C. M. O'D., Wang J. (2003) Experimental study of evaporation and isotopic mass fractionation of potassium in silicate melts. Geochim. Cosmochim. Acta 67, 773-786], and in H 2 by Cohen et al. [Cohen B. A., Hewins R. H., Alexander C. M. O'D. (2004) The formation of <span class="hlt">chondrules</span> by open-system melting of nebular condensates. Geochim. Cosmochim. Acta 68, 1661-1675]. Vapor pressures were calculated using the thermodynamic model of Ghiorso and Sack [Ghiorso M. S., Sack R. O. (1995) Chemical mass transfer in magmatic processes IV. A revised and internally consistent thermodynamic model for the interpolation and extrapolation of liquid-solid equilibria in magmatic systems at elevated temperatures and pressures. Contrib. Mineral. Petrol. 119, 197-212], except for the late, FeO-free stages of the Wang et al. (2001) and Cohen et al. (2004) experiments, where the CMAS activity model of Berman [Berman R. G. (1983) A thermodynamic model for multicomponent melts, with application to the system CaO-MgO-Al 2O 3-SiO 2. Ph.D. thesis, University of British Columbia] was used. From these vapor pressures, evaporation coefficients ( α) were obtained that give the best fits to the time variation of the residue compositions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR32A..08B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR32A..08B"><span>Constraints from Naturally Deformed Peridotites on Controls on <span class="hlt">Olivine</span> Lattice Preferred Orientation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bernard, R. E.; Behr, W. M.</p> <p>2016-12-01</p> <p>Seismic anisotropy in the upper mantle is produced primarily by lattice preferred orientations (LPO) in <span class="hlt">olivine</span> formed during viscous deformation. Because seismic anisotropy is one of the principal means of characterizing upper mantle flow directions, it is critical to understand how LPO is affected by deformation conditions. Laboratory experiments suggest that water content and stress magnitude each play key roles in the development of LPO in <span class="hlt">olivine</span> under experimental conditions, but it is unclear to what extent these results apply to natural conditions. We use peridotite xenoliths from a wide range of tectonic settings (Lunar Craters, Geronimo, and San Carlos volcanic fields in the Basin and Range; Cima and Deadman Lake volcanic fields in the Mojave; the Navajo Volcanic field in the Colorado Plateau; and the Potrillo volcanic field in the Rio Grande Rift region) to investigate correlations between water content, stress, and <span class="hlt">olivine</span> LPO in natural rocks. Water contents were measured using Secondary Ion Mass Spectrometry, stress magnitudes using paleopiezometry, and LPOs using electron backscatter diffraction. The samples examined exhibit a range of fabric types, including A-, B-, C-, and E-type LPOs. Mojave xenoliths show no difference in water content between A- and E-type LPO; instead, differences in fabric type appear to reflect variations in strain magnitude. Samples from the Navajo volcanic field do show a correlation between water influx and stress magnitude as they exhibit abundant hydrous minerals and high water contents, stress magnitudes greater than 250 MPa and B-type <span class="hlt">olivine</span> LPOs. Additional results from other xenolith suites will be presented at the meeting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013M%26PSA..76.5154S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013M%26PSA..76.5154S"><span>Multiple <span class="hlt">Olivine</span> Phase Transitions in the Shocked Martian Meteorite Tissint</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sharp, T. G.; Hu, J.; Walton, E. L.</p> <p>2013-09-01</p> <p>In some melt regions of Tissint <span class="hlt">olivine</span> dissociated into silicate perovskite + magnesiowüstite while in others it transformed into ringwoodite. These different reactions and reaction mechanisms can be explained by local temperature variations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1915509H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1915509H"><span>The nature of the lithosphere-asthenosphere boundary from laboratory investigations of <span class="hlt">olivine</span> anisotropy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, Lars; Qi, Chao; Warren, Jessica; Kohlstedt, David; Holtzman, Benjamin; Wallis, David</p> <p>2017-04-01</p> <p>The nature of the lithosphere-asthenosphere boundary (LAB) determines the mechanical coupling between rigid plates and the underlying convecting mantle. Seismological studies reveal distinct reflectors (G discontinuity) in the uppermost oceanic mantle that are sometimes interpreted as the LAB. The discontinuity in seismic velocity is suggested to arise from abrupt changes in composition, including the melt fraction. Interestingly, these reflectors roughly correlate with the location of discontinuities in radial seismic anisotropy, but do not correlate with the location of discontinuities in azimuthal anisotropy. To investigate the correlation between these datasets, we draw on recent laboratory measurements of crystallographic texture development in <span class="hlt">olivine</span>-rich rocks. The textural evolution of dry <span class="hlt">olivine</span> aggregates has been well described in recent experiments, while micromechanical models are available for incorporating these observations into larger-scale models of upper-mantle flow. Unfortunately, the systematics of textural evolution in melt-bearing <span class="hlt">olivine</span> aggregates have not been similarly described. Here we present a new experimental data set detailing the evolution of anisotropy during deformation of partially molten peridotite. Torsion experiments were conducted on samples composed of San Carlos <span class="hlt">olivine</span> and basaltic melt at a temperature of 1473 K and a confining pressure of 300 MPa. Seismically fast axes of <span class="hlt">olivine</span> tend to lie at a high angle to the flow direction in a manner similar to previous experiments. The anisotropy in these samples is weak compared to that in dry, melt-free <span class="hlt">olivine</span> deformed to similar strains. The anisotropy also exhibits relatively little change in strength and orientation with progressive deformation. Detailed microstructural analyses allow us to distinguish between competing models for the grain-scale deformation processes, favoring one in which crystallographically controlled grain shapes govern grain rotations. We</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ApJ...758...14K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ApJ...758...14K"><span>Gaseous Structures in <span class="hlt">Barred</span> Galaxies: Effects of the <span class="hlt">Bar</span> Strength</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Woong-Tae; Seo, Woo-Young; Kim, Yonghwi</p> <p>2012-10-01</p> <p>Using hydrodynamic simulations, we investigate the physical properties of gaseous substructures in <span class="hlt">barred</span> galaxies and their relationships with the <span class="hlt">bar</span> strength. The gaseous medium is assumed to be isothermal and unmagnetized. The <span class="hlt">bar</span> potential is modeled as a Ferrers prolate with index n. To explore situations with differing <span class="hlt">bar</span> strength, we vary the <span class="hlt">bar</span> mass f <span class="hlt">bar</span> relative to the spheroidal component as well as its aspect ratio { R}. We derive expressions as functions of f <span class="hlt">bar</span> and { R} for the <span class="hlt">bar</span> strength Qb and the radius r(Qb ) where the maximum <span class="hlt">bar</span> torque occurs. When applied to observations, these expressions suggest that <span class="hlt">bars</span> in real galaxies are most likely to have f <span class="hlt">bar</span> ~ 0.25-0.50 and n <~ 1. Dust lanes approximately follow one of the x 1-orbits and tend to be straighter under a stronger and more elongated <span class="hlt">bar</span>, but are insensitive to the presence of self-gravity. A nuclear ring of a conventional x 2 type forms only when the <span class="hlt">bar</span> is not so massive or elongated. The radius of an x 2-type ring is generally smaller than the inner Lindblad resonance, decreases systematically with increasing Qb , and is slightly larger when self-gravity is included. This is evidence that the ring position is not determined by the resonance, but instead by the amount of angular momentum loss at dust-lane shocks. Nuclear spirals exist only when the ring is of the x 2 type and is sufficiently large in size. Unlike the other features, nuclear spirals are transient in that they start out being tightly wound and weak, and then, due to the nonlinear effect, unwind and become stronger until they turn into shocks, with an unwinding rate that is higher for larger Qb . The mass inflow rate to the galaxy center is found to be less than 0.01 M ⊙ yr-1 for models with Qb <~ 0.2, while becoming larger than 0.1 M ⊙ yr-1 when Qb >~ 0.2 and self-gravity is included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Icar..280..328T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Icar..280..328T"><span><span class="hlt">Olivine</span> on Vesta as exogenous contaminants brought by impacts: Constraints from modeling Vesta's collisional history and from impact simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Turrini, D.; Svetsov, V.; Consolmagno, G.; Sirono, S.; Pirani, S.</p> <p>2016-12-01</p> <p>The survival of asteroid Vesta during the violent early history of the Solar System is a pivotal constraint on theories of planetary formation. Particularly important from this perspective is the amount of <span class="hlt">olivine</span> excavated from the vestan mantle by impacts, as this constrains both the interior structure of Vesta and the number of major impacts the asteroid suffered during its life. The NASA Dawn mission revealed that <span class="hlt">olivine</span> is present on Vesta's surface in limited quantities, concentrated in small patches at a handful of sites not associated with the two large impact basins Rheasilvia and Veneneia. The first detections were interpreted as the result of the excavation of endogenous <span class="hlt">olivine</span>, even if the depth at which the detected <span class="hlt">olivine</span> originated was a matter of debate. Later works raised instead the possibility that the <span class="hlt">olivine</span> had an exogenous origin, based on the geologic and spectral features of the deposits. In this work, we quantitatively explore the proposed scenario of a exogenous origin for the detected vestan <span class="hlt">olivine</span> to investigate whether its presence on Vesta can be explained as a natural outcome of the collisional history of the asteroid over the last one or more billion years. To perform this study we took advantage of the impact contamination model previously developed to study the origin and amount of dark and hydrated materials observed by Dawn on Vesta, a model we updated by performing dedicated hydrocode impact simulations. We show that the exogenous delivery of <span class="hlt">olivine</span> by the same impacts that shaped the vestan surface can offer a viable explanation for the currently identified <span class="hlt">olivine</span>-rich sites without violating the constraint posed by the lack of global <span class="hlt">olivine</span> signatures on Vesta. Our results indicate that no mantle excavation is in principle required to explain the observations of the Dawn mission and support the idea that the vestan crust could be thicker than indicated by simple geochemical models based on the Howardite</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRE..122.2702Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRE..122.2702Z"><span>Electrical Investigation of Metal-<span class="hlt">Olivine</span> Systems and Application to the Deep Interior of Mercury</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zhou; Pommier, Anne</p> <p>2017-12-01</p> <p>We report electrical conductivity measurements on metal-<span class="hlt">olivine</span> systems at about 5 and 6 GPa and up to 1,675°C in order to investigate the electrical properties of core-mantle boundary (CMB) systems. Electrical experiments were conducted in the multianvil apparatus using the impedance spectroscopy technique. The samples are composed of one metal layer (Fe, FeS, FeSi2, or Fe-Ni-S-Si) and one polycrystalline <span class="hlt">olivine</span> layer, with the metal:<span class="hlt">olivine</span> ratio ranging from 1:0.7 to 1:9.2. For all samples, we observe that the bulk electrical conductivity increases with temperature from 10-2.5 to 101.8 S/m, which is higher than the conductivity of polycrystalline <span class="hlt">olivine</span> but lower than the conductivity of the pure metal phase at similar conditions. In some experiments, a conductivity jump is observed at the temperature corresponding to the melting temperature of the metallic phase. Both the metal:<span class="hlt">olivine</span> ratio and the metal phase geometry control the electrical conductivity of the two-layer samples. By combining electrical results, textural analyses of the samples, and previous studies of the structure and composition of Mercury's interior, we propose an electrical profile of the deep interior of the planet that accounts for a layered CMB-outer core structure. The electrical model agrees with existing conductivity estimates of Mercury's lower mantle and CMB using magnetic observations and thermodynamic calculations, and thus, supports the hypothesis of a layered CMB-outermost core structure in the present-day interior of Mercury. We propose that the layered CMB-outer core structure is possibly electrically insulating, which may influence the planet's structure and cooling history.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25394792','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25394792"><span>Paleomagnetism. Solar nebula magnetic fields recorded in the Semarkona meteorite.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fu, Roger R; Weiss, Benjamin P; Lima, Eduardo A; Harrison, Richard J; Bai, Xue-Ning; Desch, Steven J; Ebel, Denton S; Suavet, Clément; Wang, Huapei; Glenn, David; Le Sage, David; Kasama, Takeshi; Walsworth, Ronald L; Kuan, Aaron T</p> <p>2014-11-28</p> <p>Magnetic fields are proposed to have played a critical role in some of the most enigmatic processes of planetary formation by mediating the rapid accretion of disk material onto the central star and the formation of the first solids. However, there have been no experimental constraints on the intensity of these fields. Here we show that dusty <span class="hlt">olivine</span>-bearing <span class="hlt">chondrules</span> from the Semarkona meteorite were magnetized in a nebular field of 54 ± 21 microteslas. This intensity supports <span class="hlt">chondrule</span> formation by nebular shocks or planetesimal collisions rather than by electric currents, the x-wind, or other mechanisms near the Sun. This implies that background magnetic fields in the terrestrial planet-forming region were likely 5 to 54 microteslas, which is sufficient to account for measured rates of mass and angular momentum transport in protoplanetary disks. Copyright © 2014, American Association for the Advancement of Science.</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/2017AGUFMMR41D0426J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR41D0426J"><span>Deformation Microstructures of the Yugu Peridotites in the Gyeonggi Massif, Korea: Implications for <span class="hlt">Olivine</span> Fabric Transition in Mantle Shear Zones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jung, H.; Park, M.</p> <p>2017-12-01</p> <p>Large-scale emplaced peridotite bodies may provide insights into plastic deformation process and tectonic evolution in the mantle shear zone. Due to the complexity of deformation microstructures and processes in natural mantle rocks, the evolution of pre-existing <span class="hlt">olivine</span> fabrics is still not well understood. In this study, we examine well-preserved transitional characteristics of microstructures and <span class="hlt">olivine</span> fabrics developed in a mantle shear zone from the Yugu peridotite body, the Gyeonggi Massif, Korean Peninsula. The Yugu peridotite body predominantly comprises spinel harzburgite together with minor lherzolite, dunite, and clinopyroxenite. We classified highly deformed peridotites into four textural types based on their microstructural characteristics: proto-mylonite; proto-mylonite to mylonite transition; mylonite; and ultra-mylonite. <span class="hlt">Olivine</span> fabrics changed from A-type (proto-mylonite) via D-type (mylonite) to E-type (ultra-mylonite). <span class="hlt">Olivine</span> fabric transition is interpreted as occurring under hydrous conditions at low temperature and high strain, because of characteristics such as Ti-clinohumite defects (and serpentine) and fluid inclusion trails in <span class="hlt">olivine</span>, and a hydrous mineral (pargasite) in the matrix, especially in the ultra-mylonitic peridotites. Even though the ultra-mylonitic peridotites contained extremely small (24-30 μm) <span class="hlt">olivine</span> neoblasts, the <span class="hlt">olivine</span> fabrics showed a distinct (E-type) pattern rather than a random one. Analysis of the lattice preferred orientation strength, dislocation microstructures, recrystallized grain-size, and deformation mechanism maps of <span class="hlt">olivine</span> suggest that the proto-mylonitic, mylonitic, and ultra-mylonitic peridotites were deformed by dislocation creep (A-type), DisGBS (D-type), and combination of dislocation and diffusion creep (E-type), respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080009736','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080009736"><span>Synchrotron X-Ray Diffraction Studies of <span class="hlt">Olivine</span> from Comet Wild 2</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2008-01-01</p> <p>We have analyzed a collection of the Comet Wild 2 coma grains returned by the NASA Stardust Mission, using micro-area Laue diffraction equipment. The purpose of the diffraction experiment is to permit the structure refinement of <span class="hlt">olivine</span> including site occupancies. In addition to the intrinsic importance of the <span class="hlt">olivine</span> structures for revealing the thermal history of Wild 2 materials, we wish to test reports that <span class="hlt">olivine</span> recovered after hypervelocity capture in silica aerogel has undergone a basic structural change due to capture heating [1]. The diffraction equipment placed at beam line BL- 4B1 of PF, KEK was developed with a micropinhole and an imaging plate (Fuji Co. Ltd.) using the Laue method combined with polychromatic X-ray of synchrotron radiation operated at energy of 2.5 GeV. The incident beam is limited to 1.6 m in diameter by a micropinhole set just upstream of the sample [2, 3]. It is essential to apply a microbeam to obtain diffracted intensities with high signal to noise ratios. This equipment has been successfully applied to various extraterrestrial materials, including meteorites and interplanetary dust particles [4]. The Laue pattern of the sample C2067,1,111,4 (Fig. 1) was successfully taken on an imaging plate after a 120 minute exposure (Fig. 2).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MinPe.tmp...91M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MinPe.tmp...91M"><span>Petrogenesis of ultramafic rocks and <span class="hlt">olivine</span>-rich troctolites from the East Taiwan Ophiolite in the Lichi mélange</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morishita, Tomoaki; Ghosh, Biswajit; Soda, Yusuke; Mizukami, Tomoyuki; Tani, Ken-ichiro; Ishizuka, Osamu; Tamura, Akihiro; Komaru, Chihiro; Aari, Shoji; Yang, Hsiao-Chin; Chen, Wen-Shan</p> <p>2017-12-01</p> <p>We examine ultramafic and <span class="hlt">olivine</span>-rich troctolite blocks of the East Taiwan Ophiolite (ETO) in the Lichi Mélange. Although ultramafic rocks are extensively serpentinized, the primary minerals, such as <span class="hlt">olivine</span>, orthopyroxene, clinopyroxene, spinel and plagioclase can be identified. The ultramafic rocks are classified into harzburgite (± clinopyroxene), dunite, and <span class="hlt">olivine</span> websterite. Major and trace element compositions of the primary minerals in harzburgites, such as the Cr# [= Cr/(Cr + Al) atomic ratio] of chromian spinel (0.3-0.58) and incompatible elements-depleted trace element patterns of clinopyroxenes, indicate their residue origin after partial melting with less flux components. These compositions are similar to those from mid-ocean ridge peridotites as well as back-arc peridotites from the Philippine Sea Plate. The <span class="hlt">olivine</span> websterite contains discrete as well as occasional locally concentrated plagioclase grains. Petrological characteristics coupled with similarity in trace element patterns of clinopyroxenes in the harzburgite and <span class="hlt">olivine</span> websterite samples indicate that the <span class="hlt">olivine</span> websterite is likely formed by clinopyroxene addition to a lherzolitic/harzburgitic peridotite from a pyroxene-saturated mafic melt. Dunite with medium Cr# spinels indicates cumulus or replacement by melt-peridotite reaction origins. Mineral composition of <span class="hlt">olivine</span>-rich troctolite cannot be explained by simple crystallization from basaltic magmas, but shows a chemical trend expected for products after melt-peridotite interactions. Mineral compositions of the dunite and <span class="hlt">olivine</span>-rich troctolite are also within chemical ranges of mid-ocean ridge samples, and are slightly different from back-arc samples from the Philippine Sea Plate. We conclude that peridotites in the ETO are not derived from the northern extension of the Luzon volcanic arc mantle. Further geochronological study is, however, required to constrain the origin of the ETO ophiolite, because peridotites are probably</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140012962','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140012962"><span>Experimental Constraints on a Vesta Magma Ocean</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hoff, C.; Jones, J. H.; Le, L.</p> <p>2014-01-01</p> <p>A magma ocean model was devised to relate eucrites (basalts) and diogenites (orthopyroxenites), which are found mixed together as clasts in a suite of polymict breccias known as howardites. The intimate association of eucritic and diogenitic clasts in howardites argues strongly that these three classes of achondritic meteorites all originated from the same planetoid. Reflectance spectral evidence (including that from the DAWN mission) has long suggested that Vesta is indeed the Eucrite Parent Body. Specifically, the magma ocean model was generated as follows: (i) the bulk Vesta composition was taken to be 0.3 CV chondrite + 0.7 L chondrite but using only 10% of the Na2O from this mixture; (ii) this composition is allowed to crystallize at 500 <span class="hlt">bar</span> until approx. 80% of the system is solid <span class="hlt">olivine</span> + low-Ca pyroxene; (iii) the remaining 20% liquid crystallizes at one <span class="hlt">bar</span> from 1250C to 1110C, a temperature slightly above the eucrite solidus. All crystallization calculations were performed using MELTS. In this model, diogenites are produced by cocrystallization of <span class="hlt">olivine</span> and pyroxene in the >1250C temperature regime, with Main Group eucrite liquids being generated in the 1300-1250C temperature interval. Low-Ca pyroxene reappears at 1210C in the one-<span class="hlt">bar</span> calculations and fractionates the residual liquid to produce evolved eucrite compositions (Stannern Trend). We have attempted to experimentally reproduce the <1250C portion of the MELTS Vesta magma ocean. In the MELTS calculation, the change from 500 <span class="hlt">bar</span> to one <span class="hlt">bar</span> results in a shift of the <span class="hlt">olivine</span>:low-Ca pyroxene boundary so that the 1250C liquid is now in the <span class="hlt">olivine</span> field and, consequently, <span class="hlt">olivine</span> should be the first-crystallizing phase, followed by low-Ca pyroxene at 1210C, and plagioclase at 1170C. Because at one <span class="hlt">bar</span> the <span class="hlt">olivine</span>:low-Ca pyroxene boundary is a peritectic, fractional crystallization of the 1210C liquid proceeds with only pyroxene crystallization until plagioclase appears. Thus, the predictions of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR41D0424Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR41D0424Z"><span>Grain Boundary Sliding in <span class="hlt">Olivine</span> + Clinopyroxene Aggregates: Weakening Mechanism and Microstructure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, N.; Hirth, G.; Cooper, R. F.; Kruckenberg, S. C.</p> <p>2017-12-01</p> <p>Constraining the viscosity of <span class="hlt">olivine</span>-rich aggregates is critical for modeling geodynamic processes in the upper mantle. The presence of pyroxenes can complicate the rheology of mantle rocks owing to heterogeneous phase boundary properties and the potential impacts of incompatible elements on interface viscosity. Thus, in the grain boundary sliding (GBS) regime, it may be inappropriate to extrapolate flow laws of end-member aggregates to predict the behavior of multiphase aggregates. We deformed mixtures of fine-grained <span class="hlt">olivine</span> (Ol) and clinopyroxene (Cpx) with various phase ratios in a general shear geometry at a confining pressure of 1.5 GPa, 1100-1200ºC and strain rate of 10­-3-10-5 s-1 to shear strains up to 8.5. We observed a peak stress followed by weakening in each experiment (except for those at 1200ºC), yet at steady state Ol-Cpx samples are substantially weaker than either pure Ol or pure Cpx end members scaled to the same grain size. Flow law parameters are quantified and indicate that the dominant deformation mechanism is reaction-limited diffusional creep. In addition, the results are consistent with a microphysical model that does not require the diffusion of Si (Sundberg & Cooper, 2008), providing an explanation for the observed weakening of <span class="hlt">olivine</span> and pyroxene aggregates. <span class="hlt">Olivine</span> exhibits an axial-[010] fabric or a B-type fabric. Analysis of low-angle (2º-10º) boundary axes indicate the activation of (010)[100] slip system, but no evidence for activation of the (010)[001] slip system that is hypothesized to generate a B-type fabric by dislocation creep. In the samples with strong fabric, we sorted the grains by their grain orientation spread (GOS, a measurement of how substructured the grain is or how active the dislocations were in the grain). The low-GOS grains have smaller grain sizes, smaller aspect ratios and weaker shape preferred orientation compared to high-GOS grains. Yet, low-GOS grains also have the strongest B-type fabric, while</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AAS...22120601K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AAS...22120601K"><span>Effects of the <span class="hlt">Bar</span> Strength of Gaseous Features in <span class="hlt">Barred</span> Galaxies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Woong-Tae; Seo, W.; Kim, Y.