Sample records for cr fe-silicon layers

  1. Effect of NiFeCr seed and capping layers on exchange bias and planar Hall voltage response of NiFe/Au/IrMn trilayer structures

    NASA Astrophysics Data System (ADS)

    Talantsev, Artem; Elzwawy, Amir; Kim, CheolGi

    2018-05-01

    Thin films and cross junctions, based on NiFe/Au/IrMn structures, were grown on Ta and NiFeCr seed layers by magnetron sputtering. The effects of substitution of Ta with NiFeCr in seed and capping layers on an exchange bias field are studied. A threefold improvement of the exchange bias value in the structures, grown with NiFeCr seed and capping layers, is demonstrated. The reasons for this effect are discussed. Formation of clusters in the NiFeCr capping layer is proved by atomic force microscopy technique. Ta replacement on NiFeCr in the capping layer results in the enhancement of magnetoresistive response and a reduction of noise.

  2. Etching Selectivity of Cr, Fe and Ni Masks on Si & SiO2 Wafers

    NASA Astrophysics Data System (ADS)

    Garcia, Jorge; Lowndes, Douglas H.

    2000-10-01

    During this Summer 2000 I joined the Semiconductors and Thin Films group led by Dr. Douglas H. Lowndes at Oak Ridge National Laboratory’s Solid State Division. Our objective was to evaluate the selectivity that Trifluoromethane (CHF3), and Sulfur Hexafluoride (SF6) plasmas have for Si, SiO2 wafers and the Ni, Cr, and Fe masks; being this etching selectivity the ratio of the etching rates of the plasmas for each of the materials. We made use of Silicon and Silicon Dioxide-coated wafers that have Fe, Cr or Ni masks. In the semiconductor field, metal layers are often used as masks to protect layers underneath during processing steps; when these wafers are taken to the dry etching process, both the wafer and the mask layers’ thickness are reduced.

  3. TEM/STEM study of Zircaloy-2 with protective FeAl(Cr) layers under simulated BWR environment and high-temperature steam exposure

    NASA Astrophysics Data System (ADS)

    Park, Donghee; Mouche, Peter A.; Zhong, Weicheng; Mandapaka, Kiran K.; Was, Gary S.; Heuser, Brent J.

    2018-04-01

    FeAl(Cr) thin-film depositions on Zircaloy-2 were studied using transmission electron microscopy (TEM) and scanning transmission electron microscopy (STEM) with respect to oxidation behavior under simulated boiling water reactor (BWR) conditions and high-temperature steam. Columnar grains of FeAl with Cr in solid solution were formed on Zircaloy-2 coupons using magnetron sputtering. NiFe2O4 precipitates on the surface of the FeAl(Cr) coatings were observed after the sample was exposed to the simulated BWR environment. High-temperature steam exposure resulted in grain growth and consumption of the FeAl(Cr) layer, but no delamination at the interface. Outward Al diffusion from the FeAl(Cr) layer occurred during high-temperature steam exposure (700 °C for 3.6 h) to form a 100-nm-thick alumina oxide layer, which was effective in mitigating oxidation of the Zircaloy-2 coupons. Zr intermetallic precipitates formed near the FeAl(Cr) layer due to the inward diffusion of Fe and Al. The counterflow of vacancies in response to the Al and Fe diffusion led to porosity within the FeAl(Cr) layer.

  4. Microstructure and properties of FeSiCr/PA6 composites by injection molding using FeSiCr powders by phosphating and coupling treatment

    NASA Astrophysics Data System (ADS)

    Wang, Lulu; Qiao, Liang; Zheng, Jingwu; Cai, Wei; Ying, Yao; Li, Wangchang; Che, Shenglei; Yu, Jing

    2018-04-01

    FeSiCr/PA6 composites were prepared by injection molding using the FeSiCr powders modified by different phosphating agents and KH550 coupling agent. The resistivity, impact strength, magnetic permeability and magnetic loss of the FeSiCr/PA6 composites were measured. The morphologies of different FeSiCr powders and the FeSiCr/PA6 composites were also observed by scanning electron microscope (SEM). The results showed that 1-Hydroxyethylidene-1,1-diphosphonic acid, phytic acid and H3PO4 could improve the electrical resistivity of FeSiCr powders by forming the dense phosphating layer except diphenylphosphinic acid. However, the resistivity of FeSiCr/PA6 composites using the FeSiCr powders treated by all the four phosphating agents had no obvious increase though the phosphating layer on the surface of FeSiCr powder came into being. The nylon insulation layer had much stronger influence than the phosphating layer on electrical resistivity of the composites. After adding appropriate KH550 coupling agent, the impact strengths of FeSiCr/PA6 composites were significantly improved, which may be associated with the tiny gap between FeSiCr powder and PA6 matrix. The effects of the phosphating agents on the magnetic permeability and loss of the FeSiCr/PA6 were small and the mechanism were also discussed.

  5. Reduction of Chromite in Liquid Fe-Cr-C-Si Alloys

    NASA Astrophysics Data System (ADS)

    Demir, Orhan; Eric, R. Hurman

    1994-08-01

    The kinetics and the mechanism of the reduction of chromite in Fe-Cr-C-Si alloys were studied in the temperature range of 1534 °C to 1702 °C under an inert argon atmosphere. The rotating cylinder technique was used. The melt consisted of 10 and 20 wt Pct chromium, the carbon content varied from 2.8 wt Pct to saturation, and the silicon content varied from 0 to 2 wt Pct. The rotational speed of the chromite cylinder ranged from 100 to 1000 rpm. The initial chromium to iron ratios of the melts varied between 0.11 and 0.26. In Fe-C melts, the effect of rotational speed on the reduction of chromite was very limited. Carbon saturation (5.4 wt Pct) of the alloy caused the reduction to increase 1.5 times over the reduction observed in the unsaturated (4.87 wt Pct) alloy at a given rotational speed. The addition of chromium to the carbon-saturated Fe-C alloy increased the reduction rate. The addition of silicon to the liquid phase increased the reduction rate drastically. The reduction of chromite in Fe-Cr-C melts is hindered because of the formation of, approximately, a 1.5-mm-thick M7C3-type carbide layer around the chromite cylinders. This carbide layer did not form when silicon was present in the melt. It was found that the reduction rate is controlled by the liquid-state mass transfer of oxygen. The calculated apparent activation energies for diffusion were 102.9 and 92.9 kJ/mol of oxygen in the Si-O and C-O systems, respectively.

  6. Characteristics of Ni-Cr-Fe laser clad layers on EA4T steel

    NASA Astrophysics Data System (ADS)

    Chen, Wenjing; Chen, Hui; Wang, Yongjing; Li, Congchen; Wang, Xiaoli

    2017-07-01

    The Ni-Cr-Fe metal powder was deposited on EA4T steel by laser cladding technology. The microstructure and chemical composition of the cladding layer were analyzed by optical microscopy (OM), scanning electron microscopy (SEM) and X-ray diffraction (XRD). The bonding ability between the cladding layer and the matrix was measured. The results showed that the bonding between the cladding layer and the EA4T steel was metallurgical bonding. The microstructure of cladding layer was composed of planar crystals, columnar crystals and dendrite, which consisted of Cr2Ni3, γ phase, M23C6 and Ni3B phases. When the powder feeding speed reached 4 g/min, the upper bainite occurred in the heat affected zone (HAZ). Moreover, the tensile strength of the joint increased, while the yield strength and the ductility decreased.

  7. Highly (002) textured large grain bcc Cr{sub 80}Mn{sub 20} seed layer on Cr{sub 50}Ti{sub 50} amorphous layer for FePt-C granular film

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

    Jeon, Seong-Jae, E-mail: jsjigst@ecei.tohoku.ac.jp; Saito, Shin; Hinata, Shintaro

    Effect of bcc Cr{sub 80}Mn{sub 20} seed layer and Cr{sub 50}Ti{sub 50} amorphous texture inducing layer on the heteroepitaxy system in FePt-C granular film was studied by introducing a new concept of the layered structure. The concept suggested that the large grain seed layer in which the crystallographic texture was initially formed on an amorphous layer in the layered structure can reduce the angular distribution of (002) c-axis crystal orientation in the FePt-C granular film owing to heteroepitaxial growth. Structure analysis by X-ray diffraction revealed that (1) when the substrate heating temperature was elevated from 300 °C to 500 °C, grain sizemore » in the seed layer increased from 9.8 nm to 11.6 nm, and then decreased with further increasing the substrate temperature. The reduction of the grain size over 500 °C corresponds to the crystallization of the amorphous texture inducing layer, (2) when the grain size increased from 9.8 nm to 11.6 nm, the angular distribution of the (002) orientation in the seed layer dramatically decreased from 13.7° to 4.1°. It was shown that the large grain seed layer increased the perpendicular hysteresis in FePt-C granular film.« less

  8. Stability domain of alumina thermally grown on Fe-Cr-Al-based model alloys and modified surface layers exposed to oxygen-containing molten Pb

    NASA Astrophysics Data System (ADS)

    Jianu, A.; Fetzer, R.; Weisenburger, A.; Doyle, S.; Bruns, M.; Heinzel, A.; Hosemann, P.; Mueller, G.

    2016-03-01

    The paper gives experimental results concerning the morphology, composition, structure and thickness of the oxide scales grown on Fe-Cr-Al-based bulk alloys during exposure to oxygen-containing molten lead. The results are discussed and compared with former results obtained on Al-containing surface layers, modified by melting with intense pulsed electron beam and exposed to similar conditions. The present and previous results provide the alumina stability domain and also the criterion of the Al/Cr ratio for the formation of a highly protective alumina layer on the surface of Fe-Cr-Al-based alloys and on modified surface layers exposed to molten lead with 10-6 wt.% oxygen at 400-600 °C. The protective oxide scales, grown on alumina-forming Fe-Cr-Al alloys under the given experimental conditions, were transient aluminas, namely, kappa-Al2O3 and theta-Al2O3.

  9. Growth, Structural, Electronic, and Magnetic Characterization of GaN, CrN, Fe Islands on CrN, and Fe/CrN Bilayer Thin Films

    NASA Astrophysics Data System (ADS)

    Alam, Khan

    -order magnetic phase transition from paramagnetic (room temperature) to antiferromagnetic (low temperature) at 280+/-3 K. Our experiments suggest that the structural transition in CrN thin films occur in out-of-plane direction, and epitaxial constraints suppress the in-plane transition; therefore, the low temperature crystal structure of CrN is tetragonal. This new model explains our structural and magnetic data at low temperatures, but it is different than the previously published orthorhombic model. In third project, I studied exchange bias and exchange spring effect in MBE grown Fe/CrN bilayer thin films. We grew Fe/CrN bilayer thin films on MgO(001) substrate by molecular beam epitaxy, and studied them using variable temperature vibrating sample magnetometry, polarized neutron reflectometry, x-ray reflectivity, and cross-sectional transmission electron microscopy. We observed exchange bias and exchange spring effect in all bilayer thin films. We studied the relationship of exchange bias, blocking temperature, and coercivity with Fe and CrN layers thicknesses. We used polarized neutron beam reflectometry to see if spins at Fe/CrN interface are pinned. We found a thin ferromagnetically ordered CrN layer at the interface. In my final project, I studied growth of submonolayer Fe islands on CrN thin films. These films are prepared in two stages: first, a CrN layer is grown by MBE and then a submonolayer Fe is deposited at room temperature from a carefully degassed e-beam evaporator. The films are studied at liquid helium temperature using low temperature scanning tunneling microscopy and spectroscopy. Islands are seen in STM images, after the Fe deposition, at the edges as well as at the center of atomically flat CrN terraces. However, numerical calculations performed by our collaborator Ponce-P'erez from Benem'erita Universidad Aut'onoma de Puebla show that the Fe islands are energetically unstable on the surface. The Fe atoms substitute Cr atoms in the surface layer and the Cr

  10. Vector magnetometry of Fe/Cr/Fe trilayers with biquadratic coupling

    NASA Astrophysics Data System (ADS)

    Mansell, R.; Petit, D.; Fernández-Pacheco, A.; Lee, J. H.; Chin, S.-L.; Lavrijsen, R.; Cowburn, R. P.

    2017-05-01

    The magnetic reversal of epitaxial Fe/Cr/Fe trilayer samples grown on GaAs is studied. In wedged samples both long and short period coupling oscillations associated with Ruderman-Kittel-Kasuya-Yosida (RKKY) coupling in Cr are seen in the easy axis saturation fields. By using vector vibrating sample magnetometry and both longitudinal and transverse magneto-optical Kerr effect magnetometry we are able to determine the exact reversal path of both the magnetic layers. Changes in the reversal behavior are seen with sub-monolayer changes of the thickness of the Cr interlayer. The two main reversal paths are described in terms of whether the reversal is dominated by bilinear RKKY coupling, which leads to an antiparallel state at remanence or by biquadratic coupling which leads to a 90 degree alignment of layers at remanence. The changing reversal behaviour is discussed with respect to the possibility of using such systems for multilayer memory applications and, in particular, the limits on the required accuracy of the sample growth.

  11. Investigation of the mechanical properties of FeNiCrMnSi high entropy alloy wear resistant

    NASA Astrophysics Data System (ADS)

    Buluc, G.; Florea, I.; Chelariu, R.; Popescu, G.; Carcea, I.

    2016-06-01

    In this paper we investigated microstructure, hardness and wear resistance for FeNiCrMnAl, high entropy alloy. The FeNiCrMnSi, high entropy alloy was elaborated in a medium induction furnace, by choosing the silicon, as an alliance element within the equi- atomic high entropy alloy, we managed to obtain a dendritic structure, the formation of intermetallic compounds or separated silicon. The medium hardness value of the investigated alloy was 948.33 HV and the medium value of the friction coefficient was 0.6655 in the first 20 seconds and 0.5425 for 1667 seconds. The volume loss of the high entropy alloy FeNiCrMnSi was 0.0557 mm3.

  12. MBE growth and FMR, BLS and MOKE studies of exchange coupling in Fe whisker/Cr/Fe(001) and in Fe/Cu/Fe(001) 'loose spin' structures

    NASA Astrophysics Data System (ADS)

    Heinrich, B.; From, M.; Cochran, J. F.; Kowalewski, M.; Atlan, D.; Celinski, Z.; Myrtle, K.

    1995-02-01

    The exchange coupling has been studied in structures which consist of two ferromagnetic layers separated by non-ferromagnetic spacers (trilayers). The exchange coupling was measured using FMR and BLS techniques in the temperature range 77-400 K. Two systems were investigated: (a) Fe whisker/Cr/Fe(001) and (b) Fe/Cr/Fe(001). The oscillatory thickness dependence of the exchange coupling through a spin-density wave Cr spacer will be discussed and compared with recent data obtained by other groups. Cu interlayers were deposited either in a pure form, or a single monolayer of {Cu}/{Fe} alloy ('loose spins') was inserted between two pure bcc Cu(001) layers. Several such 'loose spin' structures were engineered to test the behavior of 'loose spin' structures. It was found that the presence of Fe impurity atoms has a strong tendency to decrease the direct bilinear exchange coupling. The contribution of 'loose spins' to the exchange coupling can be made significant, and even dominant, by a suitable choice of the RKKY coupling energy between the 'loose spins' and the surrounding ferromagnetic layers.

  13. Preliminary Microstructural and Microscratch Results of Ni-Cr-Fe and Cr3C2-NiCr Coatings on Magnesium Substrate

    NASA Astrophysics Data System (ADS)

    Istrate, B.; Munteanu, C.; Lupescu, S.; Benchea, M.; Vizureanu, P.

    2017-06-01

    Thermal coatings have a large scale application in aerospace and automotive field, as barriers improving wear mechanical characteristics and corrosion resistance. In present research, there have been used two types of coatings, Ni-Cr-Fe, respectively Cr3C2-NiCr which were deposited on magnesium based alloys (pure magnesium and Mg-30Y master alloy). There have been investigated the microstructural aspects through scanning electronic microscopy and XRD analysis and also a series of mechanical characteristics through microscratch and indentation determinations. The results revealed the formation of some adherent layers resistant to the penetration of the metallic indenter, the coatings did not suffer major damages. Microstructural analysis highlighted the formation of Cr3C2, Cr7C3, Cr3Ni2, Cr7Ni3, FeNi3, Cr-Ni phases. Also, the apparent coefficient of friction for Ni-Cr-Fe coatings presents superior values than Cr3C2-NiCr coatings.

  14. The effect of the MgO buffer layer thickness on magnetic anisotropy in MgO/Fe/Cr/MgO buffer/MgO(001)

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

    Kozioł-Rachwał, Anna, E-mail: a.koziolrachwal@aist.go.jp; AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, al. Mickiewicza 30, 30-059 Kraków; Nozaki, Takayuki

    2016-08-28

    The relationship between the magnetic properties and MgO buffer layer thickness d was studied in epitaxial MgO/Fe(t)/Cr/MgO(d) layers grown on MgO(001) substrate in which the Fe thickness t ranged from 0.4 nm to 1.1 nm. For 0.4 nm ≤ t ≤ 0.7 nm, a non-monotonic coercivity dependence on the MgO buffer thickness was shown by perpendicular magneto-optic Kerr effect magnetometry. For thicker Fe films, an increase in the buffer layer thickness resulted in a spin reorientation transition from perpendicular to the in-plane magnetization direction. Possible origins of these unusual behaviors were discussed in terms of the suppression of carbon contamination at the Fe surface and changes inmore » the magnetoelastic anisotropy in the system. These results illustrate a method to control magnetic anisotropy in MgO/Fe/Cr/MgO(d) via an appropriate choice of MgO buffer layer thickness d.« less

  15. Hafnium influence on the microstructure of FeCrAl alloys

    NASA Astrophysics Data System (ADS)

    Geanta, V.; Voiculescu, I.; Stanciu, E.-M.

    2016-06-01

    Due to their special properties at high temperatures, FeCrAl alloys micro-alloyed with Zr can be regarded as potential materials for use at nuclear power plants, generation 4R. These materials are resistant to oxidation at high temperatures, to corrosion, erosion and to the penetrating radiations in liquid metal environments. Also, these are able to form continuously, by the self-generation process of an oxide coating with high adhesive strength. The protective oxide layers must be textured and regenerable, with a good mechanical strength, so that crack and peeling can not appear. To improve the mechanical and chemical characteristics of the oxide layer, we introduced limited quantities of Zr, Ti, Y, Hf, Ce in the range of 1-3%wt in the FeCrAl alloy. These elements, with very high affinity to the oxygen, are capable to stabilize the alumina structure and to improve the oxide adherence to the metallic substrate. FeCrAl alloys microalloyed with Hf were prepared using VAR (Vacuum Arc Remelting) unit, under high argon purity atmosphere. Three different experimental alloys have been prepared using the same metallic matrix of Fe-14Cr-5Al, by adding of 0.5%wt Hf, 1.0%wt Hf and respectively 1.5%wt Hf. The microhardness values for the experimental alloys have been in the range 154 ... 157 HV0.2. EDAX analyses have been performed to determine chemical composition on the oxide layer and in the bulk of sample and SEM analyze has been done to determine the microstructural features. The results have shown the capacity of FeCrAl alloy to form oxide layers, with different texture and rich in elements such as Al and Hf.

  16. Magnetic interaction reversal in watermelon nanostructured Cr-doped Fe nanoclusters

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

    Kaur, Maninder; Dai, Qilin; Bowden, Mark

    2013-01-01

    Cr-doped core-shell Fe/Fe-oxide nanoclusters (NCs) were synthesized at varied atomic percentages of Cr from 0 at. % to 8 at. %. The low concentrations of Cr (<10 at. %) were selected in order to inhibit the complete conversion of the Fe-oxide shell to Cr2O3 and the Fe core to FeCr alloy. The magnetic interaction in Fe/Fe-oxide NCs (rv25 nm) can be controlled by antiferromagnetic Cr-dopant. We report the origin of r-FeCr phase at very low Cr concentration (2 at. %) unlike in previous studies, and the interaction reversal from dipolar to exchange interaction in watermelon-like Cr-doped core-shell NCs. The giantmore » magnetoresistance (GMR) effect,1,2 where an antiferromagnetic (AFM) exchange coupling exists between two ferromagnetic (FM) layers separated by a certain type of magnetic or non-magnetic spacer,3 has significant potential for application in the magnetic recording industry. Soon after the discovery of the GMR, the magnetic properties of multilayer systems (FeCr) became a subject of intensive study. The application of bulk iron-chromium (Fe-Cr) alloys has been of great interest, as these alloys exhibit favorable prop- erties including corrosion resistance, high strength, hardness, low oxidation rate, and strength retention at elevated temper- ature. However, the structural and magnetic properties of Cr-doped Fe nanoclusters (NCs) have not been investigated in-depth. Of all NCs, Fe-based clusters have unique magnetic properties as well as favorable catalytic characteristics in reactivity, selectivity, and durability.4 The incorporation of dopant of varied type and concentration in Fe can modify its chemical ordering, thereby optimizing its electrical, optical, and magnetic properties and opening up many new applications. The substitution of an Fe atom (1.24 A°) by a Cr atom (1.25 A° ) can easily modify the magnetic properties, since (i) the curie temperature (Tc ) of Fe is 1043 K, while Cr is an itinerant AFM with a bulk Neel temperature TN =311 K, and

  17. Surface modification to improve fireside corrosion resistance of Fe-Cr ferritic steels

    DOEpatents

    Park, Jong-Hee; Natesan, Krishnamurti; Rink, David L.

    2010-03-16

    An article of manufacture and a method for providing an Fe--Cr ferritic steel article of manufacture having a surface layer modification for corrosion resistance. Fe--Cr ferritic steels can be modified to enhance their corrosion resistance to liquid coal ash and other chemical environments, which have chlorides or sulfates containing active species. The steel is modified to form an aluminide/silicide passivating layer to reduce such corrosion.

  18. Preparation and electrical properties of Cr 2O 3 gate insulator embedded with Fe dot

    NASA Astrophysics Data System (ADS)

    Yokota, Takeshi; Kuribayashi, Takaaki; Murata, Shotaro; Gomi, Manabu

    2008-09-01

    We investigated the electrical properties of a metal (Au)/insulator (magneto-electric materials: Cr 2O 3)/magnetic materials (Fe)/tunnel layer (Cr 2O 3)/semiconductor (Si) capacitor. This capacitor shows the typical capacitance-voltage ( C- V) properties of an Si-MIS capacitor with hysteresis depending on the Fe dispersibility which is determined by the deposition condition. The C- V curve of the only sample having a 0.5 nm Fe layer was seen to have a hysteresis window with a clockwise trace, indicating that electrons have been injected into the ultra-thin Fe layer. The samples having Fe layers of other thicknesses show a counterclockwise trace, which indicates that the film has mobile ionic charges due to the dispersed Fe. These results indicated that the charge-injection site, which works as a memory, in the Cr 2O 3 can be prepared by Fe insertion, which is deposited using well-controlled conditions. The results also revealed the possibility of an MIS capacitor containing both ferromagnetic materials and an ME insulating layer in a single system.

  19. Thin Carbon Layers on Nanostructured Silicon-Properties and Applications

    NASA Astrophysics Data System (ADS)

    Angelescu, Anca; Kleps, Irina; Miu, Mihaela; Simion, Monica; Bragaru, Adina; Petrescu, Stefana; Paduraru, Crina; Raducanu, Aurelia

    Thin carbon layers such as silicon carbide (SiC) and diamond like carbon (DLC) layers on silicon, or on nanostructured silicon substrats were obtained by different methods. This paper is a review of our results in the areas of carbon layer microfabrication technologies and their properties related to different microsystem apllications. So, silicon membranes using a-SiC or DLC layers as etching mask, as well as silicon carbide membranes using a combined porous silicon — DLC structure were fabricated for sensor applications. A detailed evaluation of the field emission (FE) properties of these films was done to demonstrate their capability to be used in field emission devices. Carbon thin layers on nanostructured silicon samples were also investigated with respect to the living cell adhesion on these structures. The experiments indicate that the cell attachment on the surface of carbon coatings can be controlled by deposition parameters during the technological process.

  20. High-temperature oxidation of advanced FeCrNi alloy in steam environments

    NASA Astrophysics Data System (ADS)

    Elbakhshwan, Mohamed S.; Gill, Simerjeet K.; Rumaiz, Abdul K.; Bai, Jianming; Ghose, Sanjit; Rebak, Raul B.; Ecker, Lynne E.

    2017-12-01

    Alloys of iron-chromium-nickel are being explored as alternative cladding materials to improve safety margins under severe accident conditions. Our research focuses on non-destructively investigating the oxidation behavior of the FeCrNi alloy "Alloy 33" using synchrotron-based methods. The evolution and structure of oxide layer formed in steam environments were characterized using X-ray diffraction, hard X-ray photoelectron spectroscopy, X-ray fluorescence methods and scanning electron microscopy. Our results demonstrate that a compact and continuous oxide scale was formed consisting of two layers, chromium oxide and spinel phase (FeCr2O4) oxides, wherein the concentration of the FeCr2O4 phase decreased from the surface to the bulk-oxide interface.

  1. Characteristics of Eutectic α(Cr,Fe)-(Cr,Fe)23C6 in the Eutectic Fe-Cr-C Hardfacing Alloy

    NASA Astrophysics Data System (ADS)

    Lai, Hsuan-Han; Hsieh, Chih-Chun; Lin, Chi-Ming; Wu, Weite

    2017-01-01

    A specific eutectic (Cr,Fe)-(Cr,Fe)23C6 structure had been previously reported in the research studies of Fe-Cr-C hardfacing alloys. In this study, a close observation and discussion of the eutectic (Cr,Fe)-(Cr,Fe)23C6 were conducted. The eutectic solidification occurred when the chromium content of the alloy exceeded 35 wt pct. The eutectic structure showed a triaxial radial fishbone structure which was the so called "complex regular structure." Lamellar costa plates showed local asymmetry at two sides of a spine. Individual costae were able to combine as one, and spines showed extra branches. Costae that were nearly parallel to the heat flow direction were longer than those that were vertical to the heat flow direction. The triaxial spines preferred to intersect at 120 deg, while the costae preferred to intersect the spine at 90 deg and 35.26 deg due to the lattice relationships. The solidified metal near the fusion boundary showed an irregular structure instead of a complex regular structure. The reason for the irregular morphology was the high growth rate near the fusion boundary.

  2. Electrical transport properties in Fe-Cr nanocluster-assembled granular films

    NASA Astrophysics Data System (ADS)

    Wang, Xiong-Zhi; Wang, Lai-Sen; Zhang, Qin-Fu; Liu, Xiang; Xie, Jia; Su, A.-Mei; Zheng, Hong-Fei; Peng, Dong-Liang

    2017-09-01

    The Fe100-xCrx nanocluster-assembled granular films with Cr atomic fraction (x) ranging from 0 to 100 were fabricated by using a plasma-gas-condensation cluster deposition system. The TEM characterization revealed that the uniform Fe clusters were coated with a Cr layer to form a Fe-Cr core-shell structure. Then, the as-prepared Fe100-xCrx nanoclusters were randomly assembled into a granular film in vacuum environments with increasing the deposition time. Because of the competition between interfacial resistance and shunting effect of Cr layer, the room temperature resistivity of the Fe100-xCrx nanocluster-assembled granular films first increased and then decreased with increasing the Cr atomic fraction (x), and revealed a maximum of 2 × 104 μΩ cm at x = 26 at.%. The temperature-dependent longitudinal resistivity (ρxx), magnetoresistance (MR) effect and anomalous Hall effect (AHE) of these Fe100-xCrx nanocluster-assembled granular films were also studied systematically. As the x increased from 0 to 100, the ρxx of all samples firstly decreased and then increased with increasing the measuring temperature. The dependence of ρxx on temperature could be well addressed by a mechanism incorporated for the fluctuation-induced-tunneling (FIT) conduction process and temperature-dependent scattering effect. It was found that the anomalous Hall effect (AHE) had no legible scaling relation in Fe100-xCrx nanocluster-assembled granular films. However, after deducting the contribution of tunneling effect, the scaling relation was unambiguous. Additionally, the Fe100-xCrx nanocluster-assembled granular films revealed a small negative magnetoresistance (MR), which decreased with the increase of x. The detailed physical mechanism of the electrical transport properties in these Fe100-xCrx nanocluster-assembled granular films was also studied.

  3. Radiation effects on interface reactions of U/Fe, U/(Fe+Cr), and U/(Fe+Cr+Ni)

    DOE PAGES

    Shao, Lin; Chen, Di; Wei, Chaochen; ...

    2014-10-01

    We study the effects of radiation damage on interdiffusion and intermetallic phase formation at the interfaces of U/Fe, U/(Fe + Cr), and U/(Fe + Cr + Ni) diffusion couples. Magnetron sputtering is used to deposit thin films of Fe, Fe + Cr, or Fe + Cr + Ni on U substrates to form the diffusion couples. One set of samples are thermally annealed under high vacuum at 450 C or 550 C for one hour. A second set of samples are annealed identically but with concurrent 3.5 MeV Fe++ ion irradiation. The Fe++ ion penetration depth is sufficient to reachmore » the original interfaces. Rutherford backscattering spectrometry analysis with high fidelity spectral simulations is used to obtain interdiffusion profiles, which are used to examine differences in U diffusion and intermetallic phase formation at the buried interfaces. For all three diffusion systems, Fe++ ion irradiations enhance U diffusion. Furthermore, the irradiations accelerate the formation of intermetallic phases. In U/Fe couples, for example, the unirradiated samples show typical interdiffusion governed by Fick’s laws, while the irradiated ones show step-like profiles influenced by Gibbs phase rules.« less

  4. Lattice relations and solidification of the complex regular eutectic (Cr,Fe)-(Cr,Fe)23C6

    NASA Astrophysics Data System (ADS)

    Lai, Hsuan-Han; Hsieh, Chih-Chun; Lin, Chi-Ming; Wu, Weite

    2017-05-01

    The eutectic (Cr,Fe)-(Cr,Fe)23C6 showed a triaxial fishbone structure and could be categorized as a "complex regular structure". In this study, the lattice relations of the fishbone (Cr,Fe)23C6 were examined and the solidification process was observed using a transmission electron microscope and a confocal laser scanning microscope. For one of the three fish bones in a eutectic cell, parallel (Cr,Fe)23C6 lamellas at one side of the spine had the same lattice direction, as did those in the (Cr,Fe) phase. The lattices of neighboring (Cr,Fe)23C6 and (Cr,Fe) phases were not coherent. Lamellar (Cr,Fe)23C6 on opposite sides of a spine had different lattice directions, and their lattice boundary was in the spine. By using the confocal laser scanning microscope, the solidification of lamellar eutectic structure could be observed. At the low cooling rate of 5 o C·min-1, parallel lamellas would grow thick blocks instead of thin plates. To obtain a thin lamellar eutectic structure, the cooling rate should be higher, like the rate in welding.

  5. Hydrogen permeation in FeCrAl alloys for LWR cladding application

    NASA Astrophysics Data System (ADS)

    Hu, Xunxiang; Terrani, Kurt A.; Wirth, Brian D.; Snead, Lance L.

    2015-06-01

    FeCrAl, an advanced oxidation-resistant iron-based alloy class, is a highly prevalent candidate as an accident-tolerant fuel cladding material. Compared with traditional zirconium alloy fuel cladding, increased tritium permeation through FeCrAl fuel cladding to the primary coolant is expected, raising potential safety concerns. In this study, the hydrogen permeability of several FeCrAl alloys was obtained using a static permeation test station, which was calibrated and validated using 304 stainless steel. The high hydrogen permeability of FeCrAl alloys leads to concerns with respect to potentially significant tritium release when used for fuel cladding in LWRs. The total tritium inventory inside the primary coolant of a light water reactor was quantified by applying a 1-dimensional steady state tritium diffusion model to demonstrate the dependence of tritium inventory on fuel cladding type. Furthermore, potential mitigation strategies for tritium release from FeCrAl fuel cladding were discussed and indicate the potential for application of an alumina layer on the inner clad surface to serve as a tritium barrier. More effort is required to develop a robust, economical mitigation strategy for tritium permeation in reactors using FeCrAl clad fuel assemblies.

  6. High-temperature oxidation of advanced FeCrNi alloy in steam environments

    DOE PAGES

    Elbakhshwan, Mohamed S.; Gill, Simerjeet K.; Rumaiz, Abdul K.; ...

    2017-07-04

    Alloys of iron-chromium-nickel are being explored as alternative cladding materials to improve safety margins under severe accident conditions. Here, our research focuses on non-destructively investigating the oxidation behavior of the FeCrNi alloy “Alloy 33” using synchrotron-based methods. The evolution and structure of oxide layer formed in steam environments were characterized using X-ray diffraction, hard X-ray photoelectron spectroscopy, X-ray fluorescence methods and scanning electron microscopy. In conclusion, our results demonstrate that a compact and continuous oxide scale was formed consisting of two layers, chromium oxide and spinel phase (FeCr 2O 4) oxides, wherein the concentration of the FeCr 2O 4 phasemore » decreased from the surface to the bulk-oxide interface.« less

  7. Removal of Cr(VI) from groundwater by Fe(0)

    NASA Astrophysics Data System (ADS)

    Gao, Yanjiao; Liu, Rui

    2017-11-01

    This research was conducted to investigate the treatment of hexavalent chromium (Cr(VI)) by iron powder (Fe(0)) columns of simulated permeable reactive barriers with and without calcium carbonate (CaCO3). Two columns filled with Fe(0) were used as Cr(VI) removal equipment running at a flow velocity of 10 ml/min at room temperature. After 200 days running of the two columns, the results showed that Fe(0) was an effective material for Cr(VI) reduction with an average removal rate of above 84.6%. The performance of Column 2 with CaCO3 was better than Column 1 without CaCO3 in terms of average Cr(VI) removal rate. The presence of CaCO3 buffered the increasing pH caused by Fe(0) corrosion in Column 2 and enhanced the removal rate of Column 2. Scanning Electron Microscopy (SEM) images of Fe(0) in the three stages of running of the two columns illustrated that the coat layer of Column 1 was a little thicker than that of Column 2. Energy-dispersive spectrometry (EDS) results showed that the surface of Fe(0) of Column 2 contained more chromium elements. Raman spectroscopy found that all iron oxide was generated on the Fe(0) surface of Column 1 and Column 2 and chromium class objects were only detected on Fe(0) surface in Column 2.

  8. Microstructure and properties of Fe-based composite coating by laser cladding Fe-Ti-V-Cr-C-CeO2 powder

    NASA Astrophysics Data System (ADS)

    Zhang, Hui; Zou, Yong; Zou, Zengda; Wu, Dongting

    2015-01-01

    In situ TiC-VC reinforced Fe-based cladding layer was obtained on low carbon steel surface by laser cladding with Fe-Ti-V-Cr-C-CeO2 alloy powder. The microstructure, phases and properties of the cladding layer were investigated by X-ray diffractometry (XRD), scanning electron microscopy (SEM), energy dispersive spectrometry (EDS), transmission electron microscopy (TEM), potentio-dynamic polarization and electro-chemical impedance spectroscopy (EIS). Results showed Fe-Ti-V-Cr-C-CeO2 alloy powder formed a good cladding layer without defects such as cracks and pores. The phases of the cladding layer were α-Fe, γ-Fe, TiC, VC and TiVC2. The microstructures of the cladding layer matrix were lath martensite and retained austenite. The carbides were polygonal blocks with a size of 0.5-2 μm and distributed uniformly in the cladding layer. High resolution transmission electron microscopy showed the carbide was a complex matter composed of nano TiC, VC and TiVC2. The cladding layer with a hardness of 1030 HV0.2 possessed good wear and corrosion resistance, which was about 16.85 and 9.06 times than that of the substrate respectively.

  9. Brillouin light scattering on Fe/Cr/Fe thin-film sandwiches

    NASA Astrophysics Data System (ADS)

    Kabos, P.; Patton, C. E.; Dima, M. O.; Church, D. B.; Stamps, R. L.; Camley, R. E.

    1994-04-01

    The aim of this work is to perform Brillouin light scattering measurements of the field and wave-vector dependencies of the frequencies of the fundamental magnetic excitations in Fe/Cr/Fe thin film sandwiches with antiferromagnetically coupled magnetic layers, correlate these results with magnetization versus field data on such films, and compare the observed dependencies with theory for low-wave number spin-wave modes in sandwich films. The measurements were made for the in-plane static magnetic field H along the crystallographic and directions, with the in-plane wave vector k always perpendicular to H.

  10. Hydrogen permeation in FeCrAl alloys for LWR cladding application

    DOE PAGES

    Hu, Xunxiang; Terrani, Kurt A.; Wirth, Brian D.; ...

    2015-03-19

    FeCrAl is an advanced oxidation-resistant iron-based alloy class, is a highly prevalent candidate as an accident-tolerant fuel cladding material. Compared with traditional zirconium alloy fuel cladding, increased tritium permeation through FeCrAl fuel cladding to the primary coolant is expected, raising potential safety concerns. In our study, the hydrogen permeability of several FeCrAl alloys was obtained using a static permeation test station, which was calibrated and validated using 304 stainless steel. The high hydrogen permeability of FeCrAl alloys leads to concerns with respect to potentially significant tritium release when used for fuel cladding in LWRs. Also, the total tritium inventory insidemore » the primary coolant of a light water reactor was quantified by applying a 1-dimensional steady state tritium diffusion model to demonstrate the dependence of tritium inventory on fuel cladding type. Furthermore, potential mitigation strategies for tritium release from FeCrAl fuel cladding were discussed and indicate the potential for application of an alumina layer on the inner clad surface to serve as a tritium barrier. More effort is required to develop a robust, economical mitigation strategy for tritium permeation in reactors using FeCrAl clad fuel assemblies.« less

  11. AsMo7O27-bridged dinuclear sandwich-type heteropolymolybdates of Cr(III) and Fe(III): magnetism of [MM'(AsMo7O27)2]12- with MM' = FeFe, CrFe, and CrCr.

    PubMed

    Xu, Haisheng; Li, Lili; Liu, Bin; Xue, Ganglin; Hu, Huaiming; Fu, Feng; Wang, Jiwu

    2009-11-02

    Two new dinuclear sandwich-type heteropolymolybdates based on the mulitidendate inorganic fragment [AsMo(7)O(27)] and Cr(III) and Fe(III) ions, namely, the homometallic sandwich polyoxometalate (POM) (NH(4))(12)[Fe(2)(AsMo(7)O(27))(2)] x 12 H(2)O (1) and the first example of the "symmetrical" heterometallic Cr(III)-Fe(III) sandwich POM, (NH(4))(12)[FeCr(AsMo(7)O(27))(2)] x 13 H(2)O (2), were simultaneously synthesized in high yield. Their magnetic properties are thoroughly investigated together with the homometallic sandwich POM (NH(4))(12)[Cr(2)(AsMo(7)O(27))(2)] x 11 H(2)O (3). The chi(M)T values for compounds 1-3 at 300 K correspond well to the calculated spin-only values for Fe(III) (S = 5/2) and Cr(III) (S = 3/2) with g(Fe) = g(Cr) = 2. Upon cooling, the chi(M)T values decline monotonously and reach 0.14, 1.00, and 0.11 cm(3) K mol(-1) at 2.0 K for 1, 2, and 3, respectively, indicating a significant antiferromagnetic exchange between the magnetic centers with J = -2.09, -4.09, and -6.26 cm(-1), respectively, for 1, 2, and 3. The magnetic results clearly establish that compound 2 is formed by bimetallic Cr(III)-Fe(III) units and not by a mixture of the two antiferromagnetically coupled homometallic species. Their thermal properties are also characterized.

  12. First-principles investigation of Cr-doped Fe2B: Structural, mechanical, electronic and magnetic properties

    NASA Astrophysics Data System (ADS)

    Wei, Xiang; Chen, Zhiguo; Zhong, Jue; Wang, Li; Wang, Yipeng; Shu, Zhongliang

    2018-06-01

    The structural, mechanical, electronic and magnetic properties of Fe8-xCrxB4 (x = 0, 0.25, 0.5, 1, 2, 3, 4, 5, 6, 7 and 8) have been investigated by first-principles calculation. It was found that the calculated structural parameters are well consistent with available experimental data. Moreover, all studied compounds are thermodynamically stable phases. On the whole, the moduli of the compounds firstly increase and then decrease with the increase of Cr concentration, whereas the variation of hardness exhibits more fluctuations. All Cr-doped Fe2B have better ductility than Fe2B except Fe2Cr6B4 and Fe5Cr3B4. Interestingly, Fe4Cr4B4 is of not only the slightly larger hardness, but also much better ductility than Fe2B. As the Cr concentration is lower than 20 wt%, the hardness of Cr-doped Fe2B slightly decreases with increasing Cr, whereas the sharply increased hardness of (Fe, Cr)2B in Fe-B alloys or boriding layer should be attributed to the multiple alloying effects resulting from Cr and the other alloying elements. The electronic structures revealed that the Fe-B and/or Cr-B bonds are mainly responsible for their mechanical properties, and the M-N (M = Fe or Cr, N = Fe or Cr) bonds in 〈2 2 0〉 and 〈1 1 3〉 orientations show covalent character. Additionally, the magnetic moments (Ms) of the compounds do not monotonically decrease with increasing Cr.

  13. Neutron irradiation effects in Fe and Fe-Cr at 300 °C

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

    Chen, Wei-Ying; Miao, Yinbin; Gan, Jian

    2016-06-01

    Fe and Fe-Cr (Cr = 10–16 at.%) specimens were neutron-irradiated at 300 °C to 0.01, 0.1 and 1 dpa. The TEM observations indicated that the Cr significantly reduced the mobility of dislocation loops and suppressed vacancy clustering, leading to distinct damage microstructures between Fe and Fe-Cr. Irradiation-induced dislocation loops in Fe were heterogeneously observed in the vicinity of grown-in dislocations, whereas the loop distribution observed in Fe-Cr is much more uniform. Voids were observed in the irradiated Fe samples, but not in irradiated Fe-Cr samples. Increasing Cr content in Fe-Cr results in a higher density, and a smaller size ofmore » irradiation-induced dislocation loops. Orowan mechanism was used to correlate the observed microstructure and hardening, which showed that the hardening in Fe-Cr can be attributed to the formation of dislocation loops and α' precipitates.« less

  14. Formation and investigation of ultrathin layers of Co2FeSi ferromagnetic alloy synthesized on silicon covered with a CaF2 barrier layer

    NASA Astrophysics Data System (ADS)

    Grebenyuk, G. S.; Gomoyunova, M. V.; Pronin, I. I.; Vyalikh, D. V.; Molodtsov, S. L.

    2016-03-01

    Ultrathin (∼2 nm) films of Co2FeSi ferromagnetic alloy were formed on silicon by solid-phase epitaxy and studied in situ. Experiments were carried out in an ultrahigh vacuum (UHV) using substrates of Si(1 1 1) single crystals covered with a 5 nm thick CaF2 barrier layer. The elemental and phase composition as well as the magnetic properties of the synthesized films were analyzed by photoelectron spectroscopy using synchrotron radiation and by magnetic linear dichroism in photoemission of Fe 3p and Co 3p electrons. The study shows that the synthesis of the Co2FeSi ferromagnetic alloy occurs in the temperature range of 200-400 °C. At higher temperatures, the films become island-like and lose their ferromagnetic properties, as the CaF2 barrier layer is unable to prevent a mass transfer between the film and the Si substrate, which violates the stoichiometry of the alloy.

  15. Spin-orbit torque in Cr/CoFeAl/MgO and Ru/CoFeAl/MgO epitaxial magnetic heterostructures

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

    Wen, Zhenchao; Kim, Junyeon; Sukegawa, Hiroaki

    2016-05-15

    We study the spin-orbit torque (SOT) effective fields in Cr/CoFeAl/MgO and Ru/CoFeAl/MgO magnetic heterostructures using the adiabatic harmonic Hall measurement. High-quality perpendicular-magnetic-anisotropy CoFeAl layers were grown on Cr and Ru layers. The magnitudes of the SOT effective fields were found to significantly depend on the underlayer material (Cr or Ru) as well as their thicknesses. The damping-like longitudinal effective field (ΔH{sub L}) increases with increasing underlayer thickness for all heterostructures. In contrast, the field-like transverse effective field (ΔH{sub T}) increases with increasing Ru thickness while it is almost constant or slightly decreases with increasing Cr thickness. The sign of ΔH{submore » L} observed in the Cr-underlayer devices is opposite from that in the Ru-underlayer devices while ΔH{sub T} shows the same sign with a small magnitude. The opposite directions of ΔH{sub L} indicate that the signs of spin Hall angle in Cr and Ru are opposite, which are in good agreement with theoretical predictions. These results show sizable contribution from SOT even for elements with small spin orbit coupling such as 3d Cr and 4d Ru.« less

  16. Local lattice distortion in NiCoCr, FeCoNiCr and FeCoNiCrMn concentrated alloys investigated by synchrotron X-ray diffraction

    DOE PAGES

    Tong, Yang; Jin, Ke; Bei, Hongbin; ...

    2018-05-26

    Severe lattice distortion is presumptively considered as a core effect of high-entropy alloys, but quantitative measurements are still missing. Here, we demonstrate that the lattice distortion in high-entropy alloys can be quantitatively analyzed based on pair distribution function obtained from synchrotron X-ray diffraction. By applying this method to equiatomic NiCoCr, FeCoNiCr and FeCoNiCrMn concentrated alloys, we found that the local lattice distortion in the NiCoCr (0.23%) and FeCoNiCrMn (0.24%) alloys are comparable while negligible in the FeCoNiCr alloy (0.04%). Furthermore, the origin of local lattice distortion in the NiCoCr and FeCoNiCrMn concentrated alloys was discussed.

  17. Local lattice distortion in NiCoCr, FeCoNiCr and FeCoNiCrMn concentrated alloys investigated by synchrotron X-ray diffraction

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

    Tong, Yang; Jin, Ke; Bei, Hongbin

    Severe lattice distortion is presumptively considered as a core effect of high-entropy alloys, but quantitative measurements are still missing. Here, we demonstrate that the lattice distortion in high-entropy alloys can be quantitatively analyzed based on pair distribution function obtained from synchrotron X-ray diffraction. By applying this method to equiatomic NiCoCr, FeCoNiCr and FeCoNiCrMn concentrated alloys, we found that the local lattice distortion in the NiCoCr (0.23%) and FeCoNiCrMn (0.24%) alloys are comparable while negligible in the FeCoNiCr alloy (0.04%). Furthermore, the origin of local lattice distortion in the NiCoCr and FeCoNiCrMn concentrated alloys was discussed.

  18. Interdiffusion behavior of U3Si2 with FeCrAl via diffusion couple studies

    NASA Astrophysics Data System (ADS)

    Hoggan, Rita E.; He, Lingfeng; Harp, Jason M.

    2018-04-01

    Uranium silicide (U3Si2) is a candidate to replace uranium oxide (UO2) as light water reactor (LWR) fuel because of its higher thermal conductivity and higher fissile density relative to the current standard, UO2. A class of Fe, Cr, Al alloys collectively known as FeCrAl alloys that have superior mechanical and oxidation resistance are being considered as an alternative to the standard Zirconium based LWR cladding. The interdiffusion behavior between FeCrAl and U3Si2 is investigated in this study. Commercially available FeCrAl, along with U3Si2 pellets were placed in diffusion couples. Individual tests were ran at temperatures ranging from 500 °C to 1000 °C for 30 h and 100 h. The interdiffusion was analyzed with an optical microscope, scanning electron microscope, and transmission electron microscope. Uniform and planar interdiffusion layers along the material interface were illustrated with backscatter electron micrographs and energy-dispersive X-ray spectroscopy. Electron diffraction was used to validate phases present in the system, including distinct U2Fe3Si/UFe2 and UFeSi layers at the material interface. U and Fe diffused far into the FeCrAl and U3Si2 matrix, respectively, in the higher temperature tests. No interaction was observed at 500 °C for 30 h.

  19. Large magnetization and high Curie temperature in highly disordered nanoscale Fe2CrAl thin films

    NASA Astrophysics Data System (ADS)

    Dulal, Rajendra P.; Dahal, Bishnu R.; Forbes, Andrew; Pegg, Ian L.; Philip, John

    2017-02-01

    We have successfully grown nanoscale Fe2CrAl thin films on polished Si/SiO2 substrates using an ultra-high vacuum deposition with a base pressure of 9×10-10 Torr. The thickness of thin films ranges from 30 to 100 nm. These films exhibit cubic crystal structure with lattice disorder and display ferromagnetic behavior. The Curie temperature is greater than 400 K, which is much higher than that reported for bulk Fe2CrAl. The magnetic moments of the films varies from 2.5 to 2.8 μB per formula unit, which is larger than the reported bulk values. Thus, the disordered nanoscale Fe2CrAl films exhibit strong Fe-Fe exchange interactions through Fe-Cr-Fe and Fe-Al-Fe layers, resulting in both a large magnetization and a high Curie temperature.

  20. Epitaxial Fe16N2 thin film on nonmagnetic seed layer

    NASA Astrophysics Data System (ADS)

    Hang, Xudong; Zhang, Xiaowei; Ma, Bin; Lauter, Valeria; Wang, Jian-Ping

    2018-05-01

    Metastable α″ -Fe16N2 has attracted much interest as a candidate for rare-earth-free hard magnetic materials. We demonstrate that Fe16N2 thin films were grown epitaxially on Cr seed layers with MgO (001) substrates by facing-target sputtering. Good crystallinity with the epitaxial relation MgO (001 )[110 ] ∥ Cr (001 )[100 ] ∥ Fe16N2 (001 )[100 ] was obtained. The chemical order parameter, which quantifies the degree of N ordering in the Fe16N2 (the N-disordered phase is α' -Fe8N martensite), reaches 0.75 for Cr-seeded samples. Cr has a perfect lattice constant match with Fe16N2, and no noticeable strain can be assigned to Fe16N2. The intrinsic saturation magnetization of this non-strained Fe16N2 thin film at room temperature is determined to be 2.31 T by polarized neutron reflectometry and confirmed with vibrating sample magnetometry. Our work provides a platform to directly study the magnetic properties of high purity Fe16N2 films with a high order parameter.

  1. Anneal-Hardening Behavior of Cr-Fe-C Alloy Deposits Prepared in a Cr3+-Based Bath with Fe2+ Ions

    PubMed Central

    Huang, Ching An; Chen, Jhih You; Wang, Hai

    2017-01-01

    Cr-Fe-C alloy deposits were successfully prepared on high-carbon tool steel in a Cr3+-based electroplating bath containing Fe2+ ions and suitable complex agents. A Cr-based alloy deposit was obtained with an electroplating current density higher than 25 Adm−2, and a Fe-based alloy deposit was obtained using a current density of 20 Adm−2. Following electroplating, these alloy deposited specimens were annealed via rapid thermal annealing (RTA) at 500 °C for different periods up to 30 s. The experimental results show that Cr- and Fe-based alloy deposits could be significantly hardened after RTA at 500 °C for a few seconds. The maximum hardness was that of the Cr-Fe-C alloy deposit annealed at 500 °C for 10 s. The maximum hardness of 1205 Hv was detected from the annealed Cr-based alloy deposit prepared with 30 ASD. The hardening mechanism of annealed Cr- and Fe-based alloy deposits is attributed to the precipitation of C-related membranes. The hardness values of the annealed Cr- and Fe-based alloy deposits increase with the increasing degree of crystallization of the C-related membranes. PMID:29206206

  2. Oxalato-bridged dinuclear complexes of Cr(III) and Fe(III): synthesis, structure, and magnetism of [(C2H5)4N]4[MM'(ox)(NCS)8] with MM' = CrCr, FeFe, and CrFe.

    PubMed

    Triki, S; Bérézovsky, F; Sala Pala, J; Coronado, E; Gómez-García, C J; Clemente, J M; Riou, A; Molinié, P

    2000-08-21

    A new series of homo- and heterometallic oxalato-bridged dinuclear compounds of formulas [Et4N]4[MM'(ox)(NCS)8] ([Et4N]+ = [(C2H5)4N]+; ox = C2O4(2-)) with MM' = Cr(III)-Cr(III) (1), Fe(III)-Fe(III) (2), and Cr(III)-Fe(III) (3) is reported. They have been structurally characterized by infrared spectra and single-crystal X-ray diffraction. The three compounds are isostructural and crystallize in the orthorhombic space group Cmca with Z = 8, a = 16.561(8) A, b = 13.481(7) A, and c = 28.168(8) A for 1, a = 16.515(2) A, b = 13.531(1) A, and c = 28.289(4) A for 2, a = 16.664(7) A, b = 13.575(6) A, and c = 28.386(8) A for 3. The structure of 3 is made up of a discrete dinuclear anion [CrFe(ox)(NCS)8]4- and four disordered [Et4N]+ cations, each of them located on special positions. The anion, in a crystallographically imposed C2h symmetry, contains metal cations in distorted octahedral sites. The Cr(ox)Fe group, which is planar within 0.02 A, presents an intramolecular metal-metal distance of 5.43 A. Magnetic susceptibility measurements indicate antiferromagnetic pairwise interactions for 1 and 2 with J = -3.23 and -3.84 cm-1, respectively, and ferromagnetic Cr-Fe coupling with J = 1.10 cm-1 for 3 (J being the parameter of the exchange Hamiltonian H = -2JS1S2). The ESR spectra at different temperatures confirm the magnetic susceptibility data.

  3. Tribological Behavior of Al-Cr Coating Obtained by Dgpsm and IIP Composite Technology

    NASA Astrophysics Data System (ADS)

    Luo, Xixi; Yao, Zhengjun; Zhang, Pingze; Zhou, Keyin; Chen, Yu; Tao, Xuewei

    An Al-Cr composite alloyed layer composed of an Al enriched layer, a Cr enriched layer and a transition layer from the surface to the bulk along the cross-section was deposited on a 45# steel substrate by composite technology, where Cr was deposited using double glow plasma surface metallurgy (DGPSM), and Al was then implanted by ion implantation (IIP) to achieve higher micro-hardness and excellent abrasive resistance. The composite alloyed layer is approximately 5μm, and as metallurgical adherence to the substrate. The phases are Al8Cr5, Fe2AlCr, Cr23C6, Cr (Al) and Fe (Cr, Al) solid solution. The wear resistance tests were performed under various rotational speed (i.e. 280, 560 and 840r/min) with silicon nitride balls as the counterface material at ambient temperature. The Al-Cr composite alloyed layer exhibits excellent wear resistance when the speed is 280r/min with a friction coefficient as low as 0.3, which is attributed to Al8Cr5 in the Al implanted layer that withstands abrasive wear. Better wear resistance (friction coefficient: 0.254) at 560r/min is resulted from the formation of a high micro-hardness zone, and an oxidation layer with lubrication capacity. In addition, the composite alloyed layer suffers severe oxidative wear and adhesive wear at 840r/min due to the increment of the frictional heating. When compared to the 45# steel substrate, the enhanced wear resistance of the Al-Cr composite alloyed layer demonstrates the viable method developed in this work.

  4. Electronic properties of excess Cr at Fe site in FeCr{sub 0.02}Se alloy

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

    Kumar, Sandeep, E-mail: sandeepk.iitb@gmail.com; Singh, Prabhakar P.

    2015-06-24

    We have studied the effect of substitution of transition-metal chromium (Cr) in excess on Fe sub-lattice in the electronic structure of iron-selenide alloys, FeCr{sub 0.02}Se. In our calculations, we used Korringa-Kohn-Rostoker coherent potential approximation method in the atomic sphere approximation (KKR-ASA-CPA). We obtained different band structure of this alloy with respect to the parent FeSe and this may be reason of changing their superconducting properties. We did unpolarized calculations for FeCr{sub 0.02}Se alloy in terms of density of states (DOS) and Fermi surfaces. The local density approximation (LDA) is used in terms of exchange correlation potential.

  5. Buried oxide layer in silicon

    DOEpatents

    Sadana, Devendra Kumar; Holland, Orin Wayne

    2001-01-01

    A process for forming Silicon-On-Insulator is described incorporating the steps of ion implantation of oxygen into a silicon substrate at elevated temperature, ion implanting oxygen at a temperature below 200.degree. C. at a lower dose to form an amorphous silicon layer, and annealing steps to form a mixture of defective single crystal silicon and polycrystalline silicon or polycrystalline silicon alone and then silicon oxide from the amorphous silicon layer to form a continuous silicon oxide layer below the surface of the silicon substrate to provide an isolated superficial layer of silicon. The invention overcomes the problem of buried isolated islands of silicon oxide forming a discontinuous buried oxide layer.

  6. Effects of Fe2O3 addition on the nitridation of silicon powder

    NASA Technical Reports Server (NTRS)

    Hasegawa, Y.; Inomata, Y.; Kijima, K.; Matsuyama, T.

    1977-01-01

    The reaction of silicon powder and nitrogen was studied in the range of 1300-1400 C. When an addition of Fe2O3 was more than 0.8wt%, the reaction was linear and compared to samples with no Fe2O3, the reaction velocity increased 5 to 10 times. The reactions were mediated by the process of peeling and cracking in a thin layer of Si2N4 formed on the silicon particles or on the surface of the Fe-Si melts. As the addition of Fe2O3 increased, the reaction activation energy for highly pure samples decreased. Fe2O3 which exceeded the Si3N4 solubility limits was finally converted to d-Fe.

  7. Magnetic interaction reversal in watermelon nanostructured Cr-doped Fe nanoclusters

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

    Kaur, Maninder; Qiang, You, E-mail: youqiang@uidaho.edu; Dai, Qilin

    2013-11-11

    Cr-doped core-shell Fe/Fe-oxide nanoclusters (NCs) were synthesized at varied atomic percentages of Cr from 0 at. % to 8 at. %. The low concentrations of Cr (<10 at. %) were selected in order to inhibit the complete conversion of the Fe-oxide shell to Cr{sub 2}O{sub 3} and the Fe core to FeCr alloy. The magnetic interaction in Fe/Fe-oxide NCs (∼25 nm) can be controlled by antiferromagnetic Cr-dopant. We report the origin of σ-FeCr phase at very low Cr concentration (2 at. %) unlike in previous studies, and the interaction reversal from dipolar to exchange interaction in watermelon-like Cr-doped core-shell NCs.

  8. Development and property evaluation of nuclear grade wrought FeCrAl fuel cladding for light water reactors

    DOE PAGES

    Yamamoto, Yukinori; Pint, Bruce A.; Terrani, Kurt A.; ...

    2015-10-19

    Development of nuclear grade, iron-based wrought FeCrAl alloys has been initiated for light water reactor (LWR) fuel cladding to serve as a substitute for zirconium-based alloys with enhanced accident tolerance. Ferritic alloys with sufficient chromium and aluminum additions can exhibit significantly improved oxidation kinetics in high-temperature steam environments when compared to zirconium-based alloys. In the first phase, a set of model FeCrAl alloys containing 10–20Cr, 3–5Al, and 0–0.12Y in weight percent, were prepared by conventional arc-melting and hot-working processes to explore the effect of composition on the properties of FeCrAlY alloys. It was found that the tensile properties were insensitivemore » to the alloy compositions studied; however, the steam oxidation resistance strongly depended on both the chromium and the aluminum contents. The second phase development focused on strengthening Fe-13Cr-5Al with minor alloying additions of molybdenum, niobium, and silicon. Combined with an optimized thermo-mechanical treatment, a thermally stable microstructure was produced with improved tensile properties at temperatures up to 741°C.« less

  9. Synthesis and study of electronic state of Sr2CrO2Co2As2 with CoAs conduction layers

    NASA Astrophysics Data System (ADS)

    Suzuki, Atsushi; Ohta, Hiroto; Aruga Katori, Hiroko

    2017-06-01

    We successfully synthesized a new member of compounds with the CoAs layer, Sr2CrO2Co2As2, and its partially substituted systems Sr2CrO2(Tmx Co1- x )2As2 (Tm = Fe, Ni), and measured magnetization and electric resistivity of these polycrystalline compounds. As a result of magnetic measurement for Sr2CrO2Co2As2, magnetic moments of Co do not construct an itinerant electronic ferromagnetism unlike other compounds with the CoPn (Pn=P and As) layers. Both Sr2CrO2(Tmx Co1- x )2As2 with Tm = Fe and Ni also do not show an itinerant electronic ferromagnetism down to 2 K. For each solid solution of Sr2CrO2(Fe x Co1- x )2As2 with x > 0.0, ρ weakly increases with the decrease of T at low temperature region, indicating that the mixed occupancy of Cr and Fe within the conducting layers occurs in Sr2CrO2(Fe x Co1- x )2As2. We conclude that the absence of ferromagnetism in Sr2CrO2Co2As2 is due to the self-electron-doping from Cr to the conduction bands and the attempt to recover the ferromagnetism by the hole-doping effect is prevented by the mixed occupancy of Cr and Fe in Sr2CrO2 (Fe x Co1- x )2As2 with x > 0.0. The result of our structural analysis supports that the disappearance of itinerant electronic ferromagnetism in Sr2CrO2Co2As2 is due to the self-electron-doping from Cr.

  10. Plasma-Sprayed High Entropy Alloys: Microstructure and Properties of AlCoCrFeNi and MnCoCrFeNi

    NASA Astrophysics Data System (ADS)

    Ang, Andrew Siao Ming; Berndt, Christopher C.; Sesso, Mitchell L.; Anupam, Ameey; S, Praveen; Kottada, Ravi Sankar; Murty, B. S.

    2015-02-01

    High entropy alloys (HEAs) represent a new class of materials that present novel phase structures and properties. Apart from bulk material consolidation methods such as casting and sintering, HEAs can also be deposited as a surface coating. In this work, thermal sprayed HEA coatings are investigated that may be used as an alternative bond coat material for a thermal barrier coating system. Nanostructured HEAs that were based on AlCoCrFeNi and MnCoCrFeNi were prepared by ball milling and then plasma sprayed. Splat studies were assessed to optimise the appropriate thermal spray parameters and spray deposits were prepared. After mechanical alloying, aluminum-based and manganese-based HEA powders revealed contrary prominences of BCC and FCC phases in their X-ray diffraction patterns. However, FCC phase was observed as the major phase present in both of the plasma-sprayed AlCoCrFeNi and MnCoCrFeNi coatings. There were also minor oxide peaks detected, which can be attributed to the high temperature processing. The measured porosity levels for AlCoCrFeNi and MnCoCrFeNi coatings were 9.5 ± 2.3 and 7.4 ± 1.3 pct, respectively. Three distinct phase contrasts, dark gray, light gray and white, were observed in the SEM images, with the white regions corresponding to retained multicomponent HEAs. The Vickers hardness (HV0.3kgf) was 4.13 ± 0.43 and 4.42 ± 0.60 GPa for AlCoCrFeNi and MnCoCrFeNi, respectively. Both type of HEAs coatings exhibited anisotropic mechanical behavior due to their lamellar, composite-type microstructure.

  11. Double-spiral magnetic structure of the Fe/Cr multilayer revealed by nuclear resonance reflectivity

    NASA Astrophysics Data System (ADS)

    Andreeva, M. A.; Baulin, R. A.; Chumakov, A. I.; Rüffer, R.; Smirnov, G. V.; Babanov, Y. A.; Devyaterikov, D. I.; Milyaev, M. A.; Ponomarev, D. A.; Romashev, L. N.; Ustinov, V. V.

    2018-01-01

    We have studied the magnetization depth profiles in a [57Fe (dFe) /Cr (dCr) ]30 multilayer with ultrathin Fe layers and nominal thickness of the chromium spacers dCr≈2.0 nm using nuclear resonance scattering of synchrotron radiation. The presence of a broad pure-magnetic half-order (1/2) Bragg reflection has been detected at zero external field. The joint fit of the reflectivity curves and Mössbauer spectra of reflectivity measured near the critical angle and at the "magnetic" peak reveals that the magnetic structure of the multilayer is formed by two spirals, one in the odd and another one in the even iron layers, with the opposite signs of rotation. The double-spiral structure starts from the surface with the almost-antiferromagnetic alignment of the adjacent Fe layers. The rotation of the two spirals leads to nearly ferromagnetic alignment of the two magnetic subsystems at some depth, where the sudden turn of the magnetic vectors by ˜180∘ (spin flop) appears, and both spirals start to rotate in opposite directions. The observation of this unusual double-spiral magnetic structure suggests that the unique properties of giant magnetoresistance devices can be further tailored using ultrathin magnetic layers.

  12. Anomalously large ferromagnetic resonance linewidth in the Gd/Cr/Fe film plane

    NASA Astrophysics Data System (ADS)

    Sun, Li; Zhang, Wen; Wong, Ping Kwan Johnny; Yin, Yuli; Jiang, Sheng; Huang, Zhaocong; Zhai, Ya; Yao, Zhongyu; Du, Jun; Sui, Yunxia; Zhai, Hongru

    2018-04-01

    As an important parameter for characterizing the magnetization dynamics, Gilbert damping constant α in a thin film or a multilayer is generally extracted from the linear fitting of the frequency-dependence of the ferromagnetic resonance linewidth, sometimes accompanied with a tiny deviation of the linewidth to a smaller value at the low-frequency or high-frequency region due to the two-magnon scattering with an in-plane-field configuration, in which an in-plane magnetic field H perpendicular to a microwave field h was applied in film plane during measurement. In contrast, here we report, in ultrathin Gd/Cr/Fe multilayers, an anomalously large linewidth in the film plane at the low-frequency region. For the first time, we have successfully extracted the Gilbert damping constant from perfect theoretical fitting to the experimental data, by considering the effective direction of the magnetization around in precession staying out of the film plane when the in-pane H at which the precession starts is below the saturation field. This magnetization deviation from the film plane is found to have an obvious contribution to the enhanced linewidth caused by two magnon scattering, while slightly reduce the intrinsic linewidth. Under the same resonance frequency, the deviation angle reaches the maximum values at tCr = 1.0 nm while decreases when tCr increases to 1.5 nm, which coincides with the trend of the surface perpendicular anisotropy constant K⊥. A reduced intrinsic damping constant α is obtained as the introduction of Gd layer and Cr layer as a result of the competition between the spin pumping effect and the interfacial effects at the Fe/Gd and Fe/Cr interfaces. While the decreasing α for film with Cr layer thickness increasing to 1.5 nm might means the contribution of the electron density of states at the Fermi energy n(EF). This study offers an effective way to accurately obtain the intrinsic damping constant of spintronic materials/devices, which is essential

  13. Study of ion beam sputtered Fe/Si interfaces as a function of Si layer thickness

    NASA Astrophysics Data System (ADS)

    Kumar, Anil; Brajpuriya, Ranjeet; Singh, Priti

    2018-01-01

    The exchange interaction in metal/semiconductor interfaces is far from being completely understood. Therefore, in this paper, we have investigated the nature of silicon on the Fe interface in the ion beam deposited Fe/Si/Fe trilayers keeping the thickness of the Fe layers fixed at 3 nm and varying the thickness of the silicon sandwich layer from 1.5 nm to 4 nm. Grazing incidence x-ray diffraction and atomic force microscopy techniques were used, respectively, to study the structural and morphological changes in the deposited films as a function of layer thickness. The structural studies show silicide formation at the interfaces during deposition and better crystalline structure of Fe layers at a lower spacer layer thickness. The magnetization behavior was investigated using magneto-optical Kerr effect, which clearly shows that coupling between the ferromagnetic layers is highly influenced by the semiconductor spacer layer thickness. A strong antiferromagnetic coupling was observed for a value of tSi = 2.5 nm but above this value an unexpected behavior of hysteresis loop (step like) with two coercivity values is recorded. For spacer layer thickness greater than 2.5 nm, an elemental amorphous Si layer starts to appear in the spacer layer in addition to the silicide layer at the interfaces. It is observed that in the trilayer structure, Fe layers consist of various stacks, viz., Si doped Fe layers, ferromagnetic silicide layer, and nonmagnetic silicide layer at the interfaces. The two phase hysteresis loop is explained on the basis of magnetization reversal of two ferromagnetic layers, independent of each other, with different coercivities. X-ray photo electron spectroscopy technique was also used to study interfaces characteristics as a function of tSi.

  14. The Reduction of Cr(VI) to Cr(III) by Natural Fe-Bearing Minerals: A Synchrotron XAS Study

    NASA Astrophysics Data System (ADS)

    Xu, H.; Guo, X.; Ding, M.; Migdissov, A. A.; Boukhalfa, H.; Sun, C.; Roback, R. C.; Reimus, P. W.; Katzman, D.

    2017-12-01

    Cr(VI) in the form of CrO42- is a pollutant species in groundwater and soils that can pose health and environmental problems. Cr(VI) associated with use as a corrosion inhibitor at a power plant from 1956-1972 is present in a deep groundwater aquifer at Los Alamos National Laboratory. A potential remediation strategy for the Cr contamination is reduction of Cr(VI) to Cr(III) via the acceptance of electrons from naturally occurring or induced Fe(II) occurring in Fe-bearing minerals. In this work, using synchrotron-based X-ray techniques, we investigated the Cr reduction behavior by Fe-bearing minerals from outcrop and core samples representative of the contaminated portion of the aquifer. Samples were exposed to solutions with a range of known Cr (VI) concentrations. XANES and EXAFS spectra showed that all the Cr(VI) had been reduced to Cr(III), and micro XRF mapping revealed close correlation of Cr and Fe distribution, implying that Fe(II) in minerals reduced Cr(VI) in the solution. Similar behavior was observed from in-situ XANES measurements on Cr reduction and adsorption by mineral separates from the rock samples in Cr(VI)-bearing solutions. In addition, to obtain reference parameters for interpreting the data of natural samples, we collected Cr and Fe EXAFS spectra of Cr(III)-Fe(III) hydroxide solid solutions, which show progressive changes in the local structure around Cr and Fe over the whole series.

  15. Snoek Relaxation in Fe-Cr Alloys and Interstitial-Substitutional Interaction

    NASA Astrophysics Data System (ADS)

    Golovin, I. S.; Blanter, M. S.; Schaller, R.

    1997-03-01

    The internal friction (IF) spectra of -Fe, Fe-Cr ferritic alloys and Cr have been investigated in a frequency range of 0.01 to 10 Hz. A Snoek-type relaxation was found in all the investigated C doped Fe-Cr alloys, starting from pure Fe and finishing with pure Cr. The temperature location of the Snoek peak (Tmax) in -Fe was found to be 315 K (1 Hz). The activation energy deduced from the T - f shift was 0.81 eV. Tmax in Cr was 433 K with an activation energy of 1.11 eV. The Snoek-type peaks in Fe-Cr alloys are much wider than in pure Fe or pure Cr. The temperature location of the peak versus chromium content curve exhibits a maximum in the vicinity of 35 wt% Cr (Tmax was 573 to 578 K, f 1.2 Hz and the activation energy was about 1.45 eV). It is important that Cr atoms in α-Fe have a more pronounced influence on the temperature location of the peak than Fe atoms have in chromium. A new model based on the atomic interactions is proposed to explain the influence of composition on Snoek peak location. The internal friction has been simulated by a Monte Carlo method, using C-C and C-substitutional atom (s) interaction energies. A model of long-range strain-induced (elastic) interaction supplemented by the chemical interaction in the two nearest coordination shells around an immobile substitutional atom was used for the C-s interaction. The interatomic interaction was supposed to affect IF by changing both the carbon atom arrangement (short-range order) and the energy of C atoms in octahedral interstices, and therefore the activation energy of IF. The peak temperatue calculated coincides well with the experimental ones if the value for the chemical interaction in the first coordination shell (Hchem) for C-Cr in Fe is - 0.15 eV and for C-Fe in Cr +0.15 eV. The difference in the influence of Cr in α-Fe and Fe in Cr is accounted for by a difference in the elastic and chemical interaction both between the carbon atoms and the substitutional atoms. The relaxation process in

  16. Preparation and Oxidation Performance of Y and Ce-Modified Cr Coating on open-cell Ni-Cr-Fe Alloy Foam by the Pack Cementation

    NASA Astrophysics Data System (ADS)

    Pang, Q.; Hu, Z. L.; Wu, G. H.

    2016-12-01

    Metallic foams with a high fraction of porosity, low density and high-energy absorption capacity are a rapidly emerging class of novel ultralight weight materials for various engineering applications. In this study, Y-Cr and Ce-Cr-coated Ni-Cr-Fe alloy foams were prepared via the pack cementation method, and the effects of Y and Ce addition on the coating microstructure and oxidation performance were analyzed in order to improve the oxidation resistance of open-cell nickel-based alloy foams. The results show that the Ce-Cr coating is relatively more uniform and has a denser distribution on the surface of the nickel-based alloy foam. The surface grains of the Ce-Cr-coated alloy foam are finer compared to those of the Y-Cr-coated alloy foam. An obvious Ce peak appears on the interface between the coating and the alloy foam strut, which gives rise to a "site-blocking" effect for the short-circuit transport of the cation in the substrate. X-ray diffraction analysis shows that the Y-Cr-coated alloy foam mainly consists of Cr, (Fe, Ni) and (Ni, Cr) phases in the surface layer. The Ce-Cr-coated alloy foam is mainly composed of Cr and (Ni, Cr) phases. Furthermore, the addition of Y and Ce clearly lead to an improvement in the oxidation resistance of the coated alloy foams in the temperature range of 900-1000 °C. The addition of Ce is especially effective in enhancing the diffusion of chromium to the oxidation front, thus, accelerating the formation of a Cr2O3 layer.

  17. Buffer layer dependence of magnetoresistance effects in Co2Fe0.4Mn0.6Si/MgO/Co50Fe50 tunnel junctions

    NASA Astrophysics Data System (ADS)

    Sun, Mingling; Kubota, Takahide; Takahashi, Shigeki; Kawato, Yoshiaki; Sonobe, Yoshiaki; Takanashi, Koki

    2018-05-01

    Buffer layer dependence of tunnel magnetoresistance (TMR) effects was investigated in Co2Fe0.4Mn0.6Si (CFMS)/MgO/Co50Fe50 magnetic tunnel junctions (MTJs). Pd, Ru and Cr were selected for the buffer layer materials, and MTJs with three different CFMS thicknesses (30, 5, and 0.8 nm) were fabricated. A maximum TMR ratio of 136% was observed in the Ru buffer layer sample with a 30-nm-thick CFMS layer. TMR ratios drastically degraded for the CFMS thickness of 0.8 nm, and the values were 26% for Cr buffer layer and less than 1% for Pd and Ru buffer layers. From the annealing temperature dependence of the TMR ratios, amounts of interdiffusion and effects from the lattice mismatch were discussed.

  18. Importance of doping and frustration in itinerant Fe-doped Cr 2Al

    DOE PAGES

    Susner, M. A.; Parker, D. S.; Sefat, A. S.

    2015-05-12

    We performed an experimental and theoretical study comparing the effects of Fe-doping of Cr 2Al, an antiferromagnet with a N el temperature of 670 K, with known results on Fe-doping of antiferromagnetic bcc Cr. (Cr 1-xFe x) 2Al materials are found to exhibit a rapid suppression of antiferromagnetic order with the presence of Fe, decreasing T N to 170 K for x=0.10. Antiferromagnetic behavior disappears entirely at x≈0.125 after which point increasing paramagnetic behavior is exhibited. Moreover, this is unlike the effects of Fe doping of bcc antiferromagnetic Cr, in which T N gradually decreases followed by the appearance ofmore » a ferromagnetic state. Theoretical calculations explain that the Cr 2Al-Fe suppression of magnetic order originates from two effects: the first is band narrowing caused by doping of additional electrons from Fe substitution that weakens itinerant magnetism; the second is magnetic frustration of the Cr itinerant moments in Fe-substituted Cr 2Al. In pure-phase Cr 2Al, the Cr moments have an antiparallel alignment; however, these are destroyed through Fe substitution and the preference of Fe for parallel alignment with Cr. This is unlike bulk Fe-doped Cr alloys in which the Fe anti-aligns with the Cr atoms, and speaks to the importance of the Al atoms in the magnetic structure of Cr 2Al and Fe-doped Cr 2Al.« less

  19. Surface microstructure and high temperature corrosion resistance of arc-sprayed FeCrAl coating irradiated by high current pulsed electron beam

    NASA Astrophysics Data System (ADS)

    Hao, Shengzhi; Zhao, Limin; He, Dongyun

    2013-10-01

    The surface microstructure of arc-sprayed FeCrAl coating irradiated by high current pulsed electron beam (HCPEB) with long pulse duration of 200 μs was characterized by using optical microscopy, scanning electron microscopy and X-ray diffractometry. The distribution of chemical composition in modified surface layer was measured with electron probe micro-analyzer. The high temperature corrosion resistance of FeCrAl coating was tested in a saturated Na2SO4 and K2SO4 solution at 650 °C. After HCPEB irradiation, the coarse surface of arc-sprayed coating was changed as discrete bulged nodules with smooth and compact appearance. When using low energy density of 20 J/cm2, the surface modified layer was continuous entirely with an average melting depth of ˜30 μm. In the surface remelted layer, Fe and Cr elements gave a uniform distribution, while Al and O elements agglomerated particularly at the concave part between nodule structures to form α-Al2O3 phase. After high temperature corrosion tests, the FeCrAl coating treated with HCPEB of 20 J/cm2 remained a glossy surface with weight increment of ˜51 mg/cm2, decreased by 20% as compared to the initial sample. With the increasing energy density of HCPEB irradiation, the integrity of surface modified layer got segmented due to the formation of larger bulged nodules and cracks at the concave parts. For the HCPEB irradiation of 40 J/cm2, the high temperature corrosion resistance of FeCrAl coating was deteriorated drastically.

  20. Ring head recording on perpendicular media: Output spectra for CoCr and CoCr/NiFe media

    NASA Astrophysics Data System (ADS)

    Stubbs, D. P.; Whisler, J. W.; Moe, C. D.; Skorjanec, J.

    1985-04-01

    The recording density response for sputtered CoCr (thickness=0.5 μm) and CoCr/NiFe (t=0.25 μm/0.5 μm) as well as evaporated CoNi (t=0.12 μm) and Co surface-doped iron oxide particulate media has been measured by reading and writing with Mn-Zn ferrite heads (gap length=0.375 μm, track width=37 μm) in contact with the media. Measurements to 200 kfc/i (thousand flux changes per inch) show a gap null around 115 kfc/i. The data have been normalized by dividing out the head sensitivity to obtain the value of spacing plus transition width (d+a) for the various media. For the CoCr media this value varied from 0.075-0.088 μm; for CoNi, 0.100 μm, and for the particulate medium, 0.163 μm. In addition, testing with a larger gapped Mn-Zn ferrite head (g=2.43 μm) shows that the head fields are distorted by the soft magnetic underlayer in dual layer CoCr/NiFe samples when the gap length is large compared to the distance to the underlayer.

  1. Negative-Electrode Catalysts for Fe/Cr Redox Cells

    NASA Technical Reports Server (NTRS)

    Gahn, R. F.; Hagedorn, N.

    1987-01-01

    Electrodes perform more consistently and less expensive. Surfaces catalyzed by bismuth and bismuth/lead developed for application on chromium electrode in iron/chromium redox electrochemical energy storage system. NASA Fe/Cr storage system incorporates two soluble electrodes consisting of acidified solutions of iron chloride (FeC13 and FeC12) and chromium chloride (CrC13 and CrC12) oxidized and reduced in power-conversion unit to store and produce electricity. Electrolytes circulated with pumps and stored in external tanks.

  2. Seebeck Coefficient of Cation-Substituted Disulfides CuCr1-x Fe x S2 and Cu1-x Fe x CrS2

    NASA Astrophysics Data System (ADS)

    Korotaev, Evgeniy V.; Syrokvashin, Mikhail M.; Filatova, Irina Yu.; Pelmenev, Konstantin G.; Zvereva, Valentina V.; Peregudova, Natalya N.

    2018-03-01

    The effect of cation substitution on the Seebeck coefficient of CuCr1-x Fe x S2 (x = 0 to 0.30) and Cu1-x Fe x CrS2 (x = 0 to 0.03) in the temperature range of 100 K to 450 K has been investigated. Increasing iron concentration led to a metal-insulator transition which suppressed the thermoelectric power. However, for low iron concentration (x < 0.03), the Seebeck coefficient of CuCr1-x Fe x S2 and Cu1-x Fe x CrS2 exceeded the values for the undoped copper-chromium disulfide matrix CuCrS2 at temperature below 300 K.

  3. Temperature dependence of the exchange coupling in the Fe(001) whisker/11 ML Cr/20 ML Fe structure

    NASA Astrophysics Data System (ADS)

    From, M.; Liao, L. X.; Cochran, J. F.; Heinrich, B.

    1994-05-01

    The exchange coupling between iron layers separated by 11 monolayers (ML) of Cr(001) has been investigated using a structure in which the Cr(001) was grown on a bulk iron whisker Fe(001) surface at a temperature of approximately 300 °C. This temperature was selected to produce near optimum smoothness of the Cr layer. The Cr(001) deposition was followed by the deposition of 20 ML of Fe(001) at room temperature, and by the deposition of a 20 ML Au(001) protective layer. The frequencies corresponding to the magnetic excitations in this structure were measured by means of Brillouin light scattering (BLS). One of the observed frequencies corresponds to a surface mode in the bulk iron whisker. Another observed frequency corresponds to the lowest lying precessional mode of the magnetization in the 20 ML thick Fe(001) thin film. Typically, the thin film frequency exhibits a dependence on applied magnetic field that displays two cusps. The positions of the cusps are dependent on the exchange coupling between the 20 ML Fe film and the bulk iron substrate. The surface mode frequency increases monotonically with increasing field over most of the field range investigated. However, at the field corresponding to the low field cusp in the thin film frequency, the surface mode frequency undergoes an abrupt jump in magnitude. We have used the position of the cusps in the thin film data to deduce values for the bilinear, J1, and biquadratic, J2, coupling terms, where the coupling energy is written in the form EAB=-J1 cos(Δφ)+J2 cos2(Δφ); Δφ is the angle between the thin film and bulk iron magnetizations. Measurements of J1 and J2 have been carried out at six temperatures that span the range 100-350 K. Both J1 and J2 are found to depend strongly on temperature. The data are well described by the quadratic expression J2=-0.54+1.46 ×‖J1‖-0.52×J12, where J1 and J2 are expressed in erg/cm2. The large nonzero intercept and the linear term probably imply a significant intrinsic

  4. Cr(VI) Sorption by Nanosized FeS-Coated Sand

    NASA Astrophysics Data System (ADS)

    Park, M.; Jeong, H. Y.; Lee, S.; Kang, N.; Kim, K. H.; Choi, H. J.

    2015-12-01

    Cr(VI) sorption experiments were conducted as a function of pH (4.7, 7.0 and 9.7) using nanosized FeS-coated sand under anoxic environments. Under the experimental conditions, the sand used, with the FeS content of 0.068 mmol per 1 g sand, completely reduced the initially added Cr(VI) to Cr(III) over the pH range examined. The sorption of the once-reduced Cr(III) varied greatly with the solution pH. By the solution-phase analysis, significant amounts of Cr(III) remained as dissolved species at pH 4.7. On the other hands, dissolved Cr was below the detection limit (0.2 μM) at pH 7.0 and 9.7, indicating the greater sorption of Cr(III) at neutral to basic pH than acidic pH. From Cr-K edge X-ray absorption spectroscopy (XAS) analysis of the solid products, the sorbed Cr was shown to be present predominantly as trivalent state in all samples. Regardless of pH, the second coordination shell around Cr (i.e., the Cr-Cr(Fe) shell) was shown to be located at ~2.6 Å, which was far shorter than those in Cr(III)-bearing model compounds such as Cr(OH)3(s) and [Cr, Fe](OH)3(s). Furthermore, the coordination numbers of the second and third shells in the sorption samples (N = 0.7-1.8) were much lower than those in Cr(OH)3(s) and [Cr, Fe](OH)3(s). Taken together, the sorption of the once-reduced Cr(III) was likely to occur via surface-mediated processes (e.g., surface complexation and/or surface precipitation) rather than the bulk-phase precipitation. Financial support was provided by the "R&D Project on Environmental Management of Geologic CO2 Storage" from the KEITI (Project Number: 2014001810003).

  5. Formation of unusual Cr5+ charge state in CaCr0.5Fe0.5O3 perovskite

    NASA Astrophysics Data System (ADS)

    Dai, Jian-Hong; Zhao, Qing; Sun, Qian; Zhang, Shuo; Wang, Xiao; Shen, Xu-Dong; Liu, Zhe-Hong; Shen, Xi; Yu, Ri-Cheng; Chan, Ting-Shan; Li, Lun-Xiong; Zhou, Guang-Hui; Yang, Yi-feng; Jin, Chang-Qing; Long, You-Wen

    2018-03-01

    A new oxide CaCr0.5Fe0.5O3 was prepared under high pressure and temperature conditions. It crystallizes in a B-site disordered Pbnm perovskite structure. The charge combination is determined to be Cr5+/Fe3+ with the presence of unusual Cr5+ state in octahedral coordination, although Cr4+ and Fe4+ occur in the related perovskites CaCrO3 and CaFeO3. The randomly distributed Cr5+ and Fe3+ spins lead to short-range ferromagnetic coupling, whereas an antiferromagnetic phase transition takes place near 50 K due to the Fe3+–O–Fe3+ interaction. In spite of the B-site Cr5+/Fe3+ disorder, the compound exhibits electrical insulating behavior. First-principles calculations further demonstrate the formation of {CaCr}}0.55+{Fe}}0.53+{{{O}}}3 charge combination, and the electron correlation effect of Fe3+ plays an important role for the insulting ground state. CaCr0.5Fe0.5O3 provides the first Cr5+ perovskite system with octahedral coordination, opening a new avenue to explore novel transition-metal oxides with exotic charge states. Project supported by the National Natural Science Foundation of China (Grant Nos. 11574378, 51772324, and 61404052),the National Basic Research Program of China (Grant No. 2014CB921500), and the Chinese Academy of Sciences (Grant Nos. YZ201555, QYZDB-SSW-SLH013, GJHZ1773, and XDB07030300).

  6. Effect of Al and Cr Content on Air and Steam Oxidation of FeCrAl Alloys and Commercial APMT Alloy

    DOE PAGES

    Unocic, Kinga A.; Yamamoto, Yukinori; Pint, Bruce A.

    2017-03-09

    To develop the next generation of accident-tolerant fuel cladding for light-water nuclear reactors, wrought FeCrAlY alloys with varying amounts of Cr and Al and commercial Kanthal APMT alloy were evaluated for short-term (4 h) oxidation resistance in steam and air at 1200–1475 °C. Model alloys with lower Cr contents and higher Al contents were evaluated in this paper as lower Cr contents are desirable for radiation damage resistance during operation. As expected, a synergistic effect was found between the Cr and Al contents to enable protective Al 2O 3 formation under these conditions. Characterization of the alumina scales formed inmore » steam found that the scale morphology was affected by the alloy Y content and detailed scanning transmission electron microscopy (STEM) detected Y segregation along scale grain boundaries at 1200 °C. However, after 4 h at 1475 °C, Y and Hf were not segregated to the oxide grain boundaries formed on APMT and the scale had a single layer structure. Finally, compared to oxidation in air, STEM characterization of the outer scale showed differences in the Fe and Cr distributions in steam.« less

  7. Microstructure and Mechanical Properties of Cr-SiC Particles-Reinforced Fe-Based Alloy Coating

    NASA Astrophysics Data System (ADS)

    Wang, Fu-cheng; Du, Xiao-dong; Zhan, Ma-ji; Lang, Jing-wei; Zhou, Dan; Liu, Guang-fu; Shen, Jian

    2015-12-01

    In this study, SiC particles were first coated with Cr to form a layer that can protect the SiC particles from dissolution in the molten pool. Then, the Cr-SiC powder was injected into the tail of molten pool during plasma-transferred arc welding process (PTAW), where the temperature was relatively low, to prepare Cr-SiC particles reinforced Fe-based alloy coating. The microstructure and phase composition of the powder and surface coatings were analyzed, and the element distribution and hardness at the interfacial region were also evaluated. The protective layer consists of Cr3Si, Cr7C3, and Cr23C6, which play an important role in the microstructure and mechanical properties. The protective layer is dissolved in the molten pool forming a flocculent region and a transition region between the SiC particles and the matrix. The tribological performance of the coating was also assessed using a ring-block sliding wear tester with GGr15 grinding ring under 490 and 980 N load. Cr-SiC particles-reinforced coating has a lower wear rate than the unreinforced coating.

  8. Antiferromagnetic structure and electronic properties of BaCr2As2 and BaCrFeAs2

    NASA Astrophysics Data System (ADS)

    Filsinger, Kai A.; Schnelle, Walter; Adler, Peter; Fecher, Gerhard H.; Reehuis, Manfred; Hoser, Andreas; Hoffmann, Jens-Uwe; Werner, Peter; Greenblatt, Martha; Felser, Claudia

    2017-05-01

    Recent theoretical studies suggest that superconductivity may be found in doped chromium pnictides with crystal structures similar to their iron counterparts. Here, we report a comprehensive study on the magnetic arsenides BaCr2As2 and BaCrFeAs2 (space group I 4 /m m m ), which are possible mother compounds with d4 and d5 electron configurations, respectively. DFT-based calculations of the electronic structure evidence metallic antiferromagnetic ground states for both compounds. By powder neutron diffraction, we confirm for BaCr2As2 a robust ordering in the antiferromagnetic G -type structure at TN=580 K with μCr=1.9 μB . Anomalies in the lattice parameters point to magnetostructural coupling effects. In BaCrFeAs2, the Cr and Fe atoms randomly occupy the transition-metal site and G -type order is found below 265 K with μCr /Fe=1.1 μB . 57Fe Mössbauer spectroscopy demonstrates that only a small ordered moment is associated with the Fe atoms, in agreement with electronic structure calculations leading to μFe˜0 . The temperature dependence of the hyperfine field does not follow that of the total moments. Both compounds are metallic but show large enhancements of the linear specific heat. Electrical transport in BaCrFeAs2 is dominated by the atomic disorder and the partial magnetic disorder of Fe. Our results indicate that Néel-type order is unfavorable for Fe moments and thus it is destabilized with increasing Fe content.

  9. Effects of spin entropy and lattice strain from mixed-trivalent Fe3+/Cr3+ on the electronic, thermoelectric and optical properties of delafossite CuFe1-x Cr x O2 (x  =  0.25, 0.5, 0.75)

    NASA Astrophysics Data System (ADS)

    Ruttanapun, Chesta; Maensiri, Santi

    2015-12-01

    Mixed-trivalent Fe3+/Cr3+ content CuFe1-x Cr x O2 (x  =  0.25, 0.5, and 0.75) compounds were synthesized to investigate the effects of spin entropy, and lattice strain on their electronic, thermoelectric and optical properties. The XPS results showed the existence of mixed Cu1+/Cu2+, Fe3+/Fe4+ and Cr2+/Cr3+ ion states in the structures. The mixed Fe3+/Cr3+ions caused a strong correlation to occur between the spin and the orbitals of the carriers in the octahedral layer of the sample, affecting the carrier degeneracy Seebeck coefficient behaviour, and the Cu2+ and Fe4+ ions caused an effect of enhancing the electric conductivity. These effects meant that CuFe0.75Cr0.25O2 had the highest electrical conductivity, an enhanced Seebeck coefficient compared to that of CuFeO2-based compounds, and the highest thermopower value. The lowest thermal conductivity was that of CuFe0.5Cr0.5O2, which was a result of the mismatched atomic radii of the mixed trivalent Fe3+(0.645 Å)/Cr3+(0.615 Å), which caused the lattice strain to occur in the structure and thus affected the point defect scattering of the phonon thermal conductivity. The lowest total thermal conductivity was that of CuFe0.5Cr0.5O2, because it had the maximum lattice strain. Overall, the effect of the mixed trivalent elements caused CuFe0.75Cr0.25O2 to have the highest value of the dimensionless figure of merit ZT, with a value that was four times that of CuFeO2-based compounds and six times that of CuCrO2-based compounds. With regard to optical properties, the lattice strain causes the indirect optical gap to increase with increasing x content, but has no effect on the direct optical gap. These results verified that the mixed-trivalent Fe3+/Cr3+ content of CuFe1-x Cr x O2 (x  =  0.25, 0.5, and 0.75) affected the electronic, thermoelectric and optical properties of the structure by causing spin entropy and lattice strain to occur.

  10. Cr(VI) removal by FeS-coated alumina, silica, and natural sand

    NASA Astrophysics Data System (ADS)

    Park, M.; Lee, S.; Jeong, H. Y.

    2014-12-01

    Removal of Cr(VI) was investigated using mackinawite (FeS)-coated mineral sorbents under anoxic conditions. The sorbents included alumina (Al), silica (WS), and natural sand (NS). By analysis of both solution and solid phases, all FeS-coated sorbents were found to reduce Cr(VI) into Cr(III). The sorption extent and mechanism of Cr(VI) strongly depended on the pH conditions. Only at pH 4.5, significant amounts of the dissolved Cr remained in the solution. Titration of dissolved Cr(III) and Fe(III) by NaOH solutions indicated that no bulk-phase precipitation occurred at pH 4.5. Also, the removal of Cr(VI) at pH 4.5 was the greatest by FeS-coated NS. Consistent with these, Cr-K edge EXAFS revealed that Cr was removed by FeS-coated NS via surface precipitation, and that it was immobilized by FeS-coated WS and Al by forming surface clusters. Regardless of FeS-coated sorbents, at pH 7.0 and pH 9.5, the initially added Cr(VI) was quantitatively removed from the solution phase. By EXAFS analysis, the Cr sorption by FeS-coated Al was mainly due to the bulk-phase precipitation of Cr(OH)3(s) or [Cr, Fe](OH)3(s). In case of FeS-coated WS and NS, the short Cr-Cr distance (~2.6 Å) at pH 7.0 and pH 9.5 was not simply accounted for by the bulk precipitation as either hydroxide (rCr-Cr ~ 3.0 Å), and it would rather result from the surface precipitation. Such a difference in the coordination structure among FeS-coated sorbents was likely due to in the lower surface area of the former available for the surface precipitation.

  11. Magnetism of CrO overlayers on Fe(001)bcc surface: first principles calculations

    NASA Astrophysics Data System (ADS)

    Félix-Medina, Raúl Enrique; Leyva-Lucero, Manuel Andrés; Meza-Aguilar, Salvador; Demangeat, Claude

    2018-04-01

    Riva et al. [Surf. Sci. 621, 55 (2014)] as well as Calloni et al. [J. Phys.: Condens. Matter 26, 445001 (2014)] have studied the oxydation of Cr films deposited on Fe(001)bcc through low-energy electron diffraction, Auger electron spectroscopy and scanning tunneling microscopy. In the present work we perform a density functional approach within Quantum Expresso code in order to study structural and magnetic properties of CrO overlayers on Fe(001)bcc. The calculations are performed using DFT+U. The investigated systems include O/Cr/Fe(001)bcc, Cr/O/Fe(001)bcc, Cr0.25O0.75/Fe(001)bcc, as well as the O coverage Ox/Cr/Fe(001)bcc (x = 0.25; 0.50). We have found that the ordered CrO overlayer presents an antiferromagnetic coupling between Cr and Fe atoms. The O atoms are located closer to the Fe atoms of the surface than the Cr atoms. The ground state of the systems O/Cr/Fe(001)bcc and Cr/O/Fe(001)bcc corresponds to the O/Cr/Fe(001)bcc system with a magnetic coupling c(2 × 2). The effect of the O monolayer on Cr/Fe(001)bcc changes the ground state from p(1 × 1) ↓ to c(2 × 2) and produces an enhancement of the magnetic moments. The Ox overlayer on Cr/Fe(001)bcc produces an enhancement of the Cr magnetic moments.

  12. Method and apparatus for stable silicon dioxide layers on silicon grown in silicon nitride ambient

    NASA Technical Reports Server (NTRS)

    Cohen, R. A.; Wheeler, R. K. (Inventor)

    1974-01-01

    A method and apparatus for thermally growing stable silicon dioxide layers on silicon is disclosed. A previously etched and baked silicon nitride tube placed in a furnace is used to grow the silicon dioxide. First, pure oxygen is allowed to flow through the tube to initially coat the inside surface of the tube with a thin layer of silicon dioxide. After the tube is coated with the thin layer of silicon dioxide, the silicon is oxidized thermally in a normal fashion. If the tube becomes contaminated, the silicon dioxide is etched off thereby exposing clean silicon nitride and then the inside of the tube is recoated with silicon dioxide. As is disclosed, the silicon nitride tube can also be used as the ambient for the pyrolytic decomposition of silane and ammonia to form thin layers of clean silicon nitride.

  13. Phase Evolution and Properties of Al2CrFeNiMo x High-Entropy Alloys Coatings by Laser Cladding

    NASA Astrophysics Data System (ADS)

    Wu, Wei; Jiang, Li; Jiang, Hui; Pan, Xuemin; Cao, Zhiqiang; Deng, Dewei; Wang, Tongmin; Li, Tingju

    2015-10-01

    A series of Al2CrFeNiMo x ( x = 0 to 2.0 at.%) high-entropy alloys coatings was synthesized on stainless steel by laser cladding. The effect of Mo content on the microstructures and mechanical properties of Al2CrFeNiMo x coatings was studied. The results show that the laser clad layer consists of the cladding zone, bonding zone, and heat-affected zone. The Al2CrFeNiMo x coatings are composed of two simple body-center cubic phases and the cladding zone is mainly composed of equiaxed grains. When the content of Mo reaches 2 at.%, a eutectic structure is found in the interdendritic regions. The surface microhardness of the Al2CrFeNiMo2 coating is 678 HV, which is about three times higher than that of the substrate (243 HV). Compared with stainless steel, the wear resistance of the coatings has been improved greatly. The wear mass loss of the Al2CrFeNiMo alloy is 9.8 mg, which is much less than that of the substrate (18.9 mg) and its wear scar width is the lowest among the Al2CrFeNiMo x coatings, indicating that the wear resistance of the Al2CrFeNiMo is the best.

  14. Comparison of reproduce signal and noise of conventional and keepered CoCrTa/Cr thin film media

    NASA Astrophysics Data System (ADS)

    Sin, Kyusik; Ding, Juren; Glijer, Pawel; Sivertsen, John M.; Judy, Jack H.; Zhu, Jian-Gang

    1994-05-01

    We studied keepered high coercivity CoCrTa/Cr thin film media with a Cr isolation layer between the CoCrTa storage and an overcoating of an isotropic NiFe soft magnetic layer. The influence of the thickness of the NiFe and Cr layers, and the effects of head bias current on the signal output and noise, were studied using a thin film head. The reproduced signal increased by 7.3 dB, but the signal-to-noise ratio decreased by 4 dB at a linear density of 2100 fr/mm (53.3 kfr/in.) with a 1000 Å thick NiFe keeper layer. The medium noise increased with increasing NiFe thickness and the signal output decreased with decreasing Cr thickness. A low output signal obtained with very thin Cr may be due to magnetic interactions between the keeper layer and magnetic media layer. It is observed that signal distortion and timing asymmetry of the output signals depend on the thickness of the keeper layer and the head bias current. The signal distortion increased and the timing asymmetry decreased as the head bias current was increased. These results may be associated with different permeability of the keeper under the poles of the thin film head due to the superposition of head bias and bit fields.

  15. Advanced experimental study on giant magnetoresistance of Fe/Cr superlattices by rf-sputtering

    NASA Astrophysics Data System (ADS)

    Obi, Y.; Takanashi, K.; Mitani, Y.; Tsuda, N.; Fujimori, H.

    1992-02-01

    The study on MagnetoResistance (MR) has been performed for the Fe/Cr SuperLattice (SL) produced by the rf-sputtering method. Especially the effect of the preparation condition on MR has been investigated in detail. The MR oscillates with respect to the Cr layer thickness ( tCr) as was reported by Parkin et al. [1]. The characteristic experimental results is that the MR depends strongly on the Ar pressure. This indicates that the size of the MR is greatly affected by the interface roughness of the SL induced by the different Ar pressure during sputtering.

  16. Epitaxial growth of silicon for layer transfer

    DOEpatents

    Teplin, Charles; Branz, Howard M

    2015-03-24

    Methods of preparing a thin crystalline silicon film for transfer and devices utilizing a transferred crystalline silicon film are disclosed. The methods include preparing a silicon growth substrate which has an interface defining substance associated with an exterior surface. The methods further include depositing an epitaxial layer of silicon on the silicon growth substrate at the surface and separating the epitaxial layer from the substrate substantially along the plane or other surface defined by the interface defining substance. The epitaxial layer may be utilized as a thin film of crystalline silicon in any type of semiconductor device which requires a crystalline silicon layer. In use, the epitaxial transfer layer may be associated with a secondary substrate.

  17. Stability of Fe-Cr alloy interconnects under CH 4-H 2O atmosphere for SOFCs

    NASA Astrophysics Data System (ADS)

    Horita, Teruhisa; Xiong, Yueping; Yamaji, Katsuhiko; Sakai, Natsuko; Yokokawa, Harumi

    The chemical stability of Fe-Cr alloys (ZMG232 and SUS430) was examined under humidified CH 4 gases at 1073 K to simulate the real anode atmosphere in SOFC operation. Surface microstructure change and oxide scale layer formation were observed on the oxidized Fe-Cr alloy surfaces. The main reaction products were Mn-Cr-(Fe) spinels for both alloys. Secondary ion mass spectrometry (SIMS) was applied to measure the elemental distribution of minor and major elements around the oxide scale/alloy interface. A high concentration of Mn on the oxide scale surface suggested the fast diffusion of Mn in the oxide scale to form the spinels. Annealing in CH 4-H 2O made the oxide scale thicker with duration time on the alloy surface. The parabolic growth rates ( kp) of oxide scale layer were evaluated from the thickness of oxide scales by secondary ion mass spectrometry (SIMS) depth profiles, which were calculated to the following: kp=6.25×10 -6 μm 2/s for SUS430 and kp=4.42×10 -6 μm 2/s for ZMG232. The electrical conductivity of oxidized alloys showed the semi-conductor temperature dependence for both alloys. The electrical conductivity of oxidized ZMG232 alloy was higher than that of oxidized SUS430.

  18. Development of ODS FeCrAl alloys for accident-tolerant fuel cladding

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

    Dryepondt, Sebastien N.; Hoelzer, David T.; Pint, Bruce A.

    2015-09-18

    FeCrAl alloys are prime candidates for accident-tolerant fuel cladding due to their excellent oxidation resistance up to 1400 C and good mechanical properties at intermediate temperature. Former commercial oxide dispersion strengthened (ODS) FeCrAl alloys such as PM2000 exhibit significantly better tensile strength than wrought FeCrAl alloys, which would alloy for the fabrication of a very thin (~250 m) ODS FeCrAl cladding and limit the neutronic penalty from the replacement of Zr-based alloys by Fe-based alloys. Several Fe-12-Cr-5Al ODS alloys where therefore fabricated by ball milling FeCrAl powders with Y2O3 and additional oxides such as TiO 2 or ZrO 2. Themore » new Fe-12Cr-5Al ODS alloys showed excellent tensile strength up to 800 C but limited ductility. Good oxidation resistance in steam at 1200 and 1400 C was observed except for one ODS FeCrAl alloy containing Ti. Rolling trials were conducted at 300, 600 C and 800 C to simulate the fabrication of thin tube cladding and a plate thickness of ~0.6mm was reached before the formation of multiple edge cracks. Hardness measurements at different stages of the rolling process, before and after annealing for 1h at 1000 C, showed that a thinner plate thickness could likely be achieved by using a multi-step approach combining warm rolling and high temperature annealing. Finally, new Fe-10-12Cr-5.5-6Al-Z gas atomized powders have been purchased to fabricate the second generation of low-Cr ODS FeCrAl alloys. The main goals are to assess the effect of O, C, N and Zr contents on the ODS FeCrAl microstructure and mechanical properties, and to optimize the fabrication process to improve the ductility of the 2nd gen ODS FeCrAl while maintaining good mechanical strength and oxidation resistance.« less

  19. Method of forming buried oxide layers in silicon

    DOEpatents

    Sadana, Devendra Kumar; Holland, Orin Wayne

    2000-01-01

    A process for forming Silicon-On-Insulator is described incorporating the steps of ion implantation of oxygen into a silicon substrate at elevated temperature, ion implanting oxygen at a temperature below 200.degree. C. at a lower dose to form an amorphous silicon layer, and annealing steps to form a mixture of defective single crystal silicon and polycrystalline silicon or polycrystalline silicon alone and then silicon oxide from the amorphous silicon layer to form a continuous silicon oxide layer below the surface of the silicon substrate to provide an isolated superficial layer of silicon. The invention overcomes the problem of buried isolated islands of silicon oxide forming a discontinuous buried oxide layer.

  20. Fabrication of a novel NiFe2O4/Zn-Al layered double hydroxide intercalated with EDTA composite and its adsorption behavior for Cr(VI) from aqueous solution

    NASA Astrophysics Data System (ADS)

    Deng, Lin; Shi, Zhou; Wang, Li; Zhou, Shiqing

    2017-05-01

    A novel magnetic NiFe2O4/Zn-Al layered double hydroxide intercalated with EDTA composite (NiFe2O4/ZnAl-EDTA LDH) was prepared through modified coprecipitation method and employed for adsorptive removal of Cr(VI) from aqueous solution. The adsorbents were characterized using Brunauer-Emmett-Teller (BET), scanning electron microscopy (SEM), transmission electron microscope (TEM), X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FTIR), vibrating sample magnetometer (VSM), and X-ray photoelectron spectroscopy (XPS). Factors affecting the Cr(VI) adsorption, such as initial solution pH, adsorbent dosage, contact time, initial Cr(VI) concentration, temperature and coexisting ions, were studied systematically. Experiments results show that the magnetic NiFe2O4/ZnAl-EDTA LDH exhibits high adsorption efficiency within a wide pH range of 3.0-7.0 (R>80% at Cr(VI) concentration 50 mg L-1, contact time 360 min, and adsorbent dosage 2 g/L) and quick separation property. The adsorption process is fitted well with the Langmuir isotherm and pseudo-second-order kinetic model. The maximum theoretical adsorption capacity is found to be 77.22 mg g-1 at pH 6.0 and 318 K. The positive ΔH value (2.907 kJ mol-1) and negative ΔG value (-4.722 kJ mol-1) at 298-318 K reveals that the adsorption process is feasible, spontaneous and endothermic. Coexisting anions (PO43-, SO42-, CO32-, HCO3-, Cl-, and NO3-) have no significant effect on Cr(VI) removal. The mechanism study indicates that the adsorption of Cr(VI) onto NiFe2O4/ZnAl-EDTA LDH mainly involves electrostatic attraction and ion exchange interaction. It is interesting to note that a proportion of Cr(VI) adsorbed on the adsorbent surface are reduced to Cr(III) during the adsorption process. Results from this study demonstrate the potential utility of the magnetic NiFe2O4/ZnAl-EDTA LDH that could be developed into a viable technology for efficient removal of Cr(VI) from aqueous solution.

  1. Tough cryogenic alloys from the Fe-Mn and Fe-Mn-Cr systems

    NASA Technical Reports Server (NTRS)

    Schanfein, M. J.; Zackay, V. F.; Morris, J. W., Jr.

    1974-01-01

    By adjusting composition, metastable gamma (austenite) and epsilon (hexagonal) martensite may be retained in Fe-Mn and Fe-Mn-Cr alloys and used to impact toughness through the TRIP mechanism. The resulting alloys have excellent toughness at cryogenic temperatures. The best alloys obtained to date are: Fe-20Mn, with sigma (sub y) = 79ksi and K sub IC = 275ksi square root of (in) at 77 K, and Fc-16Mn-8Cr, with sigma sub y = 85ksi and K sub IC = 72ksi square root of (in) at 77 K.

  2. Irradiation-induced formation of a spinel phase at the FeCr/MgO interface

    DOE PAGES

    Xu, Yun; Yadav, Satyesh Kumar; Aguiar, Jeffery A.; ...

    2015-04-27

    Oxide dispersion strengthened ferritic/martensitic alloys have attracted significant attention for their potential uses in future nuclear reactors and storage vessels, as the metal/oxide interfaces act as stable high-strength sinks for point defects while also dispersing helium. Here, in order to unravel the evolution and interplay of interface structure and chemistry upon irradiation in these types of materials, an atomically sharp FeCr/MgO interface was synthesized at 500 °C and separately annealed and irradiated with Ni 3+ ions at 500 °C. After annealing, a slight enrichment of Cr atoms was observed at the interface, but no other structural changes were found. However,more » under irradiation, sufficient Cr diffuses across the interface into the MgO to form a Cr-enriched transition layer that contains spinel precipitates. First-principles calculations indicate that it is energetically favorable to incorporate Cr, but not Fe, substitutionally into MgO. Furthermore, our results indicate that irradiation can be used to form new phases and complexions at interfaces, which may have different radiation tolerance than the pristine structures.« less

  3. Development of low-Cr ODS FeCrAl alloys for accident-tolerant fuel cladding

    NASA Astrophysics Data System (ADS)

    Dryepondt, Sebastien; Unocic, Kinga A.; Hoelzer, David T.; Massey, Caleb P.; Pint, Bruce A.

    2018-04-01

    Low-Cr oxide dispersion strengthened (ODS) FeCrAl alloys were developed as accident tolerant fuel cladding because of their excellent oxidation resistance at very high temperature, high strength and improved radiation tolerance. Fe-12Cr-5Al wt.% gas atomized powder was ball milled with Y2O3+FeO, Y2O3+ZrO2 or Y2O3+TiO2, and the resulting powders were extruded at 950 °C. The resulting fine grain structure, particularly for the Ti and Zr containing alloys, led to very high strength but limited ductility. Comparison with variants of commercial PM2000 (Fe-20Cr-5Al) highlighted the significant impact of the powder consolidation step on the alloy grain size and, therefore, on the alloy mechanical properties at T < 500 °C. These low-Cr compositions exhibited good oxidation resistance at 1400 °C in air and steam for 4 h but could not form a protective alumina scale at 1450 °C, similar to observations for fine grained PM2000 alloys. The effect of alloy grain size, Zr and Ti additions, and impurities on the alloy mechanical and oxidation behaviors are discussed.

  4. [CrIII(NCMe)6]3+--a labile CrIII source enabling formation of Cr[M(CN)6] (M=V, Cr, Mn, Fe) Prussian blue-type magnetic materials.

    PubMed

    Nelson, Kendric J; Daniels, Matthew C; Reiff, William M; Troff, Shayla A; Miller, Joel S

    2007-11-26

    The kinetic inertness of the hexaaquachromium(III) (kH2O=2.4x10(-6) s(-1)) has led to challenges with respect to incorporating CrIII ions into Prussian blue-type materials; however, hexakis(acetonitrile)chromium(III) was shown to be substantially more labile (approximately 10(4) times) and enables a new synthetic route for the synthesis of these materials via nonaqueous solvents. The synthesis, spectroscopic, and physical properties of Cr[M(CN)6] (M=V, Cr, Mn, Fe) Prussian blue analogues synthesized from [CrIII(NCMe)6]3+ and the corresponding [MIII(CN)6]3- are described. All these compounds {(NEt4)0.02CrIII[VIII(CN)6]0.98(BF4)(0.08).0.10MeCN (1), CrIII[CrIII(CN)6].0.16MeCN (2), CrIII[MnIII(CN)6].0.10MeCN (3), and (NEt4)0.04CrIII0.64CrIV0.40[FeII(CN)6]0.40[FeIII(CN)6]0.60(BF4)(0.16).1.02MeCN (4)} are ferrimagnets exhibiting cluster-glass behavior. Strong antiferromagnetic coupling was observed for M=V, Cr, and Mn with Weiss constants (theta) ranging from -132 to -524 K; and in 2, where the strongest coupling is observed (theta=-524 K), the highest Tc (110 K) value was observed. Weak antiferromagnetic coupling was observed for M=Fe (theta=-12 K) leading to the lowest Tc (3 K) value in this series. Weak coupling and the low Tc value observed in 4 were additionally contributed by the presence of both [FeII(CN)6]4- and [FeIII(CN)6]3- as confirmed by 57Fe-Mössbauer spectroscopy.

  5. Solar cell with silicon oxynitride dielectric layer

    DOEpatents

    Shepherd, Michael; Smith, David D

    2015-04-28

    Solar cells with silicon oxynitride dielectric layers and methods of forming silicon oxynitride dielectric layers for solar cell fabrication are described. For example, an emitter region of a solar cell includes a portion of a substrate having a back surface opposite a light receiving surface. A silicon oxynitride (SiO.sub.xN.sub.y, 0layer is disposed on the back surface of the portion of the substrate. A semiconductor layer is disposed on the silicon oxynitride dielectric layer.

  6. Process for depositing Cr-bearing layer

    DOEpatents

    Ellis, Timothy W.; Lograsso, Thomas A.; Eshelman, Mark A.

    1995-05-09

    A method of applying a Cr-bearing layer to a substrate, comprises introducing an organometallic compound, in vapor or solid powder form entrained in a carrier gas to a plasma of an inductively coupled plasma torch or device to thermally decompose the organometallic compound and contacting the plasma and the substrate to be coated so as to deposit the Cr-bearing layer on the substrate. A metallic Cr, Cr alloy or Cr compound such as chromium oxide, nitride and carbide can be provided on the substrate. Typically, the organometallic compound is introduced to an inductively coupled plasma torch that is disposed in ambient air so to thermally decompose the organometallic compound in the plasma. The plasma is directed at the substrate to deposit the Cr-bearing layer or coating on the substrate.

  7. Process for depositing Cr-bearing layer

    DOEpatents

    Ellis, T.W.; Lograsso, T.A.; Eshelman, M.A.

    1995-05-09

    A method of applying a Cr-bearing layer to a substrate, comprises introducing an organometallic compound, in vapor or solid powder form entrained in a carrier gas to a plasma of an inductively coupled plasma torch or device to thermally decompose the organometallic compound and contacting the plasma and the substrate to be coated so as to deposit the Cr-bearing layer on the substrate. A metallic Cr, Cr alloy or Cr compound such as chromium oxide, nitride and carbide can be provided on the substrate. Typically, the organometallic compound is introduced to an inductively coupled plasma torch that is disposed in ambient air so to thermally decompose the organometallic compound in the plasma. The plasma is directed at the substrate to deposit the Cr-bearing layer or coating on the substrate. 7 figs.

  8. Literature review report on atomistic modeling tools for FeCrAl alloys

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

    Zhang, Yongfeng; Schwen, Daniel; Martinez, Enrique

    2015-12-01

    This reports summarizes the literature review results on atomistic tools, particularly interatomic potentials used in molecular dynamics simulations, for FeCrAl ternary alloys. FeCrAl has recently been identified as a possible cladding concept for accident tolerant fuels for its superior corrosion resistance. Along with several other concepts, an initial evaluation and recommendation are desired for FeCrAl before it’s used in realistic fuels. For this purpose, sufficient understanding on the in-reactor behavior of FeCrAl needs to be grained in a relatively short timeframe, and multiscale modeling and simulations have been selected as an efficient measure to supplement experiments and in-reactor testing formore » better understanding on FeCrAl. For the limited knowledge on FeCrAl alloys, the multiscale modeling approach relies on atomistic simulations to obtain the missing material parameters and properties. As a first step, atomistic tools have to be identified and this is the purpose of the present report. It was noticed during the literature survey that no interatomic potentials currently available for FeCrAl. Here, we summarize the interatomic potentials available for FeCr alloys for possible molecular dynamics studies using FeCr as surrogate materials. Other atomistic methods such as lattice kinetic Monte Carlo are also included in this report. A couple of research topics at the atomic scale are suggested based on the literature survey.« less

  9. Synthesis and characterization of Cr doped CoFe2O4

    NASA Astrophysics Data System (ADS)

    Verma, Kavita; Patel, K. R.; Ram, Sahi; Barbar, S. K.

    2016-05-01

    Polycrystalline samples of pure and Cr-doped cobalt ferrite (CoFe2O4 and CoCrFeO4) were prepared by solid state reaction route method. X-ray diffraction pattern infers that both the samples are in single phase with Fd3m space group. Slight reduction in the lattice parameter of CoCrFeO4 has been observed as compared to CoFe2O4. The dielectric dispersion has been explained on the basis of Fe2+ ↔ Fe3+ hopping mechanism. The polarizations at lower frequencies are mainly attributed to electronic exchange between Fe2+ ↔ Fe3+ ions on the octahedral site in the ferrite lattice. In the present system a part from n-type charge carrier (Fe3+/Fe2+), the presence of (Co3+/Co2+) ions give rise to p-type charge carrier. Therefore in addition to n-type charge carrier, the local displacement of p-type charge carrier in direction of external electric field also contributes to net polarization. However, the dielectric constant and loss tangent of CoCrFeO4 are found to be lower than CoFe2O4 and is attributed to the availability of ferrous ion. CoCrFeO4 have less amount of ferrous ion available for polarization as compared to that of CoFe2O4. The impedance spectra reveal a grain interior contribution to the conduction process.

  10. Formation of thick stratiform Fe-Ti oxide layers in layered intrusion and frequent replenishment of fractionated mafic magma: Evidence from the Panzhihua intrusion, SW China

    NASA Astrophysics Data System (ADS)

    Song, Xie-Yan; Qi, Hua-Wen; Hu, Rui-Zhong; Chen, Lie-Meng; Yu, Song-Yue; Zhang, Jia-Fei

    2013-03-01

    Panzhihua intrusion is one of the largest layered intrusions that hosts huge stratiform Fe-Ti oxide layers in the central part of the Emeishan large igneous province, SW China. Up to 60 m thick stratiform massive Fe-Ti oxide layers containing 85 modal% of magnetite and ilmenite and overlying magnetite gabbro compose cyclic units of the Lower Zone of the intrusion. The cyclic units of the Middle Zone consist of magnetite gabbro and overlying gabbro. In these cyclic units, contents of Fe2O3(t), TiO2 and Cr and Fe3+/Ti4+ ratio of the rocks decrease upward, Cr content of magnetite and forsterite percentage of olivine decrease as well. The Upper Zone consists of apatite gabbro characterized by enrichment of incompatible elements (e.g., 12-18 ppm La, 20-28 ppm Y) and increasing of Fe3+/Ti4+ ratio (from 1.3 to 2.3) upward. These features indicate that the Panzhihua intrusion was repeatedly recharged by more primitive magma and evolved magmas had been extracted. Calculations using MELTS indicate that extensive fractionation of olivine and clinopyroxene in deep level resulted in increasing Fe and Ti contents in the magma. When these Fe-Ti-enriched magmas were emplaced along the base of the Panzhihua intrusion, Fe-Ti oxides became an early crystallization phase, leading to a residual magma of lower density. We propose that the unusually thick stratiform Fe-Ti oxide layers resulted from coupling of gravity settling and sorting of the crystallized Fe-Ti oxides from Fe-Ti-enriched magmas and frequent magma replenishment along the floor of the magma chamber.

  11. Irradiation-enhanced α' precipitation in model FeCrAl alloys

    DOE PAGES

    Edmondson, Philip D.; Briggs, Samuel A.; Yamamoto, Yukinori; ...

    2016-02-17

    We have irradiated the model FeCrAl alloys with varying compositions (Fe(10–18)Cr(10–6)Al at.%) with a neutron at ~ 320 to damage levels of ~ 7 displacements per atom (dpa) to investigate the compositional influence on the formation of irradiation-induced Cr-rich α' precipitates using atom probe tomography. In all alloys, significant number densities of these precipitates were observed. Cluster compositions were investigated and it was found that the average cluster Cr content ranged between 51.1 and 62.5 at.% dependent on initial compositions. Furthermore, this is significantly lower than the Cr-content of α' in binary FeCr alloys. As a result, significant partitioning ofmore » the Al from the α' precipitates was also observed.« less

  12. Silicon induced Fe deficiency affects Fe, Mn, Cu and Zn distribution in rice (Oryza sativa L.) growth in calcareous conditions.

    PubMed

    Carrasco-Gil, Sandra; Rodríguez-Menéndez, Sara; Fernández, Beatriz; Pereiro, Rosario; de la Fuente, Vicenta; Hernandez-Apaolaza, Lourdes

    2018-04-01

    A protective effect by silicon in the amelioration of iron chlorosis has recently been proved for Strategy 1 species, at acidic pH. However in calcareous conditions, the Si effect on Fe acquisition and distribution is still unknown. In this work, the effect of Si on Fe, Mn, Cu and Zn distribution was studied in rice (Strategy 2 species) under Fe sufficiency and deficiency. Plants (+Si or-Si) were grown initially with Fe, and then Fe was removed from the nutrient solution. The plants were then analysed using a combined approach including LA-ICP-MS images for each element of interest, the analysis of the Fe and Si concentration at different cell layers of root and leaf cross sections by SEM-EDX, and determining the apoplastic Fe, total micronutrient concentration and oxidative stress indexes. A different Si effect was observed depending on plant Fe status. Under Fe sufficiency, Si supply increased Fe root plaque formation, decreasing Fe concentration inside the root and increasing the oxidative stress in the plants. Therefore, Fe acquisition strategies were activated, and Fe translocation rate to the aerial parts was increased, even under an optimal Fe supply. Under Fe deficiency, +Si plants absorbed Fe from the plaque more rapidly than -Si plants, due to the previous activation of Fe deficiency strategies during the growing period (+Fe + Si). Higher Fe plaque formation due to Si supply during the growing period reduced Fe uptake and could activate Fe deficiency strategies in rice, making it more efficient against Fe chlorosis alterations. Silicon influenced Mn and Cu distribution in root. Copyright © 2018 Elsevier Masson SAS. All rights reserved.

  13. Manganese containing layer for magnetic recording media

    DOEpatents

    Lambeth, David N.; Lee, Li-Lien; Laughlin, David E.

    1999-01-01

    The present invention provides for a magnetic recording media incorporating Mn-containing layers between a substrate and a magnetic layer to provide media having increased coercivity and lower noise. The Mn-containing layer can be incorporated in a rotating, translating or stationary recording media to operate in conjunction with magnetic transducing heads for recording and reading of magnetic data, as well as other applications. The magnetic recording medium of the invention preferably includes a Co or Co alloy film magnetic layer, and Mn-containing layer, preferably comprised of VMn, TiMn, MnZn, CrMnMo, CrMnW, CrMnV, and CrMnTi, and most preferably a CrMn alloy, disposed between the substrate and the magnetic layer to promote an epitaxial crystalline structure in the magnetic layer. The medium can further include seed layers, preferably polycrystalline MgO for longitudinal media, underlayers, and intermediate layers. Underlayers and intermediate layers are comprised of materials having either an A2 structure or a B2-ordered crystalline structure disposed between the seed layer and the magnetic layer. Materials having an A2 structure are preferably Cr or Cr alloys, such as CrV, CrMo, CrW and CrTi. Materials having a B2-ordered structure having a lattice constant that is substantially comparable to that of Cr, such as those preferably selected from the group consisting of NiAl, AILCo, FeAl, FeTi, CoFe, CoTi, CoHf, CoZr, NiTi, CuBe, CuZn, A-LMn, AlRe, AgMg, and Al.sub.2 FeMn.sub.2, and is most preferably FeAl or NiAl.

  14. Hydrogen-Resistant Fe/Ni/Cr-Base Superalloy

    NASA Technical Reports Server (NTRS)

    Bhat, Biliyar N.; Chen, Po-Shou; Panda, Binayak

    1994-01-01

    Strong Fe/Ni/Cr-base hydrogen- and corrosion-resistant alloy developed. Superalloy exhibits high strength and exceptional resistance to embrittlement by hydrogen. Contains two-phase microstructure consisting of conductivity precipitated phase in conductivity matrix phase. Produced in wrought, weldable form and as castings, alloy maintains high ductility and strength in air and hydrogen. Strength exceeds previously known Fe/Cr/Ni hydrogen-, oxidation-, and corrosion-resistant alloys. Provides higher strength-to-weight ratios for lower weight in applications as storage vessels and pipes that must contain hydrogen.

  15. Mechanical properties of neutron-irradiated model and commercial FeCrAl alloys

    NASA Astrophysics Data System (ADS)

    Field, Kevin G.; Briggs, Samuel A.; Sridharan, Kumar; Howard, Richard H.; Yamamoto, Yukinori

    2017-06-01

    The development and understanding of the mechanical properties of neutron-irradiated FeCrAl alloys is increasingly a critical need as these alloys continue to become more mature for nuclear reactor applications. This study focuses on the mechanical properties of model FeCrAl alloys and of a commercial FeCrAl alloy neutron-irradiated to up to 13.8 displacements per atom (dpa) at irradiation temperatures between 320 and 382 °C. Tensile tests were completed at room temperature and at 320 °C, and a subset of fractured tensile specimens was examined by scanning electron microscopy. Results showed typical radiation hardening and embrittlement indicative of high chromium ferritic alloys with strong chromium composition dependencies at lower doses. At and above 7.0 dpa, the mechanical properties saturated for both the commercial and model FeCrAl alloys, although brittle cleavage fracture was observed at the highest dose in the model FeCrAl alloy with the highest chromium content (18 wt %). The results suggest the composition and microstructure of FeCrAl alloys plays a critical role in the mechanical response of FeCrAl alloys irradiated near temperatures relevant to light water reactors.

  16. Viability of thin wall tube forming of ATF FeCrAl

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

    Maloy, Stuart Andrew; Aydogan, Eda; Anderoglu, Osman

    Fabrication of thin walled tubing of FeCrAl alloys is critical to its success as a candidate enhanced accident-tolerant fuel cladding material. Alloys that are being investigated are Generation I and Generation II FeCrAl alloys produced at ORNL and an ODS FeCrAl alloy, MA-956 produced by Special Metals. Gen I and Gen II FeCrAl alloys were provided by ORNL and MA-956 was provided by LANL (initially produced by Special Metals). Three tube development efforts were undertaken. ORNL led the FeCrAl Gen I and Gen II alloy development and tube processing studies through drawing tubes at Rhenium Corporation. LANL received alloys frommore » ORNL and led tube processing studies through drawing tubes at Century Tubing. PNNL led the development of tube processing studies on MA-956 through pilger processing working with Sandvik Corporation. A summary of the recent progress on tube development is provided in the following report and a separate ORNL report: ORNL/TM-2015/478, “Development and Quality Assessments of Commercial Heat Production of ATF FeCrAl Tubes”.« less

  17. Eutectic equilibria in the quaternary system Fe-Cr-Mn-C

    NASA Technical Reports Server (NTRS)

    Nowotny, H.; Wayne, S.; Schuster, J. C.

    1982-01-01

    The constitution of the quaternary system, Fe-Cr-Mn-C and to a lesser extent of the quinary system, Fe-Cr-Mn-Al-C were examined for in situ composite alloy candidates. Multivariant eutectic compositions were determined from phase equilibria studies wherein M7C3 carbides (approximately 30% by volume) formed from the melt within gamma iron. An extended field of the hexagonal carbide, (Cr, Fe, Mn)7 C3, was found without undergoing transformation to the orthorhombic structure. Increasing stability for this carbide was found for higher ratios of Cr/Fe(+) Cr + Mn. Aluminum additions promoted a ferritic matrix while manganese favored the desired gamma austenitic matrix. In coexistence with the matrix phase, chromium enters preferentially the carbide phase while manganese distributes equally between the gamma matrix and the M7C3 carbide. The composition and lattice parameters of the carbide and matrix phases were determined to establish their respective stabilities.

  18. Microstructure and mechanical behavior of Zr substrates coated with FeCrAl and Mo by cold-spraying

    NASA Astrophysics Data System (ADS)

    Park, Dong Jun; Kim, Hyun Gil; Jung, Yang Il; Park, Jung Hwan; Yang, Jae Ho; Koo, Yang Hyun

    2018-06-01

    FeCrAl and Mo layers were cold-sprayed onto a Zr surface, with the Mo layer introduced between the FeCrAl coating and the Zr matrix preventing high-temperature interdiffusion. Microstructural characterization of the first-deposited Mo layer and the Zr matrix immediately below the Mo/Zr interface was performed using transmission electron microscopy, and near-interface elemental distributions were obtained using energy-dispersive X-ray spectroscopy. The deformation of the coated Mo powder induced the formation of microbands and mechanically interlocked nanoscale structures. The mechanical behavior of Zr with a coating layer was compared with those characteristic of conventional Zr samples. The coated sample showed smaller strength reduction in the test conducted at elevated temperature. The hardness and fracture morphology of the Zr matrix near the interface region were investigated to determine the effect of impacting Mo particles on the matrix microstructure. The enhanced hardness and cleavage fracture morphology of the Zr matrix immediately below the Mo/Zr interface indicated the occurrence of localized deformation owing to Mo particle impact.

  19. Magnetism and electronic structure of CoFeCrX (X = Si, Ge) Heusler alloys

    NASA Astrophysics Data System (ADS)

    Jin, Y.; Kharel, P.; Lukashev, P.; Valloppilly, S.; Staten, B.; Herran, J.; Tutic, I.; Mitrakumar, M.; Bhusal, B.; O'Connell, A.; Yang, K.; Huh, Y.; Skomski, R.; Sellmyer, D. J.

    2016-08-01

    The structural, electronic, and magnetic properties of CoFeCrX (X = Si, Ge) Heusler alloys have been investigated. Experimentally, the alloys were synthesized in the cubic L21 structure with small disorder. The cubic phase of CoFeCrSi was found to be highly stable against heat treatment, but CoFeCrGe disintegrated into other new compounds when the temperature reached 402 °C (675 K). Although the first-principle calculation predicted the possibility of tetragonal phase in CoFeCrGe, the tetragonal phase could not be stabilized experimentally. Both CoFeCrSi and CoFeCrGe compounds showed ferrimagnetic spin order at room temperature and have Curie temperatures (TC) significantly above room temperature. The measured TC for CoFeCrSi is 790 K but that of CoFeCrGe could not be measured due to its dissociation into new compounds at 675 K. The saturation magnetizations of CoFeCrSi and CoFeCrGe are 2.82 μB/f.u. and 2.78 μB/f.u., respectively, which are close to the theoretically predicted value of 3 μB/f.u. for their half-metallic phases. The calculated band gaps for CoFeCrSi and CoFeCrGe are, respectively, 1 eV and 0.5 eV. These materials have potential for spintronic device applications, as they exhibit half-metallic electronic structures with large band gaps, and Curie temperatures significantly above room temperature.

  20. Improve oxidation resistance at high temperature by nanocrystalline surface layer

    NASA Astrophysics Data System (ADS)

    Xia, Z. X.; Zhang, C.; Huang, X. F.; Liu, W. B.; Yang, Z. G.

    2015-08-01

    An interesting change of scale sequence occurred during oxidation of nanocrystalline surface layer by means of a surface mechanical attrition treatment. The three-layer oxide structure from the surface towards the matrix is Fe3O4, spinel FeCr2O4 and corundum (Fe,Cr)2O3, which is different from the typical two-layer scale consisted of an Fe3O4 outer layer and an FeCr2O4 inner layer in conventional P91 steel. The diffusivity of Cr, Fe and O is enhanced concurrently in the nanocrystalline surface layer, which causes the fast oxidation in the initial oxidation stage. The formation of (Fe,Cr)2O3 inner layer would inhabit fast diffusion of alloy elements in the nanocrystalline surface layer of P91 steel in the later oxidation stage, and it causes a decrease in the parabolic oxidation rate compared with conventional specimens. This study provides a novel approach to improve the oxidation resistance of heat resistant steel without changing its Cr content.

  1. Electronic and Optical Properties of a Semiconducting Spinel (Fe 2 CrO 4 )

    DOE PAGES

    Chambers, Scott A.; Droubay, Timothy C.; Kaspar, Tiffany C.; ...

    2017-01-13

    Epitaxial chromium ferrite (Fe 2CrO 4), prepared by state-of-the-art oxygen plasma assisted molecular beam epitaxy, is shown to exhibit unusual electronic transport properties driven by the crystallographic structure and composition of the material. By replacing 1/3 of the Fe cations with Cr converts the host ferrimagnet from a metal into a semiconductor by virtue of its fixed valence (3+); Cr substitutes for Fe at B sites in the spinel lattice. Conversely, replacing 2/3 of the Fe cations with Cr results in an insulator. Three candidate conductive paths, all involving electron hopping between Fe 2+ and Fe 3+, are identified inmore » Fe 2CrO 4. Moreover, Fe 2CrO 4 is shown to be photoconductive across the visible portion of the electromagnetic spectrum. As a result, this material is of potential interest for important photo-electrochemical processes such as water splitting.« less

  2. Atomistic simulation of the influence of Cr on the mobility of the edge dislocation in Fe(Cr) alloys

    NASA Astrophysics Data System (ADS)

    Hafez Haghighat, S. M.; Terentyev, D.; Schäublin, R.

    2011-10-01

    In this work Fe-Cr compounds, as model alloys for the ferritic base steels that are considered as main candidates for the structural materials of the future fusion reactors, are studied using molecular dynamics simulations. The Cr or so-called α' precipitates, which are obstacles to dislocations, affect mechanical properties, leading to hardening and loss of ductility. The flow stress to move an edge dislocation in a Cr solid solution in pure Fe is studied as a function of Cr content. The strength of a nanometric Cr precipitate as obstacle to an edge dislocation in pure Fe is investigated as a function of its Cr content. Results show that with increasing Cr content the precipitate obstacle strength increases, with a strong sensitivity to the local atomic order. Temperature induces a monotonic decrease of the flow stress of the Cr solid solution and of the Cr precipitate obstacle strength.

  3. Buried Porous Silicon-Germanium Layers in Monocrystalline Silicon Lattices

    NASA Technical Reports Server (NTRS)

    Fathauer, Robert W. (Inventor); George, Thomas (Inventor); Jones, Eric W. (Inventor)

    1998-01-01

    Monocrystalline semiconductor lattices with a buried porous semiconductor layer having different chemical composition is discussed and monocrystalline semiconductor superlattices with a buried porous semiconductor layers having different chemical composition than that of its monocrystalline semiconductor superlattice are discussed. Lattices of alternating layers of monocrystalline silicon and porous silicon-germanium have been produced. These single crystal lattices have been fabricated by epitaxial growth of Si and Si-Ge layers followed by patterning into mesa structures. The mesa structures are strain etched resulting in porosification of the Si-Ge layers with a minor amount of porosification of the monocrystalline Si layers. Thicker Si-Ge layers produced in a similar manner emitted visible light at room temperature.

  4. Aqueous chemical growth of alpha-Fe2O3-alpha-Cr203 nanocompositethin films

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

    Vayssieres, Lionel; Guo, Jinghua; Nordgren, Joseph

    2001-06-30

    We are reporting here on the inexpensive fabrication and optical properties of an iron(III) oxide chromium(III) oxide nanocomposite thin film of corundum crystal structure. Its novel and unique-designed architecture consists of uniformed, well-defined and oriented nanorods of Hematite (alpha-Fe2O3) of 50 nm in diameter and 500nm in length and homogeneously distributed nonaggregated monodisperse spherical nanoparticles of Eskolaite (alpha-Cr2O3) of 250 nm in diameter. This alpha-Fe2O3 alpha-Cr2O3 nanocomposite thin film is obtained by growing, directly onto transparent polycrystalline conducting substrate, an oriented layer of hematite nanorods and growing subsequently, the eskolaite layer. The synthesis is carried out by a template-free, low-temperature,more » multilayer thin film coating process using aqueous solution of metal salts as precursors. Almost 100 percent of the light is absorbed by the composite film between 300 and 525 nm and 40 percent at 800 nm which yields great expectations as photoanode materials for photovoltaic cells and photocatalytic devices.« less

  5. Mechanical properties of neutron-irradiated model and commercial FeCrAl alloys

    DOE PAGES

    Field, Kevin G.; Briggs, Samuel A.; Sridharan, Kumar; ...

    2017-03-28

    The development and understanding of the mechanical properties of neutron-irradiated FeCrAl alloys is increasingly a critical need as these alloys continue to become more mature for nuclear reactor applications. This study focuses on the mechanical properties of model FeCrAl alloys and of a commercial FeCrAl alloy neutron-irradiated to up to 13.8 displacements per atom (dpa) at irradiation temperatures between 320 and 382 °C. Tensile tests were completed at room temperature and at 320 °C, and a subset of fractured tensile specimens was examined by scanning electron microscopy. Results showed typical radiation hardening and embrittlement indicative of high chromium ferritic alloysmore » with strong chromium composition dependencies at lower doses. At and above 7.0 dpa, the mechanical properties saturated for both the commercial and model FeCrAl alloys, although brittle cleavage fracture was observed at the highest dose in the model FeCrAl alloy with the highest chromium content (18 wt %). Finally, the results suggest the composition and microstructure of FeCrAl alloys plays a critical role in the mechanical response of FeCrAl alloys irradiated near temperatures relevant to light water reactors.« less

  6. Magnetic effect on oxide-scale growth of Fe-5Cr alloy

    NASA Astrophysics Data System (ADS)

    Zhou, C. H.; Li, X. W.; Wang, S. H.; Ma, H. T.

    2018-01-01

    The oxidation behaviour of Fe-5Cr alloy was investigated at 650°C in the presence of magnetic field. Results indicated that the oxide scales were both consisted of an outer Fe-oxide scale and an inner mixed-oxide scale in the presence or absence of magnetic field. The oxide-scale growth of Fe-5Cr alloy, gained by measuring the oxide-scale thickness, was verified to follow parabolic lawyer. And the oxidation kinetics showed that the applied magnetic field retarded the oxide-scale growth of Fe-5Cr alloy.

  7. Role of Y in the oxidation resistance of CrAlYN coatings

    NASA Astrophysics Data System (ADS)

    Domínguez-Meister, S.; El Mrabet, S.; Escobar-Galindo, R.; Mariscal, A.; Jiménez de Haro, M. C.; Justo, A.; Brizuela, M.; Rojas, T. C.; Sánchez-López, J. C.

    2015-10-01

    CrAlYN coatings with different aluminum (4-12 at.%) and yttrium (2-5 at.%) contents are deposited by d.c. reactive magnetron sputtering on silicon and M2 steel substrates using metallic targets and Ar/N2 mixtures. The influence of the nanostructure and chemical elemental distribution on the oxidation resistance after heating in air at 1000 °C is studied by means of cross-sectional scanning electron microscopy (X-SEM), energy dispersive X-ray analysis (EDX), X-ray diffraction (XRD) and glow discharge optical emission spectroscopy (GD-OES). The sequential exposure to the metallic targets during the synthesis leads to a multilayer structure where concentration of metallic elements (Cr, Al and Y) is changing periodically. A good oxidation resistance is observed when Al- and Y-rich regions are separated by well-defined CrN layers, maintaining crystalline coherence along the columnar structure. This protective behavior is independent of the type of substrate and corresponds to the formation of a thin mixed (Al, Cr)-oxide scale that protects the film underneath. The GD-OES and XRD analysis have demonstrated that Y acts as a reactive element, blocking the Fe and C atoms diffusion from the steel and favoring higher Al/Cr ratio in the passivation layer after heating. The coating with Y content around 4 at.% exhibited the best performance with a thinner oxide scale, a delay in the CrN decomposition and transformation to Cr2N, and a more effective Fe and C blocking.

  8. Methods To Determine the Silicone Oil Layer Thickness in Sprayed-On Siliconized Syringes.

    PubMed

    Loosli, Viviane; Germershaus, Oliver; Steinberg, Henrik; Dreher, Sascha; Grauschopf, Ulla; Funke, Stefanie

    2018-01-01

    The silicone lubricant layer in prefilled syringes has been investigated with regards to siliconization process performance, prefilled syringe functionality, and drug product attributes, such as subvisible particle levels, in several studies in the past. However, adequate methods to characterize the silicone oil layer thickness and distribution are limited, and systematic evaluation is missing. In this study, white light interferometry was evaluated to close this gap in method understanding. White light interferometry demonstrated a good accuracy of 93-99% for MgF 2 coated, curved standards covering a thickness range of 115-473 nm. Thickness measurements for sprayed-on siliconized prefilled syringes with different representative silicone oil distribution patterns (homogeneous, pronounced siliconization at flange or needle side, respectively) showed high instrument (0.5%) and analyst precision (4.1%). Different white light interferometry instrument parameters (autofocus, protective shield, syringe barrel dimensions input, type of non-siliconized syringe used as base reference) had no significant impact on the measured average layer thickness. The obtained values from white light interferometry applying a fully developed method (12 radial lines, 50 mm measurement distance, 50 measurements points) were in agreement with orthogonal results from combined white and laser interferometry and 3D-laser scanning microscopy. The investigated syringe batches (lot A and B) exhibited comparable longitudinal silicone oil layer thicknesses ranging from 170-190 nm to 90-100 nm from flange to tip and homogeneously distributed silicone layers over the syringe barrel circumference (110- 135 nm). Empty break-loose (4-4.5 N) and gliding forces (2-2.5 N) were comparably low for both analyzed syringe lots. A silicone oil layer thickness of 100-200 nm was thus sufficient for adequate functionality in this particular study. Filling the syringe with a surrogate solution including short

  9. Effect of annealing on magnetoresistance and microstructure of multilayered CoFe/Cu systems with different buffer layer

    NASA Astrophysics Data System (ADS)

    Bannikova, N. S.; Milyaev, M. A.; Naumova, L. I.; Proglyado, V. V.; Krinitsina, T. P.; Chernyshova, T. A.; Ustinov, V. V.

    2015-02-01

    The effects of annealing on the structure, magnetic hysteresis, and magnetoresistance of [Co90Fe10(15 Å)/Cu(23 Å)] n superlattices with Cr and Co90Fe10 buffer layers of different thicknesses have been studied. The optimum temperature and time of annealing that increase the magnetoresistance were shown to depend on the buffer layer thickness. The coefficients of effective interlayer diffusion due to the annealing have been determined.

  10. Atomistic simulations of stainless steels: a many-body potential for the Fe-Cr-C system.

    PubMed

    Henriksson, K O E; Björkas, C; Nordlund, K

    2013-11-06

    Stainless steels found in real-world applications usually have some C content in the base Fe-Cr alloy, resulting in hard and dislocation-pinning carbides-Fe3C (cementite) and Cr23C6-being present in the finished steel product. The higher complexity of the steel microstructure has implications, for example, for the elastic properties and the evolution of defects such as Frenkel pairs and dislocations. This makes it necessary to re-evaluate the effects of basic radiation phenomena and not simply to rely on results obtained from purely metallic Fe-Cr alloys. In this report, an analytical interatomic potential parameterization in the Abell-Brenner-Tersoff form for the entire Fe-Cr-C system is presented to enable such calculations. The potential reproduces, for example, the lattice parameter(s), formation energies and elastic properties of the principal Fe and Cr carbides (Fe3C, Fe5C2, Fe7C3, Cr3C2, Cr7C3, Cr23C6), the Fe-Cr mixing energy curve, formation energies of simple C point defects in Fe and Cr, and the martensite lattice anisotropy, with fair to excellent agreement with empirical results. Tests of the predictive power of the potential show, for example, that Fe-Cr nanowires and bulk samples become elastically stiffer with increasing Cr and C concentrations. High-concentration nanowires also fracture at shorter relative elongations than wires made of pure Fe. Also, tests with Fe3C inclusions show that these act as obstacles for edge dislocations moving through otherwise pure Fe.

  11. Atomistic simulations of stainless steels: a many-body potential for the Fe-Cr-C system

    NASA Astrophysics Data System (ADS)

    Henriksson, K. O. E.; Björkas, C.; Nordlund, K.

    2013-11-01

    Stainless steels found in real-world applications usually have some C content in the base Fe-Cr alloy, resulting in hard and dislocation-pinning carbides—Fe3C (cementite) and Cr23C6—being present in the finished steel product. The higher complexity of the steel microstructure has implications, for example, for the elastic properties and the evolution of defects such as Frenkel pairs and dislocations. This makes it necessary to re-evaluate the effects of basic radiation phenomena and not simply to rely on results obtained from purely metallic Fe-Cr alloys. In this report, an analytical interatomic potential parameterization in the Abell-Brenner-Tersoff form for the entire Fe-Cr-C system is presented to enable such calculations. The potential reproduces, for example, the lattice parameter(s), formation energies and elastic properties of the principal Fe and Cr carbides (Fe3C, Fe5C2, Fe7C3, Cr3C2, Cr7C3, Cr23C6), the Fe-Cr mixing energy curve, formation energies of simple C point defects in Fe and Cr, and the martensite lattice anisotropy, with fair to excellent agreement with empirical results. Tests of the predictive power of the potential show, for example, that Fe-Cr nanowires and bulk samples become elastically stiffer with increasing Cr and C concentrations. High-concentration nanowires also fracture at shorter relative elongations than wires made of pure Fe. Also, tests with Fe3C inclusions show that these act as obstacles for edge dislocations moving through otherwise pure Fe.

  12. Porous Silicon as Antireflecting Layer

    NASA Astrophysics Data System (ADS)

    Kosoglu, Gulsen; Yumak, Mehmet; Okmen, Selim; Ozatay, Ozhan; Skarlatos, Yani; Garcia, Carlos

    2013-03-01

    The main aim in photovoltaic industry is to produce efficient and energy competitive solar cell modules at low cost. Efficient AntiReflection Coatings (ARC) improve light collection and thereby increase the current output of solar cells. Broadband ARCs are desirable for efficient application over the entire solar spectrum and porous silicon layers as antireflective coating layers provide successful light collection. In the study the most critical physical parameters of porous silicon are examined, homogeneous and uniform porous layers are produced. The photoluminescence spectrum and optical parameters of porous layers have been investigated, and we are now in the process of improving the efficiency of the device by modulating the structure of the porous silicon layers and studying its photovoltaic characteristics. We would like to thank to Mr. Aziz U. Caliskan and his group for their valuable support from TUBITAK YITAL. This Project is supported by Bogazici University Research Funding: 5782, TUBITAK Grant : 209T099, and Bogazici University Infrared Funding: 6121.

  13. Microstructural control of FeCrAl alloys using Mo and Nb additions

    DOE PAGES

    Sun, Zhiqian; Bei, Hongbin; Yamamoto, Yukinori

    2017-08-14

    The effects of Mo and Nb additions on the microstructure and mechanical properties of two FeCrAl alloys were studied in this paper. Fine and uniform recrystallized grain structures (~ 20–30 μm) were achieved in both alloys through suitable annealing after warm-rolling. The formation of Fe 2Nb-type Laves phase precipitates in the Nb-containing FeCrAl alloy effectively stabilized the deformed and recrystallized microstructures. The Mo-containing FeCrAl alloy exhibited strong γ texture fiber after annealing at 650–900 °C, whereas the annealed Nb-containing FeCrAl alloy had much weaker texture. Finally, both strength and ductility decreased as the grain size increased in both alloys.

  14. Precipitation of α' in neutron irradiated commercial FeCrAl alloys

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

    Field, Kevin G.; Littrell, Kenneth C.; Briggs, Samuel A.

    2017-08-17

    In this paper, Alkrothal 720 and Kanthal APMT™, two commercial FeCrAl alloys, were neutron irradiated up to damage doses of 7.0 displacements per atom (dpa) in the temperature range of 320 to 382 °C to characterize the α' precipitation in these alloys using small-angle neutron scattering. Both alloys exhibited α' precipitation. Kanthal APMT™ exhibited higher number densities and volume fraction, a result attributed to its higher Cr content compared with Alkrothal 720. Finally, trends observed as a function of damage dose (dpa) are consistent with literature trends for both FeCr and FeCrAl alloys

  15. Database on Performance of Neutron Irradiated FeCrAl Alloys

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

    Field, Kevin G.; Briggs, Samuel A.; Littrell, Ken

    The present report summarizes and discusses the database on radiation tolerance for Generation I, Generation II, and commercial FeCrAl alloys. This database has been built upon mechanical testing and microstructural characterization on selected alloys irradiated within the High Flux Isotope Reactor (HFIR) at Oak Ridge National Laboratory (ORNL) up to doses of 13.8 dpa at temperatures ranging from 200°C to 550°C. The structure and performance of these irradiated alloys were characterized using advanced microstructural characterization techniques and mechanical testing. The primary objective of developing this database is to enhance the rapid development of a mechanistic understanding on the radiation tolerancemore » of FeCrAl alloys, thereby enabling informed decisions on the optimization of composition and microstructure of FeCrAl alloys for application as an accident tolerant fuel (ATF) cladding. This report is structured to provide a brief summary of critical results related to the database on radiation tolerance of FeCrAl alloys.« less

  16. Strengthening due to Cr-rich precipitates in Fe-Cr alloys: Effect of temperature and precipitate composition

    NASA Astrophysics Data System (ADS)

    Terentyev, D.; Hafez Haghighat, S. M.; Schäublin, R.

    2010-03-01

    Molecular dynamics (MD) simulations were carried out to study the interaction between nanometric Cr precipitates and a 1/2 ⟨111⟩{110} edge dislocation (ED) in pure Fe and Fe-9 at. % Cr (Fe-9Cr) random alloy. The aim of this work is to estimate the variation in the pinning strength of the Cr precipitate as a function of temperature, its chemical composition and the matrix composition in which the precipitate is embedded. The dislocation was observed to shear Cr precipitates rather than by-pass via the formation of the Orowan loop, even though a pronounced screw dipole was emerged in the reactions with the precipitates of size larger than 4.5 nm. The screw arms of the formed dipole were not observed to climb thus no point defects were left inside the sheared precipitates, irrespective of simulation temperature. Both Cr solution and Cr precipitates, embedded in the Fe-9Cr matrix, were seen to contribute to the flow stress. The decrease in the flow stress with temperature in the alloy containing Cr precipitates is, therefore, related to the simultaneous change in the matrix friction stress, precipitate resistance, and dislocation flexibility. Critical stress estimated from MD simulations was seen to have a strong dependence on the precipitate composition. If the latter decreases from 95% down to 80%, the corresponding critical stress decreases almost as twice. The results presented here suggest a significant contribution to the flow stress due to the α -α' separation, at least for EDs. The obtained data can be used to validate and to parameterize dislocation dynamics models, where the temperature dependence of the obstacle strength is an essential input data.

  17. Structure and magnetic properties of Co2FeSi film deposited on Si/SiO2 substrate with Cr buffer layer

    NASA Astrophysics Data System (ADS)

    Chatterjee, Payel; Basumatary, Himalay; Raja, M. Manivel

    2018-05-01

    Co2FeSi thin films of 25 nm thickness with 50 nm thick Cr buffer layer was deposited on thermally oxidized Si substrates. Structural and magnetic properties of the films were studied as a function of annealing temperature and substrate temperatures. While the coercivity increases with increase in annealing temperature, it is found to decrease with increase in substrate temperature. A minimum coercivity of 18 Oe has been obtained for the film deposited at 550°C substrate temperature. This was attributed to the formation of L12 phase as observed from the GIXRD studies. The films with a good combination of soft magnetic properties and L21 crystal structure are suitable for spintronic applications.

  18. Characterization of High Damping Fe-Cr-Mo and Fe-Cr-Al Alloys for Naval Ships Application.

    DTIC Science & Technology

    1988-03-01

    austenitic , and martensitic. The high damping Fe-Cr-based alloys are closely related to ferritic stainless steels . Ferritic stainless steel consists of an Fe...cm reveme it Prectiaq #no ’uenf r oy o.o(a tflrowf U S9GO..P Damping; Ship Silencing; Ferritic Stainless Steels ; Ti-Ni 7 LhV I,. Cintunue on roere .r...decreased. E. METALLURGY OF THE IRON-CHROMIUM ALLOY SYSTEM 1. Physical Properties Stainless steels are divided into three main classes: ferritic

  19. Dislocation loop evolution during in-situ ion irradiation of model FeCrAl alloys

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

    Haley, Jack C.; Briggs, Samuel A.; Edmondson, Philip D.

    Model FeCrAl alloys of Fe-10%Cr-5%Al, Fe-12%Cr-4.5%Al, Fe-15%Cr-4%Al, and Fe-18%Cr-3%Al (in wt %) were irradiated with 1 MeV Kr++ ions in-situ with transmission electron microscopy to a dose of 2.5 displacements per atom (dpa) at 320 °C. In all cases, the microstructural damage consisted of dislocation loops with ½< 111 > and <100 > Burgers vectors. The proportion of ½< 111 > dislocation loops varied from ~50% in the Fe-10%Cr-5%Al model alloy and the Fe-18Cr%-3%Al model alloy to a peak of ~80% in the model Fe-15%Cr-4.5%Al alloy. The dislocation loop volume density increased with dose for all alloys and showed signsmore » of approaching an upper limit. The total loop populations at 2.5 dpa had a slight (and possibly insignificant) decline as the chromium content was increased from 10 to 15 wt %, but the Fe-18%Cr-3%Al alloy had a dislocation loop population ~50% smaller than the other model alloys. As a result, the largest dislocation loops in each alloy had image sizes of close to 20 nm in the micrographs, and the median diameters for all alloys ranged from 6 to 8 nm. Nature analysis by the inside-outside method indicated most dislocation loops were interstitial type.« less

  20. Dislocation loop evolution during in-situ ion irradiation of model FeCrAl alloys

    DOE PAGES

    Haley, Jack C.; Briggs, Samuel A.; Edmondson, Philip D.; ...

    2017-07-06

    Model FeCrAl alloys of Fe-10%Cr-5%Al, Fe-12%Cr-4.5%Al, Fe-15%Cr-4%Al, and Fe-18%Cr-3%Al (in wt %) were irradiated with 1 MeV Kr++ ions in-situ with transmission electron microscopy to a dose of 2.5 displacements per atom (dpa) at 320 °C. In all cases, the microstructural damage consisted of dislocation loops with ½< 111 > and <100 > Burgers vectors. The proportion of ½< 111 > dislocation loops varied from ~50% in the Fe-10%Cr-5%Al model alloy and the Fe-18Cr%-3%Al model alloy to a peak of ~80% in the model Fe-15%Cr-4.5%Al alloy. The dislocation loop volume density increased with dose for all alloys and showed signsmore » of approaching an upper limit. The total loop populations at 2.5 dpa had a slight (and possibly insignificant) decline as the chromium content was increased from 10 to 15 wt %, but the Fe-18%Cr-3%Al alloy had a dislocation loop population ~50% smaller than the other model alloys. As a result, the largest dislocation loops in each alloy had image sizes of close to 20 nm in the micrographs, and the median diameters for all alloys ranged from 6 to 8 nm. Nature analysis by the inside-outside method indicated most dislocation loops were interstitial type.« less

  1. Development and Validation of Accident Models for FeCrAl Cladding

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

    Gamble, Kyle Allan Lawrence; Hales, Jason Dean

    2016-08-01

    The purpose of this milestone report is to present the work completed in regards to material model development for FeCrAl cladding and highlight the results of applying these models to Loss of Coolant Accidents (LOCA) and Station Blackouts (SBO). With the limited experimental data available (essentially only the data used to create the models) true validation is not possible. In the absence of another alternative, qualitative comparisons during postulated accident scenarios between FeCrAl and Zircaloy-4 cladded rods have been completed demonstrating the superior performance of FeCrAl.

  2. Fine structure of Fe-Co-Ga and Fe-Cr-Ga alloys with low Ga content

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

    Kleinerman, Nadezhda M., E-mail: kleinerman@imp.uran.ru; Serikov, Vadim V., E-mail: kleinerman@imp.uran.ru; Vershinin, Aleksandr V., E-mail: kleinerman@imp.uran.ru

    2014-10-27

    Investigation of Ga influence on the structure of Fe-Cr and Fe-Co alloys was performed with the use of {sup 57}Fe Mössbauer spectroscopy and X-ray diffraction methods. In the alloys of the Fe-Cr system, doping with Ga handicaps the decomposition of solid solutions, observed in the binary alloys, and increases its stability. In the alloys with Co, Ga also favors the uniformity of solid solutions. The analysis of Mössbauer experiments gives some grounds to conclude that if, owing to liquation, clusterization, or initial stages of phase separation, there exist regions enriched in iron, some amount of Ga atoms prefer to entermore » the nearest surroundings of iron atoms, thus forming binary Fe-Ga regions (or phases)« less

  3. Layered-to-Rock-Salt Transformation in Desodiated Na xCrO 2 ( x 0.4)

    DOE PAGES

    Bo, Shou-Hang; Li, Xin; Toumar, Alexandra J.; ...

    2016-02-01

    O3 layered sodium transition metal oxides (i.e., NaMO 2, M = Ti, V, Cr, Mn, Fe, Co, Ni) are a promising class of cathode materials for Na-ion battery applications. These materials, however, all suffer from severe capacity decay when the extraction of Na exceeds certain capacity limits. Understanding the causes of this capacity decay is critical to unlocking the potential of these materials for battery applications. In this work, we investigate the structural origins of capacity decay for one of the compounds in this class, NaCrO 2. The (de)sodiation processes of NaCrO 2 were studied both in situ and exmore » situ through X-ray and electron diffraction measurements. We demonstrate that Na xCrO 2 (0 < x < 1) remains in the layered structural framework without Cr migration up to a composition of Na 0.4CrO 2. Further removal of Na beyond this composition triggers a layered-to-rock-salt transformation, which converts P'3-Na 0.4CrO 2 into the rock-salt CrO 2 phase. This structural transformation proceeds via the formation of an intermediate O3 Na δCrO 2 phase that contains Cr in both Na and Cr slabs and shares very similar lattice dimensions with those of rock-salt CrO 2. It is intriguing to note that intercalation of alkaline ions (i.e., Na + and Li + ) into the rock-salt CrO 2 and O3 Na δCrO 2 structures is actually possible, albeit in a limited amount (~0.2 per formula unit). When these results were analyzed under the context of electrochemistry data, it was apparent that preventing the layered-to-rock-salt transformation is crucial to improve the cyclability of NaCrO 2. Possible strategies for mitigating this detrimental phase transition are proposed.« less

  4. Atomic-Layer-Deposited Transparent Electrodes for Silicon Heterojunction Solar Cells

    DOE PAGES

    Demaurex, Benedicte; Seif, Johannes P.; Smit, Sjoerd; ...

    2014-11-01

    We examine damage-free transparent-electrode deposition to fabricate high-efficiency amorphous silicon/crystalline silicon heterojunction solar cells. Such solar cells usually feature sputtered transparent electrodes, the deposition of which may damage the layers underneath. Using atomic layer deposition, we insert thin protective films between the amorphous silicon layers and sputtered contacts and investigate their effect on device operation. We find that a 20-nm-thick protective layer suffices to preserve, unchanged, the amorphous silicon layers beneath. Insertion of such protective atomic-layer-deposited layers yields slightly higher internal voltages at low carrier injection levels. However, we identify the presence of a silicon oxide layer, formed during processing,more » between the amorphous silicon and the atomic-layer-deposited transparent electrode that acts as a barrier, impeding hole and electron collection.« less

  5. Hydrogen permeation characteristics of some Fe-Cr-Al alloys

    NASA Astrophysics Data System (ADS)

    Van Deventer, E. H.; Maroni, V. A.

    1983-01-01

    Hydrogen permeation data are reported for two Fe-Cr-Al alloys, Type-405 SS (Cr 14-A1 0.2) and a member of the Fecralloy family of alloys (Cr 16-A1 5). The hydrogen permeability of each alloy (in a partially oxidized condition) was measured over a period of several weeks at randomly selected temperatures (between 150 and 850°C) and upstream H 2 pressures (between 2 and 1.5 × 10 4 Pa). The permeabilities showed considerable scatter with both time and temperature and were 10 2 to 10 3 times lower than those of pure iron, even in strongly reducing environments. The exponent, n, for the relationship between upstream H 2 pressure, P, and permeability, φ, ( φ ~ Pn) was closer to 0.7 than to the expected 0.5, indicating a process limited by surface effects (e.g., surface oxide films) as opposed to bulk material effects. Comparison of these results with prior permeation measurements on other Fe-Cr-Al alloys, on Fe-Cr alloys, and on pure iron shows that the presence of a few weight percent aluminum offers the best prospects for achieving low tritium permeabilities with martensitic and ferritic steels used in fusion-reactor first wall and blanket applications.

  6. Status of FeCrAl ODS Irradiations in the High Flux Isotope Reactor

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

    Field, Kevin G.; Howard, Richard H.

    2016-08-19

    FeCrAl oxide-dispersion strengthened (ODS) alloys are an attractive sub-set alloy class of the more global FeCrAl material class for nuclear applications due to their high-temperature steam oxidation resistance and hypothesized enhanced radiation tolerance. A need currently exists to determine the radiation tolerance of these newly developed alloys. To address this need, a preliminary study was conducted using the High Flux Isotope Reactor (HFIR) to irradiate an early generation FeCrAl ODS alloy, 125YF. Preliminary post-irradiation examination (PIE) on these irradiated specimens have shown good radiation tolerance at elevated temperatures (≥330°C) but possible radiation-induced hardening and embrittlement at irradiations of 200°C tomore » a damage level of 1.9 displacement per atom (dpa). Building on this experience, a new series of irradiations are currently being conceptualized. This irradiation series called the FCAD irradiation program will irradiate the latest generation FeCrAl ODS and FeCr ODS alloys to significantly higher doses. These experiments will provide the necessary information to determine the mechanical performance of irradiated FeCrAl ODS alloys at light water reactor and fast reactor conditions.« less

  7. The effect of annealing on structure and hardness of (Fe-Cr)-50 at.% Al coatings synthesized by mechanical alloying

    NASA Astrophysics Data System (ADS)

    Ciswandi, Aryanto, Didik; Irmaniar, Tjahjono, Arif; Sudiro, Toto

    2018-05-01

    In this research, the deposition of (Fe-Cr)-50at.% Al coatings on low carbon steel was carried out by a mechanical alloying (MA) technique. The MA was performed in a shaker mill for 4 hours. Two types of Fe-Cr powders as starting material were used, high purity Fe-Cr powders: (Fe-12.5Cr)-50Al and (Fe-25Cr)-50Al, and Fe-Cr lump powder: (50FeCr)-50Al (in at.%). The coated samples were then annealed in a vacuum furnace at 700°C for 1h. The characterizations of coating structure before and after annealing were studied by XRD and SEM-EDX, while the coating hardness was measured by micro-Vickers hardness tester. Before annealing, all of coating composition were composed mainly of (Fe,Cr)Al phase. After annealing, the FeAl and Fe0.99Cr0.02Al0.99 intermetallic phases was formed in the (Fe-12.5Cr)-50Al and (Fe-25Cr)-50Al coatings. In addition, Fe2CrAlwas also found in the (Fe-25Cr)-50Al coating. Whilethe AlCr2 intermetallic phase was detected as the main phase of (50FeCr)-50Al coating. The cross-sectional microstructure showed that the (Fe-12.5Cr)-50Al and (Fe-25Cr)-50Al coatings have a smoother structure compared to (50FeCr)-50Al coating. The annealing led to intermetallic phase formation and an increasing coating hardness.

  8. Thermal stability of intermetallic phases in Fe-rich Fe-Cr-Ni-Mo alloys

    DOE PAGES

    Yang, Ying; Tan, Lizhen; Busby, Jeremy T.

    2015-06-12

    Understanding the stability of precipitate phases in the Fe-rich Fe-Cr-Ni-Mo alloys is critical to the alloy design and application of Mo-containing Austenitic steels. Coupled with thermodynamic modeling, stability of the chi and Laves phases in two Fe-Cr-Ni-Mo alloys were investigated at 1000, 850 and 700 °C for different annealing time. The morphologies, compositions and crystal structures of the matrix and precipitate phases were carefully examined by Scanning Electron Microscopy, Electron Probe Microanalysis, X-ray diffraction and Transmission Electron Microscopy. The two key findings resulted from this work. One is that the chi phase is stable at high temperature and transformed intomore » the Laves phase at low temperature. The other is that both the chi and Laves phases have large solubilites of Cr, Mo and Ni, among which the Mo solubility has a major role on the relative stability of the precipitate phases. The developed thermodynamic models were then applied to evaluating the Mo effect on the stability of precipitate phases in AISI 316 and NF709 alloys.« less

  9. Amorphous silicon carbide passivating layers for crystalline-silicon-based heterojunction solar cells

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

    Boccard, Mathieu; Holman, Zachary C.

    Amorphous silicon enables the fabrication of very high-efficiency crystalline-silicon-based solar cells due to its combination of excellent passivation of the crystalline silicon surface and permeability to electrical charges. Yet, amongst other limitations, the passivation it provides degrades upon high-temperature processes, limiting possible post-deposition fabrication possibilities (e.g., forcing the use of low-temperature silver pastes). We investigate the potential use of intrinsic amorphous silicon carbide passivating layers to sidestep this issue. The passivation obtained using device-relevant stacks of intrinsic amorphous silicon carbide with various carbon contents and doped amorphous silicon are evaluated, and their stability upon annealing assessed, amorphous silicon carbide beingmore » shown to surpass amorphous silicon for temperatures above 300 °C. We demonstrate open-circuit voltage values over 700 mV for complete cells, and an improved temperature stability for the open-circuit voltage. Transport of electrons and holes across the hetero-interface is studied with complete cells having amorphous silicon carbide either on the hole-extracting side or on the electron-extracting side, and a better transport of holes than of electrons is shown. Also, due to slightly improved transparency, complete solar cells using an amorphous silicon carbide passivation layer on the hole-collecting side are demonstrated to show slightly better performances even prior to annealing than obtained with a standard amorphous silicon layer.« less

  10. Amorphous silicon carbide passivating layers for crystalline-silicon-based heterojunction solar cells

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

    Boccard, Mathieu; Holman, Zachary C.

    With this study, amorphous silicon enables the fabrication of very high-efficiency crystalline-silicon-based solar cells due to its combination of excellent passivation of the crystalline silicon surface and permeability to electrical charges. Yet, amongst other limitations, the passivation it provides degrades upon high-temperature processes, limiting possible post-deposition fabrication possibilities (e.g., forcing the use of low-temperature silver pastes). We investigate the potential use of intrinsic amorphous silicon carbide passivating layers to sidestep this issue. The passivation obtained using device-relevant stacks of intrinsic amorphous silicon carbide with various carbon contents and doped amorphous silicon are evaluated, and their stability upon annealing assessed, amorphousmore » silicon carbide being shown to surpass amorphous silicon for temperatures above 300°C. We demonstrate open-circuit voltage values over 700 mV for complete cells, and an improved temperature stability for the open-circuit voltage. Transport of electrons and holes across the hetero-interface is studied with complete cells having amorphous silicon carbide either on the hole-extracting side or on the electron-extracting side, and a better transport of holes than of electrons is shown. Also, due to slightly improved transparency, complete solar cells using an amorphous silicon carbide passivation layer on the hole-collecting side are demonstrated to show slightly better performances even prior to annealing than obtained with a standard amorphous silicon layer.« less

  11. Amorphous silicon carbide passivating layers for crystalline-silicon-based heterojunction solar cells

    DOE PAGES

    Boccard, Mathieu; Holman, Zachary C.

    2015-08-14

    With this study, amorphous silicon enables the fabrication of very high-efficiency crystalline-silicon-based solar cells due to its combination of excellent passivation of the crystalline silicon surface and permeability to electrical charges. Yet, amongst other limitations, the passivation it provides degrades upon high-temperature processes, limiting possible post-deposition fabrication possibilities (e.g., forcing the use of low-temperature silver pastes). We investigate the potential use of intrinsic amorphous silicon carbide passivating layers to sidestep this issue. The passivation obtained using device-relevant stacks of intrinsic amorphous silicon carbide with various carbon contents and doped amorphous silicon are evaluated, and their stability upon annealing assessed, amorphousmore » silicon carbide being shown to surpass amorphous silicon for temperatures above 300°C. We demonstrate open-circuit voltage values over 700 mV for complete cells, and an improved temperature stability for the open-circuit voltage. Transport of electrons and holes across the hetero-interface is studied with complete cells having amorphous silicon carbide either on the hole-extracting side or on the electron-extracting side, and a better transport of holes than of electrons is shown. Also, due to slightly improved transparency, complete solar cells using an amorphous silicon carbide passivation layer on the hole-collecting side are demonstrated to show slightly better performances even prior to annealing than obtained with a standard amorphous silicon layer.« less

  12. Method of producing buried porous silicon-geramanium layers in monocrystalline silicon lattices

    NASA Technical Reports Server (NTRS)

    Fathauer, Robert W. (Inventor); George, Thomas (Inventor); Jones, Eric W. (Inventor)

    1997-01-01

    Lattices of alternating layers of monocrystalline silicon and porous silicon-germanium have been produced. These single crystal lattices have been fabricated by epitaxial growth of Si and Si--Ge layers followed by patterning into mesa structures. The mesa structures are stain etched resulting in porosification of the Si--Ge layers with a minor amount of porosification of the monocrystalline Si layers. Thicker Si--Ge layers produced in a similar manner emitted visible light at room temperature.

  13. Cr incorporated phase transformation in Y 2O 3 under ion irradiation

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

    Li, Nan; Yadav, Satyesh Kumar; Xu, Yun

    Under irradiation, chemical species can redistribute in ways not expected from equilibrium behavior. In oxide-dispersed ferritic alloys, the phenomenon of irradiation-induced Cr redistribution at the metal/oxide interfaces has drawn recent attention. Here, the thermal and irradiation stability of the FeCr/Y 2O 3 interface has been systematically studied. Trilayer thin films of 90 nm Fe - 20 at.% Cr (1 st layer)/100 nm Y 2O 3 (2 nd layer)/135 nm Fe - 20 at.% Cr (3 rd layer) were deposited on MgO substrates at 500 °C. After irradiation, Cr diffuses towards and enriches the FeCr/Y 2O 3 interface. Further, correlated withmore » Cr redistributed into the oxide, an amorphous layer is generated at the interface. In the Y 2O 3 layer, the original cubic phase is observed to transform to the monoclinic phase after irradiation. Meanwhile, nanosized voids, with relatively larger size at interfaces, are also observed in the oxide layer. First-principles calculations reveal that Cr substitution of Y interstitials in Y 2O 3 containing excess Y interstitials is favored and the irradiation-induced monoclinic phase enhances this process. Lastly, our findings provide new insights that may aid in the development of irradiation resistant oxide-dispersed ferritic alloys.« less

  14. Cr incorporated phase transformation in Y2O3 under ion irradiation

    PubMed Central

    Li, N.; Yadav, S. K.; Xu, Y.; Aguiar, J. A.; Baldwin, J. K.; Wang, Y. Q.; Luo, H. M.; Misra, A.; Uberuaga, B. P.

    2017-01-01

    Under irradiation, chemical species can redistribute in ways not expected from equilibrium behavior. In oxide-dispersed ferritic alloys, the phenomenon of irradiation-induced Cr redistribution at the metal/oxide interfaces has drawn recent attention. Here, the thermal and irradiation stability of the FeCr/Y2O3 interface has been systematically studied. Trilayer thin films of 90 nm Fe - 20 at.% Cr (1st layer)/100 nm Y2O3 (2nd layer)/135 nm Fe - 20 at.% Cr (3rd layer) were deposited on MgO substrates at 500 °C. After irradiation, Cr diffuses towards and enriches the FeCr/Y2O3 interface. Further, correlated with Cr redistributed into the oxide, an amorphous layer is generated at the interface. In the Y2O3 layer, the original cubic phase is observed to transform to the monoclinic phase after irradiation. Meanwhile, nanosized voids, with relatively larger size at interfaces, are also observed in the oxide layer. First-principles calculations reveal that Cr substitution of Y interstitials in Y2O3 containing excess Y interstitials is favored and the irradiation-induced monoclinic phase enhances this process. Our findings provide new insights that may aid in the development of irradiation resistant oxide-dispersed ferritic alloys. PMID:28091522

  15. Cr incorporated phase transformation in Y 2O 3 under ion irradiation

    DOE PAGES

    Li, Nan; Yadav, Satyesh Kumar; Xu, Yun; ...