</p> <p>2013-01-01</p> <p><span class="hlt">Barred</span> galaxies commonly possess gaseous structures such as a pair of dust lanes, a nuclear ring, and nuclear spirals at their centers. We use hydrodynamic simulations to study the physical properties of the gaseous structures in <span class="hlt">barred</span> galaxies and their relationships with the <span class="hlt">bar</span> strength. We vary the <span class="hlt">bar</span> mass fbar relative to the spheroidal component as well as its aspect ratio. We derive expressions for the <span class="hlt">bar</span> strength Qb and the radius where the maximum <span class="hlt">bar</span> torque occurs. When applied to observations, these expressions suggest that <span class="hlt">bars</span> in real galaxies are most likely to have fbar = 0.25-0.5. Dust lanes approximately follow one of x1-orbits and tend to be more straight under a stronger and more elongated <span class="hlt">bar</span>. A nuclear ring of a conventional x2 type forms only when the <span class="hlt">bar</span> is not so massive or elongated. The radius of an x2-type ring is generally smaller than the inner Lindblad resonance, decreases systematically with increasing Qb, evidencing that the ring position is not determined by the resonance but by the <span class="hlt">bar</span> strength. Nuclear spirals exist only when the ring is of the x2-type and sufficiently large in size. Unlike the other features, nuclear spirals are transient in that they start out as being tightly-wound and weak, and then due to the nonlinear effect unwind and become stronger until turning into shocks, with an unwinding rate higher for larger Qb. These results suggest that the <span class="hlt">bar</span> strength is the primary factor that determine the properties of gaseous structures in <span class="hlt">barred</span> galaxies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFMMR14A..07L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFMMR14A..07L"><span>Hydrogen Incorporation into <span class="hlt">Olivine</span> at 9-15 GPa: Implication for Water Dynamics near the 410-km Seismic Discontinuity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Litasov, K.; Ohtani, E.; Kagi, H.; Shatskiy, A.; Ghosh, S.; Lakshtanov, D.; Bass, J.; Matveev, S.</p> <p>2006-12-01</p> <p>The hydrogen solubility and hydrogen incorporation mechanism into (Mg,Fe)2SiO4 <span class="hlt">olivine</span> have been studied at pressures of 9-15 GPa and temperatures of 1100-2000°C. Samples were synthesized using a multianvil apparatus from Fo90 + 4-15 wt.% H2O mixture without controlling oxygen fugacity. Also, pure forsterite crystals were synthesized in KHCO3-Mg(OH)2 flux. Samples were studied by Fourier Transform Infrared spectroscopy (FTIR) and H (H2O) contents were calculated from IR spectra using the calibration by Bell et al. (2003). The hydrogen solubility increases with pressure, but the temperature dependence is complex. The hydrogen solubility increases from 1100-1400°C and then decreases at 1400-2000°C. Maximum hydrogen solubility, equivalent to 1.15 wt.% H2O, was determined in <span class="hlt">olivine</span> at 13.5 GPa and 1400°C. At temperatures of 1800-2000°C the H2O contents of <span class="hlt">olivine</span> are very low (280-590 ppm). Hydrogen solubility in Fo90 is consistent with that in pure forsterite studied by Lemaire et al. (2004) and Smyth et al. (2006) indicating minor influence of Fe on hydrogen incorporation. The IR spectra of <span class="hlt">olivines</span> are composed of several OH absorption bands at 3300-3613 cm-1. IR spectra with the E-field vector parallel to the a-axis show the strongest absorbance, dominated by peaks at 3613 and 3579 cm-1. Although structural calculations are consistent with hydrogen incorporation into octahedral vacancies in <span class="hlt">olivine</span> (e.g. Smyth et al., 2006; Kudoh et al., 2006) we strongly suggest that majority of observed peaks (at 3533, 3548, 3566, 3579, and 3613 cm-1) are due to hydrogen associated with Si- vacancies. This is consistent with microprobe analyses of the samples, which show a clear deficit of Si in <span class="hlt">olivines</span> at the highest H2O-contents. Minor bands at 3300-3400 cm-1 may be due to Fe3+ substitution and those at 3400-3500 cm-1 due to vacancies in Mg structural positions. The peak at 3598 cm-1 previously attributed to Mg-vacancies should be addressed to Si-vacancies. The strongest</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ERL.....8a4009K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ERL.....8a4009K"><span>Geoengineering impact of open ocean dissolution of <span class="hlt">olivine</span> on atmospheric CO2, surface ocean pH and marine biology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Köhler, Peter; Abrams, Jesse F.; Völker, Christoph; Hauck, Judith; Wolf-Gladrow, Dieter A.</p> <p>2013-03-01</p> <p>Ongoing global warming induced by anthropogenic emissions has opened the debate as to whether geoengineering is a ‘quick fix’ option. Here we analyse the intended and unintended effects of one specific geoengineering approach, which is enhanced weathering via the open ocean dissolution of the silicate-containing mineral <span class="hlt">olivine</span>. This approach would not only reduce atmospheric CO2 and oppose surface ocean acidification, but would also impact on marine biology. If dissolved in the surface ocean, <span class="hlt">olivine</span> sequesters 0.28 g carbon per g of <span class="hlt">olivine</span> dissolved, similar to land-based enhanced weathering. Silicic acid input, a byproduct of the <span class="hlt">olivine</span> dissolution, alters marine biology because silicate is in certain areas the limiting nutrient for diatoms. As a consequence, our model predicts a shift in phytoplankton species composition towards diatoms, altering the biological carbon pumps. Enhanced <span class="hlt">olivine</span> dissolution, both on land and in the ocean, therefore needs to be considered as ocean fertilization. From dissolution kinetics we calculate that only <span class="hlt">olivine</span> particles with a grain size of the order of 1 μm sink slowly enough to enable a nearly complete dissolution. The energy consumption for grinding to this small size might reduce the carbon sequestration efficiency by ˜30%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12016311','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12016311"><span>Seismic evidence for <span class="hlt">olivine</span> phase changes at the 410- and 660-kilometer discontinuities.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lebedev, Sergei; Chevrot, Sébastien; van der Hilst, Rob D</p> <p>2002-05-17</p> <p>The view that the seismic discontinuities bounding the mantle transition zone at 410- and 660-kilometer depths are caused by isochemical phase transformations of the <span class="hlt">olivine</span> structure is debated. Combining converted-wave measurements in East Asia and Australia with seismic velocities from regional tomography studies, we observe a correlation of the thickness of, and wavespeed variations within, the transition zone that is consistent with <span class="hlt">olivine</span> structural transformations. Moreover, the seismologically inferred Clapeyron slopes are in agreement with the mineralogical Clapeyron slopes of the (Mg,Fe)2SiO4 spinel and postspinel transformations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011GeCoA..75.7612B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011GeCoA..75.7612B"><span>Temperature dependence of sulfide and sulfate solubility in <span class="hlt">olivine</span>-saturated basaltic magmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Beermann, O.; Botcharnikov, R. E.; Holtz, F.; Diedrich, O.; Nowak, M.</p> <p>2011-12-01</p> <p>The sulfur concentration at pyrrhotite- and anhydrite-saturation in primitive hydrous basaltic melt of the 2001-2002 eruption of Mt. Etna was determined at 200 MPa, T = 1050-1250 °C and at log fO 2 from FMQ to FMQ+2.2 (FMQ is Fayalite-Magnetite-Quartz oxygen buffer). At 1050 °C Au sample containers were used. A double-capsule technique, using a single crystal <span class="hlt">olivine</span> sample container closed with an <span class="hlt">olivine</span> piston, embedded in a sealed Au 80Pd 20 capsule, was developed to perform experiments in S-bearing hydrous basaltic systems at T > 1050 °C. Pyrrhotite is found to be a stable phase coexisting with melt at FMQ-FMQ+0.3, whereas anhydrite is stable at FMQ+1.4-FMQ+2.2. The S concentration in the melt increases almost linearly from 0.12 ± 0.01 to 0.39 ± 0.02 wt.% S at FeS-saturation and from 0.74 ± 0.01 to 1.08 ± 0.04 wt.% S at anhydrite-saturation with T ranging from 1050-1250 °C. The relationships between S concentration at pyrrhotite and/or anhydrite saturation, MgO content of the <span class="hlt">olivine</span>-saturated melt, T, and log fO 2 observed in this study and from previous data are used to develop an empirical model for estimating the magmatic T and fO 2 from the S and MgO concentrations of H 2O-bearing <span class="hlt">olivine</span>-saturated basaltic melts. The model can also be used to determine maximum S concentrations, if fO 2 and MgO content of the melt are known. The application of the model to compositions of melt inclusions in <span class="hlt">olivines</span> from Mt. Etna indicates that the most primitive magmas trapped in inclusions might have been stored at log fO 2 slightly higher than FMQ+1 and at T = 1100-1150 °C, whereas more evolved melts could have been trapped at T ⩽ 1100 °C. These values are in a good agreement with the estimates obtained by other independent methods reported in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790063561&hterms=ionic+liquid&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dionic%2Bliquid','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790063561&hterms=ionic+liquid&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dionic%2Bliquid"><span>The solubility of <span class="hlt">olivine</span> in basaltic liquids - An ionic model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Herzberg, C. T.</p> <p>1979-01-01</p> <p>A model is presented which enables the temperature at which <span class="hlt">olivine</span> is in equilibrium with any alkali-depleted basaltic compound to be calculated to within + or - 30 C. It is noted that the error increases substantially when applied to terrestrial basalts which contain several weight percent alkalis. In addition the model predicts and quantifies the reduced activity of SiO4(4-) monomers due to increasing SiO2 concentrations in the melt. It is shown that the coordination of alumina in melts which precipitate <span class="hlt">olivine</span> only appears to be dominantly octahedral, while titanium acts as a polmerizing agent by interconnecting previously isolated SiO4(4-) monomers. It is concluded that the model is sufficiently sensitive to show that there are small repulsive forces between Mg(2+) and calcium ions which are in association with normative diopside in the melt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Icar..300..287C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Icar..300..287C"><span><span class="hlt">Olivine</span>-bearing lithologies on the Moon: Constraints on origins and transport mechanisms from M3 spectroscopy, radiative transfer modeling, and GRAIL crustal thickness</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Corley, Laura M.; McGovern, Patrick J.; Kramer, Georgiana Y.; Lemelin, Myriam; Trang, David; Gillis-Davis, Jeffrey J.; Taylor, G. Jeffrey; Powell, Kathryn E.; Kiefer, Walter S.; Wieczorek, Mark; Zuber, Maria T.</p> <p>2018-01-01</p> <p>High-resolution hyperspectral data from Chandrayaan-1's Moon Mineralogy Mapper (M3) allow detection of <span class="hlt">olivine</span> on the lunar surface. <span class="hlt">Olivine</span> exposed at the surface may originate as mantle material or igneous products (intrusive or extrusive). Potential transport mechanisms include excavation of the mantle or lower crustal material by impacts that form basins and complex craters, differentiation of impact melt sheets, or magmatic emplacement of lavas, cumulates, or xenoliths. A sample of the lunar mantle, which has not been conclusively identified in the lunar sample collection, would yield fundamental new insights into the composition, structure, and evolution of the lunar interior. <span class="hlt">Olivine</span> identified in remote spectral data is generally accepted to originate from the primary mantle, because abundant <span class="hlt">olivine</span> is expected to exist in the mantle and lower crust, yet have sparse occurrences in the upper crust. In this study, we identified 111 M3 single-pixel spectra with characteristic absorption features consistent with <span class="hlt">olivine</span> at Crisium, Nectaris, and Humorum basins and near the craters Roche and Tsiolkovsky. In an effort to determine the origins and transport mechanisms that led to these individual exposures, we estimated mineral abundances using radiative transfer modeling and examined crustal thickness estimates, topography and slope maps, and images from the Lunar Reconnaissance Orbiter Camera (LROC). At Crisium basin, where crustal thickness is near 0 km (Wieczorek et al., 2013), mantle <span class="hlt">olivine</span> may have been exposed by basin-forming impact and deposited on the rim. Picard crater, which is superposed on the floor of Crisium, also exhibits potential mantle <span class="hlt">olivine</span> in its ejecta. Within Nectaris basin, <span class="hlt">olivine</span> exposures are confined to the rims of small craters on the mare, which are inferred to excavate a layer of <span class="hlt">olivine</span>-rich mare basalt. <span class="hlt">Olivine</span> occurrences on the rim of Humorum basin, including those located on a graben, are likely to be cumulates of shallow</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.V23B2978S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.V23B2978S"><span>Lithium Zoning in Kīlauea <span class="hlt">Olivine</span>: Growth vs. Diffusion?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shea, T.; Lynn, K. J.; Garcia, M. O.; Costa Rodriguez, F.</p> <p>2016-12-01</p> <p>Lithium is a fast-diffusing element with the potential to characterize magmatic processes that occur on timescales of hours to days [1]. However, Li diffusion in <span class="hlt">olivine</span> is complex. Experimental studies show that it can diffuse via two paths: a `fast' interstitial mechanism and a `slow' vacancy mechanism [1]. Charge balancing relationships with other incompatible trace elements may also play a role in Li diffusion [2]. A detailed study of lithium zoning in natural <span class="hlt">olivine</span> was undertaken to better understand how Li is correlated with other trace elements and determine if Li diffusion profiles can be used to extract meaningful timescales of magmatic processes. <span class="hlt">Olivine</span> crystals from the Keanakāko`i explosive period at Kīlauea Volcano (HI) were used in this study because (a) the lavas and tephra generally contain phenocrysts of only <span class="hlt">olivine</span> in a rapidly quenched glass, which avoid complications of multi-phase systems and post-eruptive diffusion; (b) we previously constrained the magmatic histories of these crystals using major and minor elements; and (c) at concentrations (e.g. 1-10 ppm) and temperatures (e.g. 1150-1250 °C) typical of Kīlauea basalts, Li diffusion is probably dominated by the vacancy mechanism [1]. Euhedral crystals were carefully oriented and mounted on either the a- or b- crystallographic axes (c-axis is always within the plane of section) and polished to the crystal core. High precision LA-ICP-MS analyses of Li (2σ = 0.08 ppm), Na, Al, P, and Cr complement EPMA profiles of Si, Mg, Fe, Ni, and Ca (200 nA current). Core-to-rim transects were collected along two axes (c and a or b) to identify potential diffusion anisotropy effects for Li and other elements. Li zoning is correlated with Na, indicative of a growth signature (also observed for Al, P, and Cr), or is decoupled from incompatible trace elements and have profiles that indicate diffusive re-equilibration. Modeling of Li diffusion profiles yields timescales of hours to days, which probably</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI51A0291B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI51A0291B"><span>Assessing δ18O heterogeneity in Icelandic <span class="hlt">olivine</span> crystals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bar Rasmussen, M.; Halldorsson, S. A.; Martin, W.; Gibson, S. A.; Hilton, D. R.</p> <p>2017-12-01</p> <p>δ18O systematics of Icelandic basalts are notably distinct from MORB-sourced basalts. This difference has previously been attributed to interaction with low δ18O meteoric water in the crust or slight heterogeneity within the Icelandic mantle [1]. Studies addressing this issue have mostly involved batch mineral laser-fluorination analysis which cannot resolve any intra-mineral δ18O variability that might be present due to shallow-level processes, e.g. crustal contamination [2]. We present a study of <span class="hlt">olivine</span> crystals found in basalts covering the neovolcanic rift and flank zones as well as older Tertiary crust, in which we couple in-situ δ18O-measurements with major and trace elements using SIMS, high-precision EMP and LA ICP-MS. Most samples have previously been analysed for 3He/4He which ranges from 6.7 to 47.8 RA, the largest span reported for any oceanic island [3]. Our analysed <span class="hlt">olivine</span> grains, range in Fo# between 79.9 to 91.8 with limited intra-grain variability. Independent of Fo#, we observe a variation in δ18O(Ol) of >3 ‰ across Iceland, with most crystals plotting below the expected depleted mantle-value ( 5.1 ± 0.2‰ [4]). The lowest δ18O(Ol) of +2.77 ‰, is found in crystals with Fo# 86 from central Iceland, closest to the inferred plume head [3]. Trace element ratios for these <span class="hlt">olivine</span> grains (e.g. Zn/Fe) strongly indicate a peridotitic mantle source, which implies a shallow (likely crustal) origin of low δ18O(Ol) for this region. In contrast, <span class="hlt">olivine</span> crystals from the South Iceland Volcanic Zone (a region of active rift propagation and transitional to alkalic volcanism) display trace element ratios that are indicative of a greater amount of pyroxenite in their melt source region. The δ18O(Ol) of these samples vary significantly (from +3.45 to +4.98 ‰) which, together with their elevated 3He/4He values, implies entrainment of a lower δ18O mantle-source by a less-degassed mantle plume source. Further modelling will be performed to evaluate</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.1698S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.1698S"><span><span class="hlt">Olivine</span> dissolution in the presence of heterotrophic bacteria (Pseudomonas reactants) extracted from Icelandic groundwater of the CO2 injection pilot site</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shirokova, Liudmila; Pokrovsky, Oleg; Benezeth, Pascale; Gerard, Emmanuelle; Menez, Benedicte; Alfredsson, Helgi</p> <p>2010-05-01</p> <p>This work is aimed at experimental modeling of the effect of heterotrophic bacteria on dissolution of important rock-forming mineral, <span class="hlt">olivine</span>, at the conditions of CO2 storage and sequestration. Heterotrophic aerobic gram-negative bacteria were extracted from deep underground water (HK31, 1700 m deep and, t = 25-30°C) of basaltic aquifer located within the Hellisheidi CO2 injection pilot site (Iceland). Following this sampling, we separated, using culture on nutrient agar plates, four different groups of gram-negative aerobic bacteria. The enzymatic activity of studied species has been evaluated using Biolog Ecoplates and their genetic identification was performed using 18-S RNA analysis. The optimal growth conditions of bacteria on Brain Hearth Broth nutrient have been determined as 5 to 37°C and growth media pH varied from 7.0-8.2. Culturing experiments allowed determining the optimal physico-chemical conditions for bacteria experiments in the presence of basic Ca, Mg-containing silicates. <span class="hlt">Olivine</span> (Fo92) was chosen as typical mineral of basalt, widely considered in carbon dioxide sequestration mechanisms. Dissolution experiments were performed in constant-pH (7 to 9), bicarbonate-buffered (0.001 to 0.05 M) nutrient-diluted media in batch reactors at 0-30 <span class="hlt">bars</span> of CO2 in the presence of various biomass of Pseudomonas reactants. The release rate of magnesium, silica and iron was measured as a function of time in the presence of live, actively growing, dead (autoclaved or glutaraldehyde-treated) cells and bacteria exometabolites. Both nutrient media diluted 10 times (to 100 mg DOC/L) and inert electrolyte (NaCl, no DOC) were used. Our preliminary results indicate that the pH and dissolved organic matter are the first-order parameters that control the element release from <span class="hlt">olivine</span> at far from equilibrium conditions. The SEM investigation of reacted surfaces reveal formation of surface roughness with much stronger mineral alteration in the presence of live bacteria</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22912685','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22912685"><span><span class="hlt">Olivine</span> weathering in soil, and its effects on growth and nutrient uptake in Ryegrass (Lolium perenne L.): a pot experiment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>ten Berge, Hein F M; van der Meer, Hugo G; Steenhuizen, Johan W; Goedhart, Paul W; Knops, Pol; Verhagen, Jan</p> <p>2012-01-01</p> <p>Mineral carbonation of basic silicate minerals regulates atmospheric CO(2) on geological time scales by locking up carbon. Mining and spreading onto the earth's surface of fast-weathering silicates, such as <span class="hlt">olivine</span>, has been proposed to speed up this natural CO(2) sequestration ('enhanced weathering'). While agriculture may offer an existing infrastructure, weathering rate and impacts on soil and plant are largely unknown. Our objectives were to assess weathering of <span class="hlt">olivine</span> in soil, and its effects on plant growth and nutrient uptake. In a pot experiment with perennial ryegrass (Lolium perenne L.), weathering during 32 weeks was inferred from bioavailability of magnesium (Mg) in soil and plant. <span class="hlt">Olivine</span> doses were equivalent to 1630 (OLIV1), 8150, 40700 and 204000 (OLIV4) kg ha(-1). Alternatively, the soluble Mg salt kieserite was applied for reference. <span class="hlt">Olivine</span> increased plant growth (+15.6%) and plant K concentration (+16.5%) in OLIV4. At all doses, <span class="hlt">olivine</span> increased bioavailability of Mg and Ni in soil, as well as uptake of Mg, Si and Ni in plants. <span class="hlt">Olivine</span> suppressed Ca uptake. Weathering estimated from a Mg balance was equivalent to 240 kg ha(-1) (14.8% of dose, OLIV1) to 2240 kg ha(-1) (1.1%, OLIV4). This corresponds to gross CO(2) sequestration of 290 to 2690 kg ha(-1) (29 10(3) to 269 10(3) kg km(-2).) Alternatively, weathering estimated from similarity with kieserite treatments ranged from 13% to 58% for OLIV1. The Olsen model for <span class="hlt">olivine</span> carbonation predicted 4.0% to 9.0% weathering for our case, independent of <span class="hlt">olivine</span> dose. Our % values observed at high doses were smaller than this, suggesting negative feedbacks in soil. Yet, weathering appears fast enough to support the 'enhanced weathering' concept. In agriculture, <span class="hlt">olivine</span> doses must remain within limits to avoid imbalances in plant nutrition, notably at low Ca availability; and to avoid Ni accumulation in soil and crop.