    2017-01-16

    Under irradiation, chemical species can redistribute in ways not expected from equilibrium behavior. In oxide-dispersed ferritic alloys, the phenomenon of irradiation-induced Cr redistribution at the metal/oxide interfaces has drawn recent attention. Here, the thermal and irradiation stability of the FeCr/Y 2O 3 interface has been systematically studied. Trilayer thin films of 90 nm Fe - 20 at.% Cr (1 st layer)/100 nm Y 2O 3 (2 nd layer)/135 nm Fe - 20 at.% Cr (3 rd layer) were deposited on MgO substrates at 500 °C. After irradiation, Cr diffuses towards and enriches the FeCr/Y 2O 3 interface. Further, correlated withmore » Cr redistributed into the oxide, an amorphous layer is generated at the interface. In the Y 2O 3 layer, the original cubic phase is observed to transform to the monoclinic phase after irradiation. Meanwhile, nanosized voids, with relatively larger size at interfaces, are also observed in the oxide layer. First-principles calculations reveal that Cr substitution of Y interstitials in Y 2O 3 containing excess Y interstitials is favored and the irradiation-induced monoclinic phase enhances this process. Lastly, our findings provide new insights that may aid in the development of irradiation resistant oxide-dispersed ferritic alloys.« less

  16. At last! The single-crystal X-ray structure of a naturally occurring sample of the ilmenite-type oxide FeCrO3.

    PubMed

    Pérez-Cruz, María Ana; Elizalde-González, María de la Paz; Escudero, Roberto; Bernès, Sylvain; Silva-González, Rutilo; Reyes-Ortega, Yasmi

    2015-10-01

    A natural single crystal of the ferrimagnetic oxide FeCrO3, which was found in an opencast mine situated in the San Luis Potosí State in Mexico, has been characterized in order to elucidate some outstanding issues about the actual structure of this material. The single-crystal X-ray analysis unambiguously shows that transition metal cations are segregated in alternating layers normal to the threefold crystallographic axis, affording a structure isomorphous to that of ilmenite (FeTiO3), in the space group R3̅. The possible occurrence of cation antisite and vacancy defects is below the limit of detection available from X-ray data. Structural and magnetic results are in agreement with the coherent slow intergrowth of magnetic phases provided by the two antiferromagnetic corundum-type parent oxides Fe2O3 (hematite) and Cr2O3 (eskolaite). Our results are consistent with the most recent density functional theory (DFT) studies carried out on digital FeCrO3 [Sadat Nabi & Pentcheva (2011). Phys. Rev. B, 83, 214424], and suggest that synthetic samples of FeCrO3 might present a cation distribution different to that of the ilmenite structural type.

  17. Radiation tolerance of neutron-irradiated model Fe-Cr-Al alloys

    DOE PAGES

    Field, Kevin G.; Hu, Xunxiang; Littrell, Kenneth C.; ...

    2015-07-14

    The Fe Cr Al alloy system has the potential to form an important class of enhanced accident-tolerant cladding materials in the nuclear power industry owing to the alloy system's higher oxidation resistance in high-temperature steam environments compared with traditional zirconium-based alloys. However, radiation tolerance of Fe Cr Al alloys has not been fully established. In this study, a series of Fe Cr Al alloys with 10 18 wt % Cr and 2.9 4.9 wt % Al were neutron irradiated at 382 C to 1.8 dpa to investigate the irradiation-induced microstructural and mechanical property evolution as a function of alloy composition.more » Dislocation loops with Burgers vector of a/2 111 and a 100 were detected and quantified. Results indicate precipitation of Cr-rich is primarily dependent on the bulk chromium composition. Mechanical testing of sub-size-irradiated tensile specimens indicates the hardening response seen after irradiation is dependent on the bulk chromium composition. Furthermore, a structure property relationship was developed; it indicated that the change in yield strength after irradiation is caused by the formation of these radiation-induced defects and is dominated by the large number density of Cr-rich α' precipitates at sufficiently high chromium contents after irradiation.« less

  18. An ab initio study on the structural, electronic and mechanical properties of quaternary full-Heusler alloys FeMnCrSn and FeMnCrSb

    NASA Astrophysics Data System (ADS)

    Erkişi, Aytaç

    2018-06-01

    The quaternary full Heusler alloys FeMnCrSn and FeMnCrSb, which have face-centred cubic (FCC) crystal structure and conform to ? space group with 216 space number, have been investigated using Generalised Gradient Approximation (GGA) in the Density Functional Theory (DFT) as implemented in VASP (Vienna Ab initio Simulation Package) software. These alloys are considered in ferromagnetic (FM) order. After the investigation of structural stability of these alloys, their mechanical and thermal properties and also electronic band structures have been examined. The calculated spin-polarised electronic band structures and total electronic density of states (DOS) within GGA approximation show that these alloys can exhibit both metallic and half-metallic characters in different structural phases. The calculated formation enthalpies and the plotted energy-volume graphs show that Type-III phase is most stable structural phase for these materials. Also, FeMnCrSb alloy in Type-I/Type-III phases and FeMnCrSn alloy in Type-III phase show half-metallic behaviour with integer total magnetic moments almost 2 and 1 μB per formula unit, respectively, since there are band gaps observed in spin-down states, whereas they have metallic behaviour in majority bands. Other structural phases of both systems are also metallic. Moreover, the calculated elastic constants and the estimated anisotropy shear factors indicate that these materials are stable mechanically in all of three phases except FeMnCrSn in Type-I phase that does not satisfy Born stability criteria in this phase and have high anisotropic behaviour.

  19. Interaction of Fe-Al-Cr-C with the melt of an alkali metal carbonate

    NASA Astrophysics Data System (ADS)

    Nikitina, E. V.

    2015-08-01

    The interaction of an Fe-Al-Cr-C (29.5 wt % Fe, 29.35 wt % Cr, 2.56 wt % C, 38.59 wt % Al) alloy with the melt of a lithium, sodium, or potassium carbonate containing 1-5 wt % addition to a salt phase is studied by gravimetry and measuring the corrosion potential and anode polarization curves in the temperature range 500-600°C. As passivators, the substances that decrease the corrosion losses due to hardening and thickening of an oxide film (lithium, sodium, potassium hydroxides) are used. As corrosion stimulators (activators), sodium chloride, fluoride, and sulfate are used. The coalloying of iron with chromium and aluminum results in high corrosion resistance against both frontal (continuous) and local (pitting, intercrystalline) corrosion as a result of formation of chemically resistant and high-adhesion oxide layers with their participation. X-ray diffraction analysis reveals gamma aluminum oxide, spinel (alumochromite) traces, and lithium aluminate at the surface.

  20. Transmission Electron Microscopy (TEM) Study of the Oxide Layers Formed on Fe-12Cr-4Al Ferritic Alloy in an Oxygenated Pb-Bi Environment at 800°C

    NASA Astrophysics Data System (ADS)

    Popovic, M. P.; Yang, Y.; Bolind, A. M.; Ozdol, V. B.; Olmsted, D. L.; Asta, M.; Hosemann, P.

    2018-06-01

    Liquid lead-bismuth eutectic (LBE) can serve as a heat transfer fluid for advanced nuclear applications as well as concentrated solar power but poses corrosion challenges for the structural materials at elevated temperatures. Oxide passivation of the surfaces of these materials during exposure to liquid LBE can inhibit such material degradation. In this study, transmission electron microscopy of oxides formed on Fe-Cr-Al alloy during exposure to low-oxygenated LBE at 800°C has been performed. A complex structure of the oxide film has been revealed, consisting of a homogeneous inner layer of mostly Al2O3 and a heterogeneous outer layer.

  1. Developments of the Physical and Electrical Properties of NiCr and NiCrSi Single-Layer and Bi-Layer Nano-Scale Thin-Film Resistors.

    PubMed

    Cheng, Huan-Yi; Chen, Ying-Chung; Li, Chi-Lun; Li, Pei-Jou; Houng, Mau-Phon; Yang, Cheng-Fu

    2016-02-25

    In this study, commercial-grade NiCr (80 wt % Ni, 20 wt % Cr) and NiCrSi (55 wt % Ni, 40 wt % Cr, 5 wt % Si) were used as targets and the sputtering method was used to deposit NiCr and NiCrSi thin films on Al₂O₃ and Si substrates at room temperature under different deposition time. X-ray diffraction patterns showed that the NiCr and NiCrSi thin films were amorphous phase, and the field-effect scanning electronic microscope observations showed that only nano-crystalline grains were revealed on the surfaces of the NiCr and NiCrSi thin films. The log (resistivity) values of the NiCr and NiCrSi thin-film resistors decreased approximately linearly as their thicknesses increased. We found that the value of temperature coefficient of resistance (TCR value) of the NiCr thin-film resistors was positive and that of the NiCrSi thin-film resistors was negative. To investigate these thin-film resistors with a low TCR value, we designed a novel bi-layer structure to fabricate the thin-film resistors via two different stacking methods. The bi-layer structures were created by depositing NiCr for 10 min as the upper (or lower) layer and depositing NiCrSi for 10, 30, or 60 min as the lower (or upper) layer. We aim to show that the stacking method had no apparent effect on the resistivity of the NiCr-NiCrSi bi-layer thin-film resistors but had large effect on the TCR value.

  2. Phase stability and magnetic behavior of FeCrCoNiGe high-entropy alloy

    NASA Astrophysics Data System (ADS)

    Huang, Shuo; Vida, Ádám; Molnár, Dávid; Kádas, Krisztina; Varga, Lajos Károly; Holmström, Erik; Vitos, Levente

    2015-12-01

    We report an alternative FeCrCoNiGe magnetic material based on FeCrCoNi high-entropy alloy with Curie point far below the room temperature. Investigations are done using first-principles calculations and key experimental measurements. Results show that the equimolar FeCrCoNiGe system is decomposed into a mixture of face-centered cubic and body-centered cubic solid solution phases. The increased stability of the ferromagnetic order in the as-cast FeCrCoNiGe composite, with measured Curie temperature of 640 K, is explained using the exchange interactions.

  3. Zoned Cr, Fe-spinel from the La Perouse layered gabbro, Fairweather Range, Alaska

    USGS Publications Warehouse

    Czamanske, G.K.; Himmelberg, G.R.; Goff, F.E.

    1976-01-01

    Zoned spinel of unusual composition and morphology has been found in massive pyrrhotite-chalcopyrite-pent-landite ore from the La Perouse layered gabbro intrusion in the Fairweather Range, southeastern Alaska. The spinel grains show continuous zoning from cores with up to 53 wt.% Cr2O3 to rims with less than 11 wt.% Cr2O3. Their composition is exceptional because they contain less than 0.32 wt.% MgO and less than 0.10 wt.% Al2O3 and TiO2. Also notable are the concentrations of MnO and V2O3, which reach 4.73 and 4.50 wt.%, respectively, in the cores. The spinel is thought to have crystallized at low oxygen fugacity and at temperatures above 900??C, directly from a sulfide melt that separated by immiscibility from the gabbroic parental magma. ?? 1976.

  4. Ion irradiation testing and characterization of FeCrAl candidate alloys

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

    Anderoglu, Osman; Aydogan, Eda; Maloy, Stuart Andrew

    2014-10-29

    The Fuel Cycle Research and Development program’s Advanced Fuels Campaign has initiated a multifold effort aimed at facilitating development of accident tolerant fuels. This effort involves development of fuel cladding materials that will be resistant to oxidizing environments for extended period of time such as loss of coolant accident. Ferritic FeCrAl alloys are among the promising candidates due to formation of a stable Al₂O₃ oxide scale. In addition to being oxidation resistant, these promising alloys need to be radiation tolerant under LWR conditions (maximum dose of 10-15 dpa at 250 – 350°C). Thus, in addition to a number of commerciallymore » available alloys, nuclear grade FeCrAl alloys developed at ORNL were tested using high energy proton irradiations and subsequent characterization of irradiation hardening and damage microstructure. This report summarizes ion irradiation testing and characterization of three nuclear grade FeCrAl cladding materials developed at ORNL and four commercially available Kanthal series FeCrAl alloys in FY14 toward satisfying FCRD campaign goals.« less

  5. A study of deformation and strain induced in bulk by the oxide layers formation on a Fe-Cr-Al alloy in high-temperature liquid Pb-Bi eutectic

    DOE PAGES

    Popovic, M. P.; Chen, K.; Shen, H.; ...

    2018-03-29

    At elevated temperatures, heavy liquid metals and their alloys are known to create a highly corrosive environment that causes irreversible degradation of most iron-based materials. In this paper, it has been found that an appropriate concentration of oxygen in the liquid alloy can significantly reduce this issue by creating a passivating oxide scale that controls diffusion, especially if Al is present in Fe-based materials (by Al-oxide formation). However, the increase of the temperature and of oxygen content in liquid phase leads to the increase of oxygen diffusion into bulk, and to promotion of the internal Al oxidation. This can causemore » a strain in bulk near the oxide layer, due either to mismatch between the thermal expansion coefficients of the oxides and bulk material, or to misfit of the crystal lattices (bulk vs. oxides). This work investigates the strain induced into proximal bulk of a Fe-Cr-Al alloy by oxide layers formation in liquid lead-bismuth eutectic utilizing synchrotron X-ray Laue microdiffraction. Finally, it is found that internal oxidation is the most likely cause for the strain in the metal rather than thermal expansion mismatch as a two-layer problem.« less

  6. A study of deformation and strain induced in bulk by the oxide layers formation on a Fe-Cr-Al alloy in high-temperature liquid Pb-Bi eutectic

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

    Popovic, M. P.; Chen, K.; Shen, H.

    At elevated temperatures, heavy liquid metals and their alloys are known to create a highly corrosive environment that causes irreversible degradation of most iron-based materials. In this paper, it has been found that an appropriate concentration of oxygen in the liquid alloy can significantly reduce this issue by creating a passivating oxide scale that controls diffusion, especially if Al is present in Fe-based materials (by Al-oxide formation). However, the increase of the temperature and of oxygen content in liquid phase leads to the increase of oxygen diffusion into bulk, and to promotion of the internal Al oxidation. This can causemore » a strain in bulk near the oxide layer, due either to mismatch between the thermal expansion coefficients of the oxides and bulk material, or to misfit of the crystal lattices (bulk vs. oxides). This work investigates the strain induced into proximal bulk of a Fe-Cr-Al alloy by oxide layers formation in liquid lead-bismuth eutectic utilizing synchrotron X-ray Laue microdiffraction. Finally, it is found that internal oxidation is the most likely cause for the strain in the metal rather than thermal expansion mismatch as a two-layer problem.« less

  7. Microstructure characterization and strengthening mechanisms of oxide dispersion strengthened (ODS) Fe-9%Cr and Fe-14%Cr extruded bars

    NASA Astrophysics Data System (ADS)

    Chauhan, A.; Bergner, F.; Etienne, A.; Aktaa, J.; de Carlan, Y.; Heintze, C.; Litvinov, D.; Hernandez-Mayoral, M.; Oñorbe, E.; Radiguet, B.; Ulbricht, A.

    2017-11-01

    The collaborative study is focused on the relationship between microstructure and yield stress for an ODS Fe-9%Cr-based transformable alloy and an ODS Fe-14%Cr-based ferritic alloy. The contributions to the total room temperature yield stress arising from various strengthening mechanisms are addressed on the basis of a comprehensive description of the microstructures uncovered by means of transmission electron microscopy (TEM), electron backscatter diffraction (EBSD), small-angle neutron scattering (SANS) and atom probe tomography (APT). While these methods provide a high degree of complementarity, a reasonable agreement was found in cases of overlap of information. The derived set of microstructure parameters along with reported strengthening equations was used to calculate the room temperature yield stress. The estimates were critically compared with the measured yield stress for an extended set of alloys including data reported for Fe-Cr model alloys and steels thus covering one order of magnitude or more in grain size, dislocation density, particle density and yield stress. The comparison shows that particle strengthening, dislocation forest strengthening, and Hall-Petch strengthening are the major contributions and that a mixed superposition rule reproduces the measured yield stress within experimental scatter for the whole extended set of alloys. The wide variation of microstructures additionally underpins the conclusions and goes beyond previous work, in which one or few ODS steels and narrow microstructure variations were typically covered.

  8. Low temperature electrodeposition of silicon layers

    NASA Astrophysics Data System (ADS)

    Pauporté, Thierry; Qi, Shuo; Viana, Bruno

    2018-02-01

    The electrodeposition of silicon at room temperature in 1-Butyl-1-methylpyrrolidinium bis(trifluoromethanesulfonyl)imide and N-Propyl-N-methylpyrrolidinium bis(trifluoromethanesulfonyl)imide ionic liquids containing SiCl4 salt is shown. The electrodeposition window has been determined by cyclic voltammetry. Layers have been deposited in a three electrode cell placed in an inert atmosphere and at constant applied potential. The characterizations by x-ray diffraction and Raman spectroscopy showed the formation of a layer made of amorphous silicon. The scanning electron microscopy examination revealed that the layers were featureless and well-covering.

  9. Magnetic cluster expansion simulation and experimental study of high temperature magnetic properties of Fe-Cr alloys.

    PubMed

    Lavrentiev, M Yu; Mergia, K; Gjoka, M; Nguyen-Manh, D; Apostolopoulos, G; Dudarev, S L

    2012-08-15

    We present a combined experimental and computational study of high temperature magnetic properties of Fe-Cr alloys with chromium content up to about 20 at.%. The magnetic cluster expansion method is applied to model the magnetic properties of random Fe-Cr alloys, and in particular the Curie transition temperature, as a function of alloy composition. We find that at low (3-6 at.%) Cr content the Curie temperature increases with the increase of Cr concentration. It is maximum at approximately 6 at.% Cr and then decreases for higher Cr content. The same feature is found in thermo-magnetic measurements performed on model Fe-Cr alloys, where a 5 at.% Cr alloy has a higher Curie temperature than pure Fe. The Curie temperatures of 10 and 15 at.% Cr alloys are found to be lower than the Curie temperature of pure Fe.

  10. Observation of magnetization and exchange bias reversals in NdFe0.5Cr0.5O3

    NASA Astrophysics Data System (ADS)

    Sharannia, M. P.; De, Santanu; Singh, Ripandeep; Das, A.; Nirmala, R.; Santhosh, P. N.

    2017-05-01

    Polycrystalline NdFe0.5Cr0.5O3 has orthorhombic structure with Pnma space group and is magnetically ordered at room temperature as confirmed by neutron diffraction. The magnetic structure involves CxGyFz type ordering of Fe3+/Cr3+ ions. NdFe0.5Cr0.5O3 shows magnetization reversal and sign reversal of exchange bias at 16 K. Nd3+ moments that get induced by the internal field of |Fe+Cr| sublattice couple antiferromagnetically with the ferromagnetic component of |Fe+Cr| sublattice. Nd3+ moments overcome the |Fe+Cr| moments at 16 K below which the material shows negative magnetization and positive exchange bias.

  11. Developments of the Physical and Electrical Properties of NiCr and NiCrSi Single-Layer and Bi-Layer Nano-Scale Thin-Film Resistors

    PubMed Central

    Cheng, Huan-Yi; Chen, Ying-Chung; Li, Chi-Lun; Li, Pei-Jou; Houng, Mau-Phon; Yang, Cheng-Fu

    2016-01-01

    In this study, commercial-grade NiCr (80 wt % Ni, 20 wt % Cr) and NiCrSi (55 wt % Ni, 40 wt % Cr, 5 wt % Si) were used as targets and the sputtering method was used to deposit NiCr and NiCrSi thin films on Al2O3 and Si substrates at room temperature under different deposition time. X-ray diffraction patterns showed that the NiCr and NiCrSi thin films were amorphous phase, and the field-effect scanning electronic microscope observations showed that only nano-crystalline grains were revealed on the surfaces of the NiCr and NiCrSi thin films. The log (resistivity) values of the NiCr and NiCrSi thin-film resistors decreased approximately linearly as their thicknesses increased. We found that the value of temperature coefficient of resistance (TCR value) of the NiCr thin-film resistors was positive and that of the NiCrSi thin-film resistors was negative. To investigate these thin-film resistors with a low TCR value, we designed a novel bi-layer structure to fabricate the thin-film resistors via two different stacking methods. The bi-layer structures were created by depositing NiCr for 10 min as the upper (or lower) layer and depositing NiCrSi for 10, 30, or 60 min as the lower (or upper) layer. We aim to show that the stacking method had no apparent effect on the resistivity of the NiCr-NiCrSi bi-layer thin-film resistors but had large effect on the TCR value. PMID:28344296

  12. Magnetic susceptibilities of liquid Cr-Au, Mn-Au and Fe-Au alloys

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

    Ohno, S.; Shimakura, H.; Tahara, S.

    The magnetic susceptibility of liquid Cr-Au, Mn-Au, Fe-Au and Cu-Au alloys was investigated as a function of temperature and composition. Liquid Cr{sub 1-c}Au{sub c} with 0.5 ≤ c and Mn{sub 1-c}Au{sub c} with 0.3≤c obeyed the Curie-Weiss law with regard to their dependence of χ on temperature. The magnetic susceptibilities of liquid Fe-Au alloys also exhibited Curie-Weiss behavior with a reasonable value for the effective number of Bohr magneton. On the Au-rich side, the composition dependence of χ for liquid TM-Au (TM=Cr, Mn, Fe) alloys increased rapidly with increasing TM content, respectively. Additionally, the composition dependences of χ for liquidmore » Cr-Au, Mn-Au, and Fe-Au alloys had maxima at compositions of 50 at% Cr, 70 at% Mn, and 85 at% Fe, respectively. We compared the composition dependences of χ{sub 3d} due to 3d electrons for liquid binary TM-M (M=Au, Al, Si, Sb), and investigated the relationship between χ{sub 3d} and E{sub F} in liquid binary TM-M alloys at a composition of 50 at% TM.« less

  13. NiFeCo/Cu superlattices with high magnetoresistive sensitivity and weak hysteresis

    NASA Astrophysics Data System (ADS)

    Bannikova, N. S.; Milyaev, M. A.; Naumova, L. I.; Krinitsina, T. P.; Patrakov, E. I.; Proglyado, V. V.; Chernyshova, T. A.; Ustinov, V. V.

    2016-10-01

    The microstructure and the magetoresistive characteristics of [NiFeCo/Cu]8 superlattices prepared by magnetron sputtering with various thickness of the buffer NiFeCr layer and exhibiting a giant magnetoresistive effect have been studied. It has been found that these nanostructures are formed with a strong or weak hysteresis depending on the structure (bcc or fcc) formed in the NiFeCr buffer layer. The method of the substantial decrease in the hysteresis loop width of the magnetoresistance by using the composite Ta/NiFeCr buffer layer has been suggested.

  14. Fe3O4–Silicone Mixture as Flexible Actuator

    PubMed Central

    Song, Kahye

    2018-01-01

    In this study, we introduce Fe3O4-silicone flexible composite actuators fabricated by combining silicone and iron oxide particles. The actuators exploit the flexibility of silicone and the electric conductivity of iron oxide particles. These actuators are activated by electrostatic force using the properties of the metal particles. Herein, we investigate the characteristic changes in actuation performance by increasing the concentration of iron oxide from 1% to 20%. The developed flexible actuators exhibit a resonant frequency near 3 Hz and their actuation amplitudes increase with increasing input voltage. We found that the actuator can move well at metal particle concentrations >2.5%. We also studied the changes in actuation behavior, depending on the portion of the Fe3O4-silicone in the length. Overall, we experimentally analyzed the characteristics of the newly proposed metal particle-silicone composite actuators. PMID:29738466

  15. Antifuse with a single silicon-rich silicon nitride insulating layer

    DOEpatents

    Habermehl, Scott D.; Apodaca, Roger T.

    2013-01-22

    An antifuse is disclosed which has an electrically-insulating region sandwiched between two electrodes. The electrically-insulating region has a single layer of a non-hydrogenated silicon-rich (i.e. non-stoichiometric) silicon nitride SiN.sub.X with a nitrogen content X which is generally in the range of 0layer. The SiN.sub.X layer thickness can also be made sufficiently large so that Poole-Frenkel emission will be the primary electrical conduction mechanism in the antifuse. Different types of electrodes are disclosed including electrodes formed of titanium silicide, aluminum and silicon. Arrays of antifuses can also be formed.

  16. Electrochemical and surface analysis of the Fe-Cr-Ru system in non-oxidizing acid solutions

    NASA Astrophysics Data System (ADS)

    Tjong, S. C.

    1990-03-01

    The effect of ruthenium addition on the spontaneous passivation behaviour of Fe-40Cr alloy in 0.5M H 2SO 4 and 0.5M HCl acid solutions has been studied. Auger and XPS techniques were also used to investigate the surface chemistries of the spontaneously passivated film. Electrochemical measurements indicate that the Fe-40Cr-0.1Ru and Fe-40Cr-0.2Ru alloys exhibit spontaneous passivation upon exposing them in both hydrochloric and sulphuric acid solutions from 25 to 85 ° C. However, the transition time for spontaneous passivation reduces dramatically with an increase in the ruthenium content and solution temperature. Furthermore, this transition time also decreases for the investigated alloys exposed in a less aggressive sulphuric acid solution. AES results show that ruthenium and chromium are enriched in the spontaneous passive films formed on the Fe-40Cr-0.1Ru alloy in both hydrochloric and sulphuric acid solutions at 25 °C, and also in the spontaneous passive film formed on the Fe-40Cr-0.2Ru alloy in hydrochloric acid solution at 25 ° C. AES does not detect the presence of ruthenium in the spontaneous passive film formed on the Fe-40Cr-0.2Ru alloy in sulphuric acid solution. However, XPS analysis shows that ruthenium and chromium are incorporated into the spontaneous passive films formed on the Fe-40Cr-0.1Ru and Fe-40Cr-0.2Ru alloys in both hydrochloric and sulphuric acid solutions as Ru 4+ and Cr 3+ species.

  17. Specific features of the atomic structure of metallic layers of multilayered (CoFeZr/SiO2)32 and (CoFeZr/ a-Si)40 nanostructures with different interlayers

    NASA Astrophysics Data System (ADS)

    Domashevskaya, E. P.; Guda, A. A.; Chernyshev, A. V.; Sitnikov, V. G.

    2017-02-01

    Multilayered nanostructures (MN) were prepared by ion-beam successive sputtering from two targets, one of which was a metallic Co45Fe45Zr10 alloy plate and another target was a quartz (SiO2) or silicon plate on the surface of a rotating glass-ceramic substrate in an argon atmosphere. The Co and Fe K edges X-ray absorption fine structure of XANES in the (CoFeZr/SiO2)32 sample with oxide interlayers was similar to XANES of metallic Fe foil. This indicated the existence in metallic layers of multilayered CoFeZr nanocrystals with a local environment similar to the atomic environment in solid solutions on the base of bcc Fe structure, which is also confirmed by XRD data. XANES near the Co and Fe K edges absorption in another multilayered nanostructure with silicon interlayers (CoFeZr/ a-Si)40 differs from XANES of MN with dielectric SiO2 interlayer, which demonstrates a dominant influence of the Fe-Si and Co-Si bonds in the local environment of 3 d Co and Fe metals when they form CoFeSi-type silicide phases in thinner bilayers of this MN.

  18. Nanoindentation of Electropolished FeCrAl Alloy Welds

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

    Weaver, Jordan; Aydogan, Eda; Mara, Nathan Allan

    The present report summarizes Berkovich nanoindentation modulus and hardness measurements on two candidate FeCrAl alloys (C35M and C37M) on as-received (AR) and welded samples. In addition, spherical nanoindentation stress-strain measurements were performed on individual grains to provide further information and demonstrate the applicability of these protocols to mechanically characterizing welds in FeCrAl alloys. The indentation results are compared against the reported tensile properties for these alloys to provide relationships between nanoindentation and tensile tests and insight into weldsoftening for these FeCrAl alloys. Hardness measurements revealed weld-softening for both alloys in good agreement with tensile test results. C35M showed a largermore » reduction in hardness at the weld center from the AR material compared to C37M; this is also consistent with tensile tests. In general, nanohardness was shown to be a good predictor of tensile yield strength and ultimate tensile stress for FeCrAl alloys. Spherical nanoindentation measurements revealed that the fusion zone (FZ) + heat affected zone (HAZ) has a very low defect density typical of well-annealed metals as indicated by the frequent pop-in events. Spherical nanoindentation yield strength, Berkovich hardness, and tensile yield strength measurements on the welded material all show that the C37M welded material has a higher strength than C35M welded material. From the comparison of nanoindentation and tensile tests, EBSD microstructure analysis, and information on the processing history, it can be deduced that the primary driver for weld-softening is a change in the defect structure at the grain-scale between the AR and welded material. These measurements serve as baseline data for utilizing nanoindentation for studying the effects of radiation damage on these alloys.« less

  19. Degradation of the Giant Magnetoresistance in Fe/Cr Multilayers Due to Ar-Ion Beam Mixing

    NASA Astrophysics Data System (ADS)

    Kopcewicz, M.; Stobiecki, F.; Jagielski, J.; Szymański, B.; Schmidt, M.; Kalinowska, J.

    2002-12-01

    The influence of 200 keV Ar-ion irradiation on the interlayer coupling in the Fe/Cr multilayer system exhibiting the giant magnetoresistance effect (GMR) is studied by conversion electron Mössbauer spectroscopy (CEMS), VSM hysteresis loops, magnetoresistivity and electric resistivity measurements and supplemented by the small-angle X-ray diffraction (SAXRD). The increase of Ar ion dose causes an increase of interface roughness, as evidenced by the increase of the Fe step-sites detected by CEMS as a result of which the GMR gradually decreases and vanishes at doses exceeding 1×1014 Ar/cm2. A degradation of GMR with increasing Ar-ion dose is related to the formation of pinholes between Fe layers and the decrease of the antiferromagnetically coupled fraction.

  20. Interstitial loop transformations in FeCr

    DOE PAGES

    Béland, Laurent Karim; Osetsky, Yuri N.; Stoller, Roger E.; ...

    2015-03-27

    Here, we improve the Self-Evolving Atomistic Kinetic Monte Carlo (SEAKMC) algorithm by integrating the Activation Relaxation Technique nouveau (ARTn), a powerful open-ended saddle-point search method, into the algorithm. We use it to investigate the reaction of 37-interstitial 1/2[1 1 1] and 1/2[View the MathML source] loops in FeCr at 10 at.% Cr. They transform into 1/2[1 1 1], 1/2[View the MathML source], [1 0 0] and [0 1 0] 74-interstitial clusters with an overall barrier of 0.85 eV. We find that Cr decoration locally inhibits the rotation of crowdions, which dictates the final loop orientation. Moreover, the final loop orientationmore » depends on the details of the Cr decoration. Generally, a region of a given orientation is favored if Cr near its interface with a region of another orientation is able to inhibit reorientation at this interface more than the Cr present at the other interfaces. Also, we find that substitutional Cr atoms can diffuse from energetically unfavorable to energetically favorable sites within the interlocked 37-interstitial loops conformation with barriers of less than 0.35 eV.« less

  1. Photo-EMF sensitivity of porous silicon thin layer-crystalline silicon heterojunction to ammonia adsorption.

    PubMed

    Vashpanov, Yuriy; Jung, Jae Il; Kwack, Kae Dal

    2011-01-01

    A new method of using photo-electromotive force in detecting gas and controlling sensitivity is proposed. Photo-electromotive force on the heterojunction between porous silicon thin layer and crystalline silicon wafer depends on the concentration of ammonia in the measurement chamber. A porous silicon thin layer was formed by electrochemical etching on p-type silicon wafer. A gas and light transparent electrical contact was manufactured to this porous layer. Photo-EMF sensitivity corresponding to ammonia concentration in the range from 10 ppm to 1,000 ppm can be maximized by controlling the intensity of illumination light.

  2. Understanding phase stability of Al-Co-Cr-Fe-Ni high entropy alloys

    DOE PAGES

    Zhang, Chuan; Zhang, Fan; Diao, Haoyan; ...

    2016-07-19

    The concept of high entropy alloy (HEA) opens a vast unexplored composition range for alloy design. As a well-studied system, Al-Co-Cr-Fe-Ni has attracted tremendous amount of attention to develop new-generation low-density structural materials for automobile and aerospace applications. In spite of intensive investigations in the past few years, the phase stability within this HEA system is still poorly understood and needs to be clarified, which poses obstacles to the discovery of promising Al-Co-Cr-Fe-Ni HEAs. In the present work, the CALPHAD approach is employed to understand the phase stability and explore the phase transformation within the Al-Co-Cr-Fe-Ni system. As a result,more » the phase-stability mapping coupled with density contours is then constructed within the composition - temperature space, which provides useful guidelines for the design of low-density Al-Co-Cr-Fe-Ni HEAs with desirable properties.« less

  3. Understanding phase stability of Al-Co-Cr-Fe-Ni high entropy alloys

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

    Zhang, Chuan; Zhang, Fan; Diao, Haoyan

    The concept of high entropy alloy (HEA) opens a vast unexplored composition range for alloy design. As a well-studied system, Al-Co-Cr-Fe-Ni has attracted tremendous amount of attention to develop new-generation low-density structural materials for automobile and aerospace applications. In spite of intensive investigations in the past few years, the phase stability within this HEA system is still poorly understood and needs to be clarified, which poses obstacles to the discovery of promising Al-Co-Cr-Fe-Ni HEAs. In the present work, the CALPHAD approach is employed to understand the phase stability and explore the phase transformation within the Al-Co-Cr-Fe-Ni system. As a result,more » the phase-stability mapping coupled with density contours is then constructed within the composition - temperature space, which provides useful guidelines for the design of low-density Al-Co-Cr-Fe-Ni HEAs with desirable properties.« less

  4. From solid solution to cluster formation of Fe and Cr in α-Zr

    NASA Astrophysics Data System (ADS)

    Burr, P. A.; Wenman, M. R.; Gault, B.; Moody, M. P.; Ivermark, M.; Rushton, M. J. D.; Preuss, M.; Edwards, L.; Grimes, R. W.

    2015-12-01

    To understand the mechanisms by which the re-solution of Fe and Cr additions increase the corrosion rate of irradiated Zr alloys, the solubility and clustering of Fe and Cr in model binary Zr alloys was investigated using a combination of experimental and modelling techniques - atom probe tomography (APT), x-ray diffraction (XRD), thermoelectric power (TEP) and density functional theory (DFT). Cr occupies both interstitial and substitutional sites in the α-Zr lattice; Fe favours interstitial sites, and a low-symmetry site that was not previously modelled is found to be the most favourable for Fe. Lattice expansion as a function of Fe and Cr content in the α-Zr matrix deviates from Vegard's law and is strongly anisotropic for Fe additions, expanding the c-axis while contracting the a-axis. Matrix content of solutes cannot be reliably estimated from lattice parameter measurements, instead a combination of TEP and APT was employed. Defect clusters form at higher solution concentrations, which induce a smaller lattice strain compared to the dilute defects. In the presence of a Zr vacancy, all two-atom clusters are more soluble than individual point defects and as many as four Fe or three Cr atoms could be accommodated in a single Zr vacancy. The Zr vacancy is critical for the increased apparent solubility of defect clusters; the implications for irradiation induced microstructure changes in Zr alloys are discussed.

  5. Optimized Gen-II FeCrAl cladding production in large quantity for campaign testing

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

    Yamamoto, Yukinori; Sun, Zhiqian; Pint, Bruce A.

    2016-06-03

    There are two major objectives in this report; (1) to optimize microstructure control of ATF FeCrAl alloys during tube drawing processes, and (2) to provide an update on the progress of ATF FeCrAl tube production via commercial manufacturers. Experimental efforts have been made to optimize the process parameters balancing the tube fabricability, especially for tube drawing processes, and microstructure control of the final tube products. Lab-scale sheet materials of Gen II FeCrAl alloys (Mo-containing and Nb-containing FeCrAl alloys) were used in the study, combined with a stepwise warm-rolling process and intermediate annealing, aiming to simulate the tube drawing process inmore » a commercial tube manufacturer. The intermediate annealing at 650ºC for 1h was suggested for the tube-drawing process of Mo-containing FeCrAl alloys because it successfully softened the material by recovering the work hardening introduced through the rolling step, without inducing grain coarsening due to recrystallization. The final tube product is expected to have stabilized deformed microstructure providing the improved tensile properties with sufficient ductility. Optimization efforts on Nb-containing FeCrAl alloys focused on the effect of alloying additions and annealing conditions on the stability of deformed microstructure. Relationships between the second-phase precipitates (Fe 2Nb-Laves phase) and microstructure stability are discussed. FeCrAl tube production through commercial tube manufacturers is currently in progress. Three different manufacturers, Century Tubes, Inc. (CTI), Rhenium Alloys, Inc. (RAI), and Superior Tube Company, Inc. (STC), are providing capabilities for cold-drawing, warm-drawing, and HPTR cold-pilgering, respectively. The first two companies are currently working on large quantity tube production (expected 250 ft length) of Gen I model FeCrAl alloy (B136Y3, at CTI) and Gen II (C35M4, at RAI), with the process parameters obtained from the experimental

  6. Reduction and Simultaneous Removal of 99 Tc and Cr by Fe(OH) 2 (s) Mineral Transformation

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

    Saslow, Sarah A.; Um, Wooyong; Pearce, Carolyn I.

    Technetium (Tc) remains a priority remediation concern due to persistent challenges, including rapid re-oxidation of immobilized Tc, and competing contaminants, e.g. Cr(VI), that inhibit targeted Tc reduction and incorporation into stable mineral phases. Here Fe(OH) 2(s) is investigated as a comprehensive solution for overcoming these challenges, by serving as both the reductant, (Fe(II)), and immobilization agent to form Tc-incorporated magnetite (Fe 3O 4). Trace metal analysis suggests removal of Tc(VII) and Cr(VI) from solution occurs simultaneously; however, complete removal and reduction of Cr(VI) is achieved earlier than the removal/reduction of co-mingled Tc(VII). Bulk oxidation state analysis of the magnetite solidmore » phase by XANES confirms that the majority of Tc is Tc(IV), which is corroborated by XPS. Furthermore, EXAFS results show successful Tc(IV) incorporation into magnetite octahedral sites without additional substitution of Cr or Tc into neighboring Fe octahedral sites. XPS analysis of Cr confirms reduction to Cr(III) and the formation of a Cr-incorporated spinel, Cr2O 3, and Cr(OH)3 phases. Spinel (modeled as Fe 3O 4), goethite, and feroxyhyte are detected in all reacted solid phase samples analyzed by XRD, where Tc(IV) incorporation has little effect on the spinel lattice structure. In the presence of Cr(III) a spinel phase along the magnetite-chromite (Fe 3O 4-FeCr 2O 4) solid-solution line is formed.« less

  7. Deep Drawing Behavior of CoCrFeMnNi High-Entropy Alloys

    NASA Astrophysics Data System (ADS)

    Bae, Jae Wung; Moon, Jongun; Jang, Min Ji; Ahn, Dong-Hyun; Joo, Soo-Hyun; Jung, Jaimyun; Yim, Dami; Kim, Hyoung Seop

    2017-09-01

    Herein, the deep drawability and deep drawing behavior of an equiatomic CoCrFeMnNi HEA and its microstructure and texture evolution are first studied for future applications. The CoCrFeMnNi HEA is successfully drawn to a limit drawing ratio (LDR) of 2.14, while the planar anisotropy of the drawn cup specimen is negligible. The moderate combination of strain hardening exponent and strain rate sensitivity and the formation of deformation twins in the edge region play important roles in successful deep drawing. In the meanwhile, the texture evolution of CoCrFeMnNi HEA has similarities with conventional fcc metals.

  8. Characterization of a heterobimetallic nonheme Fe(III)-O-Cr(III) species formed by O2 activation.

    PubMed

    Zhou, Ang; Kleespies, Scott T; Van Heuvelen, Katherine M; Que, Lawrence

    2015-10-01

    We report the generation and spectroscopic characterization of a heterobimetallic [(TMC)Fe(III)-O-Cr(III)(OTf)4] species (1) by bubbling O2 into a mixture of Fe(TMC)(OTf)2 and Cr(OTf)2 in NCCH3. Complex 1 also formed quantitatively by adding Cr(OTf)2 to [Fe(IV)(O)(TMC)(NCCH3)](2+). The proposed O2 activation mechanism involves the trapping of a Cr-O2 adduct by Fe(TMC)(OTf)2.

  9. Characterization of a Heterobimetallic Nonheme Fe(III)-O-Cr(III) Species Formed by O2 Activation

    PubMed Central

    Zhou, Ang; Kleespies, Scott T.; Van Heuvelen, Katherine M.; Que, Lawrence

    2015-01-01

    We report the generation and spectroscopic characterization of a heterobimetallic [(TMC)FeIII-O-CrIII(OTf)4] species (1) by O2 bubbling into a mixture of Fe(TMC)(OTf)2 and Cr(OTf)2 in NCCH3. Complex 1 also formed quantitatively by adding Cr(OTf)2 to [FeIV(O)(TMC)(NCCH3)]2+. The proposed O2 activation mechanism involves the trapping by a Cr-O2 adduct by Fe(TMC)(OTf)2. PMID:26265081

  10. In vitro cytotoxicity of Fe-Cr-Nb-B magnetic nanoparticles under high frequency electromagnetic field

    NASA Astrophysics Data System (ADS)

    Chiriac, Horia; Petreus, Tudor; Carasevici, Eugen; Labusca, Luminita; Herea, Dumitru-Daniel; Danceanu, Camelia; Lupu, Nicoleta

    2015-04-01

    The heating potential, cytotoxicity, and efficiency of Fe68.2Cr11.5Nb0.3B20 magnetic nanoparticles (MNPs), as such or coated with a chitosan layer, to decrease the cell viability in a cancer cell culture model by using high frequency alternating magnetic fields (AMF) have been studied. The specific absorption rate varied from 215 W/g for chitosan-free MNPs to about 190 W/g for chitosan-coated ones, and an equilibrium temperature of 46 °C was reached when chitosan-coated MNPs were subjected to AMF. The chitosan-free Fe68.2Cr11.5Nb0.3B20 MNPs proved a good biocompatibility and low cytotoxicity in all testing conditions, while the chitosan-coated ones induced strong tumoricidal effects when a cell-particle simultaneous co-incubation approach was used. In high frequency AMF, the particle-mediated heat treatment has proved to be a critical cause for decreasing in vitro the viability of a cancer cell line.

  11. Magnetism, structures and stabilities of cluster assembled TM@Si nanotubes (TM = Cr, Mn and Fe): a density functional study.

    PubMed

    Dhaka, Kapil; Bandyopadhyay, Debashis

    2016-08-02

    The present study reports transition metal (TM = Cr, Mn and Fe) doped silicon nanotubes with tunable band structures and magnetic properties by careful selection of cluster assemblies as building blocks using the first-principles density functional theory. We found that the transition metal doping and in addition, the hydrogen termination process can stabilize the pure silicon nanoclusters or cluster assemblies and then it could be extended as magnetic nanotubes with finite magnetic moments. Study of the band structures and density of states (DOS) of different empty and TM doped nanotubes (Type 1 to Type 4) show that these nanotubes are useful as metals, semiconductors, semi-metals and half-metals. These designer magnetic materials could be useful in spintronics and magnetic devices of nanoscale order.

  12. Microstructure and abrasive wear properties of Fe-Cr-C hardfacing alloy cladding manufactured by Gas Tungsten Arc Welding (GTAW)

    NASA Astrophysics Data System (ADS)

    Chen, Jie-Hao; Hsieh, Chih-Chun; Hua, Pei-Shing; Chang, Chia-Ming; Lin, Chi-Ming; Wu, Paxon Ti-Yuan; Wu, Weite

    2013-01-01

    A series of Fe-Cr-C hardfacing alloys is deposited by gas tungsten arc welding and subjected to abrasive wear testing. Pure Fe with various amounts of CrC (Cr:C=4:1) powders are mixed as the fillers and used to deposit hardfacing alloys on low carbon steel. Depending on the various CrC additions to the alloy fillers, the claddings mainly contain hypoeutectic, near eutectic, or hypereutectic microstructures of austenite γ-Fe phase and (Cr,Fe)7C3 carbides on hardfacing alloys, respectively. When 30% CrC is added to the filler, the finest microstructure is achieved, which corresponds to the γ-Fe+(Cr,Fe)7C3 eutectic structure. With the addition of 35% and 40% CrC to the fillers, the results show that the cladding consists of the massive primary (Cr,Fe)7C3 as the reinforcing phase and interdendritic γ-Fe+(Cr,Fe)7C3 eutectics as the matrix. The (Cr,Fe)7C3 carbide-reinforced claddings have high hardness and excellent wear resistance under abrasive wear test conditions. Concerning the abrasive wear feature observable on the worn surface, the formation and fraction of massive primary (Cr,Fe)7C3 carbides predominates the wear resistance of hardfacing alloys. Abrasive particles result in continuous plastic grooves when the cladding has primary γ-Fe phase in a hypoeutectic structure.

  13. Thermodynamic analysis of chemical compatibility of several compounds with Fe-Cr-Al alloys

    NASA Technical Reports Server (NTRS)

    Misra, Ajay K.

    1993-01-01

    Chemical compatibility between Fe-19.8Cr-4.8Al (weight percent), which is the base composition for the commercial superalloy MA956, and several carbides, borides, nitrides, oxides, and silicides was analyzed from thermodynamic considerations. The effect of addition of minor alloying elements, such as Ti, Y, and Y2O3, to the Fe-Cr-Al alloy on chemical compatibility between the alloy and various compounds was also analyzed. Several chemically compatible compounds that can be potential reinforcement materials and/or interface coating materials for Fe-Cr-Al based composites were identified.

  14. Structural classification of RAO3( MO) n compounds ( R =Sc, In, Y, or lanthanides; A =Fe(III), Ga, Cr, or Al; M =divalent cation; n = 1-11)

    NASA Astrophysics Data System (ADS)

    Kimizuka, Noboru; Mohri, Takahiko

    1989-01-01

    A series of new compounds RAO3( MO) n ( n = 1-11) having spinel, YbFe 2O 4, or InFeO 3(ZnO) n types of structures were newly synthesized ( R =Sc, In, Y, Lu, Yb, Tm, or Er; A =Fe(III), Ga, Cr, or Al; M =Mg, Mn, Fe(II), Co, Ni, Zn, or Cd) at elevated temperatures. The conditions of synthesis and the lattice constants for these compounds are reported. The stacking sequences of the InO 1.5, (FeZn)O 2.5, and ZnO layers for InFeO 3(ZnO) 10 and the TmO 1.5, (AlZn)O 2.5, and ZnO layers for TmAlO 3(ZnO) 11 are presented, respectively. The crystal structures of the( RAO3) m( MO) n phases ( R =Sc, In, Y, or lanthanide elements; A =Fe(III), Ga, Cr, or Al; M =divalent cation elements; m and n =integer) are classified into four crystal structure types (K 2NiF 4, CaFe 2O 4, YbFe 2O 4, and spinel), based upon the constituent cations R, A, and M

  15. Irradiation of Wrought FeCrAl Tubes in the High Flux Isotope Reactor

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

    Linton, Kory D.; Field, Kevin G.; Petrie, Christian M.

    The Advanced Fuels Campaign within the Nuclear Technology Research and Development program of the Department of Energy Office of Nuclear Energy is seeking to improve the accident tolerance of light water reactors. Alumina-forming ferritic alloys (e.g., FeCrAl) are one of the leading candidate materials for fuel cladding to replace traditional zirconium alloys because of the superior oxidation resistance of FeCrAl. However, there are still some unresolved questions regarding irradiation effects on the microstructure and mechanical properties of FeCrAl at end-of-life dose levels. In particular, there are concerns related to irradiation-induced embrittlement of FeCrAl alloys due to secondary phase formation. Tomore » address this issue, Oak Ridge National Laboratory has developed a new experimental design to irradiate shortened cladding tube specimens with representative 17×17 array pressurized water reactor diameter and thickness in the High Flux Isotope Reactor (HFIR) under relevant temperatures (300–350°C). Post-irradiation examination will include studies of dimensional change, microstructural changes, and mechanical performance. This report briefly summarizes the capsule design concept and the irradiation test matrix for six rabbit capsules. Each rabbit contains two FeCrAl alloy tube specimens. The specimens include Generation I and Generation II FeCrAl alloys with varying processing conditions, Cr concentrations, and minor alloying elements. The rabbits were successfully assembled, welded, evaluated, and delivered to the HFIR along with a complete quality assurance fabrication package. Pictures of the rabbit assembly process and detailed dimensional inspection of select specimens are included in this report. The rabbits were inserted into HFIR starting in cycle 472 (May 2017).« less

  16. Studies on redox H 2-CO 2 cycle on CoCr xFe 2- xO 4

    NASA Astrophysics Data System (ADS)

    Ma, Ling Juan; Chen, Lin Shen; Chen, Song Ying

    2009-01-01

    Completely reduced CoCr xFe 2-xO 4 can be used to decompose CO 2. It was found that for pure CoFe 2O 4 there is no FeO formation in the first step while there is formation in the second step. For CoCr 0.08Fe 2-0.08O 4, there is no FeO formed in all the oxidation process, because of effect of Cr 3+. Pure CoFe 2O 4 was destroyed at the first reaction cycle of H 2 reduction and CO 2 oxidation, while doped Cr 3+ spinel CoCr 0.08Fe 1.92O 4 showed good stability. The results from H 2-TG, CO 2-TG and XRD show that the addition of Cr 3+ to CoFe 2O 4 can inhibit the increasing of crystallite size and the sintering of alloy. Most importantly, the CoCr 0.08Fe 1.92O 4 can be used to decompose CO 2 repeatedly, implying that it is a potential catalyst for dealing with the CO 2 as a 'green house effect' gas.

  17. SOI-silicon as structural layer for NEMS applications

    NASA Astrophysics Data System (ADS)

    Villarroya, Maria; Figueras, Eduard; Perez-Murano, Francesc; Campabadal, Francesca; Esteve, Jaume; Barniol, Nuria

    2003-04-01

    The objective of this paper is to present the compatibilization between a standard CMOS on bulk silicon process and the fabrication of nanoelectromechanical systems using Silicon On Insulator (SOI) wafers as substrate. This compatibilization is required as first step to fabricate a very high sensitive mass sensor based on a resonant cantilever with nanometer dimensions using the crystal silicon COI layer as the structural layer. The cantilever is driven electrostatically to its resonance frequency by an electrode placed parallel to the cantilever. A capacitive readout is performed. To achieve very high resolution, very small dimensions of the cantilever (nanometer range) are needed. For this reason, the control and excitation circuitry has to be integrated on the same substrate than the cantilever. Prior to the development of this sensor, it is necessary to develop a substrate able to be used first to integrate a standard CMOS circuit and afterwards to fabricate the nano-resonator. Starting from a SOI wafer and using very simple processes, the SOI silicon layer is removed, except from the areas in which nano-structures will be fabricated; obtaining a silicon substrate with islands with a SOI structure. The CMOS circuitry will be integrated on the bulk silicon region, while the remainder SOI region will be used for the nanoresonator. The silicon oxide of this SOI region is used as insulator; and as sacrificial layer, etched to release the cantilever from the substrate. To assure the cover of the different CMOS layers over the step of the islands, it is essential to avoid very sharp steps.

  18. Influence of the Ar-ion irradiation on the giant magnetoresistance in Fe/Cr multilayers

    NASA Astrophysics Data System (ADS)

    Kopcewicz, M.; Stobiecki, F.; Jagielski, J.; Szymański, B.; Schmidt, M.; Dubowik, J.; Kalinowska, J.

    2003-05-01

    The influence of 200 keV Ar-ion irradiation on the interlayer coupling in Fe/Cr multilayers exhibiting the giant magnetoresistance (GMR) effect is studied by the conversion electron Mössbauer spectroscopy (CEMS), vibrating sample magnetometer hysteresis loops, magnetoresistivity, and electric resistivity measurements and supplemented by the small-angle x-ray diffraction. The increase of Ar-ion dose causes an increase of interface roughness, as evidenced by the increase of the Fe step sites detected by CEMS. The modification of microstructure induces changes in magnetization reversal indicating a gradual loss of antiferromagnetic (AF) coupling correlated with the degradation of the GMR effect. Distinctly weaker degradation of AF coupling and the GMR effect observed for irradiated samples with a thicker Cr layer thickness suggest that observed effects are caused by pinholes creation. The measurements of temperature dependence of remanence magnetization confirm increase of pinhole density and sizes during implantation. Other effects which can influence spin dependent contribution to the resistance, such as interface roughness as well as shortening of mean-free path of conduction electrons, are also discussed.

  19. Handbook of the Materials Properties of FeCrAl Alloys For Nuclear Power Production Applications

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

    Yamamoto, Yukinori; Snead, Mary A.; Field, Kevin G.

    FeCrAl alloys are a class of alloys that have seen increased interest for nuclear power applications including as accident tolerant fuel cladding, structural components for fast fission reactors, and as first wall and blanket structures for fusion reactors. FeCrAl alloys are under consideration for these applications due to their inherent corrosion resistance, stress corrosion cracking resistance, radiation-induced swelling resistance, and high temperature oxidation resistance. A substantial amount of research effort has been completed to design, develop, and begin commercial scaling of FeCrAl alloys for nuclear power applications over the past half a century. These efforts have led to the developmentmore » of an extensive database on material properties and process knowledge for FeCrAl alloys but not within a consolidated format. The following report is the first edition of a materials handbook to consolidate the state-of-the-art on FeCrAl alloys for nuclear power applications. This centralized database focuses solely on wrought FeCrAl alloys, oxide dispersion strengthened alloys, although discussed in brief, are not covered. Where appropriate, recommendations for applications of the data is provided and current knowledge gaps are identified.« less

  20. BISON Fuel Performance Analysis of FeCrAl cladding with updated properties

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

    Sweet, Ryan; George, Nathan M.; Terrani, Kurt A.

    2016-08-30

    In order to improve the accident tolerance of light water reactor (LWR) fuel, alternative cladding materials have been proposed to replace zirconium (Zr)-based alloys. Of these materials, there is a particular focus on iron-chromium-aluminum (FeCrAl) alloys due to much slower oxidation kinetics in high-temperature steam than Zr-alloys. This should decrease the energy release due to oxidation and allow the cladding to remain integral longer in the presence of high temperature steam, making accident mitigation more likely. As a continuation of the development for these alloys, suitability for normal operation must also be demonstrated. This research is focused on modeling themore » integral thermo-mechanical performance of FeCrAl-cladded fuel during normal reactor operation. Preliminary analysis has been performed to assess FeCrAl alloys (namely Alkrothal 720 and APMT) as a suitable fuel cladding replacement for Zr-alloys, using the MOOSE-based, finite-element fuel performance code BISON and the best available thermal-mechanical and irradiation-induced constitutive properties. These simulations identify the effects of the mechanical-stress and irradiation response of FeCrAl, and provide a comparison with Zr-alloys. In comparing these clad materials, fuel rods have been simulated for normal reactor operation and simple steady-state operation. Normal reactor operating conditions target the cladding performance over the rod lifetime (~4 cycles) for the highest-power rod in the highest-power fuel assembly under reactor power maneuvering. The power histories and axial temperature profiles input into BISON were generated from a neutronics study on full-core reactivity equivalence for FeCrAl using the 3D full core simulator NESTLE. Evolution of the FeCrAl cladding behavior over time is evaluated by using steady-state operating conditions such as a simple axial power profile, a constant cladding surface temperature, and a constant fuel power history. The fuel rod designs

  1. Low-cost Fe--Ni--Cr alloys for high temperature valve applications

    DOEpatents

    Muralidharan, Govindarajan

    2017-03-28

    An Fe--Ni--Cr alloy is composed essentially of, in terms of weight percent: 1 to 3.5 Al, up to 2 Co, 15 to 19.5 Cr, up to 2 Cu, 23 to 40 Fe, up to 0.3 Hf, up to 4 Mn, 0.15 to 2 Mo, up to 0.15 Si, up to 1.05 Ta, 2.8 to 4.3 Ti, up to 0.5 W, up to 0.06 Zr, 0.02 to 0.15 C, 0.0001 to 0.007 N, balance Ni, wherein, in terms of atomic percent: 6.5.ltoreq.Al+Ti+Zr+Hf+Ta.ltoreq.10, 0.33.ltoreq.Al/(Al+Ti+Zr+Hf+Ta).ltoreq.0.065, 4.ltoreq.(Fe+Cr)/(Al+Ti+Zr+Hf+Ta).ltoreq.10, the alloy being essentially free of Nb and V.

  2. 2nd Gen FeCrAl ODS Alloy Development For Accident-Tolerant Fuel Cladding

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

    Dryepondt, Sebastien N.; Massey, Caleb P.; Edmondson, Philip D.

    Extensive research at ORNL aims at developing advanced low-Cr high strength FeCrAl alloys for accident tolerant fuel cladding. One task focuses on the fabrication of new low Cr oxide dispersion strengthened (ODS) FeCrAl alloys. The first Fe-12Cr-5Al+Y 2O 3 (+ ZrO 2 or TiO 2) ODS alloys exhibited excellent tensile strength up to 800 C and good oxidation resistance in steam up to 1400 C, but very limited plastic deformation at temperature ranging from room to 800 C. To improve alloy ductility, several fabrication parameters were considered. New Fe-10-12Cr-6Al gas-atomized powders containing 0.15 to 0.5wt% Zr were procured and ballmore » milled for 10h, 20h or 40h with Y2O3. The resulting powder was then extruded at temperature ranging from 900 to 1050 C. Decreasing the ball milling time or increasing the extrusion temperature changed the alloy grain size leading to lower strength but enhanced ductility. Small variations of the Cr, Zr, O and N content did not seem to significantly impact the alloy tensile properties, and, overall, the 2nd gen ODS FeCrAl alloys showed significantly better ductility than the 1st gen alloys. Tube fabrication needed for fuel cladding will require cold or warm working associated with softening heat treatments, work was therefore initiated to assess the effect of these fabrications steps on the alloy microstructure and properties. This report has been submitted as fulfillment of milestone M3FT 16OR020202091 titled, Report on 2nd Gen FeCrAl ODS Alloy Development for the Department of Energy Office of Nuclear Energy, Advanced Fuel Campaign of the Fuel Cycle R&D program.« less

  3. Analysis of the FeCrAl Accident Tolerant Fuel Concept Benefits during BWR Station Blackout Accidents

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

    Robb, Kevin R

    2015-01-01

    Iron-chromium-aluminum (FeCrAl) alloys are being considered for fuel concepts with enhanced accident tolerance. FeCrAl alloys have very slow oxidation kinetics and good strength at high temperatures. FeCrAl could be used for fuel cladding in light water reactors and/or as channel box material in boiling water reactors (BWRs). To estimate the potential safety gains afforded by the FeCrAl concept, the MELCOR code was used to analyze a range of postulated station blackout severe accident scenarios in a BWR/4 reactor employing FeCrAl. The simulations utilize the most recently known thermophysical properties and oxidation kinetics for FeCrAl. Overall, when compared to the traditionalmore » Zircaloy-based cladding and channel box, the FeCrAl concept provides a few extra hours of time for operators to take mitigating actions and/or for evacuations to take place. A coolable core geometry is retained longer, enhancing the ability to stabilize an accident. Finally, due to the slower oxidation kinetics, substantially less hydrogen is generated, and the generation is delayed in time. This decreases the amount of non-condensable gases in containment and the potential for deflagrations to inhibit the accident response.« less

  4. Starting points for the study of non-Fermi liquid-like properties of FeCrAs

    NASA Astrophysics Data System (ADS)

    O'Brien, Patrick James

    FeCrAs exhibits non-Fermi liquid-like behavior because of its odd combination of thermodynamic, transport, and magnetic properties. In particular, the resistivity of FeCrAs is not characteristic of a metal or an insulator and so remains a mystery. In this thesis, we seek a model to describe its properties. In FeCrAs, local moments reside on the Cr sites, and there is some conduction. We study the simplest possible model on the kagome lattice that features local moments and itinerant electrons, the kagome Kondo Lattice Model. We present the phase diagram of this model, which features a host of complex spin orders, one of which is the √3 x √3, the experimentally observed magnetic ground state in FeCrAs. The kagome Kondo Lattice Model, having one itinerant d-orbital band on the kagome lattice, does not fully capture the microscopic physics of FeCrAs. The kagome Kondo Lattice Model also will not de- scribe the mutilation of the Fermi surface. To investigate the microscopic properties, we calculated LDA and LDA+U results. These results and GGA results from another group all exhibit high d-orbital density of states at the Fermi energy as well as low p-orbital density of states at the Fermi energy. The DFT results motivated us to construct a model based on the chemistry and full geometry of the FeCrAs crystal. The model we construct is an effective hopping model consisting of only d-orbital operators that we call the Optimal Overlap Hopping Model (OOHM). We calculate the band structure that results from the OOHM, and this band structure can be compared to ARPES measurements. As an example of how one can use the OOHM, we calculate a dynamic spin structure factor from within the OOHM, and we compare it to neutron scattering data. We consider both the OOHM and the Kondo Lattice Model on the kagome lattice as starting points from which we can launch studies of FeCrAs, and we present the existing theories for FeCrAs on a metallicity spectrum to illustrate the various

  5. Advanced ODS FeCrAl alloys for accident-tolerant fuel cladding

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

    Dryepondt, Sebastien N; Unocic, Kinga A; Hoelzer, David T

    2014-09-01

    ODS FeCrAl alloys are being developed with optimum composition and properties for accident tolerant fuel cladding. Two oxide dispersion strengthened (ODS) Fe-15Cr-5Al+Y2O3 alloys were fabricated by ball milling and extrusion of gas atomized metallic powder mixed with Y2O3 powder. To assess the impact of Mo on the alloy mechanical properties, one alloy contained 1%Mo. The hardness and tensile properties of the two alloys were close and higher than the values reported for fine grain PM2000 alloy. This is likely due to the combination of a very fine grain structure and the presence of nano oxide precipitates. The nano oxide dispersionmore » was however not sufficient to prevent grain boundary sliding at 800 C and the creep properties of the alloys were similar or only slightly superior to fine grain PM2000 alloy. Both alloys formed a protective alumina scale at 1200 C in air and steam and the mass gain curves were similar to curves generated with 12Cr-5Al+Y2O3 (+Hf or Zr) ODS alloys fabricated for a different project. To estimate the maximum temperature limit of use for the two alloys in steam, ramp tests at a rate of 5 C/min were carried out in steam. Like other ODS alloys, the two alloys showed a significant increase of the mas gains at T~ 1380 C compared with ~1480 C for wrought alloys of similar composition. The beneficial effect of Yttrium for wrought FeCrAl does not seem effective for most ODS FeCrAl alloys. Characterization of the hardness of annealed specimens revealed that the microstructure of the two alloys was not stable above 1000 C. Concurrent radiation results suggested that Cr levels <15wt% are desirable and the creep and oxidation results from the 12Cr ODS alloys indicate that a lower Cr, high strength ODS alloy with a higher maximum use temperature could be achieved.« less

  6. Interfacial layers in high-temperature-oxidized NiCrAl

    NASA Technical Reports Server (NTRS)

    Larson, L. A.; Browning, R.; Poppa, H.; Smialek, J.

    1983-01-01

    The utility of Auger electron spectroscopy combined with ball cratering for depth analysis of oxide and diffusion layers produced in a Ni-14Cr-24Al alloy by oxidation in air at 1180 C for 25 hr is demonstrated. During postoxidation cooling, the oxide layers formed by this alloy spalled profusely. The remaining very thin oxide was primarily Cr2O3 with a trace of Ni. The underlying metal substrate exhibited gamma/gamma-prime and beta phases with a metallic interfacial layer which was similar to the bulk gamma/gamma-prime phase but slightly enriched in Cr and Al. These data are compared to electron microprobe results from a nominally identical alloy. The diffusion layer thickness is modelled with a simple mass balance equation and compared to recent results on the diffusion process in NiCrAl alloys.

  7. Parametric and experimentally informed BWR Severe Accident Analysis Utilizing FeCrAl - M3FT-17OR020205041

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

    Ott, Larry J.; Howell, Michael; Robb, Kevin R.

    Iron-chromium-aluminum (FeCrAl) alloys are being considered as advanced fuel cladding concepts with enhanced accident tolerance. At high temperatures, FeCrAl alloys have slower oxidation kinetics and higher strength compared with zirconium-based alloys. FeCrAl could be used for fuel cladding and spacer or mixing vane grids in light water reactors and/or as channel box material in boiling water reactors (BWRs). There is a need to assess the potential gains afforded by the FeCrAl accident-tolerant-fuel (ATF) concept over the existing zirconium-based materials employed today. To accurately assess the response of FeCrAl alloys under severe accident conditions, a number of FeCrAl properties and characteristicsmore » are required. These include thermophysical properties as well as burst characteristics, oxidation kinetics, possible eutectic interactions, and failure temperatures. These properties can vary among different FeCrAl alloys. Oak Ridge National Laboratory has pursued refined values for the oxidation kinetics of the B136Y FeCrAl alloy (Fe-13Cr-6Al wt %). This investigation included oxidation tests with varying heating rates and end-point temperatures in a steam environment. The rate constant for the low-temperature oxidation kinetics was found to be higher than that for the commercial APMT FeCrAl alloy (Fe-21Cr-5Al-3Mo wt %). Compared with APMT, a 5 times higher rate constant best predicted the entire dataset (root mean square deviation). Based on tests following heating rates comparable with those the cladding would experience during a station blackout, the transition to higher oxidation kinetics occurs at approximately 1,500°C. A parametric study varying the low-temperature FeCrAl oxidation kinetics was conducted for a BWR plant using FeCrAl fuel cladding and channel boxes using the MELCOR code. A range of station blackout severe accident scenarios were simulated for a BWR/4 reactor with Mark I containment. Increasing the FeCrAl low-temperature oxidation

  8. Reduction of Cr(VI) to Cr(III) by green rust - sulphate

    NASA Astrophysics Data System (ADS)

    Skovbjerg, L.; Stipp, S.

    2003-04-01

    Chromium is widely used in industrial processes such as leather tanning, electro-plating and as colour pigments. Unfortunately, hexavalent chromium is both toxic and very soluble so it can be a problem for groundwater resources. Given the right redox conditions, however, Cr(VI) can be reduced to trivalent chromium, which is much less soluble and is an essential trace nutrient. Fe(II), an element common in soil and sediments under anaerobic conditions, can serve as a reducing agent for Cr(VI). Green Rust (GR) is a layered Fe(II),Fe(III)-hydroxide with various anions compensating charge in the interlayers. It is very effective in reducing Cr(VI) to Cr(III). GR exists in nature and is thought to be precursor for the formation of Fe(III)-oxides and oxyhydroxides at the redox boundary. It may be that the formation of GR is a key process in the effectiveness of reactive barriers for groundwater remediation that are based on Fe(0). The purpose of this work is to investigate the mechanisms controlling Cr(VI) reduction by Green Rust, to examine the effect of Cr adsorption and incorporation on GR morphology and composition, and to define the role of parameters such as interlayer anion, initial Cr(VI) concentration and time. We are using freshly synthesised material that has not been dried to avoid structural changes that may accompany dehydration and rehydration. X-Ray Diffraction (XRD) is used to characterise mineral structural changes and Atomic Force Microscopy (AFM), to examine changes in morphology as reactions take place. By adjusting the concentration of Cr(VI), we can control the rate of surface change and we can observe the nanoscale particles directly.

  9. Density Functional Study for Chemical Reaction between Cr and Fe with Sodium Diethyldithiocarbamate (NaDDC)

    NASA Astrophysics Data System (ADS)

    Setiyanto, Henry; Muhida, Rifki; Kishi, Tomoya; Rahman, Md. Mahmudur; Dipojono, Hermawan K.; Diño, Wilson A.; Matsumoto, Shigeno; Kasai, Hideaki

    Analytical chemistry in the perspective of ab initio molecular orbital calculation is introduced by investigating the chemical reaction between transition metals Cr and Fe with sodium diethyldithiocarbamate (NaDDC), a complexing agent to detect and extract Cr in human blood sample. Using density functional theory—based calculations, we determine the stable structure of the Cr-DDC and Fe-DDC complexes and obtain its dissociation energies. We found dissociation energy values of -3.24 and -2.67 eV for Cr and Fe complexes, respectively; and hence the formation of the former complex is more favorable than the formation of the latter.

  10. Design of alumina forming FeCrAl steels for lead or lead-bismuth cooled fast reactors

    NASA Astrophysics Data System (ADS)

    Lim, Jun; Hwang, Il Soon; Kim, Ji Hyun

    2013-10-01

    Iron-chromium-aluminum alloys containing 15-20 wt.% Cr and 4-6 wt.% Al have shown excellent corrosion resistance in the temperature range up to 600 °C or higher in liquid lead and lead-bismuth eutectic environments by the formation of protective Al2O3 layers. However, the higher Cr and Al concentrations in ferritic alloys could be problematic because of severe embrittlement in the manufacturing process as well as in service, caused by the formation of brittle phases. For this reason, efforts worldwide have so far mainly focused on the development of aluminizing surface treatments. However, aluminizing surface treatments have major disadvantages of cost, processing difficulties and reliability issues. In this study, a new FeCrAl alloy is proposed for structural materials in lead and lead-bismuth cooled nuclear applications. The alloy design relied on corrosion experiments in high temperature lead and lead-bismuth eutectic environments and computational thermodynamic calculations using the commercial software, JMatPro. The design of new alloys has focused on the optimization of Cr and Al levels for the formation of an external Al2O3 layer which can provide excellent oxidation and corrosion resistance in liquid lead alloys in the temperature range 300-600 °C while still retaining workable mechanical properties.

  11. Elastic Modulus Measurement of ORNL ATF FeCrAl Alloys

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

    Thompson, Zachary T.; Terrani, Kurt A.; Yamamoto, Yukinori

    2015-10-01

    Elastic modulus and Poisson’s ratio for a number of wrought FeCrAl alloys, intended for accident tolerant fuel cladding application, are determined via resonant ultrasonic spectroscopy. The results are reported as a function of temperature from room temperature to 850°C. The wrought alloys were in the fully annealed and unirradiated state. The elastic modulus for the wrought FeCrAl alloys is at least twice that of Zr-based alloys over the temperature range of this study. The Poisson’s ratio of the alloys was 0.28 on average and increased very slightly with increasing temperature.

  12. Rough SERS substrate based on gold coated porous silicon layer prepared on the silicon backside surface

    NASA Astrophysics Data System (ADS)

    Dridi, H.; Haji, L.; Moadhen, A.

    2017-04-01

    We report in this paper a novel method to elaborate rough Surface Enhanced Raman Scattering (SERS) substrate. A single layer of porous silicon was formed on the silicon backside surface. Morphological characteristics of the porous silicon layer before and after gold deposition were influenced by the rough character (gold size). The reflectance measurements showed a dependence of the gold nano-grains size on the surface nature, through the Localized Surface Plasmon (LSP) band properties. SERS signal of Rhodamine 6G used as a model analyte, adsorbed on the rough porous silicon layer revealed a marked enhancement of its vibrational modes intensities.

  13. Formation mechanisms of neutral Fe layers in the thermosphere at Antarctica studied with a thermosphere-ionosphere Fe/Fe+ (TIFe) model

    NASA Astrophysics Data System (ADS)

    Chu, Xinzhao; Yu, Zhibin

    2017-06-01

    With a thermosphere-ionosphere Fe/Fe+ (TIFe) model developed from first principles at the University of Colorado, we present the first quantitative investigation of formation mechanisms of thermospheric Fe layers observed by lidar in Antarctica. These recently discovered neutral metal layers in the thermosphere between 100 and 200 km provide unique tracers for studies of fundamental processes in the space-atmosphere interaction region. The TIFe model formulates and expands the TIFe theory originally proposed by Chu et al. that the thermospheric Fe layers are produced through the neutralization of converged Fe+ layers. Through testing mechanisms and reproducing the 28 May 2011 event at McMurdo, we conceive the lifecycle of meteoric metals via deposition, transport, chemistry, and wave dynamics for thermospheric Fe layers with gravity wave signatures. While the meteor injection of iron species is negligible above 120 km, the polar electric field transports metallic ions Fe+ upward from their main deposition region into the E-F regions, providing the major source of Fe+ (and accordingly Fe) in the thermosphere. Atmospheric wave-induced vertical shears of vertical and horizontal winds converge Fe+ to form dense Fe+ layers. Direct electron-Fe+ recombination is the major channel to neutralize Fe+ layers to form Fe above 120 km. Fe layer shapes are determined by multiple factors of neutral winds, electric field, and aurora activity. Gravity-wave-induced vertical wind plays a key role in forming gravity-wave-shaped Fe layers. Aurora particle precipitation enhances Fe+ neutralization by increasing electron density while accelerating Fe loss via charge transfer with enhanced NO+ and O2+ densities.Plain Language SummaryThe discoveries of neutral metal <span class="hlt">layers</span> reaching near 200 km in the thermosphere have significant scientific merit because such discoveries challenge the current understandings of upper atmospheric composition</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000JNuM..280..235B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000JNuM..280..235B"><span>Effects of the accumulated annealing parameter on the corrosion characteristics of a Zr-0.5Nb-1.0Sn-0.5<span class="hlt">Fe</span>-0.25<span class="hlt">Cr</span> alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baek, Jong Hyuk; Jeong, Yong Hwan; Kim, In Sup</p> <p>2000-07-01</p> <p>Corrosion behavior, hydrogen pickup, oxide microstructure, and precipitate characterization have been studied in order to investigate the effect of the accumulated annealing parameter on the corrosion characteristics in a Zr-Nb-Sn-<span class="hlt">Fe-Cr</span> alloy. An autoclave corrosion test was carried out in 400°C steam for 300 days on the Zr-0.5Nb-1.0Sn-0.5<span class="hlt">Fe</span>-0.25<span class="hlt">Cr</span> alloy, which had been given 18 different accumulated annealing parameters. The corrosion rate increased with increasing the accumulated annealing parameter. To investigate the crystal structure of oxide <span class="hlt">layer</span>, the corroded specimens were prepared to have an equal oxide thickness (˜1.6 μm) by controlling exposure time. The relative fraction of tetragonal ZrO 2 also decreased gradually with increasing accumulated annealing parameter. From the hydrogen analysis of the corroded samples for 300 days, it was observed that, with increasing the size of precipitates, the hydrogen pickup was enhanced. It was revealed from transmission electron microscope (TEM) observation of the oxide that the larger precipitates still remained to be oxidized in the oxide <span class="hlt">layer</span> and had undergone a reduction of <span class="hlt">Fe/Cr</span> ratio from 2.1 to 1.5. The oxidation of the precipitates in the oxide gave rise to a volume expansion at the precipitate-oxide interface. This volume change could lead to the transformation in the oxide phase from tetragonal ZrO 2 to monoclinic ZrO 2 and in oxide structure from columnar grain to equiaxed grain. The precipitate in a Zr-0.5Nb-1.0Sn-0.5<span class="hlt">Fe</span>-0.25<span class="hlt">Cr</span> alloy is composed of Nb, <span class="hlt">Fe</span>, and <span class="hlt">Cr</span> and the Nb content in the precipitate increase with increasing accumulated annealing parameter. Thus, it can be thought that Nb within precipitates plays a key role in the microstructural change of oxide.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1942m0024K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1942m0024K"><span>Magnetocaloric effect in cubic spinel Co(<span class="hlt">Cr</span>0.95<span class="hlt">Fe</span>0.05)2O4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumar, Ram; Rayaprol, S.; Xiao, Y.; Ji, W.; Siruguri, V.; Pal, D.</p> <p>2018-04-01</p> <p>The crystal structure, magnetic properties and magnetocaloric effect (MCE) of Co(<span class="hlt">Cr</span>0.95<span class="hlt">Fe</span>0.05)2O4 have been studied. Co(<span class="hlt">Cr</span>0.95<span class="hlt">Fe</span>0.05)2O4 synthesized by solid-state reaction method, crystallizes in normal cubic spinel structure with Fd-3m space group. Neutron powder diffraction (NPD) and magnetic measurements when compared to the undoped Co<span class="hlt">Cr</span>2O4, show that the compound is ferrimagnetic (FIM) and transition temperature (TC) is enhanced due to <span class="hlt">Fe</span> substitution. Analysis of structural and magnetic properties shows the existence of two different sites of magnetic clusters due to <span class="hlt">Fe/Cr</span> cation disorder. The competition between the moments of the two different sub-lattices gives rise to the temperature induced magnetization reversal at compensation tempearature (Tcomp) = 44 K. The magnetocaloric effect (simply the change in magnetic entropy i.e, -ΔSM) has been observed in Co(<span class="hlt">Cr</span>0.95<span class="hlt">Fe</span>0.05)2O4 with different applied magnetic fields (max. H = 90 kOe). We found maximum change of magnetic entropy ˜1.2 J/kg K, for a field change of 90 kOe at FIM transition temperature (TC˜110 K) with relative cooling power (RCP) of ˜13 J/kg. Moreover, the sign change of -ΔSM across the compensation temperature (Tcomp˜ 44 K) shows another phase transition across Tcomp in Co(<span class="hlt">Cr</span>0.95<span class="hlt">Fe</span>0.05)2O4. The values of MCE and RCP are also appreciable so as to consider Co(<span class="hlt">Cr</span>0.95<span class="hlt">Fe</span>0.05)2O4 as a magnetic refrigerant above liquid nitrogen temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1942i0011J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1942i0011J"><span>First principles investigations of <span class="hlt">Fe</span>2<span class="hlt">Cr</span>Si Heusler alloys by substitution of Co at <span class="hlt">Fe</span> site</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jain, Rakesh; Lakshmi, N.; Jain, Vivek Kumar; Chandra, Aarti R.</p> <p>2018-04-01</p> <p>Electronic structure and magnetic properties of <span class="hlt">Fe</span>2-xCox<span class="hlt">Cr</span>Si Heusler alloys have been investigated by varying Co concentration from x = 0 to 2. On increasing Co concentration, lattice constant and magnetic moment of <span class="hlt">Fe</span>2-xCox<span class="hlt">Cr</span>Si alloys increase. These alloys show true half metallic Ferromagnetic behavior with 100% spin polarization. Band gap of the alloys also increase from 0.54 eV to 0.85 eV on increasing Co concentration making these alloys promising materials for spintronics based device applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22689669-assessment-phase-constitution-al-rich-region-rapidly-solidified-al-co-fe-cr-alloys','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22689669-assessment-phase-constitution-al-rich-region-rapidly-solidified-al-co-fe-cr-alloys"><span>Assessment of phase constitution on the Al-rich region of rapidly solidified Al-Co-<span class="hlt">Fe-Cr</span> alloys</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>Wolf, W., E-mail: witorw@gmail.com</p> <p></p> <p>The formation of quasicrystalline approximants in rapidly solidified Al-Co-<span class="hlt">Fe-Cr</span> alloys was investigated. Alloys of atomic composition Al{sub 71}Co{sub 13}<span class="hlt">Fe</span>{sub 8}<span class="hlt">Cr</span>{sub 8}, Al{sub 77}Co{sub 11}<span class="hlt">Fe</span>{sub 6}<span class="hlt">Cr</span>{sub 6} and Al{sub 76}Co{sub 19}<span class="hlt">Fe</span>{sub 4}<span class="hlt">Cr</span>{sub 1} were produced using melt spinning and arc melting methods and their microstructural characterization was carried out by X-ray diffraction, scanning electron microscopy and transmission electron microscopy. Up to the present there is no consensus in the literature regarding the formation of quasicrystalline phase or quasicrystalline approximants in the Al{sub 71}Co{sub 13}<span class="hlt">Fe</span>{sub 8}<span class="hlt">Cr</span>{sub 8} alloy. This work presents, for the first time, a detailed structural characterization of selected alloysmore » in the Al-Co-<span class="hlt">Fe-Cr</span> system close to the atomic composition Al{sub 71}Co{sub 13}<span class="hlt">Fe</span>{sub 8}<span class="hlt">Cr</span>{sub 8}. The results indicated the samples to be composed, mostly, by two intermetallic phases, which are quaternary extensions of Al{sub 5}Co{sub 2} and Al{sub 13}Co{sub 4} and are quasicrystalline approximants. Although the Al{sub 5}Co{sub 2} phase has already been reported in the Al{sub 71}Co{sub 13}<span class="hlt">Fe</span>{sub 8}<span class="hlt">Cr</span>{sub 8} alloy, the presence of the monoclinic Al{sub 13}Co{sub 4} is now identified for the first time in the as cast state. In the binary Al-Co system a quasicrystalline phase is known to form in a rapidly solidified alloy with composition close to the monoclinic and orthorhombic Al{sub 13}Co{sub 4} phases. This binary quasicrystalline phase presents an average valence electron per atom (e/a) between 1.7 and 1.9; thus, in addition to the Al{sub 71}Co{sub 13}<span class="hlt">Fe</span>{sub 8}<span class="hlt">Cr</span>{sub 8} alloy, the compositions Al{sub 77}Co{sub 11}<span class="hlt">Fe</span>{sub 6}<span class="hlt">Cr</span>{sub 6} and Al{sub 76}Co{sub 19}<span class="hlt">Fe</span>{sub 4}<span class="hlt">Cr</span>{sub 1} were chosen to be within the region of formation of the quaternary extension of the Al{sub 13}Co{sub 4} phase and also within the (e/a) of 1.7 to 1.9. However, no quasicrystalline phase is present in any of the studied alloys. The Al-Co-<span class="hlt">Fe-Cr</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4185382','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4185382"><span>Coupled ferroelectric polarization and magnetization in spinel <span class="hlt">FeCr</span>2S4</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lin, L.; Zhu, H. X.; Jiang, X. M.; Wang, K. F.; Dong, S.; Yan, Z. B.; Yang, Z. R.; Wan, J. G.; Liu, J.-M.</p> <p>2014-01-01</p> <p>One of the core issues for multiferroicity is the strongly coupled ferroelectric polarization and magnetization, while so far most multiferroics have antiferromagnetic order with nearly zero magnetization. Magnetic spinel compounds with ferrimagnetic order may be alternative candidates offering large magnetization when ferroelectricity can be activated simultaneously. In this work, we investigate the ferroelectricity and magnetism of spinel <span class="hlt">FeCr</span>2S4 in which the <span class="hlt">Fe</span>2+ sublattice and <span class="hlt">Cr</span>3+ sublattice are coupled in antiparallel alignment. Well defined ferroelectric transitions below the <span class="hlt">Fe</span>2+ orbital ordering termperature Too = 8.5 K are demonstrated. The ferroelectric polarization has two components. One component arises mainly from the noncollinear conical spin order associated with the spin-orbit coupling, which is thus magnetic field sensitive. The other is probably attributed to the Jahn-Teller distortion induced lattice symmetry breaking, occuring below the orbital ordering of <span class="hlt">Fe</span>2+. Furthermore, the coupled ferroelectric polarization and magnetization in response to magnetic field are observed. The present work suggests that spinel <span class="hlt">FeCr</span>2S4 is a multiferroic offering both ferroelectricity and ferrimagnetism with large net magnetization. PMID:25284432</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1427334-effect-molybdenum-corrosion-behavior-high-entropy-alloys-cocrfeni-cocrfeni-mo-under-sodium-chloride-aqueous-conditions','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1427334-effect-molybdenum-corrosion-behavior-high-entropy-alloys-cocrfeni-cocrfeni-mo-under-sodium-chloride-aqueous-conditions"><span>Effect of Molybdenum on the Corrosion Behavior of High-Entropy Alloys Co<span class="hlt">CrFe</span>Ni 2 and Co<span class="hlt">CrFe</span>Ni 2 Mo 0.25 under Sodium Chloride Aqueous Conditions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Rodriguez, Alvaro A.; Tylczak, Joseph H.; Gao, Michael C.; ...</p> <p>2018-01-01</p> <p>The corrosion behavior of high-entropy alloys (HEAs) Co<span class="hlt">CrFe</span>Ni 2 and Co<span class="hlt">CrFe</span>Ni 2 Mo 0.25 was investigated in 3.5 wt. percent sodium chloride (NaCl) at 25°C by electrochemical methods. Their corrosion parameters were compared to those of HASTELLOY® C-276 (UNS N10276) and stainless steel 316L (UNS 31600) to assess the suitability of HEAs for potential industrial applications in NaCl simulating seawater type environments. The corrosion rates were calculated using corrosion current determined from electrochemical experiments for each of the alloys. In addition, potentiodynamic polarization measurements can indicate active, passive, and transpassive behavior of the metal as well as potential susceptibility to pittingmore » corrosion. Cyclic voltammetry (CV) can confirm the alloy susceptibility to pitting corrosion. Electrochemical impedance spectroscopy (EIS) elucidates the corrosion mechanism under studied conditions. The results of the electrochemical experiments and scanning electron microscopy (SEM) analyses of the corroded surfaces revealed general corrosion on alloy Co<span class="hlt">CrFe</span>Ni 2 Mo 0.25 and HASTELLOY C-276 and pitting corrosion on alloy Co<span class="hlt">CrFe</span>Ni 2 and stainless steel 316L.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1427334-effect-molybdenum-corrosion-behavior-high-entropy-alloys-cocrfeni-cocrfeni-mo-under-sodium-chloride-aqueous-conditions','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1427334-effect-molybdenum-corrosion-behavior-high-entropy-alloys-cocrfeni-cocrfeni-mo-under-sodium-chloride-aqueous-conditions"><span>Effect of Molybdenum on the Corrosion Behavior of High-Entropy Alloys Co<span class="hlt">CrFe</span>Ni 2 and Co<span class="hlt">CrFe</span>Ni 2 Mo 0.25 under Sodium Chloride Aqueous Conditions</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>Rodriguez, Alvaro A.; Tylczak, Joseph H.; Gao, Michael C.</p> <p></p> <p>The corrosion behavior of high-entropy alloys (HEAs) Co<span class="hlt">CrFe</span>Ni 2 and Co<span class="hlt">CrFe</span>Ni 2 Mo 0.25 was investigated in 3.5 wt. percent sodium chloride (NaCl) at 25°C by electrochemical methods. Their corrosion parameters were compared to those of HASTELLOY® C-276 (UNS N10276) and stainless steel 316L (UNS 31600) to assess the suitability of HEAs for potential industrial applications in NaCl simulating seawater type environments. The corrosion rates were calculated using corrosion current determined from electrochemical experiments for each of the alloys. In addition, potentiodynamic polarization measurements can indicate active, passive, and transpassive behavior of the metal as well as potential susceptibility to pittingmore » corrosion. Cyclic voltammetry (CV) can confirm the alloy susceptibility to pitting corrosion. Electrochemical impedance spectroscopy (EIS) elucidates the corrosion mechanism under studied conditions. The results of the electrochemical experiments and scanning electron microscopy (SEM) analyses of the corroded surfaces revealed general corrosion on alloy Co<span class="hlt">CrFe</span>Ni 2 Mo 0.25 and HASTELLOY C-276 and pitting corrosion on alloy Co<span class="hlt">CrFe</span>Ni 2 and stainless steel 316L.« 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_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JNuM..407..205L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JNuM..407..205L"><span>A study of early corrosion behaviors of <span class="hlt">FeCr</span>Al alloys in liquid lead-bismuth eutectic environments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lim, Jun; Nam, Hyo On; Hwang, Il Soon; Kim, Ji Hyun</p> <p>2010-12-01</p> <p>Lead and lead-bismuth eutectic (LBE) alloy have been increasingly receiving attention as heavy liquid metal coolants (HLMC) for future nuclear energy systems. The compatibility of structural materials and components with lead-bismuth eutectic liquid at high temperature is one of key issues for the commercialization of lead fast reactors. In the present study, the corrosion behaviors of iron-based alumina-forming alloys (Kanthal-AF®, PM2000, MA956) were investigated by exposing to stagnant LBE environments at 500 °C and 550 °C for up to 500 h. After exposures, the thickness and chemistry of the oxide <span class="hlt">layer</span> on the specimens were analyzed by scanning electron microscopy, scanning transmission electron microscopy and energy dispersive X-ray spectroscopy. As a result, the oxide characteristics and the corrosion resistance were compared. In this study, it was shown that the corrosion resistance of <span class="hlt">FeCr</span>Al ODS steels (PM2000, MA956) are superior to that of <span class="hlt">FeCr</span>Al ferritic steel (Kanthal-AF®) in higher temperature LBE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/866471','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/866471"><span>Superlattice doped <span class="hlt">layers</span> for amorphous <span class="hlt">silicon</span> photovoltaic cells</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Arya, Rajeewa R.</p> <p>1988-01-12</p> <p>Superlattice doped <span class="hlt">layers</span> for amorphous <span class="hlt">silicon</span> photovoltaic cells comprise a plurality of first and second lattices of amorphous <span class="hlt">silicon</span> alternatingly formed on one another. Each of the first lattices has a first optical bandgap and each of the second lattices has a second optical bandgap different from the first optical bandgap. A method of fabricating the superlattice doped <span class="hlt">layers</span> also is disclosed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1342837','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1342837"><span>A physics-based crystallographic modeling framework for describing the thermal creep behavior of <span class="hlt">Fe-Cr</span> alloys</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>Wen, Wei; Capolungo, Laurent; Patra, Anirban</p> <p></p> <p>This Report addresses the Milestone M2MS-16LA0501032 of NEAMS Program (“Develop hardening model for <span class="hlt">FeCr</span>Al cladding), with a deadline of 09/30/2016. Here we report a constitutive law for thermal creep of <span class="hlt">FeCr</span>Al. This Report adds to and complements the one for Milestone M3MS-16LA0501034 (“Interface hardening models with MOOSE-BISON”), where we presented a hardening law for irradiated <span class="hlt">FeCr</span>Al. The last component of our polycrystal-based constitutive behavior, namely, an irradiation creep model for <span class="hlt">FeCr</span>Al, will be developed as part of the FY17 Milestones, and the three regimes will be coupled and interfaced with MOOSE-BISON.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS.985a2039R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS.985a2039R"><span>The reactive element effect of yttrium and yttrium <span class="hlt">silicon</span> on high temperature oxidation of Ni<span class="hlt">Cr</span>Al coating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ramandhany, S.; Sugiarti, E.; Desiati, R. D.; Martides, E.; Junianto, E.; Prawara, B.; Sukarto, A.; Tjahjono, A.</p> <p>2018-03-01</p> <p>The microstructure formed on the bond coat affects the oxidation resistance, particularly the formation of a protective oxide <span class="hlt">layer</span>. The adhesion of bond coat and TGO increased significantly by addition of reactive element. In the present work, the effect of yttrium and yttrium <span class="hlt">silicon</span> as reactive element (RE) on Ni<span class="hlt">Cr</span>Al coating was investigated. The Ni<span class="hlt">Cr</span>Al (without RE) and Ni<span class="hlt">Cr</span>AlX (X:Y or YSi) bond coating were deposited on Hastelloy C-276 substrate by High Velocity Oxygen Fuel (HVOF) method. Isothermal oxidation was carried out at 1000 °C for 100 hours. The results showed that the addition of RE could prevent the breakaway oxidation. Therefore, the coating with reactive element were more protective against high temperature oxidation. Furthermore, the oxidation rate of Ni<span class="hlt">Cr</span>AlY coating was lower than Ni<span class="hlt">Cr</span>AlYSi coating with the total mass change was ±2.394 mg/cm2 after 100 hours of oxidation. The thickness of oxide scale was approximately 1.18 μm consisting of duplex oxide scale of spinel Ni<span class="hlt">Cr</span>2O4 in outer scale and protective α-Al2O3 in inner scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12526565','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12526565"><span>The <span class="hlt">Cr</span>IIL reduction of [2<span class="hlt">Fe</span>-2S] ferredoxins and site of attachment of <span class="hlt">Cr</span>III using 1H NMR and site-directed mutagenesis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Im, S C; Worrall, J A; Liu, G; Aliverti, A; Zanetti, G; Luchinat, C; Bertini, I; Sykes, A G</p> <p>2000-04-17</p> <p>The recently reported NMR solution structure of <span class="hlt">Fe</span>IIIFeIII parsley FdI has made possible 2D NOESY NMR studies to determine the point of attachment of <span class="hlt">Cr</span>IIIL in <span class="hlt">FeIIIFeIII...Cr</span>IIIL. The latter <span class="hlt">Cr</span>-modified product was obtained by reduction of <span class="hlt">Fe</span>IIIFeIII parsley and spinach FdI forms with [<span class="hlt">Cr</span>(15-aneN4) (H2O)2]2+ (15-aneN4 = 1,4,8,12-tetraazacyclopentadecane), referred to here as <span class="hlt">Cr</span>IIL, followed by air oxidation and chromatographic purification. From a comparison of NMR cross-peak intensities of native and <span class="hlt">Cr</span>-modified proteins, two surface sites designated A and B, giving large paramagnetic <span class="hlt">Cr</span>IIIL broadening of a number of amino acid peaks, have been identified. The effects at site A (residues 19-22, 27, and 30) are greater than those at site B (residues 92-94 and 96), which is on the opposite side of the protein. From metal (ICP-AES) and electrospray ionization mass spectrometry (EIMS) analyses on the <span class="hlt">Cr</span>-modified protein, attachment of a single <span class="hlt">Cr</span>IIIL only is confirmed for both parsley and spinach FdI and FdII proteins. Electrostatic interaction of the 3+ <span class="hlt">Cr</span>IIIL center covalently attached to one protein molecule (charge approximately -18) with a second (like) molecule provides an explanation for the involvement of two regions. Thus for 3-4 mM <span class="hlt">FeIIIFeIII...Cr</span>IIIL solutions used in NMR studies (<span class="hlt">Cr</span>IIIL attached at A), broadening effects due to electrostatic interactions at B on a second molecule are observed. Experiments with the Cys18Ala spinach FdI variant have confirmed that the previously suggested Cys-18 at site A is not the site of <span class="hlt">Cr</span>IIIL attachment. Line broadening at Val-22 of A gives the largest effect, and <span class="hlt">Cr</span>IIIL attachment at one or more adjacent (conserved) acidic residues in this region is indicated. The ability of <span class="hlt">Cr</span>IIL to bind in some (parsley and spinach) but not all cases (Anabaena variabilis) suggests that intramolecular H-bonding of acidic residues at A is relevant. The parsley and spinach <span class="hlt">FeIIFeIII...Cr</span>IIIL products undergo a second stage of reduction</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1357974-investigation-fecral-cladding-behavior-under-normal-operating-loss-coolant-conditions','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1357974-investigation-fecral-cladding-behavior-under-normal-operating-loss-coolant-conditions"><span>An investigation of <span class="hlt">FeCr</span>Al cladding behavior under normal operating and loss of coolant conditions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Gamble, Kyle A.; Barani, Tommaso; Pizzocri, David; ...</p> <p>2017-04-30</p> <p>Iron-chromium-aluminum (<span class="hlt">FeCr</span>Al) alloys are candidates to be used as nuclear fuel cladding for increased accident tolerance. An analysis of the response of <span class="hlt">FeCr</span>Al under normal operating and loss of coolant conditions has been performed using fuel performance modeling. In particular, recent information on <span class="hlt">FeCr</span>Al material properties and phenomena from separate effects tests has been implemented in the BISON fuel performance code and analyses of integral fuel rod behavior with <span class="hlt">FeCr</span>Al cladding have been performed. BISON simulations included both light water reactor normal operation and loss-of-coolant accidental transients. In order to model fuel rod behavior during accidents, a cladding failure criterionmore » is desirable. For <span class="hlt">FeCr</span>Al alloys, a failure criterion is developed using recent burst experiments under loss of coolant like conditions. The added material models are utilized to perform comparative studies with Zircaloy-4 under normal operating conditions and oxidizing and non-oxidizing out-of-pile loss of coolant conditions. The results indicate that for all conditions studied, <span class="hlt">FeCr</span>Al behaves similarly to Zircaloy-4 with the exception of improved oxidation performance. Here, further experiments are required to confirm these observations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1357974','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1357974"><span>An investigation of <span class="hlt">FeCr</span>Al cladding behavior under normal operating and loss of coolant conditions</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>Gamble, Kyle A.; Barani, Tommaso; Pizzocri, David</p> <p></p> <p>Iron-chromium-aluminum (<span class="hlt">FeCr</span>Al) alloys are candidates to be used as nuclear fuel cladding for increased accident tolerance. An analysis of the response of <span class="hlt">FeCr</span>Al under normal operating and loss of coolant conditions has been performed using fuel performance modeling. In particular, recent information on <span class="hlt">FeCr</span>Al material properties and phenomena from separate effects tests has been implemented in the BISON fuel performance code and analyses of integral fuel rod behavior with <span class="hlt">FeCr</span>Al cladding have been performed. BISON simulations included both light water reactor normal operation and loss-of-coolant accidental transients. In order to model fuel rod behavior during accidents, a cladding failure criterionmore » is desirable. For <span class="hlt">FeCr</span>Al alloys, a failure criterion is developed using recent burst experiments under loss of coolant like conditions. The added material models are utilized to perform comparative studies with Zircaloy-4 under normal operating conditions and oxidizing and non-oxidizing out-of-pile loss of coolant conditions. The results indicate that for all conditions studied, <span class="hlt">FeCr</span>Al behaves similarly to Zircaloy-4 with the exception of improved oxidation performance. Here, further experiments are required to confirm these observations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29488927','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29488927"><span>Nuclear resonance reflectivity from a [57<span class="hlt">Fe/Cr</span>]30 multilayer with the Synchrotron Mössbauer Source.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Andreeva, Marina A; Baulin, Roman A; Chumakov, Aleksandr I; Rüffer, Rudolf; Smirnov, Gennadii V; Babanov, Yurii A; Devyaterikov, Denis I; Milyaev, Mikhail A; Ponomarev, Dmitrii A; Romashev, Lazar N; Ustinov, Vladimir V</p> <p>2018-03-01</p> <p>Mössbauer reflectivity spectra and nuclear resonance reflectivity (NRR) curves have been measured using the Synchrotron Mössbauer Source (SMS) for a [ 57 <span class="hlt">Fe/Cr</span>] 30 periodic multilayer, characterized by the antiferromagnetic interlayer coupling between adjacent 57 <span class="hlt">Fe</span> <span class="hlt">layers</span>. Specific features of the Mössbauer reflectivity spectra measured with π-polarized radiation of the SMS near the critical angle and at the `magnetic' maximum on the NRR curve are analyzed. The variation of the ratio of lines in the Mössbauer reflectivity spectra and the change of the intensity of the `magnetic' maximum under an applied external field has been used to reveal the transformation of the magnetic alignment in the investigated multilayer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMMM..439...17L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMMM..439...17L"><span>Effect of a Co<span class="hlt">Fe</span>B <span class="hlt">layer</span> on the anisotropic magnetoresistance of Ta/Co<span class="hlt">FeB/MgO/NiFe/MgO/CoFe</span>B/Ta films</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Minghua; Shi, Hui; Dong, Yuegang; Ding, Lei; Han, Gang; Zhang, Yao; Liu, Ye; Yu, Guanghua</p> <p>2017-10-01</p> <p>The anisotropic magnetoresistance (AMR) and magnetic properties of Ni<span class="hlt">Fe</span> films can be remarkably enhanced via Co<span class="hlt">Fe</span>B <span class="hlt">layer</span>. In the case of an ultrathin Ni<span class="hlt">Fe</span> film having a Ta/Co<span class="hlt">FeB/MgO/NiFe/MgO/CoFe</span>B/Ta structure, the Co<span class="hlt">Fe</span>B/MgO <span class="hlt">layers</span> suppressed the formation of magnetic dead <span class="hlt">layers</span> and the interdiffusions and interface reactions between the Ni<span class="hlt">Fe</span> and Ta <span class="hlt">layers</span>. The AMR reached a maximum value of 3.56% at 450 °C. More importantly, a single Ni<span class="hlt">Fe</span> (1 1 1) peak can be formed resulting in higher AMR values for films having Co<span class="hlt">Fe</span>B <span class="hlt">layer</span>. This enhanced AMR also originated from the significant specular reflection of electrons owing to the crystalline MgO <span class="hlt">layer</span>, together with the sharp interfaces with the Ni<span class="hlt">Fe</span> <span class="hlt">layer</span>. These factors together resulted in higher AMR and improved magnetic properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhDT.......108Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhDT.......108Z"><span>Physical Properties of Ni<span class="hlt">FeCr</span>Co-based High-Entropy Alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zaddach, Alexander Joseph</p> <p></p> <p>Conventional alloy design has been based on improving the properties of a single base, or solvent, element through relatively small additions of other elements. More recently, research has been conducted on alloys that contain multiple principal elements, particularly multi-component equiatomic alloys. When such alloys form solid solution phases, they are termed "high-entropy alloys" (HEAs) due to their high configurational entropy. These alloys often have favorable properties compared to conventional dilute solution alloys, but their compositional complexity and relative novelty means that they remain difficult to design and their basic properties are often unknown. The motivation for this work is a detailed experimental exploration of some of the basic physical properties of Ni<span class="hlt">FeCr</span>Co-based alloys. Ni<span class="hlt">FeCr</span>CoMn was one of the first equiatomic HEAs developed. As the compositional space within this single system is extremely large, this work focuses primarily on equiatomic alloys and a limited subset of non-equiatomic alloys chosen for their specific properties. Several alloys are prepared using both conventional methods (arc melting) and nonequilibrium methods (mechanical alloying). Properties studied include stacking fault energy, bulk mechanical properties, single crystal elastic constants, and magnetic properties. The equiatomic Ni<span class="hlt">FeCr</span>Co and Ni<span class="hlt">FeCr</span>CoMn alloys were found to have a moderate to low stacking fault energy, 18 -- 30 mJ m-2. As they are single-phase, fcc alloys, they have high tensile ductility. Additionally, they also exhibit high work-hardening rates, resulting in high toughness. Ni<span class="hlt">FeCr</span>Co outperforms the 5-component equiatomic alloy in ductility and toughness. A 5-component alloy with higher Co content to reduce the stacking fault energy also performs well. The single crystal elastic constants were measured using nanoindentation modulus measurements of grains of known orientation. The measured elastic constants were consistent with those calculated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22269403-magnetic-properties-fe-doped-smcro-sub-perovskite','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22269403-magnetic-properties-fe-doped-smcro-sub-perovskite"><span>Magnetic properties of <span class="hlt">Fe</span> doped Sm<span class="hlt">Cr</span>O{sub 3} perovskite</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>Bakshi, Venugopal Rao; Devarasetty, Suresh Babu, E-mail: s-devarasetty1956@yahoo.co.uk; Prasad, Bandi Vittal</p> <p>2014-04-24</p> <p>The compound Sm<span class="hlt">Cr</span>{sub 1−x} <span class="hlt">Fe</span>{sub x}O{sub 3} perovskites were prepared by citric acid route. the samples were characterized by XRD and SEM. The temperature and field dependent magnetization measurements were carried out in the temperature range of 5K −400 K at 0.01T field and −5T to 5T field at 2K. Sm<span class="hlt">Cr</span>O3 compound has shown two magnetic transition temperatures at 197 K and 38 K. The observed behavior at 197 K is the characteristic of anti-ferromagnetic ordering of <span class="hlt">Cr</span>{sup 3+} moments with weak ferromagnetism. The drop in magnetization below 38 K is due to the spin reorientation of Sm{sup 3+} inmore » anti ferromagnetic arrangement and <span class="hlt">Cr</span>{sup 3+}spins. the doping of <span class="hlt">Fe</span> in Sm<span class="hlt">Cr</span>O{sub 3} compound has shown a decrease in T{sub N1} and also the two magnetization reversals at 177K and 57K. The magnetic behavior at low temperatures is (T« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1350922-combined-apt-sans-investigation-phase-precipitation-neutron-irradiated-model-fecral-alloys','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1350922-combined-apt-sans-investigation-phase-precipitation-neutron-irradiated-model-fecral-alloys"><span>A combined APT and SANS investigation of α' phase precipitation in neutron-irradiated model <span class="hlt">FeCr</span>Al alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Briggs, Samuel A.; Edmondson, Philip D.; Littrell, Kenneth C.; ...</p> <p>2017-03-01</p> <p>Here, <span class="hlt">FeCr</span>Al alloys are currently under consideration for accident-tolerant fuel cladding applications in light water reactors owing to their superior high-temperature oxidation and corrosion resistance compared to the Zr-based alloys currently employed. However, their performance could be limited by precipitation of a <span class="hlt">Cr</span>-rich α' phase that tends to embrittle high-<span class="hlt">Cr</span> ferritic <span class="hlt">Fe</span>-based alloys. In this study, four <span class="hlt">FeCr</span>Al model alloys with 10–18 at.% <span class="hlt">Cr</span> and 5.8–9.3 at.% Al were neutron-irradiated to nominal damage doses up to 7.0 displacements per atom at a target temperature of 320 °C. Small angle neutron scattering techniques were coupled with atom probe tomography to assessmore » the composition and morphology of the resulting α' precipitates. It was demonstrated that Al additions partially destabilize the α' phase, generally resulting in precipitates with lower <span class="hlt">Cr</span> contents when compared with binary <span class="hlt">Fe-Cr</span> systems. The precipitate morphology evolution with dose exhibited a transient coarsening regime akin to previously observed behavior in aged <span class="hlt">Fe-Cr</span> alloys. Similar behavior to predictions of the LSW/UOKV models suggests that α' precipitation in irradiated <span class="hlt">FeCr</span>Al is a diffusion-limited process with coarsening mechanisms similar to those in thermally aged high-<span class="hlt">Cr</span> ferritic alloys.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080005004','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080005004"><span><span class="hlt">Silicon</span> based substrate with environmental/thermal barrier <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Eaton, Jr., Harry Edwin (Inventor); Allen, William Patrick (Inventor); Jacobson, Nathan S. (Inventor); Bansal, Narottam P. (Inventor); Opila, Elizabeth J. (Inventor); Smialek, James L. (Inventor); Lee, Kang N. (Inventor); Spitsberg, Irene T. (Inventor); Wang, Hongyu (Inventor); Meschter, Peter Joel (Inventor)</p> <p>2002-01-01</p> <p>A barrier <span class="hlt">layer</span> for a <span class="hlt">silicon</span> containing substrate which inhibits the formation of gaseous species of <span class="hlt">silicon</span> when exposed to a high temperature aqueous environment comprises a barium-strontium alumino silicate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080004987','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080004987"><span><span class="hlt">Silicon</span> based substrate with environmental/ thermal barrier <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Eaton, Jr., Harry Edwin (Inventor); Allen, William Patrick (Inventor); Jacobson, Nathan S. (Inventor); Bansal, Nanottam P. (Inventor); Opila, Elizabeth J. (Inventor); Smialek, James L. (Inventor); Lee, Kang N. (Inventor); Spitsberg, Irene T. (Inventor); Wang, Hongyu (Inventor); Meschter, Peter Joel (Inventor)</p> <p>2002-01-01</p> <p>A barrier <span class="hlt">layer</span> for a <span class="hlt">silicon</span> containing substrate which inhibits the formation of gaseous species of <span class="hlt">silicon</span> when exposed to a high temperature aqueous environment comprises a barium-strontium alumino silicate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007MMTA...38.1244C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007MMTA...38.1244C"><span>Selective Internal Oxidation as a Mechanism for Intergranular Stress Corrosion Cracking of Ni-<span class="hlt">Cr-Fe</span> Alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Capell, Brent M.; Was, Gary S.</p> <p>2007-06-01</p> <p>The mechanism of selective internal oxidation (SIO) for intergranular stress corrosion cracking (IGSCC) of nickel-base alloys has been investigated through a series of experiments using high-purity alloys and a steam environment to control the formation of NiO on the surface. Five alloys (Ni-9<span class="hlt">Fe</span>, Ni-5<span class="hlt">Cr</span>, Ni-5<span class="hlt">Cr</span>-9<span class="hlt">Fe</span>, Ni-16<span class="hlt">Cr</span>-9<span class="hlt">Fe</span>, and Ni-30<span class="hlt">Cr</span>-9<span class="hlt">Fe</span>) were used to investigate oxidation and intergranular cracking behavior for hydrogen-to-water vapor partial pressure ratios (PPRs) between 0.001 and 0.9. The Ni-9<span class="hlt">Fe</span>, Ni-5<span class="hlt">Cr</span>, and Ni-5<span class="hlt">Cr</span>-9<span class="hlt">Fe</span> alloys formed a uniform Ni(OH)2 film at PPRs less than 0.09, and the higher chromium alloys formed chromium-rich oxide films over the entire PPR range studied. Corrosion coupon results show that grain boundary oxides extended for significant depths (>150 nm) below the sample surface for all but the highest <span class="hlt">Cr</span> containing alloy. Constant extension rate tensile (CERT) test results showed that intergranular cracking varied with PPR and cracking was more pronounced at a PPR value where nonprotective Ni(OH)2 was able to form and a link between the nonprotective Ni(OH)2 film and the formation of grain boundary oxides is suggested. The observation of grain boundary oxides in stressed and unstressed samples as well as the influence of alloy content on IG cracking and oxidation support SIO as a mechanism for IGSCC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OptLT..99..374X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OptLT..99..374X"><span>Laser cladding assisted by friction stir processing for preparation of deformed crack-free Ni-<span class="hlt">Cr-Fe</span> coating with nanostructure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xie, Siyao; Li, Ruidi; Yuan, Tiechui; Chen, Chao; Zhou, Kechao; Song, Bo; Shi, Yusheng</p> <p>2018-02-01</p> <p>Although laser cladding has find its widespread application in surface hardening, this technology has been significantly limited by the solidification crack, which usually initiates along grain boundary due to the brittle precipitation in grain boundary and networks formation during the laser rapid melting/solidification process. This paper proposed a novel laser cladding technology assisted by friction stir processing (FSP) to eliminate the usual metallurgical defects by the thermomechanical coupling effect of FSP with the Ni-<span class="hlt">Cr-Fe</span> as representative coating material. By the FSP assisted laser cladding, the crack in laser cladding Ni-<span class="hlt">Cr-Fe</span> coating was eliminated and the coarse networks of laser cladding coating was transformed into dispersed nanoparticles. Moreover, the plastic <span class="hlt">layers</span> with thicknesses 47-140 μm can be observed, with gradient grain refinement from substrate to the top surface in which grain size reached 300 nm and laser photocoagulation net second phase crushed in the <span class="hlt">layer</span>. In addition, cracks closed in the plastic zone. The refinement of grain resulted the hardness increased to over 400 HV, much higher than the 300 HV of the laser cladding structure. After FSP, the friction coefficient decreased from 0.6167 to 0.5645 which promoted the wear resistance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1248639-solute-redistribution-phase-stability-fecr-tio2x-interfaces-under-ion-irradiation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1248639-solute-redistribution-phase-stability-fecr-tio2x-interfaces-under-ion-irradiation"><span>Solute redistribution and phase stability at <span class="hlt">FeCr</span>/TiO 2–x interfaces under ion irradiation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Xu, Y.; Aguiar, J. A.; Yadav, S. K.; ...</p> <p>2015-02-26</p> <p><span class="hlt">Cr</span> diffusion in trilayer thin films of 100 nm Fe–18<span class="hlt">Cr</span>/125 nm TiO 2–x/100 nm Fe–18<span class="hlt">Cr</span> deposited on MgO substrates at 500 °C was studied by either annealing at 500 °C or Ni 3+ ion irradiation at 500 °C. Microchemistry and microstructure evolution at the metal/oxide interfaces were investigated using (high-resolution) transmission electron microscopy, energy-dispersive X-ray spectroscopy and electron energy loss spectroscopy. Diffusion of <span class="hlt">Cr</span> into the O-deficient TiO 2 <span class="hlt">layer</span>, with negligible segregation to the <span class="hlt">FeCr</span>/TiO 2–x interface itself, was observed under both annealing and irradiation. <span class="hlt">Cr</span> diffusion into TiO 2–x was enhanced in ion-irradiated samples as compared to annealed.more » Irradiation-induced voids and amorphization of TiO 2–x was also observed. The experimental results are rationalized using first-principles calculations that suggest an energetic preference for substituting Ti with <span class="hlt">Cr</span> in sub-stoichiometric TiO 2. Furthermore, the implications of these results on the irradiation stability of oxide-dispersed ferritic alloys are discussed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1364301-processability-evaluation-mo-containing-fecral-alloy-seamless-thin-wall-tube-fabrication','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1364301-processability-evaluation-mo-containing-fecral-alloy-seamless-thin-wall-tube-fabrication"><span>Processability evaluation of a Mo-containing <span class="hlt">FeCr</span>Al alloy for seamless thin-wall tube fabrication</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sun, Zhiqian; Yamamoto, Yukinori</p> <p>2017-06-10</p> <p>The processability of a Mo-containing <span class="hlt">FeCr</span>Al alloy (<span class="hlt">Fe</span>-13<span class="hlt">Cr</span>-5.2Al-2Mo base, in wt%), developed for accident-tolerant nuclear fuel claddings, was evaluated through a stepwise rolling process at 400 °C under two different inter-pass annealing conditions (i.e., 650 °C for 1 h and at 870 °C for 30 min). The inter-pass annealing at 870 °C easily softened the <span class="hlt">FeCr</span>Al alloy; however, it led to the formation of coarse grains of ~200 µm. On the other hand, the <span class="hlt">FeCr</span>Al alloy maintained elongated, deformed grains with the inter-pass annealing at 650 °C, but the annealed samples showed relatively high deformation resistance and strong texture. Importantmore » aspects concerning the processability and microstructural control of <span class="hlt">FeCr</span>Al alloys, such as deformation inhomogeneity, texture development, and grain coarsening, were discussed. Optimized processing conditions were recommended, based on the results, to achieve desirable microstructures with balanced processability and mechanical properties.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMEP...26.3071G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMEP...26.3071G"><span>Microstructure and Room-Temperature Mechanical Properties of <span class="hlt">FeCr</span>MoVTi x High-Entropy Alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Jun; Huang, Xuefei; Huang, Weigang</p> <p>2017-07-01</p> <p><span class="hlt">FeCr</span>MoVTi x ( x values represent the molar ratio, where x = 0, 0.5, 1.0, 1.5, and 2.0) high-entropy alloys were prepared by a vacuum arc melting method. The effects of Ti element on the microstructure and room-temperature mechanical properties of the as-cast <span class="hlt">FeCr</span>MoVTi x alloys were investigated. The results show that the prepared alloys exhibited typical dendritic microstructure and the size of the microstructure became fine with increasing Ti content. The <span class="hlt">FeCr</span>MoV alloy exhibited a single body-centered cubic structure (BCC1) and the alloys prepared with Ti element exhibited BCC1 + BCC2 mixed structure. The new BCC2 phase is considered as (<span class="hlt">Fe</span>, Ti)-rich phase and was distributed in the dendrite region. With the increase of Ti content, the volume fraction of the BCC2 phase increased and its shape changed from a long strip to a network. For the <span class="hlt">FeCr</span>MoV alloy, the fracture strength, plastic strain, and hardness reached as high as 2231 MPa, 28.2%, and 720 HV, respectively. The maximum hardness of 887 HV was obtained in the <span class="hlt">FeCr</span>MoVTi alloy. However, the fracture strength, yield stress, and plastic strain of the alloys decreased continuously as Ti content increased. In the room-temperature compressive test, the alloys showed typical brittle fracture characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JOM....67i2047P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JOM....67i2047P"><span>Development of Simultaneous Corrosion Barrier and Optimized Microstructure in <span class="hlt">FeCr</span>Al Heat-Resistant Alloy for Energy Applications. Part 1: The Protective Scale</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pimentel, G.; Aranda, M. M.; Chao, J.; González-Carrasco, J. L.; Capdevila, C.</p> <p>2015-09-01</p> <p>Coarse-grained <span class="hlt">Fe</span>-based oxide dispersion-strengthened (ODS) steels are a class of advanced materials for combined cycle gas turbine systems to deal with operating temperatures and pressures of around 1100°C and 15-30 bar in aggressive environments, which would increase biomass energy conversion efficiencies up to 45% and above. This two-part paper reports the possibility of the development of simultaneous corrosion barrier and optimized microstructure in a <span class="hlt">FeCr</span>Al heat-resistant alloy for energy applications. The first part reports the mechanism of generating a dense, self-healing α-alumina <span class="hlt">layer</span> by thermal oxidation, during a heat treatment that leads to a coarse-grained microstructure with a potential value for high-temperature creep resistance in a <span class="hlt">FeCr</span>Al ODS ferritic alloy, which will be described in more detail in the second part.</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://www.osti.gov/servlets/purl/1379209','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1379209"><span>Low-cost, high-strength <span class="hlt">Fe--Ni--Cr</span> alloys for high temperature exhaust valve application</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Muralidharan, Govindarajan</p> <p>2017-09-05</p> <p>An <span class="hlt">Fe--Ni--Cr</span> alloy is composed essentially of, in terms of wt. %: 2.4 to 3.7 Al, up to 1.05 Co, 14.8 to 15.9 <span class="hlt">Cr</span>, 25 to 36 <span class="hlt">Fe</span>, up to 1.2 Hf, up to 4 Mn, up to 0.6 Mo, up to 2.2 Nb, up to 1.05 Ta, 1.9 to 3.6 Ti, up to 0.08 W, up to 0.03 Zr, 0.18 to 0.27 C, up to 0.0015 N, balance Ni, wherein, in terms of atomic percent: 8.5.ltoreq.Al+Ti+Zr+Hf+Ta.ltoreq.11.5, 0.53.ltoreq.Al/(Al+Ti+Zr+Hf+Ta).ltoreq.0.65, and 0.16.ltoreq.<span class="hlt">Cr/(Fe+Ni+Cr</span>+Mn).ltoreq.0.21, the alloy being essentially free of Cu, Si, and V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22658117-fabrication-core-shell-fe-sub-sub-mil-fe-magnetic-microspheres-removal-cr-vi-aqueous-solution','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22658117-fabrication-core-shell-fe-sub-sub-mil-fe-magnetic-microspheres-removal-cr-vi-aqueous-solution"><span>Fabrication of core-shell <span class="hlt">Fe</span>{sub 3}O{sub 4}@MIL-100(<span class="hlt">Fe</span>) magnetic microspheres for the removal of <span class="hlt">Cr</span>(VI) in aqueous solution</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>Yang, Qingxiang, E-mail: qxyangzz@163.com; Zhao, Qianqian; Ren, ShuangShuang</p> <p></p> <p>Facile regeneration of an adsorbent is very important for commercial feasibility. One typical highly porous metal-organic framework (MOF) materials based on MIL-100(<span class="hlt">Fe</span>) and magnetic iron oxide particles (denoted as MMCs) with diameter about of 350 nm were successfully synthesized. The growth of MIL-100(<span class="hlt">Fe</span>) shell on the surface of <span class="hlt">Fe</span>{sub 3}O{sub 4} was utilized precursor as crystal seed via in-situ step hydrothermal reaction. It is a simple way to obtain well organized core-shell MOF composites, compared to the step-by-step method. MMCs were firstly used to uptake of <span class="hlt">Cr</span>(VI) anions in aqueous solution. Adsorption experiments were carried out in batch sorption mode investigatingmore » with the factors of contact time (0–1000 min), pH (from 2 to 12), dose of adsorbent (4–25 mg), and initial <span class="hlt">Cr</span>(VI) concentration (range from 10 to 100 ppm). - Graphical abstract: One typical highly porous metal-organic framework (MOF) materials based on MIL-100(<span class="hlt">Fe</span>) and magnetic iron oxide particles (denoted as MMCs) were successfully synthesized. Utilizing <span class="hlt">Fe</span>{sub 3}O{sub 4} precursor as crystal seed to grow MIL-100(<span class="hlt">Fe</span>) shell by in-situ step hydrothermal reaction. It is a simple way to obtain core-shell MOF composites. MMCs could effectively uptake of <span class="hlt">Cr</span>(VI) anions in aqueous solution. - Highlights: • <span class="hlt">Fe</span>{sub 3}O{sub 4}@MIL-100(<span class="hlt">Fe</span>) composites with core-shell structure were successfully prepared through a simple method. • The influence factors on <span class="hlt">Cr</span>(VI) adsorption by <span class="hlt">Fe</span>{sub 3}O{sub 4}@MIL-100(<span class="hlt">Fe</span>) were investigated. • <span class="hlt">Cr</span>(VI) can efficiently adsorbed by <span class="hlt">Fe</span>{sub 3}O{sub 4}@MIL-100(<span class="hlt">Fe</span>) composites from aqueous solution.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..253a2008G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..253a2008G"><span>Quality of Metal Deposited Flux Cored Wire With the System <span class="hlt">Fe-C-Si-Mn-Cr</span>-Mo-Ni-V-Co</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gusev, Aleksander I.; Kozyrev, Nikolay A.; Osetkovskiy, Ivan V.; Kryukov, Roman E.; Kozyreva, Olga A.</p> <p>2017-10-01</p> <p>Studied the effect of the introduction of vanadium and cobalt into the charge powder fused wire system <span class="hlt">Fe-C-Si-Mn-Cr</span>-Ni-Mo-V, used in cladding assemblies and equipment parts and mechanisms operating under abrasive and abrasive shock loads. the cored wires samples were manufactured in the laboratory conditions and using appropriate powder materials and as a carbonfluoride contained material were used the dust from gas purification of aluminum production, with the following components composition, %: Al2O3 = 21-46.23; F = 18-27; Na2O = 8-15; K2O = 0.4-6; CaO = 0.7-2.3; Si2O = 0.5-2.48; <span class="hlt">Fe</span>2O3 = 2.1-3.27; C = 12.5-30.2; MnO = 0.07-0.9; MgO = 0.06-0.9; S = 0.09-0.19; P = 0.1-0.18. Surfacing was produced on the St3 metal plates in 6 <span class="hlt">layers</span> under the AN-26C flux by welding truck ASAW-1250. Cutting and preparation of samples for research had been implemented. The chemical composition and the hydrogen content of the weld metal were determined by modern methods. The hardness and abrasion rate of weld metal had been measured. Conducted metallographic studies of weld metal: estimated microstructure, grain size, contamination of oxide non-metallic inclusions. Metallographic studies showed that the microstructure of the surfaced <span class="hlt">layer</span> by cored wire system <span class="hlt">Fe-C-Si-Mn-Cr</span>-Mo-Ni-V-Co is uniform, thin dendrite branches are observed. The microstructure consists of martensite, which is formed inside the borders of the former austenite grain retained austenite present in small amounts in the form of separate islands, and thin <span class="hlt">layers</span> of δ-ferrite, which is located on the borders of the former austenite grains. Carried out an assessment the effect of the chemical composition of the deposited metal on the hardness and wear and hydrogen content. In consequence of multivariate correlation analysis, it was determined dependence to the hardness of the deposited <span class="hlt">layer</span> and the wear resistance of the mass fraction of the elements included in the flux-cored wires of the system <span class="hlt">Fe-C-Si-Mn-Cr</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22486316-highly-tunable-magnetism-silicene-doped-cr-fe-atoms-under-isotropic-uniaxial-tensile-strain','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22486316-highly-tunable-magnetism-silicene-doped-cr-fe-atoms-under-isotropic-uniaxial-tensile-strain"><span>Highly tunable magnetism in silicene doped with <span class="hlt">Cr</span> and <span class="hlt">Fe</span> atoms under isotropic and uniaxial tensile strain</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>Zheng, Rui; Ni, Jun, E-mail: junni@mail.tsinghua.edu.cn; Collaborative Innovative Center of Quantum Matter, Beijing 100084</p> <p>2015-12-28</p> <p>We have investigated the magnetic properties of silicene doped with <span class="hlt">Cr</span> and <span class="hlt">Fe</span> atoms under isotropic and uniaxial tensile strain by the first-principles calculations. We find that <span class="hlt">Cr</span> and <span class="hlt">Fe</span> doped silicenes show strain-tunable magnetism. (1) The magnetism of <span class="hlt">Cr</span> and <span class="hlt">Fe</span> doped silicenes exhibits sharp transitions from low spin states to high spin states by a small isotropic tensile strain. Specially for <span class="hlt">Fe</span> doped silicene, a nearly nonmagnetic state changes to a high magnetic state by a small isotropic tensile strain. (2) The magnetic moments of <span class="hlt">Fe</span> doped silicene also show a sharp jump to ∼2 μ{sub B} at amore » small threshold of the uniaxial strain, and the magnetic moments of <span class="hlt">Cr</span> doped silicene increase gradually to ∼4 μ{sub B} with the increase of uniaxial strain. (3) The electronic and magnetic properties of <span class="hlt">Cr</span> and <span class="hlt">Fe</span> doped silicenes are sensitive to the magnitude and direction of the external strain. The highly tunable magnetism may be applied in the spintronic devices.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800039318&hterms=Atomic+spectroscopy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DAtomic%2Bspectroscopy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800039318&hterms=Atomic+spectroscopy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DAtomic%2Bspectroscopy"><span>Spectroscopy and atomic physics of highly ionized <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, and Ni for tokamak plasmas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Feldman, U.; Doschek, G. A.; Cheng, C.-C.; Bhatia, A. K.</p> <p>1980-01-01</p> <p>The paper considers the spectroscopy and atomic physics for some highly ionized <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, and Ni ions produced in tokamak plasmas. Forbidden and intersystem wavelengths for <span class="hlt">Cr</span> and Ni ions are extrapolated and interpolated using the known wavelengths for <span class="hlt">Fe</span> lines identified in solar-flare plasmas. Tables of transition probabilities for the B I, C I, N I, O I, and F I isoelectronic sequences are presented, and collision strengths and transition probabilities for <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, and Ni ions of the Be I sequence are given. Similarities of tokamak and solar spectra are discussed, and it is shown how the atomic data presented may be used to determine ion abundances and electron densities in low-density plasmas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/863565','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/863565"><span>Amorphous <span class="hlt">silicon</span> Schottky barrier solar cells incorporating a thin insulating <span class="hlt">layer</span> and a thin doped <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Carlson, David E.</p> <p>1980-01-01</p> <p>Amorphous <span class="hlt">silicon</span> Schottky barrier solar cells which incorporate a thin insulating <span class="hlt">layer</span> and a thin doped <span class="hlt">layer</span> adjacent to the junction forming metal <span class="hlt">layer</span> exhibit increased open circuit voltages compared to standard rectifying junction metal devices, i.e., Schottky barrier devices, and rectifying junction metal insulating <span class="hlt">silicon</span> devices, i.e., MIS devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AcSpA.121..544A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AcSpA.121..544A"><span>Synthesis and spectral characterizations of trivalent ions (<span class="hlt">Cr</span>3+, <span class="hlt">Fe</span>3+) doped CdO nanopowders</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aswani, T.; Babu, B.; Pushpa Manjari, V.; Joyce Stella, R.; Thirumala Rao, G.; Rama Krishna, Ch.; Ravikumar, R. V. S. S. N.</p> <p>2014-03-01</p> <p>Trivalent transition metal ions (<span class="hlt">Cr</span>3+, <span class="hlt">Fe</span>3+) doped CdO nanopowders via sonication in the presence of Sodium lauryl sulfate as stabilizing agent were synthesized and characterized. Powder XRD studies indicate that the obtained CdO has a cubic phase and concluded that the trivalent ions doping induced the lattice constants to change some extent. Optical absorption spectra exhibited the characteristic bands of <span class="hlt">Cr</span>3+ and <span class="hlt">Fe</span>3+ ions in octahedral site symmetry. Crystal field (Dq) and inter-electronic repulsion (B and C) parameters are evaluated for <span class="hlt">Cr</span>3+ doped CdO nanopowders as Dq = 1540, B = 619 and C = 3327 cm-1 and for <span class="hlt">Fe</span>3+ doped CdO nanopowders Dq = 920, B = 690, C = 2750 cm-1. EPR spectra of the <span class="hlt">Cr</span>3+ and <span class="hlt">Fe</span>3+ doped CdO nanopowders exhibited resonances at g = 1.973 and g = 2 respectively which indicate distorted octahedral site for both ions with the host. Photoluminescence spectra shows the emission bands in violet and bluish green regions for <span class="hlt">Cr</span>3+ doped CdO, ultraviolet and blue emissions for <span class="hlt">Fe</span>3+ doped CdO nanopowders. The CIE chromaticity coordinates were also evaluated from the emission spectrum. FT-IR spectra indicate the presence of various functional groups of host lattice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1012869-chromium-grain-boundary-segregation-effect-ion-beam-cleaning-fe-ni-cr-alloys','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1012869-chromium-grain-boundary-segregation-effect-ion-beam-cleaning-fe-ni-cr-alloys"><span>Chromium Grain-boundary Segregation and Effect of Ion Beam Cleaning on <span class="hlt">Fe-Ni-Cr</span> Alloys</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>Saraf, Laxmikant V.</p> <p>2011-04-01</p> <p>The grain boundaries play important role to control the mechanical strength of ternary alloys. From spacecrafts to naval vessels to nuclear reactors, stress corrosion cracking, brittleness, oxidation mostly originates at the grain boundaries and cause long term structural stability problems in most of the metallic structures [1]. <span class="hlt">Fe-Ni-Cr</span> based ternary metal alloys have been widely studied for more than fifty years [2, 3]. Despite of vast amount of research, chromium diffusion in stainless steel or other Ni-<span class="hlt">Fe-Cr</span> based ternary alloys is still an open scientific problem with challenges in structural stability and corrosion resistance [4]. Particularly, austenite <span class="hlt">Fe-Ni-Cr</span> is lookedmore » upon favorably in space and jet engine industry for their improved resistance to stress corrosion cracking [5]. In solid oxide fuel cells (SOFC), Ni-alloys are frequently used as interconnects and seals [6]. In this communication, simultaneous energy dispersive spectroscopy (EDS) and electron backscatter diffraction (EBSD) mapping is utilized to study chemical and structural aspects of chromium segregation in <span class="hlt">Fe-Ni-Cr</span> alloy. A focused Ga-ion beam is also utilized to study the effect of ion beam cleaning on EBSD image quality (IQ) and inverse pole figure (IPF) maps of <span class="hlt">Fe-Ni-Cr</span> alloy.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22275627-half-metallicity-tetragonal-distortion-semi-heusler-alloy-fecrse','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22275627-half-metallicity-tetragonal-distortion-semi-heusler-alloy-fecrse"><span>Half-metallicity and tetragonal distortion in semi-Heusler alloy <span class="hlt">FeCr</span>Se</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>Huang, H. M., E-mail: smilehhm@163.com; Luo, S. J.; Yao, K. L.</p> <p>2014-01-28</p> <p>Full-potential linearized augmented plane wave methods are carried out to investigate the electronic structures and magnetic properties in semi-Heusler alloy <span class="hlt">FeCr</span>Se. Results show that <span class="hlt">FeCr</span>Se is half-metallic ferromagnet with the half-metallic gap 0.31 eV at equilibrium lattice constant. Calculated total magnetic moment of 2.00μ{sub B} per formula unit follows the Slater-Pauling rule quite well. Two kinds of structural changes are used to investigate the sensitivity of half-metallicity. It is found that the half-metallicity can be retained when lattice constant is changed by −4.56% to 3.52%, and the results of tetragonal distortion indicate the half-metallicity can be kept at the range ofmore » c/a ratio from 0.85 to 1.20. The Curie temperature, cohesive energy, and heat of formations of <span class="hlt">FeCr</span>Se are also discussed.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.13202006G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.13202006G"><span>Study of optical and luminescence properties of <span class="hlt">silicon</span> — semiconducting silicide — <span class="hlt">silicon</span> multilayer nanostructures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Galkin, N. G.; Galkin, K. N.; Dotsenko, , S. A.; Goroshko, D. L.; Shevlyagin, A. V.; Chusovitin, E. A.; Chernev, I. M.</p> <p>2017-01-01</p> <p>By method of in situ differential spectroscopy it was established that at the formation of monolayer <span class="hlt">Fe</span>, <span class="hlt">Cr</span>, Ca, Mg silicide and Mg stannide islands on the atomically clean <span class="hlt">silicon</span> surface an appearance of loss peaks characteristic for these materials in the energy range of 1.1-2.6 eV is observed. An optimization of growth processes permit to grow monolithic double nanoheterostructures (DNHS) with embedded <span class="hlt">Fe</span>, <span class="hlt">Cr</span> and Ca nanocrystals, and also polycrystalline DNHS with NC of Mg silicide and Mg stannide and Ca disilicide. By methods of optical spectroscopy and Raman spectroscopy it was shown that embedded NC form intensive peaks in the reflectance spectra at energies up to 2.5 eV and Raman peaks. In DNS with β-<span class="hlt">Fe</span>Si2 NC a photoluminescence and electroluminescence at room temperature were firstly observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22584110-new-series-triple-molybdates-aga-sub-moo-sub-sub-mg-cr-fe-mn-al-cr-fe-sc-framework-structures-mobile-silver-ion-sublattices','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22584110-new-series-triple-molybdates-aga-sub-moo-sub-sub-mg-cr-fe-mn-al-cr-fe-sc-framework-structures-mobile-silver-ion-sublattices"><span>New series of triple molybdates AgA{sub 3}R(MoO{sub 4}){sub 5} (A=Mg, R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>; A=Mn, R=Al, <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Sc, In) with framework structures and mobile silver ion sublattices</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>Kotova, Irina Yu.; Buryat State University, Smolin St. 24a, Ulan-Ude 670000, Buryat Republic; Solodovnikov, Sergey F.</p> <p></p> <p>Triple molybdates AgA{sub 3}R(MoO{sub 4}){sub 5} (A=Mg, R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>; A=Mn, R=Al, <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Sc, In) of the NaMg{sub 3}In(MoO{sub 4}){sub 5} type were synthesized and single crystals of AgMg{sub 3}R(MoO{sub 4}){sub 5} (R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>) were grown. In their structures, the MoO{sub 4} tetrahedra, pairs and trimers of edge-shared (Mg, R)O{sub 6} octahedra are connected by common vertices to form a 3D framework. Large framework cavities involve Ag{sup +} cations disordered on three nearby positions with CN=3+1 or 4+1. Alternating (Mg, R)O{sub 6} octahedra and MoO{sub 4} tetrahedra in the framework form quadrangular windows penetrable for Ag{sup +} at elevated temperatures.more » Above 653–673 K, the newly obtained molybdates demonstrate abrupt reduction of the activation energy to 0.4–0.6 eV. At 773 K, AgMg{sub 3}Al(MoO{sub 4}){sub 5} shows electric conductivity 2.5·10{sup −2} S/cm and E{sub a}=0.39 eV compatible with characteristics of the best ionic conductors of the NASICON type. - Graphical abstract: Triple molybdates AgA{sub 3}R(MoO{sub 4}){sub 5} (A=Mg, R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>; A=Mn, R=Al, <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Sc, In) of the NaMg{sub 3}In(MoO{sub 4}){sub 5} type were synthesized, AgMg{sub 3}R(MoO{sub 4}){sub 5} (R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>) were structurally characterized, ion-conductive properties of AgMg{sub 3}Al(MoO{sub 4}){sub 5} were measured. Display Omitted - Highlights: • Triple molybdates AgA{sub 3}R(MoO{sub 4}){sub 5} (A=Mg, R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>; A=Mn, R=Al, <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Sc, In) of the NaMg{sub 3}In(MoO{sub 4}){sub 5} type were synthesized. • Single crystals of AgMg{sub 3}R(MoO{sub 4}){sub 5} (R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>) were grown and their crystal structures were determined. • Disordering Ag{sup +} ions and penetrable framework structures of AgMg{sub 3}R(MoO{sub 4}){sub 5} (R=<span class="hlt">Cr</span>, <span class="hlt">Fe</span>) suggest 2D-character of silver-ion mobility. • Measured ion-conductive properties of AgMg{sub 3}Al(MoO{sub 4}){sub 5} are compatible with characteristics of the best ionic conductors of the NASICON type.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22611613-magnetostrictive-gmr-spin-valves-composite-fega-feco-free-layers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22611613-magnetostrictive-gmr-spin-valves-composite-fega-feco-free-layers"><span>Magnetostrictive GMR spin valves with composite <span class="hlt">FeGa/Fe</span>Co free <span class="hlt">layers</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>Liu, Luping; Institute of Materials Science, School of Materials Science and Engineering, Shanghai University, Shanghai 200072; Zhan, Qingfeng, E-mail: zhanqf@nimte.ac.cn, E-mail: runweili@nimte.ac.cn</p> <p>2016-03-15</p> <p>We have fabricated strain-sensitive spin valves on flexible substrates by utilizing the large magnetostrictive <span class="hlt">Fe</span>Ga alloy to promote the strain sensitivity and the composite free <span class="hlt">layer</span> of <span class="hlt">FeGa/Fe</span>Co to avoid the drastic reduction of giant magnetoresistance (GMR) ratio. This kind of spin valve (SV-<span class="hlt">FeGa/Fe</span>Co) displays a MR ratio about 5.9%, which is comparable to that of the conventional spin valve (SV-<span class="hlt">Fe</span>Co) with a single <span class="hlt">Fe</span>Co free <span class="hlt">layer</span>. Different from the previously reported works on magnetostrictive spin valves, the SV-<span class="hlt">FeGa/Fe</span>Co displays an asymmetric strain dependent GMR behavior. Upon increasing the lateral strain, the MR ratio for the ascending branch decreases moremore » quickly than that for the descending branch, which is ascribed to the formation of a spiraling spin structure around the <span class="hlt">FeGa/Fe</span>Co interface under the combined influences of both magnetic field and mechanical strain. A strain sensitivity of GF = 7.2 was achieved at a magnetic bias field of -30 Oe in flexible SV-<span class="hlt">FeGa/Fe</span>Co, which is significantly larger than that of SV-<span class="hlt">Fe</span>Co.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1340453-mechanisms-radiation-induced-segregation-crfeconi-based-single-phase-concentrated-solid-solution-alloys','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1340453-mechanisms-radiation-induced-segregation-crfeconi-based-single-phase-concentrated-solid-solution-alloys"><span>Mechanisms of radiation-induced segregation in <span class="hlt">CrFe</span>CoNi-based single-phase concentrated solid solution alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>He, Mo-Rigen; Wang, Shuai; Shi, Shi; ...</p> <p>2016-12-31</p> <p>Single-phase concentrated solid solution alloys have attracted wide interest due to their superior mechanical properties and enhanced radiation tolerance, which make them promising candidates for the structural applications in next-generation nuclear reactors. However, little has been understood about the intrinsic stability of their as-synthesized, high-entropy configurations against radiation damage. In this paper, we report the element segregation in <span class="hlt">CrFe</span>CoNi, <span class="hlt">CrFe</span>CoNiMn, and <span class="hlt">CrFe</span>CoNiPd equiatomic alloys when subjected to 1250 kV electron irradiations at 400 °C up to a damage level of 1 displacement per atom. <span class="hlt">Cr/Fe</span>/Mn/Pd can deplete and Co/Ni can accumulate at radiation-induced dislocation loops, while the actively segregating elementsmore » are alloy-specific. Moreover, electron-irradiated matrix of <span class="hlt">CrFe</span>CoNiMn and <span class="hlt">CrFe</span>CoNiPd shows L1 0 (NiMn)-type ordering decomposition and <001>-oriented spinodal decomposition between Co/Ni and Pd, respectively. Finally, these findings are rationalized based on the atomic size difference and enthalpy of mixing between the alloying elements, and identify a new important requirement to the design of radiation-tolerant alloys through modification of the composition.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1407805-dislocation-loop-formation-model-fecral-alloys-after-neutron-irradiation-below-dpa','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1407805-dislocation-loop-formation-model-fecral-alloys-after-neutron-irradiation-below-dpa"><span>Dislocation loop formation in model <span class="hlt">FeCr</span>Al alloys after neutron irradiation below 1 dpa</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Field, Kevin G.; Briggs, Samuel A.; Sridharan, Kumar; ...</p> <p>2017-08-01</p> <p><span class="hlt">FeCr</span>Al alloys with varying compositions and microstructures are under consideration for accident-tolerant fuel cladding, but limited details exist on dislocation loop formation and growth for this class of alloys under neutron irradiation. Four model <span class="hlt">FeCr</span>Al alloys with chromium contents ranging from 10.01 to 17.51 wt % and alunimum contents of 4.78 to 2.93 wt % were neutron irradiated to doses of 0.3–0.8 displacements per atom (dpa) at temperatures of 335–355°C. On-zone STEM imaging revealed a mixed population of black dots and larger dislocation loops with either a/2< 111 > or a< 100 > Burgers vectors. Weak composition dependencies were observedmore » and varied depending on whether the defect size, number density, or ratio of defect types was of interest. Here, the results were found to mirror those of previous studies on <span class="hlt">FeCr</span>Al and <span class="hlt">FeCr</span> alloys irradiated under similar conditions, although distinct differences exist.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JNuM..495...20F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JNuM..495...20F"><span>Dislocation loop formation in model <span class="hlt">FeCr</span>Al alloys after neutron irradiation below 1 dpa</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, Kevin G.; Briggs, Samuel A.; Sridharan, Kumar; Yamamoto, Yukinori; Howard, Richard H.</p> <p>2017-11-01</p> <p><span class="hlt">FeCr</span>Al alloys with varying compositions and microstructures are under consideration for accident-tolerant fuel cladding, but limited details exist on dislocation loop formation and growth for this class of alloys under neutron irradiation. Four model <span class="hlt">FeCr</span>Al alloys with chromium contents ranging from 10.01 to 17.51 wt % and aluminum contents of 4.78 to 2.93 wt % were neutron irradiated to doses of 0.3-0.8 displacements per atom (dpa) at temperatures of 335-355 °C. On-zone STEM imaging revealed a mixed population of black dots and larger dislocation loops with either a / 2 〈 111 〉 or a 〈 100 〉 Burgers vectors. Weak composition dependencies were observed and varied depending on whether the defect size, number density, or ratio of defect types was of interest. Results were found to mirror those of previous studies on <span class="hlt">FeCr</span>Al and <span class="hlt">FeCr</span> alloys irradiated under similar conditions, although distinct differences exist.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29624046','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29624046"><span>Chromium Trioxide Hole-Selective Heterocontacts for <span class="hlt">Silicon</span> Solar Cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lin, Wenjie; Wu, Weiliang; Liu, Zongtao; Qiu, Kaifu; Cai, Lun; Yao, Zhirong; Ai, Bin; Liang, Zongcun; Shen, Hui</p> <p>2018-04-25</p> <p>A high recombination rate and high thermal budget for aluminum (Al) back surface field are found in the industrial p-type <span class="hlt">silicon</span> solar cells. Direct metallization on lightly doped p-type <span class="hlt">silicon</span>, however, exhibits a large Schottky barrier for the holes on the <span class="hlt">silicon</span> surface because of Fermi-level pinning effect. As a result, low-temperature-deposited, dopant-free chromium trioxide (<span class="hlt">Cr</span>O x , x < 3) with high stability and high performance is first applied in a p-type <span class="hlt">silicon</span> solar cell as a hole-selective contact at the rear surface. By using 4 nm <span class="hlt">Cr</span>O x between the p-type <span class="hlt">silicon</span> and Ag, we achieve a reduction of the contact resistivity for the contact of Ag directly on p-type <span class="hlt">silicon</span>. For further improvement, we utilize a <span class="hlt">Cr</span>O x (2 nm)/Ag (30 nm)/<span class="hlt">Cr</span>O x (2 nm) multilayer film on the contact between Ag and p-type crystalline <span class="hlt">silicon</span> (c-Si) to achieve a lower contact resistance (40 mΩ·cm 2 ). The low-resistivity Ohmic contact is attributed to the high work function of the uniform <span class="hlt">Cr</span>O x film and the depinning of the Fermi level of the SiO x <span class="hlt">layer</span> at the <span class="hlt">silicon</span> interface. Implementing the advanced hole-selective contacts with <span class="hlt">Cr</span>O x /Ag/<span class="hlt">Cr</span>O x on the p-type <span class="hlt">silicon</span> solar cell results in a power conversion efficiency of 20.3%, which is 0.1% higher than that of the cell utilizing 4 nm <span class="hlt">Cr</span>O x . Compared with the commercialized p-type solar cell, the novel <span class="hlt">Cr</span>O x -based hole-selective transport material opens up a new possibility for c-Si solar cells using high-efficiency, low-temperature, and dopant-free deposition techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhSS...59.2211H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhSS...59.2211H"><span>Spectral ellipsometry as a method for characterization of nanosized films with ferromagnetic <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hashim, H.; Singkh, S. P.; Panina, L. V.; Pudonin, F. A.; Sherstnev, I. A.; Podgornaya, S. V.; Shpetnyi, I. A.; Beklemisheva, A. V.</p> <p>2017-11-01</p> <p>Nanosized films with ferromagnetic <span class="hlt">layers</span> are widely used in nanoelectronics, sensor systems and telecommunications. Their properties may strongly differ from those of bulk materials that is on account of interfaces, intermediate <span class="hlt">layers</span> and diffusion. In the present work, spectral ellipsometry and magnetooptical methods are adapted for characterization of the optical parameters and magnetization processes in two- and three-<span class="hlt">layer</span> <span class="hlt">Cr/NiFe</span>, Al/Ni<span class="hlt">Fe</span> and <span class="hlt">Cr(Al)/Ge/NiFe</span> films onto a sitall substrate for various thicknesses of <span class="hlt">Cr</span> and Al <span class="hlt">layers</span>. At a <span class="hlt">layer</span> thickness below 20 nm, the complex refractive coefficients depend pronouncedly on the thickness. In two-<span class="hlt">layer</span> films, remagnetization changes weakly over a thickness of the top <span class="hlt">layer</span>, but the coercive force in three-<span class="hlt">layer</span> films increases by more than twice upon remagnetization, while increasing the top <span class="hlt">layer</span> thickness from 4 to 20 nm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1427657-effects-laves-phase-particles-recovery-recrystallization-behaviors-nb-containing-fecral-alloys','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1427657-effects-laves-phase-particles-recovery-recrystallization-behaviors-nb-containing-fecral-alloys"><span>Effects of Laves phase particles on recovery and recrystallization behaviors of Nb-containing <span class="hlt">FeCr</span>Al alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sun, Zhiqian; Edmondson, Philip D.; Yamamoto, Yukinori</p> <p>2017-11-15</p> <p>The microstructures and mechanical properties of deformed and annealed Nb-containing <span class="hlt">FeCr</span>Al alloys were investigated. Fine dispersion of <span class="hlt">Fe</span> 2Nb-type Laves phase particles was observed in the bcc-<span class="hlt">Fe</span> matrix after applying a thermomechanical treatment, especially along grain/subgrain boundaries, which effectively stabilized the recovered and recrystallized microstructures compared with the Nb-free <span class="hlt">FeCr</span>Al alloy. The stability of recovered areas increased with Nb content up to 1 wt%. The recrystallized grain structure in Nb-containing <span class="hlt">FeCr</span>Al alloys consisted of elongated grains along the rolling direction with a weak texture when annealed below 1100 °C. An abnormal relationship between recrystallized grain size and annealing temperature wasmore » found. Microstructural inhomogeneity in the deformed and annealed states was explained based on the Taylor factor. Annealed Nb-containing <span class="hlt">FeCr</span>Al alloys showed a good combination of strength and ductility, which is desirable for their application as fuel cladding in light-water reactors.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1185657-development-ods-fecral-compatibility-fusion-fission-energy-applications','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1185657-development-ods-fecral-compatibility-fusion-fission-energy-applications"><span>Development of ODS <span class="hlt">FeCr</span>Al for compatibility in fusion and fission energy applications</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Pint, Bruce A.; Dryepondt, Sebastien N.; Unocic, Kinga A.; ...</p> <p>2014-11-15</p> <p>In this paper, oxide dispersion strengthened (ODS) <span class="hlt">FeCr</span>Al alloys with 12–15% <span class="hlt">Cr</span> are being evaluated for improved compatibility with Pb-Li for a fusion energy application and with high temperature steam for a more accident-tolerant light water reactor fuel cladding application. A 12% <span class="hlt">Cr</span> content alloy showed low mass losses in static Pb-Li at 700°C, where a LiAlO 2 surface oxide formed and inhibited dissolution into the liquid metal. All the evaluated compositions formed a protective scale in steam at 1200°C, which is not possible with ODS <span class="hlt">FeCr</span> alloys. However, most of the compositions were not protective at 1400°C, which ismore » a general and somewhat surprising problem with ODS <span class="hlt">FeCr</span>Al alloys that is still being studied. More work is needed to optimize the alloy composition, microstructure and oxide dispersion, but initial promising tensile and creep results have been obtained with mixed oxide additions, i.e. Y 2O 3 with ZrO 2, HfO 2 or TiO 2.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAP...121h5306D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAP...121h5306D"><span>Passivation mechanism in <span class="hlt">silicon</span> heterojunction solar cells with intrinsic hydrogenated amorphous <span class="hlt">silicon</span> oxide <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Deligiannis, Dimitrios; van Vliet, Jeroen; Vasudevan, Ravi; van Swaaij, René A. C. M. M.; Zeman, Miro</p> <p>2017-02-01</p> <p>In this work, we use intrinsic hydrogenated amorphous <span class="hlt">silicon</span> oxide <span class="hlt">layers</span> (a-SiOx:H) with varying oxygen content (cO) but similar hydrogen content to passivate the crystalline <span class="hlt">silicon</span> wafers. Using our deposition conditions, we obtain an effective lifetime (τeff) above 5 ms for cO ≤ 6 at. % for passivation <span class="hlt">layers</span> with a thickness of 36 ± 2 nm. We subsequently reduce the thickness of the <span class="hlt">layers</span> using an accurate wet etching method to ˜7 nm and deposit p- and n-type doped <span class="hlt">layers</span> fabricating a device structure. After the deposition of the doped <span class="hlt">layers</span>, τeff appears to be predominantly determined by the doped <span class="hlt">layers</span> themselves and is less dependent on the cO of the a-SiOx:H <span class="hlt">layers</span>. The results suggest that τeff is determined by the field-effect rather than by chemical passivation.</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://www.osti.gov/biblio/5998249-structural-classification-rao-sub-mo-sub-compounds-sc-lanthanides-fe-iii-ga-cr-al-divalent-cation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5998249-structural-classification-rao-sub-mo-sub-compounds-sc-lanthanides-fe-iii-ga-cr-al-divalent-cation"><span>Structural classification of RAO/sub 3/(MO)/sub n/ compounds (R = Sc, In, Y, or lanthanides; A = <span class="hlt">Fe</span>(III), Ga, <span class="hlt">Cr</span>, or Al; M = divalent cation; n = 1-11)</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>Kimizuka, N.; Mohri, T.</p> <p></p> <p>A series of new compounds (RAO/sub 3/MO)/sub n/ (n = 1-11) having spinel, Yb<span class="hlt">Fe</span>/sub 2/O/sub 4/, or In<span class="hlt">Fe</span>O/sub 3/(ZnO)/sub n/ types of structures were newly synthesized (R = Sc, In, Y, Lu, Yb, Tm, or Er; A = <span class="hlt">Fe</span>(III), Ga, <span class="hlt">Cr</span>, or Al; M = Mg, Mn, <span class="hlt">Fe</span>(II), Co, Ni, Zn, or Cd) at elevated temperatures. The conditions of synthesis and the lattice constants for these compounds are reported. The stacking sequences of the InO/sub 1.5/, (<span class="hlt">Fe</span>Zn)O/sub 2.5/, and ZnO <span class="hlt">layers</span> for In<span class="hlt">Fe</span>O/sub 3/(ZnO)/sub 10/ and the TmO/sub 1.5/, (AlZn)O/sub 2.5/, and ZnO <span class="hlt">layers</span> for TmAlO/sub 3/(ZnO)/sub 11/ are presented,more » respectively. The crystal structures of the (RAO/sub 3/)/sub m/(MO)/sub n/ phases R = Sc, In, Y, or lanthanide elements; A = <span class="hlt">Fe</span>(III), Ga, <span class="hlt">Cr</span>, or Al; M = divalent cation elements; m and n = integer are classified into four crystal structure types (K/sub 2/NiF/sub 4/, Ca<span class="hlt">Fe</span>/sub 2/O/sub 4/, Yb<span class="hlt">Fe</span>/sub 2/O/sub 4/, and spinel), based upon the constituent cations R, A, and M.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1248881','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1248881"><span>Nanostructured <span class="hlt">Fe-Cr</span> Alloys for Advanced Nuclear Energy Applications</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>Scattergood, Ronald O.</p> <p>2016-04-26</p> <p>We have completed research on the grain-size stabilization of model nanostructured <span class="hlt">Fe</span>14<span class="hlt">Cr</span> base alloys at high temperatures by the addition of non-equilibrium solutes. <span class="hlt">Fe</span>14<span class="hlt">Cr</span> base alloys are representative for nuclear reactor applications. The neutron flux in a nuclear reactor will generate He atoms that coalesce to form He bubbles. These can lead to premature failure of the reactor components, limiting their lifetime and increasing the cost and capacity for power generation. In order to mitigate such failures, <span class="hlt">Fe</span>14<span class="hlt">Cr</span> base alloys have been processed to contain very small nano-size oxide particles (less than 10 nm in size) that trap He atomsmore » and reduce bubble formation. Theoretical and experimental results indicate that the grain boundaries can also be very effective traps for He atoms and bubble formation. An optimum grain size will be less than 100 nm, ie., nanocrystalline alloys must be used. Powder metallurgy methods based on high-energy ball milling can produce <span class="hlt">Fe-Cr</span> base nanocrystalline alloys that are suitable for nuclear energy applications. The problem with nanocrystalline alloys is that excess grain-boundary energy will cause grains to grow at higher temperatures and their propensity for He trapping will be lost. The nano-size oxide particles in current generation nuclear alloys provide some grain size stabilization by reducing grain-boundary mobility (Zener pinning – a kinetic effect). However the current mitigation strategy minimizing bubble formation is based primarily on He trapping by nano-size oxide particles. An alternate approach to nanoscale grain size stabilization has been proposed. This is based on the addition of small amounts of atoms that are large compared to the base alloy. At higher temperatures these will diffuse to the grain boundaries and will produce an equilibrium state for the grain size at higher temperatures (thermodynamic stabilization – an equilibrium effect). This would be preferred compared to a kinetic effect</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JPhCS.660a2124P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JPhCS.660a2124P"><span><span class="hlt">Silicon</span> MEMS bistable electromagnetic vibration energy harvester using double-<span class="hlt">layer</span> micro-coils</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Podder, P.; Constantinou, P.; Mallick, D.; Roy, S.</p> <p>2015-12-01</p> <p>This work reports the development of a MEMS bistable electromagnetic vibrational energy harvester (EMVEH) consisting of a <span class="hlt">silicon</span>-on-insulator (SOI) spiral spring, double <span class="hlt">layer</span> micro-coils and miniaturized Nd<span class="hlt">Fe</span>B magnets. Furthermore, with respect to the spiral <span class="hlt">silicon</span> spring based VEH, four different square micro-coil topologies with different copper track width and number of turns have been investigated to determine the optimal coil dimensions. The micro-generator with the optimal micro-coil generated 0.68 micro-watt load power over an optimum resistive load at 0.1g acceleration, leading to normalized power density of 3.5 kg.s/m3. At higher accelerations the load power increased, and the vibrating magnet collides with the planar micro-coil producing wider bandwidth. Simulation results show that a substantially wider bandwidth could be achieved in the same device by introducing bistable nonlinearity through a repulsive configuration between the moving and fixed permanent magnets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24370387','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24370387"><span>Effects of environment on the release of Ni, <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, and Co from new and recast Ni-<span class="hlt">Cr</span> alloy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Oyar, Perihan; Can, Gülşen; Atakol, Orhan</p> <p>2014-07-01</p> <p>The addition of previously cast alloy to new alloy for economic reasons may increase the release of elements. The purpose of this study was to analyze the effects of the immersion period, immersion media, and addition of previously cast alloy to new alloy on the release of elements. Disk-shaped specimens were prepared from a Ni-<span class="hlt">Cr</span> alloy (Ni: 61 wt%, <span class="hlt">Cr</span>: 26 wt%, Mo: 11 wt%, Si: 1.5 wt%, <span class="hlt">Fe</span>, Ce, Al, and Co <1 wt%) (Remanium CS; Dentaurum) with new alloy (group N) and 50% new/50% recast alloy (group R). After the immersion of the specimens in both NaCl (pH 4) and artificial saliva (pH 6.7) for 3, 7, 14, 30, and 60 days, the release of ions was determined by using atomic absorption spectrometry. Data were analyzed with a 3-way ANOVA (α=.001). The release of Ni was significantly affected by the immersion period, of Ni and <span class="hlt">Cr</span> by the alloy and media (P<.01), and of <span class="hlt">Fe</span> by the alloy (P<.01). Ion release from the recast alloy in artificial saliva was 109.71 for Ni, 6.49 for <span class="hlt">Cr</span>, 223.22 for <span class="hlt">Fe</span>, and 29.90 μg/L for Co. The release of Co in NaCl was below the detection limit in both groups. The release of Ni in NaCl and artificial saliva increased with the length of the immersion period in both groups. The release of <span class="hlt">Cr</span> and <span class="hlt">Fe</span> was higher in artificial saliva than in NaCl in group R, regardless of the immersion period. The release of Co in NaCl was below the detection limit in both groups. Copyright © 2014 The Editorial Council for the Journal of Prosthetic Dentistry. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22597776-magnetic-cluster-expansion-model-random-ordered-magnetic-face-centered-cubic-fe-ni-cr-alloys','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22597776-magnetic-cluster-expansion-model-random-ordered-magnetic-face-centered-cubic-fe-ni-cr-alloys"><span>Magnetic cluster expansion model for random and ordered magnetic face-centered cubic <span class="hlt">Fe-Ni-Cr</span> alloys</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>Lavrentiev, M. Yu., E-mail: Mikhail.Lavrentiev@ukaea.uk; Nguyen-Manh, D.; Dudarev, S. L.</p> <p></p> <p>A Magnetic Cluster Expansion model for ternary face-centered cubic <span class="hlt">Fe-Ni-Cr</span> alloys has been developed, using DFT data spanning binary and ternary alloy configurations. Using this Magnetic Cluster Expansion model Hamiltonian, we perform Monte Carlo simulations and explore magnetic structures of alloys over the entire range of compositions, considering both random and ordered alloy structures. In random alloys, the removal of magnetic collinearity constraint reduces the total magnetic moment but does not affect the predicted range of compositions where the alloys adopt low-temperature ferromagnetic configurations. During alloying of ordered fcc <span class="hlt">Fe</span>-Ni compounds with <span class="hlt">Cr</span>, chromium atoms tend to replace nickel rathermore » than iron atoms. Replacement of Ni by <span class="hlt">Cr</span> in ordered alloys with high iron content increases the Curie temperature of the alloys. This can be explained by strong antiferromagnetic <span class="hlt">Fe-Cr</span> coupling, similar to that found in bcc <span class="hlt">Fe-Cr</span> solutions, where the Curie temperature increase, predicted by simulations as a function of <span class="hlt">Cr</span> concentration, is confirmed by experimental observations. In random alloys, both magnetization and the Curie temperature decrease abruptly with increasing chromium content, in agreement with experiment.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JNuM..498..137Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JNuM..498..137Z"><span>Response of <span class="hlt">Cr</span> and <span class="hlt">Cr</span>-Al coatings on Zircaloy-2 to high temperature steam</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhong, Weicheng; Mouche, Peter A.; Heuser, Brent J.</p> <p>2018-01-01</p> <p>The oxidation behavior of chromium (<span class="hlt">Cr</span>) and chromium-aluminum (<span class="hlt">Cr</span>Al) coatings with various compositions deposited on Zircaloy-2 to 700 °C high-temperature steam (HTS) exposure has been investigated. <span class="hlt">Cr</span>Al coatings with higher Al compositions demonstrate lower oxidation weight gain. A <span class="hlt">layer</span> of γ-alumina developed on the <span class="hlt">Cr</span>Al coatings with Al composition over 43 at%, while Al2O3 and <span class="hlt">Cr</span>2O3 developed on <span class="hlt">Cr</span>Al coatings with Al composition below 33 at%. Oxidation of Zircaloy-2 substrate was inhibited by the 1um coatings to 20 h HTS exposure. Coating constituent elements diffused into the substrate and formed intermetallic phases with the Zircaloy substrate. Thicker <span class="hlt">layers</span> of intermetallic phases developed on the coatings with higher Al composition. The intermetallic phases included <span class="hlt">Fe</span> and Ni, indicating the dissolution of second phase particles (SPPs) during HTS exposure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e6501D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e6501D"><span>Improvement of perpendicular anisotropy of columnar <span class="hlt">Fe</span>Pt-ZrO2-C films with <span class="hlt">Fe</span>Pt insert <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dong, Kaifeng; Mo, Wenqin; Jin, Fang; Song, Junlei; Cheng, Weimin; Wang, Haiwei</p> <p>2018-05-01</p> <p>The effects of various thicknesses of <span class="hlt">Fe</span>Pt insert <span class="hlt">layer</span> on the microstructure and magnetic properties of <span class="hlt">Fe</span>Pt-ZrO2-C thin films have been investigated. It is found that with inserting 0.4 nm <span class="hlt">Fe</span>Pt films between the TiON intermediate <span class="hlt">layer</span> and <span class="hlt">Fe</span>Pt-ZrO2-C <span class="hlt">layer</span>, the perpendicular anisotropy indicated by Hc⊥/Hc//ratio would increase from 4 to 13.1, suggesting the perpendicular anisotropy could be improved a lot with using <span class="hlt">Fe</span>Pt insert <span class="hlt">layer</span>. Simultaneously, the <span class="hlt">Fe</span>Pt grains of <span class="hlt">Fe</span>Pt-ZrO2-C thin films maintained columnar structure and the grain isolation could also be improved in a certain degree. With further increase of the <span class="hlt">Fe</span>Pt insert <span class="hlt">layer</span> thickness, although the perpendicular anisotropy was still larger than that without <span class="hlt">Fe</span>Pt insert <span class="hlt">layer</span>, the grain size of the <span class="hlt">Fe</span>Pt-ZrO2-C films would increase and the isolation would be deteriorated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1190745-computational-discovery-ferromagnetic-semiconducting-single-layer-crsnte3','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1190745-computational-discovery-ferromagnetic-semiconducting-single-layer-crsnte3"><span>Computational discovery of ferromagnetic semiconducting single-<span class="hlt">layer</span> <span class="hlt">Cr</span>SnTe 3</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zhuang, Houlong L.; Xie, Yu; Kent, P. R. C.; ...