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3415406','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3415406"><span><span class="hlt">Olivine</span> Weathering in Soil, and Its Effects on Growth and Nutrient Uptake in Ryegrass (Lolium perenne L.): A Pot Experiment</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>ten Berge, Hein F. M.; van der Meer, Hugo G.; Steenhuizen, Johan W.; Goedhart, Paul W.; Knops, Pol; Verhagen, Jan</p> <p>2012-01-01</p> <p>Mineral carbonation of basic silicate minerals regulates atmospheric CO2 on geological time scales by locking up carbon. Mining and spreading onto the earth's surface of fast-weathering silicates, such as <span class="hlt">olivine</span>, has been proposed to speed up this natural CO2 sequestration (‘enhanced weathering’). While agriculture may offer an existing infrastructure, weathering rate and impacts on soil and plant are largely unknown. Our objectives were to assess weathering of <span class="hlt">olivine</span> in soil, and its effects on plant growth and nutrient uptake. In a pot experiment with perennial ryegrass (Lolium perenne L.), weathering during 32 weeks was inferred from bioavailability of magnesium (Mg) in soil and plant. <span class="hlt">Olivine</span> doses were equivalent to 1630 (OLIV1), 8150, 40700 and 204000 (OLIV4) kg ha−1. Alternatively, the soluble Mg salt kieserite was applied for reference. <span class="hlt">Olivine</span> increased plant growth (+15.6%) and plant K concentration (+16.5%) in OLIV4. At all doses, <span class="hlt">olivine</span> increased bioavailability of Mg and Ni in soil, as well as uptake of Mg, Si and Ni in plants. <span class="hlt">Olivine</span> suppressed Ca uptake. Weathering estimated from a Mg balance was equivalent to 240 kg ha−1 (14.8% of dose, OLIV1) to 2240 kg ha−1 (1.1%, OLIV4). This corresponds to gross CO2 sequestration of 290 to 2690 kg ha−1 (29 103 to 269 103 kg km−2.) Alternatively, weathering estimated from similarity with kieserite treatments ranged from 13% to 58% for OLIV1. The Olsen model for <span class="hlt">olivine</span> carbonation predicted 4.0% to 9.0% weathering for our case, independent of <span class="hlt">olivine</span> dose. Our % values observed at high doses were smaller than this, suggesting negative feedbacks in soil. Yet, weathering appears fast enough to support the ‘enhanced weathering’ concept. In agriculture, <span class="hlt">olivine</span> doses must remain within limits to avoid imbalances in plant nutrition, notably at low Ca availability; and to avoid Ni accumulation in soil and crop. PMID:22912685</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015DokES.465.1168T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015DokES.465.1168T"><span>Composition of primary fluid and melt inclusions in regenerated <span class="hlt">olivines</span> from hypabyssal kimberlites of the Malokuonapskaya pipe (Yakutia)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tomilenko, A. A.; Kuzmin, D. V.; Bulbak, T. A.; Timina, T. Yu.; Sobolev, N. V.</p> <p>2015-11-01</p> <p>The primary fluid and melt inclusions in regenerated zonal crystals of <span class="hlt">olivine</span> from kimberlites of the Malokuonapskaya pipe were first examined by means of microthermometry, optic and scanning electron microscopy, and Raman spectroscopy. The high-pressure genesis of homogenous central parts of the <span class="hlt">olivines</span> was revealed, probably under intense metasomatism at early hypogene stages with subsequent regeneration in the kimberlitic melt. The <span class="hlt">olivine</span> crystals were regenerated from silicate-carbonate melts at about 1100°C. The composition of the kimberlitic melt was changed by way of an increase in the calcium content.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890049160&hterms=Ultrafine+particles&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DUltrafine%2Bparticles','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890049160&hterms=Ultrafine+particles&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DUltrafine%2Bparticles"><span>Ultrafine-grained mineralogy and matrix chemistry of <span class="hlt">olivine</span>-rich chondritic interplanetary dust particles</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rietmeijer, F. J. M.</p> <p>1989-01-01</p> <p><span class="hlt">Olivine</span>-rich chondritic interplanetary dust particles (IDPs) are an important subset of fluffy chondritic IDPs collected in the earth's stratosphere. Particles in this subset are characterized by a matrix of nonporous, ultrafine-grained granular units. Euhedral single crystals, crystals fragments, and platey single crystals occur dispersed in the matrix. Analytical electron microscopy of granular units reveals predominant magnesium-rich <span class="hlt">olivines</span> and FeNi-sulfides embedded in amorphous carbonaceous matrix material. The variable ratio of ultrafine-grained minerals vs. carbonaceous matrix material in granular units support variable C/Si ratios, and some fraction of sulfur is associated with carbonaceous matrix material. The high Mg/(Mg+Fe) ratios in granular units is similar to this distribution in P/Comet Halley dust. The chondritic composition of fine-grained, polycrystalline IDPs gradually breaks down into nonchondritic, and ultimately, single mineral compositions as a function of decreased particle mass. The relationship between particle mass and composition in the matrix of <span class="hlt">olivine</span>-rich chondritic IDPs is comparable with the relationship inferred for P/Comet Halley dust.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR23A2677W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR23A2677W"><span>The impact of water on dislocation content and slip system activity in <span class="hlt">olivine</span> constrained by HR-EBSD and visco-plastic self-consistent simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wallis, D.; Hansen, L. N.; Tasaka, M.; Kumamoto, K. M.; Lloyd, G. E.; Parsons, A. J.; Kohlstedt, D. L.; Wilkinson, A. J.</p> <p>2016-12-01</p> <p>Changes in concentration of H+ ions in <span class="hlt">olivine</span> have impacts on its rheological behaviour and therefore on tectonic processes involving mantle deformation. Deformation experiments on aggregates of wet <span class="hlt">olivine</span> exhibit different evolution of crystal preferred orientations (CPO) and substructure from experiments on dry <span class="hlt">olivine</span>, suggesting that elevated H+ concentrations impact activity of dislocation slip-systems. We use high angular-resolution electron backscatter diffraction (HR-EBSD) to map densities of different types of geometrically necessary dislocations (GND) in polycrystalline <span class="hlt">olivine</span> deformed experimentally under wet and dry conditions and also in nature. HR-EBSD provides unprecedented angular resolution, resolving misorientations < 0.01°. We also employ visco-plastic self-consistent (VPSC) simulations to investigate changes in slip-system activity. HR-EBSD maps from experimental samples demonstrate that <span class="hlt">olivine</span> deformed under hydrous conditions contains higher proportions of (001)[100] and (100)[001] edge dislocations than <span class="hlt">olivine</span> deformed under anhydrous conditions. Furthermore, maps of wet <span class="hlt">olivine</span> exhibit more polygonal subgrain boundaries indicative of enhanced recovery by dislocation climb. VPSC simulations with low critical resolved shear stresses for the (001)[100] and (100)[001] slip systems reproduce an unusual CPO with bimodal maxima of both [100] and [001] observed in wet <span class="hlt">olivine</span> aggregates. Analysis of a mylonitic lherzolite xenolith from Lesotho reveals the same unusual CPO and similar proportions of dislocation types to `wet' experimental samples, supporting the applicability of these findings to natural deformation conditions. These results support suggestions that H+ impacts the flow properties of <span class="hlt">olivine</span> by altering dislocation activity and climb, while also providing full quantification of GND content. In particular, the relative proportions of dislocation types may provide a basis for identifying <span class="hlt">olivine</span> deformed under wet and dry</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('https://www.ncbi.nlm.nih.gov/pubmed/28686286','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28686286"><span>3-D microstructure of <span class="hlt">olivine</span> in complex geological materials reconstructed by correlative X-ray μ-CT and EBSD analyses.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kahl, W-A; Dilissen, N; Hidas, K; Garrido, C J; López-Sánchez-Vizcaíno, V; Román-Alpiste, M J</p> <p>2017-11-01</p> <p>We reconstruct the 3-D microstructure of centimetre-sized <span class="hlt">olivine</span> crystals in rocks from the Almirez ultramafic massif (SE Spain) using combined X-ray micro computed tomography (μ-CT) and electron backscatter diffraction (EBSD). The semidestructive sample treatment involves geographically oriented drill pressing of rocks and preparation of oriented thin sections for EBSD from the μ-CT scanned cores. The μ-CT results show that the mean intercept length (MIL) analyses provide reliable information on the shape preferred orientation (SPO) of texturally different <span class="hlt">olivine</span> groups. We show that statistical interpretation of crystal preferred orientation (CPO) and SPO of <span class="hlt">olivine</span> becomes feasible because the highest densities of the distribution of main <span class="hlt">olivine</span> crystal axes from EBSD are aligned with the three axes of the 3-D ellipsoid calculated from the MIL analyses from μ-CT. From EBSD data we distinguish multiple CPO groups and by locating the thin sections within the μ-CT volume, we assign SPO to the corresponding <span class="hlt">olivine</span> crystal aggregates, which confirm the results of statistical comparison. We demonstrate that the limitations of both methods (i.e. no crystal orientation data in μ-CT and no spatial information in EBSD) can be overcome, and the 3-D orientation of the crystallographic axes of <span class="hlt">olivines</span> from different orientation groups can be successfully correlated with the crystal shapes of representative <span class="hlt">olivine</span> grains. Through this approach one can establish the link among geological structures, macrostructure, fabric and 3-D SPO-CPO relationship at the hand specimen scale even in complex, coarse-grained geomaterials. © 2017 The Authors Journal of Microscopy © 2017 Royal Microscopical Society.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28757219','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28757219"><span><span class="hlt">Olivine</span>, dolomite and ceramic filters in one vessel to produce clean gas from biomass.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rapagnà, Sergio; Gallucci, Katia; Foscolo, Pier Ugo</p> <p>2018-01-01</p> <p>Heavy organic compounds produced during almond shells gasification in a steam and/or air atmosphere, usually called tar, are drastically reduced in the product gas by using simultaneously in one vessel a ceramic filter placed in the freeboard and a mixture of <span class="hlt">olivine</span> and dolomite particles in the fluidized bed of the gasifier. The content of tar in the product gas during a reference gasification test with air, in presence of fresh <span class="hlt">olivine</span> particles only, was 8600mg/Nm 3 of dry gas. By gasifying biomass with steam at the same temperature level of 820°C in a bed of <span class="hlt">olivine</span> and dolomite (20% by weight), and in the presence of a catalytic ceramic filter inserted in the freeboard of the fluidized bed gasifier, the level of tar was brought down to 57mg/Nm 3 of dry producct gas, with a decrease of more than two orders of magnitude. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoJI.210..284S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoJI.210..284S"><span>Network topology of <span class="hlt">olivine</span>-basalt partial melts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Skemer, Philip; Chaney, Molly M.; Emmerich, Adrienne L.; Miller, Kevin J.; Zhu, Wen-lu</p> <p>2017-07-01</p> <p>The microstructural relationship between melt and solid grains in partially molten rocks influences many physical properties, including permeability, rheology, electrical conductivity and seismic wave speeds. In this study, the connectivity of melt networks in the <span class="hlt">olivine</span>-basalt system is explored using a systematic survey of 3-D X-ray microtomographic data. Experimentally synthesized samples with 2 and 5 vol.% melt are analysed as a series of melt tubules intersecting at nodes. Each node is characterized by a coordination number (CN), which is the number of melt tubules that intersect at that location. Statistically representative volumes are described by coordination number distributions (CND). Polyhedral grains can be packed in many configurations yielding different CNDs, however widely accepted theory predicts that systems with small dihedral angles, such as <span class="hlt">olivine</span>-basalt, should exhibit a predominant CN of four. In this study, melt objects are identified with CN = 2-8, however more than 50 per cent are CN = 4, providing experimental verification of this theoretical prediction. A conceptual model that considers the role of heterogeneity in local grain size and melt fraction is proposed to explain the formation of nodes with CN ≠ 4. Correctly identifying the melt network topology is essential to understanding the relationship between permeability and porosity, and hence the transport properties of partial molten mantle rocks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25167424','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25167424"><span>Three-dimensional coherent x-ray diffraction imaging of molten iron in mantle <span class="hlt">olivine</span> at nanoscale resolution.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jiang, Huaidong; Xu, Rui; Chen, Chien-Chun; Yang, Wenge; Fan, Jiadong; Tao, Xutang; Song, Changyong; Kohmura, Yoshiki; Xiao, Tiqiao; Wang, Yong; Fei, Yingwei; Ishikawa, Tetsuya; Mao, Wendy L; Miao, Jianwei</p> <p>2013-05-17</p> <p>We report quantitative 3D coherent x-ray diffraction imaging of a molten Fe-rich alloy and crystalline <span class="hlt">olivine</span> sample, synthesized at 6 GPa and 1800 °C, with nanoscale resolution. The 3D mass density map is determined and the 3D distribution of the Fe-rich and Fe-S phases in the <span class="hlt">olivine</span>-Fe-S sample is observed. Our results indicate that the Fe-rich melt exhibits varied 3D shapes and sizes in the <span class="hlt">olivine</span> matrix. This work has potential for not only improving our understanding of the complex interactions between Fe-rich core-forming melts and mantle silicate phases but also paves the way for quantitative 3D imaging of materials at nanoscale resolution under extreme pressures and temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28706268','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28706268"><span>Effect of water activity on rates of serpentinization of <span class="hlt">olivine</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lamadrid, Hector M; Rimstidt, J Donald; Schwarzenbach, Esther M; Klein, Frieder; Ulrich, Sarah; Dolocan, Andrei; Bodnar, Robert J</p> <p>2017-07-14</p> <p>The hydrothermal alteration of mantle rocks (referred to as serpentinization) occurs in submarine environments extending from mid-ocean ridges to subduction zones. Serpentinization affects the physical and chemical properties of oceanic lithosphere, represents one of the major mechanisms driving mass exchange between the mantle and the Earth's surface, and is central to current origin of life hypotheses as well as the search for microbial life on the icy moons of Jupiter and Saturn. In spite of increasing interest in the serpentinization process by researchers in diverse fields, the rates of serpentinization and the controlling factors are poorly understood. Here we use a novel in situ experimental method involving <span class="hlt">olivine</span> micro-reactors and show that the rate of serpentinization is strongly controlled by the salinity (water activity) of the reacting fluid and demonstrate that the rate of serpentinization of <span class="hlt">olivine</span> slows down as salinity increases and H 2 O activity decreases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatCo...816107L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatCo...816107L"><span>Effect of water activity on rates of serpentinization of <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lamadrid, Hector M.; Rimstidt, J. Donald; Schwarzenbach, Esther M.; Klein, Frieder; Ulrich, Sarah; Dolocan, Andrei; Bodnar, Robert J.</p> <p>2017-07-01</p> <p>The hydrothermal alteration of mantle rocks (referred to as serpentinization) occurs in submarine environments extending from mid-ocean ridges to subduction zones. Serpentinization affects the physical and chemical properties of oceanic lithosphere, represents one of the major mechanisms driving mass exchange between the mantle and the Earth's surface, and is central to current origin of life hypotheses as well as the search for microbial life on the icy moons of Jupiter and Saturn. In spite of increasing interest in the serpentinization process by researchers in diverse fields, the rates of serpentinization and the controlling factors are poorly understood. Here we use a novel in situ experimental method involving <span class="hlt">olivine</span> micro-reactors and show that the rate of serpentinization is strongly controlled by the salinity (water activity) of the reacting fluid and demonstrate that the rate of serpentinization of <span class="hlt">olivine</span> slows down as salinity increases and H2O activity decreases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AGUFM.V42A0318I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AGUFM.V42A0318I"><span>Partitioning of H2O on high pressure phase transformation of <span class="hlt">olivine</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.; Wada, T.; Sasaki, R.; Irifune, T.; Yurimoto, H.</p> <p>2003-12-01</p> <p>Water is the most abundant volatile component on the Earth's surface, and it has been supplied to the Earth's interiors by subducted slab. Water influences the physical properties and melting temperature of minerals. <span class="hlt">Olivine</span> is the most abundant mineral in the mantle, and it is clarified that the high-pressure polymorphs of <span class="hlt">olivine</span>, wadsleyite and ringwoodite, can contain 3wt% of H2O in their crystal structures (e.g. Inoue et al., 1995, 1998). However, the partitioning of H2O among these minerals has not been clarified yet except for <span class="hlt">olivine</span>-wadsleyite transformation (Chen et al., 2003). We have determined the partitioning of H2O between wadsleyite and ringwoodite and between ringwoodite and perovskite, and clarified the distribution of H2O among upper mantle, mantle transition zone and lower mantle. High-pressure experiments were conducted by MA-8 type (Kawai-type) high-pressure apparatus in Ehime University, and the chemical compositions were determined by EPMA. The water contents of minerals were measured by SIMS in Tokyo Institute of Technology. We succeeded to synthesize large (approximately 50 μ m) coexisting crystals of wadsleyite and ringwoodite, and of ringwoodite and perovskite, and we could clarify the partitioning of H2O between those coexisting minerals. The partition coefficients between wadsleyite and ringwoodite and between ringwoodite and perovskite were about 2 and about 10 or more, respectively. We (Chen et al., 2003) have already determined that the partition coefficients between wadsleyite and <span class="hlt">olivine</span> is about 5, so the partitioning among upper mantle, 410-520km and 520-660km of mantle transition zone, and lower mantle are 4:20:10:1. Thus the mantle transition zone should be a strong water reservoir in the Earth's interiors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CoMP..173...41P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CoMP..173...41P"><span>Transport properties of <span class="hlt">olivine</span> grain boundaries from electrical conductivity experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pommier, Anne; Kohlstedt, David L.; Hansen, Lars N.; Mackwell, Stephen; Tasaka, Miki; Heidelbach, Florian; Leinenweber, Kurt</p> <p>2018-05-01</p> <p>Grain boundary processes contribute significantly to electronic and ionic transports in materials within Earth's interior. We report a novel experimental study of grain boundary conductivity in highly strained <span class="hlt">olivine</span> aggregates that demonstrates the importance of misorientation angle between adjacent grains on aggregate transport properties. We performed electrical conductivity measurements of melt-free polycrystalline <span class="hlt">olivine</span> (Fo90) samples that had been previously deformed at 1200 °C and 0.3 GPa to shear strains up to γ = 7.3. The electrical conductivity and anisotropy were measured at 2.8 GPa over the temperature range 700-1400 °C. We observed that (1) the electrical conductivity of samples with a small grain size (3-6 µm) and strong crystallographic preferred orientation produced by dynamic recrystallization during large-strain shear deformation is a factor of 10 or more larger than that measured on coarse-grained samples, (2) the sample deformed to the highest strain is the most conductive even though it does not have the smallest grain size, and (3) conductivity is up to a factor of 4 larger in the direction of shear than normal to the shear plane. Based on these results combined with electrical conductivity data for coarse-grained, polycrystalline <span class="hlt">olivine</span> and for single crystals, we propose that the electrical conductivity of our fine-grained samples is dominated by grain boundary paths. In addition, the electrical anisotropy results from preferential alignment of higher-conductivity grain boundaries associated with the development of a strong crystallographic preferred orientation of the grains.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=PIA09348&hterms=fingerprints&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dfingerprints','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=PIA09348&hterms=fingerprints&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dfingerprints"><span><span class="hlt">Olivine</span> in the Southern Isidis Basin</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2007-01-01</p> <p><p/> The Compact Reconnaissance Imaging Spectrometer for Mars (CRISM) took this observation of the transition region between Libya Montes and the Isidis Basin on Mars at 17:16 UTC (12:16 p.m. EST) on January 2, 2007, near 3.6 degrees north latitude, 84.1 degrees east longitude. The image was taken in 544 colors covering 0.36-3.92 micrometers, and shows features as small as 18 meters (60 feet) across. The image is about 11 kilometers (7 miles) wide at its narrowest point. <p/> The Isidis Basin resulted from of a gigantic impact on the surface of Mars early in the planet's history. The southern rim, where this target is located, is a region of complex geology and part of the planetary dichotomy boundary that separates the older southern highlands from the lower, younger northern plains. The image on the left was constructed from three visible wavelengths (RGB: 0.71, 0.60, 0.53 microns) and is a close approximation of how the surface would appear to the human eye. The image on the right was constructed from three infrared wavelengths (RGB: 2.49, 1.52, 1.08 microns) chosen to highlight variations in the mineralogy of the area. Of interest is that features in this image not only differ in color, but also in texture and morphology. The gray areas absorb similarly at all wavelengths used in this image, but display absorptions at other wavelengths related to the iron- and magesium-rich mineral pyroxene. The reddest areas absorb strongly at the wavelengths used for green and blue, which is attributable to another iron- and magesium-rich mineral, <span class="hlt">olivine</span>. The brownish areas show subdued mineral absorptions and could represent some type of mixture between the other two materials. The presence of the mineral <span class="hlt">olivine</span> is particularly interesting because <span class="hlt">olivine</span> easily weathers to other minerals; thus, its presence indicates either the lack of weathering in this region or relatively recent exposure. <p/> CRISM's mission: Find the spectral fingerprints of aqueous and hydrothermal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPSC...11..238S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPSC...11..238S"><span>Behaviour of phase functions of <span class="hlt">Olivine</span> and Augite assemblages in the wavelength range 0.3-18 μm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salgueiro da Silva, M. A.; Seixas, T. M.; Maturilli, A.; Helbert, J.</p> <p>2017-09-01</p> <p>We tested the validity of the wavelength-independent phase function assumption by measuring BDR of <span class="hlt">olivine</span> and augite mineral assemblages in the extended spectral range 0.3-18 μm. Because quasi-isotropic scattering is present in both OL and AUG assemblages with grain-size dependent features, it is not clear that this is an intrinsic effect attributed to the wavelength dependence of the optical constants of <span class="hlt">olivine</span> and augite minerals. Our results show that the application of Hapke model to <span class="hlt">olivine</span> and augite BDR spectra in the MIR range requires a wavelength- and, possibly, grain size-dependent phase function.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...845...87L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...845...87L"><span>The Carnegie-Irvine Galaxy Survey. V. Statistical Study of <span class="hlt">Bars</span> and Buckled <span class="hlt">Bars</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Zhao-Yu; Ho, Luis C.; Barth, Aaron J.