</p> <p>2015-07-06</p> <p>Despite many single-<span class="hlt">layer</span> materials being reported in the past decade, few of them exhibit magnetism. Here we perform first-principles calculations using accurate hybrid density functional methods (HSE06) to predict that single-<span class="hlt">layer</span> <span class="hlt">Cr</span>SnTe 3 (CST) is a ferromagnetic semiconductor, with band gaps of 0.9 and 1.2 eV for the majority and minority spin channels, respectively. We determine the Curie temperature as 170 K, significantly higher than that of single-<span class="hlt">layer</span> <span class="hlt">Cr</span>SiTe 3 (90K) and <span class="hlt">Cr</span>GeTe 3 (130 K). This is due to the enhanced ionicity of the Sn-Te bond, which in turn increases the superexchange coupling between the magnetic <span class="hlt">Cr</span> atoms. Wemore » further explore the mechanical and dynamical stability and strain response of this single-<span class="hlt">layer</span> material for possible epitaxial growth. Lastly, our study provides an intuitive approach to understand and design novel single-<span class="hlt">layer</span> magnetic semiconductors for a wide range of spintronics and energy applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..202a2037A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..202a2037A"><span>Optimizing Heat Treatment Process of <span class="hlt">Fe</span>-13<span class="hlt">Cr</span>-3Mo-3Ni Martensitic Stainless of Steel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anwar, M. S.; Prifiharni, S.; Mabruri, E.</p> <p>2017-05-01</p> <p>The <span class="hlt">Fe</span>-13<span class="hlt">Cr</span>-3Mo-3Ni stainless steels are modified into martensitic stainless steels for steam turbine blades application. The working temperature of steam turbine was around 600 - 700 °C. The improvement properties of turbine blade material is necessary to maintain steam turbine work. The previous research revealed that it has corrosion resistance of <span class="hlt">Fe</span>-13<span class="hlt">Cr</span>-3Mo-3Ni which is better than 13<span class="hlt">Cr</span> stainless steels in the chloride environment. In this work, the effect of heat treatment on microstructure and hardness of <span class="hlt">Fe</span>-13<span class="hlt">Cr</span>-3Mo-3Ni stainless steels has been studied. The steel was prepared by induction melting followed by hot forging. The steels were austenitized at 1000, 1050, and 1100 °C for 1 hour and were tempered at 600, 650, and 700 °C for 1 hour. The steels were then subjected to metallographic observation and hardness test of Rockwell C. The optimal heat treatment of <span class="hlt">Fe</span>-13<span class="hlt">Cr</span>-3Mo-3Ni was carried out austenitized in 1050 °C and tempered in 600 - 700 °C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080004666','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080004666"><span><span class="hlt">Silicon</span> based substrate with calcium aluminosilicate/thermal barrier <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Eaton, Jr., Harry Edwin (Inventor); Allen, William Patrick (Inventor); Miller, Robert Alden (Inventor); Jacobson, Nathan S. (Inventor); Smialek, James L. (Inventor); Opila, Elizabeth J. (Inventor); Lee, Kang N. (Inventor); Nagaraj, Bangalore A. (Inventor); Wang, Hongyu (Inventor); Meschter, Peter Joel (Inventor)</p> <p>2001-01-01</p> <p>A barrier <span class="hlt">layer</span> for a <span class="hlt">silicon</span> containing substrate which inhibits the formation of gaseous species of <span class="hlt">silicon</span> when exposed to a high temperature aqueous environment comprises a calcium alumino silicate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3499143','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3499143"><span>Phosphorus diffusion gettering process of multicrystalline <span class="hlt">silicon</span> using a sacrificial porous <span class="hlt">silicon</span> <span class="hlt">layer</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></p> <p>2012-01-01</p> <p>The aims of this work are to getter undesirable impurities from low-cost multicrystalline <span class="hlt">silicon</span> (mc-Si) wafers and then enhance their electronic properties. We used an efficient process which consists of applying phosphorus diffusion into a sacrificial porous <span class="hlt">silicon</span> (PS) <span class="hlt">layer</span> in which the gettered impurities have been trapped after the heat treatment. As we have expected, after removing the phosphorus-rich PS <span class="hlt">layer</span>, the electrical properties of the mc-Si wafers were significantly improved. The PS <span class="hlt">layers</span>, realized on both sides of the mc-Si substrates, were formed by the stain-etching technique. The phosphorus treatment was achieved using a liquid POCl3-based source on both sides of the mc-Si wafers. The realized phosphorus/PS/Si/PS/phosphorus structures were annealed at a temperature ranging between 700°C and 950°C under a controlled O2 atmosphere, which allows phosphorus to diffuse throughout the PS <span class="hlt">layers</span> and to getter eventual metal impurities towards the phosphorus-doped PS <span class="hlt">layer</span>. The effect of this gettering procedure was investigated by means of internal quantum efficiency and the dark current–voltage (I-V) characteristics. The minority carrier lifetime measurements were made using a WTC-120 photoconductance lifetime tester. The serial resistance and the shunt resistance carried out from the dark I-V curves confirm this gettering-related solar cell improvement. It has been shown that the photovoltaic parameters of the gettered <span class="hlt">silicon</span> solar cells were improved with regard to the ungettered one, which proves the beneficial effect of this gettering process on the conversion efficiency of the multicrystalline <span class="hlt">silicon</span> solar cells. PMID:22846070</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26632759','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26632759"><span>Aluminium alloyed iron-silicide/<span class="hlt">silicon</span> solar cells: A simple approach for low cost environmental-friendly photovoltaic technology.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kumar Dalapati, Goutam; Masudy-Panah, Saeid; Kumar, Avishek; Cheh Tan, Cheng; Ru Tan, Hui; Chi, Dongzhi</p> <p>2015-12-03</p> <p>This work demonstrates the fabrication of silicide/<span class="hlt">silicon</span> based solar cell towards the development of low cost and environmental friendly photovoltaic technology. A heterostructure solar cells using metallic alpha phase (α-phase) aluminum alloyed iron silicide (<span class="hlt">Fe</span>Si(Al)) on n-type <span class="hlt">silicon</span> is fabricated with an efficiency of 0.8%. The fabricated device has an open circuit voltage and fill-factor of 240 mV and 60%, respectively. Performance of the device was improved by about 7 fold to 5.1% through the interface engineering. The α-phase <span class="hlt">FeSi(Al)/silicon</span> solar cell devices have promising photovoltaic characteristic with an open circuit voltage, short-circuit current and a fill factor (FF) of 425 mV, 18.5 mA/cm(2), and 64%, respectively. The significant improvement of α-phase <span class="hlt">Fe</span>Si(Al)/n-Si solar cells is due to the formation p(+-)n homojunction through the formation of re-grown crystalline <span class="hlt">silicon</span> <span class="hlt">layer</span> (~5-10 nm) at the silicide/<span class="hlt">silicon</span> interface. Thickness of the regrown <span class="hlt">silicon</span> <span class="hlt">layer</span> is crucial for the silicide/<span class="hlt">silicon</span> based photovoltaic devices. Performance of the α-<span class="hlt">Fe</span>Si(Al)/n-Si solar cells significantly depends on the thickness of α-<span class="hlt">Fe</span>Si(Al) <span class="hlt">layer</span> and process temperature during the device fabrication. This study will open up new opportunities for the Si based photovoltaic technology using a simple, sustainable, and los cost method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMOp...65....1W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMOp...65....1W"><span>Broadband wavelength conversion in hydrogenated amorphous <span class="hlt">silicon</span> waveguide with <span class="hlt">silicon</span> nitride <span class="hlt">layer</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, Jiang; Li, Yongfang; Wang, Zhaolu; Han, Jing; Huang, Nan; Liu, Hongjun</p> <p>2018-01-01</p> <p>Broadband wavelength conversion based on degenerate four-wave mixing is theoretically investigated in a hydrogenated amorphous <span class="hlt">silicon</span> (a-Si:H) waveguide with <span class="hlt">silicon</span> nitride inter-cladding <span class="hlt">layer</span> (a-Si:HN). We have found that enhancement of the non-linear effect of a-Si:H waveguide nitride intermediate <span class="hlt">layer</span> facilitates broadband wavelength conversion. Conversion bandwidth of 490 nm and conversion efficiency of 11.4 dB were achieved in a numerical simulation of a 4 mm-long a-Si:HN waveguide under 1.55 μm continuous wave pumping. This broadband continuous-wave wavelength converter has potential applications in photonic networks, a type of readily manufactured low-cost highly integrated optical circuits.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20702514-quantitative-determination-clustered-silicon-concentration-substoichiometric-silicon-oxide-layer','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20702514-quantitative-determination-clustered-silicon-concentration-substoichiometric-silicon-oxide-layer"><span>Quantitative determination of the clustered <span class="hlt">silicon</span> concentration in substoichiometric <span class="hlt">silicon</span> oxide <span class="hlt">layer</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>Spinella, Corrado; Bongiorno, Corrado; Nicotra, Giuseppe</p> <p>2005-07-25</p> <p>We present an analytical methodology, based on electron energy loss spectroscopy (EELS) and energy-filtered transmission electron microscopy, which allows us to quantify the clustered <span class="hlt">silicon</span> concentration in annealed substoichiometric <span class="hlt">silicon</span> oxide <span class="hlt">layers</span>, deposited by plasma-enhanced chemical vapor deposition. The clustered Si volume fraction was deduced from a fit to the experimental EELS spectrum using a theoretical description proposed to calculate the dielectric function of a system of spherical particles of equal radii, located at random in a host material. The methodology allowed us to demonstrate that the clustered Si concentration is only one half of the excess Si concentration dissolvedmore » in the <span class="hlt">layer</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1237610','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1237610"><span>Fuel Performance Calculations for <span class="hlt">FeCr</span>Al Cladding in BWRs</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>George, Nathan; Sweet, Ryan; Maldonado, G. Ivan</p> <p>2015-01-01</p> <p>This study expands upon previous neutronics analyses of the reactivity impact of alternate cladding concepts in boiling water reactor (BWR) cores and directs focus toward contrasting fuel performance characteristics of <span class="hlt">FeCr</span>Al cladding against those of traditional Zircaloy. Using neutronics results from a modern version of the 3D nodal simulator NESTLE, linear power histories were generated and supplied to the BISON-CASL code for fuel performance evaluations. BISON-CASL (formerly Peregrine) expands on material libraries implemented in the BISON fuel performance code and the MOOSE framework by providing proprietary material data. By creating material libraries for Zircaloy and <span class="hlt">FeCr</span>Al cladding, the thermomechanical behaviormore » of the fuel rod (e.g., strains, centerline fuel temperature, and time to gap closure) were investigated and contrasted.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e6412N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e6412N"><span>Room-temperature ferromagnetic transitions and the temperature dependence of magnetic behaviors in <span class="hlt">FeCoNiCr</span>-based high-entropy alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Na, Suok-Min; Yoo, Jin-Hyeong; Lambert, Paul K.; Jones, Nicholas J.</p> <p>2018-05-01</p> <p>High-entropy alloys (HEAs) containing multiple principle alloying elements exhibit unique properties so they are currently receiving great attention for developing innovative alloy designs. In <span class="hlt">Fe</span>CoNi-based HEAs, magnetic behaviors strongly depend on the addition of alloying elements, usually accompanied by structural changes. In this work, the effect of non-magnetic components on the ferromagnetic transition and magnetic behaviors in equiatomic <span class="hlt">FeCoNiCr</span>X (X=Al, Ga, Mn and Sn) HEAs was investigated. Alloy ingots of nominal compositions of HEAs were prepared by arc melting and the button ingots were cut into discs for magnetic measurements as functions of magnetic field and temperature. The HEAs of <span class="hlt">FeCoNiCr</span>Mn and <span class="hlt">FeCoNiCr</span>Sn show typical paramagnetic behaviors, composed of solid solution FCC matrix, while the additions of Ga and Al in <span class="hlt">FeCoNiCr</span> exhibit ferromagnetic behaviors, along with the coexistence of FCC and BCC phases due to spinodal decomposition. The partial phase transition in both HEAs with the additions of Ga and Al would enhance ferromagnetic properties due to the addition of the BCC phase. The saturation magnetization for the base alloy <span class="hlt">FeCoNiCr</span> is 0.5 emu/g at the applied field of 20 kOe (TC = 104 K). For the HEAs of <span class="hlt">FeCoNiCr</span>Ga and <span class="hlt">FeCoNiCr</span>Al, the saturation magnetization significantly increased to 38 emu/g (TC = 703 K) and 25 emu/g (TC = 277 K), respectively. To evaluate the possibility of solid solution FCC and BCC phases in <span class="hlt">FeCoNiCr</span>-type HEAs, we introduced a parameter of valence electron concentration (VEC). The proposed rule for solid solution formation by the VEC was matched with <span class="hlt">FeCoNiCr</span>-type HEAs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22645495-photon-annealing-silicon-implanted-gallium-nitride-layers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22645495-photon-annealing-silicon-implanted-gallium-nitride-layers"><span>On the photon annealing of <span class="hlt">silicon</span>-implanted gallium-nitride <span class="hlt">layers</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>Seleznev, B. I., E-mail: Boris.Seleznev@novsu.ru; Moskalev, G. Ya.; Fedorov, D. G.</p> <p>2016-06-15</p> <p>The conditions for the formation of ion-doped <span class="hlt">layers</span> in gallium nitride upon the incorporation of <span class="hlt">silicon</span> ions followed by photon annealing in the presence of <span class="hlt">silicon</span> dioxide and nitride coatings are analyzed. The conditions of the formation of ion-doped <span class="hlt">layers</span> with a high degree of impurity activation are established. The temperature dependences of the surface concentration and mobility of charge carriers in ion-doped GaN <span class="hlt">layers</span> annealed at different temperatures are studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e6407K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e6407K"><span>Magnetic and magnetocaloric properties of Ho<span class="hlt">Cr</span>0.75<span class="hlt">Fe</span>0.25O3 compound</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kotnana, Ganesh; Babu, P. D.; Jammalamadaka, S. Narayana</p> <p>2018-05-01</p> <p>We report on the magnetic and magnetocaloric properties of Ho<span class="hlt">Cr</span>0.75<span class="hlt">Fe</span>0.25O3 compound around the Néel temperature (TN), which is due to <span class="hlt">Cr</span>3+ ordering. Susceptibility (χ) vs. temperature (T) graph of Ho<span class="hlt">Cr</span>0.75<span class="hlt">Fe</span>0.25O3 compound infer two transitions due to the ordering of <span class="hlt">Cr</span>3+ moments (TN ˜ 155 K) and Ho3+ moments (TNHo ˜ 8 K). Magnetic entropy (-ΔSM) value of 1.14 J kg-1 K-1 around 157.5 K with a magnetic field (H) of 90 kOe is attributed to antiferromagnetic (AFM) ordering of <span class="hlt">Cr</span>3+ moments. A maximum value of adiabatic temperature (ΔTad) ˜ 0.41 K around TN is obtained and is found to increases with applied magnetic field. Negative slope for H/M vs. M2 graph is evident for Ho<span class="hlt">Cr</span>0.75<span class="hlt">Fe</span>0.25O3 compound below TN, which indicates the first order phase transition. Quantified values of -ΔSM and ΔTad open the way to explore rare earth orthochromites for the MCE properties and refrigeration applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780009204','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780009204"><span>Phase relations in the <span class="hlt">Fe-Ni-Cr</span>-S system and the sulfidation of an austenitic stainless steel</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jacob, K. T.; Rao, D. B.; Nelson, H. G.</p> <p>1977-01-01</p> <p>The stability fields of various sulfide phases that form on <span class="hlt">Fe-Cr</span>, <span class="hlt">Fe</span>-Ni, Ni-<span class="hlt">Cr</span> and <span class="hlt">Fe-Cr</span>-Ni alloys were developed as a function of temperature and the partial pressure of sulfur. The calculated stability fields in the ternary system were displayed on plots of log P sub S sub 2 versus the conjugate extensive variable which provides a better framework for following the sulfidation of <span class="hlt">Fe-Cr</span>-Ni alloys at high temperatures. Experimental and estimated thermodynamic data were used in developing the sulfur potential diagrams. Current models and correlations were employed to estimate the unknown thermodynamic behavior of solid solutions of sulfides and to supplement the incomplete phase diagram data of geophysical literature. These constructed stability field diagrams were in excellent agreement with the sulfide phases and compositions determined during a sulfidation experiment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009SSSci..11.1444B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009SSSci..11.1444B"><span>Structural and Mössbauer characterization of the ball milled <span class="hlt">Fe</span> x(<span class="hlt">Cr</span> 2O 3) 1- x system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Biondo, Valdecir; de Medeiros, Suzana Nóbrega; Paesano, Andrea, Jr.; Ghivelder, Luis; Hallouche, Bachir; da Cunha, João Batista Marimon</p> <p>2009-08-01</p> <p>The <span class="hlt">Fe</span> x(<span class="hlt">Cr</span> 2O 3) 1- x system, with 0.10 ≤ X ≤ 0.80, was mechanically processed for 24 h in a high-energy ball-mill. In order to examine the possible formation of iron-chromium oxides and alloys, the milled samples were, later, thermally annealed in inert (argon) and reducing (hydrogen) atmospheres. The as-milled and annealed products were characterized by X-ray diffraction, Mössbauer spectroscopy, transmission electron microscopy and magnetization. The as-milled samples showed the formation of an <span class="hlt">Fe</span> 1+ YCr 2- YO 4- δ nanostructured and disordered spinel phase, the α 1-<span class="hlt">Fe(Cr</span>) and α 2-<span class="hlt">Cr(Fe</span>) solid solutions and the presence of non-exhausted precursors. For the samples annealed in inert atmosphere, the chromite (<span class="hlt">FeCr</span> 2O 4) formation and the recrystallization of the precursors were verified. The hydrogen treated samples revealed the reduction of the spinel phase, with the phase separation of the chromia phase and retention of the <span class="hlt">Fe-Cr</span> solid solutions. All the samples, either as-milled or annealed, presented the magnetization versus applied field curves typical for superparamagnetic systems.</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('http://adsabs.harvard.edu/abs/2010JPS...195.3605B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JPS...195.3605B"><span>Co<span class="hlt">Fe</span> 2O 4 spinel protection coating thermally converted from the electroplated Co-<span class="hlt">Fe</span> alloy for solid oxide fuel cell interconnect application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bi, Z. H.; Zhu, J. H.; Batey, J. L.</p> <p></p> <p>Co<span class="hlt">Fe</span> 2O 4 has been demonstrated as a potential spinel coating for protecting the <span class="hlt">Cr</span>-containing ferritic interconnects. This spinel had an electrical conductivity of 0.85 S cm -1 at 800 °C in air and an average coefficient of thermal expansion (CTE) of 11.80 × 10 -6 K -1 from room temperature to 800 °C. A series of Co-<span class="hlt">Fe</span> alloys were co-deposited onto the Crofer 22 APU ferritic steel via electroplating with an acidic chloride solution. After thermal oxidation in air at 800 °C, a Co<span class="hlt">Fe</span> 2O 4 spinel <span class="hlt">layer</span> was attained from the plated Co 0.40<span class="hlt">Fe</span> 0.60 film. Furthermore, a channeled Crofer 22 APU interconnect electrodeposited with a 40-μm Co 0.40<span class="hlt">Fe</span> 0.60 alloy film as a protective coating was evaluated in a single-cell configuration. The presence of the dense, <span class="hlt">Cr</span>-free Co<span class="hlt">Fe</span> 2O 4 spinel <span class="hlt">layer</span> was effective in blocking the <span class="hlt">Cr</span> migration/transport and thus contributed to the improvement in cell performance stability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SuTMP...6b4001W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SuTMP...6b4001W"><span><span class="hlt">Silicon</span> content design of <span class="hlt">Cr</span>SiN films for good anti-corrosion and anti-wear performances in NaOH solution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Haixin; Ye, Yuwei; Wang, Chunting; Zhang, Guangan; Liu, Wei</p> <p>2018-06-01</p> <p>The <span class="hlt">Cr</span>SiN films with different <span class="hlt">silicon</span> contents were fabricated by medium frequency magnetron sputtering. The 304L stainless steel and Si (1 0 0) wafer were used for substrate specimens. Film plasticity, corrosion and tribological behaviors in 0.1 M NaOH solution were systematically investigated. Results show that the plasticity of <span class="hlt">Cr</span>N film could be improved by the addition of <span class="hlt">silicon</span>. During the corrosion test, with the increase of <span class="hlt">silicon</span> content, the corrosion current density exhibited a descending trend and impedance presented a rising trend. The COF and wear rate of as-prepared <span class="hlt">Cr</span>SiN film initially decreased and then increased as the <span class="hlt">silicon</span> content increased. The <span class="hlt">Cr</span>SiN film with 12.7 at.% Si exhibited the lowest COF of 0.04 and a wear rate of 6.746  ×  10‑8 mm3 Nm‑1 in 0.1 M NaOH solution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA42A..05C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA42A..05C"><span>Thermosphere-Ionosphere <span class="hlt">Fe/Fe</span>+ (TIFe) <span class="hlt">Layers</span> and Their Coupling with Geomagnetic Storms and Solar Wind</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chu, X.; Xu, Z.; Zhao, J.; Yu, Z.; Knipp, D. J.; Kilcommons, L. M.; Chen, C.; Fong, W.; Barry, I. F.; Hartinger, M.</p> <p>2016-12-01</p> <p>The discovery of thermospheric neutral <span class="hlt">Fe</span> <span class="hlt">layers</span> by lidar observations in Antarctica has opened a new door to explore the space-atmosphere interactions with ground-based instruments, especially in the least understood but crucially important altitude range of 100-200 km. These neutral metal <span class="hlt">layers</span> provide excellent tracers for modern resonance lidars to measure the neutral wind and temperature directly, complementing the radar measurements of the ionosphere and the magnetometer measurements of the geomagnetic field. Even more exciting, the neutral metal <span class="hlt">layers</span> in the thermosphere provide a natural laboratory to test our fundamental understandings of the atmosphere-ionosphere-magnetosphere (AIM) coupling and processes. The stunning <span class="hlt">Fe</span> <span class="hlt">layer</span> event on 28 May 2011 with clear gravity wave signatures has been simulated successfully with the University of Colorado Thermosphere-Ionosphere <span class="hlt">Fe/Fe</span>+ (TIFe) model, confirming the theoretical hypothesis that such thermospheric <span class="hlt">Fe</span> <span class="hlt">layers</span> are produced through the neutralization of converged <span class="hlt">Fe+layers</span>. Over 5.5 years of lidar observations at McMurdo have revealed many more cases with variety of patterns - besides the `gravity wave' patterns, there are `diffusive' patterns with both upward and downward phase progressions of <span class="hlt">Fe</span> <span class="hlt">layers</span>, and `superposition' patterns with both gravity wave signature and diffusive background. Surprisingly, these <span class="hlt">Fe</span> <span class="hlt">layer</span> events exhibit close correlations with geomagnetic storms. They also correspond to remarkable activity of extreme solar wind events, e.g., high-speed stream (HSS) and coronal mass ejection (CME), etc. This paper conducts a systematic investigation of the coupling among TIFe <span class="hlt">layers</span>, geomagnetic storms, solar wind and IMF via combining ground-based lidar, magnetometer, and SuperDARN data with DMSP, ACE and WIND satellite data along with the TIFe model simulations. We aim to quantitatively determine the relationship between TIFe and magnetic storms, and explore the mechanisms responsible for</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27836472','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27836472"><span>Facile preparation of magnetic mesoporous Mn<span class="hlt">Fe</span>2O4@SiO2-CTAB composites for <span class="hlt">Cr</span>(VI) adsorption and reduction.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Na; Fu, Fenglian; Lu, Jianwei; Ding, Zecong; Tang, Bing; Pang, Jiabin</p> <p>2017-01-01</p> <p>Chromium-contaminated water is regarded as one of the biggest threats to human health. In this study, a novel magnetic mesoporous Mn<span class="hlt">Fe</span> 2 O 4 @SiO 2 -CTAB composite was prepared by a facile one-step modification method and applied to remove <span class="hlt">Cr</span>(VI). X-ray diffraction, scanning electron microscopy, transmission electron microscopy, specific surface area, and vibrating sample magnetometer were used to characterize Mn<span class="hlt">Fe</span> 2 O 4 @SiO 2 -CTAB composites. The morphology analysis showed that the composites displayed a core-shell structure. The outer shell was mesoporous silica with CTAB and the core was Mn<span class="hlt">Fe</span> 2 O 4 nanoparticles, which ensured the easy separation by an external magnetic field. The performance of Mn<span class="hlt">Fe</span> 2 O 4 @SiO 2 -CTAB composites in <span class="hlt">Cr</span>(VI) removal was far better than that of bare Mn<span class="hlt">Fe</span> 2 O 4 nanoparticles. There were two reasons for the effective removal of <span class="hlt">Cr</span>(VI) by Mn<span class="hlt">Fe</span> 2 O 4 @SiO 2 -CTAB composites: (1) mesoporous silica shell with abundant CTA + significantly enhanced the <span class="hlt">Cr</span>(VI) adsorption capacity of the composites; (2) a portion of <span class="hlt">Cr</span>(VI) was reduced to less toxic <span class="hlt">Cr</span>(III) by Mn<span class="hlt">Fe</span> 2 O 4 , followed by <span class="hlt">Cr</span>(III) immobilized on Mn<span class="hlt">Fe</span> 2 O 4 @SiO 2 -CTAB composites, which had been demonstrated by X-ray photoelectron spectroscopy results. The adsorption of <span class="hlt">Cr</span>(VI) onto Mn<span class="hlt">Fe</span> 2 O 4 @SiO 2 -CTAB followed the Freundlich isotherm model and pseudo-second-order model. Tests on the regeneration and reuse of the composites were performed. The removal efficiency of <span class="hlt">Cr</span>(VI) still retained 92.4% in the sixth cycle. Mn<span class="hlt">Fe</span> 2 O 4 @SiO 2 -CTAB composites exhibited a great potential for the removal of <span class="hlt">Cr</span>(VI) from water. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMSA41A4049R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMSA41A4049R"><span>Influence of Sporadic E <span class="hlt">layers</span> on Mesospheric Na and <span class="hlt">Fe</span> <span class="hlt">Layers</span> over Arecibo</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raizada, S.; Tepley, C. A.; Zhou, Q.; Sarkhel, S.; Mathews, J. D.; Aponte, N.; Kerr, R.</p> <p>2014-12-01</p> <p>Arecibo offers unique opportunity to investigate the structure of the mesospheric metal <span class="hlt">layers</span> and their response to Sporadic E as observed by the incoherent scatter radar data. Previous studies have shown higher occurrences of sporadic activity in the neutral <span class="hlt">Fe</span> <span class="hlt">layers</span> as compared to Na at mid-latitudes. Other studies demonstrated that Sporadic Na (NaS) <span class="hlt">layers</span> are more common at low and high latitudes as compared to <span class="hlt">Fe</span>S. It is important to note that case studies based on a few nights of observations are significant as they can shed more light on factors that are important on short term scales. These efforts can also help in evaluation of the role played by these factors in the climatological or global studies. In this study, we have used two adjacent nights of simultaneous Na and <span class="hlt">Fe</span> data obtained using resonance lidars at Arecibo, while the co-located Incoherent Scatter Radar (ISR) provides information about Sporadic E (ES). On both the nights (17 and 18 March 2004) ES was observed with electron densities exceeding 3000 electrons/cc. Some interesting observations are worth noting: The <span class="hlt">Fe</span> main <span class="hlt">layer</span> (below 90 km) was stronger than the corresponding sporadic <span class="hlt">layer</span> around 95 km. However, Na data displayed a weaker main <span class="hlt">layer</span> below 90 km with stronger NaS activity. Hence, the ratio of densities determined within <span class="hlt">layers</span> of 3 km thickness centered at 97 km and at 87 km are less than 1 for <span class="hlt">Fe</span> and exceeds 1 in the case of Na. A correlation analysis between Na/Ne and <span class="hlt">Fe</span>/Ne also displays dissimilarities in the 94-100 km altitude range. An onsite all-sky imager recorded similar wave activities on both the nights with both ripple and band type structures that were observed in the 557.7 nm airglow. We will discuss the dissimilar response of Na and <span class="hlt">Fe</span> to Sporadic E activity in relation to neutralization lifetimes of their respective ions and their sensitivity to temperatures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/865233','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/865233"><span>Heat treatment of Ni<span class="hlt">CrFe</span> alloy to optimize resistance to intergrannular stress corrosion</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Steeves, Arthur F.; Bibb, Albert E.</p> <p>1984-01-01</p> <p>A process of producing a Ni<span class="hlt">CrFe</span> alloy having a high resistance to stress corrosion cracking comprising heating a Ni<span class="hlt">CrFe</span> alloy to a temperature sufficient to enable the carbon present in the alloy body in the form of carbide deposits to enter into solution, rapidly cool the alloy body, and heat the cooled body to a temperature between 1100.degree. to 1500.degree. F. for about 1 to 30 hours.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhSS...54.1433K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhSS...54.1433K"><span>Magnetomechanical effect in <span class="hlt">silicon</span> (Cz-Si) surface <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koplak, O. V.; Dmitriev, A. I.; Morgunov, R. B.</p> <p>2012-07-01</p> <p>The mechanical properties of near-surface <span class="hlt">layers</span> of Czochralski-grown <span class="hlt">silicon</span> crystals Cz- n-Si(111) have been found to undergo changes in response to an external constant magnetic field ( B ˜ 0.1 T). A magnetically induced variation in the microhardness, Young's modulus, and coefficient of plasticity of <span class="hlt">silicon</span> crystals correlates with the change in the lattice parameter and internal stresses of the sample. The growth of an oxide film under exposure to a magnetic field plays the principal role in the magnetomechanical effect due to a decrease in the concentration of oxygen complexes in the near-surface <span class="hlt">layers</span> of the sample. In microstructured <span class="hlt">silicon</span>, where the surface is considerably more developed, the magnetic field induces more profound changes in the internal stresses as compared to single crystals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PlST...19d5502S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PlST...19d5502S"><span>Fabrication and characterization of He-charged ODS-<span class="hlt">FeCr</span>Ni films deposited by a radio-frequency plasma magnetron sputtering technique</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, Liang; Wang, Xianping; Wang, Le; Zhang, Ying; Liu, Wang; Jiang, Weibing; Zhang, Tao; Fang, Qianfeng; Liu, Changsong</p> <p>2017-04-01</p> <p>He-charged oxide dispersion strengthened (ODS) <span class="hlt">FeCr</span>Ni films were prepared by a radio-frequency (RF) plasma magnetron sputtering method in a He and Ar mixed atmosphere at 150 °C. As a comparison, He-charged <span class="hlt">FeCr</span>Ni films were also fabricated at the same conditions through direct current (DC) plasma magnetron sputtering. The doping of He atoms and Y2O3 in the <span class="hlt">FeCr</span>Ni films was realized by the high backscattered rate of He ions and Y2O3/<span class="hlt">FeCr</span>Ni composite target sputtering method, respectively. Inductive coupled plasma (ICP) and x-ray photoelectron spectroscopy (XPS) analysis confirmed the existence of Y2O3 in <span class="hlt">FeCr</span>Ni films, and Y2O3 content hardly changed with sputtering He/Ar ratio. Cross-sectional scanning electron microscopy (SEM) shows that the <span class="hlt">FeCr</span>Ni films were composed of dense columnar nanocrystallines and the thickness of the films was obviously dependent on He/Ar ratio. Nanoindentation measurements revealed that the <span class="hlt">FeCr</span>Ni films fabricated through DC/RF plasma magnetron sputtering methods exhibited similar hardness values at each He/Ar ratio, while the dispersion of Y2O3 apparently increased the hardness of the films. Elastic recoil detection (ERD) showed that DC/RF magnetron sputtered <span class="hlt">FeCr</span>Ni films contained similar He amounts (˜17 at.%). Compared with the minimal change of He level with depth in DC-sputtered films, the He amount decreases gradually in depth in the RF-sputtered films. The Y2O3-doped <span class="hlt">FeCr</span>Ni films were shown to exhibit much smaller amounts of He owing to the lower backscattering possibility of Y2O3 and the inhibition effect of nano-sized Y2O3 particles on the He element.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26894287','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26894287"><span><span class="hlt">Cr</span>(VI) reduction and immobilization by novel carbonaceous modified magnetic <span class="hlt">Fe</span>3O4/halloysite nanohybrid.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tian, Xike; Wang, Weiwei; Tian, Na; Zhou, Chaoxin; Yang, Chao; Komarneni, Sridhar</p> <p>2016-05-15</p> <p>In this work, a novel "Dumbbell-like" magnetic <span class="hlt">Fe</span>3O4/Halloysite nanohybrid (<span class="hlt">Fe</span>3O4/HNTs@C) with oxygen-containing organic group grafting on the surface of natural halloysite nanotubes (HNTs) and homogeneous <span class="hlt">Fe</span>3O4 nanospheres selectively aggregating at the tips of modified halloysite nanotubes was successfully synthesized. XRD, TEM, IR spectroscopy, XPS and VSM were used to characterize this newly halloysite nanohybrid and its formation mechanism was discussed. <span class="hlt">Cr</span>(VI) ions adsorption experiments showed that the <span class="hlt">Fe</span>3O4/halloysite nanohybrid exhibited higher adsorption ability with a maximum adsorption capacity of 132 mg/L at 303K, which is about 100 times higher than that of unmodified halloysite nanotubes. More importantly, with the reduction of <span class="hlt">Fe</span>3O4 and electron-donor effect of oxygen-containing organic groups, <span class="hlt">Cr</span>(VI) ions were easily reduced into low toxicity <span class="hlt">Cr</span>(III) and then adsorbed onto the surface of halloysite nanohybrid. In addition, appreciable magnetization was observed due to the aggregation of magnetite nanoparticles, which make adsorbent facility separated from aqueous solutions after <span class="hlt">Cr</span> pollution adsorption. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JNuM..503..250A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JNuM..503..250A"><span>Microstructure and mechanical properties of <span class="hlt">FeCr</span>Al alloys under heavy ion irradiations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aydogan, E.; Weaver, J. S.; Maloy, S. A.; El-Atwani, O.; Wang, Y. Q.; Mara, N. A.</p> <p>2018-05-01</p> <p><span class="hlt">FeCr</span>Al ferritic alloys are excellent cladding candidates for accident tolerant fuel systems due to their high resistance to oxidation as a result of formation of a protective Al2O3 scale at high temperatures in steam. In this study, we report the irradiation response of the 10<span class="hlt">Cr</span> and 13<span class="hlt">Cr</span> <span class="hlt">FeCr</span>Al cladding tubes under <span class="hlt">Fe</span>2+ ion irradiation up to ∼16 dpa at 300 °C. Dislocation loop size, density and characteristics were determined using both two-beam bright field transmission electron microscopy and on-zone scanning transmission electron microscopy techniques. 10<span class="hlt">Cr</span> (C06M2) tube has a lower dislocation density, larger grain size and a slightly weaker texture compared to the 13<span class="hlt">Cr</span> (C36M3) tube before irradiation. After irradiation to 0.7 dpa and 16 dpa, the fraction of <100> type sessile dislocations decreases with increasing <span class="hlt">Cr</span> amount in the alloys. It has been found that there is neither void formation nor α‧ precipitation as a result of ion irradiations in either alloy. Therefore, dislocation loops were determined to be the only irradiation induced defects contributing to the hardening. Nanoindentation testing before the irradiation revealed that the average nanohardness of the C36M3 tube is higher than that of the C06M2 tube. The average nanohardness of irradiated tube samples saturated at 1.6-2.0 GPa hardening for both tubes between ∼3.4 dpa and ∼16 dpa. The hardening calculated based on transmission electron microscopy was found to be consistent with nanohardness measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1425772-microstructure-mechanical-properties-fecral-alloys-under-heavy-ion-irradiations','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1425772-microstructure-mechanical-properties-fecral-alloys-under-heavy-ion-irradiations"><span>Microstructure and mechanical properties of <span class="hlt">FeCr</span>Al alloys under heavy ion irradiations</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>Aydogan, E.; Weaver, J. S.; Maloy, S. A.</p> <p></p> <p><span class="hlt">FeCr</span>Al ferritic alloys are excellent cladding candidates for accident tolerant fuel systems due to their high resistance to oxidation as a result of formation of a protective Al 2O 3 scale at high temperatures in steam. In this study, we report the irradiation response of the 10<span class="hlt">Cr</span> and 13<span class="hlt">Cr</span> <span class="hlt">FeCr</span>Al cladding tubes under <span class="hlt">Fe</span> 2+ ion irradiation up to ~16 dpa at 300 °C. Dislocation loop size, density and characteristics were determined using both two beam bright field transmission electron microscopy and on-zone scanning transmission electron microscopy techniques. 10<span class="hlt">Cr</span> (C06M2) tube has a lower dislocation density, larger grain size andmore » a slightly weaker texture compared to the 13<span class="hlt">Cr</span> (C36M3) tube before irradiation. After irradiation to 0.7 dpa and 16 dpa, the fraction of <100> type sessile dislocations decreases with increasing <span class="hlt">Cr</span> amount in the alloys. It has been found that there is neither void formation nor α' precipitation as a result of ion irradiations in either alloy. Therefore, dislocation loops were determined to be the only irradiation induced defects contributing to the hardening. Nanoindentation testing before the irradiation revealed that the average nanohardness of the C36M3 tube is higher than that of the C06M2 tube. The average nanohardness of irradiated tube samples saturated at 1.6-2.0 GPa hardening for both tubes between ~3.4 dpa and ~16 dpa. The hardening calculated based on transmission electron microscopy was found to be consistent with nanohardness measurements.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1425772-microstructure-mechanical-properties-fecral-alloys-under-heavy-ion-irradiations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1425772-microstructure-mechanical-properties-fecral-alloys-under-heavy-ion-irradiations"><span>Microstructure and mechanical properties of <span class="hlt">FeCr</span>Al alloys under heavy ion irradiations</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Aydogan, E.; Weaver, J. S.; Maloy, S. A.; ...</p> <p>2018-03-02</p> <p><span class="hlt">FeCr</span>Al ferritic alloys are excellent cladding candidates for accident tolerant fuel systems due to their high resistance to oxidation as a result of formation of a protective Al 2O 3 scale at high temperatures in steam. In this study, we report the irradiation response of the 10<span class="hlt">Cr</span> and 13<span class="hlt">Cr</span> <span class="hlt">FeCr</span>Al cladding tubes under <span class="hlt">Fe</span> 2+ ion irradiation up to ~16 dpa at 300 °C. Dislocation loop size, density and characteristics were determined using both two beam bright field transmission electron microscopy and on-zone scanning transmission electron microscopy techniques. 10<span class="hlt">Cr</span> (C06M2) tube has a lower dislocation density, larger grain size andmore » a slightly weaker texture compared to the 13<span class="hlt">Cr</span> (C36M3) tube before irradiation. After irradiation to 0.7 dpa and 16 dpa, the fraction of <100> type sessile dislocations decreases with increasing <span class="hlt">Cr</span> amount in the alloys. It has been found that there is neither void formation nor α' precipitation as a result of ion irradiations in either alloy. Therefore, dislocation loops were determined to be the only irradiation induced defects contributing to the hardening. Nanoindentation testing before the irradiation revealed that the average nanohardness of the C36M3 tube is higher than that of the C06M2 tube. The average nanohardness of irradiated tube samples saturated at 1.6-2.0 GPa hardening for both tubes between ~3.4 dpa and ~16 dpa. The hardening calculated based on transmission electron microscopy was found to be consistent with nanohardness measurements.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1372256-reactivity-fe-ii-associated-goethite-formed-during-short-redox-cycles-toward-cr-vi-reduction-under-oxic-conditions','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1372256-reactivity-fe-ii-associated-goethite-formed-during-short-redox-cycles-toward-cr-vi-reduction-under-oxic-conditions"><span>The reactivity of <span class="hlt">Fe</span>(II) associated with goethite formed during short redox cycles toward <span class="hlt">Cr</span>(VI) reduction under oxic conditions</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>Tomaszewski, Elizabeth J.; Lee, Seungyeol; Rudolph, Jared</p> <p></p> <p>Chromium (<span class="hlt">Cr</span>) is a toxic metal that causes a myriad of health problems and enters the environment as a result of anthropogenic activities and/or natural processes. The toxicity and solubility of chromium is linked to its oxidation state; <span class="hlt">Cr</span>(III) is poorly soluble and relatively nontoxic, while <span class="hlt">Cr</span>(VI) is soluble and a known carcinogen. Solid <span class="hlt">Fe</span>(II) in iron-bearing minerals, such as pyrite, magnetite, and green rusts, reduce the oxidation state of chromium, reducing its toxicity and mobility. However, these minerals are not the only potential sources of solid-associated <span class="hlt">Fe</span>(II) available for <span class="hlt">Cr</span>(VI) reduction. For example, ferric (<span class="hlt">Fe</span>(III)) (hydr)oxides, such as goethitemore » or hematite, can have <span class="hlt">Fe</span>(II) in the solid without phase transformation; however, the reactivity of <span class="hlt">Fe</span>(II) within <span class="hlt">Fe</span>(III) (hydr)oxides with contaminants, has not been previously investigated. Here, we cyclically react goethite with dissolved <span class="hlt">Fe</span>(II) followed by dissolved O2, leading to the formation of reactive <span class="hlt">Fe</span>(II) associated with goethite. In separate reactors, the reactivity of this <span class="hlt">Fe</span>(II) is probed under oxic conditions, by exposure to chromate (<span class="hlt">Cr</span>O42 -) after either one, two, three or four redox cycles. <span class="hlt">Cr</span> is not present during redox cycling; rather, it is introduced to a subset of the solid after each oxidation half-cycle. Analysis of X-ray absorption near edge structure (XANES) spectra reveals that the extent of <span class="hlt">Cr</span>(VI) reduction to <span class="hlt">Cr</span>(III) depends not only on solid <span class="hlt">Fe</span>(II) content but also surface area and mean size of ordered crystalline domains, determined by BET surface area analysis and X-ray diffraction (XRD), respectively. Shell-by-shell fitting of the extended X-ray absorption fine structure (EXAFS) spectra demonstrates chromium forms both single and double corner sharing complexes on the surface of goethite, in addition to sorbed <span class="hlt">Cr</span>(III) species. Finally, transmission electron microscope (TEM) imaging and X-ray energy-dispersive spectroscopy (EDS) illustrate that <span class="hlt">Cr</span> preferentially</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EL.....63...69D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EL.....63...69D"><span>Hydrogen vibrations in austenitic fcc <span class="hlt">Fe-Cr</span>-Mn-Ni steels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Danilkin, S. A.; Fuess, H.; Wipf, H.; Ivanov, A.; Gavriljuk, V. G.; Delafosse, D.; Magnin, T.</p> <p>2003-07-01</p> <p>By neutron spectroscopy, we studied vibrations of H interstitials in two austenitic fcc steels (<span class="hlt">Fe</span>0.55<span class="hlt">Cr</span>0.20Mn0.10Ni0.15 and <span class="hlt">Fe</span>0.54<span class="hlt">Cr</span>0.27Ni0.19) doped with 0.37 and 0.33 at% H. The band modes, in which H vibrates with its metal neighbours, cause a weak intensity in the energy range of the acoustic vibrations of the H-free steels. The energies of the fundamental and the twofold local-mode excitations, in which H vibrates against its metal neighbours, were ~ 130 and ~ 260 meV, respectively. The respective peaks in the spectra were broadened because the metal neighbours of H, and thus its vibrational energies, vary from interstitial site to interstitial site. The above energy values support an H occupation of octahedral interstitial sites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvB..94s5307Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvB..94s5307Z"><span>Density functional theory study of bulk and single-<span class="hlt">layer</span> magnetic semiconductor <span class="hlt">Cr</span>PS4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhuang, Houlong L.; Zhou, Jia</p> <p>2016-11-01</p> <p>Searching for two-dimensional (2D) materials with multifunctionality is one of the main goals of current research in 2D materials. Magnetism and semiconducting are certainly two desirable functional properties for a single 2D material. In line with this goal, here we report a density functional theory (DFT) study of bulk and single-<span class="hlt">layer</span> magnetic semiconductor <span class="hlt">Cr</span>PS4. We find that the ground-state magnetic structure of bulk <span class="hlt">Cr</span>PS4 exhibits the A-type antiferromagnetic ordering, which transforms to ferromagnetic (FM) ordering in single-<span class="hlt">layer</span> <span class="hlt">Cr</span>PS4. The calculated formation energy and phonon spectrum confirm the stability of single-<span class="hlt">layer</span> <span class="hlt">Cr</span>PS4. The band gaps of FM single-<span class="hlt">layer</span> <span class="hlt">Cr</span>PS4 calculated with a hybrid density functional are within the visible-light range. We also study the effects of FM ordering on the optical absorption spectra and band alignments for water splitting, indicating that single-<span class="hlt">layer</span> <span class="hlt">Cr</span>PS4 could be a potential photocatalyst. Our work opens up ample opportunities of energy-related applications of single-<span class="hlt">layer</span> <span class="hlt">Cr</span>PS4.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006MeScT..17..519Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006MeScT..17..519Z"><span>High temperature and frequency pressure sensor based on <span class="hlt">silicon</span>-on-insulator <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Y. L.; Zhao, L. B.; Jiang, Z. D.</p> <p>2006-03-01</p> <p>Based on <span class="hlt">silicon</span> on insulator (SOI) technology, a novel high temperature pressure sensor with high frequency response is designed and fabricated, in which a buried <span class="hlt">silicon</span> dioxide <span class="hlt">layer</span> in the <span class="hlt">silicon</span> material is developed by the separation by implantation of oxygen (SIMOX) technology. This <span class="hlt">layer</span> can isolate leak currents between the top <span class="hlt">silicon</span> <span class="hlt">layer</span> for the detecting circuit and body <span class="hlt">silicon</span> at a temperature of about 200 °C. In addition, the technology of <span class="hlt">silicon</span> and glass bonding is used to create a package of the sensor without internal strain. A structural model and test data from the sensor are presented. The experimental results showed that this kind of sensor possesses good static performance in a high temperature environment and high frequency dynamic characteristics, which may satisfy the pressure measurement demands of the oil industry, aviation and space, and so on.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1361343-design-properties-weldability-advanced-oxidation-resistant-fecral-alloys','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1361343-design-properties-weldability-advanced-oxidation-resistant-fecral-alloys"><span>Design, properties, and weldability of advanced oxidation-resistant <span class="hlt">FeCr</span>Al alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Gussev, M. N.; Field, K. G.; Yamamoto, Y.</p> <p>2017-05-05</p> <p><span class="hlt">FeCr</span>Al alloys are promising as corrosion- and oxidation-resistance materials for extreme high-temperature applications. However, further alloy design and improvement requires a delicate balance between workability, weldability, propensity for '-phase formation, among other factors. Here, a series of advanced oxidant resistant <span class="hlt">FeCr</span>Al alloys were produced and investigated. Variants with Al (+2%), Nb (+1%), and TiC (0.1, 0.3, and 1%) additions over the reference alloy (<span class="hlt">Fe</span>-13%<span class="hlt">Cr</span>-5%Al) were characterized in detail before and after controlled laser beam welding using tensile tests with digital image correlation, SEM-EBSD analysis, and fractography. All investigated alloys demonstrated yield stress in the weldment over 500 MPa; no welding-inducedmore » cracking was observed. However, it was shown that the increase in the Al-content over 5% was detrimental leading to a brittle fracture mechanism and decreased ductility in the weldment. At the same time, Nb and TiC additions were beneficial for preventing grain growth and reducing local softening (yield stress reduction) in the heat-affected zone. The 1% TiC addition also effectively refined grain size in the weldment.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1361343','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1361343"><span>Design, properties, and weldability of advanced oxidation-resistant <span class="hlt">FeCr</span>Al alloys</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>Gussev, M. N.; Field, K. G.; Yamamoto, Y.</p> <p></p> <p><span class="hlt">FeCr</span>Al alloys are promising as corrosion- and oxidation-resistance materials for extreme high-temperature applications. However, further alloy design and improvement requires a delicate balance between workability, weldability, propensity for '-phase formation, among other factors. Here, a series of advanced oxidant resistant <span class="hlt">FeCr</span>Al alloys were produced and investigated. Variants with Al (+2%), Nb (+1%), and TiC (0.1, 0.3, and 1%) additions over the reference alloy (<span class="hlt">Fe</span>-13%<span class="hlt">Cr</span>-5%Al) were characterized in detail before and after controlled laser beam welding using tensile tests with digital image correlation, SEM-EBSD analysis, and fractography. All investigated alloys demonstrated yield stress in the weldment over 500 MPa; no welding-inducedmore » cracking was observed. However, it was shown that the increase in the Al-content over 5% was detrimental leading to a brittle fracture mechanism and decreased ductility in the weldment. At the same time, Nb and TiC additions were beneficial for preventing grain growth and reducing local softening (yield stress reduction) in the heat-affected zone. The 1% TiC addition also effectively refined grain size in the weldment.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e5223Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e5223Z"><span>Mechanical properties of <span class="hlt">silicon</span> in subsurface damage <span class="hlt">layer</span> from nano-grinding studied by atomistic simulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zhiwei; Chen, Pei; Qin, Fei; An, Tong; Yu, Huiping</p> <p>2018-05-01</p> <p>Ultra-thin <span class="hlt">silicon</span> wafer is highly demanded by semi-conductor industry. During wafer thinning process, the grinding technology will inevitably induce damage to the surface and subsurface of <span class="hlt">silicon</span> wafer. To understand the mechanism of subsurface damage (SSD) <span class="hlt">layer</span> formation and mechanical properties of SSD <span class="hlt">layer</span>, atomistic simulation is the effective tool to perform the study, since the SSD <span class="hlt">layer</span> is in the scale of nanometer and hardly to be separated from underneath undamaged <span class="hlt">silicon</span>. This paper is devoted to understand the formation of SSD <span class="hlt">layer</span>, and the difference between mechanical properties of damaged <span class="hlt">silicon</span> in SSD <span class="hlt">layer</span> and ideal <span class="hlt">silicon</span>. With the atomistic model, the nano-grinding process could be performed between a <span class="hlt">silicon</span> workpiece and diamond tool under different grinding speed. To reach a thinnest SSD <span class="hlt">layer</span>, nano-grinding speed will be optimized in the range of 50-400 m/s. Mechanical properties of six damaged <span class="hlt">silicon</span> workpieces with different depths of cut will be studied. The SSD <span class="hlt">layer</span> from each workpiece will be isolated, and a quasi-static tensile test is simulated to perform on the isolated SSD <span class="hlt">layer</span>. The obtained stress-strain curve is an illustration of overall mechanical properties of SSD <span class="hlt">layer</span>. By comparing the stress-strain curves of damaged <span class="hlt">silicon</span> and ideal <span class="hlt">silicon</span>, a degradation of Young's modulus, ultimate tensile strength (UTS), and strain at fracture is observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4668570','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4668570"><span>Aluminium alloyed iron-silicide/<span class="hlt">silicon</span> solar cells: A simple approach for low cost environmental-friendly photovoltaic technology</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kumar Dalapati, Goutam; Masudy-Panah, Saeid; Kumar, Avishek; Cheh Tan, Cheng; Ru Tan, Hui; Chi, Dongzhi</p> <p>2015-01-01</p> <p>This work demonstrates the fabrication of silicide/<span class="hlt">silicon</span> based solar cell towards the development of low cost and environmental friendly photovoltaic technology. A heterostructure solar cells using metallic alpha phase (α-phase) aluminum alloyed iron silicide (<span class="hlt">Fe</span>Si(Al)) on n-type <span class="hlt">silicon</span> is fabricated with an efficiency of 0.8%. The fabricated device has an open circuit voltage and fill-factor of 240 mV and 60%, respectively. Performance of the device was improved by about 7 fold to 5.1% through the interface engineering. The α-phase <span class="hlt">FeSi(Al)/silicon</span> solar cell devices have promising photovoltaic characteristic with an open circuit voltage, short-circuit current and a fill factor (FF) of 425 mV, 18.5 mA/cm2, and 64%, respectively. The significant improvement of α-phase <span class="hlt">Fe</span>Si(Al)/n-Si solar cells is due to the formation p+−n homojunction through the formation of re-grown crystalline <span class="hlt">silicon</span> <span class="hlt">layer</span> (~5–10 nm) at the silicide/<span class="hlt">silicon</span> interface. Thickness of the regrown <span class="hlt">silicon</span> <span class="hlt">layer</span> is crucial for the silicide/<span class="hlt">silicon</span> based photovoltaic devices. Performance of the α-<span class="hlt">Fe</span>Si(Al)/n-Si solar cells significantly depends on the thickness of α-<span class="hlt">Fe</span>Si(Al) <span class="hlt">layer</span> and process temperature during the device fabrication. This study will open up new opportunities for the Si based photovoltaic technology using a simple, sustainable, and los cost method. PMID:26632759</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('https://www.osti.gov/servlets/purl/864267','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/864267"><span>Fabricating amorphous <span class="hlt">silicon</span> solar cells by varying the temperature _of the substrate during deposition of the amorphous <span class="hlt">silicon</span> <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Carlson, David E.</p> <p>1982-01-01</p> <p>An improved process for fabricating amorphous <span class="hlt">silicon</span> solar cells in which the temperature of the substrate is varied during the deposition of the amorphous <span class="hlt">silicon</span> <span class="hlt">layer</span> is described. Solar cells manufactured in accordance with this process are shown to have increased efficiencies and fill factors when compared to solar cells manufactured with a constant substrate temperature during deposition of the amorphous <span class="hlt">silicon</span> <span class="hlt">layer</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1832m0042S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1832m0042S"><span>Study of interlayer coupling between <span class="hlt">Fe</span>Pt and <span class="hlt">Fe</span>CoB thin films through MgO spacer <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singh, Sadhana; Kumar, Dileep; Gupta, Mukul; Reddy, V. Raghvendra</p> <p>2017-05-01</p> <p>Interlayer exchange coupling between hard-<span class="hlt">Fe</span>Pt and soft-<span class="hlt">Fe</span>CoB magnetic <span class="hlt">layers</span> has been studied with increasing thickness of insulator MgO spacer <span class="hlt">layer</span> in <span class="hlt">FePt/MgO/Fe</span>CoB sandwiched structure. A series of the samples were prepared in identical condition using ion beam sputtering method and characterized for their magnetic and structural properties using magneto-optical Kerr effect (MOKE) and X-ray reflectivity measurements. The nature of coupling between <span class="hlt">Fe</span>Pt and <span class="hlt">Fe</span>CoB was found to be ferromagnetic which decreases exponentially with increasing thickness of MgO <span class="hlt">layer</span>. At very low thickness of MgO <span class="hlt">layer</span>, both <span class="hlt">layers</span> were found strongly coupled thus exhibiting coherent magnetization reversal. At higher thickness, both <span class="hlt">layers</span> were found decoupled and magnetization reversal occurred at different switching fields. Strong coupling at very low thickness is attributed to pin holes in MgO <span class="hlt">layer</span> which lead to direct coupling whereas on increasing thickness, coupling may arise due to magneto-static interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SRL....24S0010L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SRL....24S0010L"><span>EFFECT OF Mg AND TEMPERATURE ON <span class="hlt">Fe</span>-Al ALLOY <span class="hlt">LAYER</span> IN <span class="hlt">Fe</span>/(Zn-6%Al-x%Mg) SOLID-LIQUID DIFFUSION COUPLES</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liang, Liu; Liu, Ya-Ling; Liu, Ya; Peng, Hao-Ping; Wang, Jian-Hua; Su, Xu-Ping</p> <p></p> <p><span class="hlt">Fe</span>/(Zn-6%Al-x%Mg) solid-liquid diffusion couples were kept at various temperatures for different periods of time to investigate the formation and growth of the <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span>. Scanning electron microscopy (SEM), energy dispersive spectrometry (EDS) and X-ray diffraction (XRD) were used to study the constituents and morphology of the <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span>. It was found that the <span class="hlt">Fe</span>2Al5Znx phase <span class="hlt">layer</span> forms close to the iron sheet and the <span class="hlt">Fe</span>Al3Znx phase <span class="hlt">layer</span> forms near the side of the melted Zn-6%Al-3%Mg in diffusion couples. When the <span class="hlt">Fe</span>/(Zn-6%Al-3%Mg) diffusion couple is kept at 510∘C for more than 15min, a continuous <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span> is formed on the interface of the diffusion couple. Among all <span class="hlt">Fe</span>/(Zn-6%Al-x%Mg) solid-liquid diffusion couples, the <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span> on the interface of the <span class="hlt">Fe</span>/(Zn-6% Al-3% Mg) diffusion couple is the thinnest. The <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span> forms only when the diffusion temperature is above 475∘. These results show that the <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span> in <span class="hlt">Fe</span>/(Zn-6%Al-x%Mg) solid-liquid diffusion couples is composed of <span class="hlt">Fe</span>2Al5Znx and <span class="hlt">Fe</span>Al3Znx phase <span class="hlt">layers</span>. Increasing the diffusing temperature and time period would promote the formation and growth of the <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span>. When the Mg content in the <span class="hlt">Fe</span>/(Zn-6%Al-x%Mg) diffusion couples is 3%, the growth of the <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span> is inhibited. These results may explain why there is no obvious <span class="hlt">Fe</span>-Al alloy <span class="hlt">layer</span> formed on the interface of steel with a Zn-6%Al-3%Mg coating.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1942m0031B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1942m0031B"><span>Ferroelectric properties of oxalate and phenanthroline based 1-D single chain molecular magnet [{<span class="hlt">FeII(Δ)Fe</span>II(Λ)}0.5{<span class="hlt">CrII(Δ)Cr</span>II(Λ)}0.5(ox)2(phen)2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bhatt, Pramod; Mukadam, M. D.; Mandal, B. P.; Yusuf, S. M.</p> <p>2018-04-01</p> <p>The one-dimensional (1-D) single chain molecular magnet [{<span class="hlt">FeII(Δ)Fe</span>II(Λ)}0.5{<span class="hlt">CrII(Δ)Cr</span>II(Λ)}0.5(ox)2(phen)2] is hydrothermally synthesized using oxalate (ox) and phenanthroline (phen) ligands with transition metal ions (<span class="hlt">Fe</span> and <span class="hlt">Cr</span>). The compound is characterized using x-ray diffraction, dc magnetization measurements and P-E ferroelectric loop measurements. The diffraction analysis using Rietveld refinement confirms a single phase formation of the compound in monoclinic structure with space group of P21. The compound crystallizes in 1-D chain like structure containing two different crystallographic sites of metal ions (Δ- and Λ-), which are bridged by the ox ligand and Phen ligand. These two metals site are different in bond length and bond angles results lattice distortions. The lattice distortion induces ferroelectric behavior in the compound which is discussed in terms of lattice distortion induced dipole moments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97x5409W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97x5409W"><span><span class="hlt">Layer</span> and doping tunable ferromagnetic order in two-dimensional <span class="hlt">Cr</span> S2 <span class="hlt">layers</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, Cong; Zhou, Xieyu; Pan, Yuhao; Qiao, Jingsi; Kong, Xianghua; Kaun, Chao-Cheng; Ji, Wei</p> <p>2018-06-01</p> <p>Interlayer coupling is of vital importance for manipulating physical properties, e.g., electronic band gap, in two-dimensional materials. However, tuning magnetic properties in these materials is yet to be addressed. Here, we found the in-plane magnetic orders of <span class="hlt">Cr</span> S2 mono and few <span class="hlt">layers</span> are tunable between striped antiferromagnetic (sAFM) and ferromagnetic (FM) orders by manipulating charge transfer between <span class="hlt">Cr</span> t2 g and eg orbitals. Such charge transfer is realizable through interlayer coupling, direct charge doping, or substituting S with Cl atoms. In particular, the transferred charge effectively reduces a portion of <span class="hlt">Cr</span>4 + to <span class="hlt">Cr</span>3 +, which, together with delocalized S p orbitals and their resulting direct S-S interlayer hopping, enhances the double-exchange mechanism favoring the FM rather than sAFM order. An exceptional interlayer spin-exchange parameter was revealed over -10 meV , an order of magnitude stronger than available results of interlayer magnetic coupling. It addition, the charge doping could tune <span class="hlt">Cr</span> S2 between p - and n -doped magnetic semiconductors. Given these results, several prototype devices were proposed for manipulating magnetic orders using external electric fields or mechanical motion. These results manifest the role of interlayer coupling in modifying magnetic properties of <span class="hlt">layered</span> materials and shed considerable light on manipulating magnetism in these materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1333089-heterogeneous-dislocation-loop-formation-near-grain-boundaries-neutron-irradiated-commercial-fecral-alloy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1333089-heterogeneous-dislocation-loop-formation-near-grain-boundaries-neutron-irradiated-commercial-fecral-alloy"><span>Heterogeneous dislocation loop formation near grain boundaries in a neutron-irradiated commercial <span class="hlt">FeCr</span>Al alloy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Field, Kevin G.; Briggs, Samuel A.; Hu, Xunxiang; ...</p> <p>2016-11-01</p> <p><span class="hlt">FeCr</span>Al alloys are an attractive materials class for nuclear power applications due to their increased environmental compatibility over more traditional nuclear materials. Preliminary studies into the radiation tolerance of <span class="hlt">FeCr</span>Al alloys under accelerated neutron testing between 300-400 °C have shown post-irradiation microstructures containing dislocation loops and <span class="hlt">Cr</span>-rich ' phase. Although these initial works established the post-irradiation microstructures, little to no focus was applied towards the influence of pre-irradiation microstructures on this response. Here, a well annealed commercial <span class="hlt">FeCr</span>Al alloy, Alkrothal 720, was neutron irradiated to 1.8 dpa at 382 °C and then the role of random high angle grain boundariesmore » on the spatial distribution and size of dislocation loops, dislocation loops, and black dot damage was analyzed using on-zone scanning transmission electron microscopy. Results showed a clear heterogeneous dislocation loop formation with dislocation loops showing an increased number density and size, black dot damage showing a significant number density decrease, and an increased size of dislocation loops in the vicinity directly adjacent to the grain boundary. Lastly, these results suggest the importance of the pre-irradiation microstructure on the radiation tolerance of <span class="hlt">FeCr</span>Al alloys.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080004656','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080004656"><span><span class="hlt">Silicon</span> based substrate with calcium aluminosilicate environmental/thermal barrier <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Eaton, Jr., Harry Edwin (Inventor); Allen, William Patrick (Inventor); Miller, Robert Alden (Inventor); Jacobson, Nathan S. (Inventor); Smialek, James L. (Inventor); Opila, Elizabeth J. (Inventor); Lee, Kang N. (Inventor); Nagaraj, Bangalore A. (Inventor); Wang, Hongyu (Inventor); Meschter, Peter Joel (Inventor)</p> <p>2001-01-01</p> <p>A barrier <span class="hlt">layer</span> for a <span class="hlt">silicon</span> containing substrate which inhibits the formation of gaseous species of <span class="hlt">silicon</span> when exposed to a high temperature aqueous environment comprises a calcium alumino silicate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910040296&hterms=AB+INITIO&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DAB%2BINITIO','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910040296&hterms=AB+INITIO&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DAB%2BINITIO"><span>An ab initio study of <span class="hlt">Fe</span>(CO)n, n = 1,5, and <span class="hlt">Cr</span>(CO)6</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barnes, Leslie A.; Rosi, Marzio; Bauschlicher, Charles W., Jr.</p> <p>1991-01-01</p> <p>Ab initio calculations have been performed for <span class="hlt">Cr</span>(CO)6 and <span class="hlt">Fe</span>(CO)n, n = 1,5. Basis sets of better than double zeta quality are used, and correlation is included using the modified coupler-pair functional method. The computed geometries and force constants are in reasonable agreement with experiment. The sequential bond dissociation energies of CO from <span class="hlt">Fe</span>(CO)5 are estimated to be: 39, 31, 25, 22, and greater than 5 kcal/mol. It is noted that the first bond dissociation energy is relative to the singlet ground state of <span class="hlt">Fe</span>(CO)5 and the lowest singlet state of <span class="hlt">Fe</span>(CO)4, whereas the second is relative to the ground triplet states of <span class="hlt">Fe</span>(CO)4 and <span class="hlt">Fe</span>(CO)3. In addition, the binding energy for <span class="hlt">Fe</span>-CO would be modified to 18 kcal/mol if dissociation occurred to the <span class="hlt">Fe</span>(5F) excited state asymptote. The CO binding energies for <span class="hlt">Fe</span> and <span class="hlt">Cr</span> are found to be in poorer agreement with experiment than those found in a previous study on Ni(CO)4. The origins of this difference are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030111577&hterms=formation+mineral+oxide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dformation%2Bmineral%2Boxide','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030111577&hterms=formation+mineral+oxide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dformation%2Bmineral%2Boxide"><span><span class="hlt">Fe-Ti-Cr</span>-Oxides in Martian Meteorite EETA79001 Studied by Point-counting Procedure 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>Wang, Alian; Kuebler, Karla E.; Jolliff, Bradley L.; Haskin, Larry A.</p> <p>2003-01-01</p> <p><span class="hlt">Fe-Ti-Cr</span>-Oxide minerals contain much information about rock petrogenesis and alteration. Among the most important in the petrology of common intrusive and extrusive rocks are those of the <span class="hlt">Fe</span>O-TiO2-<span class="hlt">Cr</span>2O3 compositional system chromite, ulv spinel-magnetite, and ilmenite-hematite. These minerals retain memories of oxygen fugacity. Their exsolution into companion mineral pairs give constraints on formation temperature and cooling rate. Laser Raman spectroscopy is anticipated to be a powerful technique for characterization of materials on the surface of Mars. A Mars Microbeam Raman Spectrometer (MMRS) is under development. It combines a micro sized laser beam and an automatic point-counting mechanism, and so can detect minor minerals or weak Raman-scattering phases such as <span class="hlt">Fe</span>- Ti-<span class="hlt">Cr</span>-oxides in mixtures (rocks & soils), and provide information on grain size and mineral mode. Most <span class="hlt">Fe-Ti-Cr</span>-oxides produce weaker Raman signals than those from oxyanionic minerals, e.g. carbonates, sulfates, phosphates, and silicates, partly because most of them are intrinsically weaker Raman scatters, and partly because their dark colors limit the penetration depth of the excitation laser beam (visible wavelength) and of the Raman radiation produced. The purpose of this study is to show how well the <span class="hlt">Fe-Ti-Cr</span>-oxides can be characterized by on-surface planetary exploration using Raman spectroscopy. We studied the basic Raman features of common examples of these minerals using well-characterized individual mineral grains. The knowledge gained was then used to study the <span class="hlt">Fe-Ti-Cr</span>-oxides in Martian meteorite EETA79001, especially effects of compositional and structural variations on their Raman features.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JMMM..310E.618K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JMMM..310E.618K"><span>Crystallographic and magnetic properties of sol-gel synthesized T xCo 1-x<span class="hlt">Fe</span> 2O 4 (T=Mn and <span class="hlt">Cr</span>) thin films</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Kwang Joo; Kyung Kim, Hee; Ran Park, Young; Choi, Seung-li; Eun Kim, Sung; Jung Lee, Hee; Yun Park, Jae; Jin Kim, Sam</p> <p></p> <p>Effects of Mn and <span class="hlt">Cr</span> substitution for Co on crystallographic and magnetic properties of inverse-spinel Co<span class="hlt">Fe</span> 2O 4 thin films were investigated. The crystal structure of the samples remain cubic for x<1 with the lattice constant ( a0) increasing with x for Mn doping and remaining constant for <span class="hlt">Cr</span> doping. Tetrahedral <span class="hlt">Fe</span> 2+ ions were detected in <span class="hlt">Cr</span> xCo 1-x<span class="hlt">Fe</span> 2O 4 by Mössbauer spectroscopy while no such ions existed in Mn xCo 1-x<span class="hlt">Fe</span> 2O 4. The appearance of the tetrahedral <span class="hlt">Fe</span> 2+ ions can be explained in terms of the <span class="hlt">Cr</span> 3+ substitution for the octahedral Co 2+ sites with the resultant charge imbalance being compensated by a reduction of the tetrahedral <span class="hlt">Fe</span> 3+ into <span class="hlt">Fe</span> 2+. The observed variation in a0 and magnetic properties can be partly explained in terms of Mn 2+ and <span class="hlt">Cr</span> 3+ substitution of octahedral sites in Mn xCo 1-x<span class="hlt">Fe</span> 2O 4 and <span class="hlt">Cr</span> xCo 1-x<span class="hlt">Fe</span> 2O 4, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1376503-magnetic-properties-crmnfeconi-high-entropy-alloy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1376503-magnetic-properties-crmnfeconi-high-entropy-alloy"><span>Magnetic properties of the <span class="hlt">CrMnFe</span>CoNi high-entropy alloy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Schneeweiss, Oldřich; Friák, Martin; Dudová, Marie; ...</p> <p>2017-07-28</p> <p>In this paper, we present experimental data showing that the equiatomic <span class="hlt">CrMnFe</span>CoNi high-entropy alloy undergoes two magnetic transformations at temperatures below 100 K while maintaining its fcc structure down to 3 K. The first transition, paramagnetic to spin glass, was detected at 93 K and the second transition of the ferromagnetic type occurred at 38 K. Field-assisted cooling below 38 K resulted in a systematic vertical shift of the hysteresis curves. Strength and direction of the associated magnetization bias was proportional to the strength and direction of the cooling field and shows a linear dependence with a slope of 0.006more » ± 0.001 emu T. The local magnetic moments of individual atoms in the <span class="hlt">CrMnFe</span>CoNi quinary fcc random solid solution were investigated by ab initio (electronic density functional theory) calculations. Results of the numerical analysis suggest that, irrespective of the initial configuration of local magnetic moments, the magnetic moments associated with <span class="hlt">Cr</span> atoms align antiferromagnetically with respect to a cumulative magnetic moment of their first coordination shell. The ab initio calculations further showed that the magnetic moments of <span class="hlt">Fe</span> and Mn atoms remain strong (between 1.5 and 2 μ B), while the local moments of Ni atoms effectively vanish. Finally, these results indicate that interactions of Mn- and/or <span class="hlt">Fe</span>-located moments with the surrounding magnetic structure account for the observed macroscopic magnetization bias.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ApSS..264..391H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ApSS..264..391H"><span>Electrochemically deposited cobalt/platinum (Co/Pt) film into porous <span class="hlt">silicon</span>: Structural investigation and magnetic properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harraz, F. A.; Salem, A. M.; Mohamed, B. A.; Kandil, A.; Ibrahim, I. A.</p> <p>2013-01-01</p> <p>A nanostructured CoPt magnetic film was deposited from a single electrolyte into porous <span class="hlt">silicon</span> <span class="hlt">layer</span> by an electrochemical technique, followed by annealing at 600 °C in Ar atmosphere during which the CoPt alloy was converted to L10 ordered phase. Porous <span class="hlt">silicon</span> with pore diameter between 5 and 100 nm was firstly fabricated by galvanostatic anodization of n-type <span class="hlt">silicon</span> wafer in the presence of <span class="hlt">Cr</span>O3 as oxidizing agent and ethanol or sodium lauryl sulfate as surfactants. The role of the surfactant on the produced pore size and morphology was investigated by means of UV-vis spectra. As-formed porous <span class="hlt">silicon</span> was consequently used as a template for the electrodeposition of magnetic CoPt film. The phase formation, microstructure and the magnetic properties were fully analyzed by XRD, <span class="hlt">FE</span>-SEM, EDS and VSM measurements. It was found that, upon annealing the coercivity was significantly increased due to the transformation to the L10 ordered structure. The saturation magnetization and remanence ratio were also found to increase, indicating no loss of Co content or oxidation reaction after the annealing. Results of synthesis and characterization of CoPt/porous <span class="hlt">silicon</span> nanocomposite are addressed and thoroughly discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/20020590-high-temperature-oxidation-behavior-mechanism-new-type-wrought-ni-fe-cr-al-superalloy-up','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/20020590-high-temperature-oxidation-behavior-mechanism-new-type-wrought-ni-fe-cr-al-superalloy-up"><span>High-temperature oxidation behavior and mechanism of a new type of wrought Ni-<span class="hlt">Fe-Cr</span>-Al superalloy up to 1300 C</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>Huang, J.; Fang, H.; Fu, X.</p> <p></p> <p>The oxidation behavior of a new type of wrought Ni-<span class="hlt">Fe-Cr</span>-Al superalloys has been investigated systematically in the temperature range of 1,100 to 1,300 C. Results are compared with those of alloy 214, Inconel 600, and GH 3030. It is shown that the oxidation resistance of the new superalloys is excellent and much better than that of the comparison alloys. Scanning electron microscopy (SEM), electron probe microanalysis (EPMA), and X-ray diffraction (XRD) experiments reveal that the excellent oxidation resistance of the new superalloy is due to the formation of a dense, stable and continuous Al{sub 2}O{sub 3} and <span class="hlt">Cr</span>{sub 2}O{sub 3}more » oxide <span class="hlt">layer</span> at high temperatures. Differential thermal analysis (DTA) shows that the formation of <span class="hlt">Cr</span>{sub 2}O{sub 3} and Al{sub 2}O{sub 3} oxide <span class="hlt">layers</span> on the new superalloy reaches a maximum at 1,060 and 1,356 C, respectively. The <span class="hlt">Cr</span>{sub 2}O{sub 3} <span class="hlt">layer</span> peels off easily, and the single dense Al{sub 2}O{sub 3} <span class="hlt">layer</span> remains, giving good oxidation resistance at temperatures higher than 1,150 C. In addition, the new superalloy possesses high mechanical strength at high temperatures. On-site tests showed that the new superalloy has ideal oxidation resistance and can be used at high temperatures up to 1,300 C in various oxidizing and corrosion atmospheres, such as those containing SO{sub 2}, CO{sub 2} etc., for long periods.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1394351','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1394351"><span>Development of Computational Tools for Modeling Thermal and Radiation Effects on Grain Boundary Segregation and Precipitation in <span class="hlt">Fe-Cr</span>-Ni-based Alloys</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>Yang, Ying</p> <p></p> <p>This work aims at developing computational tools for modeling thermal and radiation effects on solute segregation at grain boundaries (GBs) and precipitation. This report described two major efforts. One is the development of computational tools on integrated modeling of thermal equilibrium segregation (TES) and radiation-induced segregation (RIS), from which synergistic effects of thermal and radiation, pre-existing GB segregation have been taken into consideration. This integrated modeling was used in describing the <span class="hlt">Cr</span> and Ni segregation in the <span class="hlt">Fe-Cr</span>-Ni alloys. The other effort is thermodynamic modeling on the <span class="hlt">Fe-Cr</span>-Ni-Mo system which includes the major alloying elements in the investigated alloys inmore » the Advanced Radiation Resistant Materials (ARRM) program. Through thermodynamic calculation, we provide baseline thermodynamic stability of the hardening phase Ni2(<span class="hlt">Cr</span>,Mo) in selected Ni-based super alloys, and contribute knowledge on mechanistic understanding on the formation of Ni2(<span class="hlt">Cr</span>,Mo) in the irradiated materials. The major outcomes from this work are listed in the following: 1) Under the simultaneous thermal and irradiation conditions, radiation-induced segregation played a dominant role in the GB segregation. The pre-existing GB segregation only affects the subsequent radiation-induced segregation in the short time. For the same element, the segregation tendency of <span class="hlt">Cr</span> and Ni due to TES is opposite to it from RIS. The opposite tendency can lead to the formation of W-shape profile. These findings are consistent with literature observation of the transitory W-shape profile. 2) While TES only affects the distance of one or two atomic <span class="hlt">layers</span> from GBs, the RIS can affect a broader distance from GB. Therefore, the W-shape due to pre-existing GB segregation is much narrower than that due to composition gradient formed during the transient state. Considering the measurement resolution of Auger or STEM analysis, the segregation tendency due to RIS should play a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007JaJAP..46L.465V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007JaJAP..46L.465V"><span>Strong White Photoluminescence from Carbon-Incorporated <span class="hlt">Silicon</span> Oxide Fabricated by Preferential Oxidation of <span class="hlt">Silicon</span> in Nano-Structured Si:C <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vasin, Andriy V.; Ishikawa, Yukari; Shibata, Noriyoshi; Salonen, Jarno; Lehto, Vesa-Pekka</p> <p>2007-05-01</p> <p>A new approach to development of light-emitting SiO2:C <span class="hlt">layers</span> on Si wafer is demonstrated. Carbon-incorporated <span class="hlt">silicon</span> oxide was fabricated by three-step procedure: (1) formation of the porous <span class="hlt">silicon</span> (por-Si) <span class="hlt">layer</span> by ordinary anodization in HF:ethanol solution; (2) carbonization at 1000 °C in acetylene flow (formation of por-Si:C <span class="hlt">layer</span>); (3) oxidation in the flow of moisturized argon at 800 °C (formation of SiO2:C <span class="hlt">layer</span>). Resulting SiO2:C <span class="hlt">layer</span> exhibited very strong and stable white photoluminescence at room temperature. It is shown that high reactivity of water vapor with nano-crystalline <span class="hlt">silicon</span> and inertness with amorphous carbon play a key role in the formation of light-emitting SiO2:C <span class="hlt">layer</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EL....11956003G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EL....11956003G"><span>Cascade debris overlap mechanism of 〈100〉 dislocation loop formation in <span class="hlt">Fe</span> and <span class="hlt">FeCr</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Granberg, F.; Byggmästar, J.; Sand, A. E.; Nordlund, K.</p> <p>2017-09-01</p> <p>Two types of dislocation loops are observed in irradiated α-<span class="hlt">Fe</span>, the 1/2〈111〉 loop and the 〈100〉 loop. Atomistic simulations consistently predict that only the energetically more favourable 1/2〈111〉 loops are formed directly in cascades, leaving the formation mechanism of 〈100〉 loops an unsolved question. We show how 〈100〉 loops can be formed when cascades overlap with random pre-existing primary radiation damage in <span class="hlt">Fe</span> and <span class="hlt">FeCr</span>. This indicates that there are no specific constraints involved in the formation of 〈100〉 loops, and can explain their common occurrence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1253237','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1253237"><span>Evaluation on the Effect of Composition on Radiation Hardening and Embrittlement in Model <span class="hlt">FeCr</span>Al Alloys</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>Field, Kevin G.; Briggs, Samuel A.; Edmondson, Philip</p> <p>2015-09-18</p> <p>This report details the findings of post-radiation mechanical testing and microstructural characterization performed on a series of model and commercial <span class="hlt">FeCr</span>Al alloys to assist with the development of a cladding technology with enhanced accident tolerance. The samples investigated include model alloys with simple ferritic grain structure and two commercial alloys with minor solute additions. These samples were irradiated in the High Flux Isotope Reactor (HFIR) at Oak Ridge National Laboratory (ORNL) up to nominal doses of 7.0 dpa near or at Light Water Reactor (LWR) relevant temperatures (300-400 C). Characterization included a suite of techniques including small angle neutron scatteringmore » (SANS), atom probe tomography (APT), and transmission based electron microscopy techniques. Mechanical testing included tensile tests at room temperature on sub-sized tensile specimens. The goal of this work was to conduct detailed characterization and mechanical testing to begin establishing empirical and/or theoretical structure-property relationships for radiation-induced hardening and embrittlement in the <span class="hlt">FeCr</span>Al alloy class. Development of such relationships will provide insight on the performance of <span class="hlt">FeCr</span>Al alloys in an irradiation environment and will enable further development of the alloy class for applications within a LWR environment. A particular focus was made on establishing trends, including composition and radiation dose. The report highlights in detail the pertinent findings based on this work. This report shows that radiation hardening in the alloys is primarily composition dependent due to the phase separation in the high-<span class="hlt">Cr</span> <span class="hlt">FeCr</span>Al alloys. Other radiation induced/enhanced microstructural features were less dependent on composition and when observed at low number densities, were not a significant contributor to the observed mechanical responses. Pre-existing microstructure in the alloys was found to be important, with grain boundaries and pre</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1456785-elastic-moduli-thermal-expansion-coefficients-medium-entropy-subsystems-crmnfeconi-high-entropy-alloy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1456785-elastic-moduli-thermal-expansion-coefficients-medium-entropy-subsystems-crmnfeconi-high-entropy-alloy"><span>Elastic moduli and thermal expansion coefficients of medium-entropy subsystems of the <span class="hlt">CrMnFe</span>CoNi high-entropy alloy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Laplanche, Guillaume; Gadaud, P.; Barsch, C.; ...</p> <p>2018-02-23</p> <p>Elastic moduli of a set of equiatomic alloys (<span class="hlt">CrFe</span>CoNi, <span class="hlt">Cr</span>CoNi, <span class="hlt">CrFe</span>Ni, <span class="hlt">Fe</span>CoNi, MnCoNi, Mn<span class="hlt">Fe</span>Ni, and CoNi), which are medium-entropy subsystems of the <span class="hlt">CrMnFe</span>CoNi high-entropy alloy were determined as a function of temperature over the range 293 K–1000 K. Thermal expansion coefficients were determined for these alloys over the temperature range 100 K–673 K. All alloys were single-phase and had the face-centered cubic (FCC) crystal structure, except <span class="hlt">CrFe</span>Ni which is a two-phase alloy containing a small amount of body-centered cubic (BCC) precipitates in a FCC matrix. The temperature dependences of thermal expansion coefficients and elastic moduli obtained here are useful formore » quantifying fundamental aspects such as solid solution strengthening, and for structural analysis/design. Furthermore, using the above results, the yield strengths reported in literature for these alloys were normalized by their shear moduli to reveal the influence of shear modulus on solid solution strengthening.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1456785','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1456785"><span>Elastic moduli and thermal expansion coefficients of medium-entropy subsystems of the <span class="hlt">CrMnFe</span>CoNi high-entropy alloy</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>Laplanche, Guillaume; Gadaud, P.; Barsch, C.</p> <p></p> <p>Elastic moduli of a set of equiatomic alloys (<span class="hlt">CrFe</span>CoNi, <span class="hlt">Cr</span>CoNi, <span class="hlt">CrFe</span>Ni, <span class="hlt">Fe</span>CoNi, MnCoNi, Mn<span class="hlt">Fe</span>Ni, and CoNi), which are medium-entropy subsystems of the <span class="hlt">CrMnFe</span>CoNi high-entropy alloy were determined as a function of temperature over the range 293 K–1000 K. Thermal expansion coefficients were determined for these alloys over the temperature range 100 K–673 K. All alloys were single-phase and had the face-centered cubic (FCC) crystal structure, except <span class="hlt">CrFe</span>Ni which is a two-phase alloy containing a small amount of body-centered cubic (BCC) precipitates in a FCC matrix. The temperature dependences of thermal expansion coefficients and elastic moduli obtained here are useful for quantifying fundamental aspects suchmore » as solid solution strengthening, and for structural analysis/design. Furthermore, using the above results, the yield strengths reported in literature for these alloys were normalized by their shear moduli to reveal the influence of shear modulus on solid solution strengthening.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28734357','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28734357"><span>YSZ-based sensor using <span class="hlt">Cr-Fe</span>-based spinel-oxide electrodes for selective detection of CO.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Anggraini, Sri Ayu; Fujio, Yuki; Ikeda, Hiroshi; Miura, Norio</p> <p>2017-08-22</p> <p>A selective carbon monoxide (CO) sensor was developed by the use of both of Cu<span class="hlt">CrFe</span>O 4 and Co<span class="hlt">CrFe</span>O 4 as the sensing electrode (SE) for yttria-stabilized zirconia (YSZ)-based potentiometric sensor. The sensing-characteristic examinations of the YSZ-based sensors using each of spinel oxides as the single-SE sensor showed that Cu<span class="hlt">CrFe</span>O 4 -SE had the ability to detect CO, hydrocarbons and NO x gases, while Co<span class="hlt">CrFe</span>O 4 -SE was sensitive to hydrocarbons and NO x gases. Thus, when both SEs were paired as a combined-SEs sensor, the resulting sensor could generate a selective response to CO at 450 °C under humid conditions. The sensor was also capable of detecting CO in the concentration range of 20-700 ppm. Its sensing mechanism that was examined via polarization-curve measurements was confirmed to be based on mixed-potential model. The CO response generated by the combined-SEs sensor was unaffected by the change of water vapor concentration in the range of 1.3-11.5 vol% H 2 O. Additionally, the sensing performance was stable during 13 days tested. Copyright © 2017 Elsevier B.V. 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_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/2018JNuM..504..221G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JNuM..504..221G"><span>Impact of neutron irradiation on mechanical performance of <span class="hlt">FeCr</span>Al alloy laser-beam weldments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gussev, M. N.; Cakmak, E.; Field, K. G.</p> <p>2018-06-01</p> <p>Oxidation-resistant iron-chromium-aluminum (<span class="hlt">FeCr</span>Al) alloys demonstrate better performance in Loss-of-Coolant Accidents, compared with austenitic- and zirconium-based alloys. However, further deployment of <span class="hlt">FeCr</span>Al-based materials requires detailed characterization of their performance under irradiation; moreover, since welding is one of the key operations in fabrication of light water reactor fuel cladding, <span class="hlt">FeCr</span>Al alloy weldment performance and properties also should be determined prior to and after irradiation. Here, advanced C35M alloy (<span class="hlt">Fe</span>-13%<span class="hlt">Cr</span>-5%Al) and variants with aluminum (+2%) or titanium carbide (+1%) additions were characterized after neutron irradiation in Oak Ridge National Laboratory's High Flux Isotope Reactor at 1.8-1.9 dpa in a temperature range of 195-559 °C. Specimen sets included as-received (AR) materials and specimens after controlled laser-beam welding. Tensile tests with digital image correlation (DIC), scanning electron microscopy-electron back scatter diffraction analysis, fractography, and x-ray tomography analysis were performed. DIC allowed for investigating local yield stress in the weldments, deformation hardening behavior, and plastic anisotropy. Both AR and welded material revealed a high degree of radiation-induced hardening for low-temperature irradiation; however, irradiation at high-temperatures (i.e., 559 °C) had little overall effect on the mechanical performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JMEP...24.1918Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JMEP...24.1918Z"><span>Phase Transformation and Aging Behavior of Al0.5Co<span class="hlt">CrFe</span>NiSi0.2 High-Entropy Alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, C.; Wu, G. F.; Dai, P. Q.