</p> <p>2017-08-01</p> <p>Simulations have shown that <span class="hlt">bars</span> are subject to a vertical buckling instability that transforms thin <span class="hlt">bars</span> into boxy or peanut-shaped structures, but the physical conditions necessary for buckling to occur are not fully understood. We use the large sample of local disk galaxies in the Carnegie-Irvine Galaxy Survey to examine the incidence of <span class="hlt">bars</span> and buckled <span class="hlt">bars</span> across the Hubble sequence. Depending on the disk inclination angle (I), a buckled <span class="hlt">bar</span> reveals itself as either a boxy/peanut-shaped bulge (at high I) or as a barlens structure (at low I). We visually identify <span class="hlt">bars</span>, boxy/peanut-shaped bulges, and barlenses, and examine the dependence of <span class="hlt">bar</span> and buckled <span class="hlt">bar</span> fractions on host galaxy properties, including Hubble type, stellar mass, color, and gas mass fraction. We find that the <span class="hlt">barred</span> and unbarred disks show similar distributions in these physical parameters. The <span class="hlt">bar</span> fraction is higher (70%-80%) in late-type disks with low stellar mass (M * < 1010.5 M ⊙) and high gas mass ratio. In contrast, the buckled <span class="hlt">bar</span> fraction increases to 80% toward massive and early-type disks (M * > 1010.5 M ⊙), and decreases with higher gas mass ratio. These results suggest that <span class="hlt">bars</span> are more difficult to grow in massive disks that are dynamically hotter than low-mass disks. However, once a <span class="hlt">bar</span> forms, it can easily buckle in the massive disks, where a deeper potential can sustain the vertical resonant orbits. We also find a probable buckling <span class="hlt">bar</span> candidate (ESO 506-G004) that could provide further clues to understand the timescale of the buckling process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017stis.rept....3S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017stis.rept....3S"><span>Enabling Narrow(est) IWA Coronagraphy with STIS <span class="hlt">BAR</span>5 and <span class="hlt">BAR</span>10 Occulters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schneider, Glenn; Gaspar, Andras; Debes, John; Gull, Theodore; Hines, Dean; Apai, Daniel; Rieke, George</p> <p>2017-09-01</p> <p>The Space Telescope Imaging Spectrograph's (STIS) <span class="hlt">BAR</span>5 coronagraphic occulter was designed to provide high-contrast, visible-light, imaging in close (> 0.15") angular proximity to bright point-sources. We explored and verified the functionality and utility of the <span class="hlt">BAR</span>5 occulter. We also investigated, and herein report on, the use of the <span class="hlt">BAR</span>10 rounded corners as narrow-angle occulters and compare IWA vs. contrast performance for the <span class="hlt">BAR</span>5, <span class="hlt">BAR</span>10, and Wedge occulters. With that, we provide recommendations for the most efficacious <span class="hlt">BAR</span>5 and <span class="hlt">BAR</span>10 use on-orbit in support of GO science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.T44A..06R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.T44A..06R"><span><span class="hlt">Olivine</span> Slip-system Activity at High Pressure: Implications for Upper-Mantle Rheology and Seismic Anisotropy (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raterron, P.; Castelnau, O.; Geenen, T.; Merkel, S.</p> <p>2013-12-01</p> <p>The past decade abounded in technical developments allowing the investigation of materials rheology at high pressure (P > 3 GPa) [1]. This had a significant impact on our understanding of <span class="hlt">olivine</span> rheology in the Earth asthenosphere, where P is in the range 3 - 13 GPa. A dislocation slip-system transition induced by pressure has been documented in dry Fe-bearing <span class="hlt">olivine</span> [2]; it induces changes in <span class="hlt">olivine</span> aggregate lattice preferred orientation (LPO) [3,4], which may explain the seismic velocity anisotropy attenuation observed at depths > 200 km in the upper mantle [5]. Deformation experiments carried out on <span class="hlt">olivine</span> single crystals at high pressure allowed quantifying the effect of P on individual slip system activities [6]. Integration of these data, together with data on lattice friction arising from computational models (e.g., [7]), into analytical or mean-field numerical models for aggregate plasticity gave insight on the viscosity and LPO of <span class="hlt">olivine</span> aggregates deformed at geological conditions in the dislocation creep regime [8,9]. We will review these recent findings and their implications for upper mantle rheology and seismic anisotropy. [1] Raterron & Merkel, 2009, J. Sync. Rad., 16, 748 ; [2] Raterron et al., 2009, PEPI, 172, 74 ; [3] Jung et al., 2009, Nature Geoscience, 2, 73 ; [4] Ohuchi et al., 2011, EPSL, 304, 55 ; [5] Mainprice et al., 2005, Nature, 433, 731 ; [6] Raterron et al., 2012, PEPI, 200-201, 105 ; [7] Durinck et al., 2007, EJM, 19, 631 ; [8] Castelnau et al., 2010, C.R. Physique, 11, 304 ; [9] Raterron et al., 2011, PEPI, 188, 26</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AAS...22942708H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AAS...22942708H"><span><span class="hlt">Bar</span> Evolution and <span class="hlt">Bar</span> Properties from Disc Galaxies in the Early Universe</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hutchinson-Smith, Tenley; Simmons, Brooke</p> <p>2017-01-01</p> <p><span class="hlt">Bars</span> in disc galaxies indicate a large collection of stars in a specific configuration of orbits that give the galaxy center a rectangular looking feature. Astronomers have discovered that these <span class="hlt">bars</span> affect the distribution of matter in galaxies, and are also related to galaxy stellar mass and star formation history. Little is known about the specifics of how <span class="hlt">bars</span> evolve and drive the evolution of their host galaxies because only a handful of <span class="hlt">bars</span> have been studied in detail so far. I have examined a sample of 8,221 <span class="hlt">barred</span> galaxies from the early universe to identify and examine correlations with galaxy properties. The data comes from Galaxy Zoo, an online citizen science project that allows anyone to classify and measure detailed properties of galaxies. I present results including the fraction of galaxies in the sample that have <span class="hlt">bars</span>, and the variation of galaxy properties with <span class="hlt">bar</span> length, including galaxy color and stellar mass. I also compare these results to <span class="hlt">barred</span> galaxies in the local universe. I will discuss the implications of these results in the context of galaxy evolution overall, including the effect of dark matter on <span class="hlt">bars</span> and galaxy evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.465..145D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.465..145D"><span>Origin of crystalline silicates from Comet 81P/Wild 2: Combined study on their oxygen isotopes and mineral chemistry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Defouilloy, Céline; Nakashima, Daisuke; Joswiak, David J.; Brownlee, Donald E.; Tenner, Travis J.; Kita, Noriko T.</p> <p>2017-05-01</p> <p>In order to explore the link between comet 81P/Wild 2 and materials in primitive meteorites, seven particles 5 to 15 μm in diameter from comet 81P/Wild 2 have been analyzed for their oxygen isotope ratios using a secondary ion mass spectrometer. Most particles are single minerals consisting of <span class="hlt">olivine</span> or pyroxene with Mg# higher than 85, which are relatively minor in 81P/Wild 2 particles (∼1/3 of the 16O-poor cluster). Four particles extracted from Track 149 are 16O-poor and show Δ17O (= δ17O - 0.52 × δ18O) values from -2‰ to +1‰, similar to previous studies, while one enstatite (En99) particle shows lower Δ17O value of - 7 ± 4 ‰ (2 σ). This compositional range has not been reported among 16O-poor particles in 81P/Wild 2, but is commonly observed among <span class="hlt">chondrules</span> in carbonaceous chondrites and in particular in CR chondrites. The distribution in Δ17O indicates that 16O-poor 81P/Wild 2 particles are most similar to <span class="hlt">chondrules</span> (and their fragments) in the CR chondrites and Tagish Lake-like WIS91600 chondrite <span class="hlt">chondrule</span> silicate grains, which indicates that they likely come from a reservoir with similar dust/ice ratios as CR chondrites and WIS91600. However, differences in the Mg# distribution imply that the 81P/Wild 2 reservoir was comparatively more oxidized, with a higher dust enrichment. Two nearly pure enstatite grains from track 172 are significantly enriched in 16O, with δ18O values of - 51.2 ± 1.5 ‰ (2 σ) and - 43.0 ± 1.3 ‰ (2 σ), respectively, and Δ17O values of - 22.3 ± 1.9 ‰ (2 σ) and - 21.3 ± 2.3 ‰ (2 σ), respectively. They are the first 16O-rich pyroxenes found among 81P/Wild 2 particles, with similar Δ17O values to those of 16O-rich low-iron, manganese-enriched (LIME) <span class="hlt">olivine</span> and CAI (calcium and aluminum-rich inclusions) - like particles from 81P/Wild 2. The major element and oxygen isotopic compositions of the pyroxenes are similar to those of enstatite in amoeboid <span class="hlt">olivine</span> aggregates (AOAs) in primitive chondrites, in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090006950','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090006950"><span>Rb-Sr and Sm-Nd Studies of <span class="hlt">Olivine</span>-Phyric Shergottites RBT 04262 and LAR 06319: Isotopic Evidence for Relationship to Enriched Basaltic Shergottites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nyquist, L.E.; Shih, C.-Y.; Reese, Y.</p> <p>2009-01-01</p> <p>RBT 04262 and LAR 06319 are two Martian meteorites recently discovered in Antarctica. Both contain abundant <span class="hlt">olivines</span>, and were classified as <span class="hlt">olivine</span>-phyric shergottites. A detailed petrographic study of RBT 04262 suggested it should be reclassified as a lherzolitic shergottite. However, the moderately LREE-depleted REE distribution pattern indicated that it is closely related to enriched basaltic shergottites like Shergotty, Zagami, Los Angeles, etc. In earlier studies of a similarly olivinephyric shergottite NWA 1068 which contains 21% modal <span class="hlt">olivine</span>, it was shown that it probably was produced from an enriched basaltic shergottite magma by <span class="hlt">olivine</span> accumulation . As for LAR 06319, recent petrographic studies suggested that it is different from either lherzolitic shergottites or the highly LREE-depleted <span class="hlt">olivine</span>-phyric shergottites. We performed Rb-Sr and Sm-Nd isotopic analyses on RBT 04262 and LAR 06319 to determine their crystallization ages and Sr and Nd isotopic signatures, and to better understand the petrogenetic relationships between them and other basaltic, lherzolitic and depleted <span class="hlt">olivine</span>-phyric shergottites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22663252-carnegie-irvine-galaxy-survey-statistical-study-bars-buckled-bars','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22663252-carnegie-irvine-galaxy-survey-statistical-study-bars-buckled-bars"><span>The Carnegie-Irvine Galaxy Survey. V. Statistical Study of <span class="hlt">Bars</span> and Buckled <span class="hlt">Bars</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>Li, Zhao-Yu; Ho, Luis C.; Barth, Aaron J., E-mail: lizy@shao.ac.cn</p> <p></p> <p>Simulations have shown that <span class="hlt">bars</span> are subject to a vertical buckling instability that transforms thin <span class="hlt">bars</span> into boxy or peanut-shaped structures, but the physical conditions necessary for buckling to occur are not fully understood. We use the large sample of local disk galaxies in the Carnegie-Irvine Galaxy Survey to examine the incidence of <span class="hlt">bars</span> and buckled <span class="hlt">bars</span> across the Hubble sequence. Depending on the disk inclination angle ( i ), a buckled <span class="hlt">bar</span> reveals itself as either a boxy/peanut-shaped bulge (at high i ) or as a barlens structure (at low i ). We visually identify <span class="hlt">bars</span>, boxy/peanut-shaped bulges, andmore » barlenses, and examine the dependence of <span class="hlt">bar</span> and buckled <span class="hlt">bar</span> fractions on host galaxy properties, including Hubble type, stellar mass, color, and gas mass fraction. We find that the <span class="hlt">barred</span> and unbarred disks show similar distributions in these physical parameters. The <span class="hlt">bar</span> fraction is higher (70%–80%) in late-type disks with low stellar mass ( M {sub *} < 10{sup 10.5} M {sub ⊙}) and high gas mass ratio. In contrast, the buckled <span class="hlt">bar</span> fraction increases to 80% toward massive and early-type disks ( M {sub *} > 10{sup 10.5} M {sub ⊙}), and decreases with higher gas mass ratio. These results suggest that <span class="hlt">bars</span> are more difficult to grow in massive disks that are dynamically hotter than low-mass disks. However, once a <span class="hlt">bar</span> forms, it can easily buckle in the massive disks, where a deeper potential can sustain the vertical resonant orbits. We also find a probable buckling <span class="hlt">bar</span> candidate (ESO 506−G004) that could provide further clues to understand the timescale of the buckling process.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1993Metic..28R.344E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1993Metic..28R.344E"><span>Constraints on Nubular Electromagnetic Pulses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eisenhour, D. D.; Buseck, P. R.</p> <p>1993-07-01</p> <p>Chondritic meteorites contain an abundance of silicate minerals with opaque inclusions of oxides, sulfides, and metals. These host silicates interact differently from their enclosed opaques to electromagnetic (EM) radiation; specifically, silicates are inefficient at absorbing EM energy in the visible and near infrared while metals, sulfides, and Fe oxides absorb strongly in this frequency range. In the presence of a strong electromagnetic pulse (EMP), this preferential absorption leads to the selective heating of the opaque inclusions and can produce unique textures ("dirty snowballs": intimate, ~spherical intergrowths of silicate and opaque minerals with radii of < 1 to 10 micrometers) that record the passage of the EMP. Many <span class="hlt">chondrules</span>, CAIs, and isolated silicate grains within chondritic meteorites exhibit these unique features, suggesting that strong EMPs were common in the early solar nebula [1]. Here we discuss new constraints on nebular EMPs obtained from both experimental simulations and calculations of radiative heat transport. To test the feasibility of producing "dirty snowball" textures by EMP heating, <span class="hlt">olivines</span> and pyroxenes containing metal and sulfide inclusions were heated with a 10 watt, argon-ion, CW laser operated at 514 nm. Comparisons between meteoritic "dirty snowball" textures and experimentally produced textures confirm the ability to produce the meteoritic textures by EMP heating and suggest heating times and fluxes of 0.25 to 10 seconds and 10^9 to 10^10 ergs cm^-2 sec^-1. Fluxes less than 10^9 ergs cm^-2 sec^-1 were insufficient to melt metal and sulfide inclusions, while fluxes greater than 10^10 ergs cm^-2 sec^-1 resulted in complete melting of metal, sulfide, and silicates. The experimentally determined heating time scales suggest that radiative equilibrium was reached in the "dirty snowball" formation process, indicating that the range of observed textures is controlled by cooling rates. Calculations of radiative absorption and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5594423','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5594423"><span>Effect of water activity on rates of serpentinization of <span class="hlt">olivine</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>Lamadrid, Hector M.; Rimstidt, J. Donald; Schwarzenbach, Esther M.; Klein, Frieder; Ulrich, Sarah; Dolocan, Andrei; Bodnar, Robert J.</p> <p>2017-01-01</p> <p>The hydrothermal alteration of mantle rocks (referred to as serpentinization) occurs in submarine environments extending from mid-ocean ridges to subduction zones. Serpentinization affects the physical and chemical properties of oceanic lithosphere, represents one of the major mechanisms driving mass exchange between the mantle and the Earth’s surface, and is central to current origin of life hypotheses as well as the search for microbial life on the icy moons of Jupiter and Saturn. In spite of increasing interest in the serpentinization process by researchers in diverse fields, the rates of serpentinization and the controlling factors are poorly understood. Here we use a novel in situ experimental method involving <span class="hlt">olivine</span> micro-reactors and show that the rate of serpentinization is strongly controlled by the salinity (water activity) of the reacting fluid and demonstrate that the rate of serpentinization of <span class="hlt">olivine</span> slows down as salinity increases and H2O activity decreases. PMID:28706268</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI21A0400Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI21A0400Z"><span>Electrical Investigation of Metal-<span class="hlt">Olivine</span> Systems and Application to the Deep Interior of Mercury</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Z.; Pommier, A.</p> <p>2017-12-01</p> <p>Transfers of mass, heat, and electric currents between a silicate mantle and an underlying metallic core characterize the Core-Mantle Boundary (CMB) region of terrestrial planets. In particular, constraining the structure and chemistry of the CMB region of Mercury is crucial to understand its thermal state and unique magnetic activity. To probe the physical and chemical processes of the Hermean CMB, we conducted an electrical study of metal-<span class="hlt">olivine</span> systems at pressure, temperature, and chemistry conditions relevant to the mantle and CMB region of Mercury. Electrical measurements were performed at 5-7 GPa and up to 1675ºC during heating and cooling in the multi-anvil apparatus using impedance spectroscopy. Samples are made of one metal layer (Fe, FeS, FeSi2, or Fe-Ni-S-Si systems) and one polycrystalline <span class="hlt">olivine</span> (Fo90) layer, with the metal:<span class="hlt">olivine</span> ratio ranging from 1:0.7 to 1:9.2. For all samples, we observe that bulk electrical conductivity increases with temperature from 10-2.5 to 101.8 S/m, which is higher than the conductivity of polycrystalline <span class="hlt">olivine</span> but lower than the one of the metal phase at similar conditions. In some experiments, a conductivity jump is observed at a temperature corresponding to the melting temperature of the metal phase. This conductivity increase cannot be explained by the electrical properties of liquid metal as metal is less conductive with increasing temperature. We observe that both the metal:<span class="hlt">olivine</span> ratio and the change in metal phase geometry during heating best explain the bulk conductivity. By combining our electrical results, textural analyses of the samples and previous experimental and numerical works, we propose an electrical profile of the deep interior of Mercury. Comparison of our model with existing conductivity estimates of Mercury's lowermost mantle and CMB from magnetic field observations and thermodynamic calculations supports the hypothesis of a layered CMB-outermost core structure in present-day Mercury.</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/2017PCM....44..203U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PCM....44..203U"><span>Morphological changes of <span class="hlt">olivine</span> grains reacted with amino acid solutions by impact process</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Umeda, Yuhei; Takase, Atsushi; Fukunaga, Nao; Sekine, Toshimori; Kobayashi, Takamichi; Furukawa, Yoshihiro; Kakegawa, Takeshi</p> <p>2017-03-01</p> <p>Early oceans on Earth might have contained certain amounts of biomolecules such as amino acids, and they were subjected to meteorite impacts, especially during the late heavy bombardment. We performed shock recovery experiments by using a propellant gun in order to simulate shock reactions among <span class="hlt">olivine</span> as a representative meteorite component, water and biomolecules in oceans in the process of marine meteorite impacts. In the present study, recovered solid samples were analyzed by using X-ray powder diffraction method, scanning electron microscopy, electron probe microanalysis, and transmission electron microscopy with energy-dispersive X-ray spectrometry. The analytical results on shocked products in the recovered sample showed (1) morphological changes of <span class="hlt">olivine</span> to fiber- and bamboo shoot-like crystals, and to pulverized grains; and features of lumpy surfaces affected by hot water, (2) the formation of carbon-rich substances derived from amino acids, and (3) the incorporation of metals from container into samples. According to the present results, fine-grained <span class="hlt">olivine</span> in meteorites might have morphologically changed and shock-induced chemical reactions might have been enhanced so that amino acids related to the origin of life may have transformed to carbon-rich substances by impacts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007E%26PSL.261..134B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007E%26PSL.261..134B"><span>The infrared signature of water associated with trivalent cations in <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berry, Andrew J.; O'Neill, Hugh St. C.; Hermann, Jörg; Scott, Dean R.</p> <p>2007-09-01</p> <p>Forsterite crystals were synthesised under water saturated conditions at 1400 °C and 1.5 GPa doped with trace amounts of either B, Al, Sc, Ti, V, Cr, Mn, Fe, Co, Ga, Y, Zr, In, Sm, Gd, Dy, Tm, or Lu. The common and intense hydroxyl stretching bands in the infrared spectra of spinel peridotite <span class="hlt">olivine</span>, at 3572 and 3525 cm -1, were only reproduced in the presence of Ti. Those samples where the trace element substitutes as the trivalent cation on the Mg 2+ site were identified from a systematic variation in concentration with the trivalent ionic radius. The hydroxyl region of all samples is essentially identical except for between 3300 and 3400 cm -1. This region is characterised by one or more bands, with the energy of the most intense feature being correlated with the ionic radius of the trivalent cation. The integrated intensity of these hydroxyl bands also correlates with the concentration of the trivalent cation. These correlations provide unambiguous evidence that bands, or peaks, in this region correspond to water at defect sites associated with trivalent cations. "Trivalent peaks" are sometimes observed in samples of mantle <span class="hlt">olivine</span> and most likely indicate water associated with Fe 3+. The water at this site is not incorporated under normal mantle conditions and should not be included in estimates of the water capacity of mantle <span class="hlt">olivine</span>. These results emphasise the importance of identifying the infrared signature of different water substitution mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.B51I0524F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.B51I0524F"><span>Bacterial Oxidation of Iron in <span class="hlt">Olivine</span>: Implications for the Subsurface Biosphere, Global Chemical Cycles, and Life 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>Fisk, M. R.; Popa, R.; Smith, A. R.; Popa, R.; Boone, J.</p> <p>2011-12-01</p> <p>We isolated 21 species of bacteria from subseafloor and terrestrial basalt environments and which thrive on <span class="hlt">olivine</span> at neutral pH. Cell numbers increase four to five orders of magnitude over three weeks in media where the only metabolic energy comes from the oxidation of Fe(II) in <span class="hlt">olivine</span>. The subseafloor bacteria were isolated from a borehole on the flank of Juan de Fuca Ridge in the northeast Pacific basin where the temperature ranged from 4 up to 64 °C over four years. Terrestrial isolates originated from the basalt-ice boundary in a lava tube on the flank of Newberry Caldera in the Cascades of Oregon. The borehole water was either seawater or seawater plus subseafloor formation water and the lava tube ice was frozen meteoric or ground water. Although microorganisms capable of oxidizing iron for growth are known, microbes that oxidize iron from silicate minerals at neutral pH have not previously been cultured. The 21 species in this study are the first neutrophilic, iron-oxidizing bacteria (nFeOB) to be isolated and cultured that grow on <span class="hlt">olivine</span>. These nFeOB are primary producers and we believe that they are a widespread component of the subsurface biosphere. In addition to their ability use iron from <span class="hlt">olivine</span>, these microbes assimilate carbon from bicarbonate in solution and can grow when oxygen pressures are low. They also use nitrate as an alternative electron acceptor to oxygen in anaerobiosis. Since basalt is the most common rock in the Earth's crust and iron is the fourth most abundant element in the crust, we believe nFeOB are likely to be a significant portion of the subsurface biosphere. They are likely to affect, and perhaps in some environments control, the weathering rate of <span class="hlt">olivine</span> and possibly of pyroxene and basalt glass. <span class="hlt">Olivine</span> is a component of Mars's surface and it is present on other rocky bodies in the solar system. The ability of these bacteria to use Fe(II) from <span class="hlt">olivine</span>, to assimilate carbon, to grow at low temperature, and to use low</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.V31B0615M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.V31B0615M"><span>Complications in Determining Oxygen Fugacities From <span class="hlt">Olivine</span>-Melt Equilibrium Illustrated by the Pu'u'O'o Lavas, Hawaii</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McCann, V. E.; Barton, M.; Thornber, C. R.</p> <p>2005-12-01</p> <p>We have shown previously that oxygen fugacities calculated from <span class="hlt">olivine</span>-melt equilibrium using rim compositions agree well with those calculated from analyzed Fe3+/σFe for MORB and for Icelandic OIB (MORB - average ΔFMQ -0.72 versus -0.70, Iceland average ΔFMQ -0.49 versus -0.58). The agreement between oxygen fugacities calculated from Ol-melt equilibrium and those calculated from analyzed Fe3+/σFe is excellent for individual samples of MORB from the FAMOUS region and Blanco Trough ( difference in calculated ΔFMQ < 0.30). Published analyses of Fe3+/σFe yield oxygen fugacilties of ΔFMQ= -0.72±0.43 for lavas from Kilauea and Mauna Loa, and ΔFMQ=0.91±0.72 for Loihi, very close to those for MORB. Oxygen fugacities determined using carefully selected Ol-melt analyses (ΔFMQ= -0.43±0.32) are in reasonable agreement with those determined from Fe3+/σFe for Kilauea and Mauna Loa, and agreement between fO2 calculated from Ol-melt equilibrium (ΔFMQ= -0.26) and that calculated from Fe3+/σFe (ΔFMQ= -0.64) is excellent for one sample from Kilauea. However, <span class="hlt">olivine</span>-melt pairs from some samples, including those from the Pu'u'O'o lavas, yield anomalously high or low estimates of fO2 (average ΔFMQ =-0.6907, range -4.07 to +0.34). We suggest that these anomalous values reflect the complex history of <span class="hlt">olivines</span> in these lavas, in particular the effects of magma mixing. Some <span class="hlt">olivines</span> in the Pu'u'O'o lavas clearly have rims that are anomalously rich in Fa, whereas others have rims that are anomalously rich in Fo and do not appear to have equilibrium compositions. Given the dependence of <span class="hlt">olivine</span> composition on melt Fe3+/σFe, there is no simple method to determine the equilibrium composition of <span class="hlt">olivine</span> for a particular melt. However, detailed zoning profiles and analyses of microphenocrysts allow probable equilibrium compositions to be identified. We suggest that the average fO2 of Hawaiian lavas lies close to (ΔFMQ= -1) based on published results using spinel</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012NIMPB.286..243A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012NIMPB.286..243A"><span>SAXS study of ion tracks in San Carlos <span class="hlt">olivine</span> and Durango apatite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Afra, B.; Rodriguez, M. D.; Lang, M.; Ewing, R. C.; Kirby, N.; Trautmann, C.; Kluth, P.</p> <p>2012-09-01</p> <p>Ion tracks were generated in crystalline San Carlos <span class="hlt">olivine</span> (Mg,Fe)2SiO4 and Durango apatite Ca10(PO4)6F2 using different heavy ions (58Ni, 101Ru, 129Xe, 197Au, and 238U) with energies ranging between 185 MeV and 2.6 GeV. The tracks and their annealing behavior were studied by means of synchrotron based small angle X-ray scattering in combination with in situ annealing. Track radii vary as a function of electronic energy loss but are very similar in both minerals. Furthermore, the annealing behavior of the track radii has been investigated and preliminary results reveal a lower recovery rate of the damaged area in <span class="hlt">olivine</span> compared with apatite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhG...45e5002W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhG...45e5002W"><span>Studying W‧ boson contributions in \\<span class="hlt">bar</span>{B} \\rightarrow {D}^{(* )}{{\\ell }}^{-}{\\<span class="hlt">bar</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, Yi-Long; Wei, Bin; Sheng, Jin-Huan; Wang, Ru-Min; Yang, Ya-Dong</p> <p>2018-05-01</p> <p>Recently, the Belle collaboration reported the first measurement of the τ lepton polarization P τ (D*) in \\<span class="hlt">bar</span>{B}\\to {D}* {τ }-{\\<span class="hlt">bar</span>{ν }}τ decay and a new measurement of the rate of the branching ratios R(D*), which are consistent with the Standard Model (SM) predictions. These could be used to constrain the New Physics (NP) beyond the SM. In this paper, we probe \\<span class="hlt">bar</span>{B}\\to {D}(* ){{\\ell }}-{\\<span class="hlt">bar</span>{ν }}{\\ell } (ℓ = e, μ, τ) decays in the model-independent way and in the specific G(221) models with lepton flavour universality. Considering the theoretical uncertainties and the experimental errors at the 95% C.L., we obtain the quite strong bounds on the model-independent parameters {C}{{LL}}{\\prime },{C}{{LR}}{\\prime },{C}{{RR}}{\\prime },{C}{{RL}}{\\prime },{g}V,{g}A,{g}V{\\prime },{g}A{\\prime } and the specific G(221) model parameter rates. We find that the constrained NP couplings have no obvious effects on all (differential) branching ratios and their rates, nevertheless, many NP couplings have very large effects on the lepton spin asymmetries of \\<span class="hlt">bar</span>{B}\\to {D}(* ){{\\ell }}-{\\<span class="hlt">bar</span>{ν }}{\\ell } decays and the forward–backward asymmetries of \\<span class="hlt">bar</span>{B}\\to {D}* {{\\ell }}-{\\<span class="hlt">bar</span>{ν }}{\\ell }. So we expect precision measurements of these observables would be researched by LHCb and Belle-II.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810062284&hterms=Iron+oxide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DIron%2Boxide','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810062284&hterms=Iron+oxide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DIron%2Boxide"><span>Near-infrared spectral reflectance of mineral mixtures - Systematic combinations of pyroxenes, <span class="hlt">olivine</span>, and iron oxides</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Singer, R. B.</p> <p>1981-01-01</p> <p>Near-infrared spectral reflectance data are presented for systematic variations in weight percent of two component mixtures of ferromagnesium and iron oxide minerals used to study the dark materials on Mars. <span class="hlt">Olivine</span> spectral features are greatly reduced in contrast by admixture of other phases but remain distinctive even for low <span class="hlt">olivine</span> contents. Clinopyroxene and orthopyroxene mixtures show resolved pyroxene absorptions near 2 microns. Limonite greatly modifies pyroxene and <span class="hlt">olivine</span> reflectance, but does not fully eliminate distinctive spectral characteristics. Using only spectral data in the 1 micron region, it is difficult to differentiate orthopyroxene and limonite in a mixture. All composite mineral absorptions were either weaker than or intermediate in strength to the end-member absorptions and have bandwidths greater than or equal to those for the end members. In general, spectral properties in an intimate mixture combine in a complex, nonadditive manner, with features demonstrating a regular but usually nonlinear variation as a function of end-member phase proportions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUFMDI33A1129B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUFMDI33A1129B"><span>Precipitation of Excess Hydrogen in <span class="hlt">Olivine</span> During Cooling Under Pressures: An Experimental Study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Borinski, S.; Karato, S.</p> <p>2007-12-01</p> <p>Water (hydrogen) content in <span class="hlt">olivine</span> transported from the upper mantle is used to infer the water content in the upper mantle (e.g., Bell and Rossman 1992). However, since hydrogen diffusion is known to be fast, processes of hydrogen loss need to be examined. In many literature, diffusion loss (or gain) of hydrogen is usually considered, but in addition to diffusion loss, hydrogen could also precipitate inside of <span class="hlt">olivine</span> as small inclusions. Consider an upward transport of <span class="hlt">olivine</span>-bearing rock that originally contained a large amount of hydrogen in the deep interior. As this rock is transported to the shallow region, the solubility limit of hydrogen will decrease because of the reduction of pressure (and temperature) (Kohlstedt et al. 1996, Zhao et al 2004). Consequently, excess hydrogen will precipitate to form water bubbles and/or hydrous minerals as inclusions. Frequently observed submicron-scale inclusions of hydrous minerals (Khisina and Wirth 2002, Kitamura et al. 1987) may correspond to these precipitation products. If that is the case, hydrogen content corresponding to these minerals should not be excluded when estimating the hydrogen content of a sample in the Earth's upper mantle. However, kinetics of precipitation of hydrogen from <span class="hlt">olivine</span> have not been investigated in the laboratory. We have conducted a series of experimental study in which we annealed hydrogen-saturated <span class="hlt">olivine</span> single crystals in two different P- T conditions. The starting material was an <span class="hlt">olivine</span> crystal in which ~1,135 H/106Si (70 wt ppm H2O) was dissolved at P= 3.5 GPa and T=1,573 K. A small piece of this crystal (0.5 mm3) was placed in a multianvil at P=3.5 GPa and either at T= 873K or 1,173K with oxygen fugacity, fO2, buffered by the Ni-NiO solid-state reaction and silica activity, aSiO2, buffered by the presence of orthopyroxene powder in contact with the crystal. Annealing experiments were conducted up to 72 hours. Hydroxyl concentrations were determined from infrared spectra</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820038745&hterms=Paradox+value&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DParadox%2Bvalue','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820038745&hterms=Paradox+value&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DParadox%2Bvalue"><span>Lunar highland rocks - Element partitioning among minerals. II - Electron microprobe analyses of Al, P, Ca, Ti, Cr, Mn and Fe in <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Smith, J. V.; Hansen, E. C.; Steele, I. M.</p> <p>1980-01-01</p> <p>Lunar <span class="hlt">olivines</span> from anorthosites, granulitic impactites, and rocks in the Mg-rich plutonic trend were subjected to electron probe measurements for Al, P, Ca, Ti, Cr and Mn, which show that the FeO/MnO ratio for lunar <span class="hlt">olivines</span> lies between 80 and 110 with little difference among the rock types. The low values of Ca in lunar <span class="hlt">olivines</span> indicate slow cooling to subsolidus temperatures, with blocking temperatures of about 750 C for 67667 and 1000 C for 60255,73-alpha determined by the Finnerty and Boyd (1978) experiments. An important paradox is noted in the low Ti content of Fe-rich <span class="hlt">olivines</span> from anorthosites, although both Ti and Fe tend to become enriched in liquid during fractional distillation. Except for Ca and Mn, <span class="hlt">olivine</span> from anorthosites has lower minor element values than other rock types. Formation from a chemically distinct system is therefore implied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V13E..04S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V13E..04S"><span>Experimentally determined isotope effect during Mg-Fe interdiffusion in <span class="hlt">olivine</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sio, C. K. I.; Roskosz, M.; Dauphas, N.; Bennett, N.; Mock, T. D.; Shahar, A.</p> <p>2017-12-01</p> <p>Isotopic fractionation provides the most direct means to investigate the nature of chemical zoning in minerals, which can be produced by either diffusive transport or crystal growth. Misinterpreting the nature of chemical zoning can result in erroneous conclusions regarding magmatic cooling rates and diffusion timescales. Isotopes are useful in this regard because the light isotopes diffuse faster than their heavier counterparts. As a result, isotopic fractionations should be associated with chemical zoning profiles if they are diffusion-driven. In contrast, little isotopic fractionation is associated with crystal growth during slow cooling at magmatic temperatures. The isotope effect for diffusion is described by β and is related to the mass (m) and diffusivity (D) of isotopes i and j of an element via: Di/Dj = (mj/mi)β. To model isotopic profiles, knowledge of β is required. Several estimates of β for Mg and Fe diffusion in <span class="hlt">olivine</span> have been reported using natural samples but these estimates are uncertain because they depend on the choice of modeling parameters (Sio et al., 2013; Oeser et al., 2015; Collinet et al., 2017). We have experimentally determined β for Fe (βFe) in <span class="hlt">olivine</span> as a function of crystallographic orientation, composition, and temperature. Thirty experiments have been conducted by juxtaposing crystallographically oriented <span class="hlt">olivine</span> crystals to make Fo83.4-Fo88.8 and Fo88.8-Fo100 diffusion couples. These diffusion couples were annealed in a 1 atm gas mixing furnace at 1200 °C, 1300 °C or 1400 °C at QFM - 1.5 for up to 15 days. Chemical profiles were characterized using an electron microprobe and isotopic analyses were done using laser ablation MC-ICPMS. We found a crystallographic dependence of βFe for the Fo88.8-Fo100 couple where βFe [100] ≈ βFe [010] > βFe [001]. For the Fo83.4-Fo88.8 couple, βFe is 0.16 ± 0.09 (2σ) for all 3 major crystallographic axes. A temperature dependence of βFe could not be resolved. These</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1981tcs..meet.....P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1981tcs..meet.....P"><span>Evaluation of <span class="hlt">olivine</span> ceramic refractories for thermal-energy-storage application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Palmour, H., III; Gay, B. M.; Cochran, R. L.</p> <p></p> <p>The degree of improvement in thermal and mechanical performance that can be obtained with an <span class="hlt">olivine</span> thermal storage brick made of domestic materials using advanced processing techniques compared with state-of-the-art as represented by commercial European bricks is discussed. The goals and results of the study are given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008GeCoA..72.4397B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008GeCoA..72.4397B"><span>Oxygen isotope heterogeneity and disequilibria of <span class="hlt">olivine</span> crystals in large volume Holocene basalts from Iceland: Evidence for magmatic digestion and erosion of Pleistocene hyaloclastites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bindeman, Ilya; Gurenko, Andrey; Sigmarsson, Olgeir; Chaussidon, Marc</p> <p>2008-09-01</p> <p>This work considers petrogenesis of the largest Holocene basaltic fissure eruptions of Iceland, which are also the largest in the world: Laki (1783-84 AD, 15 km 3), Eldgjá (934 AD, 18 km 3), Veidivötn (900, 1480 AD, multiple eruptions, >2 km 3), Núpahraun (ca. 4000 BP, >1 km 3) and Thjórsárhraun (ca 8000 BP, >20 km 3). We present oxygen isotope laser fluorination analyses of 55 individual and bulk <span class="hlt">olivine</span> crystals, coexisting individual and bulk plagioclase phenocrysts, and their host basaltic glasses with average precision of better than 0.1‰ (1SD). We also report O isotope analyses of cores and rims of 61 <span class="hlt">olivine</span> crystals by SIMS with average precision on single spots of 0.24‰ (1SD) in 13 samples coupled with electron microprobe data for major and trace elements in these <span class="hlt">olivines</span>. Within each individual sample, we have found that basaltic glass is relatively homogeneous with respect to oxygen isotopes, plagioclase phenocrysts exhibit crystal to crystal variability, while individual <span class="hlt">olivines</span> span from the values in equilibrium with the low-δ 18O matrix glass to those being three permil higher in δ 18O than the equilibrium. <span class="hlt">Olivine</span> cores with maximum value of 5.2‰ are found in many of these basalts and suggest that the initial magma was equilibrated with normal-δ 18O mantle. No <span class="hlt">olivines</span> or their intracrystalline domains are found with bulk or spot value higher than those found in MORB <span class="hlt">olivines</span>. The δ 18O variability of 0.3-3‰ exists for <span class="hlt">olivine</span> grains from different lavas, and variable core-to-rim oxygen isotopic zoning is present in selected <span class="hlt">olivine</span> grains. Many <span class="hlt">olivines</span> in the same sample are not zoned, while a few grains are zoned with respect to oxygen isotopes and exhibit small core-to-core variations in Fe-Mg, Ni, Mn, Ca. Grains that are zoned in both Mg# and δ 18O exhibit positive correlation of these two parameters. Electron microprobe analysis shows that most <span class="hlt">olivines</span> equilibrated with the transporting melt, and thin Fe-richer rim is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.T33D..05D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.T33D..05D"><span>Alignment of <span class="hlt">olivine</span> crystals during diffusion creep in oceanic peridotite mylonites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Deems, N. J.; Warren, J. M.; Wolfson-Schwehr, M.</p> <p>2014-12-01</p> <p>At small grain sizes (<10 µm), <span class="hlt">olivine</span> is expected to deform by diffusion creep at lithospheric conditions. Microstructural analysis by electron backscatter diffraction of 13 peridotite mylonites from St. Paul's Rocks (SPR) indicates that <span class="hlt">olivine</span> has a pronounced axial-[010] lattice preferred orientation (i.e. [010] clusters perpendicular to foliation, while [100] and [001] are dispersed in the foliation plane) and a mean grain size of ~7µm. Holtzman et al. (2003) has observed similar LPOs in partially molten samples experimentally deformed under simple shear at lithospheric conditions. The occurrence of a lattice preferred orientation (LPO) is typically interpreted as indicating deformation by dislocation creep. In addition, compositional maps of the samples show that amphibole (pargasite) is ubiquitous. As the presence of pargasite in peridotites is controlled in part by the activity of plagioclase and water at high temperatures (Lynkins and Jenkins, 1992), we infer this as evidence for the presence of pre- to syn-tectonic trapped melt. In order to explain the observed LPO in SPR mylonites, we evaluate the hypothesis that alignment occurred during diffusion creep, such as observed in experiments by Sundberg and Cooper (2008) and Miyazaki et al., (2013). To explore this hypothesis, we conducted analyses of low angle (2-10°) rotation axis inverse pole figures (IPFs), which can often provide insight into the operative slip system(s). Analyses of low angle IPFs from SPR, however, showed no definitive correlation to any one particular slip system. On the other hand, high angle IPFs showed intense clustering of rotational axes at 75-90° about [010], indicating that [100] and [001] align nearly perpendicular to [010]. Based on the IPF analysis and evidence of pre- to syn-tectonic melt, we conclude that the presence of melt lubricated grain boundaries, which resulted in rigid rotation of grains and alignment of the [010] axes controlled by the orthorhombic crystal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR23A..07M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR23A..07M"><span>Densification and Grain Growth in Polycrystalline <span class="hlt">Olivine</span> Rocks Synthesized By Evacuated Hot-Pressing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meyers, C. D.; Kohlstedt, D. L.; Zimmerman, M. E.</p> <p>2017-12-01</p> <p>Experiments on laboratory-synthesized <span class="hlt">olivine</span>-rich rocks form the starting material for many investigations of physical processes in the Earth's upper mantle (e.g., creep behavior, ionic diffusion, and grain growth). Typically, a fit of a constitutive law to experimental data provides a description of the kinetics of a process needed to extrapolate across several orders of magnitude from laboratory to geological timescales. Although grain-size is a critical parameter in determining physical properties such as viscosity, broad disagreement persists amongst the results of various studies of grain growth kinetics in <span class="hlt">olivine</span>-rich rocks. Small amounts of impurities or porosity dramatically affect the kinetics of grain growth. In this study, we developed an improved method for densifying <span class="hlt">olivine</span>-rich rocks fabricated from powdered, gem-quality single crystals that involves evacuating the pore space, with the aim of refining measurements of the kinetics of mantle materials. In previous studies, <span class="hlt">olivine</span> powders were sealed in a metal can and hydrostatically annealed at roughly 300 MPa and 1250 °C. These samples, which appear opaque and milky-green, typically retain a small amount of porosity. Consequently, when annealed at 1 atm, extensive pore growth occurs, inhibiting grain growth. In addition, Fourier-transform infrared and confocal Raman spectroscopy reveal absorption peaks characteristic of CO2 in the pores of conventionally hot-pressed material. To avoid trapping of adsorbed contaminants, we developed an evacuated hot-pressing method, wherein the pore space of powder compacts is vented to vacuum during heating and pressurization. This method produces a highly dense, green-tinted, transparent material. No CO2 absorptions peaks exist in evacuated hot-pressed material. When reheated to annealing temperatures at 1 atm, the evacuated hot-pressed material undergoes limited pore growth and dramatically enhanced grain-growth rates. High-strain deformation experiments on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20020086706','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20020086706"><span><span class="hlt">Bar</span> Code Labels</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1988-01-01</p> <p>American <span class="hlt">Bar</span> Codes, Inc. developed special <span class="hlt">bar</span> code labels for inventory control of space shuttle parts and other space system components. ABC labels are made in a company-developed anodizing aluminum process and consecutively marketed with <span class="hlt">bar</span> code symbology and human readable numbers. They offer extreme abrasion resistance and indefinite resistance to ultraviolet radiation, capable of withstanding 700 degree temperatures without deterioration and up to 1400 degrees with special designs. They offer high resistance to salt spray, cleaning fluids and mild acids. ABC is now producing these <span class="hlt">bar</span> code labels commercially or industrial customers who also need labels to resist harsh environments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940019898','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940019898"><span>A dynamic melting model for the origin of Apollo 15 <span class="hlt">olivine</span>-normative and quartz-normative mare basalts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vetter, Scott K.; Shervais, John W.</p> <p>1993-01-01</p> <p>Early studies of mare basalts from the Apollo 15 site established that two distinct groups are represented: the <span class="hlt">olivine</span>-normative basalts (ONB) and the quartz-normative basalts (QNB). The ONB and QNB suites are distinguished petrographically by their phenocryst assemblages (the ONB's are <span class="hlt">olivine</span>-phyric, the QNB's are generally pyroxene-phyric) and chemically by their major element compositions: the QNB's are higher in SiO2 and MgO/FeO, and lower in FeO and TiO2 than ONB's with similar MgO contents. Experimental data show that the QNB suite is derived from a more magnesian, <span class="hlt">olivine</span>-normative parent magma, a conclusion which is supported by the recent discovery of high-SiO2 <span class="hlt">olivine</span>-normative basalt clasts in breccia 15498. The high-SiO2 ONB's fall on <span class="hlt">olivine</span> control lines with primitive QNB's, and least-squares mixing calculations are consistent with the high-SiO2 ONB's being parental to the more evolved QNB suite. These high-SiO2 ONB's are included as part of the 'QNB suite'. Our major element modeling results also are consistent with the conclusions of earlier studies which showed that the ONB and QNB suites cannot be related to one another by low pressure crystal fractionation. The combination of high Mg#, high SiO2, and low TiO2 in the QNB suite precludes a relationship to the ONB suite by simple removal of liquidus minerals (<span class="hlt">olivine</span> and pigeonite). Despite these significant differences in petrography and major element composition, both groups have nearly identical trace element concentrations and chondrite-normalized abundance patterns. The major question to be addressed by any petrogenetic model for Apollo 15 mare basalts is how to form mare basalt suites with distinctly different major element characteristics but nearly identical trace element compositions. The similarity in trace element concentrations imply compositionally similar source regions and similar percent melting, but these conclusions are not easily reconciled with the observed differences in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LPICo2085.6047S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LPICo2085.6047S"><span>Prevalence of the Ancient Wood-Ljungdahl Pathway in a Subseafloor <span class="hlt">Olivine</span> Community</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, A. R.; Mueller, R.; Fisk, M. R.; Mason, O. U.; Popa, R.; Kieft, B.; Colwell, F. S.</p> <p>2018-05-01</p> <p>The ancient Wood-Ljungdahl pathway used for biosynthesis and energy generation was found to be the predominant metabolic pathway in a microbial community from <span class="hlt">olivine</span> grains incubated in the Juan de Fuca subseafloor aquifer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870064149&hterms=amoeba&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Damoeba','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870064149&hterms=amoeba&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Damoeba"><span>Alteration of Al-rich inclusions inside amoeboid <span class="hlt">olivine</span> aggregates in the Allende meteorite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hashimoto, Akihiko; Grossman, Lawrence</p> <p>1987-01-01</p> <p>The primary phases of Al-rich inclusions in amoeboid <span class="hlt">olivine</span> aggregates have undergone alteration reactions with the solar nebular gas. The simplest interpretation of the present observations is that melilite was the first primary phase to disappear with falling temperature, and was replaced by grossular + anorthite + feldspathoids, followed by fassaite; spinel was the last phase to be altered. Thermodynamic calculations suggest that Na-rich phlogopite could have formed at about 470 K and chlorite at about 328 K at a water fugacity of 0.000001, which is that of a gas of solar composition in this temperature range. The <span class="hlt">olivine</span> around Al-rich inclusions is not serpentized, indicating the cessation of gas-solid equilibrium above 274 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140000409','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140000409"><span>Ar-Ar and Rb-Sr Ages of the Tissint <span class="hlt">Olivine</span>-phyric Martian Shergottite</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Park, J.; Herzog, G. F.; Nyquist, L. E.; Shih, C.