</p> <p>2015-05-01</p> <p>An Al0.5Co<span class="hlt">CrFe</span>NiSi0.2 high-entropy alloy was prepared by vacuum arc melting. The alloy was aged from 700 to 1100 °C. The effects of aging on the phase transformation and mechanical performances were explored. The as-cast alloy showed a dendritic (DR) microstructure. The DR region was an <span class="hlt">Fe,Cr</span>-rich FCC phase, while the interdendritic (ID) region was a spinodal structure composed of <span class="hlt">Fe,Cr</span>-rich BCC (A2) and Ni,Al-rich BCC (B2) phases. At aging temperatures between 700 and 900 °C, the <span class="hlt">Fe,Cr</span>-rich BCC (A2) phase in the ID region transformed into σ and <span class="hlt">Fe,Cr</span>-rich FCC phases. Meanwhile, some Ni,Al-rich FCC phase particles precipitated from the DR region. During aging at 1100 °C, the DR microstructure disappeared, and a microstructure composed of <span class="hlt">Fe,Cr</span>-rich FCC and Ni,Al-rich BCC (B2) phases both possessing a lamellar shape was developed. The alloy exhibited evident hardening and lower tensile strain when the aging temperature was lower than 1000 °C, which was mainly attributed to the generation of the σ phase in the ID region. However, a contrasting behavior was observed when the aging temperature was higher than 1000 °C, which was attributed to the redissolution of the σ phase and the microstructure coarsening.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29729604','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29729604"><span>A novel method for vanadium slag comprehensive utilization to synthesize Zn-Mn ferrite and <span class="hlt">Fe-V-Cr</span> alloy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Shi-Yuan; Li, Shu-Jin; Wu, Shun; Wang, Li-Jun; Chou, Kuo-Chih</p> <p>2018-07-15</p> <p>Vanadium slag is a by-product from steelmaking process of vanadium-titanium magnetite, which mainly contains <span class="hlt">Fe</span>O, MnO, V 2 O 3 , and <span class="hlt">Cr</span> 2 O 3 , The elements <span class="hlt">Fe</span> and Mn are major components of Mn-Zn ferrite. The elements V and <span class="hlt">Cr</span> are major components of V-<span class="hlt">Cr</span> alloy. In view of the potential application in these study, a Mn 0.8 Zn 0.2 <span class="hlt">Fe</span> 2 O 4 of high saturation magnetization (Ms = 68.6 emu/g) and low coercivity (Hc = 3.3 Oe) was successfully synthesized from the leaching solutions of vanadium slag by adding appropriate chemical reagents, ZnCl 2 and MnCl 2 ·4H 2 O, via roasting at 1300 °C for 1 h. The minor components (CaO and SiO 2 ) in the leaching solution of vanadium slag segregated to the grain boundaries resulting in increasing the resistivity of ferrite. The value of DC resistivity of Mn 0.8 Zn 0.2 <span class="hlt">Fe</span> 2 O 4 at 25 °C reached 1230.7Ω m. The residue containing <span class="hlt">Fe</span>, V and <span class="hlt">Cr</span> was chlorinated by AlCl 3 and the <span class="hlt">Fe</span> 3+ , V 3+ , and <span class="hlt">Cr</span> 3+ ions were released into the NaCl-KCl eutectic. The current-time curve for the electrolysis of molten salt was investigated. Alloy (<span class="hlt">Fe</span>, V, and <span class="hlt">Cr</span>) of granular shape was obtained. The residue can be used to produce the mulite. This process provided a new approach to utilize slag from steelmaking. Copyright © 2018 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29749421','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29749421"><span>Highly-active oxygen evolution electrocatalyzed by an <span class="hlt">Fe</span>-doped Ni<span class="hlt">Cr</span>2O4 nanoparticle film.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhao, Jinxiu; Li, Xianghong; Cui, Guanwei; Sun, Xuping</p> <p>2018-05-11</p> <p>Alkaline water splitting offers a simple method for the mass production of hydrogen but suffers from the sluggish kinetics of the anodic oxygen evolution reaction (OER). Here, we report on the development of an <span class="hlt">Fe</span>-doped Ni<span class="hlt">Cr</span>2O4 nanoparticle film on Ni foam (<span class="hlt">Fe-NiCr</span>2O4/NF) as a non-noble-metal OER electrocatalyst with superior catalytic activity at alkaline pH. Such <span class="hlt">Fe-NiCr</span>2O4/NF demands overpotentials as low as 228 and 318 mV to drive current densities of 20 and 500 mA cm-2, respectively, in 1.0 M KOH. Notably, it also shows strong long-term electrochemical durability with its activity being retained for at least 60 h.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991JAP....69.4789G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991JAP....69.4789G"><span><span class="hlt">Layered</span> magnetic structures: Antiferromagnetic-type interlayer coupling and magnetoresistance due to antiparallel alignment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grünberg, P.; Demokritov, S.; Fuss, A.; Vohl, M.; Wolf, J. A.</p> <p>1991-04-01</p> <p><span class="hlt">Layered</span> <span class="hlt">Fe/Cr</span> structures are known to display antiferromagnetic-type interlayer coupling and a new magnetoresistance (MR) effect due to antiparallel magnetization alignment. The strength of the coupling is found to be similar in multilayered structures and in double <span class="hlt">layers</span>. The oscillatory behavior of the coupling, previously found by Parkin, More, and Roche [Phys. Rev. Lett. 64, 2304 (1990)] on sputtered polycrystalline samples, is here confirmed for epitaxial samples, obtained by thermal evaporation. The new MR effect is interpreted as due to a spin-dependent scattering of the electrons at the <span class="hlt">Fe-Cr</span> interfaces. The investigations have been extended to <span class="hlt">Fe</span>/V, <span class="hlt">Fe</span>/Mn, <span class="hlt">Fe</span>/Cu, Co/Au, Co/<span class="hlt">Cr</span>, and Co/Cu structures where the antiparallel alignment of the ferromagnetic <span class="hlt">layers</span> is obtained via hysteresis effects. A MR effect due to antiparallel alignment, which is strong for Co/Au and Co/Cu but weak in the other cases, has been found.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29772182','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29772182"><span>Oxidation of <span class="hlt">Cr(III)-Fe</span>(III) Mixed-phase Hydroxides by Chlorine: Implications on the Control of Hexavalent Chromium in Drinking Water.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chebeir, Michelle; Liu, Haizhou</p> <p>2018-05-17</p> <p>The occurrence of chromium (<span class="hlt">Cr</span>) as an inorganic contaminant in drinking water is widely reported. One source of <span class="hlt">Cr</span> is its accumulation in iron-containing corrosion scales of drinking water distribution systems as <span class="hlt">Cr(III)-Fe</span>(III) hydroxide, i.e., Fex<span class="hlt">Cr</span>(1-x)(OH)3(s), where x represents the <span class="hlt">Fe</span>(III) molar content and typically varies between 0.25 and 0.75. This study investigated the kinetics of inadvertent hexavalent chromium <span class="hlt">Cr</span>(VI) formation via the oxidation of Fex<span class="hlt">Cr</span>(1-x)(OH)3(s) by chlorine as a residual disinfectant in drinking water, and examined the impacts of <span class="hlt">Fe</span>(III) content and drinking water chemical parameters including pH, bromide and bicarbonate on the rate of <span class="hlt">Cr</span>(VI) formation. Data showed that an increase in <span class="hlt">Fe</span>(III) molar content resulted in a significant decrease in the stoichiometric <span class="hlt">Cr</span>(VI) yield and the rate of <span class="hlt">Cr</span>(VI) formation, mainly due to chlorine decay induced by <span class="hlt">Fe</span>(III) surface sites. An increase in bicarbonate enhanced the rate of <span class="hlt">Cr</span>(VI) formation, likely due to the formation of <span class="hlt">Fe</span>(III)-carbonato surface complexes that slowed down the scavenging reaction with chlorine. The presence of bromide significantly accelerated the oxidation of Fex<span class="hlt">Cr</span>(1-x)(OH)3(s) by chlorine, resulting from the catalytic effect of bromide acting as an electron shuttle. A higher solution pH between 6 and 8.5 slowed down the oxidation of <span class="hlt">Cr</span>(III) by chlorine. These findings suggested that the oxidative conversion of chromium-containing iron corrosion products in drinking water distribution systems can lead to the occurrence of <span class="hlt">Cr</span>(VI) at the tap, and the abundance of iron, and a careful control of pH, bicarbonate and bromide levels can assist the control of <span class="hlt">Cr</span>(VI) formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhD...50r5002C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhD...50r5002C"><span>Interplay of electronic, structural and magnetic properties as the driving feature of high-entropy Co<span class="hlt">CrFe</span>NiPd alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calvo-Dahlborg, M.; Cornide, J.; Tobola, J.; Nguyen-Manh, D.; Wróbel, J. S.; Juraszek, J.; Jouen, S.; Dahlborg, U.</p> <p>2017-05-01</p> <p>The structural and magnetic properties of Co<span class="hlt">CrFe</span> y Ni and Co<span class="hlt">CrFe</span>Ni-Pd x alloys earlier investigated experimentally by x-ray and neutron diffraction techniques and magnetometry have been theoretically reproduced using two complementary approaches for electronic structure calculations, i.e. the Korringa-Kohn-Rostoker method with the coherent potential approximation (KKR-CPA) and implemented in the ab initio framework of density functional theory and the Vienna ab initio simulation package (VASP) for supercell models of high-entropy alloy (HEA) structures. The comparison between experimental results and calculations of the lattice constants by both calculation methods indicate that the structure of Co<span class="hlt">CrFe</span> y Ni is well described by ordered fcc configurations. The values of local magnetic moments on <span class="hlt">Fe</span>, Co, <span class="hlt">Cr</span>, and Ni atoms depend not only on the Pd concentration but on chemical disordering. In the case of the Co<span class="hlt">CrFe</span>Ni-Pd x alloys, the KKR-CPA and the VASP calculations of disordered configurations reproduce the experimental values at 5 K up to equimolar composition and at 300 K above. The experimental values above the equimolar composition at 5 K are not satisfactorily reproduced by any of the calculations. The divergence between the experimental and calculated values is related to the variation of the ferromagnetic to paramagnetic transition temperature as a function of palladium content and to the existence of several phases, <span class="hlt">FeCoCr</span>-rich above room temperature and <span class="hlt">FeCr</span>Pd-rich below, observed by diffraction and detected by microscopy and atom probe investigations. VASP calculations of a <span class="hlt">FeCr</span>Pd-rich phase effectively reproduced both the lattice constant and magnetization of the alloy above equimolar composition. An important conclusion of this work is that the combined analysis of the electronic, structural, and magnetic properties plays an important role in understanding the complexity of magnetic HEAs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5413246','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/5413246"><span>Heat treatment of Ni<span class="hlt">CrFe</span> alloy 600 to optimize resistance to intergranular stress corrosion</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Steeves, A.F.; Bibb, A.E.</p> <p></p> <p>A process of producing a Ni<span class="hlt">CrFe</span> alloy having a high resistance to stress corrosion cracking comprises heating a Ni<span class="hlt">CrFe</span> alloy to a temperature sufficient to enable the carbon present in the alloy body in the form of carbide deposits to enter into solution, rapidly cooling the alloy body, and heating the cooled body to a temperature between 1100 to 1500/sup 0/F for about 1 to 30 hours.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27596718','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27596718"><span>Growth characteristics of primary M7C3 carbide in hypereutectic <span class="hlt">Fe-Cr</span>-C alloy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Sha; Zhou, Yefei; Xing, Xiaolei; Wang, Jibo; Ren, Xuejun; Yang, Qingxiang</p> <p>2016-09-06</p> <p>The microstructure of the hypereutectic <span class="hlt">Fe-Cr</span>-C alloy is observed by optical microscopy (OM). The initial growth morphology, the crystallographic structure, the semi-molten morphology and the stacking faults of the primary M7C3 carbide are observed by scanning electron microscopy (SEM) and transmission electron microscopy (TEM). The in-suit growth process of the primary M7C3 carbide was observed by confocal laser microscope (CLM). It is found that the primary M7C3 carbide in hypereutectic <span class="hlt">Fe-Cr</span>-C alloy is irregular polygonal shape with several hollows in the center and gaps on the edge. Some primary M7C3 carbides are formed by <span class="hlt">layers</span> of shell or/and consist of multiple parts. In the initial growth period, the primary M7C3 carbide forms protrusion parallel to {} crystal planes. The extending and revolving protrusion forms the carbide shell. The electron backscattered diffraction (EBSD) maps show that the primary M7C3 carbide consists of multiple parts. The semi-molten M7C3 carbide contains unmelted shell and several small-scale carbides inside, which further proves that the primary M7C3 carbide is not an overall block. It is believed that the coalescence of the primary M7C3 carbides is ascribed to the growing condition of the protrusion and the gap filling process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5011776','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5011776"><span>Growth characteristics of primary M7C3 carbide in hypereutectic <span class="hlt">Fe-Cr</span>-C alloy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Liu, Sha; Zhou, Yefei; Xing, Xiaolei; Wang, Jibo; Ren, Xuejun; Yang, Qingxiang</p> <p>2016-01-01</p> <p>The microstructure of the hypereutectic <span class="hlt">Fe-Cr</span>-C alloy is observed by optical microscopy (OM). The initial growth morphology, the crystallographic structure, the semi-molten morphology and the stacking faults of the primary M7C3 carbide are observed by scanning electron microscopy (SEM) and transmission electron microscopy (TEM). The in-suit growth process of the primary M7C3 carbide was observed by confocal laser microscope (CLM). It is found that the primary M7C3 carbide in hypereutectic <span class="hlt">Fe-Cr</span>-C alloy is irregular polygonal shape with several hollows in the center and gaps on the edge. Some primary M7C3 carbides are formed by <span class="hlt">layers</span> of shell or/and consist of multiple parts. In the initial growth period, the primary M7C3 carbide forms protrusion parallel to {} crystal planes. The extending and revolving protrusion forms the carbide shell. The electron backscattered diffraction (EBSD) maps show that the primary M7C3 carbide consists of multiple parts. The semi-molten M7C3 carbide contains unmelted shell and several small-scale carbides inside, which further proves that the primary M7C3 carbide is not an overall block. It is believed that the coalescence of the primary M7C3 carbides is ascribed to the growing condition of the protrusion and the gap filling process. PMID:27596718</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000030652','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000030652"><span>Cyclic Oxidation of <span class="hlt">FeCr</span>AlY/Al2O3 Composites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nesbitt, James A.; Draper, Susan L.; Barrett, Charles A.</p> <p>1999-01-01</p> <p>Three-ply <span class="hlt">FeCr</span>AlY/Al2O3 composites and <span class="hlt">FeCr</span>AlY matrix-only samples were cyclically oxidized at 1000 C and 1100 C for up to 1000 1-hr cycles. Fiber ends were exposed at the ends of the composite samples. Following cyclic oxidation, cracks running parallel to and perpendicular to the fibers were observed on the large surface of the composite. In addition, there was evidence of increased scale damage and spallation around the exposed fiber ends, particularly around the middle ply fibers. This damage was more pronounced at the higher temperature. The exposed fiber ends showed cracking between fibers in the outer plies, occasionally with <span class="hlt">Fe</span> and <span class="hlt">Cr</span>-rich oxides growing out of the cracks. Large gaps developed at the fiber/matrix interface around many of the fibers, especially those in the outer plies. Oxygen penetrated many of these gaps resulting in significant oxide formation at the fiber/matrix interface far within the composite sample. Around several fibers, the matrix was also internally oxidized showing Al2O3 precipitates in a radial band around the fibers. The results show that these composites have poor cyclic oxidation resistance due to the CTE mismatch and inadequate fiber/matrix bond strength at temperatures of 1000 C and above.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005JSSCh.178.1830G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005JSSCh.178.1830G"><span>Synthesis and characterization of Cd <span class="hlt">Cr</span> and Zn Cd <span class="hlt">Cr</span> <span class="hlt">layered</span> double hydroxides intercalated with dodecyl sulfate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Ying; Zhang, He; Zhao, Lan; Li, Guo-Dong; Chen, Jie-Sheng; Xu, Lin</p> <p>2005-06-01</p> <p>Cd-<span class="hlt">Cr</span> and Zn-Cd-<span class="hlt">Cr</span> <span class="hlt">layered</span> double hydroxides (Cd<span class="hlt">Cr</span>-LDH and ZnCd<span class="hlt">Cr</span>-LDH) containing alkyl sulfate as the interlamellar anion have been prepared through a coprecipitation technique. The resulting compounds were characterized using X-ray diffraction, infrared spectroscopy, thermogravimetric analysis, and scanning electron microscopy. Magnetic property measurements indicate that antiferromagnetic interactions occur between the chromium ions in the two compounds at low temperatures. The introduction of zinc influences the ligand field of <span class="hlt">Cr</span> III and the <span class="hlt">Cr</span> III-<span class="hlt">Cr</span> III interactions in the LDH compound. It is found that both Cd<span class="hlt">Cr</span>-LDH and ZnCd<span class="hlt">Cr</span>-LDH can be delaminated by dispersion in formamide, leading to translucent and stable colloidal solutions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..440.1277Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..440.1277Z"><span>Polyethylenimine functionalized <span class="hlt">Fe</span>3O4/steam-exploded rice straw composite as an efficient adsorbent for <span class="hlt">Cr</span>(VI) removal</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Shengli; Wang, Zhikai; Chen, Haoyu; Kai, Chengcheng; Jiang, Man; Wang, Qun; Zhou, Zuowan</p> <p>2018-05-01</p> <p>Polyethyleneimine functionalized <span class="hlt">Fe</span>3O4/steam-exploded rice straw composite (<span class="hlt">Fe</span>3O4-PEI-SERS), which combines magnetic separation with adsorption of PEI functionalized biosorbent, was successfully prepared via a simple glutaraldehyde crosslinking method. Its adsorption potential for the removal of <span class="hlt">Cr</span>(VI) was systematically studied in batch mode. Results showed that <span class="hlt">Cr</span>(VI) adsorption on <span class="hlt">Fe</span>3O4-PEI-SESERS was highly pH-dependent, and the optimum pH was 2.0. The time to reach equilibrium was related to initial <span class="hlt">Cr</span>(VI) concentration and was 1 and 6 h for 200 and 300 mg/L of <span class="hlt">Cr</span>(VI), respectively. The adsorption system followed pseudo-second-order kinetic model and Langmuir isotherm. Its maximum adsorption capacity was 280.11, 317.46 and 338.98 mg/g at 25, 35 and 45 °C, respectively. The competitive uptake from coexisting ions (K+, Na+, Cu2+, Cl- and NO3-) was insignificant except SO42-. After six adsorption/desorption cycles, the adsorbent retained good adsorption capacity. The <span class="hlt">Cr</span>(VI) removal involved its partial reduction into <span class="hlt">Cr</span>(III). Due to the properties of high adsorption capacity, strong magnetic responsiveness, good reusability and <span class="hlt">Cr</span>(VI) detoxification, the <span class="hlt">Fe</span>3O4-PEI-SESERS has a potential application in <span class="hlt">Cr</span>(VI) removal from wastewater.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhRvB..81v4410C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhRvB..81v4410C"><span>Antiferromagnetic <span class="hlt">layer</span> thickness dependence of noncollinear uniaxial and unidirectional anisotropies in Ni<span class="hlt">Fe/FeMn/CoFe</span> trilayers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, Hyeok-Cheol; You, Chun-Yeol; Kim, Ki-Yeon; Lee, Jeong-Soo; Shim, Je-Ho; Kim, Dong-Hyun</p> <p>2010-06-01</p> <p>We have investigated the dependence of magnetic anisotropies of the exchange-biased Ni<span class="hlt">Fe/FeMn/CoFe</span> trilayers on the antiferromagnetic (AF) <span class="hlt">layer</span> thickness (tAF) by measuring in-plane angular-dependent ferromagnetic resonance fields. The resonance fields of Ni<span class="hlt">Fe</span> and Co<span class="hlt">Fe</span> sublayers are shifted to lower and higher values compared to those of single unbiased ferromagnetic (F) <span class="hlt">layers</span>, respectively, due to the interfacial exchange coupling when tAF≥2nm . In-plane angular dependence of resonance field reveals that uniaxial and unidirectional anisotropies coexist in the film plane, however, they are not collinear with each other. It is found that these peculiar noncollinear anisotropies significantly depend on tAF . The angle of misalignment displays a maximum around tAF=5nm and converges to zero when tAF is thicker than 10 nm. Contributions from thickness-dependent AF anisotropy and spin frustrations at both F/AF interfaces due to the structural imperfections should be accounted in order to understand the AF-<span class="hlt">layer</span> thickness dependence of noncollinear magnetic anisotropies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JNuM..500..192R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JNuM..500..192R"><span>On α‧ precipitate composition in thermally annealed and neutron-irradiated <span class="hlt">Fe</span>- 9-18<span class="hlt">Cr</span> alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reese, Elaina R.; Bachhav, Mukesh; Wells, Peter; Yamamoto, Takuya; Robert Odette, G.; Marquis, Emmanuelle A.</p> <p>2018-03-01</p> <p>Ferritic-martensitic steels are leading candidates for many nuclear energy applications. However, formation of nanoscale α‧ precipitates during thermal aging at temperatures above 450 °C, or during neutron irradiation at lower temperatures, makes these <span class="hlt">Fe-Cr</span> steels susceptible to embrittlement. To complement the existing literature, a series of <span class="hlt">Fe</span>-9 to 18 <span class="hlt">Cr</span> alloys were neutron-irradiated at temperatures between 320 and 455 °C up to doses of 20 dpa. In addition, post-irradiation annealing treatments at 500 and 600 °C were performed on a neutron-irradiated <span class="hlt">Fe</span>-18 <span class="hlt">Cr</span> alloy to validate the α-α‧ phase boundary. The microstructures were characterized using atom probe tomography and the results were analyzed in light of the existing literature. Under neutron irradiation and thermal annealing, the measured α‧ concentrations ranged from ∼81 to 96 at.% <span class="hlt">Cr</span>, as influenced by temperature, precipitate size, technique artifacts, and, possibly, cascade ballistic mixing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1410934','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1410934"><span>Radiation Tolerance of Controlled Fusion Welds in High Temperature Oxidation Resistant <span class="hlt">FeCr</span>Al Alloys</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>Gussev, Maxim N.; Field, Kevin G.</p> <p></p> <p>High temperature oxidation resistant iron-chromium-aluminum (<span class="hlt">FeCr</span>Al) alloys are candidate alloys for nuclear applications due to their exceptional performance during off-normal conditions such as a loss-of-coolant accident (LOCA) compared to currently deployed zirconium-based claddings [1]. A series of studies have been completed to determine the weldability of the <span class="hlt">FeCr</span>Al alloy class and investigate the weldment performance in the as-received (non-irradiated) state [2,3]. These initial studies have shown the general effects of composition and microstructure on the weldability of <span class="hlt">FeCr</span>Al alloys. Given this, limited details on the radiation tolerance of <span class="hlt">FeCr</span>Al alloys and their weldments exist. Here, the highest priority candidate <span class="hlt">FeCr</span>Almore » alloys and their weldments have been investigated after irradiation to enable a better understanding of <span class="hlt">FeCr</span>Al alloy weldment performance within a high-intensity neutron field. The alloys examined include C35M (<span class="hlt">Fe</span>-13%<span class="hlt">Cr</span>-5% Al) and variants with aluminum (+2%) or titanium carbide (+1%) additions. Two different sub-sized tensile geometries, SS-J type and SS-2E (or SS-mini), were neutron irradiated in the High Flux Isotope Reactor to 1.8-1.9 displacements per atom (dpa) in the temperature range of 195°C to 559°C. Post irradiation examination of the candidate alloys was completed and included uniaxial tensile tests coupled with digital image correlation (DIC), scanning electron microscopy-electron back scattered diffraction analysis (SEM-EBSD), and SEM-based fractography. In addition to weldment testing, non-welded parent material was examined as a direct comparison between welded and non-welded specimen performance. Both welded and non-welded specimens showed a high degree of radiation-induced hardening near irradiation temperatures of 200°C, moderate radiation-induced hardening near temperatures of 360°C, and almost no radiation-induced hardening at elevated temperatures near 550°C. Additionally, low-temperature irradiations</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApSS..396.1420Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApSS..396.1420Y"><span>Microstructure and corrosion properties of <span class="hlt">CrMnFe</span>CoNi high entropy alloy coating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ye, Qingfeng; Feng, Kai; Li, Zhuguo; Lu, Fenggui; Li, Ruifeng; Huang, Jian; Wu, Yixiong</p> <p>2017-02-01</p> <p>Equimolar <span class="hlt">CrMnFe</span>CoNi high entropy alloy (HEA) is one of the most notable single phase multi-component alloys up-to-date with promising mechanical properties at cryogenic temperatures. However, the study on the corrosion behavior of <span class="hlt">CrMnFe</span>CoNi HEA coating has still been lacking. In this paper, HEA coating with a nominal composition of <span class="hlt">CrMnFe</span>CoNi is fabricated by laser surface alloying and studied in detail. Microstructure and chemical composition are determined by X-ray diffraction (XRD), optical microscope (OM), scanning electron microscope (SEM) and energy dispersive spectrometer (EDS). Potentiodynamic polarization and electrochemical impedance spectroscopy (EIS) are used to investigate the corrosion behavior. The coating forms a simple FCC phase with an identical dendritic structure composed of <span class="hlt">Fe</span>/Co/Ni-rich dendrites and Mn/Ni-rich interdendrites. Both in 3.5 wt.% NaCl solution and 0.5 M sulfuric acid the coating exhibits nobler corrosion resistance than A36 steel substrate and even lower icorr than 304 stainless steel (304SS). EIS plots coupled with fitted parameters reveal that a spontaneous protective film is formed and developed during immersion in 0.5 M sulfuric acid. The fitted Rt value reaches its maximum at 24 h during a 48 h' immersion test, indicating the passive film starts to break down after that. EDS analysis conducted on a corroded surface immersed in 0.5 M H2SO4 reveals that corrosion starts from <span class="hlt">Cr</span>-depleted interdendrites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1427635-effect-electrons-defect-properties-equiatomic-nicocr-nicofecr-concentrated-solid-solution-alloys','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1427635-effect-electrons-defect-properties-equiatomic-nicocr-nicofecr-concentrated-solid-solution-alloys"><span>Effect of d electrons on defect properties in equiatomic NiCo<span class="hlt">Cr</span> and NiCo<span class="hlt">FeCr</span> concentrated solid solution alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zhao, Shijun; Egami, Takeshi; Stocks, G. Malcolm; ...</p> <p>2018-01-01</p> <p>Here, the role of d electrons in determining distributions of formation and migration energies for point defects in equiatomic NiCo<span class="hlt">Cr</span> and NiCo<span class="hlt">FeCr</span> concentrated solid solution alloys (CSAs) are studied regarding electron density deformation flexibility based on first-principles calculations. The disordered state is taken into account by constructing special quasirandom structures. The migration barriers are determined by directly optimizing the saddle point. It is found that the formation energies of interstitials in CSAs are lower than those in pure Ni, whereas the formation energies of vacancies are higher. In both NiCo<span class="hlt">Cr</span> and NiCo<span class="hlt">FeCr</span>, Co-related dumbbell interstitials exhibit lower formation energies. Notably,more » the distributions of migration energies for <span class="hlt">Cr</span> interstitials and vacancies exhibit a remarkable overlap region. A detailed analysis of electronic properties reveals that the electronic charge deformation flexibility regarding e g to t 2g transition has a dominant effect on defect energetics for different elements in CSAs. Thus the electron deformation ability is suggested as a key factor in understanding the peculiar defect behavior in CSAs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1427635-effect-electrons-defect-properties-equiatomic-nicocr-nicofecr-concentrated-solid-solution-alloys','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1427635-effect-electrons-defect-properties-equiatomic-nicocr-nicofecr-concentrated-solid-solution-alloys"><span>Effect of d electrons on defect properties in equiatomic NiCo<span class="hlt">Cr</span> and NiCo<span class="hlt">FeCr</span> concentrated solid solution alloys</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>Zhao, Shijun; Egami, Takeshi; Stocks, G. Malcolm</p> <p></p> <p>Here, the role of d electrons in determining distributions of formation and migration energies for point defects in equiatomic NiCo<span class="hlt">Cr</span> and NiCo<span class="hlt">FeCr</span> concentrated solid solution alloys (CSAs) are studied regarding electron density deformation flexibility based on first-principles calculations. The disordered state is taken into account by constructing special quasirandom structures. The migration barriers are determined by directly optimizing the saddle point. It is found that the formation energies of interstitials in CSAs are lower than those in pure Ni, whereas the formation energies of vacancies are higher. In both NiCo<span class="hlt">Cr</span> and NiCo<span class="hlt">FeCr</span>, Co-related dumbbell interstitials exhibit lower formation energies. Notably,more » the distributions of migration energies for <span class="hlt">Cr</span> interstitials and vacancies exhibit a remarkable overlap region. A detailed analysis of electronic properties reveals that the electronic charge deformation flexibility regarding e g to t 2g transition has a dominant effect on defect energetics for different elements in CSAs. Thus the electron deformation ability is suggested as a key factor in understanding the peculiar defect behavior in CSAs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/912714-band-offset-magnetic-property-engineering-epitaxial-interfaces-monolayer-m2o3-al-ga-sc-ti-ni-alpha-fe203-alpha-cr203-interface','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/912714-band-offset-magnetic-property-engineering-epitaxial-interfaces-monolayer-m2o3-al-ga-sc-ti-ni-alpha-fe203-alpha-cr203-interface"><span>BAnd offset and magnetic property engineering for epitaxial interfaces: a Monolayer of M2O3 (M=Al, Ga, Sc, Ti, Ni) at the alpha-<span class="hlt">Fe</span>203/alpha-<span class="hlt">Cr</span>203 (0001) Interface</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>Jaffe, John E; Bachorz, Rafal A; Gutowski, Maciej S</p> <p>2007-05-01</p> <p>We have used density functional theory with the gradient corrected exchange-correlation functional PW91 to study the effect of an interfactant <span class="hlt">layer</span>, where <span class="hlt">Fe</span> and <span class="hlt">Cr</span> are replaced by a different metal, on electronic and magnetic properties of an epitaxial interface between -<span class="hlt">Fe</span>2O3 and -<span class="hlt">Cr</span>2O3 in the hexagonal (0001) basal plane. We studied a monolayer of M2O3 (M=Al, Ga, Sc, Ti, Ni) sandwiched with 5 <span class="hlt">layers</span> of chromia and five <span class="hlt">layers</span> of hematite through epitaxial interfaces of two types, termed “oxygen divided” or “split metal.” We found that both the magnetic and electronic properties of the superlattice are modified by themore » interfactant monolayer. For the split metal interface, which is favored through the growth pattern of chromia and hematite, the band offset can be changed from 0.62 eV (no interfactant) up to 0.90 eV with the Sc2O3 interfactant, and down to –0.51 eV (i.e. the a-<span class="hlt">Fe</span>2O3/a-<span class="hlt">Cr</span>2O3 heterojunction changes from Type II to Type I) with the Ti2O3 interfactant, due to a massive interfacial charge transfer. The band gap of the system as a whole remains open for the interfactant monolayers based on Al, Ga, and Sc, but it closes for Ti. For Ni, the split-metal interface has a negative band offset and a small band gap. Thus, nanoscale engineering through <span class="hlt">layer-by-layer</span> growth will strongly affect the macroscopic properties of this system.« 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_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('https://www.osti.gov/biblio/22611720-effect-layer-thickness-device-response-silicon-heavily-supersaturated-sulfur','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22611720-effect-layer-thickness-device-response-silicon-heavily-supersaturated-sulfur"><span>Effect of <span class="hlt">layer</span> thickness on device response of <span class="hlt">silicon</span> heavily supersaturated with sulfur</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>Hutchinson, David; Department of Physics and Nuclear Engineering, United States Military Academy, West Point NY 10996; Mathews, Jay</p> <p>2016-05-15</p> <p>We report on a simple experiment in which the thickness of a hyperdoped <span class="hlt">silicon</span> <span class="hlt">layer</span>, supersaturated with sulfur by ion implantation followed by pulsed laser melting and rapid solidification, is systematically varied at constant average sulfur concentration, by varying the implantation energy, dose, and laser fluence. Contacts are deposited and the external quantum efficiency (EQE) is measured for visible wavelengths. We posit that the sulfur <span class="hlt">layer</span> primarily absorbs light but contributes negligible photocurrent, and we seek to support this by analyzing the EQE data for the different <span class="hlt">layer</span> thicknesses in two interlocking ways. In the first, we use the measuredmore » concentration depth profiles to obtain the approximate <span class="hlt">layer</span> thicknesses, and, for each wavelength, fit the EQE vs. <span class="hlt">layer</span> thickness curve to obtain the absorption coefficient of hyperdoped <span class="hlt">silicon</span> for that wavelength. Comparison to literature values for the hyperdoped <span class="hlt">silicon</span> absorption coefficients [S.H. Pan et al. Applied Physics Letters 98, 121913 (2011)] shows good agreement. Next, we essentially run this process in reverse; we fit with Beer’s law the curves of EQE vs. hyperdoped <span class="hlt">silicon</span> absorption coefficient for those wavelengths that are primarily absorbed in the hyperdoped <span class="hlt">silicon</span> <span class="hlt">layer</span>, and find that the <span class="hlt">layer</span> thicknesses obtained from the fit are in good agreement with the original values obtained from the depth profiles. We conclude that the data support our interpretation of the hyperdoped <span class="hlt">silicon</span> <span class="hlt">layer</span> as providing negligible photocurrent at high S concentrations. This work validates the absorption data of Pan et al. [Applied Physics Letters 98, 121913 (2011)], and is consistent with reports of short mobility-lifetime products in hyperdoped <span class="hlt">layers</span>. It suggests that for optoelectronic devices containing hyperdoped <span class="hlt">layers</span>, the most important contribution to the above band gap photoresponse may be due to photons absorbed below the hyperdoped <span class="hlt">layer</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JNuM..483...54F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JNuM..483...54F"><span>Heterogeneous dislocation loop formation near grain boundaries in a neutron-irradiated commercial <span class="hlt">FeCr</span>Al alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, Kevin G.; Briggs, Samuel A.; Hu, Xunxiang; Yamamoto, Yukinori; Howard, Richard H.; Sridharan, Kumar</p> <p>2017-01-01</p> <p><span class="hlt">FeCr</span>Al alloys are an attractive class of materials for nuclear power applications because of their increased environmental compatibility compared with more traditional nuclear materials. Preliminary studies into the radiation tolerance of <span class="hlt">FeCr</span>Al alloys under accelerated neutron testing between 300 and 400 °C have shown post-irradiation microstructures containing dislocation loops and a <span class="hlt">Cr</span>-rich α‧ phase. Although these initial studies established the post-irradiation microstructures, there was little to no focus on understanding the influence of pre-irradiation microstructures on this response. In this study, a well-annealed commercial <span class="hlt">FeCr</span>Al alloy, Alkrothal 720, was neutron irradiated to 1.8 displacements per atom (dpa) at 382 °C and then the effect of random high-angle grain boundaries on the spatial distribution and size of a〈100〉 dislocation loops, a/2〈111〉 dislocation loops, and black dot damage was analyzed using on-zone scanning transmission electron microscopy. Results showed a clear heterogeneous dislocation loop formation with a/2〈111〉 dislocation loops showing an increased number density and size, black dot damage showing a significant number density decrease, and a〈100〉 dislocation loops exhibiting an increased size in the vicinity of the grain boundary. These results suggest the importance of the pre-irradiation microstructure and, specifically, defect sink density spacing to the radiation tolerance of <span class="hlt">FeCr</span>Al alloys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e6328L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e6328L"><span>Doping effects on structural and magnetic properties of Heusler alloys <span class="hlt">Fe</span>2<span class="hlt">Cr</span>1-xCoxSi</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Yifan; Ren, Lizhu; Zheng, Yuhong; He, Shikun; Liu, Yang; Yang, Ping; Yang, Hyunsoo; Teo, Kie Leong</p> <p>2018-05-01</p> <p>In this work, 30nm <span class="hlt">Fe</span>2<span class="hlt">Cr</span>1-xCoxSi (FCCS) magnetic films were deposited on <span class="hlt">Cr</span> buffered MgO (100) substrates by sputtering. <span class="hlt">Fe</span>2<span class="hlt">Cr</span>0.5Co0.5Si exhibits the largest magnetization and optimal ordered L21 cubic structure at in-situ annealing temperature (Tia) of 450°C. The Co composition dependence of crystalline structures, surface morphology, defects, lattice distortions and their correlation with the magnetic properties are analyzed in detail. The Co-doped samples show in-plane M-H loops with magnetic squareness ratio of 1 and increasing anisotropy energy density with Co composition. Appropriate Co doping composition promotes L21 phase but higher Co composition converts L21 to B2 phase. Doping effect and lattice mismatch both are proved to increase the defect density. In addition, distortions of the FCCS lattice are found to be approximately linear with Co composition. The largest lattice distortion (c/a) is 0.969 for <span class="hlt">Fe</span>2<span class="hlt">Cr</span>0.25Co0.75Si and the smallest is 0.983 for <span class="hlt">Fe</span>2<span class="hlt">Cr</span>Si. Our analyses suggest that these tetragonal distortions mainly induced by an elastic stress from <span class="hlt">Cr</span> buffer account for the large in-plane anisotropy energy. This work paves the way for further tailoring the magnetic and structural properties of quaternary Heusler alloys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006JAP....99hM912K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006JAP....99hM912K"><span>Investigation of <span class="hlt">Cr</span> substitution in Co ferrite (CoCrx<span class="hlt">Fe</span>2-xO4) using Mossbauer spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krieble, K.; Lo, C. C. H.; Melikhov, Y.; Snyder, J. E.</p> <p>2006-04-01</p> <p>Substitution of other metals for <span class="hlt">Fe</span> in cobalt ferrite has been proposed as a method to tailor the magnetic and magnetoelastic properties for sensor and actuator applications [H. Zheng et al., Science 303, 661 (2004)]. However, to understand the effect of <span class="hlt">Cr</span> substitution, one needs atomic-level information on the local environments and interactions of the transition-metal ions. In this study, Mossbauer spectroscopy was used to investigate the local environments of the <span class="hlt">Fe</span> atoms in these materials. A series of five powder samples with compositions CoCrx<span class="hlt">Fe</span>2-xO4 (x=0.0 to 0.8) was investigated using transmission geometry. Results show two distinct six-line hyperfine patterns, indicating <span class="hlt">Fe</span> in A and B spinel sites. Increasing <span class="hlt">Cr</span> concentration is seen to decrease the hyperfine field strength for both A and B sites, as well as increasing the width of those distributions. Results for <span class="hlt">Cr</span> substitution show generally similar behavior to a prior study using Mn; however, <span class="hlt">Cr</span> substitution has more pronounced effects: the hyperfine fields decrease and distribution widths increase at greater rates for <span class="hlt">Cr</span> substitution, and the differences between A and B site behavior are more pronounced. Results are consistent with a model in which <span class="hlt">Cr</span> has an even stronger B-site preference than Mn, and displaces more of the Co from the B to the A sites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19970009935','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19970009935"><span>Oxidation Resistant Ti-Al-<span class="hlt">Fe</span> Diffusion Barrier for <span class="hlt">FeCr</span>AlY Coatings on Titanium Aluminides</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brady, Michael P. (Inventor); Smialke, James L. (Inventor); Brindley, William J. (Inventor)</p> <p>1996-01-01</p> <p>A diffusion barrier to help protect titanium aluminide alloys, including the coated alloys of the TiAl gamma + Ti3Al (alpha2) class, from oxidative attack and interstitial embrittlement at temperatures up to at least 1000 C is disclosed. The coating may comprise <span class="hlt">FeCr</span>AlX alloys. The diffusion barrier comprises titanium, aluminum, and iron in the following approximate atomic percent: Ti-(50-55)Al-(9-20)<span class="hlt">Fe</span>. This alloy is also suitable as an oxidative or structural coating for such substrates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MMI....24..371J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MMI....24..371J"><span>Microstructure and High Temperature Oxidation Property of <span class="hlt">Fe-Cr</span>-B Based Metal/Ceramic Composite Manufactured by Powder Injection Molding Process</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Joo, Yeun-Ah; Kim, Young-Kyun; Yoon, Tae-Sik; Lee, Kee-Ahn</p> <p>2018-03-01</p> <p>This study investigated the microstructure and high temperature oxidation property of <span class="hlt">Fe-Cr</span>-B metal/ceramic composite manufactured using powder injection molding process. Observations of initial microstructure showed a unique structure where α-<span class="hlt">Fe</span> and (<span class="hlt">Cr</span>, <span class="hlt">Fe</span>)2B form a continuous three-dimensional network. High temperature oxidation tests were performed at 900, 1000 and 1100 °C, for 24 h, and the oxidation weight gain according to each temperature condition was 0.13, 0.84 and 6.4 mg/cm2, respectively. The oxidation results according to time at 900 and 1000 °C conditions represented parabolic curves, and at 1100 °C condition formed a rectilinear curve. Observation and phase analysis results of the oxides identified <span class="hlt">Cr</span>2O3 and SiO2 at 900 and 1000 °C. In addition to <span class="hlt">Cr</span>2O3 and SiO2, <span class="hlt">Cr</span>BO3 and <span class="hlt">FeCr</span>2O4 formed due to phase decomposition of boride were identified at 1100 °C. Based on the findings above, this study suggested the high temperature oxidation mechanism of <span class="hlt">Fe-Cr</span>-B metal/ceramic composite manufactured using powder injection molding, and the possibility of its application as a high temperature component material was also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016HyInt.237...67F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016HyInt.237...67F"><span>Mössbauer study of oxide films of <span class="hlt">Fe</span>-, Sn-, <span class="hlt">Cr</span>- doped zirconium alloys during corrosion in autoclave</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Filippov, V. P.; Bateev, A. B.; Lauer, Yu. A.</p> <p>2016-12-01</p> <p>Mössbauer investigations were used to compare iron atom states in oxide films of binary Zr-<span class="hlt">Fe</span>, ternary Zr-<span class="hlt">Fe</span>-Cu and quaternary Zr-<span class="hlt">Fe-Cr</span>-Sn alloys. Oxide films are received in an autoclave at a temperature of 350-360 °C and at pressure of 16.8 MPa. The corrosion process decomposes the intermetallic precipitates in alloys and forms metallic iron with inclusions of chromium atoms α-<span class="hlt">Fe(Cr</span>), α-<span class="hlt">Fe</span>(Cu), α-<span class="hlt">Fe</span> 2O3 and <span class="hlt">Fe</span> 3O4 compounds. Some iron ions are formed in divalent and in trivalent paramagnetic states. The additional doping influences on corrosion kinetics and concentration of iron compounds and phases formed in oxide films. It was shown the correlation between concentration of iron in different chemical states and corrosion resistance of alloys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PMag...97..833D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PMag...97..833D"><span>Positron annihilation study of the vacancy clusters in ODS <span class="hlt">Fe</span>-14<span class="hlt">Cr</span> alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Domínguez-Reyes, R.; Auger, M. A.; Monge, M. A.; Pareja, R.</p> <p>2017-04-01</p> <p>Oxide dispersion strengthened <span class="hlt">Fe</span>14<span class="hlt">Cr</span> and <span class="hlt">Fe</span>14<span class="hlt">Cr</span>WTi alloys produced by mechanical alloying and hot isostatic pressing were subjected to isochronal annealing up to 1400 °C, and the evolution and thermal stability of the vacancy-type defects were investigated by positron annihilation spectroscopy (PAS). The results were compared to those from a non-oxide dispersion strengthened <span class="hlt">Fe</span>14<span class="hlt">Cr</span> alloy produced by following the same powder metallurgy route. The long lifetime component of the PAS revealed the existence of tridimensional vacancy clusters, or nanovoids, in all these alloys. Two recovery stages are found in the oxide dispersion strengthened alloys irrespective of the starting conditions of the samples. The first one starting at T > 750 °C is attributed to thermal shrinkage of large vacancy clusters, or voids. A strong increase in the intensity of the long lifetime after annealing at temperatures in the 800-1050 °C range indicates the development of new vacancy clusters. These defects appear to be unstable above 1050 °C, but some of them remain at temperatures as high as 1400 °C, at least for 90 min.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MARB43007D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MARB43007D"><span>Electronic, magnetic, and optical properties of Semiconducting Spinel <span class="hlt">Fe</span>2<span class="hlt">Cr</span>O4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Droubay, Tim; Kaspar, Tiffany; Nayyar, Iffat; Keavney, David; Sushko, Peter; Chambers, Scott</p> <p></p> <p>Transition metal oxides offer significant flexibility in tailoring functional properties by virtue of the high degree of solid solubility of different cations within the host lattice. For instance, the electronic properties of magnetite (<span class="hlt">Fe</span>3O4) , a ferrimagnetic half metal, can be substantially changed by substituting one third of the <span class="hlt">Fe</span> cations with Mn, Ni, Co, Zn or Mg. The actual magnetic properties of any given ferrite depend critically on whether the dopant occupies the tetrahedral (A) or octahedral (B) sites, or a mix of the two. Doping magnetite to produce a ferromagnetic semiconductor would be of considerable interest for spintronics and photocatalysis, particularly if the bandgap remains small. The detailed functional properties depend on the local structure, which is dictated in large measure by the cation sublattice(s) the dopants occupy, the valence(s) they exhibit, and the relative energy scales of competing effects, including short-range disorder, that determine the overall electronic structure. We have investigated <span class="hlt">Cr</span> as the dopant in <span class="hlt">Fe</span>3O4 by carrying out epitaxial film growth by molecular beam epitaxy and characterization, along with first principles modeling to explore new model materials. We find that replacing 1/3 of the <span class="hlt">Fe</span> atoms with <span class="hlt">Cr</span> atoms results in a low-gap, thermally robust ferrimagnetic semiconductor that is photoconductive in the visible, whereas replacing 2/3 of the <span class="hlt">Fe</span> with <span class="hlt">Cr</span> produces an insulator with no net magnetization. PNNL work supported by the U.S. Department of Energy, Office of Science, Division of Materials Sciences and Engineering.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NIMPB.393..118Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NIMPB.393..118Z"><span>The helium effect at grain boundaries in <span class="hlt">Fe-Cr</span> alloys: A first-principles study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zemła, M. R.; Wróbel, J. S.; Wejrzanowski, T.; Nguyen-Manh, D.; Kurzydłowski, K. J.</p> <p>2017-02-01</p> <p>Helium is produced in the structural materials in nuclear power plants by nuclear transmutation following neutron irradiation. Since the solubility of helium in all metals is extremely low, helium tends to be trapped at defects such as vacancies, dislocations and grain boundaries, which cause material embrittlement. Density functional theory (DFT) calculations were performed in order to investigate the helium effect at grain boundaries (GBs) in iron-chromium alloys. Both cohesive energy and magnetic properties at symmetric Σ3(1 1 1) and Σ5(2 1 0) tilt <span class="hlt">Fe</span> GBs are studied in the presence of <span class="hlt">Cr</span> and He atoms. It is found that the presence of <span class="hlt">Cr</span> atoms increases cohesive energy, at different He concentrations, and strongly influences magnetic properties at the GBs. The effect of the segregation energy of helium atom as a function of the different positions of <span class="hlt">Cr</span> atoms located inside/outside a GB has been considered. Results of the present first-principles study enable one to clarify the role of <span class="hlt">Cr</span> in understanding the helium effect in <span class="hlt">Fe-Cr</span>-based alloys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999JMMM..193...59S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999JMMM..193...59S"><span>Effects of <span class="hlt">Cr</span>-N-ZrO 2 seed <span class="hlt">layer</span> formed on glass substrates for longitudinal recording media</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suzuki, Hiroyuki; Djayaprawira, David D.; Takahashi, Yoshio; Ishikawa, Akira; Ono, Toshinori; Yahisa, Yotsuo</p> <p>1999-03-01</p> <p>Effects of <span class="hlt">Cr</span>-N-ZrO 2 seed <span class="hlt">layer</span> deposited on glass substrates before the deposition of C/Co-<span class="hlt">Cr-Pt/Cr</span>-Ti <span class="hlt">layers</span> for longitudinal recording media have been investigated. The product of v and Is, the activation volume and the saturation magnetization per unit volume, media noise Nd and S0/ Nd, which is the half value of peak-to-peak output voltage of an isolated pulse over Nd at 11.8 kFC/mm, are evaluated. We find that vIs is decreased by adding N and ZrO 2 to <span class="hlt">Cr</span> seed <span class="hlt">layer</span>. Nd is reduced as vIs decreases by adding nitrogen to the <span class="hlt">Cr</span> seed <span class="hlt">layer</span>. This is mainly due to the decreased grain sizes of both <span class="hlt">Cr</span>-Ti underlayer and Co-<span class="hlt">Cr</span>-Pt magnetic <span class="hlt">layer</span>. The Nd is further reduced by the addition of ZrO 2 to the <span class="hlt">Cr</span>-N seed <span class="hlt">layer</span>. Highest S0/ Nd is achieved for the media with <span class="hlt">Cr</span>-N-ZrO 2 seed <span class="hlt">layer</span>. On the other hand, the media with <span class="hlt">Cr</span>-ZrO 2 seed <span class="hlt">layer</span> deposited without nitrogen show the higher Nd. Therefore the decrease of the grain size by addition of nitrogen into Ar is essential to reduce Nd, and the ZrO 2 addition to the <span class="hlt">Cr</span>-N seed <span class="hlt">layer</span> seems to enhance the effect of grain size reduction by nitrogen addition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e6515H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e6515H"><span>Surface structure of MgO underlayer with Ti diffusion for (002) oriented L10 <span class="hlt">Fe</span>Pt-based heat assisted magnetic recording media</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hinata, Sintaro; Jo, Shin; Saito, Shin</p> <p>2018-05-01</p> <p>Surface morphology of the MgO <span class="hlt">layer</span> and magnetic properties of <span class="hlt">Fe</span>Pt-C <span class="hlt">layer</span> deposited on the MgO were investigated for the <span class="hlt">Fe</span>Pt-based heat assisted magnetic recording media. Stacking structure of the underlayer for the <span class="hlt">Fe</span>Pt-C <span class="hlt">layer</span> was MgO (0-5 nm)/<span class="hlt">Cr</span>80Mn20 (0-30 nm)/<span class="hlt">Cr</span>50Ti50 (0-50 nm)/glass sub.. Surface observation result for the MgO film by using an atomic force microscope revealed the existence of nodules with a height of about 2 nm and a network-like convex structure with a height difference of about sub nm (boundary wall, BW) on the MgO crystal grain boundary. Density of the nodules largely depends on the surface roughness of the <span class="hlt">Cr</span>Ti <span class="hlt">layer</span>, Ra<span class="hlt">Cr</span>Ti and it is suppressed from 10 to 2/0.5 μm2 by reducing Ra<span class="hlt">Cr</span>Ti from 420 to 260 pm. Height of the BW depends on thickness of the MgO <span class="hlt">layer</span>, tMgO and it can be suppressed by reducing tMgO to less than 4 nm. From the cross-sectional energy dispersive x-ray mapping, it is clarified that the BW is formed by atomic diffusion of Ti atoms from <span class="hlt">Cr</span>Ti <span class="hlt">layer</span> due to the substrate heating process, and a compound consists of Mg, Ti and O atoms. This BW can be used as a template to magnetically isolate the <span class="hlt">Fe</span>Pt column in the <span class="hlt">Fe</span>Pt-based granular film, such as <span class="hlt">Fe</span>Pt-SiO2, if the size of the BW is reduced to less than 10 nm. M-H loop of the <span class="hlt">Fe</span>Pt-C granular film deposited on the underlayer showed that the nodule and BW induce oxidation of the <span class="hlt">Fe</span>Pt grains, and reduction of intergranular exchange coupling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JMMM..394..212T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JMMM..394..212T"><span>Magnetic interactions in La0.7Sr0.3Mn1-xMexO3 (Me=Ga, <span class="hlt">Fe</span>, <span class="hlt">Cr</span>) manganites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Troyanchuk, I. O.; Bushinsky, M. V.; Karpinsky, D. V.; Tereshko, N. V.; Dobryansky, V. M.; Többens, D. M.; Sikolenko, V.; Efimov, V.</p> <p>2015-11-01</p> <p>Magnetic properties and crystal structure of La0.7Sr0.3Mn1-xMexO3 (Me=Ga, <span class="hlt">Fe</span>, <span class="hlt">Cr</span>; x≤0.3) have been studied by neutron powder diffraction and magnetization measurements. It is shown that substitution of manganese ions by chromium or gallium ions (x=0.3) leads to phase separation into antiferromagnetic and ferromagnetic phases whereas replacement by <span class="hlt">Fe</span> ions stabilizes spin glass state (x=0.3). Ferromagnetic interactions in <span class="hlt">Cr</span>-substituted compounds are much more pronounced than in <span class="hlt">Fe</span>- and Ga-doped ones. Magnetic properties are discussed in the model assuming a dominance of superexchange interactions. It is considered that ferromagnetism in the <span class="hlt">Cr</span>-substituted compositions is associated with nearly equal contributions from positive and negative components of the superexchange interaction between Mn3+ and <span class="hlt">Cr</span>3+ ions as well as to mixed valence of chromium ions. The spin glass state observed for the <span class="hlt">Fe</span>-doped sample (x=0.3) is associated with strong antiferromagnetic superexchange between <span class="hlt">Fe</span>3+-O-<span class="hlt">Fe</span>3+ and <span class="hlt">Fe</span>3+-O-(Mn3+, Mn4+).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JEMat..47.2042B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JEMat..47.2042B"><span>Effect of High Pressure and Temperature on Structural, Thermodynamic and Thermoelectric Properties of Quaternary Co<span class="hlt">FeCr</span>Al Alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bhat, Tahir Mohiuddin; Gupta, Dinesh C.</p> <p>2018-03-01</p> <p>Employing first-principles based on density functional theory we have investigated the structural, magneto-electronic, thermoelectric and thermodynamic properties of quaternary Heusler alloy Co<span class="hlt">FeCr</span>Al. Electronic band structure displays that Co<span class="hlt">FeCr</span>Al is an indirect band gap semiconductor in spin-down state with the band gap value of 0.65 eV. Elastic constants reveal Co<span class="hlt">FeCr</span>Al is a mechanically stable structure having a Debye temperature of 648 K along with a high melting temperature (2130 K). The thermoelectric properties in the temperature range 50-800 K have been calculated. Co<span class="hlt">FeCr</span>Al possesses a high Seebeck coefficient of - 46 μV/K at room temperature along with the huge power factor of ˜ 4.8 (1012 μW cm-1 K-2 s-1) which maximizes the figure-of-merit up to ˜ 0.75 at 800 K temperature and suggesting Co<span class="hlt">FeCr</span>Al as potential thermoelectric material. The effect of high pressure and high temperature on the thermal expansion, Grüneisen parameter and heat capacity were also studied by using the quasi-harmonic Debye model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1261062','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1261062"><span>NEAMS-ATF M3 Milestone Report: Literature Review of Modeling of Radiation-Induced Swelling in <span class="hlt">Fe-Cr</span>-Al Steels</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>Bai, Xianming; Biner, Suleyman Bulent; Jiang, Chao</p> <p>2015-12-01</p> <p><span class="hlt">Fe-Cr</span>-Al steels are proposed as accident-tolerant-fuel (ATF) cladding materials in light water reactors due to their excellent oxidation resistance at high temperatures. Currently, the understanding of their performance in reactor environment is still limited. In this review, firstly we reviewed the experimental studies of <span class="hlt">Fe-Cr</span>-Al based alloys with particular focus on the radiation effects in these alloys. Although limited data are available in literature, several previous and recent experimental studies have shown that <span class="hlt">Fe-Cr</span>-Al based alloys have very good void swelling resistance at low and moderate irradiation doses but the growth of dislocation loops is very active. Overall, the behaviormore » of radiation damage evolution is similar to that in <span class="hlt">Fe-Cr</span> ferritic/martensitic alloys. Secondly, we reviewed the rate theory-based modeling methods for modeling the coevolution of voids and dislocation loops in materials under irradiation such as Frenkel pair three-dimensional diffusion model (FP3DM) and cluster dynamics. Finally, we summarized and discussed our review and proposed our future plans for modeling radiation damage in <span class="hlt">Fe-Cr</span>-Al based alloys.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAP...122u4903L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAP...122u4903L"><span>In-depth porosity control of mesoporous <span class="hlt">silicon</span> <span class="hlt">layers</span> by an anodization current adjustment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lascaud, J.; Defforge, T.; Certon, D.; Valente, D.; Gautier, G.</p> <p>2017-12-01</p> <p>The formation of thick mesoporous <span class="hlt">silicon</span> <span class="hlt">layers</span> in P+-type substrates leads to an increase in the porosity from the surface to the interface with <span class="hlt">silicon</span>. The adjustment of the current density during the electrochemical etching of porous <span class="hlt">silicon</span> is an intuitive way to control the <span class="hlt">layer</span> in-depth porosity. The duration and the current density during the anodization were varied to empirically model porosity variations with <span class="hlt">layer</span> thickness and build a database. Current density profiles were extracted from the model in order to etch <span class="hlt">layer</span> with in-depth control porosity. As a proof of principle, an 80 μm-thick porous <span class="hlt">silicon</span> multilayer was synthetized with decreasing porosities from 55% to 35%. The results show that the assessment of the in-depth porosity could be significantly enhanced by taking into account the pure chemical etching of the <span class="hlt">layer</span> in the hydrofluoric acid-based electrolyte.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017HTMP...36..243F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017HTMP...36..243F"><span>Hot Corrosion Behavior of Stainless Steel with Al-Si/Al-Si-<span class="hlt">Cr</span> Coating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fu, Guangyan; Wu, Yongzhao; Liu, Qun; Li, Rongguang; Su, Yong</p> <p>2017-03-01</p> <p>The 1<span class="hlt">Cr</span>18Ni9Ti stainless steel with Al-Si/Al-Si-<span class="hlt">Cr</span> coatings is prepared by slurry process and vacuum diffusion, and the hot corrosion behavior of the stainless steel with/without the coatings is studied under the condition of Na2SO4 film at 950 °C in air. Results show that the corrosion kinetics of stainless steel, the stainless steel with Al-Si coating and the stainless steel with Al-Si-<span class="hlt">Cr</span> coating follow parabolic laws in several segments. After 24 h corrosion, the sequence of the mass gain for the three alloys is the stainless steel with Al-Si-<span class="hlt">Cr</span> coating < the stainless steel with Al-Si coating < the stainless steel without any coating. The corrosion products of the three alloys are <span class="hlt">layered</span>. Thereinto, the corrosion products of stainless steel without coating are divided into two <span class="hlt">layers</span>, where the outside <span class="hlt">layer</span> contains a composite of <span class="hlt">Fe</span>2O3 and <span class="hlt">Fe</span>O, and the inner <span class="hlt">layer</span> is <span class="hlt">Cr</span>2O3. The corrosion products of the stainless steel with Al-Si coating are also divided into two <span class="hlt">layers</span>, of which the outside <span class="hlt">layer</span> mainly consists of <span class="hlt">Cr</span>2O3, and the inner <span class="hlt">layer</span> is mainly SiO2. The corrosion film of the stainless steel with Al-Si-<span class="hlt">Cr</span> coating is thin and dense, which combines well with substrate. Thereinto, the outside <span class="hlt">layer</span> is mainly <span class="hlt">Cr</span>2O3, and the inside <span class="hlt">layer</span> is Al2O3. In the matrix of all of the three alloys, there exist small amount of sulfides. Continuous and protective films of <span class="hlt">Cr</span>2O3, SiO2 and Al2O3 form on the surface of the stainless steel with Al-Si and Al-Si-<span class="hlt">Cr</span> coatings, which prevent further oxidation or sulfide corrosion of matrix metals, and this is the main reason for the much smaller mass gain of the two alloys than that of the stainless steel without any coatings in the 24 h hot corrosion process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22409985-layered-structure-related-magnetic-properties-annealed-fe-ir-ultrathin-films','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22409985-layered-structure-related-magnetic-properties-annealed-fe-ir-ultrathin-films"><span><span class="hlt">Layered</span> structure and related magnetic properties for annealed <span class="hlt">Fe</span>/Ir(111) ultrathin films</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>Jiang, Pei-Cheng; Chen, Wei-Hsiang; Hsieh, Chen-Yuan</p> <p>2015-05-07</p> <p>After annealing treatments for fcc-<span class="hlt">Fe</span>/Ir(111) below 600 K, the surface <span class="hlt">layers</span> remain pseudomorphic. The Ir(111) substrate plays an important role on the expanded <span class="hlt">Fe</span> lattice. At temperatures between 750 and 800 K, the surface composition shows a stable state and a c(2 × 4) structure is observed. We discover a <span class="hlt">layered</span> structure composed of some <span class="hlt">Fe</span> atoms on the top of a <span class="hlt">Fe</span>{sub 0.5}Ir{sub 0.5} interfacial alloy supported on the Ir(111) substrate. The competition between the negative formation heat of <span class="hlt">Fe</span>{sub 0.5}Ir{sub 0.5} and surface free energy of <span class="hlt">Fe</span> causes the formation of <span class="hlt">layered</span> structure. The existence of ferromagnetic dead <span class="hlt">layer</span> coincides with themore » formation of fcc-<span class="hlt">Fe</span> for ultrathin <span class="hlt">Fe</span> on <span class="hlt">Fe</span>{sub 0.5}Ir{sub 0.5}/Ir(111). For <span class="hlt">Fe</span> films thicker than three monolayers, the linear increase of the Kerr intensity versus the <span class="hlt">Fe</span> coverage is related to the growing of bcc-<span class="hlt">Fe</span> on the surface where the <span class="hlt">Fe</span> <span class="hlt">layer</span> is incoherent to the underlying <span class="hlt">Fe</span>{sub 0.5}Ir{sub 0.5}/Ir(111). These results emphasize the importance of the substrate induced strain and <span class="hlt">layered</span> structure of <span class="hlt">Fe/Fe</span>{sub 0.5}Ir{sub 0.5}/Ir(111) on the magnetic properties and provide valuable information for future applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMMM..441..672S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMMM..441..672S"><span>Influence of fuel-nitrate ratio on the structural and magnetic properties of <span class="hlt">Fe</span> and <span class="hlt">Cr</span> based spinels prepared by solution self combustion method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sijo, A. K.</p> <p>2017-11-01</p> <p>In this study, we report the synthesis of nano-sized Co<span class="hlt">CrFe</span>O4 and Ni<span class="hlt">CrFe</span>O4 using the solution self combustion method and the variation in the magnetic and structural properties with different fuel to nitrate ratios-fuel lean, fuel rich and stoichiometric. Citric acid is used as the fuel. XRD analysis of the samples confirms the formation of pure spinel phased nanoparticles in fuel rich and stoichiometric cases. But Co<span class="hlt">CrFe</span>O4 and Ni<span class="hlt">CrFe</span>O4 samples prepared under the fuel lean condition show the presence of a small amount of impurity phases: α-Ni in fuel lean Ni<span class="hlt">CrFe</span>O4 and α-Co in fuel lean Co<span class="hlt">CrFe</span>O4. Fuel lean samples possess high magnetic saturation. The stoichiometric ratio results in finest nano-particles and structural and magnetic properties are very critically dependent on fuel to nitrate ratio.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26264738','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26264738"><span>Graphene Quantum Dot <span class="hlt">Layers</span> with Energy-Down-Shift Effect on Crystalline-<span class="hlt">Silicon</span> Solar Cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Kyung D; Park, Myung J; Kim, Do-Yeon; Kim, Soo M; Kang, Byungjun; Kim, Seongtak; Kim, Hyunho; Lee, Hae-Seok; Kang, Yoonmook; Yoon, Sam S; Hong, Byung H; Kim, Donghwan</p> <p>2015-09-02</p> <p>Graphene quantum dot (GQD) <span class="hlt">layers</span> were deposited as an energy-down-shift <span class="hlt">layer</span> on crystalline-<span class="hlt">silicon</span> solar cell surfaces by kinetic spraying of GQD suspensions. A supersonic air jet was used to accelerate the GQDs onto the surfaces. Here, we report the coating results on a <span class="hlt">silicon</span> substrate and the GQDs' application as an energy-down-shift <span class="hlt">layer</span> in crystalline-<span class="hlt">silicon</span> solar cells, which enhanced the power conversion efficiency (PCE). GQD <span class="hlt">layers</span> deposited at nozzle scan speeds of 40, 30, 20, and 10 mm/s were evaluated after they were used to fabricate crystalline-<span class="hlt">silicon</span> solar cells; the results indicate that GQDs play an important role in increasing the optical absorptivity of the cells. The short-circuit current density was enhanced by about 2.94% (0.9 mA/cm(2)) at 30 mm/s. Compared to a reference device without a GQD energy-down-shift <span class="hlt">layer</span>, the PCE of p-type <span class="hlt">silicon</span> solar cells was improved by 2.7% (0.4 percentage points).</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/2018MMTA..tmp.1547D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MMTA..tmp.1547D"><span>Effect of 0.25 and 2.0 MeV He-Ion Irradiation on Short-Range Ordering in Model (EFDA) <span class="hlt">Fe-Cr</span> Alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dubiel, Stanisław M.; Żukrowski, Jan; Serruys, Yves</p> <p>2018-05-01</p> <p>The effects of He+ irradiation on a distribution of <span class="hlt">Cr</span> atoms in <span class="hlt">Fe</span>100-x <span class="hlt">Cr</span> x (x = 5.8, 10.75, 15.15) alloys were studied by 57<span class="hlt">Fe</span> Conversion Electron Mössbauer Spectroscopy (CEMS). The alloys were irradiated with doses up to 12 × 1016 ions/cm2 with 0.25 and 2.0 MeV He+ ions. The distribution of <span class="hlt">Cr</span> atoms within the first two coordination shells around <span class="hlt">Fe</span> atoms was expressed with short-range order parameters α 1 (first-neighbor shell, 1NN), α 2 (second-neighbor shell, 2NN), and α 12 (1NN + 2NN). In non-irradiated alloys, α 1 >0 and α 2 <0 was revealed for all three samples. The value of α 12 ≈0, i.e., the distribution of <span class="hlt">Cr</span> atoms averaged over 1NN and 2NN, was random. The effect of the irradiation of the <span class="hlt">Fe</span>94.2<span class="hlt">Cr</span>5.8 alloy was similar for the two energies of He+, viz., increase of number of <span class="hlt">Cr</span> atoms in 1NN and decrease in 2NN. Consequently, the degree of ordering increased. For the other two samples, the effect of the irradiation depends on the composition, and is stronger for the less energetic ions where, for <span class="hlt">Fe</span>89.25<span class="hlt">Cr</span>10.75 alloy, the disordering disappeared and some traces of <span class="hlt">Cr</span> clustering appeared. In <span class="hlt">Fe</span>84.85<span class="hlt">Cr</span>15.15 alloy, the clustering was clear. In the samples irradiated with 2. 0 MeV He+ ions, the ordering also survived in the samples with x = 10.75 and 15.15, yet its degree became smaller than in the <span class="hlt">Fe</span>94.2<span class="hlt">Cr</span>5.8 alloy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22587063-synthesis-alfecucrmg-sub-alloy-powders-mechanical-alloying','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22587063-synthesis-alfecucrmg-sub-alloy-powders-mechanical-alloying"><span>Synthesis of Al<span class="hlt">FeCuCr</span>Mg{sub x} (x = 0, 0.5, 1, 1.7) alloy powders by mechanical alloying</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>Maulik, Ornov; Kumar, Vinod, E-mail: vkt.meta@mnit.ac.in; Adjunct Faculty, Materials Research Centre, Malaviya National Institute of Technology, Jaipur 302017</p> <p>2015-12-15</p> <p>Novel Al<span class="hlt">FeCuCr</span>Mg{sub x} (x = 0, 0.5, 1, 1.7 mol) high-entropy alloys (HEAs) were synthesized by mechanical alloying. The effect of Mg content on the phase evolution of HEAs was investigated using X-Ray diffractometry (XRD), transmission electron microscopy (TEM) and selected area electron diffraction (SAED) pattern analysis. The particle morphology and composition of HEAs were investigated by scanning electron microscopy (SEM). Thermodynamic parameters were calculated and analyzed to explain the formation of a solid solution. XRD analysis revealed BCC as major phase and FCC as a minor phase in as-milled Al<span class="hlt">FeCuCr</span> and Al<span class="hlt">FeCuCr</span>Mg{sub 0.5} HEAs. Also, XRD analysis of as-milledmore » Al<span class="hlt">FeCuCr</span>Mg, Al<span class="hlt">FeCuCr</span>Mg{sub 1.7} confirmed the formation of two BCC phases (BCC 1 and BCC 2). TEM–SAED analysis of Al<span class="hlt">FeCuCr</span>Mg{sub x} HEAs concurred with XRD results. Microstructural features and mechanism for solid solution formation have been conferred in detail. Phase formation of the present HEAs has been correlated with calculated thermodynamic parameters. Differential thermal analysis (TGA-DTA) of these alloys confirmed that there is no substantial phase change up to 500 °C. - Highlights: • Novel Al<span class="hlt">FeCuCr</span>Mg{sub x} (x = 0, 0.5, 1, 1.7) HEAs were prepared by mechanical alloying. • Phase evolution and lattice parameter were studied by X-Ray Diffraction. • Crystallite size and lattice microstrain calculated failed to obey the Williamson–Hall method. • Criterions for formation of simple solid solution were compared to the thermodynamic parameters of the present HEAs. • Increase in the Mg concentration in AlMg{sub x}<span class="hlt">FeCuCr</span> (x = 0, 0.5, 1, 1.7) HEAs supports the formation of BCC phase.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1286716-microstructural-kinetic-investigation-kcl-induced-corrosion-fecral-alloy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1286716-microstructural-kinetic-investigation-kcl-induced-corrosion-fecral-alloy"><span>A Microstructural and Kinetic Investigation of the KCl-Induced Corrosion of an <span class="hlt">FeCr</span>Al Alloy at 600 °C</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Israelsson, Niklas; Unocic, Kinga A.; Hellström, K.; ...</p> <p>2015-03-18</p> <p>In this paper, the corrosion behaviour of a <span class="hlt">FeCr</span>Al alloy was investigated at 600 °C in O 2 + H 2O with solid KCl applied. A kinetics and microstructural investigation showed that KCl accelerates corrosion and that potassium chromate formation depletes the protective scale in <span class="hlt">Cr</span>, thus triggering the formation of a fast-growing iron-rich scale. Iron oxide was found to grow both inward and outward, on either side of the initial oxide. A chromia <span class="hlt">layer</span> is formed with time underneath the iron oxide. Finally, it was found that although the alloy does not form a continuous pure alumina scale atmore » the investigated temperature, aluminium is, however, always enriched at the oxide/alloy interface.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19771373','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19771373"><span>Structural, thermal and photomagnetic properties of spin crossover [<span class="hlt">Fe</span>(bpp)2]2+ salts bearing [<span class="hlt">Cr</span>(L)(ox)2]- anions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Clemente-León, Miguel; Coronado, Eugenio; Giménez-López, M Carmen; Romero, Francisco M; Asthana, Saket; Desplanches, Cédric; Létard, Jean-François</p> <p>2009-10-14</p> <p>This paper is divided into two parts: in the first part, the influence of solvate molecules on the magnetic properties of spin crossover salts of [<span class="hlt">Fe</span>(bpp)(2)][<span class="hlt">Cr</span>(L)(ox)(2)]ClO(4) x nS (bpp = 2,6-bis(pyrazol-3yl)pyridine; L = 2,2'-bipyridine (bpy) or 1,10-phenanthroline (phen); ox = oxalate dianion; S = solvent) is analyzed. The second part is devoted to the photomagnetic properties of the previously reported [<span class="hlt">Fe</span>(bpp)(2)][<span class="hlt">Cr</span>(L)(ox)(2)](2) family of compounds. The study describes the crystal structure, differential scanning calorimetry (DSC) and magnetic properties of [<span class="hlt">Fe</span>(bpp)(2)][<span class="hlt">Cr</span>(bpy)(ox)(2)]ClO(4) x EtOH x 4 H(2)O (1) and [<span class="hlt">Fe</span>(bpp)(2)][<span class="hlt">Cr</span>(phen)(ox)(2)]ClO(4) x 1.5 EtOH x 4 H(2)O (2). Both salts are high-spin (HS) compounds. Desolvation of 1 yields a material exhibiting a gradual spin crossover that involves 50% of the <span class="hlt">Fe</span>(2+) cations. Rehydration of this desolvated salt induces a significant increase in the low-spin (LS) population. Desolvation of 2 affords a material showing a more abrupt spin crossover with thermal hysteresis (T(1/2)(increasing) = 286 K and T(1/2)(decreasing) = 273 K). This material is not very sensitive to rehydration. The anhydrous compounds [<span class="hlt">Fe</span>(bpp)(2)][<span class="hlt">Cr</span>(bpy)(ox)(2)](2) (3) and [<span class="hlt">Fe</span>(bpp)(2)][<span class="hlt">Cr</span>(phen)(ox)(2)](2) (4) display some quantitative photomagnetic conversion with T(LIESST) values of 41 and 51 K, respectively. Kinetic parameters governing the photo-induced HS-LS relaxation process have been determined and used to reproduce the T(LIESST) curves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26316044','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26316044"><span>Analysis of thin baked-on <span class="hlt">silicone</span> <span class="hlt">layers</span> by FTIR and 3D-Laser Scanning Microscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Funke, Stefanie; Matilainen, Julia; Nalenz, Heiko; Bechtold-Peters, Karoline; Mahler, Hanns-Christian; Friess, Wolfgang</p> <p>2015-10-01</p> <p>Pre-filled syringes (PFS) and auto-injection devices with cartridges are increasingly used for parenteral administration. To assure functionality, <span class="hlt">silicone</span> oil is applied to the inner surface of the glass barrel. <span class="hlt">Silicone</span> oil migration into the product can be minimized by applying a thin but sufficient <span class="hlt">layer</span> of <span class="hlt">silicone</span> oil emulsion followed by thermal bake-on versus spraying-on <span class="hlt">silicone</span> oil. <span class="hlt">Silicone</span> <span class="hlt">layers</span> thicker than 100nm resulting from regular spray-on <span class="hlt">siliconization</span> can be characterized using interferometric profilometers. However, the analysis of thin <span class="hlt">silicone</span> <span class="hlt">layers</span> generated by bake-on <span class="hlt">siliconization</span> is more challenging. In this paper, we have evaluated Fourier transform infrared (FTIR) spectroscopy after solvent extraction and a new 3D-Laser Scanning Microscopy (3D-LSM) to overcome this challenge. A multi-step solvent extraction and subsequent FTIR spectroscopy enabled to quantify baked-on <span class="hlt">silicone</span> levels as low as 21-325μg per 5mL cartridge. 3D-LSM was successfully established to visualize and measure baked-on <span class="hlt">silicone</span> <span class="hlt">layers</span> as thin as 10nm. 3D-LSM was additionally used to analyze the <span class="hlt">silicone</span> oil distribution within cartridges at such low levels. Both methods provided new, highly valuable insights to characterize the <span class="hlt">siliconization</span> after processing, in order to achieve functionality. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..290a2013B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..290a2013B"><span>Effect of dissolved hydrogen on Schottky barrier height of <span class="hlt">Fe-Cr</span> alloy heterojunction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berahim, A. N.; Zaharudin, M. Z.; Ani, M. H.; Arifin, S. K.</p> <p>2018-01-01</p> <p>The presence of water vapour at high temperature oxidation has certain effects on ferritic alloy in comparison to dry environment. It is hypothesized that at high temperature; water vapour provides hydrogen, which will dissolve into ferritic alloy substrate and altering their electronic state at the metal-oxide interface. This work aimed to clarify the change in electronic state of metal-oxide heterojunction with the presence of hydrogen/water vapour. In this study, the Schottky Barrier (SB) was created by sputtering <span class="hlt">Cr</span>2O3 onto prepared samples by using RF Magnetron sputtering machine. The existence of <span class="hlt">Fe/Cr</span>2O3 junction was characterized by using XRD. The surfaces were observed by using Optical Microscope (OM) and Scanning Electron Microscope (SEM). The samples were then exposed in dry and humid condition at temperature of 473 K and 1073 K. In dry condition, 100% Ar is flown inside the furnace, while in wet condition mixture of 95% Ar and 5% H was used. I-V measurement of the junction was done to determine the Schottky Barrier Height(SBH) of the samples in the corresponding ambient. The results show that in <span class="hlt">Fe/Cr</span>2O3 junction, with presence of hydrogen at temperature 473 K; the SBH was reduced by the scale factor of 1.054 and at 1073 K in wet ambient by factor of 1.068. Meanwhile, in <span class="hlt">Fe-Cr/Cr</span>2O3 junction with presence of hydrogen, the value of SBH was increased by scale factor of 1.068 at temperature 473 K while at 1073 K, the SBH also increased by factor of 1.009.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..428.1106R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..428.1106R"><span>In-situ Raman and X-ray photoelectron spectroscopic studies on the pitting corrosion of modified 9<span class="hlt">Cr</span>-1Mo steel in neutral chloride solution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ramya, S.; Nanda Gopala Krishna, D.; Mudali, U. Kamachi</p> <p>2018-01-01</p> <p>In-situ Raman and X-ray photoelectron spectroscopic studies were performed for the identification of native and corroded surface oxide <span class="hlt">layers</span> of modified 9<span class="hlt">Cr</span>-1Mo steel. The Raman data obtained for native oxide <span class="hlt">layer</span> of modified 9<span class="hlt">Cr</span>-1Mo steel revealed that it was mainly composed of oxides of <span class="hlt">Fe</span> and <span class="hlt">Cr</span>. The presence of alloying element Mo was found to be less significant in the native oxide film. The oxides of <span class="hlt">Cr</span> were dominant at the surface and were found to be decreasing closer to metal/oxide <span class="hlt">layer</span> interface. The changes in the chemical composition of the native films upon in-situ pitting during potentiostatic polarization experiment were characterized by in-situ Raman analysis. The corrosion products of potentiostatically polarized modified 9<span class="hlt">Cr</span>-1Mo steel was composed of dominant <span class="hlt">Fe</span> (III) phases viz., γ- <span class="hlt">Fe</span>2O3, α and γ - <span class="hlt">Fe</span>OOH along with the oxides of chromium. The results from Raman analysis were corroborated with the XPS experiments on as received and pitted samples of modified 9<span class="hlt">Cr</span>-1Mo steel specimens. It was observed that the oxides of <span class="hlt">Cr</span> and Mo contributed for the stability of the surface <span class="hlt">layer</span> by forming <span class="hlt">Cr</span>2O3 and MoO3. Also, the study attempted to find out the intermediate corrosion products inside the metastable pits to account for the pseudo passive behavior of modified 9<span class="hlt">Cr</span>-1Mo steel in 0.1 M NaCl solution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SSCom.272...48C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SSCom.272...48C"><span>Electronic structure of <span class="hlt">Cr</span> doped <span class="hlt">Fe</span>3O4 thin films by X-ray absorption near-edge structure spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Chi-Liang; Dong, Chung-Li; Asokan, Kandasami; Chern, G.; Chang, C. L.</p> <p>2018-04-01</p> <p>Present study reports the electronic structures of <span class="hlt">Cr</span> doped <span class="hlt">Fe</span>3O4 (<span class="hlt">Fe</span>3-xCrxO4 (0 ≤ x ≤ 3) grown on MgO (100) substrates in the form of thin films fabricated by a plasma-oxygen assisted Molecular Beam Epitaxy (MBE). X-ray absorption near-edge structure (XANES) spectra at <span class="hlt">Cr</span> & <span class="hlt">Fe</span> L-, and O K-edges were used to understand the electronic structure: changes in the bonding nature, valence states, and site occupancies. <span class="hlt">Cr</span> doping in <span class="hlt">Fe</span>3O4 results in the change of charge transfer, crystal structure, and selective occupation of ions in octahedral and tetrahedral sites. Such change modifies the electrical and magnetic properties due to the covalency of <span class="hlt">Cr</span> ions. The physical and chemical properties of ferrites are strongly dependent on the lattice site, ion size of dopant, and magnetic nature present at different structural symmetry of the spinel structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23862444','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23862444"><span>Electrodepositing behaviors and properties of nano <span class="hlt">Fe-Ni-Cr</span>/SiC composite coatings from trivalent chromium baths containing compound carboxylate-urea system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>He, Xinkuai; Hou, Bailong; Cai, Youxing; Li, Chen; Jiang, Yumei; Wu, Luye</p> <p>2013-06-01</p> <p>The nano <span class="hlt">Fe-Ni-Cr</span>/SiC composite coatings were prepared using pulse electrodeposition method from trivalent chromium baths containing compound carboxylate-urea system and nano SiC in ultrasonic field. The effects of the carboxylate-urea system on the nano <span class="hlt">Fe-Ni-Cr</span>/SiC composite coatings have been investigated. These results indicated that the SiC and <span class="hlt">Cr</span> contents and the thickness of the <span class="hlt">Fe-Ni-Cr</span>/SiC composite coatings could be obviously improved by the compound carboxylate-urea system. The steady-state polarization curves showed that the hydrogen evolution reaction (HER) could be significantly inhibited by the compound carboxylate-urea system, which was benefit to increase the SiC and <span class="hlt">Cr</span> contents and the thickness of the composite coatings. The cyclic voltammetry (CV) curves showed that the cathodic polarization of the matrix metal ions could be increased in the bath containing the compound carboxylate-urea system. Thus, a compact <span class="hlt">Fe-Ni-Cr</span>/SiC composite coating could be obtained using this technique. The surface morphology of the <span class="hlt">Fe-Ni-Cr</span>/SiC composite coatings checked with the scanning electron micrographs (SEM) showed that the surface smoothness could be also improved and the microcracks and pinholes could be decreased due to the presence of the compound carboxylate-urea system. The phase composition of the as-posited coating was measured by the X-ray diffraction (XRD). XRD data showed that the as-posited coating was <span class="hlt">Fe-Ni-Cr</span>/SiC composite coating. The chemical composition of the coating was investigated by energy dispersive spectrum (EDS) analysis. The result showed the functional <span class="hlt">Fe-Ni-Cr</span>/SiC composite coatings with 4.1 wt.% SiC and 25.1 wt.% <span class="hlt">Cr</span>, and 23.9 microm thickness were obtained in this study, which had best corrosion resistance according to the results of the typical potentiodynamic polarization curves of the <span class="hlt">Fe-Ni-Cr</span>/SiC composite coatings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57b1304O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57b1304O"><span>Effect of low-oxygen-concentration <span class="hlt">layer</span> on iron gettering capability of carbon-cluster ion-implanted Si wafer for CMOS image sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Onaka-Masada, Ayumi; Nakai, Toshiro; Okuyama, Ryosuke; Okuda, Hidehiko; Kadono, Takeshi; Hirose, Ryo; Koga, Yoshihiro; Kurita, Kazunari; Sueoka, Koji</p> <p>2018-02-01</p> <p>The effect of oxygen (O) concentration on the <span class="hlt">Fe</span> gettering capability in a carbon-cluster (C3H5) ion-implanted region was investigated by comparing a Czochralski (CZ)-grown <span class="hlt">silicon</span> substrate and an epitaxial growth <span class="hlt">layer</span>. A high <span class="hlt">Fe</span> gettering efficiency in a carbon-cluster ion-implanted epitaxial growth <span class="hlt">layer</span>, which has a low oxygen region, was observed by deep-level transient spectroscopy (DLTS) and secondary ion mass spectroscopy (SIMS). It was demonstrated that the amount of gettered <span class="hlt">Fe</span> in the epitaxial growth <span class="hlt">layer</span> is approximately two times higher than that in the CZ-grown <span class="hlt">silicon</span> substrate. Furthermore, by measuring the cathodeluminescence, the number of intrinsic point defects induced by carbon-cluster ion implantation was found to differ between the CZ-grown <span class="hlt">silicon</span> substrate and the epitaxial growth <span class="hlt">layer</span>. It is suggested that <span class="hlt">Fe</span> gettering by carbon-cluster ion implantation comes through point defect clusters, and that O in the carbon-cluster ion-implanted region affects the formation of gettering sinks for <span class="hlt">Fe</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhPro..12..338A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhPro..12..338A"><span>Crack Free Tungsten Carbide Reinforced Ni(<span class="hlt">Cr</span>) <span class="hlt">Layers</span> obtained by Laser Cladding</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Amado, J. M.; Tobar, M. J.; Yáñez, A.; Amigó, V.; Candel, J. J.</p> <p></p> <p>The development of hardfacing coatings has become technologically significant in many industries A common approach is the production of metal matrix composites (MMC) <span class="hlt">layers</span>. In this work Ni<span class="hlt">Cr</span>-WC MMC hardfacing <span class="hlt">layers</span> are deposited on C25 steel by means of laser cladding. Spheroidal fused tungsten carbides is used as reinforcement phase. Three different Ni<span class="hlt">Cr</span> alloys with different <span class="hlt">Cr</span> content were tested. Optimum conditions to obtain dense, uniform carbide distribution and hardness close to nominal values were defined. The effect of <span class="hlt">Cr</span> content respect to the microstructure, susceptibility for cracking and the wear rate of the resulting coating will also be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1214517','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1214517"><span>Development and quality assessments of commercial heat production of ATF <span class="hlt">FeCr</span>Al tubes</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>Yamamoto, Yukinori</p> <p>2015-09-01</p> <p>Development and quality assessment of the 2 nd generation ATF <span class="hlt">FeCr</span>Al tube production with commercial manufacturers were conducted. The manufacturing partners include Sophisticated Alloys, Inc. (SAI), Butler, PA for <span class="hlt">FeCr</span>Al alloy casting via vacuum induction melting, Oak Ridge National Laboratory (ORNL) for extrusion process to prepare the master bars/tubes to be tube-drawn, and Rhenium Alloys, Inc. (RAI), North Ridgeville, OH, for tube-drawing process. The masters bars have also been provided to Los Alamos National Laboratory (LANL) who works with Century Tubes, Inc., (CTI), San Diego, CA, as parallel tube production effort under the current program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NRL....12..248W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NRL....12..248W"><span>Enhanced Corrosion Resistance of PVD-<span class="hlt">Cr</span>N Coatings by ALD Sealing <span class="hlt">Layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wan; Zhang, Teng Fei; Ding, Ji Cheng; Kim, Chang-Min; Park, So-Won; Yang, Yang; Kim, Kwang-Ho; Kwon, Se-Hun</p> <p>2017-04-01</p> <p>Multilayered hard coatings with a <span class="hlt">Cr</span>N matrix and an Al2O3, TiO2, or nanolaminate-Al2O3/TiO2 sealing <span class="hlt">layer</span> were designed by a hybrid deposition process combined with physical vapor deposition (PVD) and atomic <span class="hlt">layer</span> deposition (ALD). The strategy was to utilize ALD thin films as pinhole-free barriers to seal the intrinsic defects to protect the <span class="hlt">Cr</span>N matrix. The influences of the different sealing <span class="hlt">layers</span> added in the coatings on the microstructure, surface roughness, and corrosion behaviors were investigated. The results indicated that the sealing <span class="hlt">layer</span> added by ALD significantly decreased the average grain size and improved the corrosion resistance of the <span class="hlt">Cr</span>N coatings. The insertion of the nanolaminate-Al2O3/TiO2 sealing <span class="hlt">layers</span> resulted in a further increase in corrosion resistance, which was attributed to the synergistic effect of Al2O3 and TiO2, both acting as excellent passivation barriers to the diffusion of corrosive substances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27739517','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27739517"><span>Interrogating the superconductor Ca10(Pt4As8)(<span class="hlt">Fe</span>2-xPtxAs2)5 <span class="hlt">Layer-by-layer</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Jisun; Nam, Hyoungdo; Li, Guorong; Karki, A B; Wang, Zhen; Zhu, Yimei; Shih, Chih-Kang; Zhang, Jiandi; Jin, Rongying; Plummer, E W</p> <p>2016-10-14</p> <p>Ever since the discovery of high-T c superconductivity in <span class="hlt">layered</span> cuprates, the roles that individual <span class="hlt">layers</span> play have been debated, due to difficulty in <span class="hlt">layer-by-layer</span> characterization. While there is similar challenge in many <span class="hlt">Fe</span>-based <span class="hlt">layered</span> superconductors, the newly-discovered Ca 10 (Pt 4 As 8 )(<span class="hlt">Fe</span> 2 As 2 ) 5 provides opportunities to explore superconductivity <span class="hlt">layer</span> by <span class="hlt">layer</span>, because it contains both superconducting building blocks (<span class="hlt">Fe</span> 2 As 2 <span class="hlt">layers</span>) and intermediate Pt 4 As 8 <span class="hlt">layers</span>. Cleaving a single crystal under ultra-high vacuum results in multiple terminations: an ordered Pt 4 As 8 <span class="hlt">layer</span>, two reconstructed Ca <span class="hlt">layers</span> on the top of a Pt 4 As 8 <span class="hlt">layer</span>, and disordered Ca <span class="hlt">layer</span> on the top of <span class="hlt">Fe</span> 2 As 2 <span class="hlt">layer</span>. The electronic properties of individual <span class="hlt">layers</span> are studied using scanning tunneling microscopy/spectroscopy (STM/S), which reveals different spectra for each surface. Remarkably superconducting coherence peaks are seen only on the ordered Ca/Pt 4 As 8 <span class="hlt">layer</span>. Our results indicate that an ordered structure with proper charge balance is required in order to preserve superconductivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4194057','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4194057"><span>Photocatalytic activity of <span class="hlt">Cr</span>-doped TiO2 nanoparticles deposited on porous multicrystalline <span class="hlt">silicon</span> films</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>2014-01-01</p> <p>This work deals with the deposition of <span class="hlt">Cr</span>-doped TiO2 thin films on porous <span class="hlt">silicon</span> (PS) prepared from electrochemical anodization of multicrystalline (mc-Si) Si wafers. The effect of <span class="hlt">Cr</span> doping on the properties of the TiO2-<span class="hlt">Cr</span>/PS/Si samples has been investigated by means of X-ray diffraction (XRD), atomic force microcopy (AFM), photoluminescence, lifetime, and laser beam-induced current (LBIC) measurements. The photocatalytic activity is carried out on TiO2-<span class="hlt">Cr</span>/PS/Si samples. It was found that the TiO2-<span class="hlt">Cr</span>/PS/mc-Si type structure degrades an organic pollutant (amido black) under ultraviolet (UV) light. A noticeable degradation of the pollutant is obtained for a <span class="hlt">Cr</span> doping of 2 at. %. This result is discussed in light of LBIC and photoluminescence measurements. PMID:25313302</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25313302','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25313302"><span>Photocatalytic activity of <span class="hlt">Cr</span>-doped TiO2 nanoparticles deposited on porous multicrystalline <span class="hlt">silicon</span> films.