-Y.; Turin, B.; Lindsay, F. N.; Delaney, J. S.; Swisher, C. C., III; Agee, C.</p> <p>2013-01-01</p> <p>The fifth martian meteorite fall, Tissint, is an <span class="hlt">olivine</span>-phyric shergottite that contains <span class="hlt">olivine</span> macrocrysts (approximately 1.5 mm) [1]. [2] reported the Sm-Nd age of Tissint as 596 plus or minus 23 Ma along with Rb-Sr data that defined no isochron. [3] reported Lu-Hf and Sm-Nd ages of 583 plus or minus 86 Ma and 616 plus or minus 67 Ma, respectively. The cosmic-ray exposure ages of Tissint are 1.10 plus or minus 0.15 Ma based on 10Be [4], and 1.0-1.1 Ma, based on 3He, 21Ne, and 38Ar [5,6].We report Ar-Ar ages and Rb-Sr data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25783318','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25783318"><span>The bridge technique for pectus <span class="hlt">bar</span> fixation: a method to make the <span class="hlt">bar</span> un-rotatable.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Park, Hyung Joo; Kim, Kyung Soo; Moon, Young Kyu; Lee, Sungsoo</p> <p>2015-08-01</p> <p>Pectus <span class="hlt">bar</span> rotation is a major challenge in pectus repair. However, to date, no satisfactory technique to completely eliminate <span class="hlt">bar</span> displacement has been introduced. Here, we propose a <span class="hlt">bar</span> fixation technique using a bridge that makes the <span class="hlt">bar</span> unmovable. The purpose of this study was to determine the efficacy of this bridge technique. A total of 80 patients underwent pectus <span class="hlt">bar</span> repair of pectus excavatum with the bridge technique from July 2013 to July 2014. The technique involved connecting 2 parallel <span class="hlt">bars</span> using plate-screws at the ends of the <span class="hlt">bars</span>. To determine <span class="hlt">bar</span> position change, the angles between the sternum and pectus <span class="hlt">bars</span> were measured on postoperative day 5 (POD5) and 4 months (POM4) and compared. The mean patient age was 17.5 years (range, 6-38 years). The mean difference between POD5 and POM4 were 0.23° (P=.602) and 0.35° (P=.338) for the upper and lower <span class="hlt">bars</span>, respectively. <span class="hlt">Bar</span> position was virtually unchanged during the follow-up, and there was no <span class="hlt">bar</span> dislocation or reoperation. A "bridge technique" designed to connect 2 parallel <span class="hlt">bars</span> using plates and screws was demonstrated as a method to avoid pectus <span class="hlt">bar</span> displacement. This approach was easy to implement without using sutures or invasive devices. Copyright © 2015 Elsevier Inc. All rights reserved.</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://adsabs.harvard.edu/abs/2016GeCoA.185..232T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeCoA.185..232T"><span>Magma transport and <span class="hlt">olivine</span> crystallization depths in Kīlauea's east rift zone inferred from experimentally rehomogenized melt inclusions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tuohy, Robin M.; Wallace, Paul J.; Loewen, Matthew W.; Swanson, Donald A.; Kent, Adam J. R.</p> <p>2016-07-01</p> <p>Concentrations of H2O and CO2 in <span class="hlt">olivine</span>-hosted melt inclusions can be used to estimate crystallization depths for the <span class="hlt">olivine</span> host. However, the original dissolved CO2 concentration of melt inclusions at the time of trapping can be difficult to measure directly because in many cases substantial CO2 is transferred to shrinkage bubbles that form during post-entrapment cooling and crystallization. To investigate this problem, we heated <span class="hlt">olivine</span> from the 1959 Kīlauea Iki and 1960 Kapoho (Hawai'i) eruptions in a 1-atm furnace to temperatures above the melt inclusion trapping temperature to redissolve the CO2 in shrinkage bubbles. The measured CO2 concentrations of the experimentally rehomogenized inclusions (⩽590 ppm for Kīlauea Iki [n = 10]; ⩽880 ppm for Kapoho, with one inclusion at 1863 ppm [n = 38]) overlap with values for naturally quenched inclusions from the same samples, but experimentally rehomogenized inclusions have higher within-sample median CO2 values than naturally quenched inclusions, indicating at least partial dissolution of CO2 from the vapor bubble during heating. Comparison of our data with predictions from modeling of vapor bubble formation and published Raman data on the density of CO2 in the vapor bubbles suggests that 55-85% of the dissolved CO2 in the melt inclusions at the time of trapping was lost to post-entrapment shrinkage bubbles. Our results combined with the Raman data demonstrate that <span class="hlt">olivine</span> from the early part of the Kīlauea Iki eruption crystallized at <6 km depth, with the majority of <span class="hlt">olivine</span> in the 1-3 km depth range. These depths are consistent with the interpretation that the Kīlauea Iki magma was supplied from Kīlauea's summit magma reservoir (∼2-5 km depth). In contrast, <span class="hlt">olivine</span> from Kapoho, which was the rift zone extension of the Kīlauea Iki eruption, crystallized over a much wider range of depths (∼1-16 km). The wider depth range requires magma transport during the Kapoho eruption from deep beneath the summit</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890001422','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890001422"><span>Chemical frost weathering of <span class="hlt">olivine</span>: Experimental study and implications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Harris, S. L.; Huguenin, R. L.</p> <p>1987-01-01</p> <p>New experimental results are reported on the frost weathering of <span class="hlt">olivine</span>. After first weathering, a decrease in Fe sup 2(+)M(2) absorption bands were noted. This decrease is related to the protonation of O(+) in the mineral. It is contented that this reaction may result in the regolith storage of 100 to 1000 m of H(sub 2) over the history of Mars.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070034483&hterms=EXERCISE+DEPENDENCE&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DEXERCISE%2BDEPENDENCE','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070034483&hterms=EXERCISE+DEPENDENCE&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DEXERCISE%2BDEPENDENCE"><span>The Effect of Metal Composition on Fe-Ni Partition Behavior between <span class="hlt">Olivine</span> and FeNi-Metal, FeNi-Carbide, FeNi-Sulfide at Elevated Pressure</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holzheid, Astrid; Grove, Timothy L.</p> <p>2005-01-01</p> <p>Metal-<span class="hlt">olivine</span> Fe-Ni exchange distribution coefficients were determined at 1500 C over the pressure range of 1 to 9 GPa for solid and liquid alloy compositions. The metal alloy composition was varied with respect to the Fe/Ni ratio and the amount of dissolved carbon and sulfur. The Fe/Ni ratio of the metal phase exercises an important control on the abundance of Ni in the <span class="hlt">olivine</span>. The Ni abundance in the <span class="hlt">olivine</span> decreases as the Fe/Ni ratio of the coexisting metal increases. The presence of carbon (up to approx. 3.5 wt.%) and sulfur (up to approx. 7.5 wt.%) in solution in the liquid Fe-Ni-metal phase has a minor effect on the partitioning of Fe and Ni between metal and <span class="hlt">olivine</span> phases. No pressure dependence of the Fe-Ni-metal-<span class="hlt">olivine</span> exchange behavior in carbon- and sulfur-free and carbon- and sulfur-containing systems was found within the investigated pressure range. To match the Ni abundance in terrestrial mantle <span class="hlt">olivine</span>, assuming an equilibrium metal-<span class="hlt">olivine</span> distribution, a sub-chondritic Fe/Ni-metal ratio that is a factor of 17 to 27 lower than the Fe/Ni ratios in estimated Earth core compositions would be required, implying higher Fe concentrations in the core forming metal phase. A simple metal-<span class="hlt">olivine</span> equilibrium distribution does not seem to be feasible to explain the Ni abundances in the Earth's mantle. An equilibrium between metal and <span class="hlt">olivine</span> does not exercise a control on the problem of Ni overabundance in the Earth's mantle. The experimental results do not contradict the presence of a magma ocean at the time of terrestrial core formation, if <span class="hlt">olivine</span> was present in only minor amounts at the time of metal segregation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.6264S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.6264S"><span><span class="hlt">Olivine</span> tablets in peridotite xenoliths: Evidence for a static, foliation-producing recrystallization mechanism operative in the strained, fluid-bearing mantle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Špaček, Petr; Habler, Gerlinde; Krmíček, Lukáš; Libowitzky, Eugen</p> <p>2014-05-01</p> <p>The term "<span class="hlt">olivine</span> tablet" is used for elongated, (sub-)idiomorphic, strain-free crystals of <span class="hlt">olivine</span> with well developed parallel crystal faces, usually found in peridotite xenoliths. While only rarely occurring in basalt-hosted xenolith suites, such peculiar grains are relatively common in specific kimberlite-hosted peridotite xenoliths and often explained as a result of fluid-assisted recrystallization in xenoliths after their entrainment in host magma. Extremely well developed <span class="hlt">olivine</span> tablets are common in some peridotite xenoliths from Pliocene Lutynia basanite (South Poland). These were studied in detail focusing on their crystallographic orientation and chemical composition in relation to their host grains, in order to learn more about their origin. The tablets are restricted to grain boundary regions of <span class="hlt">olivine</span>(I) and enstatite or occur pervasively, in some cases constituting more than half of the rock volume. Together with strain-free mosaic grains they form a second generation of <span class="hlt">olivine</span> growing at the expense of older and larger, strained <span class="hlt">olivine</span>(I) grains. The tablets are typically 0.1-1 mm (up to 3 mm) long having typical aspect ratios of 2-3 (up to >10) and exhibit a strong shape preferred orientation at local scale or in the whole sample, in the latter case forming a distinct foliation in peridotite xenoliths. Tablet grains usually exhibit a lattice preferred orientation (LPOs) similar to the host <span class="hlt">olivine</span>(I), suggesting that their orientation is inherited, likely by selective exaggerated growth of small grains at the margins of host grains (dynamically recrystallized grains were not observed directly). In some cases oriented growth of tablets along microcrackss, or planar sliding surfaces, is suggested by the microstructures. Traces of prominent tablet faces mostly correspond to (010) planes of tablet grains, while correlation to crystallographic orientations of host grains is poor. Compositional profiles across tablet/host grain boundaries (EMPA, long</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Litho.266..362X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Litho.266..362X"><span>Al-in-<span class="hlt">olivine</span> thermometry evidence for the mantle plume origin of the Emeishan large igneous province</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Rong; Liu, Yongsheng</p> <p>2016-12-01</p> <p>The Emeishan large igneous province (ELIP) is renowned for its world-class Ni-Cu-(PGE) deposits and its link with the Capitanian mass extinction. The ELIP is generally thought to be associated with a deep mantle plume; however, evidence for such a model has been challenged through geology, geophysics and geochemistry. In many large igneous province settings, <span class="hlt">olivine</span>-melt equilibrium thermometry has been used to argue for or against the existence of plumes. However, this method involves large uncertainties such as assumptions regarding melt compositions and crystallisation pressures. The Al-in-<span class="hlt">olivine</span> thermometer avoids these uncertainties and is used here to estimate the temperatures of picrites in the ELIP. The calculated maximum temperature (1440 °C) is significantly ( 250 °C) higher than the Al-in-<span class="hlt">olivine</span> temperature estimated for the average MORB, thus providing compelling evidence for the existence of thermal mantle plumes in the ELIP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ERL....11b4007H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ERL....11b4007H"><span>Iron fertilisation and century-scale effects of open ocean dissolution of <span class="hlt">olivine</span> in a simulated CO2 removal experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hauck, Judith; Köhler, Peter; Wolf-Gladrow, Dieter; Völker, Christoph</p> <p>2016-02-01</p> <p>Carbon dioxide removal (CDR) approaches are efforts to reduce the atmospheric CO2 concentration. Here we use a marine carbon cycle model to investigate the effects of one CDR technique: the open ocean dissolution of the iron-containing mineral <span class="hlt">olivine</span>. We analyse the maximum CDR potential of an annual dissolution of 3 Pg <span class="hlt">olivine</span> during the 21st century and focus on the role of the micro-nutrient iron for the biological carbon pump. Distributing the products of <span class="hlt">olivine</span> dissolution (bicarbonate, silicic acid, iron) uniformly in the global surface ocean has a maximum CDR potential of 0.57 gC/g-<span class="hlt">olivine</span> mainly due to the alkalinisation of the ocean, with a significant contribution from the fertilisation of phytoplankton with silicic acid and iron. The part of the CDR caused by ocean fertilisation is not permanent, while the CO2 sequestered by alkalinisation would be stored in the ocean as long as alkalinity is not removed from the system. For high CO2 emission scenarios the CDR potential due to the alkalinity input becomes more efficient over time with increasing ocean acidification. The alkalinity-induced CDR potential scales linearly with the amount of <span class="hlt">olivine</span>, while the iron-induced CDR saturates at 113 PgC per century (on average ˜ 1.1 PgC yr-1) for an iron input rate of 2.3 Tg Fe yr-1 (1% of the iron contained in 3 Pg <span class="hlt">olivine</span>). The additional iron-related CO2 uptake occurs in the Southern Ocean and in the iron-limited regions of the Pacific. Effects of this approach on surface ocean pH are small (\\lt 0.01).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMMR23A2637B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMMR23A2637B"><span>In Situ Deformation of <span class="hlt">Olivine</span> in the Transmission Electron Microscope: from Dislocation Velocity Measurements to Stress-Strain Curves</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bollinger, C.; Idrissi, H.; Boioli, F.; Cordier, P.</p> <p>2015-12-01</p> <p>There is a growing consensus to recognize that rheological law established for <span class="hlt">olivine</span> at high-temperature (ca. >1000°C) fail when extrapolated to low temperatures relevant for the lithospheric mantle. Hence it appears necessary to fit rheological laws against data at low temperatures where <span class="hlt">olivine</span> tends to become more and more brittle. The usual approach consists in applying confining pressure to inhibit brittleness. Here we propose an innovative approach based on the use of very small samples and numerical modelling. New commercial in situ TEM nanotensile testing equipment recently developed by Hysitron.Inc is combined with weak-beam dark-field TEM diffraction contrast imaging in order to obtain information on the elementary mechanisms controlling the plasticity of <span class="hlt">olivine</span>: namely glide of [001] screw dislocations. The <span class="hlt">olivine</span> tensile beams dedicated for in situ TEM nanomechanical testing were produced using microfabrication techniques based on MEMS-type procedures. The testing geometry was designed as to induce maximum resolved shear stresses on the [001](110) slip system. Under tensile loads between 2 and 3 GPa, ductile behaviour was reached with the development and propagation of dislocation loops across the sample allowing to measure the velocity of screw and non-screw dislocations as a function of stress. This information is introduced into a numerical model involving Dislocation Dynamics in order to obtain the stress-strain curves describing the mechanical response of <span class="hlt">olivine</span> single crystals deformed in tension at room temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930032111&hterms=weinberg&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3Dweinberg','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930032111&hterms=weinberg&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAuthor-Name%26N%3D0%26No%3D90%26Ntt%3Dweinberg"><span><span class="hlt">Bar</span>-spheroid interaction in galaxies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hernquist, Lars; Weinberg, Martin D.</p> <p>1992-01-01</p> <p>N-body simulation and linear analysis is employed to investigate the secular evolution of <span class="hlt">barred</span> galaxies, with emphasis on the interaction between <span class="hlt">bars</span> and spheroidal components of galaxies. This interaction is argued to drive secular transfer of angular momentum from <span class="hlt">bars</span> to spheroids, primarily through resonant coupling. A moderately strong <span class="hlt">bar</span>, having mass within corotation about 0.3 times the enclosed spheroid mass, is predicted to shed all its angular momentum typically in less than about 10 exp 9 yr. Even shorter depletion time scales are found for relatively more massive <span class="hlt">bars</span>. It is suggested either that spheroids around <span class="hlt">barred</span> galaxies are structured so as to inhibit strong coupling with <span class="hlt">bars</span>, or that <span class="hlt">bars</span> can form by unknown processes long after disks are established. The present models reinforce the notion that <span class="hlt">bars</span> can drive secular evolution in galaxies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI11A2337T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI11A2337T"><span>The Thermal Evolution of the Galapagos Mantle Plume: Insights from Al-in-<span class="hlt">Olivine</span> Thermometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Trela, J.; Gazel, E.; Sobolev, A. V.; Class, C.; Bizimis, M.; Jicha, B. R.; Batanova, V. G.; Denyer, P.</p> <p>2016-12-01</p> <p>The mantle plume hypothesis is widely accepted for the formation of large igneous provinces (LIP) and many ocean island basalts (OIB). Petrologic models support a mantle plume origin by indicating high mantle temperatures (>1500 °C) for some plume-melts relative to melts generated at ambient mid ocean ridge conditions (1350 °C). Mantle plumes forming LIPs and OIBs provide our primary source of information on the geochemical and lithological heterogeneity of the lower mantle. The Galapagos hotspot represents one of the most thermally and geochemically heterogeneous plumes on the planet, sustaining long-lived isotopic and lithological heterogeneity over its 90 Ma evolution. Previous petrologic studies showed that the Galapagos plume secularly cooled over time and that the decrease in the plume's temperature correlates with an increase in a recycled (pyroxenite) component. We used Al-in-<span class="hlt">olivine</span> thermometry to show that maximum <span class="hlt">olivine</span> crystallization temperatures confirm secular cooling of the Galapagos plume. <span class="hlt">Olivines</span> from the early melting stages of the plume at 90 Ma (Caribbean LIP) record the highest crystallization temperatures (1600 °C). <span class="hlt">Olivines</span> from the current archipelago record the lowest temperatures of only 1300 °C. The largest decrease in temperature occurred between 90 and 70 Ma ( 200 °C decrease) and coincides with the plume head-tail transition. <span class="hlt">Olivines</span> from the 60-90 Ma-old accreted Galapagos-tracks in Costa Rica and Panama record higher Ni, Fe/Mn, and lower Ca contents than those from the present-day archipelago, indicating a higher abundance of pyroxenite (recycled oceanic crust) entrained in parts of the plume head that melted to form the Caribbean LIP. However, the Galapagos plume was pyroxenite-rich for 40 Ma thus pyroxenite-entrainment goes beyond the plume-tail transition. Our results suggest that hotter regions of the Galapagos plume entrained larger amounts of dense, recycled components due to their greater buoyancy; however, this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.207..277C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.207..277C"><span>Crystallization history of enriched shergottites from Fe and Mg isotope fractionation in <span class="hlt">olivine</span> megacrysts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Collinet, Max; Charlier, Bernard; Namur, Olivier; Oeser, Martin; Médard, Etienne; Weyer, Stefan</p> <p>2017-06-01</p> <p>Martian meteorites are the only samples available from the surface of Mars. Among them, <span class="hlt">olivine</span>-phyric shergottites are basalts containing large zoned <span class="hlt">olivine</span> crystals with highly magnesian cores (Fo 70-85) and rims richer in Fe (Fo 45-60). The Northwest Africa 1068 meteorite is one of the most primitive "enriched" shergottites (high initial 87Sr/86Sr and low initial ε143Nd). It contains <span class="hlt">olivine</span> crystals as magnesian as Fo 77 and is a major source of information to constrain the composition of the parental melt, the composition and depth of the mantle source, and the cooling and crystallization history of one of the younger magmatic events on Mars (∼180 Ma). In this study, Fe-Mg isotope profiles analyzed in situ by femtosecond-laser ablation MC-ICP-MS are combined with compositional profiles of major and trace elements in <span class="hlt">olivine</span> megacrysts. The cores of <span class="hlt">olivine</span> megacrysts are enriched in light Fe isotopes (δ56FeIRMM-14 = -0.6 to -0.9‰) and heavy Mg isotopes (δ26MgDSM-3 = 0-0.2‰) relative to megacryst rims and to the bulk martian isotopic composition (δ56Fe = 0 ± 0.05‰, δ26Mg = -0.27 ± 0.04‰). The flat forsterite profiles of megacryst cores associated with anti-correlated fractionation of Fe-Mg isotopes indicate that these elements have been rehomogenized by diffusion at high temperature. We present a 1-D model of simultaneous diffusion and crystal growth that reproduces the observed element and isotope profiles. The simulation results suggest that the cooling rate during megacryst core crystallization was slow (43 ± 21 °C/year), and consistent with pooling in a deep crustal magma chamber. The megacryst rims then crystallized 1-2 orders of magnitude faster during magma transport toward the shallower site of final emplacement. Megacryst cores had a forsterite content 3.2 ± 1.5 mol% higher than their current composition and some were in equilibrium with the whole-rock composition of NWA 1068 (Fo 80 ± 1.5). NWA 1068 composition is thus close to a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LPICo2085.6019Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LPICo2085.6019Z"><span>Dissolution Rates and Reaction Products of <span class="hlt">Olivine</span> Interaction with Ammonia-Rich Fluid</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zandanel, A. E.; Truche, L.; Hellmann, R.; Tobie, G.; Marrocchi, Y.</p> <p>2018-05-01</p> <p><span class="hlt">Olivine</span> dissolution rates and reaction products in NH3-rich fluids are determined from experiments simulating H2O-rock interaction on Enceladus. Kinetic rates are calculated from flow through experiments and reaction products from static experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PMag...97.3172M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PMag...97.3172M"><span>Hardening mechanisms in <span class="hlt">olivine</span> single crystal deformed at 1090 °C: an electron tomography study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mussi, Alexandre; Cordier, Patrick; Demouchy, Sylvie; Hue, Benoit</p> <p>2017-11-01</p> <p>The dislocation microstructures in a single crystal of <span class="hlt">olivine</span> deformed experimentally in uniaxial compression at 1090 °C and under a confining pressure of 300 MPa, have been investigated by transmission electron tomography in order to better understand deformation mechanisms at the microscale relevant for lithospheric mantle deformations. Investigation by electron tomography reveals microstructures, which are more complex than previously described, composed of ? and ? dislocations commonly exhibiting 3D configurations. Numerous mechanisms such as climb, cross-slip, double cross-slip as well as interactions like junction formations and collinear annihilations are the source of this complexity. The diversity observed advocates for microscale deformation of <span class="hlt">olivine</span> significantly less simple than classic dislocation creep reported in metals or ice close to melting temperature. Deciphering mechanism of hardening in <span class="hlt">olivine</span> at temperatures where ionic diffusion is slow and is then expected to play very little role is crucial to better understand and thus model deformation at larger scale and at temperatures (900-1100 °C) highly relevant for the lithospheric mantle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GGG....17.4725M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GGG....17.4725M"><span>The temperature of the Icelandic mantle from <span class="hlt">olivine</span>-spinel aluminum exchange thermometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matthews, S.; Shorttle, O.; Maclennan, J.