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hajjaji, Anouar; Trabelsi, Khaled; Atyaoui, Atef; Gaidi, Mounir; Bousselmi, Latifa; Bessais, Brahim; El Khakani, My Ali</p> <p>2014-01-01</p> <p>This work deals with the deposition of <span class="hlt">Cr</span>-doped TiO2 thin films on porous <span class="hlt">silicon</span> (PS) prepared from electrochemical anodization of multicrystalline (mc-Si) Si wafers. The effect of <span class="hlt">Cr</span> doping on the properties of the TiO2-<span class="hlt">Cr</span>/PS/Si samples has been investigated by means of X-ray diffraction (XRD), atomic force microcopy (AFM), photoluminescence, lifetime, and laser beam-induced current (LBIC) measurements. The photocatalytic activity is carried out on TiO2-<span class="hlt">Cr</span>/PS/Si samples. It was found that the TiO2-<span class="hlt">Cr</span>/PS/mc-Si type structure degrades an organic pollutant (amido black) under ultraviolet (UV) light. A noticeable degradation of the pollutant is obtained for a <span class="hlt">Cr</span> doping of 2 at. %. This result is discussed in light of LBIC and photoluminescence measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1252837-built-potential-fe-cr-superlattices-improved-photoexcited-carrier-separation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1252837-built-potential-fe-cr-superlattices-improved-photoexcited-carrier-separation"><span>Built-In Potential in <span class="hlt">Fe</span> 2 O 3 -<span class="hlt">Cr</span> 2 O 3 Superlattices for Improved Photoexcited Carrier Separation</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>Kaspar, Tiffany C.; Schreiber, Daniel K.; Spurgeon, Steven R.</p> <p>2015-12-17</p> <p>We demonstrate that the different surface terminations exhibited by α-<span class="hlt">Fe</span>2O3 (hematite) and α-<span class="hlt">Cr</span>2O3 (eskolaite) in superlattices (SL) of these materials, synthesized with exquisite control by molecular beam epitaxy, determine the heterojunction interface structure and result in controllable, non-commutative band offset values. Precise atomic control of the interface structure allowed us to vary the valence band offset from 0.35 eV to 0.79 eV. This controllable band alignment can be harnessed to generate a built-in potential in <span class="hlt">Fe</span>2O3-<span class="hlt">Cr</span>2O3 SLs. For instance, in a 2.5-period SL, a built-in potential of 0.8 eV was realized as measured by x-ray photoelectron spectroscopy of Ti dopantsmore » as probe species. The high quality of the SL structure was confirmed by atom probe tomography and scanning transmission electron microscopy. Enhanced photocurrents were measured for a thick <span class="hlt">Fe</span>2O3 epitaxial film capped with an (<span class="hlt">Fe</span>2O3)3-(<span class="hlt">Cr</span>2O3)3 SL; this enhancement was attributed to efficient electron-hole separation in the SL as a result of the band alignment. The <span class="hlt">Fe-O-Cr</span> bonds at the SL interfaces also red-shifted the onset of photoconductivity to ~1.6 eV. Exploiting the band alignment and photoabsorption properties of <span class="hlt">Fe</span>2O3-<span class="hlt">Cr</span>2O3 SLs has the potential to increase the efficiency of hematite-based photoelectrochemical water splitting.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850015688','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850015688"><span>Sintered <span class="hlt">silicon</span> carbide molded body and method for its production</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Omori, M.; Sendai, M.; Ohira, K.</p> <p>1984-01-01</p> <p>Sintered <span class="hlt">silicon</span> carbide shapes are described. They are produced by using a composition containing an oxide of at least one element chosen from the group: Li, Be, Mg, Si, Ca, Ti, V, <span class="hlt">Cr</span>, Mn, <span class="hlt">Fe</span>, Co, Ni, Zn, Nb, Mo, Ba, Tc, Ta, W and Th as a supplement to known sintering aids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1800c0002P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1800c0002P"><span>Phase composition and fine structure of 0.18C-1<span class="hlt">Cr</span>-3Ni-1Mo-<span class="hlt">Fe</span> steel after plasma-electrolytic treatment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Popova, Natalya; Bayatanova, Lyayla; Nikonenko, Elena; Skakov, Mazhyn; Kozlov, Eduard</p> <p>2017-01-01</p> <p>The paper presents the transmission electron microscopy (TEM) investigation of 0.18C-1<span class="hlt">Cr</span>-3Mn-1Mo- <span class="hlt">Fe</span> steel specimens to study phase transitions and modification of fine structure after plasma-electrolytic treatment (carbonitriding at 850°C during 5 min). TEM investigations involve two points: on the specimen surface and at ˜40 µm distance from it. The experiments show that the structure in the original state is a mixture consisting of ferrite and perlite grains. Carbonitriding results in a considerable modification of the quality and quantity of steel structure. Thus, on the surface, α-phase is represented by lamellar martensite, while at ˜40 µm depth - by massive and lamellar martensite tempered at low and high temperatures. Moreover, on the subsurface of the martensite plates' boundaries retained austenite <span class="hlt">layers</span> are observed, while inside plates the particles of alloyed cementite, carbonitrides of M23(C,N)6, M2C0.61N0.39, M6,2C3,5N0,3, M(C,N)2, <span class="hlt">Cr</span>12<span class="hlt">Fe</span>32Mo7Ni7 types, and β-graphite are present. In the specimen at the depth of ˜40 µm, retained austenite <span class="hlt">layers</span> are observed on the boundaries of martensite laths and plates, while inside plates only the particles of alloyed cementite and M23(C,N)6 carbonitride are formed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..327c2062Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..327c2062Z"><span>Phase transformation in rapidly quenched <span class="hlt">Fe-Cr</span>-Co-Mo-Ti-Si-B alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhukov, D. G.; Shubakov, V. S.; Zhukova, E. Kh; Gorshenkov, M. V.</p> <p>2018-03-01</p> <p>The research results of phase transformations in <span class="hlt">Fe</span>-24<span class="hlt">Cr</span>-16Co-3Mo-0.2Ti-1Si-B alloys (with a boron content of 1 to 3% by mass) obtained by rapid quenching are presented. The structure formation regularities during the melt spinning and during the subsequent crystallization annealing in rapidly quenched bands of the <span class="hlt">Fe-Cr</span>-Co-Mo-Ti-Si-B system alloys were studied. The changes in the phase composition of the rapidly quenched <span class="hlt">Fe-Cr</span>-Co-Mo-Ti- Si-B system alloys after quenching at various quench rates and at different boron concentrations in the alloys are studied. It is shown that during crystallization from an amorphous state, at temperatures above 570 °C, in addition to the α-phase, the σ-phase appears first, followed by the γ-phase. Heat treatment of rapidly quenched bands to high-coercive state was carried out. A qualitative assessment of magnetic properties in a high-coercivity state was carried out. An evaluation of the level of magnetic properties in a high-coercivity state allows us to conclude that the application of a magnetic field during crystallization from an amorphous state leads to anisotropy of the magnetic properties, that is, an anisotropic effect of thermo-magnetic treatment is detected.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5325582-diffusion-cations-chromia-layers-grown-iron-base-alloys','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5325582-diffusion-cations-chromia-layers-grown-iron-base-alloys"><span>Diffusion of cations in chromia <span class="hlt">layers</span> grown on iron-base alloys</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>Lobnig, R.E.; Hennesen, K.; Grabke, H.J.</p> <p></p> <p>Diffusion of the cations <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Mn, and Ni in <span class="hlt">Cr</span>{sub 2}O{sub 3} has been investigated at 1,173 K. The diffusion measurements were performed on chromia <span class="hlt">layers</span> grown on the model alloys <span class="hlt">Fe</span>-20<span class="hlt">Cr</span> and <span class="hlt">Fe</span>-20<span class="hlt">Cr</span>-12Ni in order to consider effects of small amounts of dissolved alien cations in <span class="hlt">Cr</span>{sub 2}O{sub 3}. The samples were diffusion annealed in H{sub 2}-H{sub 2}O at an oxygen partial pressure close to the <span class="hlt">Cr</span>{sub 2}O{sub 3}/<span class="hlt">Cr</span> equilibrium. For all tracers the lattice-diffusion coefficients are 3-5 orders of magnitude smaller than the grain-boundary diffusion coefficients. The lattice diffusivity of Mn is about two orders of magnitudemore » greater than the other lattice-diffusion coefficients, especially in <span class="hlt">Cr</span>{sub 2}O{sub 3} grown on <span class="hlt">Fe</span>-20<span class="hlt">Cr</span>-12Ni. The values of the diffusion coefficients for <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, and Ni are in the same range. Diffusion of the tracers in <span class="hlt">Cr</span>{sub 2}O{sub 3} grown on different alloys did not show significant differences with the exception of Mn.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..432..127Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..432..127Y"><span>Surface reaction of <span class="hlt">silicon</span> chlorides during atomic <span class="hlt">layer</span> deposition of <span class="hlt">silicon</span> nitride</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yusup, Luchana L.; Park, Jae-Min; Mayangsari, Tirta R.; Kwon, Young-Kyun; Lee, Won-Jun</p> <p>2018-02-01</p> <p>The reaction of precursor with surface active site is the critical step in atomic <span class="hlt">layer</span> deposition (ALD) process. We performed the density functional theory calculation with DFT-D correction to study the surface reaction of different <span class="hlt">silicon</span> chloride precursors during the first half cycle of ALD process. SiCl4, SiH2Cl2, Si2Cl6 and Si3Cl8 were considered as the <span class="hlt">silicon</span> precursors, and an NH/SiNH2*-terminated <span class="hlt">silicon</span> nitride surface was constructed to model the thermal ALD processes using NH3 as well as the PEALD processes using NH3 plasma. The total energies of the system were calculated for the geometry-optimized structures of physisorption, chemisorption, and transition state. The order of <span class="hlt">silicon</span> precursors in energy barrier, from lowest to highest, is Si3Cl8 (0.92 eV), Si2Cl6 (3.22 eV), SiH2Cl2 (3.93 eV) and SiCl4 (4.49 eV). <span class="hlt">Silicon</span> precursor with lower energy barrier in DFT calculation showed lower saturation dose in literature for both thermal and plasma-enhanced ALD of <span class="hlt">silicon</span> nitride. Therefore, DFT calculation is a promising tool in predicting the reactivity of precursor during ALD process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22488685-application-ray-absorption-fine-structure-xafs-local-order-analysis-fe-cr-maghemite-like-materials','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22488685-application-ray-absorption-fine-structure-xafs-local-order-analysis-fe-cr-maghemite-like-materials"><span>Application of x-ray absorption fine structure (XAFS) to local-order analysis in <span class="hlt">Fe-Cr</span> maghemite-like materials</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>Montero-Cabrera, M. E., E-mail: elena.montero@cimav.edu.mx; Fuentes-Cobas, L. E.; Macías-Ríos, E.</p> <p>2015-07-23</p> <p>The maghemite-like oxide system γ-<span class="hlt">Fe</span>{sub 2-x}<span class="hlt">Cr</span>{sub x}O{sub 3} (x=0.75, 1 and 1.25) was studied by X-ray absorption fine structure (XAFS) and by synchrotron radiation X-ray diffraction (XRD). Measurements were performed at the Stanford Synchrotron Radiation Lightsource at room temperature, at beamlines 2-1, 2-3 and 4-3. High-resolution XRD patterns were processed by means of the Rietveld method. In cases of atoms being neighbors in the Periodic Table, the order/disorder degree of the considered solutions is indiscernible by “normal” (absence of “anomalous scattering”) diffraction experiments. Thus, maghemite-like materials were investigated by XAFS in both <span class="hlt">Fe</span> and <span class="hlt">Cr</span> K-edges to clarify, via short-rangemore » structure characterization, the local ordering of the investigated system. Athena and Artemis graphic user interfaces for IFEFFIT and FEFF8.4 codes were employed for XAFS spectra interpretation. Pre-edge decomposition and theoretical modeling of X-ray absorption near edge structure (XANES) transitions were performed. By analysis of the <span class="hlt">Cr</span> K-edge XANES, it has been confirmed that <span class="hlt">Cr</span> is located in an octahedral environment. Fitting of the extended X-ray absorption fine structure (EXAFS) spectra was performed under the consideration that the central atom of <span class="hlt">Fe</span> is allowed to occupy octa- and tetrahedral positions, while <span class="hlt">Cr</span> occupies only octahedral ones. Coordination number of neighboring atoms, interatomic distances and their quadratic deviation average were determined for x=1, by fitting simultaneously the EXAFS spectra of both <span class="hlt">Fe</span> and <span class="hlt">Cr</span> K-edges. The results of fitting the experimental spectra with theoretical standards showed that the cation vacancies tend to follow a regular pattern within the structure of the iron-chromium maghemite (<span class="hlt">FeCr</span>O{sub 3})« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhyB..446...92Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhyB..446...92Z"><span>Experimental evidence for the magnetic moment directions of <span class="hlt">Cr</span>2+ and <span class="hlt">Cr</span>3+ cations in the spinel ferrites Cux1Crx2<span class="hlt">Fe</span>3-x1-x2O4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, X. Y.; Xu, J.; Li, Z. Z.; Qi, W. H.; Tang, G. D.; Shang, Z. F.; Ji, D. H.; Lang, L. L.</p> <p>2014-08-01</p> <p>(A)[B]2O4 spinel ferrite samples with the composition Cux1Crx2<span class="hlt">Fe</span>3-x1-x2O4 (0.0≤x1≤0.284 and 1.04≥x2≥0.656) were prepared by a chemical co-precipitation method. X-ray diffraction patterns indicated that the samples had a single-phase cubic spinel structure. It is interesting that the saturation magnetization of the samples increased when Cu2+ or Cu3+ (with 1 or 2μB of magnetic moment) substituted for <span class="hlt">Cr</span>2+ or <span class="hlt">Cr</span>3+ (with 4 or 3μB), which cannot be obviously explained if the magnetic moments of <span class="hlt">Cr</span>2+ and <span class="hlt">Cr</span>3+ cations are assumed to be parallel to those of the <span class="hlt">Fe</span> and Cu cations. However, with the assumption that the magnetic moments of <span class="hlt">Cr</span>2+ and <span class="hlt">Cr</span>3+ cations are antiparallel to the <span class="hlt">Fe</span> and Cu cation moments in spinel ferrites, the dependence on the Cu doping level of the sample magnetic moments at 10 K was fitted successfully, using the quantum-mechanical potential barrier model earlier proposed by our group. Using the cation distributions obtained in the fitting process, the experimental observation that the magnetic moment of the samples increased with increasing Cu doping level was explained. This work therefore provides experimental evidence that the magnetic moments of the <span class="hlt">Cr</span>2+ and <span class="hlt">Cr</span>3+ cations are antiparallel to those of the <span class="hlt">Fe</span> and Cu cations in spinel ferrites.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1953l0078S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1953l0078S"><span>Structural and magnetic characterization of <span class="hlt">Fe</span>2<span class="hlt">Cr</span>Si Heusler alloy nanoparticles as spin injectors and spin based sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saravanan, G.; Asvini, V.; Kalaiezhily, R. K.; Parveen, I. Mubeena; Ravichandran, K.</p> <p>2018-05-01</p> <p>Half-metallic ferromagnetic [HMF] nanoparticles are of considerable interest in spintronics applications due to their potential use as a highly spin polarized current source. HMF exhibits a semiconductor in one spin band at the Fermi level Ef and at the other spin band they poses strong metallic nature which shows 100 % spin polarization at Ef. <span class="hlt">Fe</span> based full Heusler alloys are primary interest due to high Curie temperature. <span class="hlt">Fe</span>2<span class="hlt">Cr</span>Si Heusler alloys are synthesized using metallic powders of <span class="hlt">Fe</span>, <span class="hlt">Cr</span> and Si by mechanical alloying method. X-Ray diffractions studies were performed to analyze the structural details of <span class="hlt">Fe</span>2<span class="hlt">Cr</span>Si nanoparticles with High resolution scanning electron microscope (HRSEM) studies for the morphological details of nanoparticles and magnetic properties were studied using Vibrating sample magnetometer (VSM). XRD Data analysis conforms the Heusler alloy phase showing the existence of L21 structure. Magnetic properties are measured for synthesized samples exhibiting a soft magnetic property possessing low coercivity (HC = 60.5 Oe) and saturation magnetic moment of <span class="hlt">Fe</span>2<span class="hlt">Cr</span>Si is 3.16 µB, which is significantly higher than the ideal value of 2 µB from the Slater-Pauling rule due to room temperature measurement. The change in magnetic properties are half-metallic nature of <span class="hlt">Fe</span>2<span class="hlt">Cr</span>Si is due to the shift of the Fermi level with respect to the gap were can be used as spin sensors and spin injectors in magnetic random access memories and other spin dependent devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JMMM..322.2505G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JMMM..322.2505G"><span>Vacancy-induced spin-glass behavior of Prussian blue analogue <span class="hlt">Fe</span> II1.1<span class="hlt">Cr</span> IIx[<span class="hlt">Cr</span> III (CN) 6] 0.6- x· nH 2O nanowires</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, Bo; Yao, Jinli; Xue, Desheng</p> <p>2010-09-01</p> <p>Prussian blue analogue <span class="hlt">Fe</span> II1.1<span class="hlt">Cr</span> IIx[<span class="hlt">Cr</span> III(CN) 6] 0.6- x· nH 2O nanowires were synthesized by electrodeposition. The magnetic properties investigation indicates that the nanowires exhibit cluster spin-glass behavior, which undergoes a magnetic transition to a frozen state below about 62 K. Spin disorder arising from reduced coordination and broken exchange bonds between spin centers due to the structural defects may be the reason that causes the spin-glass freezing behavior. The negative magnetization observed at temperature lower than the compensation temperature ( Tcomp˜43 K) at a field of 10 Oe may be due to the different temperature dependences of the ferromagnetic site <span class="hlt">Fe-Cr</span> and antiferromagnetic site <span class="hlt">Cr-Cr</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57a3001H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57a3001H"><span>Interface perpendicular magnetic anisotropy in ultrathin Ta/Ni<span class="hlt">Fe</span>/Pt <span class="hlt">layered</span> structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hirayama, Shigeyuki; Kasai, Shinya; Mitani, Seiji</p> <p>2018-01-01</p> <p>Interface perpendicular magnetic anisotropy (PMA) in ultrathin Ta/Ni<span class="hlt">Fe</span>/Pt <span class="hlt">layered</span> structures was investigated through magnetization measurements. Ta/Ni<span class="hlt">Fe</span>/Pt films with Ni<span class="hlt">Fe</span> <span class="hlt">layer</span> thickness (t) values of 2 nm or more showed typical in-plane magnetization curves, which was presumably due to the dominant contribution of the shape magnetic anisotropy. The thickness dependence of the saturation magnetization of the entire Ni<span class="hlt">Fe</span> <span class="hlt">layer</span> (M s) was well analyzed using the so-called dead-<span class="hlt">layer</span> model, showing that the magnetically active part of the Ni<span class="hlt">Fe</span> <span class="hlt">layer</span> has saturation magnetization (M\\text{s}\\text{act}) independent of t and comparable to the bulk value. In the perpendicular direction, the saturation field H k was found to clearly decrease with decreasing t, while the effective field of shape magnetic anisotropy due to the active Ni<span class="hlt">Fe</span> saturation magnetization M\\text{s}\\text{act} should be independent of t. These observations show that there exists interface PMA in the <span class="hlt">layered</span> structures. The interface PMA energy density was determined to be ∼0.17 erg/cm2 using the dead-<span class="hlt">layer</span> model. Motivated by the correlation observed between M s and H k, we also attempted to interpret the experimental results using an alternative approach beyond the dead-<span class="hlt">layer</span> model; however, it gives only implications on the incomplete validity of the dead-<span class="hlt">layer</span> model and no better understanding.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1011065','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1011065"><span>Structural Disorder and Magnetism in the Spin-Gapless Semiconductor Co<span class="hlt">FeCr</span>Al</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-08-24</p> <p>of the <span class="hlt">Fe</span> doped half-Heusler and Heusler compounds CoFex<span class="hlt">Cr</span>Al and Co2-xFex<span class="hlt">Cr</span>Al (x = 0, 0.25, 0.5, 0.75, 1.0), respectively, have been studied both...Oogane, A. Hirohata, and V. K. Lazarov, “The Effect of Cobalt -Sublattice Disorder on Spin Polarisation in Co2FexMn1−xSi Heusler Alloys,” Materials 7</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22420251-liquid-phase-deposited-siloxane-based-capping-layers-silicon-solar-cells','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22420251-liquid-phase-deposited-siloxane-based-capping-layers-silicon-solar-cells"><span>Liquid-phase-deposited siloxane-based capping <span class="hlt">layers</span> for <span class="hlt">silicon</span> solar cells</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>Veith-Wolf, Boris; Wang, Jianhui; Hannu-Kuure, Milja</p> <p>2015-02-02</p> <p>We apply non-vacuum processing to deposit dielectric capping <span class="hlt">layers</span> on top of ultrathin atomic-<span class="hlt">layer</span>-deposited aluminum oxide (AlO{sub x}) films, used for the rear surface passivation of high-efficiency crystalline <span class="hlt">silicon</span> solar cells. We examine various siloxane-based liquid-phase-deposited (LPD) materials. Our optimized AlO{sub x}/LPD stacks show an excellent thermal and chemical stability against aluminum metal paste, as demonstrated by measured surface recombination velocities below 10 cm/s on 1.3 Ωcm p-type <span class="hlt">silicon</span> wafers after firing in a belt-line furnace with screen-printed aluminum paste on top. Implementation of the optimized LPD <span class="hlt">layers</span> into an industrial-type screen-printing solar cell process results in energy conversion efficiencies ofmore » up to 19.8% on p-type Czochralski <span class="hlt">silicon</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15917590','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15917590"><span>Activity and lifetime of urease immobilized using <span class="hlt">layer-by-layer</span> nano self-assembly on <span class="hlt">silicon</span> microchannels.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Forrest, Scott R; Elmore, Bill B; Palmer, James D</p> <p>2005-01-01</p> <p>Urease has been immobilized and <span class="hlt">layered</span> onto the walls of manufactured <span class="hlt">silicon</span> microchannels. Enzyme immobilization was performed using <span class="hlt">layer-by-layer</span> nano self-assembly. Alternating <span class="hlt">layers</span> of oppositely charged polyelectrolytes, with enzyme <span class="hlt">layers</span> "encased" between them, were deposited onto the walls of the <span class="hlt">silicon</span> microchannels. The polycations used were polyethylenimine (PEI), polydiallyldimethylammonium (PDDA), and polyallylamine (PAH). The polyanions used were polystyrenesulfonate (PSS) and polyvinylsulfate (PVS). The activity of the immobilized enzyme was tested by pumping a 1 g/L urea solution through the microchannels at various flow rates. Effluent concentration was measured using an ultraviolet/visible spectrometer by monitoring the absorbance of a pH sensitive dye. The architecture of PEI/PSS/PEI/urease/PEI with single and multiple <span class="hlt">layers</span> of enzyme demonstrated superior performance over the PDDA and PAH architectures. The precursor <span class="hlt">layer</span> of PEI/PSS demonstrably improved the performance of the reactor. Conversion rates of 70% were achieved at a residence time of 26 s, on d 1 of operation, and >50% at 51 s, on d 15 with a six-<span class="hlt">layer</span> PEI/urease architecture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014MS%26E...63a2160K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014MS%26E...63a2160K"><span>Low-cycle fatigue of <span class="hlt">Fe</span>-20%<span class="hlt">Cr</span> alloy processed by equal- channel angular pressing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaneko, Yoshihisa; Tomita, Ryuji; Vinogradov, Alexei</p> <p>2014-08-01</p> <p>Low-cycle fatigue properties were investigated on <span class="hlt">Fe</span>-20%<span class="hlt">Cr</span> ferritic stainless steel processed by equal channel angular pressing (ECAP). The <span class="hlt">Fe</span>-20%<span class="hlt">Cr</span> alloy bullets were processed for one to four passes via Route-Bc. The ECAPed samples were cyclically deformed at the constant plastic strain amplitude ɛpl of 5x10-4 at room temperature in air. After the 1-pass ECAP, low-angle grain boundaries were dominantly formed. During the low-cycle fatigue test, the 1-pass sample revealed the rapid softening which continued until fatigue fracture. Fatigue life of the 1-pass sample was shorter than that of a coarse-grained sample. After the 4-pass ECAP, the average grain size reduced down to about 1.5 μm. At initial stage of the low-cycle fatigue tests, the stress amplitude increased with increasing ECAP passes. At the samples processed for more than 2 passes, the cyclic softening was relatively moderate. It was found that fatigue life of the ECAPed <span class="hlt">Fe</span>-20%<span class="hlt">Cr</span> alloy excepting the 1-pass sample was improved as compared to the coarse-grained sample, even under the strain controlled fatigue condition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5513520','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5513520"><span>Organometallic Routes into the Nanorealms of Binary <span class="hlt">Fe</span>-Si Phases</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kolel-Veetil, Manoj K.; Keller, Teddy M.</p> <p>2010-01-01</p> <p>The <span class="hlt">Fe</span>-Si binary system provides several iron silicides that have varied and exceptional material properties with applications in the electronic industry. The well known <span class="hlt">Fe</span>-Si binary silicides are <span class="hlt">Fe</span>3Si, <span class="hlt">Fe</span>5Si3, <span class="hlt">Fe</span>Si, α-<span class="hlt">Fe</span>Si2 and β-<span class="hlt">Fe</span>Si2. While the iron-rich silicides <span class="hlt">Fe</span>3Si and <span class="hlt">Fe</span>5Si3 are known to be room temperature ferromagnets, the stoichiometric <span class="hlt">Fe</span>Si is the only known transition metal Kondo insulator. Furthermore, <span class="hlt">Fe</span>5Si3 has also been demonstrated to exhibit giant magnetoresistance (GMR). The <span class="hlt">silicon</span>-rich β-<span class="hlt">Fe</span>Si2 is a direct band gap material usable in light emitting diode (LED) applications. Typically, these silicides are synthesized by traditional solid-state reactions or by ion beam-induced mixing (IBM) of alternating metal and <span class="hlt">silicon</span> <span class="hlt">layers</span>. Alternatively, the utilization of organometallic compounds with reactive transition metal (<span class="hlt">Fe</span>)-carbon bonds has opened various routes for the preparation of these silicides and the <span class="hlt">silicon</span>-stabilized bcc- and fcc-<span class="hlt">Fe</span> phases contained in the <span class="hlt">Fe</span>-Si binary phase diagram. The unique interfacial interactions of carbon with the <span class="hlt">Fe</span> and Si components have resulted in the preferential formation of nanoscale versions of these materials. This review will discuss such reactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006APS..MARY22004A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006APS..MARY22004A"><span>X-ray reflectivity of ruthenium nano-oxide <span class="hlt">layer</span> in a Co<span class="hlt">Fe-Ru-CoFe</span> trilayer system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Asghari Zadeh, Saeid; Sutton, Mark; Altonian, Zaven; Mao, Ming; Lee, Chih-Ling</p> <p>2006-03-01</p> <p>A grazing incidence X-ray reflectivity technique is used to determine electron density profile(EDP) as a function of depth in Co<span class="hlt">Fe-Ru-CoFe</span> and Co<span class="hlt">Fe</span>-Ru nano oxide <span class="hlt">layer(NOL)-CoFe</span> trilayers. Four trilayers with ruthenium thicknesses of 8,8.5 and 9 å.08cm and one with Ru8.5.05cmå.05cmNOL, prepared by a dc planetary sputtering system, were investigated. For all samples, EDP shows a central peak which is related to the Ru <span class="hlt">layer</span>. Natural oxidation in all samples introduces a graded EDP of the top Co<span class="hlt">Fe</span> <span class="hlt">layer</span> that decreases gradually to zero. The large surface resistivity of Ru8.5 å.05cm NOL compared to Ru 8.5å.08cm can be related to the remarkable difference between their EDP.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JAP...103i4904A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JAP...103i4904A"><span>Ruthenium nano-oxide <span class="hlt">layer</span> in Co<span class="hlt">Fe-Ru-CoFe</span> trilayer system: An x-ray reflectivity study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Asgharizadeh, S.; Sutton, M.; Altounian, Z.; Mao, M.; Lee, C. L.</p> <p>2008-05-01</p> <p>A grazing incidence x-ray reflectivity technique is used to determine the electron density profile as a function of depth in Co<span class="hlt">Fe-Ru-CoFe</span> and Co<span class="hlt">Fe</span>-Ru nano-oxide <span class="hlt">layer</span> (NOL)-Co<span class="hlt">Fe</span> trilayers. Four trilayers with ruthenium thicknesses of 8, 8.5, and 9Å and one with Ru 8.5Å NOL, prepared by a dc planetary sputtering system, were investigated. For all samples, the electron density profile (EDP) shows a central peak that is related to the Ru <span class="hlt">layer</span>. Natural oxidation in all of the samples introduces a graded EDP of the top Co<span class="hlt">Fe</span> <span class="hlt">layers</span>, which decreases gradually to zero. The large surface resistivity of Ru 8.5Å NOL as compared to Ru 8.5Å is related to the remarkable difference between their EDPs. EDP changes have also been investigated in Ru NOL trilayers after annealing at 280°C. The Ru phase in the EDP was observed to confirm the thermal stability of the spacer <span class="hlt">layer</span> after annealing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MRE.....4f5013N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MRE.....4f5013N"><span>Characterization of Ag-porous <span class="hlt">silicon</span> nanostructured <span class="hlt">layer</span> formed by an electrochemical etching of p-type <span class="hlt">silicon</span> surface for bio-application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Naddaf, M.; Al-Mariri, A.; Haj-Mhmoud, N.</p> <p>2017-06-01</p> <p>Nanostructured <span class="hlt">layers</span> composed of silver-porous <span class="hlt">silicon</span> (Ag-PS) have been formed by an electrochemical etching of p-type (1 1 1) <span class="hlt">silicon</span> substrate in a AgNO3:HF:C2H5OH solution at different etching times (10 min-30 min). Scanning electron microscopy (SEM) and energy-dispersive x-ray spectroscopy (EDS) results reveal that the produced <span class="hlt">layers</span> consist of Ag dendrites and a <span class="hlt">silicon</span>-rich porous structure. The nanostructuring nature of the <span class="hlt">layer</span> has been confirmed by spatial micro-Raman scattering and x-ray diffraction techniques. The Ag dendrites exhibit a surface-enhanced Raman scattering (SERS) spectrum, while the porous structure shows a typical PS Raman spectrum. Upon increasing the etching time, the average size of <span class="hlt">silicon</span> nanocrystallite in the PS network decreases, while the average size of Ag nanocrystals is slightly affected. In addition, the immobilization of prokaryote Salmonella typhimurium DNA via physical adsorption onto the Ag-PS <span class="hlt">layer</span> has been performed to demonstrate its efficiency as a platform for detection of biological molecules using SERS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MMI....23..336K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MMI....23..336K"><span>Effects of particle size and forming pressure on pore properties of <span class="hlt">Fe-Cr</span>-Al porous metal by pressureless sintering</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koo, Bon-Uk; Yi, Yujeong; Lee, Minjeong; Kim, Byoung-Kee</p> <p>2017-03-01</p> <p>With increased hydrogen consumption in ammonia production, refining and synthesis, fuel cells and vehicle industries, development of the material components related to hydrogen production is becoming an important factor in industry growth. Porous metals for fabrication of hydrogen are commonly known for their relative excellence in terms of large area, lightness, lower heat capacity, high toughness, and permeability. <span class="hlt">Fe-Cr</span>-Al alloys not only have high corrosion resistance, heat resistance, and chemical stability but also ductility, excellent mechanical properties. In order to control powder size and sintering temperature effects of <span class="hlt">Fe-Cr</span>-Al porous metal fabrication, <span class="hlt">Fe-Cr</span>-Al powder was classified into 25-35 μm, 35-45 μm, 45-75 μm using an auto shaking sieve machine and then classified <span class="hlt">Fe-Cr</span>-Al powders were pressed into disk shapes using a uniaxial press machine and CIP. The pelletized <span class="hlt">Fe-Cr</span>-Al specimens were sintered at various temperatures in high vacuum. Properties such as pore size, porosity, and air permeability were evaluated using perm-porosimetry. Microstructure and phase changes were observed with SEM and XRD. Porosity and relative density were proportionated to increasing sintering temperature. With sufficient sintering at increasing temperatures, the pore size is expected to be gradually reduced. Porosity decreased with increasing sintering temperature and gradually increased necking of the powder.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1354773-cao-fese-layered-wide-gap-oxychalcogenide-semiconductor','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1354773-cao-fese-layered-wide-gap-oxychalcogenide-semiconductor"><span>(CaO)(<span class="hlt">Fe</span>Se): A <span class="hlt">layered</span> wide-gap oxychalcogenide semiconductor</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Han, Fei; Wang, Di; Malliakas, Christos D.; ...</p> <p>2015-07-20</p> <p>A new iron-oxychalcogenide (CaO)(<span class="hlt">Fe</span>Se) was obtained which crystallizes in the orthorhombic space group Pnma (No. 62) with a = 5.9175(12) Å, b = 3.8797(8) Å, c = 13.170(3) Å. The unique structure of (CaO)(<span class="hlt">Fe</span>Se) is built up of a quasi-two-dimensional network of corrugated infinite <span class="hlt">layers</span> of corner-shared <span class="hlt">Fe</span>Se 2O 2 tetrahedra that extend in the ab-plane. The <span class="hlt">Fe</span>Se 2O 2 <span class="hlt">layers</span> stack along the c-axis with Ca 2+ cations sandwiched between the <span class="hlt">layers</span>. Optical spectroscopy and resistivity measurements reveal semiconducting behavior with an indirect optical band gap of around 1.8 eV and an activation energy of 0.19(1) eV. Furthermore, electronicmore » band structure calculations at the density function level predict a magnetic configuration as ground state and confirm the presence of an indirect wide gap in (CaO)(<span class="hlt">Fe</span>Se).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999GeCoA..63.1517K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999GeCoA..63.1517K"><span>Reactive <span class="hlt">Fe</span>(II) <span class="hlt">layers</span> in deep-sea sediments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>König, Iris; Haeckel, Matthias; Drodt, Matthias; Suess, Erwin; Trautwein, Alfred X.</p> <p>1999-05-01</p> <p>The percentage of the structural <span class="hlt">Fe</span>(II) in clay minerals that is readily oxidized to <span class="hlt">Fe</span>(III) upon contact with atmospheric oxygen was determined across the downcore tan-green color change in Peru Basin sediments. This latent fraction of reactive <span class="hlt">Fe</span>(II) was only found in the green strata, where it proved to be large enough to constitute a deep reaction <span class="hlt">layer</span> with respect to the pore water O 2 and NO 3-. Large variations were detected in the proportion of the reactive <span class="hlt">Fe</span>(II) concentration to the organic matter content along core profiles. Hence, the commonly observed tan-green color change in marine sediments marks the top of a reactive <span class="hlt">Fe</span>(II) <span class="hlt">layer</span>, which may represent the major barrier to the movement of oxidation fronts in pelagic subsurface sediments. This is also demonstrated by numerical model simulations. The findings imply that geochemical barriers to pore water oxidation fronts form diagenetically in the sea floor wherever the stage of iron reduction is reached, provided that the sediments contain a significant amount of structural iron in clay minerals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97r4431P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97r4431P"><span>From mean-field localized magnetism to itinerant spin fluctuations in the "nonmetallic metal" <span class="hlt">FeCr</span>As</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Plumb, K. W.; Stock, C.; Rodriguez-Rivera, J. A.; Castellan, J.-P.; Taylor, J. W.; Lau, B.; Wu, W.; Julian, S. R.; Kim, Young-June</p> <p>2018-05-01</p> <p><span class="hlt">FeCr</span>As displays an unusual electrical response that is neither metallic in character nor divergent at low temperatures, as expected for an insulating response, and therefore it has been termed a "nonmetal metal." The anomalous resistivity occurs for temperatures below ˜900 K. We have carried out neutron scattering experiments on powder and single crystal samples to study the magnetic dynamics and critical fluctuations in <span class="hlt">FeCr</span>As. Magnetic neutron diffraction measurements find <span class="hlt">Cr</span>3 + magnetic order setting in at TN=115 K ˜10 meV with a mean-field critical exponent. Using neutron spectroscopy we observe gapless, high velocity, magnetic fluctuations emanating from magnetic positions with propagation wave vector q⃗0=(1/3 ,1/3 ) , which persists up to at least 80 meV ˜927 K, an energy scale much larger than TN. Despite the mean-field magnetic order at low temperatures, the magnetism in <span class="hlt">FeCr</span>As therefore displays a response which resembles that of itinerant magnets at high energy transfers. We suggest that the presence of stiff high-energy spin fluctuations extending up to a temperature scale of ˜900 K is the origin of the unusual temperature dependence of the resistivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014MMTA...45.5114M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014MMTA...45.5114M"><span>on the High-Temperature Performance of Ni-Based Welding Material Ni<span class="hlt">CrFe</span>-7</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mo, Wenlin; Lu, Shanping; Li, Dianzhong; Li, Yiyi</p> <p>2014-10-01</p> <p>The effects of M 23C6 ( M = <span class="hlt">Cr</span>, <span class="hlt">Fe</span>) on the high-temperature performance of the Ni<span class="hlt">CrFe</span>-7 welding rods and weld metals were studied by high-temperature tensile tests and microstructure analysis. M 23C6 at the grain boundaries (GBs) has a cube-on-cube coherence with one grain in the Ni<span class="hlt">CrFe</span>-7 weld metals, and the adjacent M 23C6 has the coherence relationship with the same grain. The grain with a coherent M 23C6 has a <span class="hlt">Cr</span>-depletion region. The number and size of M 23C6 particles can be adjusted by heat treatment and alloying. There are two temperatures [ T E1: 923 K to 1083 K (650 °C to 810 °C) and T E2: 1143 K to 1203 K (870 °C to 930 °C)] at which the GBs and grains of the Ni<span class="hlt">CrFe</span>-7 welding rod have equal strength during the high-temperature tensile test. When the temperatures are between T E1 and T E2, the strength of the GBs is lower than that of the grains, and the tensile fractures are intergranular. When the temperatures are below T E1 or over T E2, the strength of the GBs is higher than that of the grains, and the tensile fractures are dimples. M 23C6 precipitates at the GBs, which deteriorates the ductility of the welding rods at temperature between T E1 and T E2. M 23C6 aggravates ductility-dip-cracking (DDC) in the weld metals. The addition of Nb and Ti can form MX ( M = Ti, Nb, X = C, N), fix C in grain, decrease the initial precipitation temperature of M 23C6, and mitigate the precipitation of M 23C6, which is helpful for minimizing DDC in the weld.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014DokPh..59..267S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014DokPh..59..267S"><span>Perovskites Bi0.8La0.2<span class="hlt">Fe</span>O3 and Bi0.8La0.2<span class="hlt">Fe</span>0.95<span class="hlt">Cr</span>0.05O3: Crystal structure and magnetic and charge states of iron ions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sigov, A. S.; Pokatilov, V. S.; Makarova, A. O.; Pokatilov, V. V.</p> <p>2014-06-01</p> <p>Perovskites of the Bi0.8La0.2<span class="hlt">Fe</span>1 - x <span class="hlt">Cr</span> x O3 system ( x = 0, 0.05) were investigated by Mössbauer spectroscopy in the temperature range of 298-800 K. The samples were fabricated by solid-state synthesis and had a rhombic structure. Iron ions in Bi0.8La0.2<span class="hlt">Fe</span>O3 and Bi0.8La0.2<span class="hlt">Fe</span>0.95<span class="hlt">Cr</span>0.05O3 are situated in trivalent states. The magnetic transition temperatures (the Néel temperatures T N ) T N = 677.5 ± 2.5 K for Bi0.8La0.2<span class="hlt">Fe</span>O3 and T N = 647.6 ± 2.5 K for Bi0.8La0.2<span class="hlt">Fe</span>0.95<span class="hlt">Cr</span>0.05O3 are measured. The substitution of trivalent iron ions from trivalent chromium ions in the amount x = 0.05 in Bi0.8La0.2<span class="hlt">Fe</span>0.95<span class="hlt">Cr</span>0.05O3 perovskite decreases the hyperfine magnetic field at nuclei 57<span class="hlt">Fe</span> in <span class="hlt">Fe</span>+3-O-<span class="hlt">Cr</span>+3 chains by 30 kOe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.712a2097M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.712a2097M"><span>Weathering and precipitation after meteorite impact of Ni, <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Ca and Mn in K-T boundary clays from Stevns Klint</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miyano, Yumiko; Yoshiasa, Akira; Tobase, Tsubasa; Isobe, Hiroshi; Hongu, Hidetomo; Okube, Maki; Nakatsuka, Akihiko; Sugiyama, Kazumasa</p> <p>2016-05-01</p> <p>Ni, <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Ca and Mn K-edge XANES and EXAFS spectra were measured on K-T boundary clays from Stevns Klint in Denmark. According to XANES spectra and EXAFS analyses, the local structures of Ni, <span class="hlt">Cr</span> and <span class="hlt">Fe</span> in K-T boundary clays is similar to Ni(OH)2, <span class="hlt">Cr</span>2O3 and <span class="hlt">Fe</span>OOH, respectively. It is assumed that the Ni, <span class="hlt">Cr</span> and <span class="hlt">Fe</span> elements in impact related glasses is changing into stable hydrate and oxide by the weathering and diagenesis at the surface of the Earth. Ca in K-T boundary clays maintains the diopside-like structure. Local structure of Ca in K-T clays seems to keep information on the condition at meteorite impact. Mn has a local structure like MnCO3 with divalent state. It is assumed that the origin on low abundant of Mn in the <span class="hlt">Fe</span>-group element in K-T clays was the consumption by life activity and the diffusion to other parts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhLB..767...20Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhLB..767...20Z"><span>High-precision QEC values of superallowed 0+ → 0+β-emitters 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, P.; Xu, X.; Shuai, P.; Chen, R. J.; Yan, X. L.; Zhang, Y. H.; Wang, M.; Litvinov, Yu. A.; Blaum, K.; Xu, H. S.; Bao, T.; Chen, X. C.; Chen, H.; Fu, C. Y.; He, J. J.; Kubono, S.; Lam, Y. H.; Liu, D. W.; Mao, R. S.; Ma, X. W.; Sun, M. Z.; Tu, X. L.; Xing, Y. M.; Yang, J. C.; Yuan, Y. J.; Zeng, Q.; Zhou, X.; Zhou, X. H.; Zhan, W. L.; Litvinov, S.; Audi, G.; Uesaka, T.; Yamaguchi, Y.; Yamaguchi, T.; Ozawa, A.; Sun, B. H.; Sun, Y.; Xu, F. R.</p> <p>2017-04-01</p> <p>Short-lived 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni were studied by isochronous mass spectrometry at the HIRFL-CSR facility in Lanzhou. The measured precision mass excesses (ME) of 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni are - 29471 (11) keV, - 34477 (6) keV and - 39278 (4) keV, respectively. The superallowed 0+ →0+β-decay Q values were derived to be QEC (46<span class="hlt">Cr</span>) = 7604 (11) keV, QEC (50<span class="hlt">Fe</span>) = 8150 (6) keV and QEC (54Ni) = 8731 (4) keV. The values for 50<span class="hlt">Fe</span> and 54Ni are by one order of magnitude more precise than the adopted literature values. By combining the existing half-lives and branching ratios, we obtained the corrected Ft values to be Ft (50<span class="hlt">Fe</span>) = 3103 (70) s and Ft (54Ni) = 3076 (50) s. The main contribution to the Ft uncertainties is now due to β-decay branching ratios, still, more high-precision measurements of the half-lives, the masses, and especially the branching ratios are needed in order to satisfy the requirements for a stringent CVC test.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24468364','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24468364"><span>Flow microcapillary plasma mass spectrometry-based investigation of new Al-<span class="hlt">Cr-Fe</span> complex metallic alloy passivation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ott, N; Beni, A; Ulrich, A; Ludwig, C; Schmutz, P</p> <p>2014-03-01</p> <p>Al-<span class="hlt">Cr-Fe</span> complex metallic alloys are new intermetallic phases with low surface energy, low friction, and high corrosion resistance down to very low pH values (0-2). Flow microcapillary plasma mass spectrometry under potentiostatic control was used to characterize the dynamic aspect of passivation of an Al-<span class="hlt">Cr-Fe</span> gamma phase in acidic electrolytes, allowing a better insight on the parameters inducing chemical stability at the oxyhydroxide-solution interface. In sulfuric acid pH 0, low element dissolution rates (in the µg cm(-2) range after 60 min) evidenced the passive state of the Al-<span class="hlt">Cr-Fe</span> gamma phase with a preferential over-stoichiometric dissolution of Al and <span class="hlt">Fe</span> cations. Longer air-aging was found to be beneficial for stabilizing the passive film. In chloride-containing electrolytes, ten times higher Al dissolution rates were detected at open-circuit potential (OCP), indicating that the spontaneously formed passive film becomes unstable. However, electrochemical polarization at low passive potentials induces electrical field generated oxide film modification, increasing chemical stability at the oxyhydroxide-solution interface. In the high potential passive region, localized attack is initiated with subsequent active metal dissolution. © 2013 Published by Elsevier B.V.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22649622-surface-texture-single-crystal-silicon-oxidized-under-thin-sub-sub-layer','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22649622-surface-texture-single-crystal-silicon-oxidized-under-thin-sub-sub-layer"><span>Surface texture of single-crystal <span class="hlt">silicon</span> oxidized under a thin V{sub 2}O{sub 5} <span class="hlt">layer</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>Nikitin, S. E., E-mail: nikitin@mail.ioffe.ru; Verbitskiy, V. N.; Nashchekin, A. V.</p> <p></p> <p>The process of surface texturing of single-crystal <span class="hlt">silicon</span> oxidized under a V{sub 2}O{sub 5} <span class="hlt">layer</span> is studied. Intense <span class="hlt">silicon</span> oxidation at the Si–V{sub 2}O{sub 5} interface begins at a temperature of 903 K which is 200 K below than upon <span class="hlt">silicon</span> thermal oxidation in an oxygen atmosphere. A <span class="hlt">silicon</span> dioxide <span class="hlt">layer</span> 30–50 nm thick with SiO{sub 2} inclusions in <span class="hlt">silicon</span> depth up to 400 nm is formed at the V{sub 2}O{sub 5}–Si interface. The diffusion coefficient of atomic oxygen through the <span class="hlt">silicon</span>-dioxide <span class="hlt">layer</span> at 903 K is determined (D ≥ 2 × 10{sup –15} cm{sup 2} s{sup –1}). A modelmore » of low-temperature <span class="hlt">silicon</span> oxidation, based on atomic oxygen diffusion from V{sub 2}O{sub 5} through the SiO{sub 2} <span class="hlt">layer</span> to <span class="hlt">silicon</span>, and SiO{sub x} precipitate formation in <span class="hlt">silicon</span> is proposed. After removing the V{sub 2}O{sub 5} and <span class="hlt">silicon</span>-dioxide <span class="hlt">layers</span>, texture is formed on the <span class="hlt">silicon</span> surface, which intensely scatters light in the wavelength range of 300–550 nm and is important in the texturing of the front and rear surfaces of solar cells.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JMMM..399..192O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JMMM..399..192O"><span>Changes in cluster magnetism and suppression of local superconductivity in amorphous <span class="hlt">FeCr</span>B alloy irradiated by Ar+ ions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Okunev, V. D.; Samoilenko, Z. A.; Szymczak, H.; Szewczyk, A.; Szymczak, R.; Lewandowski, S. J.; Aleshkevych, P.; Malinowski, A.; Gierłowski, P.; Więckowski, J.; Wolny-Marszałek, M.; Jeżabek, M.; Varyukhin, V. N.; Antoshina, I. A.</p> <p>2016-02-01</p> <p>We show that сluster magnetism in ferromagnetic amorphous <span class="hlt">Fe</span>67<span class="hlt">Cr</span>18B15 alloy is related to the presence of large, D=150-250 Å, α-(<span class="hlt">Fe</span> <span class="hlt">Cr</span>) clusters responsible for basic changes in cluster magnetism, small, D=30-100 Å, α-(<span class="hlt">Fe</span>, <span class="hlt">Cr</span>) and <span class="hlt">Fe</span>3B clusters and subcluster atomic α-(<span class="hlt">Fe</span>, <span class="hlt">Cr</span>, B) groupings, D=10-20 Å, in disordered intercluster medium. For initial sample and irradiated one (Φ=1.5×1018 ions/cm2) superconductivity exists in the cluster shells of metallic α-(<span class="hlt">Fe</span>, <span class="hlt">Cr</span>) phase where ferromagnetism of iron is counterbalanced by antiferromagnetism of chromium. At Φ=3×1018 ions/cm2, the internal stresses intensify and the process of iron and chromium phase separation, favorable for mesoscopic superconductivity, changes for inverse one promoting more homogeneous distribution of iron and chromium in the clusters as well as gigantic (twice as much) increase in density of the samples. As a result, in the cluster shells ferromagnetism is restored leading to the increase in magnetization of the sample and suppression of local superconductivity. For initial samples, the temperature dependence of resistivity ρ(T) T2 is determined by the electron scattering on quantum defects. In strongly inhomogeneous samples, after irradiation by fluence Φ=1.5×1018 ions/cm2, the transition to a dependence ρ(T) T1/2 is caused by the effects of weak localization. In more homogeneous samples, at Φ=3×1018 ions/cm2, a return to the dependence ρ(T) T2 is observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JTST...25..526X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JTST...25..526X"><span>Formation of <span class="hlt">Cr</span>2O3 Diffusion Barrier Between <span class="hlt">Cr</span>-Contained Stainless Steel and Cold-Sprayed Ni Coatings at High Temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Ya-Xin; Luo, Xiao-Tao; Li, Cheng-Xin; Yang, Guan-Jun; Li, Chang-Jiu</p> <p>2016-02-01</p> <p>A novel approach to prepare a coating system containing an in situ grown <span class="hlt">Cr</span>2O3 diffusion barrier between a nickel top <span class="hlt">layer</span> and 310SS was reported. Cold spraying was employed to deposit Ni(O) interlayer and top nickel coating on the <span class="hlt">Cr</span>-contained stainless steel substrate. Ni(O) feedstock was prepared by mechanical alloying of pure nickel powders in ambient atmosphere, acting as an oxygen provider. The post-spray annealing was adopted to grow in situ <span class="hlt">Cr</span>2O3 <span class="hlt">layer</span> between the substrate and nickel coating. The results revealed that the diffusible oxygen can be introduced into nickel powders by mechanical alloying. The oxygen content increases to 3.25 wt.% with the increase of the ball milling duration to 8 h, while Ni(O) powders maintain a single phase of Ni. By annealing the sample in Ar atmosphere at 900 °C, a continuous <span class="hlt">Cr</span>2O3 <span class="hlt">layer</span> of 1-2 μm thick at the interface between 310SS and cold-sprayed Ni coating is formed. The diffusion barrier effect evaluation by thermal exposure at 750 °C shows that the <span class="hlt">Cr</span>2O3 oxide <span class="hlt">layer</span> effectively suppresses the outward diffusion of <span class="hlt">Fe</span> and <span class="hlt">Cr</span> in the substrate effectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/865154','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/865154"><span>Oxidation sulfidation resistance of <span class="hlt">Fe-Cr</span>-Ni alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Natesan, Ken; Baxter, David J.</p> <p>1984-01-01</p> <p>High temperature resistance of <span class="hlt">Fe-Cr</span>-Ni alloy compositions to oxidative and/or sulfidative conditions is provided by the incorporation of about 1-8 wt. % of Zr or Nb and results in a two-phase composition having an alloy matrix as the first phase and a fine grained intermetallic composition as the second phase. The presence and location of the intermetallic composition between grains of the matrix provides mechanical strength, enhanced surface scale adhesion, and resistance to corrosive attack between grains of the alloy matrix at temperatures of 500.degree.-1000.degree. C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1286988','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1286988"><span>The Analysis of the General Performance and Mechanical Behavior of Unirradiated <span class="hlt">FeCr</span>Al Alloys Before and After Welding</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>Gussev, Maxim N.; Field, Kevin G.; Yamamoto, Yukinori</p> <p>2016-06-03</p> <p>The present report summarizes and discusses the preliminary results for the in-depth characterization of the modern, nuclear-grade <span class="hlt">FeCr</span>Al alloys currently under development. The alloys were designed for enhanced radiation tolerance and weldability, and the research is currently being pursued by the Department of Energy (DOE) Nuclear Energy Enabling Technologies (NEET) program. Last year, seven candidate <span class="hlt">FeCr</span>Al alloys with well-controlled chemistry and microstructures were designed and produced; welding was performed under well-controlled conditions. The structure and general performance of unirradiated alloys were assessed using standardized and advanced microstructural characterization techniques and mechanical testing. The primary objective is to identify the bestmore » candidate alloy, or at a minimum to identify the contributing factors that increase the weldability and radiation tolerance of <span class="hlt">FeCr</span>Al alloys, therefore enabling future generations of <span class="hlt">FeCr</span>Al alloys to deliver better performance parameters. This report is structured so as to describe these critical assessments of the weldability; radiation tolerance will be reported on in later reports from this program.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1133989-non-classical-nuclei-growth-kinetics-cr-precipitates-fecr-alloys-during-ageing','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1133989-non-classical-nuclei-growth-kinetics-cr-precipitates-fecr-alloys-during-ageing"><span>Non-classical nuclei and growth kinetics of <span class="hlt">Cr</span> precipitates in <span class="hlt">FeCr</span> alloys during ageing</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, Yulan; Hu, Shenyang Y.; Zhang, Lei</p> <p>2014-01-10</p> <p>In this manuscript, we quantitatively calculated the thermodynamic properties of critical nuclei of <span class="hlt">Cr</span> precipitates in <span class="hlt">FeCr</span> alloys. The concentration profiles of the critical nuclei and nucleation energy barriers were predicted by the constrained shrinking dimer dynamics (CSDD) method. It is found that <span class="hlt">Cr</span> concentration distribution in the critical nuclei strongly depend on the overall <span class="hlt">Cr</span> concentration as well as temperature. The critical nuclei are non-classical because the concentration in the nuclei is smaller than the thermodynamic equilibrium value. These results are in agreement with atomic probe observation. The growth kinetics of both classical and non-classical nuclei was investigated bymore » the phase field approach. The simulations of critical nucleus evolution showed a number of interesting phenomena: 1) a critical classical nucleus first shrinks toward its non-classical nucleus and then grows; 2) a non-classical nucleus has much slower growth kinetics at its earlier growth stage compared to the diffusion-controlled growth kinetics. 3) a critical classical nucleus grows faster at the earlier growth stage than the non-classical nucleus. All of these results demonstrate that it is critical to introduce the correct critical nuclei in order to correctly capture the kinetics of precipitation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25988512','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25988512"><span>Epitaxial Bi2 <span class="hlt">FeCr</span>O6 Multiferroic Thin Film as a New Visible Light Absorbing Photocathode Material.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Shun; AlOtaibi, Bandar; Huang, Wei; Mi, Zetian; Serpone, Nick; Nechache, Riad; Rosei, Federico</p> <p>2015-08-26</p> <p>Ferroelectric materials have been studied increasingly for solar energy conversion technologies due to the efficient charge separation driven by the polarization induced internal electric field. However, their insufficient conversion efficiency is still a major challenge. Here, a photocathode material of epitaxial double perovskite Bi(2) <span class="hlt">FeCr</span>O(6) multiferroic thin film is reported with a suitable conduction band position and small bandgap (1.9-2.1 eV), for visible-light-driven reduction of water to hydrogen. Photoelectrochemical measurements show that the highest photocurrent density up to -1.02 mA cm(-2) at a potential of -0.97 V versus reversible hydrogen electrode is obtained in p-type Bi(2) <span class="hlt">FeCr</span>O(6) thin film photocathode grown on SrTiO(3) substrate under AM 1.5G simulated sunlight. In addition, a twofold enhancement of photocurrent density is obtained after negatively poling the Bi(2) <span class="hlt">FeCr</span>O(6) thin film, as a result of modulation of the band structure by suitable control of the internal electric field gradient originating from the ferroelectric polarization in the Bi(2) <span class="hlt">FeCr</span>O(6) films. The findings validate the use of multiferroic Bi(2) <span class="hlt">FeCr</span>O(6) thin films as photocathode materials, and also prove that the manipulation of internal fields through polarization in ferroelectric materials is a promising strategy for the design of improved photoelectrodes and smart devices for solar energy conversion. © 2015 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22645592-influence-surface-layer-electrochemical-deposition-metals-semiconductors-mesoporous-silicon','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22645592-influence-surface-layer-electrochemical-deposition-metals-semiconductors-mesoporous-silicon"><span>Influence of the Surface <span class="hlt">Layer</span> on the Electrochemical Deposition of Metals and Semiconductors into Mesoporous <span class="hlt">Silicon</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>Chubenko, E. B., E-mail: eugene.chubenko@gmail.com; Redko, S. V.; Sherstnyov, A. I.</p> <p>2016-03-15</p> <p>The influence of the surface <span class="hlt">layer</span> on the process of the electrochemical deposition of metals and semiconductors into porous <span class="hlt">silicon</span> is studied. It is shown that the surface <span class="hlt">layer</span> differs in structure and electrical characteristics from the host porous <span class="hlt">silicon</span> bulk. It is established that a decrease in the conductivity of <span class="hlt">silicon</span> crystallites that form the surface <span class="hlt">layer</span> of porous <span class="hlt">silicon</span> has a positive effect on the process of the filling of porous <span class="hlt">silicon</span> with metals and semiconductors. This is demonstrated by the example of nickel and zinc oxide. The effect can be used for the formation of nanocomposite materialsmore » on the basis of porous <span class="hlt">silicon</span> and nanostructures with a high aspect ratio.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/912300-reduction-cr-vi-under-acidic-conditions-facultative-fe-iii-reducing-bacterium-acidiphilium-cryptum','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/912300-reduction-cr-vi-under-acidic-conditions-facultative-fe-iii-reducing-bacterium-acidiphilium-cryptum"><span>Reduction of <span class="hlt">Cr</span>(VI) under acidic conditions by the facultative <span class="hlt">Fe</span>(III)-reducing bacterium Acidiphilium cryptum</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>David E. Cummings; Scott Fendorf; Rajesh K. Sani</p> <p>2007-01-01</p> <p>The potential for biological reduction of <span class="hlt">Cr</span>(VI) under acidic conditions was evaluated with the acidophilic, facultatively metal-reducing bacterium Acidiphilium cryptum strain JF-5 to explore the role of acidophilic microorganisms in the <span class="hlt">Cr</span> cycle in low-pH environments. An anaerobic suspension of washed A. cryptum cells rapidly reduced 50 M <span class="hlt">Cr</span>(VI) at pH 3.2; biological reduction was detected from pH 1.7-4.7. The reduction product, confirmed by XANES analysis, was entirely <span class="hlt">Cr</span>(III) that was associated predominantly with the cell biomass (70-80%) with the residual residing in the aqueous phase. Reduction of <span class="hlt">Cr</span>(VI) showed a pH optimum similar to that for growth and wasmore » inhibited by 5 mM HgCl2, suggesting that the reaction was enzyme-mediated. Introduction of O2 into the reaction medium slowed the reduction rate only slightly, whereas soluble <span class="hlt">Fe</span>(III) (as ferric sulfate) increased the rate dramatically, presumably by the shuttling of electrons from bioreduced <span class="hlt">Fe</span>(II) to <span class="hlt">Cr</span>(VI) in a coupled biotic-abiotic cycle. Starved cells could not reduce <span class="hlt">Cr</span>(VI) when provided as sole electron acceptor, indicating that <span class="hlt">Cr</span>(VI) reduction is not an energy-conserving process in A. cryptum. We speculate, rather, that <span class="hlt">Cr</span>(VI) reduction is used here as a detoxification mechanism.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCS..115...92D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCS..115...92D"><span>Thermal expansion properties of Ho2<span class="hlt">Fe</span>16.5<span class="hlt">Cr</span>0.5</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dan, Shovan; Mukherjee, S.; Mazumdar, Chandan; Ranganathan, R.</p> <p>2018-04-01</p> <p>We report the thermal expansion behavior of Ho2<span class="hlt">Fe</span>16.5<span class="hlt">Cr</span>0.5 compound in the range of temperature 13-483 K, using structural parameters obtained by analyzing temperature dependent x-ray diffraction (XRD) patterns. From 13 K to 300 K, the compound shows negligible thermal expansion having the coefficient of volume expansion (αV) ∼ 10-6 K -1. The thermal expansion behavior of the studied compound can be explained by the role of magnetovolume effect (MVE) below ferrimagnetic ordering temperature (394 K), in addition to normal phononic contribution. <span class="hlt">Fe</span> sublattice contribute to MVE, whereas both the rare earth and <span class="hlt">Fe</span> sublattice determine the value of saturation magnetization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JSSCh.258...86C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JSSCh.258...86C"><span>A water stable europium coordination polymer as fluorescent sensor for detecting <span class="hlt">Fe</span>3+, <span class="hlt">Cr</span>O42-, and <span class="hlt">Cr</span>2O72- ions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Chen; Zhang, Xiaolei; Gao, Peng; Hu, Ming</p> <p>2018-02-01</p> <p>A europium coordination polymer constructed by the 4‧-(4-carboxyphenyl)- 2,2‧:6‧,2″-terpyridine ligand (HL), namely, [EuL(CH3COO)Cl]n (1), has been prepared by the solvothermal method. Compound 1 was structurally characterized by the elemental analysis, FT-IR, powder X-ray diffractions (PXRD), thermogravimetric (TG) analysis, and single-crystal X-ray diffraction. Complex 1 displays a novel linear chain structure, which further extends to the 3D supramolecular structure via π···π and hydrogen bonds interactions. The luminescent properties of 1 were investigated in detail, which exhibit the fluorescent sensing for detecting <span class="hlt">Fe</span>3+, <span class="hlt">Cr</span>O42-, and <span class="hlt">Cr</span>2O72- ions in aqueous solution, respectively. In addition, 1 shows high sensitive and selective sensing for <span class="hlt">Cr</span>O42- and <span class="hlt">Cr</span>2O72- anions with the great quenching efficiency. Furthermore, the luminescent sensing mechanisms of differentiating analytes are explored in detail. It is worth noting that there exists the weak interaction between <span class="hlt">Fe</span>3+ ions and carboxylate oxygen atoms of CH3COO- groups through XPS characterization, resulting in the high quenching effect of 1.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MMTB...48.1533T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MMTB...48.1533T"><span>Chromium Extraction via Chemical Processing of <span class="hlt">Fe-Cr</span> Alloys Fine Powder with High Carbon Content</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Torres, D. M.; Navarro, R. C. S.; Souza, R. F. M.; Brocchi, E. A.</p> <p>2017-06-01</p> <p>Ferrous alloys are important raw materials for special steel production. In this context, alloys from the <span class="hlt">Fe-Cr</span> system, with typical <span class="hlt">Cr</span> weight fraction ranging from 0.45 to 0.95, are prominent, particularly for the stainless steel industry. During the process in which these alloys are obtained, there is considerable production of fine powder, which could be reused after suitable chemical treatment, for example, through coupling pyrometallurgical and hydrometallurgical processes. In the present study, the extraction of chromium from fine powder generated during the production of a <span class="hlt">Fe-Cr</span> alloy with high C content was investigated. Roasting reactions were performed at 1073 K, 1173 K, and 1273 K (800 °C, 900 °C, and 1000 °C) with 300 pct (w/w) excess NaOH in an oxidizing atmosphere (air), followed by solubilization in deionized water, selective precipitation, and subsequent calcination at 1173 K (900 °C) in order to convert the obtained chromium hydroxide to <span class="hlt">Cr</span>2O3. The maximum achieved <span class="hlt">Cr</span> recovery was around 86 pct, suggesting that the proposed chemical route was satisfactory regarding the extraction of the chromium initially present. Moreover, after X-ray diffraction analysis, the final produced oxide has proven to be pure <span class="hlt">Cr</span>2O3 with a mean crystallite size of 200 nm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27745961','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27745961"><span>Impact of <span class="hlt">Fe</span>(III) as an effective electron-shuttle mediator for enhanced <span class="hlt">Cr</span>(VI) reduction in microbial fuel cells: Reduction of diffusional resistances and cathode overpotentials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Qiang; Huang, Liping; Pan, Yuzhen; Quan, Xie; Li Puma, Gianluca</p> <p>2017-01-05</p> <p>The role of <span class="hlt">Fe</span>(III) was investigated as an electron-shuttle mediator to enhance the reduction rate of the toxic heavy metal hexavalent chromium (<span class="hlt">Cr</span>(VI)) in wastewaters, using microbial fuel cells (MFCs). The direct reduction of chromate (<span class="hlt">Cr</span>O 4 - ) and dichromate (<span class="hlt">Cr</span> 2 O 7 2- ) anions in MFCs was hampered by the electrical repulsion between the negatively charged cathode and <span class="hlt">Cr</span>(VI) functional groups. In contrast, in the presence of <span class="hlt">Fe</span>(III), the conversion of <span class="hlt">Cr</span>(VI) and the cathodic coulombic efficiency in the MFCs were 65.6% and 81.7%, respectively, 1.6 times and 1.4 folds as those recorded in the absence of <span class="hlt">Fe</span>(III). Multiple analytical approaches, including linear sweep voltammetry, Tafel plot, cyclic voltammetry, electrochemical impedance spectroscopy and kinetic calculations demonstrated that the complete reduction of <span class="hlt">Cr</span>(VI) occurred through an indirect mechanism mediated by <span class="hlt">Fe</span>(III). The direct reduction of <span class="hlt">Cr</span>(VI) with cathode electrons in the presence of <span class="hlt">Fe</span>(III) was insignificant. <span class="hlt">Fe</span>(III) played a critical role in decreasing both the diffusional resistance of <span class="hlt">Cr</span>(VI) species and the overpotential for <span class="hlt">Cr</span>(VI) reduction. This study demonstrated that the reduction of <span class="hlt">Cr</span>(VI) in MFCs was effective in the presence of <span class="hlt">Fe</span>(III), providing an alternative and environmentally benign approach for efficient remediation of <span class="hlt">Cr</span>(VI) contaminated sites with simultaneous production of renewable energy. Copyright © 2016 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SuMi...77..219M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SuMi...77..219M"><span>Correlation between optical properties surface morphology of porous <span class="hlt">silicon</span> electrodeposited by <span class="hlt">Fe</span>3+ ion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mabrouk, Asma; Lorrain, N.; Haji, M. L.; Oueslati, Meherzi</p> <p>2015-01-01</p> <p>In this paper, we analyze the photoluminescence spectra (PL) of porous <span class="hlt">silicon</span> (PS) <span class="hlt">layer</span> which is elaborated by electrochemical etching and passivated by <span class="hlt">Fe</span>3+ ions (PSF) via current density, electro-deposition and temperature measurements. We observe unusual surface morphology of PSF surface and anomalous emission behavior. The PSF surface shows regular distribution of cracks, leaving isolated regions or ;platelets; of nearly uniform thickness. These cracks become more pronounced for high current densities. The temperature dependence of the PL peak energy (EPL) presents anomalous behaviors, i.e., the PL peak energy shows a successive red/blue/redshift (S-shaped behavior) with increasing temperature that we attribute to the existence of strong potential fluctuations induced by the electrochemical etching of PS <span class="hlt">layers</span>. A competition process between localized and delocalized excitons is used to discuss these PL properties. In this case, the potential confinement plays a key role on the enhancement of PL intensity in PSF. To explain the temperature dependence of the PL intensity, we have proposed a recombination model based on the tunneling and dissociation of excitons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29565117','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29565117"><span>Highly Sensitive Switchable Heterojunction Photodiode Based on Epitaxial Bi2<span class="hlt">FeCr</span>O6 Multiferroic Thin Films.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huang, Wei; Chakrabartty, Joyprokash; Harnagea, Catalin; Gedamu, Dawit; Ka, Ibrahima; Chaker, Mohamed; Rosei, Federico; Nechache, Riad</p> <p>2018-04-18</p> <p>Perovskite multiferroic oxides are promising materials for the realization of sensitive and switchable photodiodes because of their favorable band gap (<3.0 eV), high absorption coefficient, and tunable internal ferroelectric (<span class="hlt">FE</span>) polarization. A high-speed switchable photodiode based on multiferroic Bi 2 <span class="hlt">FeCr</span>O 6 (BFCO)/SrRuO 3 (SRO)-<span class="hlt">layered</span> heterojunction was fabricated by pulsed laser deposition. The heterojunction photodiode exhibits a large ideality factor ( n = ∼5.0) and a response time as fast as 68 ms, thanks to the effective charge carrier transport and collection at the BFCO/SRO interface. The diode can switch direction when the electric polarization is reversed by an external voltage pulse. The time-resolved photoluminescence decay of the device measured at ∼500 nm demonstrates an ultrafast charge transfer (lifetime = ∼6.4 ns) in BFCO/SRO heteroepitaxial structures. The estimated responsivity value at 500 nm and zero bias is 0.38 mA W -1 , which is so far the highest reported for any <span class="hlt">FE</span> thin film photodiode. Our work highlights the huge potential for using multiferroic oxides to fabricate highly sensitive and switchable photodiodes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhRvB..80j4440N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhRvB..80j4440N"><span>Model many-body Stoner Hamiltonian for binary <span class="hlt">FeCr</span> alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nguyen-Manh, D.; Dudarev, S. L.</p> <p>2009-09-01</p> <p>We derive a model tight-binding many-body d -electron Stoner Hamiltonian for <span class="hlt">FeCr</span> binary alloys and investigate the sensitivity of its mean-field solutions to the choice of hopping integrals and the Stoner exchange parameters. By applying the local charge-neutrality condition within a self-consistent treatment we show that the negative enthalpy-of-mixing anomaly characterizing the alloy in the low chromium concentration limit is due entirely to the presence of the on-site exchange Stoner terms and that the occurrence of this anomaly is not specifically related to the choice of hopping integrals describing conventional chemical bonding between atoms in the alloy. The Bain transformation pathway computed, using the proposed model Hamiltonian, for the <span class="hlt">Fe</span>15<span class="hlt">Cr</span> alloy configuration is in excellent agreement with ab initio total-energy calculations. Our investigation also shows how the parameters of a tight-binding many-body model Hamiltonian for a magnetic alloy can be derived from the comparison of its mean-field solutions with other, more accurate, mean-field approximations (e.g., density-functional calculations), hence stimulating the development of large-scale computational algorithms for modeling radiation damage effects in magnetic alloys and steels.</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://hdl.handle.net/2060/20120009444','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120009444"><span>Apparatus and method of manufacture for depositing a composite anti-reflection <span class="hlt">layer</span> on a <span class="hlt">silicon</span> surface</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pain, Bedabrata (Inventor)</p> <p>2012-01-01</p> <p>An apparatus and associated method are provided. A first <span class="hlt">silicon</span> <span class="hlt">layer</span> having at least one of an associated passivation <span class="hlt">layer</span> and barrier is included. Also included is a composite anti-reflection <span class="hlt">layer</span> including a stack of <span class="hlt">layers</span> each with a different thickness and refractive index. Such composite anti-reflection <span class="hlt">layer</span> is disposed adjacent to the first <span class="hlt">silicon</span> <span class="hlt">layer</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1376905','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1376905"><span>Nuclear Energy Advanced Modeling and Simulation (NEAMS) Accident Tolerant Fuels High Impact Problem: Coordinate Multiscale <span class="hlt">FeCr</span>Al Modeling</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>Gamble, K. A.; Hales, J. D.; Zhang, Y.</p> <p></p> <p>Since the events at the Fukushima-Daiichi nuclear power plant in March 2011 significant research has unfolded at national laboratories, universities and other institutions into alternative materials that have potential enhanced ac- cident tolerance when compared to traditional UO2 fuel zircaloy clad fuel rods. One of the potential replacement claddings are iron-chromium-alunimum (<span class="hlt">FeCr</span>Al) alloys due to their increased oxidation resistance [1–4] and higher strength [1, 2]. While the oxidation characteristics of <span class="hlt">FeCr</span>Al are a benefit for accident tolerance, the thermal neu- tron absorption cross section of <span class="hlt">FeCr</span>Al is about ten times that of Zircaloy. This neutronic penalty necessitates thinner cladding. Thismore » allows for slightly larger pellets to give the same cold gap width in the rod. However, the slight increase in pellet diameter is not sufficient to compensate for the neutronic penalty and enriching the fuel beyond the current 5% limit appears to be necessary [5]. Current estimates indicate that this neutronic penalty will impose an increase in fuel cost of 15-35% [1, 2]. In addition to the neutronic disadvantage, it is anticipated that tritium release to the coolant will be larger because the permeability of hydrogen in <span class="hlt">FeCr</span>Al is about 100 times higher than in Zircaloy [6]. Also, radiation-induced hardening and embrittlement of <span class="hlt">FeCr</span>Al need to be fully characterized experimentally [7]. Due to the aggressive development schedule for inserting some of the potential materials into lead test assemblies or rods by 2022 [8] multiscale multiphysics modeling approaches have been used to provide insight into these the use of <span class="hlt">FeCr</span>Al as a cladding material. The purpose of this letter report is to highlight the multiscale modeling effort for iron-chromium-alunimum (<span class="hlt">FeCr</span>Al) cladding alloys as part of the Nuclear Energy Advanced Modeling and Simulation (NEAMS) program through its Accident Tolerant Fuel (ATF) High Impact Problem (HIP). The approach taken throughout the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1287032','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1287032"><span>Status Report on Irradiation Capsules Designed to Evaluate <span class="hlt">FeCr</span>Al-UO 2 Interactions</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>Field, Kevin G.; Howard, Richard H.</p> <p></p> <p>This status report provides the background and current status of a series of irradiation capsules that were designed and are being built to test the interactions between candidate <span class="hlt">FeCr</span>Al cladding for enhanced accident tolerant applications and prototypical enriched commercial UO 2 fuel in a neutron radiation environment. These capsules will test the degree, if any, of fuel cladding chemical interactions (FCCI) between <span class="hlt">FeCr</span>Al and UO 2. The capsules are to be irradiated in the Advanced Test Reactor (ATR) at Idaho National Laboratory to burn-ups of 10, 30, and 50 GWd/MT with a nominal target temperature at the interfaces between themore » pellets and clad of 350°C.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017RuMet2017..397T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017RuMet2017..397T"><span>Primary radiation damage of an <span class="hlt">FeCr</span> alloy under pressure: Atomistic simulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tikhonchev, M. Yu.; Svetukhin, V. V.</p> <p>2017-05-01</p> <p>The primary radiation damage of a binary <span class="hlt">FeCr</span> alloy deformed by applied mechanical loading is studied by an atomistic molecular dynamics simulation. Loading is simulated by specifying an applied pressure of 0.25, 1.0, and 2.5 GPa of both signs. Hydrostatic and uniaxial loading is considered along the [001], [111], [112], and [210] directions. The influence of loading on the energy of point defect formation and the threshold atomic displacement energy in single-component bcc iron is investigated. The 10-keV atomic displacement cascades in a "random" binary <span class="hlt">Fe</span>-9 at % <span class="hlt">Cr</span> alloy are simulated at an initial temperature of 300 K. The number of the point defects generated in a cascade is estimated, and the clustering of point defects and the spatial orientation of interstitial configurations are analyzed. Our results agree with the results of other researchers and supplement them.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JNuM..501..208C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JNuM..501..208C"><span>Helium accumulation and bubble formation in <span class="hlt">FeCoNiCr</span> alloy under high fluence He+ implantation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Da; Tong, Y.; Li, H.; Wang, J.; Zhao, Y. L.; Hu, Alice; Kai, J. J.</p> <p>2018-04-01</p> <p>Face-centered cubic (FCC) high-entropy alloys (HEA), as emerging alloys with equal-molar or near equal-molar constituents, show a promising radiation damage resistance under heavy ion bombardment, making them potential for structural material application in next-generation nuclear reactors, but the accumulation of light helium ions, a product of nuclear fission reaction, has not been studied. The present work experimentally studied the helium accumulation and bubble formation at implantation temperatures of 523 K, 573 K and 673 K in a homogenized FCC <span class="hlt">FeCoNiCr</span> HEA, a HEA showing excellent radiation damage resistance under heavy ion irradiation. The size and population density of helium bubbles in <span class="hlt">FeCoNiCr</span> samples were quantitatively analyzed through transmission electron microscopy (TEM), and the helium content existing in bubbles were estimated from a high-pressure Equation of State (EOS). We found that the helium diffusion in such condition was dominated by the self-interstitial/He replacement mechanism, and the corresponding activation energy in <span class="hlt">FeCoNiCr</span> is comparable with the vacancy migration energy in Ni and austenitic stainless steel but only 14.3%, 31.4% and 51.4% of the accumulated helium precipitated into helium bubbles at 523 K, 573 K and 673 K, respectively, smaller than the pure Ni case. Importantly, the small bubble size suggested that <span class="hlt">FeCoNiCr</span> HEA has a high resistance of helium bubble formation compared with Ni and steels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JOM....70b.176R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JOM....70b.176R"><span>Versatile Oxide Films Protect <span class="hlt">FeCr</span>Al Alloys Under Normal Operation and Accident Conditions in Light Water Power Reactors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rebak, Raul B.</p> <p>2018-02-01</p> <p>The US has currently a fleet of 99 nuclear power light water reactors which generate approximately 20% of the electricity consumed in the country. Near 90% of the reactors are at least 30 years old. There are incentives to make the existing reactors safer by using accident tolerant fuels (ATF). Compared to the standard UO2-zirconium-based system, ATF need to tolerate loss of active cooling in the core for a considerably longer time while maintaining or improving the fuel performance during normal operation conditions. Ferritic iron-chromium-aluminum (<span class="hlt">FeCr</span>Al) alloys have been identified as an alternative to replace current zirconium alloys. They contain <span class="hlt">Fe</span> (base) + 10-22 <span class="hlt">Cr</span> + 4-6 Al and may contain smaller amounts of other elements such as molybdenum and traces of others. <span class="hlt">FeCr</span>Al alloys offer outstanding resistance to attack by superheated steam by developing an alumina oxide on the surface in case of a loss of coolant accident like at Fukushima. <span class="hlt">FeCr</span>Al alloys also perform well under normal operation conditions both in boiling water reactors and pressurized water reactors because they are protected by a thin oxide rich in chromium. Under normal operation condition, the key element is <span class="hlt">Cr</span> and under accident conditions it is Al.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MMTB...49..581W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MMTB...49..581W"><span>Estimation of the Temperature-Dependent Nitrogen Solubility in Stainless <span class="hlt">Fe-Cr</span>-Mn-Ni-Si-C Steel Melts During Processing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wendler, Marco; Hauser, Michael; Sandig, Eckhard Frank; Volkova, Olena</p> <p>2018-04-01</p> <p>The influence of chemical composition, temperature, and pressure on the nitrogen solubility of various high alloy stainless steel grades, namely <span class="hlt">Fe</span>-14<span class="hlt">Cr</span>-(0.17-7.77)Mn-6Ni-0.5Si-0.03C [wt pct], <span class="hlt">Fe</span>-15<span class="hlt">Cr</span>-3Mn-4Ni-0.5Si-0.1C [wt pct], and <span class="hlt">Fe</span>-19<span class="hlt">Cr</span>-3Mn-4Ni-0.5Si-0.15C [wt pct], was studied in the melt. The temperature-dependent N-solubility was determined using an empirical approach proposed by Wada and Pehlke. The thus calculated N-concentrations overestimate the actual N-solubility of all the studied <span class="hlt">Fe-Cr</span>-Mn-Ni-Si-C steel melts at a given temperature and pressure. Consequently, the calculation model has to be modified by Si and C because both elements are not recognized in the original equation. The addition of the 1st and 2nd order interaction parameters for Si and C to the model by Wada and Pehlke allows a precise estimation of the temperature-dependent nitrogen solubility in the liquid steel bath, and fits very well with the measured nitrogen concentrations during processing of the steels. Moreover, the N-solubility enhancing effect of <span class="hlt">Cr</span>- and Mn-additions has been demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1341611','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1341611"><span>Interrogating the superconductor Ca- 10(Pt 4As 8)(<span class="hlt">Fe</span> 2-xPt xAs 2) 5 <span class="hlt">Layer-by-layer</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>Kim, Jisun; Zhu, Yimei; Nam, Hyoungdo</p> <p>2016-10-14</p> <p>Ever since the discovery of high-Tc superconductivity in <span class="hlt">layered</span> cuprates, the roles that individual <span class="hlt">layers</span> play have been debated, due to difficulty in <span class="hlt">layer-by-layer</span> characterization. While there is similar challenge in many <span class="hlt">Fe</span>-based <span class="hlt">layered</span> superconductors, the newly-discovered Ca 10(Pt 4As 8)(<span class="hlt">Fe</span> 2As 2) 5 provides opportunities to explore superconductivity <span class="hlt">layer</span> by <span class="hlt">layer</span>, because it contains both superconducting building blocks (<span class="hlt">Fe</span> 2As 2 <span class="hlt">layers</span>) and intermediate Pt 4As 8 <span class="hlt">layers</span>. Cleaving a single crystal under ultra-high vacuum results in multiple terminations: an ordered Pt 4As 8 <span class="hlt">layer</span>, two reconstructed Ca <span class="hlt">layers</span> on the top of a Pt 4As 8 <span class="hlt">layer</span>, andmore » disordered Ca <span class="hlt">layer</span> on the top of <span class="hlt">Fe</span> 2As 2 <span class="hlt">layer</span>. The electronic properties of individual <span class="hlt">layers</span> are studied using scanning tunneling microscopy/spectroscopy (STM/S), which reveals different spectra for each surface. Remarkably superconducting coherence peaks are seen only on the ordered Ca/Pt 4As 8 <span class="hlt">layer</span>. Our results indicate that an ordered structure with proper charge balance is required in order to preserve superconductivity.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27505358','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27505358"><span>Rapid fabrication of a <span class="hlt">silicon</span> modification <span class="hlt">layer</span> on <span class="hlt">silicon</span> carbide substrate.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bai, Yang; Li, Longxiang; Xue, Donglin; Zhang, Xuejun</p> <p>2016-08-01</p> <p>We develop a kind of magnetorheological (MR) polishing fluid for the fabrication of a <span class="hlt">silicon</span> modification <span class="hlt">layer</span> on a <span class="hlt">silicon</span> carbide substrate based on chemical theory and actual polishing requirements. The effect of abrasive concentration in MR polishing fluid on material removal rate and removal function shape is investigated. We conclude that material removal rate will increase and tends to peak value as the abrasive concentration increases to 0.3 vol. %, and the removal function profile will become steep, which is a disadvantage to surface frequency error removal at the same time. The removal function stability is also studied and the results show that the prepared MR polishing fluid can satisfy actual fabrication requirements. An aspheric reflective mirror of <span class="hlt">silicon</span> carbide modified by <span class="hlt">silicon</span> is well polished by combining magnetorheological finishing (MRF) using two types of MR polishing fluid and computer controlled optical surfacing (CCOS) processes. The surface accuracy root mean square (RMS) is improved from 0.087λ(λ=632.8  nm) initially to 0.020λ(λ=632.8  nm) in 5.5 h total and the tool marks resulting from MRF are negligible. The PSD analysis results also shows that the final surface is uniformly polished.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JAP...107iA716M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JAP...107iA716M"><span>Characterization of Cu buffer <span class="hlt">layers</span> for growth of L10-<span class="hlt">Fe</span>Ni thin films</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mizuguchi, M.; Sekiya, S.; Takanashi, K.</p> <p>2010-05-01</p> <p>A Cu(001) <span class="hlt">layer</span> was fabricated on a Au(001) <span class="hlt">layer</span> to investigate the use of Cu as a buffer <span class="hlt">layer</span> for growing L10-<span class="hlt">Fe</span>Ni thin films. The epitaxial growth of a Cu buffer <span class="hlt">layer</span> was observed using reflection high-energy electron diffraction. The flatness of the <span class="hlt">layer</span> improved drastically with an increase in the substrate temperature although the <span class="hlt">layer</span> was an alloy (AuCu3). An <span class="hlt">Fe</span>Ni thin film was epitaxially grown on the AuCu3 buffer <span class="hlt">layer</span> by alternate monatomic <span class="hlt">layer</span> deposition and the formation of an L10-<span class="hlt">Fe</span>Ni ordered alloy was expected. The AuCu3 buffer <span class="hlt">layer</span> is thus a promising candidate material for the growth of L10-<span class="hlt">Fe</span>Ni thin films.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5503316','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5503316"><span>Integration of Electrodeposited Ni-<span class="hlt">Fe</span> in MEMS with Low-Temperature Deposition and Etch 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>Schiavone, Giuseppe; Murray, Jeremy; Perry, Richard; Mount, Andrew R.; Desmulliez, Marc P. Y.; Walton, Anthony J.</p> <p>2017-01-01</p> <p>This article presents a set of low-temperature deposition and etching processes for the integration of electrochemically deposited Ni-<span class="hlt">Fe</span> alloys in complex magnetic microelectromechanical systems, as Ni-<span class="hlt">Fe</span> is known to suffer from detrimental stress development when subjected to excessive thermal loads. A selective etch process is reported which enables the copper seed <span class="hlt">layer</span> used for electrodeposition to be removed while preserving the integrity of Ni-<span class="hlt">Fe</span>. In addition, a low temperature deposition and surface micromachining process is presented in which <span class="hlt">silicon</span> dioxide and <span class="hlt">silicon</span> nitride are used, respectively, as sacrificial material and structural dielectric. The sacrificial <span class="hlt">layer</span> can be patterned and removed by wet buffered oxide etch or vapour HF etching. The reported methods limit the thermal budget and minimise the stress development in Ni-<span class="hlt">Fe</span>. This combination of techniques represents an advance towards the reliable integration of Ni-<span class="hlt">Fe</span> components in complex surface micromachined magnetic MEMS. PMID:28772683</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22402910-role-non-magnetic-material-spin-pumping-magnetization-dynamics-nife-cofeb-multilayer-systems','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22402910-role-non-magnetic-material-spin-pumping-magnetization-dynamics-nife-cofeb-multilayer-systems"><span>The role of the non-magnetic material in spin pumping and magnetization dynamics in Ni<span class="hlt">Fe</span> and Co<span class="hlt">Fe</span>B multilayer systems</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>Ruiz-Calaforra, A., E-mail: ruiz@physik.uni-kl.de; Brächer, T.; Lauer, V.</p> <p>2015-04-28</p> <p>We present a study of the effective magnetization M{sub eff} and the effective damping parameter α{sub eff} by means of ferromagnetic resonance spectroscopy on the ferromagnetic (FM) materials Ni{sub 81}<span class="hlt">Fe</span>{sub 19} (Ni<span class="hlt">Fe</span>) and Co{sub 40}<span class="hlt">Fe</span>{sub 40}B{sub 20} (Co<span class="hlt">Fe</span>B) in FM/Pt, FM/NM, and FM/NM/Pt systems with the non-magnetic (NM) materials Ru, <span class="hlt">Cr</span>, Al, and MgO. Moreover, for Ni<span class="hlt">Fe</span> <span class="hlt">layer</span> systems, the influence of interface effects is studied by way of thickness dependent measurements of M{sub eff} and α{sub eff}. Additionally, spin pumping in Ni<span class="hlt">Fe</span>/NM/Pt is investigated by means of inverse spin Hall effect (ISHE) measurements. We observe a large dependence ofmore » M{sub eff} and α{sub eff} of the Ni<span class="hlt">Fe</span> films on the adjacent NM <span class="hlt">layer</span>. While <span class="hlt">Cr</span> and Al do not induce a large change in the magnetic properties, Ru, Pt, and MgO affect M{sub eff} and α{sub eff} in different degrees. In particular, Ni<span class="hlt">Fe</span>/Ru and Ni<span class="hlt">Fe</span>/Ru/Pt systems show a large perpendicular surface anisotropy and a significant enhancement of the damping. In contrast, the magnetic properties of Co<span class="hlt">Fe</span>B films do not have a large influence of the NM adjacent material and only Co<span class="hlt">Fe</span>B/Pt systems present an enhancement of α{sub eff}. However, this enhancement is much more pronounced in Ni<span class="hlt">Fe</span>/Pt. By the introduction of the NM spacer material, this enhancement is reduced. Furthermore, a difference in symmetry between Ni<span class="hlt">Fe</span>/NM/Pt and Ni<span class="hlt">Fe</span>/NM systems in the output voltage signal from the ISHE measurements reveals the presence of spin pumping into the Pt <span class="hlt">layer</span> in all-metallic Ni<span class="hlt">Fe</span>/NM/Pt and Ni<span class="hlt">Fe</span>/Pt systems.