</p> <p>2016-11-01</p> <p>New crystallization temperatures for four eruptions from the Northern Volcanic Zone of Iceland are determined using <span class="hlt">olivine</span>-spinel aluminum exchange thermometry. Differences in the <span class="hlt">olivine</span> crystallization temperatures between these eruptions are consistent with variable extents of cooling during fractional crystallization. However, the crystallization temperatures for Iceland are systematically offset to higher temperatures than equivalent <span class="hlt">olivine</span>-spinel aluminum exchange crystallization temperatures published for MORB, an effect that cannot be explained by fractional crystallization. The highest observed crystallization temperature in Iceland is 1399 ± 20°C. In order to convert crystallization temperatures to mantle potential temperature, we developed a model of multilithology mantle melting that tracks the thermal evolution of the mantle during isentropic decompression melting. With this model, we explore the controls on the temperature at which primary melts begin to crystallize, as a function of source composition and the depth from which the magmas are derived. Large differences (200°C) in crystallization temperature can be generated by variations in mantle lithology, a magma's inferred depth of origin, and its thermal history. Combining this model with independent constraints on the magma volume flux and the effect of lithological heterogeneity on melt production, restricted regions of potential temperature-lithology space can be identified as consistent with the observed crystallization temperatures. Mantle potential temperature is constrained to be 1480-30+37 °C for Iceland and 1318-32+44 °C for MORB.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1083045','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1083045"><span>Triple <span class="hlt">bar</span>, high efficiency mechanical sealer</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Pak, Donald J.; Hawkins, Samantha A.; Young, John E.</p> <p>2013-03-19</p> <p>A clamp with a bottom clamp <span class="hlt">bar</span> that has a planar upper surface is provided. The clamp may also include a top clamp <span class="hlt">bar</span> connected to the bottom clamp <span class="hlt">bar</span>, and a pressure distribution <span class="hlt">bar</span> between the top clamp <span class="hlt">bar</span> and the bottom clamp <span class="hlt">bar</span>. The pressure distribution <span class="hlt">bar</span> may have a planar lower surface in facing relation to the upper surface of the bottom clamp <span class="hlt">bar</span>. An object is capable of being disposed in a clamping region between the upper surface and the lower surface. The width of the planar lower surface may be less than the width of the upper surface within the clamping region. Also, the pressure distribution <span class="hlt">bar</span> may be capable of being urged away from the top clamp <span class="hlt">bar</span> and towards the bottom clamp <span class="hlt">bar</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.U13B..22K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.U13B..22K"><span>Size effects in <span class="hlt">olivine</span> control strength in low-temperature plasticity regime</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumamoto, K. M.; Thom, C.; Wallis, D.; Hansen, L. N.; Armstrong, D. E. J.; Goldsby, D. L.; Warren, J. M.; Wilkinson, A. J.</p> <p>2017-12-01</p> <p>The strength of the lithospheric mantle during deformation by low-temperature plasticity controls a range of geological phenomena, including lithospheric-scale strain localization, the evolution of friction on deep seismogenic faults, and the flexure of tectonic plates. However, constraints on the strength of <span class="hlt">olivine</span> in this deformation regime are difficult to obtain from conventional rock-deformation experiments, and previous results vary considerably. We demonstrate via nanoindentation that the strength of <span class="hlt">olivine</span> in the low-temperature plasticity regime is dependent on the length-scale of the test, with experiments on smaller volumes of material exhibiting larger yield stresses. This "size effect" has previously been explained in engineering materials as a result of the role of strain gradients and associated geometrically necessary dislocations in modifying plastic behavior. The Hall-Petch effect, in which a material with a small grain size exhibits a higher strength than one with a large grain size, is thought to arise from the same mechanism. The presence of a size effect resolves discrepancies among previous experimental measurements of <span class="hlt">olivine</span>, which were either conducted using indentation methods or were conducted on polycrystalline samples with small grain sizes. An analysis of different low-temperature plasticity flow laws extrapolated to room temperature reveals a power-law relationship between length-scale (grain size for polycrystalline deformation and contact radius for indentation tests) and yield strength. This suggests that data from samples with large inherent length scales best represent the plastic strength of the coarse-grained lithospheric mantle. Additionally, the plastic deformation of nanometer- to micrometer-sized asperities on fault surfaces may control the evolution of fault roughness due to their size-dependent strength.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21498874','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21498874"><span><span class="hlt">Barring</span> intervention? Lesbian and gay <span class="hlt">bars</span> as an underutilized venue for tobacco interventions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Leibel, Katherine; Lee, Joseph G L; Goldstein, Adam O; Ranney, Leah M</p> <p>2011-07-01</p> <p>Lesbian, gay, bisexual, and transgender (LGBT) communities are at high risk for tobacco use. While LGBT communities have historically considered <span class="hlt">bars</span> to be safe places to socialize and congregate, these spaces are often tobacco-friendly environments and may have potential as sites for much needed intervention. Only a few public health interventions have attempted to work through <span class="hlt">bars</span> and clubs to decrease tobacco use in the LGBT populations. Evidence from HIV prevention suggests some potential interventions in <span class="hlt">bars</span>, and the tobacco industry has worked extensively (and successfully) to utilize <span class="hlt">bars</span> in marketing efforts. Lesbian and gay <span class="hlt">bars</span> are underutilized in tobacco control, suggesting missed avenues for chronic disease prevention programs. Researchers and communities should continue to recognize the importance of clean indoor air laws covering <span class="hlt">bars</span> and develop additional strategies for reaching LGBT populations with disparities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760056430&hterms=Glasses+SiO2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DGlasses%2BSiO2','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760056430&hterms=Glasses+SiO2&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DGlasses%2BSiO2"><span>The origin of <span class="hlt">chondrules</span> - Experimental investigation of metastable liquids in the system Mg2SiO4-SiO2</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Blander, M.; Planner, H. N.; Keil, K.; Nelson, L. S.; Richardson, N. L.</p> <p>1976-01-01</p> <p>Laser-melted magnesium silicate droplets were supercooled 400-750 C below their equilibrium liquidus temperatures before crystallization and their texture was compared with that of meteoritic and lunar <span class="hlt">chondrules</span>. Crystal morphology, width and texture were studied in relation to nucleation temperature and bulk composition. It was found that the only phase to nucleate from the forsterite-enstatite normative melts was forsterite. Highly siliceous glass, about 65% SiO2 by weight, was identified interstitially to the forsterite crystals in seven of the MgSiO4 spherules and was thought to be present in all.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeCoA.212..196V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeCoA.212..196V"><span>The parent body controls on cosmic spherule texture: Evidence from the oxygen isotopic compositions of large micrometeorites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Ginneken, M.; Gattacceca, J.; Rochette, P.; Sonzogni, C.; Alexandre, A.; Vidal, V.; Genge, M. J.</p> <p>2017-09-01</p> <p>High-precision oxygen isotopic compositions of eighteen large cosmic spherules (>500 μm diameter) from the Atacama Desert, Chile, were determined using IR-laser fluorination - Isotope Ratio Mass spectrometry. The four discrete isotopic groups defined in a previous study on cosmic spherules from the Transantarctic Mountains (Suavet et al., 2010) were identified, confirming their global distribution. Approximately 50% of the studied cosmic spherules are related to carbonaceous chondrites, 38% to ordinary chondrites and 12% to unknown parent bodies. Approximately 90% of <span class="hlt">barred</span> <span class="hlt">olivine</span> (BO) cosmic spherules show oxygen isotopic compositions suggesting they are related to carbonaceous chondrites. Similarly, ∼90% porphyritic <span class="hlt">olivine</span> (Po) cosmic spherules are related to ordinary chondrites and none can be unambiguously related to carbonaceous chondrites. Other textures are related to all potential parent bodies. The data suggests that the textures of cosmic spherules are mainly controlled by the nature of the precursor rather than by the atmospheric entry parameters. We propose that the Po texture may essentially be formed from a coarse-grained precursor having an ordinary chondritic mineralogy and chemistry. Coarse-grained precursors related to carbonaceous chondrites (i.e. <span class="hlt">chondrules</span>) are likely to either survive atmospheric entry heating or form V-type cosmic spherules. Due to the limited number of submicron nucleation sites after total melting, ordinary chondrite-related coarse-grained precursors that suffer higher peak temperatures will preferentially form cryptocrystalline (Cc) textures instead of BO textures. Conversely, the BO textures would be mostly related to the fine-grained matrices of carbonaceous chondrites due to the wide range of melting temperatures of their constituent mineral phases, allowing the preservation of submicron nucleation sites. Independently of the nature of the precursors, increasing peak temperatures form glassy textures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI51C0328S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI51C0328S"><span>Detecting metastable <span class="hlt">olivine</span> wedge beneath Japan Sea with deep earthquake coda wave interferometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Z.; Zhan, Z.</p> <p>2017-12-01</p> <p>It has been hypothesized for decades that the lower-pressure <span class="hlt">olivine</span> phase would kinetically persist in the interior of slab into the transition zone, forming a low-velocity "Metastable <span class="hlt">Olivine</span> Wedge" (MOW). MOW, if exists, would play a critical role in generating deep earthquakes and parachuting subducted slabs with its buoyancy. However, seismic evidences for MOW are still controversial, and it is suggested that MOW can only be detected using broadband waveforms given the wavefront healing effects for travel times. On the other hand, broadband waveforms are often complicated by shallow heterogeneities. Here we propose a new method using the source-side interferometry of deep earthquake coda to detect MOW. In this method, deep earthquakes are turned into virtual sensors with the reciprocity theorem, and the transient strain from one earthquake to the other is estimated by cross-correlating the coda from the deep earthquake pair at the same stations. This approach effectively isolates near-source structure from complicated shallow structures, hence provide finer resolution to deep slab structures. We apply this method to Japan subduction zone with Hi-Net data, and our preliminary result does not support a large MOW model (100km thick at 410km) as suggested by several previous studies. Metastable <span class="hlt">olivine</span> at small scales or distributed in an incoherent manner in deep slabs may still be possible.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20050162214&hterms=aluminium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Daluminium','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20050162214&hterms=aluminium&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Daluminium"><span>Chondrites and the Protoplanetary Disk, Part 3</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2004-01-01</p> <p>Contents include the following: Ca-, Al-Rich Inclusions and Ameoboid <span class="hlt">Olivine</span> Aggregates: What We Know and Don t Know About Their Origin. Aluminium-26 and Oxygen Isotopic Distributions of Ca-Al-rich Inclusions from Acfer 214 CH Chondrite. The Trapping Efficiency of Helium in Fullerene and Its Implicatiion to the Planetary Science. Constraints on the Origin of Chondritic Components from Oxygen Isotopic Compositions. Role of Planetary Impacts in Thermal Processing of Chondrite Materials. Formation of the Melilite Mantle of the Type B1 CAIs: Flash Heating or Transport? The Iodine-Xenon System in Outer and Inner Portions of <span class="hlt">Chondrules</span> from the Unnamed Antarctic LL3 Chondrite. Nucleosynthesis of Short-lived Radioactivities in Massive Stars. The Two-Fluid Analysis of the Kelvin-Helmholtz Instability in the Dust Layer of a Protoplanetary Disk: A Possible Path to the Planetesimal Formation Through the Gravitational Instability. Shock-Wave Heating Model for Chonodrule Formation: Heating Rate and Cooling Rate Constraints. Glycine Amide Hydrolysis with Water and OH Radical: A Comparative DFT Study. Micron-sized Sample Preparation for AFM and SEM. AFM, FE-SEM and Optical Imaging of a Shocked L/LL Chondrite: Implications for Martensite Formation and Wave Propagation. Infrared Spectroscopy of Chondrites and Their Components: A Link Between Meteoritics and Astronomy? Mid-Infrared Spectroscopy of CAI and Their Mineral Components. The Origin of Iron Isotope Fractionation in <span class="hlt">Chondrules</span>, CAIs and Matrix from Allende (CV3) and Chainpur (LL3) Chondrites. Protoplanetary Disk Evolution: Early Results from Spitzer. Kinetics of Evaporation-Condensation in a Melt-Solid System and Its Role on the Chemical Composition and Evolution of <span class="hlt">Chondrules</span>. Oxygen Isotope Exchange Recorded Within Anorthite Single Crystal in Vigarano CAI: Evidence for Remelting by High Temperature Process in the Solar Nebula. <span class="hlt">Chondrule</span> Forming Shock Waves in Solar Nebula by X-Ray Flares. Organic Globules with Anormalous</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/2012CoMP..164..959S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012CoMP..164..959S"><span>Settling and compaction of <span class="hlt">olivine</span> in basaltic magmas: an experimental study on the time scales of cumulate formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmidt, Max W.; Forien, Melanie; Solferino, Giulio; Bagdassarov, Nickolai</p> <p>2012-12-01</p> <p>A series of centrifuge-assisted settling experiments of 30 vol % <span class="hlt">olivine</span> in 70 vol % basaltic melt was conducted to elucidate the formation mechanisms and time scales of gravitational cumulates. The settling experiments were performed in a centrifuging piston cylinder at 200-1,500 g, 1,270-1,280 °C, and 0.8-1.1 GPa on previously annealed and texturally equilibrated samples. The mechanical settling of the dense <span class="hlt">olivine</span> suspension occurs at about 1/6 the speed of simple Stokes settling, resulting in a sedimentation exponent n = 4.1(6) in agreement with predictions from analogue systems. The porosity (φ m ) of the orthocumulate resulting from gravitational settling of crystals is about 54 % and formation times of <span class="hlt">olivine</span> orthocumulates result to 0.1-10 m day-1 (for an initial crystal content of the melt of 1-5 % and grain sizes of 2-10 mm). After mechanical settling, <span class="hlt">olivine</span> grains rest on each other, and further compaction occurs through pressure dissolution at grain contacts, <span class="hlt">olivine</span> reprecipitation where <span class="hlt">olivine</span> is in contact with melt, and concomitant expulsion of excess liquid from the cumulate layer. With centrifugation at 400 g for 50 h, porosities as low as 30.3 vol % were achieved. The <span class="hlt">olivine</span> content at the bottom of the gravitational cumulate is 1 - φm ~ log(Δρ · h · a · t), where Δρ is the density difference between crystals and melt, h the crystal layer thickness, a the acceleration, and t the time of centrifuging. Compaction is hence proportional to effective stress integrated over time indicating that pressure dissolution is the dominant mechanism for chemical compaction. The compaction limit, that is the lowermost porosity to be reached by this mechanism, is calculated by equating the lithostatic and hydraulic pressure gradients in the cumulate and results to 3-5 % porosity for the experiments. Crystal size distribution curves and a growth exponent n of 3.1(3) indicate that diffusion-controlled Ostwald ripening is the dominant crystal growth</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29087764','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29087764"><span>Ultrasound-Guided <span class="hlt">Bar</span> Edge Labeling in the Perioperative Assessment of Nuss <span class="hlt">Bar</span> Removal.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Incerti, Filippo; Bertocchini, Alessia; Ghionzoli, Marco; Messineo, Antonio</p> <p>2017-12-01</p> <p>Nuss <span class="hlt">bar</span> removal after minimally invasive repair of pectus excavatum in patients where <span class="hlt">bar</span> ends are not palpable, can be a challenging procedure for the surgeon; a blind dissection toward the <span class="hlt">bar</span> edges may lead to intercostal vessels or deep intercostal muscle injuries. In this article, we describe a fast, repeatable, low-cost technique to detect <span class="hlt">bar</span> edge and stabilizers. A perioperative scan is performed by means of a portable ultrasonograph a few minutes before the operation. The <span class="hlt">bar</span> edge stabilizer is detected as a hyperechogenic image with a concentric crescent while the <span class="hlt">bar</span> edge is detected as a hyperechogenic dashed line with net edges. The scan is performed, and the actual projection on the skin of the metal plaque bulk is then labeled on the patient's chest by an ink marker. We believe that this method may improve morbidity, operative time, and consequently, hospitalization length and costs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI43B0352R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI43B0352R"><span>An Analytical Finite-Strain Parameterization for Texture Evolution in Deformed <span class="hlt">Olivine</span> Polycrystals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ribe, N. M.; Castelnau, O.</p> <p>2017-12-01</p> <p>Current methods for calculating the evolution of flow-induced seismic anisotropy in the upper mantle describe crystal preferred orientation (CPO) using ensembles of 103-104 individual grains, and are too computationally expensive to be used in three-dimensional time-dependent convection models. We propose a much faster method based on the hypothesis that CPO of <span class="hlt">olivine</span> polycrystals is a unique function of the finite strain. Our goal is then to determine how the CPO depends on the ratios r12 and r23 of the axes of the finite strain ellipsoid and on the two independent ratios p12 and p23 of the strengths (critical resolved shear stresses) of the three independent slip systems of <span class="hlt">olivine</span>. To do this, we introduce a new analytical representation of <span class="hlt">olivine</span> CPO in terms of three `structured basis functions' (SBFs) Fs(g, r12, r23) (s = 1, 2, 3), where g is the set of three Eulerian angles that describe the orientation of a crystal lattice relative to an external reference frame. Each SBF represents the virtual CPO that would be produced by the action of only one of the slip systems of <span class="hlt">olivine</span>, and can be determined analytically to within an unknown time-dependent amplitude. The amplitudes are then determined by fitting the SBFs to the predictions of the second-order self-consistent (SOSC) model of Ponte-Castaneda (2002). To implement the SBF representation, we express the orientation distribution function (ODF) f(g) of the polycrystal approximately as a linear superposition of SBFs with weighting coefficients Cs. Substituting the superposition into the general evolution equation for the ODF and minimizing the residual error, we find that the weighting coefficients Cs(t) satisfy coupled evolution equations of the form αisCs + βisCs + γs = 0 where the coefficients αis, βis and γs can be calculated in advance from the expressions for the SBFs. These equations are solved numerically for different values of p12 and p23, yielding numerical values of Cs(r12, r23, p12, p23</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015E%26PSL.432..332M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015E%26PSL.432..332M"><span>Estimates of <span class="hlt">olivine</span>-basaltic melt electrical conductivity using a digital rock physics approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miller, Kevin J.; Montési, Laurent G. J.; Zhu, Wen-lu</p> <p>2015-12-01</p> <p>Estimates of melt content beneath fast-spreading mid-ocean ridges inferred from magnetotelluric tomography (MT) vary between 0.01 and 0.10. Much of this variation may stem from a lack of understanding of how the grain-scale melt geometry influences the bulk electrical conductivity of a partially molten rock, especially at low melt fraction. We compute bulk electrical conductivity of <span class="hlt">olivine</span>-basalt aggregates over 0.02 to 0.20 melt fraction by simulating electric current in experimentally obtained partially molten geometries. <span class="hlt">Olivine</span>-basalt aggregates were synthesized by hot-pressing San Carlos <span class="hlt">olivine</span> and high-alumina basalt in a solid-medium piston-cylinder apparatus. Run conditions for experimental charges were 1.5 GPa and 1350 °C. Upon completion, charges were quenched and cored. Samples were imaged using synchrotron X-ray micro-computed tomography (μ-CT). The resulting high-resolution, 3-dimensional (3-D) image of the melt distribution constitutes a digital rock sample, on which numerical simulations were conducted to estimate material properties. To compute bulk electrical conductivity, we simulated a direct current measurement by solving the current continuity equation, assuming electrical conductivities for <span class="hlt">olivine</span> and melt. An application of Ohm's Law yields the bulk electrical conductivity of the partially molten region. The bulk electrical conductivity values for nominally dry materials follow a power-law relationship σbulk = Cσmeltϕm with fit parameters m = 1.3 ± 0.3 and C = 0.66 ± 0.06. Laminar fluid flow simulations were conducted on the same partially molten geometries to obtain permeability, and the respective pathways for electrical current and fluid flow over the same melt geometry were compared. Our results indicate that the pathways for flow fluid are different from those for electric current. Electrical tortuosity is lower than fluid flow tortuosity. The simulation results are compared to existing experimental data, and the potential</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PPNL...15..240M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PPNL...15..240M"><span>Interference of Nonstandard Interactions with Standard Model in {B^0} \\to {π ^0}\\<span class="hlt">bar</span> vv, B_c^ - \\to {D^ - }\\<span class="hlt">bar</span> vv and \\<span class="hlt">bar</span> B_s^0 \\to {K^0}\\<span class="hlt">bar</span> vv Decays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mahmood, Shakeel; Tahir, Farida; Mir, Azeem</p> <p>2018-05-01</p> <p>We study the contributions of nonstandard neutrino interactions (NSI) to the rare decays of pseudoscalar mesons involving neutrinos in the final state {B^0} \\to {π ^0}\\<span class="hlt">bar</span> vv, B_c^ - \\to {D^ - }\\<span class="hlt">bar</span> vv and \\<span class="hlt">bar</span> B_s^0 \\to {\\<span class="hlt">bar</span> K^0}\\<span class="hlt">bar</span> vv, It is pointed that dominant contribution comes from the interference between standard model and nonstandard interaction We predict limits on NSIs free parameter ɛ uL ττ and compare them with experimental data. We further compare our results with perturbative QCD (pQCD) and QCD results for these reactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR21B0439T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR21B0439T"><span>Sintering mantle mineral aggregates with submicron grains: examples of <span class="hlt">olivine</span> and clinopyroxene</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsubokawa, Y.; Ishikawa, M.</p> <p>2017-12-01</p> <p>Physical property of the major mantle minerals play an important role in the dynamic behavior of the Earth's mantle. Recently, it has been found that nano- to sub-micron scale frictional processes might control faulting processes and earthquake instability, and ultrafine-grained mineral aggregates thus have attracted the growing interest. Here we investigated a method for preparing polycrystalline clinoyproxene and polycrystalline <span class="hlt">olivine</span> with grain size of sub-micron scale from natural crystals, two main constituents of the upper mantle. Nano-sized powders of both minerals are sintered under argon flow at temperatures ranging from 1130-1350 °C for 0.5-20 h. After sintering at 1180 °C and 1300 °C, we successfully fabricated polycrystalline clinopyroxene and polycrystalline <span class="hlt">olivine</span> with grain size of < 500 nm, respectively. Our experiments demonstrate future measurements of ultrafine-grained mineral aggregates on its physical properties of Earth's mantle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.V51C4785G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.V51C4785G"><span>Chemical Analysis of Reaction Rims on <span class="hlt">Olivine</span> Crystals in Natural Samples of Black Dacite Using Energy-Dispersive X-Ray Spectroscopy, Lassen Peak, CA.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Graham, N. A.</p> <p>2014-12-01</p> <p>Lassen Volcanic Center is the southernmost volcanic region in the Cascade volcanic arc formed by the Cascadia Subduction Zone. Lassen Peak last erupted in 1915 in an arc related event producing a black dacite material containing xenocrystic <span class="hlt">olivine</span> grains with apparent orthopyroxene reaction rims. The reaction rims on these <span class="hlt">olivine</span> grains are believed to have formed by reactions that ensued from a mixing/mingling event that occurred prior to eruption between the admixed mafic andesitic magma and a silicic dacite host material. Natural samples of the 1915 black dacite from Lassen Peak, CA were prepared into 15 polished thin sections and carbon coated for analysis using a FEI Quanta 250 Scanning Electron Microscope (SEM) to identify and measure mineral textures and disequilibrium reaction rims. Observed mineralogical textures related to magma mixing include biotite and amphibole grains with apparent dehydration/breakdown rims, pyroxene-rimmed quartz grains, high concentration of microlites in glass matrix, and pyroxene/amphibole reaction rims on <span class="hlt">olivine</span> grains. <span class="hlt">Olivine</span> dissolution is evidenced as increased iron concentration toward convolute edges of <span class="hlt">olivine</span> grains as observed by Backscatter Electron (BSE) imagery and elemental mapping using NSS spectral imaging software. In an attempt to quantify the area of reaction rim growth on <span class="hlt">olivine</span> grains within these samples, high-resolution BSE images of 30 different <span class="hlt">olivine</span> grains were collected along with Energy-Dispersive X-Ray Spectroscopy (EDS) of different phases. <span class="hlt">Olivine</span> cores and rims were extracted from BSE images using Photoshop and saved as separate image files. ImageJ software was used to calculate the area (μm2) of the core and rim of these grains. Average pyroxene reaction rim width for 30 grains was determined to be 11.68+/-1.65 μm. Rim widths of all 30 grains were averaged together to produce an overall average rim width for the Lassen Peak black dacite. By quantifying the reaction rims on <span class="hlt">olivine</span> grains</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT........99H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT........99H"><span>Evolution of the viscosity of Earth's upper mantle: Grain-boundary sliding and the role of microstructure in <span class="hlt">olivine</span> deformation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, Lars N.</p> <p></p> <p>Many features of plate tectonics cannot be explained with standard rheological models of the upper mantle. In particular, the localization of deformation at plate boundaries requires the viscosity of the constituent rocks to evolve spatially and temporally. Such rheological complexity may arise from changing microstructural state variables (e.g., grain size and crystallographic-fabric strength), but the degree to which microstructure contributes to the evolution of viscosity is unclear given our current understanding of deformation mechanisms in mantle minerals. Dislocation-accommodated grain-boundary sliding (GBS) is a potentially critical mechanism for localizing deformation in <span class="hlt">olivine</span> because it imparts a sensitivity of the viscosity to the state of the microstructure while simultaneously providing mechanisms for changing the microstructure. However, many details of GBS in <span class="hlt">olivine</span> are currently unknown including 1) the magnitude of the sensitivity of strain rate to crystallographic fabric and grain size, 2) the strength of the crystallographic fabrics produced, and 3) the anisotropy in viscosity of polycrystalline aggregates. Detailed knowledge of these unknowns is necessary to assess the importance of microstructural evolution in the operation of plate tectonics. This dissertation investigates the details of GBS in <span class="hlt">olivine</span> through four sets of laboratory-based experiments. In Chapter 2, triaxial compressive creep experiments on aggregates of San Carlos <span class="hlt">olivine</span> are used to develop a flow law for <span class="hlt">olivine</span> deforming by GBS. Extrapolations of strain rate to geological conditions using the derived flow law indicate that GBS is the dominant deformation mechanism throughout the uppermost mantle. Crystallographic fabrics observed in deformed samples are consistent with upper-mantle seismic anisotropy. In Chapter 3, torsion experiments on iron-rich <span class="hlt">olivine</span> are used to determine the rheological behavior of <span class="hlt">olivine</span> deforming by GBS at large strains. The sensitivity of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23495560','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23495560"><span>Coffee straw can replace Hader <span class="hlt">bar</span> for <span class="hlt">bar</span> retained overdentures--a clinical report.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guttal, S S; Shetty, U S</p> <p>2012-12-01</p> <p><span class="hlt">Bar</span> attachment system provides retention and support for the overdenture. Retention of a mandibular denture can be achieved by an implant-retained or natural tooth-retained <span class="hlt">bar</span> and stud attachment in the anterior segment of the mandible. A simple and cost effective treatment for more complex implant overdenture is the concept of conventional tooth-retained overdentures. The authors present a clinical report of a patient treated with a mandibular tooth-borne overdenture with a <span class="hlt">bar</span>. The <span class="hlt">bar</span> was fabricated using a coffee straw.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NIMPB.326..126A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NIMPB.326..126A"><span>Annealing behaviour of ion tracks in <span class="hlt">olivine</span>, apatite and britholite</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Afra, B.; Lang, M.; Bierschenk, T.; Rodriguez, M. D.; Weber, W. J.; Trautmann, C.; Ewing, R. C.; Kirby, N.; Kluth, P.</p> <p>2014-05-01</p> <p>Ion tracks were created in <span class="hlt">olivine</span> from San Carlos, Arizona (95% Mg2SiO4), apatite (Ca5(PO4)3(F,Cl,O)) from Durango, Mexico, and synthetic silicates with the apatite structure: Nd8Sr2(SiO4)6O2 and Nd8Ca2(SiO4)6O2 using 1.6 and 2.2 GeV Au ions. The morphology and annealing behaviour of the tracks were investigated by means of synchrotron based small angle X-ray scattering in combination with ex situ annealing. Tracks in <span class="hlt">olivine</span> annealed above ∼400 °C undergo a significant change in track radius due to recrystallisation of the damage tracks. At temperatures higher than 620 °C, the scattering images indicate fragmentation of the track cylinders into smaller subsections. Ion tracks were annealed at elevated temperatures up to 400 °C in the Durango and Ca-britholite, and up to 560 °C in Sr-britholite. While there was a significant change in the track radii in the Durango apatite, tracks in the two synthetic samples remained almost unchanged.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70023640','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70023640"><span><span class="hlt">Olivine</span>-liquid relations of lava erupted by Kilauea volcano from 1994 to 1998: Implications for shallow magmatic processes associated with the ongoing east-rift-zone eruption</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Thornber, C.R.</p> <p>2001-01-01</p> <p>From 1994 through 1998, the eruption of Ki??lauea, in Hawai'i, was dominated by steady-state effusion at Pu'u 'O??'??o that was briefly disrupted by an eruption 4 km uprift at Np??au Crater on January 30, 1997. In this paper, I describe the systematic relations of whole-rock, glass, <span class="hlt">olivine</span>, and <span class="hlt">olivine</span>-inclusion compositions of lava samples collected throughout this interval. This suite comprises vent samples and tube-contained flows collected at variable distances from the vent. The glass composition of tube lava varies systematically with distance and allows for the "vent-correction" of glass thermometry and <span class="hlt">olivine</span>-liquid KD as a function of tube-transport distance. Combined <span class="hlt">olivine</span>-liquid data for vent samples and "vent-corrected" lava-tube samples are used to document pre-eruptive magmatic conditions. KD values determined for matrix glasses and forsterite cores define three types of <span class="hlt">olivine</span> phenocrysts: type A (in equilibrium with host glass), type B (Mg-rich relative to host glass) and type C (Mg-poor relative to host glass). All three types of <span class="hlt">olivine</span> have a cognate association with melts that are present within the shallow magmatic plumbing system during this interval. During steady-state eruptive activity, the compositions of whole-rock, glass and most <span class="hlt">olivine</span> phenocrysts (type A) all vary sympathetically over time and as influenced by changes of magmatic pressure within the summit-rift-zone plumbing system. Type-A <span class="hlt">olivine</span> is interpreted as having grown during passage from the summit magmachamber along the east-rift-zone conduit. Type-B <span class="hlt">olivine</span> (high Fo) is consistent with equilibrium crystallization from bulk-rock compositions and is likely to have grown within the summit magma-chamber. Lower-temperature, fractionated lava was erupted during non-steady state activity of the Na??pau Crater eruption. Type-A and type-B <span class="hlt">olivine</span>-liquid relations indicate that this lava is a mixture of rift-stored and summit-derived magmas. Post-Na??pau lava (at Pu'u 'O?? 'o</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1943b0094B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1943b0094B"><span>Dynamic analysis of four <span class="hlt">bar</span> planar mechanism extended to six-<span class="hlt">bar</span> planar mechanism with variable topology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belleri, Basayya K.; Kerur, Shravankumar B.</p> <p>2018-04-01</p> <p>A computer-oriented procedure for solving the dynamic force analysis problem for general planar mechanisms is presented. This paper provides position analysis, velocity analysis, acceleration analysis and force analysis of six <span class="hlt">bar</span> mechanism with variable topology approach. Six <span class="hlt">bar</span> mechanism is constructed by joining two simple four <span class="hlt">bar</span> mechanisms. Initially the position, velocity and acceleration analysis of first four <span class="hlt">bar</span> mechanism are determined by using the input parameters. The outputs (angular displacement, velocity and acceleration of rocker)of first four <span class="hlt">bar</span> mechanism are used as input parameter for the second four <span class="hlt">bar</span> mechanism and the position, velocity, acceleration and forces are analyzed. With out-put parameters of second four-<span class="hlt">bar</span> mechanism the force analysis of first four-<span class="hlt">bar</span> mechanism is carried out.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5402429','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5402429"><span>Hydration-reduced lattice thermal conductivity of <span class="hlt">olivine</span> in Earth’s upper mantle</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chang, Yun-Yuan; Hsieh, Wen-Pin; Tan, Eh; Chen, Jiuhua</p> <p>2017-01-01</p> <p>Earth’s water cycle enables the incorporation of water (hydration) in mantle minerals that can influence the physical properties of the mantle. Lattice thermal conductivity of mantle minerals is critical for controlling the temperature profile and dynamics of the mantle and subducting slabs. However, the effect of hydration on lattice thermal conductivity remains poorly understood and has often been assumed to be negligible. Here we have precisely measured the lattice thermal conductivity of hydrous San Carlos <span class="hlt">olivine</span> (Mg0.9Fe0.1)2SiO4 (Fo90) up to 15 gigapascals using an ultrafast optical pump−probe technique. The thermal conductivity of hydrous Fo90 with ∼7,000 wt ppm water is significantly suppressed at pressures above ∼5 gigapascals, and is approximately 2 times smaller than the nominally anhydrous Fo90 at mantle transition zone pressures, demonstrating the critical influence of hydration on the lattice thermal conductivity of <span class="hlt">olivine</span> in this region. Modeling the thermal structure of a subducting slab with our results shows that the hydration-reduced thermal conductivity in hydrated oceanic crust further decreases the temperature at the cold, dry center of the subducting slab. Therefore, the olivine−wadsleyite transformation rate in the slab with hydrated oceanic crust is much slower than that with dry oceanic crust after the slab sinks into the transition zone, extending the metastable <span class="hlt">olivine</span> to a greater depth. The hydration-reduced thermal conductivity could enable hydrous minerals to survive in deeper mantle and enhance water transportation to the transition zone. PMID:28377520</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780004994','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780004994"><span>The effect of temperature and pressure on the distribution of iron group elements between metal and <span class="hlt">olivine</span> phases in the process of differentiation of protoplanetary material</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vinogradov, A. P.; Ilyin, N. P.; Kolomeytsava, L. N.</p> <p>1977-01-01</p> <p>The distribution patterns of Ni, Co, Mn, and Cr were studied in <span class="hlt">olivines</span> of various origins: from meteorites (chondrites, achondrites, pallasites), which are likely analogs of the protoplanetary material, to peridotite inclusions in kimberlite pipes, which are analogs of mantle material. According to X-ray microanalysis data, nickel is concentrated in peridotite <span class="hlt">olivines</span>, while manganese is concentrated in meteoritic <span class="hlt">olivines</span>. The maximum chromium content was found in ureilites, which were formed under reducing conditions. Experiments at pressures of 20 to 70 kbar and temperatures of 1100 to 2000 C have shown that in a mixture of <span class="hlt">olivine</span> and Ni metal or NiO, nickel enters the silicate phase, displacing Fe into the metallic phase. Equilibrium temperatures were estimated from the Fe, Ni distribution coefficients between the metal and <span class="hlt">olivine</span>: 1500 K for pallasites, 1600 K for <span class="hlt">olivine</span>-bronzite H6 chondrites, 1200 K for <span class="hlt">olivine</span>-hypersthene L6, 900 K for LL6, and 1900 K for ureilites (at P = 1 atm). The equilibrium conditions of peridotites are close to T = 1800 K and P over 100 kbar. It is concluded that there is a sharp difference between the conditions of differentiation of the protoplanetary material at the time meteorites were formed and the conditions of differentiation of the planets into concentric layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790046634&hterms=shaw&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dshaw','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790046634&hterms=shaw&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dshaw"><span>The Shaw meteorite - History of a chondrite consisting of impact-melted and metamorphic lithologies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Taylor, G. J.; Keil, K.; Berkley, J. L.; Lange, D. E.; Fodor, R. V.</p> <p>1979-01-01</p> <p>Three intermingled lithologies are identified in the Shaw L-group chondrite: a light-colored lithology with a poikilitic texture, consisting of <span class="hlt">olivine</span> and augite crystals surrounded by larger orthopyroxene grains; a dark-colored lithology containing remnant <span class="hlt">chondrules</span> and exhibiting a microgranular texture; and a gray lithology which appears to be intermediate between the other two. Contrary to published opinions, the Shaw meteorite contains normal L-group chondrite abundances of metal and troilite, though these phases are irregularly distributed. The lithological analyses suggest that 4.52 Byr ago an impact took place on the L-group chondrite parent object of Shaw.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1222710-bar-bar-flavor-asymmetry-proton-chiral-effective-field-theory','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1222710-bar-bar-flavor-asymmetry-proton-chiral-effective-field-theory"><span>$${{\\<span class="hlt">bar</span>{d}} - {\\<span class="hlt">bar</span>{u}}}$$ Flavor Asymmetry in the Proton in Chiral Effective Field Theory</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>Salamu, Y.; Ji, Cheung-Ryong; Melnitchouk, Wally</p> <p>2015-09-01</p> <p>Themore » $${\\<span class="hlt">bar</span> d - \\<span class="hlt">bar</span> u}$$ flavor asymmetry in the proton arising from pion loops is computed using chiral effective field theory. calculation includes both nucleon and Δ intermediate states, and uses both the fully relativistic and heavy baryon frameworks. x dependence of $${\\<span class="hlt">bar</span> d - \\<span class="hlt">bar</span> u}$$ extracted from the Fermilab E866 Drell–Yan data can be well reproduced in terms of a single transverse momentum cutoff parameter regulating the ultraviolet behavior of the loop integrals. In addition to the distribution at x > 0, corrections to the integrated asymmetry from zero momentum contributions are computed, which arise from pion rainbow and bubble diagrams at x = 0. These have not been accounted for in previous analyses, and can make important contributions to the lowest moment of $${\\<span class="hlt">bar</span> d-\\<span class="hlt">bar</span> u}$$ .« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012E%26PSL.357..355N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012E%26PSL.357..355N"><span>Oxygen isotopes in crystalline silicates of comet Wild 2: A comparison of oxygen isotope systematics between Wild 2 particles and chondritic materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakashima, Daisuke; Ushikubo, Takayuki; Joswiak, David J.; Brownlee, Donald E.; Matrajt, Graciela; Weisberg, Michael K.; Zolensky, Michael E.; Kita, Noriko T.</p> <p>2012-12-01</p> <p>Oxygen three-isotope ratios of nine crystalline silicate particles from comet Wild 2 were measured to investigate oxygen isotope systematics of cometary materials. We are able to analyze particles as small as 4 μm using an ion microprobe with a˜1×2 μm beam by locating the analysis spots with an accuracy of ±0.4 μm. Three particles of Mn-rich forsterite, known as low-iron, manganese-enriched (LIME) <span class="hlt">olivine</span>, showed extremely 16O-rich signatures (δ18O, δ17O˜-50‰), similar to refractory inclusions in chondrites. The three Mn-rich forsterite particles may have formed by condensation from an 16O-rich solar nebula gas. Other particles consist of <span class="hlt">olivine</span> and/or pyroxene with a wide range of Mg# [=molar MgO/(FeO+MgO) %] from 60 to 96. Their oxygen isotope ratios plot nearly along the carbonaceous chondrite anhydrous mineral (CCAM) and Young and Russell lines with Δ17O(=δ17O-0.52×δ18O) values of -3.0‰ to +2.5‰. These data are similar to the range observed from previous analyses of Wild 2 crystalline silicates and those of <span class="hlt">chondrules</span> in carbonaceous chondrites. Six particles extracted from Stardust track 77 show diverse chemical compositions and isotope ratios; two Mn-rich forsterites, FeO-poor pigeonite, and three FeO-rich <span class="hlt">olivines</span> with a wide range of Δ17O values from -24‰ to +1.6‰. These results confirmed that the original projectile that formed track 77 was an aggregate (>6 μm) of silicate particles that formed in various environments. The Δ17O values of ferromagnesian Wild 2 particles (including data from previous studies) increase from ˜-23‰ to+2.5‰ with decreasing Mg#: Δ17O values of Mn-rich forsterite particles (Mg#=98-99.8) cluster at -23‰, those of FeO-poor particles (Mg#=95-97) cluster at -2‰, and those of FeO-rich particles (Mg#≤90) scatter mainly from -1.5‰ to+2.5‰. Compared to <span class="hlt">chondrules</span> in primitive chondrites, the systematic trend between Mg# and Δ17O among the Wild 2 particles is most similar to that reported for CR</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Litho.284..462Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Litho.284..462Y"><span>Kinetic processes for plastic deformation of <span class="hlt">olivine</span> in the Poyi ultramafic intrusion, NW China: Insights from the textural analysis of a 1700 m fully cored succession</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yao, Zhuo-sen; Qin, Ke-zhang; Xue, Sheng-chao</p> <p>2017-07-01</p> <p>The ubiquitous presence of undulose extinction and subgrain boundaries in <span class="hlt">olivine</span> crystals is commonly perceived as originating in the mantle, however these plastic deformation features are also well developed in the Poyi ultramafic intrusion, NW China. In this case, <span class="hlt">olivine</span> was deformed through kinetic processes in a crustal magma chamber, rather than by deformation processes in the upper mantle. Moreover, accumulation and textural coarsening were critical to the characteristics of crystal size distributions (CSDs) of <span class="hlt">olivines</span> in the Poyi intrusion. The axial deformational compaction of crystal mush was revealed by virtue of other quantitative textural analyses (e.g., spatial distribution patter, alignment factor and aspect ratio). Additionally, based on the contrast of density between crystal matrix and interstitial melt, adequate stress was generated by the km-scale crystal framework in Poyi body ( 2-11 MPa) which triggered the distortion of grain-lattice in <span class="hlt">olivine</span>. The deformation mechanisms of <span class="hlt">olivine</span> primarily are dislocation creep and dislocation-accommodated grain boundary sliding (DisGBS), while diffusion creep is subsidiary. This study has revealed various kinetic processes in a magmatic system by first demonstrating the genetic relationship between mineral deformation and axial compaction of crystal mush while highlighting the uncertainty of employing the deformation features of <span class="hlt">olivine</span> in peridotite xenoliths as an indicator for a mantle origin. In contrast to the <span class="hlt">olivine</span> populations of xenocrysts that underwent fragmentation during ascent, the deformed primitive <span class="hlt">olivines</span> in compaction exhibit a distinct shortage of small grains, which is conducive to delimiting these two types of deformed grains.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1247504','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1247504"><span>Measurement of the forward-backward asymmetry of $$\\Lambda$$ and $$\\<span class="hlt">bar</span>{\\Lambda}$$ production in $$p \\<span class="hlt">bar</span>{p}$$ collisions</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>Abazov, Victor Mukhamedovich</p> <p></p> <p>Here, we studymore » $$\\Lambda$$ and $$\\<span class="hlt">bar</span>{\\Lambda}$$ production asymmetries in $$p \\<span class="hlt">bar</span>{p} \\rightarrow \\Lambda (\\<span class="hlt">bar</span>{\\Lambda}) X$$, $$p \\<span class="hlt">bar</span>{p} \\rightarrow J/\\psi \\Lambda (\\<span class="hlt">bar</span>{\\Lambda}) X$$, and $$p \\<span class="hlt">bar</span>{p} \\rightarrow \\mu^\\pm \\Lambda (\\<span class="hlt">bar</span>{\\Lambda}) X$$ events recorded by the D0 detector at the Fermilab Tevatron collider at $$\\sqrt{s} = 1.96$$ TeV. We find an excess of $$\\Lambda$$'s ($$\\<span class="hlt">bar</span>{\\Lambda}$$'s) produced in the proton (antiproton) direction. This forward-backward asymmetry is measured as a function of rapidity. We confirm that the $$\\<span class="hlt">bar</span>{\\Lambda}/\\Lambda$$ production ratio, measured by several experiments with various targets and a wide range of energies, is a universal function of "rapidity loss", i.e., the rapidity difference of the beam proton and the lambda.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1247504-measurement-forward-backward-asymmetry-lambda-bar-lambda-production-bar-collisions','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1247504-measurement-forward-backward-asymmetry-lambda-bar-lambda-production-bar-collisions"><span>Measurement of the forward-backward asymmetry of $$\\Lambda$$ and $$\\<span class="hlt">bar</span>{\\Lambda}$$ production in $$p \\<span class="hlt">bar</span>{p}$$ collisions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Abazov, Victor Mukhamedovich</p> <p>2016-02-09</p> <p>Here, we studymore » $$\\Lambda$$ and $$\\<span class="hlt">bar</span>{\\Lambda}$$ production asymmetries in $$p \\<span class="hlt">bar</span>{p} \\rightarrow \\Lambda (\\<span class="hlt">bar</span>{\\Lambda}) X$$, $$p \\<span class="hlt">bar</span>{p} \\rightarrow J/\\psi \\Lambda (\\<span class="hlt">bar</span>{\\Lambda}) X$$, and $$p \\<span class="hlt">bar</span>{p} \\rightarrow \\mu^\\pm \\Lambda (\\<span class="hlt">bar</span>{\\Lambda}) X$$ events recorded by the D0 detector at the Fermilab Tevatron collider at $$\\sqrt{s} = 1.96$$ TeV. We find an excess of $$\\Lambda$$'s ($$\\<span class="hlt">bar</span>{\\Lambda}$$'s) produced in the proton (antiproton) direction. This forward-backward asymmetry is measured as a function of rapidity. We confirm that the $$\\<span class="hlt">bar</span>{\\Lambda}/\\Lambda$$ production ratio, measured by several experiments with various targets and a wide range of energies, is a universal function of "rapidity loss", i.e., the rapidity difference of the beam proton and the lambda.« less</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. 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