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97p5105Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97p5105Z"><span>Tuning the magnetism of the top-<span class="hlt">layer</span> <span class="hlt">Fe</span>As on Ba<span class="hlt">Fe</span>2As2 (001): First-principles study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Bing-Jing; Liu, Kai; Lu, Zhong-Yi</p> <p>2018-04-01</p> <p>Magnetism may play an important role in inducing the superconductivity in iron-based superconductors. As a prototypical system, the surface of Ba<span class="hlt">Fe</span>2As2 provides a good platform for studying related magnetic properties. We have designed systematic first-principles calculations to clarify the surface magnetism of Ba<span class="hlt">Fe</span>2As2 (001), which previously has received little attention in comparison with surface structures and electronic states. We find that the surface environment has an important influence on the magnetic properties of the top-<span class="hlt">layer</span> <span class="hlt">Fe</span>As. For As-terminated surfaces, the magnetic ground state of the top-<span class="hlt">layer</span> <span class="hlt">Fe</span>As is in the staggered dimer antiferromagnetic (AFM) order, distinct from that of the bulk, while for Ba-terminated surfaces the collinear (single-stripe) AFM order is the most stable, the same as that in the bulk. When a certain coverage of Ba or K atoms is deposited onto the As-terminated surface, the calculated energy differences among different AFM orders for the top-<span class="hlt">layer</span> <span class="hlt">Fe</span>As on Ba<span class="hlt">Fe</span>2As2 (001) can be much reduced, indicating enhanced spin fluctuations. To compare our results with available scanning tunneling microscopy (STM) measurements, we have simulated the STM images of several structural/magnetic terminations. Astonishingly, when the top-<span class="hlt">layer</span> <span class="hlt">Fe</span>As is in the staggered dimer AFM order, a stripe pattern appears in the simulated STM image even when the surface Ba atoms adopt a √{2 }×√{2 } structure, while a √{2 }×√{2 } square pattern comes out for the 1 ×1 full As termination. Our results suggest: (i) the magnetic state at the Ba<span class="hlt">Fe</span>2As2 (001) surface can be quite different from that in the bulk; (ii) the magnetic properties of the top-<span class="hlt">layer</span> <span class="hlt">Fe</span>As can be tuned effectively by surface doping, which may likely induce superconductivity at the surface <span class="hlt">layer</span>; (iii) both the surface termination and the AFM order in the top-<span class="hlt">layer</span> <span class="hlt">Fe</span>As can affect the STM image of Ba<span class="hlt">Fe</span>2As2 (001), which needs to be taken into account when identifying the surface</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5853709','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5853709"><span>Heavily Boron-Doped <span class="hlt">Silicon</span> <span class="hlt">Layer</span> for the Fabrication of Nanoscale Thermoelectric Devices</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Liu, Yang; Deng, Lingxiao; Zhang, Mingliang; Zhang, Shuyuan; Ma, Jing; Song, Peishuai; Liu, Qing; Ji, An; Yang, Fuhua; Wang, Xiaodong</p> <p>2018-01-01</p> <p>Heavily boron-doped <span class="hlt">silicon</span> <span class="hlt">layers</span> and boron etch-stop techniques have been widely used in the fabrication of microelectromechanical systems (MEMS). This paper provides an introduction to the fabrication process of nanoscale <span class="hlt">silicon</span> thermoelectric devices. Low-dimensional structures such as <span class="hlt">silicon</span> nanowire (SiNW) have been considered as a promising alternative for thermoelectric applications in order to achieve a higher thermoelectric figure of merit (ZT) than bulk <span class="hlt">silicon</span>. Here, heavily boron-doped <span class="hlt">silicon</span> <span class="hlt">layers</span> and boron etch-stop processes for the fabrication of suspended SiNWs will be discussed in detail, including boron diffusion, electron beam lithography, inductively coupled plasma (ICP) etching and tetramethylammonium hydroxide (TMAH) etch-stop processes. A 7 μm long nanowire structure with a height of 280 nm and a width of 55 nm was achieved, indicating that the proposed technique is useful for nanoscale fabrication. Furthermore, a SiNW thermoelectric device has also been demonstrated, and its performance shows an obvious reduction in thermal conductivity. PMID:29385759</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..343a2037S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..343a2037S"><span>The observation of resistivity change on the ultrasonic treated <span class="hlt">Fe-Cr</span> ODS sinter alloy under magnetic field influence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Silalahi, Marzuki; Purwanto, Setyo; Mujamilah; Dimyati, Arbi</p> <p>2018-03-01</p> <p>About the observation of resistivity change on the ultrasonic treated <span class="hlt">Fe-Cr</span> ODS sinter alloy under magnetic field influence. This paper reported about the observation of the resistivity change in the ultrasonic pre-treated <span class="hlt">Fe-Cr</span> ODS sinter alloy under the influence of magnetic field at the Center for Science and Technology of Advanced Material, Nuclear Energy Agency of Indonesia. <span class="hlt">Fe-Cr</span> ODS alloy were sinthesized by vacuum sintering of <span class="hlt">Fe</span>- and <span class="hlt">Cr</span>-powder dispersed Y2O3. However, before sintering the powder mixture was subjected to the irradiation process by ultrasonic for 50 hours at 20 kHz and then isostatic pressed up to 50.91 MPa to form a coin of 10 mm in diameter. LCR meassurement revealed the decreasing of resistivity about 3 times by increasing of applied magnetic field from 0 to 70 mT. In addition, VSM meassurement was performed on both as powder material and as sintered sample. The results showed increasing the magnetization with increasing magnetic field and the curve exhibits almost exact symmetry S-form with small hysterese indicating fast changing magnetization and demagnetization capability without energy loss. This opens strong speculations about the existence of magnetoresistant property of the material which is important for many application in field of sensors or electro magnetic valves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17697697','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17697697"><span>Hydroponic phytoremediation of Cd, <span class="hlt">Cr</span>, Ni, As, and <span class="hlt">Fe</span>: can Helianthus annuus hyperaccumulate multiple heavy metals?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>January, Mary C; Cutright, Teresa J; Van Keulen, Harry; Wei, Robert</p> <p>2008-01-01</p> <p>Sundance sunflowers were subjected to contaminated solutions containing 3, 4, or 5 heavy metals, with and without EDTA. The sunflowers exhibited a metal uptake preference of Cd=<span class="hlt">Cr</span>>Ni, <span class="hlt">Cr</span>>Cd>Ni>As and <span class="hlt">Fe>As>Cd>Ni>Cr</span> without EDTA and <span class="hlt">Cr</span>>Cd>Ni, <span class="hlt">Fe>As>Cd>Cr</span>>Ni with EDTA. As uptake was not affected by other metals, but it decreased Cd and Ni concentration in the stems. The presence of <span class="hlt">Fe</span> improved the translocation of the other metals regardless of whether EDTA was present. In general, EDTA served as a hindrance to metal uptake. For the experiment with all five heavy metals, EDTA decreased Cd in the roots and stems from 2.11 to 1.36 and from 2.83 to 2.3 2mg g(-1) biomass, respectively. For the same conditions, Ni in the stems decreased from 1.98 to 0.94 mg g(-1) total metal uptake decreased from 14.95 mg to 13.89 mg, and total biomass decreased from 2.38 g to 1.99 g. These results showed an overall negative effect in addition of EDTA. However it is unknown whether the negative effect was due to toxicity posed by EDTA or the breaking of phytochelatin-metal bonds. The most important finding was the ability of Sundance sunflowers to achieve hyperaccumulator status for both As and Cd under all conditions studied. Ni hyperaccumulator status was only achieved in the presence of three metals without EDTA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPCS..110..152Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPCS..110..152Z"><span>Effects of the addition of Co, Ni or <span class="hlt">Cr</span> on the decolorization properties of <span class="hlt">Fe</span>-Si-B amorphous alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Changqin; Zhu, Zhengwang; Zhang, Haifeng</p> <p>2017-11-01</p> <p><span class="hlt">Fe</span>-based amorphous alloys show great potential in degrading azo dyes and other organic pollutants, and are widely investigated as a kind of environmental-friendly materials for wastewater remediation. In this paper, the effects of Co, Ni or <span class="hlt">Cr</span> addition on the decolorization properties of <span class="hlt">Fe</span>-Si-B amorphous alloys were studied, and the mechanism of their different effects was analyzed. Co addition could lower the activation energy of <span class="hlt">Fe</span>-Si-B amorphous alloys in decolorizing azo dyes, and had no weakening effect on the decolorization capability of <span class="hlt">Fe</span>-Si-B amorphous alloys. Ni addition led to partial crystallization of <span class="hlt">Fe</span>-Si-B amorphous alloys, and the decolorization mechanism at low temperatures changed from chemical degradation to physical adsorption. <span class="hlt">Cr</span> addition could enhance the corrosion resistance of <span class="hlt">Fe</span>-Si-B amorphous alloys, but the amorphous alloys completely lost the decolorization capability no matter at lower or higher temperatures. The results of X-ray photoelectron spectroscopy (XPS) and scanning electron microscopy (SEM) indicated that the addition of Co, Ni or <span class="hlt">Cr</span> could generate different surface structures that had significant influences on the decolorization process. Our work demonstrated that the effiecient decolorization of azo dyes by <span class="hlt">Fe</span>-based alloys could be realized only when amorphous nature and incompact surface structure were simultaneously achieved for the alloys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016OptLT..84...23Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016OptLT..84...23Z"><span>Laser surface alloying of <span class="hlt">FeCoCr</span>AlNi high-entropy alloy on 304 stainless steel to enhance corrosion and cavitation erosion resistance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, S.; Wu, C. L.; Zhang, C. H.; Guan, M.; Tan, J. Z.</p> <p>2016-10-01</p> <p><span class="hlt">FeCoCr</span>AlNi high-entropy alloy coating was synthesized with premixed high-purity Co, <span class="hlt">Cr</span>, Al and Ni powders on 304 stainless steel by laser surface alloying, aiming at improving corrosion and cavitation erosion resistance. Phase constituents, microstructure and microhardness were investigated using XRD, SEM, and microhardness tester, respectively. The cavitation erosion and electrochemical corrosion behavior of <span class="hlt">FeCoCr</span>AlNi coating in 3.5% NaCl solution were also evaluated using an ultrasonic vibrator and potentiodynamic polarization measurement. Experimental results showed that with appropriate laser processing parameters, <span class="hlt">FeCoCr</span>AlNi coating with good metallurgical bonding to the substrate could be achieved. <span class="hlt">FeCoCr</span>AlNi coating was composed of a single BCC solid solution. The formation of simple solid solutions in HEAs was the combined effect of mixing entropy (ΔSmix), mixing enthalpy (ΔHmix), atom-size difference (δ) and valence electron concentration (VEC), and the effect of ΔSmix was much larger than that of the other factors. The microhardness of the <span class="hlt">FeCoCr</span>AlNi coating was ~3 times that of the 304 stainless steel. Both the corrosion and cavitation erosion resistance of the coating were improved. The cavitation erosion resistance for <span class="hlt">FeCoCr</span>AlNi HEA coating was ~7.6 times that of 304 stainless steel. The corrosion resistance was also improved as reflected by a reduction in the current density of one order of magnitude as compared with 304 stainless steel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.4328P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.4328P"><span>High-pressure behaviour of <span class="hlt">Cr-Fe</span>-Mg-Al spinels: applications to diamond geobarometry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Periotto, Benedetta; Bruschini, Enrico; Nestola, Fabrizio; Lenaz, Davide; Princivalle, Francesco; Andreozzi, Giovanni B.; Bosi, Ferdinando</p> <p>2014-05-01</p> <p>Spinels belonging to the chromite - magnesiochromite - hercynite (<span class="hlt">FeCr</span>2O4-Mg<span class="hlt">Cr</span>2O4-<span class="hlt">Fe</span>Al2O4) system are among the most common inclusions found in diamonds (Stachel and Harris 2008). In particular, although <span class="hlt">FeCr</span>2O4 and Mg<span class="hlt">Cr</span>2O4 components sum to between 85 and 88% of spinels found in diamonds, hercynite <span class="hlt">Fe</span>Al2O4 plays a not negligible role in determining their thermo-elastic properties with concentrations reaching 7-9 % (other minor end-members like MgAl2O4, Mg<span class="hlt">Fe</span>2O4 and <span class="hlt">Fe</span>2O3 rarely reach 2-3% in total, see Lenaz et al. 2009). Recent studies were focused on the determination of the diamond formation pressure by the so-called "elastic method" (see for example Nestola et al. 2011 and references therein). It was demonstrated that accurate and precise thermo-elastic parameters are fundamental to minimize the uncertainty of formation pressure. In this work we have determined the equations of state at room temperature of three synthetic spinel end-members chromite - magnesiochromite - hercynite and one natural spinel crystal extracted from a diamond (from Udachnaya mine, Siberia, Russia) by single-crystal X-ray diffraction in situ at high-pressure. A diamond-anvil cell was mounted on a STADI IV diffractometer equipped with a point detector and motorized by SINGLE software (Angel and Finger 2011). The natural crystal was investigated to test (and possibly validate) the "empirical prediction model", capable to provide bulk modulus and its first pressure derivative only knowing the composition of the spinels found in diamonds. Such prediction model could be used to obtain pressure of formation for the diamond-spinel pair through the elastic method. Details and results will be discussed. The research was funded by the ERC Starting Grant to FN (grant agreement n° 307322). References Angel R.J., Finger L.W. (2011) SINGLE A program to control single-crystal diffractometers. Journal of Applied Crystallography, 44, 247-251. Lenaz D., Logvinova A.M., Princivalle F., Sobolev N. (2009</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAP...122k5101B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAP...122k5101B"><span>Triclinic-monoclinic-orthorhombic (T-M-O) structural transitions in phase diagram of <span class="hlt">Fe</span>VO4-<span class="hlt">Cr</span>VO4 solid solutions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bera, Ganesh; Reddy, V. R.; Rambabu, P.; Mal, P.; Das, Pradip; Mohapatra, N.; Padmaja, G.; Turpu, G. R.</p> <p>2017-09-01</p> <p>Phase diagram of <span class="hlt">Fe</span>VO4-<span class="hlt">Cr</span>VO4 solid solutions pertinent with structural and magnetic phases is presented with unambiguous experimental evidences. Solid solutions <span class="hlt">Fe</span>1-xCrxVO4 (0 ≤ x ≤ 1.0) were synthesized through the standard solid state route and studied by X-ray diffraction, scanning electron microscopy, energy dispersive spectra of X-rays, Raman spectroscopy, d.c. magnetization, and 57<span class="hlt">Fe</span> Mössbauer spectroscopic studies. <span class="hlt">Fe</span>VO4 and <span class="hlt">Cr</span>VO4 were found to be in triclinic (P-1 space group) and orthorhombic structures (Cmcm space group), respectively. <span class="hlt">Cr</span> incorporation into the <span class="hlt">Fe</span>VO4 lattice leads to the emergence of a new monoclinic phase dissimilar to the both end members of the solid solutions. In <span class="hlt">Fe</span>1-xCrxVO4 up to x = 0.10, no discernible changes in the triclinic structure were found. A new structural monoclinic phase (C2/m space group) emerges within the triclinic phase at x = 0.125, and with the increase in <span class="hlt">Cr</span> content, it gets stabilized with clear single phase signatures in the range of x = 0.175-0.25 as evidenced by the Rietveld analysis of the structures. Beyond x = 0.33, orthorhombic phase similar to <span class="hlt">Cr</span>VO4 (Cmcm space group) emerges and coexists with a monoclinic structure up to x = 0.85, which finally tends to stabilize in the range of x = 0.90-1.00. The Raman spectroscopic studies also confirm the structural transition. <span class="hlt">Fe</span>VO4 Raman spectra show the modes related to three nonequivalent V ions in the triclinic structure, where up to 42 Raman modes are observed in the present study. With the stabilization of structures having higher symmetry, the number of Raman modes decreases and the modes related to symmetry inequivalent sites collate into singular modes from the doublet structure. A systematic crossover from two magnetic transitions in <span class="hlt">Fe</span>VO4, at 21.5 K and 15.4 K to single magnetic transition in <span class="hlt">Cr</span>VO4, at 71 K (antiferromagnetic transition), is observed in magnetization studies. The intermediate solid solution with x = 0.15 shows two magnetic transitions</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/29170544','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29170544"><span>Structural, electronic, magnetic, half-metallic, mechanical, and thermodynamic properties of the quaternary Heusler compound <span class="hlt">FeCr</span>RuSi: A first-principles study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Xiaotian; Khachai, Houari; Khenata, Rabah; Yuan, Hongkuan; Wang, Liying; Wang, Wenhong; Bouhemadou, Abdelmadjid; Hao, Liyu; Dai, Xuefang; Guo, Ruikang; Liu, Guodong; Cheng, Zhenxiang</p> <p>2017-11-23</p> <p>In this paper, we have investigated the structural, electronic, magnetic, half-metallic, mechanical, and thermodynamic properties of the equiatomic quaternary Heusler (EQH) compound <span class="hlt">FeCr</span>RuSi using the density functional theory (DFT) and the quasi-harmonic Debye model. Our results reveal that <span class="hlt">FeCr</span>RuSi is a half-metallic material (HMM) with a total magnetic moment of 2.0 μ B in agreement with the well-known Slater-Pauling rule M t  = Z t  - 24. Furthermore, the origin of the half-metallic band gap in <span class="hlt">FeCr</span>RuSi is well studied through a schematic diagram of the possible d-d hybridization between <span class="hlt">Fe</span>, <span class="hlt">Cr</span> and Ru elements. The half-metallic behavior of <span class="hlt">FeCr</span>RuSi can be maintained in a relatively wide range of variations of the lattice constant (5.5-5.8 Å) under uniform strain and the c/a ratio (0.96-1.05) under tetragonal distortion. The calculated phonon dispersion, cohesive and formation energies, and mechanical properties reveal that <span class="hlt">FeCr</span>RuSi is stable with an EQH structure. Importantly, the compound of interest has been prepared and is found to exist in an EQH type structure with the presence of some B2 disorder. Moreover, the thermodynamic properties, such as the thermal expansion coefficient α, the heat capacity C V , the Grüneisen constant γ, and the Debye temperature Θ D are calculated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014MMI....20..701H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014MMI....20..701H"><span>Microstructural evolution with various Ti contents in <span class="hlt">Fe</span>-based hardfacing alloys using a GTAW technique</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hsieh, Chih-Chun; Liu, Yi-Chia; Wang, Jia-Siang; Wu, Weite</p> <p>2014-07-01</p> <p>The aim of this study is to discuss the effect of microstructural development with different Ti contents in <span class="hlt">Fe</span>-based hardfacing alloys. A series of <span class="hlt">Fe-Cr</span>-C-Si-Mn-xTi alloy fillers was deposited on SS400 low carbon steel substrate using oscillating gas tungsten arc welding. The microstructure in the <span class="hlt">Fe</span>-based hardfacing alloy without Ti content addition included: the primary γ, eutectic γ+(<span class="hlt">Fe,Cr</span>)3C, eutectic γ+(<span class="hlt">Fe,Cr</span>)2C and martensite. With increasing Ti contents, the microstructures showed the primary TiC carbide, γ phase and eutectic γ+(<span class="hlt">Fe,Cr</span>,Ti)3C. The amount and size of TiC carbide in the hardfacing <span class="hlt">layers</span> increased as the Ti content increased. However, the eutectic γ+(<span class="hlt">Fe,Cr</span>,Ti)3C content decreased as the Ti content increased. According to the results of the hardness test, the lowest hardness value (HRC 54.93) was found with 0% wt% Ti and the highest hardness (HRC 60.29) was observed with 4.87 wt% Ti.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017TePhL..43..909M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017TePhL..43..909M"><span>Precision calibration of the <span class="hlt">silicon</span> doping level in gallium arsenide epitaxial <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mokhov, D. V.; Berezovskaya, T. N.; Kuzmenkov, A. G.; Maleev, N. A.; Timoshnev, S. N.; Ustinov, V. M.</p> <p>2017-10-01</p> <p>An approach to precision calibration of the <span class="hlt">silicon</span> doping level in gallium arsenide epitaxial <span class="hlt">layers</span> is discussed that is based on studying the dependence of the carrier density in the test GaAs <span class="hlt">layer</span> on the <span class="hlt">silicon</span>- source temperature using the Hall-effect and CV profiling techniques. The parameters are measured by standard or certified measuring techniques and approved measuring instruments. It is demonstrated that the use of CV profiling for controlling the carrier density in the test GaAs <span class="hlt">layer</span> at the thorough optimization of the measuring procedure ensures the highest accuracy and reliability of doping level calibration in the epitaxial <span class="hlt">layers</span> with a relative error of no larger than 2.5%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29038543','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29038543"><span>Advanced <span class="hlt">Silicon</span>-on-Insulator: Crystalline <span class="hlt">Silicon</span> on Atomic <span class="hlt">Layer</span> Deposited Beryllium Oxide.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Min Lee, Seung; Hwan Yum, Jung; Larsen, Eric S; Chul Lee, Woo; Keun Kim, Seong; Bielawski, Christopher W; Oh, Jungwoo</p> <p>2017-10-16</p> <p><span class="hlt">Silicon</span>-on-insulator (SOI) technology improves the performance of devices by reducing parasitic capacitance. Devices based on SOI or <span class="hlt">silicon</span>-on-sapphire technology are primarily used in high-performance radio frequency (RF) and radiation sensitive applications as well as for reducing the short channel effects in microelectronic devices. Despite their advantages, the high substrate cost and overheating problems associated with complexities in substrate fabrication as well as the low thermal conductivity of <span class="hlt">silicon</span> oxide prevent broad applications of this technology. To overcome these challenges, we describe a new approach of using beryllium oxide (BeO). The use of atomic <span class="hlt">layer</span> deposition (ALD) for producing this material results in lowering the SOI wafer production cost. Furthermore, the use of BeO exhibiting a high thermal conductivity might minimize the self-heating issues. We show that crystalline Si can be grown on ALD BeO and the resultant devices exhibit potential for use in advanced SOI technology applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/5845114','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/5845114"><span>Amorphous surface <span class="hlt">layers</span> in Ti-implanted <span class="hlt">Fe</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>Knapp, J.A.; Follstaedt, D.M.; Picraux, S.T.</p> <p>1979-01-01</p> <p>Implanting Ti into high-purity <span class="hlt">Fe</span> results in an amorphous surface <span class="hlt">layer</span> which is composed of not only <span class="hlt">Fe</span> and Ti, but also C. Implantations were carried out at room temperature over the energy range 90 to 190 keV and fluence range 1 to 2 x 10/sup 16/ at/cm/sup 2/. The Ti-implanted <span class="hlt">Fe</span> system has been characterized using transmission electron microscopy (TEM), ion backscattering and channeling analysis, and (d,p) nuclear reaction analysis. The amorphous <span class="hlt">layer</span> was observed to form at the surface and grow inward with increasing Ti fluence. For an implant of 1 x 10/sup 17/ Ti/cm/sup 2/ at 180more » keV the <span class="hlt">layer</span> thickness was 150 A, while the measured range of the implanted Ti was approx. 550 A. This difference is due to the incorporation of C into the amorphous alloy by C being deposited on the surface during implantation and subsequently diffusing into the solid. Our results indicate that C is an essential constituent of the amorphous phase for Ti concentrations less than or equal to 10 at. %. For the 1 x 10/sup 17/ Ti/cm/sup 2/ implant, the concentration of C in the amorphous phase was approx. 25 at. %, while that of Ti was only approx. 3 at. %. A higher fluence implant of 2 x 10/sup 17/ Ti/cm/sup 2/ produced an amorphous <span class="hlt">layer</span> with a lower C concentration of approx. 10 at. % and a Ti concentration of approx. 20 at. %.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SRL....24S0028L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SRL....24S0028L"><span>EFFECT OF HEAT TREATMENT ON (<span class="hlt">Cr</span>, <span class="hlt">Fe</span>)7C3/γ-<span class="hlt">Fe</span> COATINGS IN SITU SYNTHESIZED BY VACUUM ELECTRON BEAM IRRADIATION</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lu, Binfeng; Chen, Yunxia; Xu, Mengjia</p> <p></p> <p>(<span class="hlt">Cr</span>, <span class="hlt">Fe</span>)7C3/γ-<span class="hlt">Fe</span> composite <span class="hlt">layer</span> has been in situ synthesized on a low carbon steel surface by vacuum electron beam VEB irradiation. The synthesized samples were then subdued to different heat treatments to improve their impaired impact toughness. The microstructure, impact toughness and wear resistance of the heat-treated samples were studied by means of optical microscope (OM), X-ray diffraction (XRD), scanning electron microscope (SEM), microhardness tester, impact test machine and tribological tester. After heat treatment, the primary and eutectic carbides remained in their original shape and size, and a large number of secondary carbides precipitated in the iron matrix. Since the Widmanstatten ferrite in the heat affected zone (HAZ) transformed to fine ferrite completely, the impact toughness of the heat-treated samples increased significantly. The microhardness of the heat-treated samples decreased slightly due to the decreased chromium content in the iron matrix. The wear resistance of 1000∘C and 900∘C heat-treated samples was almost same with the as-synthesized sample. While the wear resistance of the 800∘C heat-treated one decreased slightly because part of the austenite matrix had transformed to ferrite matrix, which reduced the bonding of carbides particulates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1364485','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1364485"><span>Sensitivity analysis of <span class="hlt">FeCr</span>Al cladding and U3Si2 fuel under accident conditions</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>Gamble, Kyle Allan Lawrence; Hales, Jason Dean</p> <p>2016-08-01</p> <p>The purpose of this milestone report is to highlight the results of sensitivity analyses performed on two accident tol- erant fuel concepts: U3Si2 fuel and <span class="hlt">FeCr</span>Al cladding. The BISON fuel performance code under development at Idaho National Laboratory was coupled to Sandia National Laboratories’ DAKOTA software to perform the sensitivity analyses. Both Loss of Coolant (LOCA) and Station blackout (SBO) scenarios were analyzed using main effects studies. The results indicate that for <span class="hlt">FeCr</span>Al cladding the input parameters with greatest influence on the output metrics of interest (fuel centerline temperature and cladding hoop strain) during the LOCA were the isotropic swellingmore » and fuel enrichment. For U3Si2 the important inputs were found to be the intergranular diffusion coefficient, specific heat, and fuel thermal conductivity. For the SBO scenario, Young’s modulus was found to be influential in <span class="hlt">FeCr</span>Al in addition to the isotropic swelling and fuel enrichment. Contrarily to the LOCA case, the specific heat of U3Si2 was found to have no effect during the SBO. The intergranular diffusion coefficient and fuel thermal conductivity were still found to be of importance. The results of the sensitivity analyses have identified areas where further research is required including fission gas behavior in U3Si2 and irradiation swelling in <span class="hlt">FeCr</span>Al. Moreover, the results highlight the need to perform the sensitivity analyses on full length fuel rods for SBO scenarios.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OptCo.414...34W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OptCo.414...34W"><span>Surface plasmons based terahertz modulator consisting of <span class="hlt">silicon</span>-air-metal-dielectric-metal <span class="hlt">layers</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, Wei; Yang, Dongxiao; Qian, Zhenhai</p> <p>2018-05-01</p> <p>An optically controlled modulator of the terahertz wave, which is composed of a metal-dielectric-metal structure etched with circular loop arrays on both the metal <span class="hlt">layers</span> and a photoexcited <span class="hlt">silicon</span> wafer separated by an air <span class="hlt">layer</span>, is proposed. Simulation results based on experimentally measured complex permittivities predict that modification of complex permittivity of the <span class="hlt">silicon</span> wafer through excitation laser leads to a significant tuning of transmission characteristics of the modulator, forming the modulation depths of 59.62% and 96.64% based on localized surface plasmon peak and propagating surface plasmon peak, respectively. The influences of the complex permittivity of the <span class="hlt">silicon</span> wafer and the thicknesses of both the air <span class="hlt">layer</span> and the <span class="hlt">silicon</span> wafer are numerically studied for better understanding the modulation mechanism. This study proposes a feasible methodology to design an optically controlled terahertz modulator with large modulation depth, high speed and suitable insertion loss, which is useful for terahertz applications in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810027155&hterms=metamorphosis&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmetamorphosis','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810027155&hterms=metamorphosis&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dmetamorphosis"><span>Si-rich <span class="hlt">Fe</span>-Ni grains in highly unequilibrated chondrites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rambaldi, E. R.; Sears, D. W.; Wasson, J. T.</p> <p>1980-01-01</p> <p>Consideration is given to the Si contents of <span class="hlt">Fe</span>-Ni grains in highly unequilibrated chondrites, which have undergone little metamorphosis and thus best preserve the record of processes in the solar nebula. Electron microprobe determinations of <span class="hlt">silicon</span> content in grains of the Bishunpur chondrite are presented for the six Si-bearing <span class="hlt">Fe</span>-Ni grains for which data could be obtained, five of which were found to be embedded in olivine chondrules. In addition, all grains are found to be <span class="hlt">Cr</span>-rich, with <span class="hlt">Cr</span> increased in concentration towards the grain edge, and to be encased in <span class="hlt">Fe</span>S shells which evidently preserved the Si that entered the <span class="hlt">Fe</span>Ni at higher temperatures. A mechanism for the production of Si-bearing metal during the condensation of the cooling solar nebula is proposed which considers the metal to have condensed heterogeneously while the mafic silicates condensed homogeneously with amounts of required undercooling in the low-pressure regions where ordinary and carbonaceous chondrites formed, resulting in Si mole fractions of 0.003 at nebular pressures less than 0.000001 atm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1246168-homogeneous-heterogeneous-fex-cr1-oh-precipitation-implications-cr-sequestration','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1246168-homogeneous-heterogeneous-fex-cr1-oh-precipitation-implications-cr-sequestration"><span>Homogeneous and Heterogeneous (Fex, <span class="hlt">Cr</span>1-x)(OH)3 Precipitation: Implications for <span class="hlt">Cr</span> Sequestration</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>Dai, Chong; Zuo, Xiaobing; Cao, B</p> <p>2016-02-16</p> <p>The formation of (<span class="hlt">Fe</span>, <span class="hlt">Cr</span>)(OH)3 nanoparticles determines the fate of aqueous <span class="hlt">Cr</span> in many aquatic environments. Using small angle X-ray scattering, precipitation rates of (<span class="hlt">Fe</span>, <span class="hlt">Cr</span>)(OH)3 nanoparticles in solution and on quartz were quantified from 0.1 mM <span class="hlt">Fe</span>(III) solutions containing 0 – 0.25 mM <span class="hlt">Cr</span>(III) at pH = 3.7 ± 0.2. Concentration ratio of aqueous <span class="hlt">Cr(III)/Fe</span>(III) controlled the chemical composition (x) of (Fex, <span class="hlt">Cr</span>1-x)(OH)3 precipitates, solutions’ supersaturation with respect to precipitates, and the surface charge of quartz. Therefore, aqueous <span class="hlt">Cr(III)/Fe</span>(III) ratio affected homogeneous (in solution) and heterogeneous (on quartz) precipitation rates of (Fex, <span class="hlt">Cr</span>1-x)(OH)3 through different mechanisms. The sequestration mechanismsmore » of <span class="hlt">Cr</span>(III) in precipitates were also investigated. In solutions with high aqueous <span class="hlt">Cr(III)/Fe</span>(III) ratios, surface enrichment of <span class="hlt">Cr</span>(III) on the precipitates occurred, resulting in slower particle growth in solution. From solutions with 0 – 0.1 mM <span class="hlt">Cr</span>(III), the particles on quartz grew from 2 to 4 nm within 1 h. Interestingly, from solution with 0.25 mM <span class="hlt">Cr</span>(III), particles of two distinct sizes (2 and 6 nm) formed on quartz, and their sizes remained unchanged throughout the reaction. Our study provided new insights on homogeneous and heterogeneous precipitation of (Fex, <span class="hlt">Cr</span>1-x)(OH)3 nanoparticles, which can help determine the fate of <span class="hlt">Cr</span> in aquatic environments.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMMM..421..472T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMMM..421..472T"><span>Simple electrodepositing of Co<span class="hlt">Fe</span>/Cu multilayers: Effect of ferromagnetic <span class="hlt">layer</span> thicknesses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tekgül, Atakan; Alper, Mürsel; Kockar, Hakan</p> <p>2017-01-01</p> <p>The Co<span class="hlt">Fe</span>/Cu magnetic multilayers were produced by changing Co<span class="hlt">Fe</span> ferromagnetic <span class="hlt">layers</span> from 3 nm to 10 nm using electrodeposition. By now, the thinnest Cu (0.5 nm) <span class="hlt">layer</span> thicknesses were used to see whether the GMR effect in the multilayers can be obtained or not since the pinning of non-magnetic <span class="hlt">layer</span> between the ferromagnetic <span class="hlt">layers</span> is required. For the proper depositions, the cyclic voltammograms was used, and the current-time transients were obtained. The Cu and Co<span class="hlt">Fe</span> <span class="hlt">layers</span> were deposited at a cathode potential of -0.3 and -1.5 V with respect to saturated calomel electrode, respectively. From the XRD patterns, the multilayers were shown to be fcc crystal structures. For the magnetization measurements, saturation magnetization increases from 160 to 600 kA/m from 3 to 8 nm ferromagnetic <span class="hlt">layer</span> thicknesses. And, the coercivity values increase until the 8 nm of the Co<span class="hlt">Fe</span> <span class="hlt">layer</span> thickness. It is seen that the thin Cu <span class="hlt">layer</span> (fixed at 0.5 nm) and pinholes support the random magnetization orientation and thus all multilayers exhibited the giant magnetoresistance (GMR) effect, and the highest GMR value was observed about 5.5%. And, the variation of GMR field sensitivity was calculated. The results show that the GMR and GMR sensitivity are compatible among the multilayers. The Co<span class="hlt">Fe</span>/Cu magnetic multilayers having GMR properties are used in GMR sensors and hard disk drive of the nano-technological devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NatSR...632146Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NatSR...632146Y"><span>Precipitation behavior of AlxCo<span class="hlt">CrFe</span>Ni high entropy alloys under ion irradiation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Tengfei; Xia, Songqin; Liu, Shi; Wang, Chenxu; Liu, Shaoshuai; Fang, Yuan; Zhang, Yong; Xue, Jianming; Yan, Sha; Wang, Yugang</p> <p>2016-08-01</p> <p>Materials performance is central to the satisfactory operation of current and future nuclear energy systems due to the severe irradiation environment in reactors. Searching for structural materials with excellent irradiation tolerance is crucial for developing the next generation nuclear reactors. Here, we report the irradiation responses of a novel multi-component alloy system, high entropy alloy (HEA) AlxCo<span class="hlt">CrFe</span>Ni (x = 0.1, 0.75 and 1.5), focusing on their precipitation behavior. It is found that the single phase system, Al0.1Co<span class="hlt">CrFe</span>Ni, exhibits a great phase stability against ion irradiation. No precipitate is observed even at the highest fluence. In contrast, numerous coherent precipitates are present in both multi-phase HEAs. Based on the irradiation-induced/enhanced precipitation theory, the excellent structural stability against precipitation of Al0.1Co<span class="hlt">CrFe</span>Ni is attributed to the high configurational entropy and low atomic diffusion, which reduces the thermodynamic driving force and kinetically restrains the formation of precipitate, respectively. For the multiphase HEAs, the phase separations and formation of ordered phases reduce the system configurational entropy, resulting in the similar precipitation behavior with corresponding binary or ternary conventional alloys. This study demonstrates the structural stability of single-phase HEAs under irradiation and provides important implications for searching for HEAs with higher irradiation tolerance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57f1302K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57f1302K"><span>Room-temperature bonding of epitaxial <span class="hlt">layer</span> to carbon-cluster ion-implanted <span class="hlt">silicon</span> wafers for CMOS image sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koga, Yoshihiro; Kadono, Takeshi; Shigematsu, Satoshi; Hirose, Ryo; Onaka-Masada, Ayumi; Okuyama, Ryousuke; Okuda, Hidehiko; Kurita, Kazunari</p> <p>2018-06-01</p> <p>We propose a fabrication process for <span class="hlt">silicon</span> wafers by combining carbon-cluster ion implantation and room-temperature bonding for advanced CMOS image sensors. These carbon-cluster ions are made of carbon and hydrogen, which can passivate process-induced defects. We demonstrated that this combination process can be used to form an epitaxial <span class="hlt">layer</span> on a carbon-cluster ion-implanted Czochralski (CZ)-grown <span class="hlt">silicon</span> substrate with a high dose of 1 × 1016 atoms/cm2. This implantation condition transforms the top-surface region of the CZ-grown <span class="hlt">silicon</span> substrate into a thin amorphous <span class="hlt">layer</span>. Thus, an epitaxial <span class="hlt">layer</span> cannot be grown on this implanted CZ-grown <span class="hlt">silicon</span> substrate. However, this combination process can be used to form an epitaxial <span class="hlt">layer</span> on the amorphous <span class="hlt">layer</span> of this implanted CZ-grown <span class="hlt">silicon</span> substrate surface. This bonding wafer has strong gettering capability in both the wafer-bonding region and the carbon-cluster ion-implanted projection range. Furthermore, this wafer inhibits oxygen out-diffusion to the epitaxial <span class="hlt">layer</span> from the CZ-grown <span class="hlt">silicon</span> substrate after device fabrication. Therefore, we believe that this bonding wafer is effective in decreasing the dark current and white-spot defect density for advanced CMOS image sensors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1185986-microstructures-mechanical-properties-compositionally-complex-co-free-fenimncr18-fcc-solid-solution-alloy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1185986-microstructures-mechanical-properties-compositionally-complex-co-free-fenimncr18-fcc-solid-solution-alloy"><span>Microstructures and mechanical properties of compositionally complex Co-free <span class="hlt">FeNiMnCr</span> 18 FCC solid solution alloy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wu, Z.; Bei, H.</p> <p>2015-07-01</p> <p>Recently, a structurally-simple but compositionally-complex <span class="hlt">FeNiCoMnCr</span> high entropy alloy was found to have excellent mechanical properties (e.g., high strength and ductility). To understand the potential of using high entropy alloys as structural materials for advanced nuclear reactor and power plants, it is necessary to have a thorough understanding of their structural stability and mechanical properties degradation under neutron irradiation. Furthermore, this requires us to develop a similar model alloy without Co because material with Co will make post-neutron-irradiation testing difficult due to the production of the 60Co radioisotope. In order to achieve this goal, a FCC-structured single-phase alloy with amore » composition of <span class="hlt">FeNiMnCr</span> 18 was successfully developed. This near-equiatomic <span class="hlt">FeNiMnCr</span> 18 alloy has good malleability and its microstructure can be controlled by thermomechanical processing. By rolling and annealing, the as-cast elongated-grained-microstructure is replaced by homogeneous equiaxed grains. The mechanical properties (e.g., strength and ductility) of the <span class="hlt">FeNiMnCr</span> 18 alloy are comparable to those of the equiatomic <span class="hlt">FeNiCoMnCr</span> high entropy alloy. Both strength and ductility increase with decreasing deformation temperature, with the largest difference occurring between 293 and 77 K. Extensive twin-bands which are bundles of numerous individual twins are observed when it is tensile-fractured at 77 K. No twin bands are detected by EBSD for materials deformed at 293 K and higher. Ultimately the unusual temperature-dependencies of UTS and uniform elongation could be caused by the development of the dense twin substructure, twin-dislocation interactions and the interactions between primary and secondary twinning systems which result in a microstructure refinement and hence cause enhanced strain hardening and postponed necking.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22483122-beol-compatible-high-tunnel-magneto-resistance-perpendicular-magnetic-tunnel-junctions-using-sacrificial-mg-layer-cofeb-free-layer-cap','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22483122-beol-compatible-high-tunnel-magneto-resistance-perpendicular-magnetic-tunnel-junctions-using-sacrificial-mg-layer-cofeb-free-layer-cap"><span>BEOL compatible high tunnel magneto resistance perpendicular magnetic tunnel junctions using a sacrificial Mg <span class="hlt">layer</span> as Co<span class="hlt">Fe</span>B free <span class="hlt">layer</span> cap</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>Swerts, J., E-mail: Johan.Swerts@imec.be; Mertens, S.; Lin, T.</p> <p></p> <p>Perpendicularly magnetized MgO-based tunnel junctions are envisaged for future generation spin-torque transfer magnetoresistive random access memory devices. Achieving a high tunnel magneto resistance and preserving it together with the perpendicular magnetic anisotropy during BEOL CMOS processing are key challenges to overcome. The industry standard technique to deposit the Co<span class="hlt">FeB/MgO/CoFe</span>B tunnel junctions is physical vapor deposition. In this letter, we report on the use of an ultrathin Mg <span class="hlt">layer</span> as free <span class="hlt">layer</span> cap to protect the Co<span class="hlt">Fe</span>B free <span class="hlt">layer</span> from sputtering induced damage during the Ta electrode deposition. When Ta is deposited directly on Co<span class="hlt">Fe</span>B, a fraction of the surface ofmore » the Co<span class="hlt">Fe</span>B is sputtered even when Ta is deposited with very low deposition rates. When depositing a thin Mg <span class="hlt">layer</span> prior to Ta deposition, the sputtering of Co<span class="hlt">Fe</span>B is prevented. The ultra-thin Mg <span class="hlt">layer</span> is sputtered completely after Ta deposition. Therefore, the Mg acts as a sacrificial <span class="hlt">layer</span> that protects the Co<span class="hlt">Fe</span>B from sputter-induced damage during the Ta deposition. The Ta-capped Co<span class="hlt">Fe</span>B free <span class="hlt">layer</span> using the sacrificial Mg interlayer has significantly better electrical and magnetic properties than the equivalent stack without protective <span class="hlt">layer</span>. We demonstrate a tunnel magneto resistance increase up to 30% in bottom pinned magnetic tunnel junctions and tunnel magneto resistance values of 160% at resistance area product of 5 Ω.μm{sup 2}. Moreover, the free <span class="hlt">layer</span> maintains perpendicular magnetic anisotropy after 400 °C annealing.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014MMTB...45..381C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014MMTB...45..381C"><span>Corrosion Behavior of High Nitrogen Nickel-Free <span class="hlt">Fe</span>-16<span class="hlt">Cr</span>-Mn-Mo-N Stainless Steels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chao, K. L.; Liao, H. Y.; Shyue, J. J.; Lian, S. S.</p> <p>2014-04-01</p> <p>The purpose of the current study is to develop austenitic nickel-free stainless steels with lower chromium content and higher manganese and nitrogen contents. In order to prevent nickel-induced skin allergy, cobalt, manganese, and nitrogen were used to substitute nickel in the designed steel. Our results demonstrated that manganese content greater than 14 wt pct results in a structure that is in full austenite phase. The manganese content appears to increase the solubility of nitrogen; however, a lower corrosion potential was found in steel with high manganese content. Molybdenum appears to be able to increase the pitting potential. The effects of <span class="hlt">Cr</span>, Mn, Mo, and N on corrosion behavior of <span class="hlt">Fe</span>-16<span class="hlt">Cr</span>-2Co-Mn-Mo-N high nitrogen stainless steels were evaluated with potentiodynamic tests and XPS surface analysis. The results reveal that anodic current and pits formation of the <span class="hlt">Fe</span>-16<span class="hlt">Cr</span>-2Co-Mn-Mo-N high nitrogen stainless steels were smaller than those of lower manganese and nitrogen content stainless steel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1239761','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1239761"><span>Preliminary Results on <span class="hlt">FeCr</span>Al Alloys in the As-received and Welded State Designed to Have Enhanced Weldability and Radiation Tolerance</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>Field, Kevin G.; Gussev, Maxim N.; Hu, Xunxiang</p> <p>2015-09-30</p> <p>The present report summarizes and discusses the recent results on developing a modern, nuclear grade <span class="hlt">FeCr</span>Al alloy designed to have enhanced radiation tolerance and weldability. The alloys used for these investigations are modern <span class="hlt">FeCr</span>Al alloys based on a <span class="hlt">Fe</span>-13<span class="hlt">Cr</span>-5Al-2Mo-0.2Si-0.05Y alloy (in wt.%, designated C35M). Development efforts have focused on assessing the influence of chemistry and microstructure on the fabricability and performance of these newly developed alloys. Specific focus was made to assess the weldability, thermal stability, and radiation tolerance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JPS...216...15K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JPS...216...15K"><span>Proton exchange membrane micro fuel cells on 3D porous <span class="hlt">silicon</span> gas diffusion <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kouassi, S.; Gautier, G.; Thery, J.; Desplobain, S.; Borella, M.; Ventura, L.; Laurent, J.-Y.</p> <p>2012-10-01</p> <p>Since the 90's, porous <span class="hlt">silicon</span> has been studied and implemented in many devices, especially in MEMS technology. In this article, we present a new approach to build miniaturized proton exchange membrane micro-fuel cells using porous <span class="hlt">silicon</span> as a hydrogen diffusion <span class="hlt">layer</span>. In particular, we propose an innovative process to build micro fuel cells from a “corrugated iron like” 3D structured porous <span class="hlt">silicon</span> substrates. This structure is able to increase up to 40% the cell area keeping a constant footprint on the <span class="hlt">silicon</span> wafer. We propose here a process route to perform electrochemically 3D porous gas diffusion <span class="hlt">layers</span> and to deposit fuel cell active <span class="hlt">layers</span> on such substrates. The prototype peak power performance was measured to be 90 mW cm-2 in a “breathing configuration” at room temperature. These performances are less than expected if we compare with a reference 2D micro fuel cell. Actually, the active <span class="hlt">layer</span> deposition processes are not fully optimized but this prototype demonstrates the feasibility of these 3D devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005JAP....98e4906F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005JAP....98e4906F"><span>Surface morphological evolution of epitaxial <span class="hlt">Cr</span>N(001) <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Frederick, J. R.; Gall, D.</p> <p>2005-09-01</p> <p><span class="hlt">Cr</span>N <span class="hlt">layers</span>, 57 and 230 nm thick, were grown on MgO(001) at Ts=600-800 °C by ultrahigh-vacuum magnetron sputter deposition in pure N2 discharges from an oblique deposition angle α=80°. <span class="hlt">Layers</span> grown at 600 °C nucleate as single crystals with a cube-on-cube epitaxial relationship with the substrate. However, rough surfaces with cauliflower-type morphologies cause the nucleation of misoriented <span class="hlt">Cr</span>N grains that develop into cone-shaped grains that protrude out of the epitaxial matrix to form triangular faceted surface mounds. The surface morphology of epitaxial <span class="hlt">Cr</span>N(001) grown at 700 °C is characterized by dendritic ridge patterns extending along the orthogonal <110> directions superposed by square-shaped super mounds with <100> edges. The ridge patterns are attributed to a Bales-Zangwill instability while the supermounds form due to atomic shadowing which leads to the formation of epitaxial inverted pyramids that are separated from the surrounding <span class="hlt">layer</span> by tilted nanovoids. Growth at 800 °C yields complete single crystals with smooth surfaces. The root-mean-square surface roughness for 230-nm-thick <span class="hlt">layers</span> decreases from 18.8 to 9.3 to 1.1 nm as Ts is raised from 600 to 700 to 800 °C. This steep decrease is due to a transition in the roughening mechanism from atomic shadowing to kinetic roughening. Atomic shadowing is dominant at 600 and 700 °C, where misoriented grains and supermounds, respectively, capture a larger fraction of the oblique deposition flux in comparison to the surrounding epitaxial matrix, resulting in a high roughening rate that is described by a power law with an exponent β>0.5. In contrast, kinetic roughening controls the surface morphology for Ts=800 °C, as well as the epitaxial fraction of the <span class="hlt">layers</span> grown at 600 and 700 °C, yielding relatively smooth surfaces and β<=0.27.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AIPC.1731n0037B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AIPC.1731n0037B"><span>Structural and magnetic properties of Prussian blue analogue molecular magnet <span class="hlt">Fe</span>1.5[<span class="hlt">Cr</span>(CN)6].mH2O</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bhatt, Pramod; Meena, S. S.; Mukadam, M. D.; Yusuf, S. M.</p> <p>2016-05-01</p> <p>Molecular magnets, based on Prussian blue analogues, <span class="hlt">Fe</span>1.5[<span class="hlt">Cr</span>(CN)6].mH2O have been synthesized in the bulk as well as nanoparticle forms using a co-precipitation method, and their structural and magnetic properties have been investigated using x-ray diffraction (XRD) Mössbauer spectroscopy and dc magnetization. The XRD study confirms the single phase crystalline and nanoparticle nature of the compounds with a face centered cubic (fcc) structure of space group Fm3m. The values of lattice constant are found to be ~10.18(5) Å and ~9.98(9)Å, for the bulk and nanoparticle samples, respectively. The dc magnetization shows a Curie temperature (TC) of ~17 K and ~5 K for the bulk and nanopartcile samples, respectively. The Mossouber spectroscopy reveal that the compound shows spin flipping from the high spin (HS) <span class="hlt">Fe</span> (<span class="hlt">CrIII-C≡N-Fe</span>II) to low spin (LS) <span class="hlt">Fe</span>II ions (<span class="hlt">CrIII-N≡C-Fe</span>II). Moreover, the TC and the HS state of the <span class="hlt">Fe</span> ions decreases (converts to its LS states) with time as well as in the nanoparticle form compared to bulk.</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('https://www.osti.gov/pages/biblio/1422734-high-precision-qec-values-superallowed-emitters','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1422734-high-precision-qec-values-superallowed-emitters"><span>High-precision Q EC values of superallowed 0 + → 0 + β-emitters 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zhang, P.; Xu, X.; Shuai, P.; ...</p> <p>2017-01-23</p> <p>Short-lived 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni were studied by isochronous mass spectrometry at the HIRFL-CSR facility in Lanzhou. The measured precision mass excesses (ME) of 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni are -29471(11) keV, -34477(6) keV and -39278(4) keV, respectively. The superallowed 0 +→0+β-decay Q values were derived to be Q EC( 46<span class="hlt">Cr</span>) =7604(11) keV, Q EC( 50<span class="hlt">Fe</span>) =8150(6) keV and Q EC( 54Ni) =8731(4) keV. The values for 50<span class="hlt">Fe</span> and 54Ni are by one order of magnitude more precise than the adopted literature values. By combining the existing half-lives and branching ratios, we obtained the corrected ℱt values to be ℱt(more » 50<span class="hlt">Fe</span>) =3103(70) s and ℱt( 54Ni) =3076(50) s. The main contribution to the ℱt uncertainties is now due to β-decay branching ratios, still, more high-precision measurements of the half-lives, the masses, and especially the branching ratios are needed in order to satisfy the requirements for a stringent CVC test.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1422734','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1422734"><span>High-precision Q EC values of superallowed 0 + → 0 + β-emitters 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni</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>Zhang, P.; Xu, X.; Shuai, P.</p> <p></p> <p>Short-lived 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni were studied by isochronous mass spectrometry at the HIRFL-CSR facility in Lanzhou. The measured precision mass excesses (ME) of 46<span class="hlt">Cr</span>, 50<span class="hlt">Fe</span> and 54Ni are -29471(11) keV, -34477(6) keV and -39278(4) keV, respectively. The superallowed 0 +→0+β-decay Q values were derived to be Q EC( 46<span class="hlt">Cr</span>) =7604(11) keV, Q EC( 50<span class="hlt">Fe</span>) =8150(6) keV and Q EC( 54Ni) =8731(4) keV. The values for 50<span class="hlt">Fe</span> and 54Ni are by one order of magnitude more precise than the adopted literature values. By combining the existing half-lives and branching ratios, we obtained the corrected ℱt values to be ℱt(more » 50<span class="hlt">Fe</span>) =3103(70) s and ℱt( 54Ni) =3076(50) s. The main contribution to the ℱt uncertainties is now due to β-decay branching ratios, still, more high-precision measurements of the half-lives, the masses, and especially the branching ratios are needed in order to satisfy the requirements for a stringent CVC test.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1849b0027N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1849b0027N"><span>Electrochemical sensing of modified ABO3 perovskite: La<span class="hlt">Fe</span>0.8 R0.2O3(R= <span class="hlt">Cr</span>, Co, Al)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vidya Rajan, N.; Alexander, L. K.</p> <p>2017-06-01</p> <p>Perovskite La<span class="hlt">Fe</span>O3 with orthorhombic structure has been synthesized by citric acid mediated solution method. The effectiveness of ionic radii and Oxidation state of the doping material on ionic conductivity of the host matrix was evaluated by B-site (<span class="hlt">Fe</span>) doping on La<span class="hlt">Fe</span>O3 with <span class="hlt">Cr</span>, Co and Al, resulting La<span class="hlt">Fe</span>0.8 R0.2O3 (R = <span class="hlt">Cr</span>, Co, Al). XRD with Rietveld refinement and Raman spectroscopic analysis demonstrate successful synthesis. The effect of the 20% B site doping on electrochemical activity is reported. The doped materials exhibit a decrease in sensing activity towards the non enzymatic detection of H2O2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123a5302L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123a5302L"><span>Suppression of interfacial voids formation during silane (SiH4)-based <span class="hlt">silicon</span> oxide bonding with a thin <span class="hlt">silicon</span> nitride capping <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Kwang Hong; Bao, Shuyu; Wang, Yue; Fitzgerald, Eugene A.; Seng Tan, Chuan</p> <p>2018-01-01</p> <p>The material properties and bonding behavior of silane-based <span class="hlt">silicon</span> oxide <span class="hlt">layers</span> deposited by plasma-enhanced chemical vapor deposition were investigated. Fourier transform infrared spectroscopy was employed to determine the chemical composition of the <span class="hlt">silicon</span> oxide films. The incorporation of hydroxyl (-OH) groups and moisture absorption demonstrates a strong correlation with the storage duration for both as-deposited and annealed <span class="hlt">silicon</span> oxide films. It is observed that moisture absorption is prevalent in the silane-based <span class="hlt">silicon</span> oxide film due to its porous nature. The incorporation of -OH groups and moisture absorption in the <span class="hlt">silicon</span> oxide films increase with the storage time (even in clean-room environments) for both as-deposited and annealed <span class="hlt">silicon</span> oxide films. Due to silanol condensation and <span class="hlt">silicon</span> oxidation reactions that take place at the bonding interface and in the bulk <span class="hlt">silicon</span>, hydrogen (a byproduct of these reactions) is released and diffused towards the bonding interface. The trapped hydrogen forms voids over time. Additionally, the absorbed moisture could evaporate during the post-bond annealing of the bonded wafer pair. As a consequence, defects, such as voids, form at the bonding interface. To address the problem, a thin <span class="hlt">silicon</span> nitride capping film was deposited on the <span class="hlt">silicon</span> oxide <span class="hlt">layer</span> before bonding to serve as a diffusion barrier to prevent moisture absorption and incorporation of -OH groups from the ambient. This process results in defect-free bonded wafers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1394222-heterogeneous-creep-deformations-correlation-microstructures-fe-alloys-strengthened-fe2nb-laves-phase','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1394222-heterogeneous-creep-deformations-correlation-microstructures-fe-alloys-strengthened-fe2nb-laves-phase"><span>Heterogeneous Creep Deformations and Correlation to Microstructures in <span class="hlt">Fe</span>-30<span class="hlt">Cr</span>-3Al Alloys Strengthened by an <span class="hlt">Fe</span> 2Nb Laves Phase</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Shassere, Benjamin; Yamamoto, Yukinori; Poplawsky, Jonathan; ...</p> <p>2017-08-07</p> <p>We have develooped a new <span class="hlt">Fe-Cr</span>-Al (FCA) alloy system with good oxidation resistance and creep strength at high temperature. The alloy system is a candidate for use in future fossil-fueled power plants. The creep strength of these alloys at 973 K (700 °C) was found to be comparable with traditional 9 pct <span class="hlt">Cr</span> ferritic–martensitic steels. A few FCA alloys with general composition of <span class="hlt">Fe</span>-30<span class="hlt">Cr</span>-3Al-.2Si-xNb (x = 0, 1, or 2) with a ferrite matrix and <span class="hlt">Fe</span> 2Nb-type Laves precipitates were prepared. The detailed microstructural characterization of samples, before and after creep rupture testing, indicated precipitation of the Laves phase withinmore » the matrix, Laves phase at the grain boundaries, and a 0.5 to 1.5 μm wide precipitate-free zone (PFZ) parallel to all the grain boundaries. In these alloys, the areal fraction of grain boundary Laves phase and the width of the PFZ controlled the cavitation nucleation and eventual grain boundary ductile failure. Finally, we used a phenomenological model to compare the creep strain rates controlled by the effects of the particles on the dislocations within the grain and at grain boundaries. (The research sponsored by US-DOE, Office of Fossil Energy, the Crosscutting Research Program).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7140406','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/7140406"><span>Improved oxidation sulfidation resistance of <span class="hlt">Fe-Cr</span>-Ni alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Natesan, K.; Baxter, D.J.</p> <p>1983-07-26</p> <p>High temperature resistance of <span class="hlt">Fe-Cr</span>-Ni alloy compositions to oxidative and/or sulfidative conditions is provided by the incorporation of about 1 to 8 wt % of Zr or Nb and results in a two-phase composition having an alloy matrix as the first phase and a fine grained intermetallic composition as the second phase. The presence and location of the intermetallic composition between grains of the matrix provides mechanical strength, enhanced surface scale adhesion, and resistance to corrosive attack between grains of the alloy matrix at temperatures of 500 to 1000/sup 0/C.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017REDS..172..364A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017REDS..172..364A"><span>Evolution of displacement cascades in <span class="hlt">Fe-Cr</span> structures with different [001] tilt 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>Abu-Shams, M.; Haider, W.; Shabib, I.</p> <p>2017-06-01</p> <p>Reduced-activation ferritic/martensitic steels of <span class="hlt">Cr</span> concentration between 2.25 and 12 wt% are candidate structural materials for next-generation nuclear reactors. In this study, molecular dynamics (MD) simulation is used to generate the displacement cascades in <span class="hlt">Fe-Cr</span> structures with different <span class="hlt">Cr</span> concentrations by using different primary knock-on atom (PKA) energies between 2 and 10 keV. A concentration-dependent model potential has been used to describe the interactions between <span class="hlt">Fe</span> and <span class="hlt">Cr</span>. Single crystals (SCs) of three different coordinate bases (e.g. [310], [510], and [530]) and bi-crystal (BC) structures with three different [001] tilt grain boundaries (GBs) (e.g. Σ5, Σ13, and Σ17) have been simulated. The Wigner-Seitz cell criterion has been used to identify the produced Frenkel pairs. The results show a marked difference between collisions observed in SCs and those in BC structures. The numbers of vacancies and interstitials are found to be significantly higher in BC structures than those found in SCs. The number of point defects exhibits a power relationship with the PKA energies; however, the <span class="hlt">Cr</span> concentration does not seem to have any influence on the number of survived point defects. In BC models, a large fraction of the total survived point defects (between 59% and 93%) tends accumulate at the GBs, which seem to trap the generated point defects. The BC structure with Σ17 GB is found to trap more defects than Σ5 and Σ13 GBs. The defect trapping is found to be dictated by the crystallographic parameters of the GBs. For all studied GBs, self-interstitial atoms (SIAs) are easily trapped within the GB region than vacancies. An analysis of defect composition reveals an enrichment of <span class="hlt">Cr</span> in SIAs, and in BC cases, more than half of the <span class="hlt">Cr</span>-SIAs are found to be located within the GB region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JMiMi..24c5011D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JMiMi..24c5011D"><span>Nested potassium hydroxide etching and protective coatings for <span class="hlt">silicon</span>-based microreactors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Mas, Nuria; Schmidt, Martin A.; Jensen, Klavs F.</p> <p>2014-03-01</p> <p>We have developed a multilayer, multichannel <span class="hlt">silicon</span>-based microreactor that uses elemental fluorine as a reagent and generates hydrogen fluoride as a byproduct. Nested potassium hydroxide etching (using <span class="hlt">silicon</span> nitride and <span class="hlt">silicon</span> oxide as masking materials) was developed to create a large number of channels (60 reaction channels connected to individual gas and liquid distributors) of significantly different depths (50-650 µm) with sloped walls (54.7° with respect to the (1 0 0) wafer surface) and precise control over their geometry. The wetted areas were coated with thermally grown <span class="hlt">silicon</span> oxide and electron-beam evaporated nickel films to protect them from the corrosive fluorination environment. Up to four Pyrex <span class="hlt">layers</span> were anodically bonded to three <span class="hlt">silicon</span> <span class="hlt">layers</span> in a total of six bonding steps to cap the microchannels and stack the reaction <span class="hlt">layers</span>. The average pinhole density in as-evaporated films was 3 holes cm-2. Heating during anodic bonding (up to 350 °C for 4 min) did not significantly alter the film composition. Upon fluorine exposure, nickel films (160 nm thick) deposited on an adhesion <span class="hlt">layer</span> of <span class="hlt">Cr</span> (10 nm) over an oxidized <span class="hlt">silicon</span> substrate (up to 500 nm thick SiO2) led to the formation of a nickel fluoride passivation <span class="hlt">layer</span>. This microreactor was used to investigate direct fluorinations at room temperature over several hours without visible signs of film erosion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014MMTA...45..201Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014MMTA...45..201Y"><span>Microstructure and Tribological Properties of AlCo<span class="hlt">CrFe</span>NiTi0.5 High-Entropy Alloy in Hydrogen Peroxide Solution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Y.; Liu, W. M.; Zhang, T. B.; Li, J. S.; Wang, J.; Kou, H. C.; Li, J.</p> <p>2014-01-01</p> <p>Microstructure and tribological properties of an AlCo<span class="hlt">CrFe</span>NiTi0.5 high-entropy alloy in high-concentration hydrogen peroxide solution were investigated in this work. The results show that the sigma phase precipitates and the content of bcc2 decrease during the annealing process. Meanwhile, the complex construction of the interdendrite region changes into simple isolated-island shape, and much more spherical precipitates are formed. Those changes of microstructure during the annealing process lead to the increase of hardness of this alloy. In the testing conditions, the AlCo<span class="hlt">CrFe</span>NiTi0.5 alloy shows smoother worn surfaces and steadier coefficient of friction curves than does the 1<span class="hlt">Cr</span>18Ni9Ti stainless steel, and SiC ceramic preserves better wear resistance than ZrO2 ceramic. After annealing, the wear resistance of the AlCo<span class="hlt">CrFe</span>NiTi0.5 alloy increases coupled with SiC counterface but decreases with ZrO2 counterface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003MMI.....9..389H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003MMI.....9..389H"><span>Role of lead in electrochemical reaction of alloy 600, alloy 690, Ni, <span class="hlt">Cr</span>, and <span class="hlt">Fe</span> in water</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hwang, Seong Sik; Kim, Joung Soo; Kim, Ju Yup</p> <p>2003-08-01</p> <p>It has been reported that lead causes stress corrosion cracking (SCC) in the secondary side of steam generators (SG) in pressurized water reactors (PWR). The materials of SG tubings are alloy 600, alloy 690, or alloy 800, among which the main alloying elements are Ni, <span class="hlt">Cr</span>, and <span class="hlt">Fe</span>. The effect of lead on the electrochemical behaviors of alloy 600 and alloy 690 using an anodic polarization technique was evaluated. We also obtained polarization curves of pure Ni, <span class="hlt">Cr</span>, and <span class="hlt">Fe</span> in water containing lead. As the amount of lead in the solution increased, critical current densities and passive current densities of alloy 600 and alloy 690 increased, while the breakdown potential of the alloys decreased. Lead increased critical current density and the passive current of <span class="hlt">Cr</span> in pH 4 and pH 10. The instability of passive film of steam generator tubings in water containing lead might arise from the instability of <span class="hlt">Cr</span> passivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/985667','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/985667"><span>Manufacture of <span class="hlt">silicon</span>-based devices having disordered sulfur-doped surface <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Carey, III; Edward, James [Newton, MA; Mazur, Eric [Concord, MA</p> <p>2008-04-08</p> <p>The present invention provides methods of fabricating a radiation-absorbing semiconductor wafer by irradiating at least one surface location of a <span class="hlt">silicon</span> substrate, e.g., an n-doped crystalline <span class="hlt">silicon</span>, by a plurality of temporally short laser pulses, e.g., femtosecond pulses, while exposing that location to a substance, e.g., SF.sub.6, having an electron-donating constituent so as to generate a substantially disordered surface <span class="hlt">layer</span> (i.e., a microstructured <span class="hlt">layer</span>) that incorporates a concentration of that electron-donating constituent, e.g., sulfur. The substrate is also annealed at an elevated temperature and for a duration selected to enhance the charge carrier density in the surface <span class="hlt">layer</span>. For example, the substrate can be annealed at a temperature in a range of about 700 K to about 900 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28333432','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28333432"><span>Atomic <span class="hlt">Layer</span> Deposition Alumina-Passivated <span class="hlt">Silicon</span> Nanowires: Probing the Transition from Electrochemical Double-<span class="hlt">Layer</span> Capacitor to Electrolytic Capacitor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gaboriau, Dorian; Boniface, Maxime; Valero, Anthony; Aldakov, Dmitry; Brousse, Thierry; Gentile, Pascal; Sadki, Said</p> <p>2017-04-19</p> <p><span class="hlt">Silicon</span> nanowires were coated by a 1-5 nm thin alumina <span class="hlt">layer</span> by atomic <span class="hlt">layer</span> deposition (ALD) in order to replace poorly reproducible and unstable native <span class="hlt">silicon</span> oxide by a highly conformal passivating alumina <span class="hlt">layer</span>. The surface coating enabled probing the behavior of symmetric devices using such electrodes in the EMI-TFSI electrolyte, allowing us to attain a large cell voltage up to 6 V in ionic liquid, together with very high cyclability with less than 4% capacitance fade after 10 6 charge/discharge cycles. These results yielded fruitful insights into the transition between an electrochemical double-<span class="hlt">layer</span> capacitor behavior and an electrolytic capacitor behavior. Ultimately, thin ALD dielectric coatings can be used to obtain hybrid devices exhibiting large cell voltage and excellent cycle life of dielectric capacitors, while retaining energy and power densities close to the ones displayed by supercapacitors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3773432','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3773432"><span>Raman Spectra of High-κ Dielectric <span class="hlt">Layers</span> Investigated with Micro-Raman Spectroscopy Comparison with <span class="hlt">Silicon</span> Dioxide</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Borowicz, P.; Taube, A.; Rzodkiewicz, W.; Latek, M.; Gierałtowska, S.</p> <p>2013-01-01</p> <p>Three samples with dielectric <span class="hlt">layers</span> from high-κ dielectrics, hafnium oxide, gadolinium-<span class="hlt">silicon</span> oxide, and lanthanum-lutetium oxide on <span class="hlt">silicon</span> substrate were studied by Raman spectroscopy. The results obtained for high-κ dielectrics were compared with spectra recorded for <span class="hlt">silicon</span> dioxide. Raman spectra suggest the similarity of gadolinium-<span class="hlt">silicon</span> oxide and lanthanum-lutetium oxide to the bulk nondensified <span class="hlt">silicon</span> dioxide. The temperature treatment of hafnium oxide shows the evolution of the structure of this material. Raman spectra recorded for as-deposited hafnium oxide are similar to the results obtained for <span class="hlt">silicon</span> dioxide <span class="hlt">layer</span>. After thermal treatment especially at higher temperatures (600°C and above), the structure of hafnium oxide becomes similar to the bulk non-densified <span class="hlt">silicon</span> dioxide. PMID:24072982</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22494959-influence-intermediate-layers-surface-condition-laser-crystallized-silicon-thin-films-solar-cell-performance','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22494959-influence-intermediate-layers-surface-condition-laser-crystallized-silicon-thin-films-solar-cell-performance"><span>Influence of intermediate <span class="hlt">layers</span> on the surface condition of laser crystallized <span class="hlt">silicon</span> thin films and solar cell performance</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>Höger, Ingmar, E-mail: ingmar.hoeger@ipht-jena.de; Gawlik, Annett; Brückner, Uwe</p> <p></p> <p>The intermediate <span class="hlt">layer</span> (IL) between glass substrate and <span class="hlt">silicon</span> plays a significant role in the optimization of multicrystalline liquid phase crystallized <span class="hlt">silicon</span> thin film solar cells on glass. This study deals with the influence of the IL on the surface condition and the required chemical surface treatment of the crystallized <span class="hlt">silicon</span> (mc-Si), which is of particular interest for a-Si:H heterojunction thin film solar cells. Two types of IL were investigated: sputtered <span class="hlt">silicon</span> nitride (SiN) and a <span class="hlt">layer</span> stack consisting of <span class="hlt">silicon</span> nitride and <span class="hlt">silicon</span> oxide (SiN/SiO). X-ray photoelectron spectroscopy measurements revealed the formation of <span class="hlt">silicon</span> oxynitride (SiO{sub x}N{sub y}) ormore » <span class="hlt">silicon</span> oxide (SiO{sub 2}) <span class="hlt">layers</span> at the surface of the mc-Si after liquid phase crystallization on SiN or SiN/SiO, respectively. We propose that SiO{sub x}N{sub y} formation is governed by dissolving nitrogen from the SiN <span class="hlt">layer</span> in the <span class="hlt">silicon</span> melt, which segregates at the crystallization front during crystallization. This process is successfully hindered, when additional SiO <span class="hlt">layers</span> are introduced into the IL. In order to achieve solar cell open circuit voltages above 500 mV, a removal of the formed SiO{sub x}N{sub y} top <span class="hlt">layer</span> is required using sophisticated cleaning of the crystallized <span class="hlt">silicon</span> prior to a-Si:H deposition. However, solar cells crystallized on SiN/SiO yield high open circuit voltage even when a simple wet chemical surface treatment is applied. The implementation of SiN/SiO intermediate <span class="hlt">layers</span> facilitates the production of mesa type solar cells with open circuit voltages above 600 mV and a power conversion efficiency of 10%.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1240581','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1240581"><span>Status Report on Irradiation Capsules Containing Welded <span class="hlt">FeCr</span>Al Specimens for Radiation Tolerance Evaluation</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>Field, Kevin G.; Howard, Richard H.</p> <p>2016-02-26</p> <p>This status report provides the background and current status of a series of irradiation capsules, or “rabbits”, that were designed and built to test the contributions of microstructure, composition, damage dose, and irradiation temperature on the radiation tolerance of candidate <span class="hlt">FeCr</span>Al alloys being developed to have enhanced weldability and radiation tolerance. These rabbits will also test the validity of using an ultra-miniature tensile specimen to assess the mechanical properties of irradiated <span class="hlt">FeCr</span>Al base metal and weldments. All rabbits are to be irradiated in the High Flux Isotope Reactor (HFIR) at Oak Ridge National Laboratory (ORNL) to damage doses up tomore » ≥15 dpa at temperatures between 200-550°C.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28683367','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28683367"><span>Efficient removal of arsenic by strategically designed and <span class="hlt">layer-by-layer</span> assembled PS@+rGO@GO@<span class="hlt">Fe</span>3O4 composites.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kang, Bong Kyun; Lim, Byeong Seok; Yoon, Yeojoon; Kwag, Sung Hoon; Park, Won Kyu; Song, Young Hyun; Yang, Woo Seok; Ahn, Yong-Tae; Kang, Joon-Wun; Yoon, Dae Ho</p> <p>2017-10-01</p> <p>The PS@+rGO@GO@<span class="hlt">Fe</span> 3 O 4 (PG-<span class="hlt">Fe</span> 3 O 4 ) hybrid composites for Arsenic removal were successfully fabricated and well dispersed using <span class="hlt">layer-by-layer</span> assembly and a hydrothermal method. The PG-<span class="hlt">Fe</span> 3 O 4 hybrid composites were composed of uniformly coated <span class="hlt">Fe</span> 3 O 4 nanoparticles on graphene oxide <span class="hlt">layers</span> with water flow space between 3D structures providing many contact area and adsorption sites for Arsenic adsorption. The PG-<span class="hlt">Fe</span> 3 O 4 hybrid composite has large surface adsorption sites and exhibits high adsorption capacities of 104 mg/g for As (III) and 68 mg/g for As (V) at 25 °C and pH 7 comparison with pure <span class="hlt">Fe</span> 3 O 4 and P-<span class="hlt">Fe</span> 3 O 4 samples. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.1639K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.1639K"><span>Synthesis of quenchable high-pressure form of magnetite (h-<span class="hlt">Fe</span>3O4) with composition [4](<span class="hlt">Fe</span>0.732+ Mg0.26)[6](<span class="hlt">Fe</span>0.713+ <span class="hlt">Cr</span>0.14Al0.10 Si0.04)2O4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koch-Müller, Monika; Mugnaioli, Enrico; Rhede, Dieter; Speziale, Sergio; Kolb, Ute; Wirth, Richard</p> <p>2014-05-01</p> <p>Cubic inverse-spinel magnetite transforms under pressure to orthorhombic normal-spinel magnetite, h-<span class="hlt">Fe</span>3O4 ( e.g. Fei et al. 1999; Bengtson et al. 2013). The pressure at which the transition takes place is still controversial. The high-pressure form is reported to be not quenchable to ambient conditions. We report the synthesis of h-magnetite which incorporates considerable amounts of additional cations (<span class="hlt">Cr</span>, Mg, Al, Si) and is quenchable to ambient conditions. Two experiments were performed at 18 GPa and 1800 ° C in a multi-anvil press. The run products were investigated by electron microprobe, transmission electron microscopy and electron diffraction tomography. We observed the formation of h-magnetite in both experiments. In experiment MA-367 we used an oxide mixture with a majoritic stoichiometry Mg1.8<span class="hlt">Fe</span>1.2(Al1.4 <span class="hlt">Cr</span>0.2Si0.2Mg0.2)Si3O12 as starting material, with Si and Mg in excess. The <span class="hlt">Fe</span>-oxide phase forms elongated aggregates 10-30 μm in length, mutually intergrown with majorite, the latter being the main phase of the run products coexisting with small amounts of stishovite. The formula for h-magnetite in run MA-367 was calculated as [4](<span class="hlt">Fe</span>0.732+ Mg0.26)[6](<span class="hlt">Fe</span>0.713+ <span class="hlt">Cr</span>0.14Al0.10 Si0.04)2O4. In the second experiment (MA-376) we used an oxide mixture corresponding to the composition of h-magnetite obtained in MA-367. In this experiment the main phase was h-magnetite with composition [4](<span class="hlt">Fe</span>0.982+)[6](<span class="hlt">Fe</span>0.683+ <span class="hlt">Cr</span>0.17Al0.13 Si0.02)2O4coexisting with very small amounts of wadsleyite. Interestingly no magnesium was incorporated into the <span class="hlt">Fe</span>-oxide in this experiment compared to MA-367 and no iron was found in the coexisting wadsleyite. For the first time it was possible to perform electron diffraction on recovered h-magnetite of both experiments and we observed that -at least in our case- the h-magnetite structure can better be described in space group Amam than in space group Bbmm as previously proposed. The substitution of <span class="hlt">Fe</span> by <span class="hlt">Cr</span>, Mg, Al and Si, all smaller in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5452098','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5452098"><span>Material Analysis of Coated <span class="hlt">Siliconized</span> <span class="hlt">Silicon</span> Carbide (SiSiC) Honeycomb Structures for Thermochemical Hydrogen Production</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Neises-von Puttkamer, Martina; Simon, Heike; Schmücker, Martin; Roeb, Martin; Sattler, Christian; Pitz-Paal, Robert</p> <p>2013-01-01</p> <p>In the present work, thermochemical water splitting with <span class="hlt">siliconized</span> <span class="hlt">silicon</span> carbide (SiSiC) honeycombs coated with a zinc ferrite redox material was investigated. The small scale coated monoliths were tested in a laboratory test-rig and characterized by X-ray diffractometry (XRD) and Scanning Electron Microscopy (SEM) with corresponding micro analysis after testing in order to characterize the changes in morphology and composition. Comparison of several treated monoliths revealed the formation of various reaction products such as SiO2, zircon (ZrSiO4), iron silicide (<span class="hlt">Fe</span>Si) and hercynite (<span class="hlt">Fe</span>Al2O4) indicating the occurrence of various side reactions between the different phases of the coating as well as between the coating and the SiSiC substrate. The investigations showed that the ferrite is mainly reduced through reaction with <span class="hlt">silicon</span> (Si), which is present in the SiSiC matrix, and <span class="hlt">silicon</span> carbide (SiC). These results led to the formulation of a new redox mechanism for this system in which Zn-ferrite is reduced through Si forming <span class="hlt">silicon</span> dioxide (SiO2) and through SiC forming SiO2 and carbon monoxide. A decline of hydrogen production within the first 20 cycles is suggested to be due to the growth of a <span class="hlt">silicon</span> dioxide and zircon <span class="hlt">layer</span> which acts as a diffusion barrier for the reacting specie. PMID:28809316</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28809316','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28809316"><span>Material Analysis of Coated <span class="hlt">Siliconized</span> <span class="hlt">Silicon</span> Carbide (SiSiC) Honeycomb Structures for Thermochemical Hydrogen Production.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Neises-von Puttkamer, Martina; Simon, Heike; Schmücker, Martin; Roeb, Martin; Sattler, Christian; Pitz-Paal, Robert</p> <p>2013-01-31</p> <p>In the present work, thermochemical water splitting with <span class="hlt">siliconized</span> <span class="hlt">silicon</span> carbide (SiSiC) honeycombs coated with a zinc ferrite redox material was investigated. The small scale coated monoliths were tested in a laboratory test-rig and characterized by X-ray diffractometry (XRD) and Scanning Electron Microscopy (SEM) with corresponding micro analysis after testing in order to characterize the changes in morphology and composition. Comparison of several treated monoliths revealed the formation of various reaction products such as SiO₂, zircon (ZrSiO₄), iron silicide (<span class="hlt">Fe</span>Si) and hercynite (<span class="hlt">Fe</span>Al₂O₄) indicating the occurrence of various side reactions between the different phases of the coating as well as between the coating and the SiSiC substrate. The investigations showed that the ferrite is mainly reduced through reaction with <span class="hlt">silicon</span> (Si), which is present in the SiSiC matrix, and <span class="hlt">silicon</span> carbide (SiC). These results led to the formulation of a new redox mechanism for this system in which Zn-ferrite is reduced through Si forming <span class="hlt">silicon</span> dioxide (SiO₂) and through SiC forming SiO₂ and carbon monoxide. A decline of hydrogen production within the first 20 cycles is suggested to be due to the growth of a <span class="hlt">silicon</span> dioxide and zircon <span class="hlt">layer</span> which acts as a diffusion barrier for the reacting specie.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123o5105R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123o5105R"><span>First-principles investigation of diffusion and defect properties of <span class="hlt">Fe</span> and Ni in <span class="hlt">Cr</span>2O3</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rak, Zs.; Brenner, D. W.</p> <p>2018-04-01</p> <p>Diffusion of <span class="hlt">Fe</span> and Ni and the energetics of <span class="hlt">Fe</span>- and Ni-related defects in chromium oxide (α-<span class="hlt">Cr</span>2O3) are investigated using first-principles Density Functional Theory calculations in combination with the climbing-image nudged elastic band method. The orientations of the spin magnetic moments of the migrating ions are taken into account and their effects on migration barriers are examined. Several possible diffusion pathways were explored through interstitial and vacancy mechanisms, and it was found that the principal mode of ion transport in <span class="hlt">Cr</span>2O3 is via vacancies. Both interstitial- and vacancy-mediated diffusions are anisotropic, with diffusion being faster in the z-direction. The energetics of defect formation indicates that the Ni-related defects are less stable than the <span class="hlt">Fe</span>-related ones. This is consistent with Ni-diffusion being faster than <span class="hlt">Fe</span>-diffusion. The results are compared with previous theoretical and experimental data and possible implications in corrosion control are discussed.</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/2018MMI....24..597O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MMI....24..597O"><span>Microstructure and Mechanical Properties of Highly Alloyed <span class="hlt">FeCr</span>MoVC Steel Fabricated by Spark Plasma Sintering</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Oh, Seung-Jin; Jun, Joong-Hwan; Lee, Min-Ha; Shon, In-Jin; Lee, Seok-Jae</p> <p>2018-05-01</p> <p>In this study, we successfully fabricated highly alloyed <span class="hlt">FeCr</span>MoVC specimens within 2 min by using the spark plasma sintering (SPS) method. The densities of the sintered specimens were almost identical to their theoretical values. Fine (Mo, V)-rich carbides with lamellar structure were precipitated along the grain boundaries of the as-sintered specimen, whereas relatively large carbides were formed additionally in the transgranular region during the tempering treatment. Compared with the specimen produced by a conventional casting method, the <span class="hlt">FeCr</span>MoVC specimens from SPS showed smaller grain size with finer carbides and higher hardness values.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1439974','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1439974"><span>Atomic-scale to Meso-scale Simulation Studies of Thermal Ageing and Irradiation Effects in <span class="hlt">Fe</span>- <span class="hlt">Cr</span> Alloys</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>Stanley, Eugene; Liu, Li</p> <p></p> <p>In this project, we target at three primary objectives: (1) Molecular Dynamics (MD) code development for <span class="hlt">Fe-Cr</span> alloys, which can be utilized to provide thermodynamic and kinetic properties as inputs in mesoscale Phase Field (PF) simulations; (2) validation and implementation of the MD code to explain thermal ageing and radiation damage; and (3) an integrated modeling platform for MD and PF simulations. These two simulation tools, MD and PF, will ultimately be merged to understand and quantify the kinetics and mechanisms of microstructure and property evolution of <span class="hlt">Fe-Cr</span> alloys under various thermal and irradiation environments</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22306293-site-preference-magnetism-lattice-vibrations-intermetallics-lufe17xtx-cr-mn-ru','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22306293-site-preference-magnetism-lattice-vibrations-intermetallics-lufe17xtx-cr-mn-ru"><span>Site preference, magnetism and lattice vibrations of intermetallics Lu₂<span class="hlt">Fe</span> 17–xT x (T=<span class="hlt">Cr</span>, Mn, Ru)</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, Jin-Chun; Qian, Ping, E-mail: qianpinghu@sohu.com; Zhang, Zhen-Feng</p> <p></p> <p>We present an atomistic study on the phase stability, site preference and lattice constants of the rare earth intermetallics Lu₂<span class="hlt">Fe</span> 17–xT x (T=<span class="hlt">Cr</span>, Mn, Ru). The calculated preferential occupation site of ternary element T is found to be the 4f site. The order of site preference is given as 4f, 12k, 12j and 6g for Lu₂<span class="hlt">Fe</span> 17–xT x. The calculated lattice parameters are corresponding to the experimental results. We have calculated the magnetic moments of Lu₂<span class="hlt">Fe</span> 17–xT x compounds. Results show that the calculated total magnetic moment of Lu₂Fe₁₇ compound is M=37.34 μ B/f.u. In addition, the total and partialmore » phonon densities of states are evaluated first for these complicated structures. - Graphical abstract: The vibrational modes are mostly excited by <span class="hlt">Fe</span> atoms, Lu contributes to the lower frequencies modes, and the contribution of Ru atoms is the same as <span class="hlt">Fe</span> atoms. Highlights: • There are no reports on lattice vibrations of Lu₂(<span class="hlt">Fe</span>, T) 17–x (T=<span class="hlt">Cr</span>, Mn, Ru) compounds. • The phase stability and site preference are evaluated first for the complex structures of Lu₂(<span class="hlt">Fe</span>, T) 17–x (T=<span class="hlt">Cr</span>, Mn, Ru) compounds. • The lattice inversion method to obtain the interatomic pair potential is the unique one.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1234450-electronic-structure-magnetism-antisite-disorder-cofecrge-comncral-quaternary-heusler-alloys','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1234450-electronic-structure-magnetism-antisite-disorder-cofecrge-comncral-quaternary-heusler-alloys"><span>Electronic structure, magnetism, and antisite disorder in Co<span class="hlt">FeCr</span>Ge and CoMn<span class="hlt">Cr</span>Al quaternary Heusler alloys</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Enamullah, .; Venkateswara, Y.; Gupta, Sachin; ...</p> <p>2015-12-10</p> <p>In this study, we present a combined theoretical and experimental study of two quaternary Heusler alloys Co<span class="hlt">FeCr</span>Ge (CFCG) and CoMn<span class="hlt">Cr</span>Al (CMCA), promising candidates for spintronics applications. Magnetization measurement shows the saturation magnetization and transition temperature to be 3 μ B, 866 K and 0.9 μ B, 358 K for CFCG and CMCA respectively. The magnetization values agree fairly well with our theoretical results and also obey the Slater-Pauling rule, a prerequisite for half metallicity. A striking difference between the two systems is their structure; CFCG crystallizes in fully ordered Y-type structure while CMCA has L2 1 disordered structure. The antisitemore » disorder adds a somewhat unique property to the second compound, which arises due to the probabilistic mutual exchange of Al positions with <span class="hlt">Cr</span>/Mn and such an effect is possibly expected due to comparable electronegativities of Al and <span class="hlt">Cr</span>/Mn. Ab initio simulation predicted a unique transition from half metallic ferromagnet to metallic antiferromagnet beyond a critical excess concentration of Al in the alloy.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1265951-influence-nanovoids-phase-separation-fecral-oxide-dispersion-strengthened-alloy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1265951-influence-nanovoids-phase-separation-fecral-oxide-dispersion-strengthened-alloy"><span>Influence of nanovoids on α-α' phase separation in <span class="hlt">FeCr</span>Al oxide dispersion strengthened alloy</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>Capdevila, Carlos; Aranda, M. M.; Rememnteria, R.</p> <p>2015-08-10</p> <p>The presence of nanovoids in the vicinity of oxide particles in <span class="hlt">FeCr</span>Al oxide dispersion strengthened (ODS) alloy has been identified. These nanovoids are inherent to the manufacturing route and remain quite resistant during heat treatments. Positron annihilation spectroscopy (PAS) experiments demonstrate that these nanovoids trap <span class="hlt">Cr</span> inside thereby reducing the <span class="hlt">Cr</span>-content in the matrix. In conclusion, this might lead to a delay in the α–α' phase separation process as observed by atom probe tomography (APT).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26942451','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26942451"><span>Ba2F2<span class="hlt">Fe</span>(1.5)Se3: An Intergrowth Compound Containing Iron Selenide <span class="hlt">Layers</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Driss, Dalel; Janod, Etienne; Corraze, Benoit; Guillot-Deudon, Catherine; Cario, Laurent</p> <p>2016-03-21</p> <p>The iron selenide compound Ba2F2<span class="hlt">Fe</span>(1.5)Se3 was synthesized by a high-temperature ceramic method. The single-crystal X-ray structure determination revealed a <span class="hlt">layered</span>-like structure built on [Ba2F2](2+) <span class="hlt">layers</span> of the fluorite type and iron selenide <span class="hlt">layers</span> [<span class="hlt">Fe</span>(1.5)Se3](2-). These [<span class="hlt">Fe</span>1.5Se3](2-) <span class="hlt">layers</span> contain iron in two valence states, namely, <span class="hlt">Fe</span>(II+) and <span class="hlt">Fe</span>(III+) located in octahedral and tetrahedral sites, respectively. Magnetic measurements are consistent with a high-spin state for <span class="hlt">Fe</span>(II+) and an intermediate-spin state for <span class="hlt">Fe</span>(III+). Moreover, susceptibility and resistivity measurements demonstrate that Ba2F2<span class="hlt">Fe</span>(1.5)Se3 is an antiferromagnetic insulator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012MSHT...54...96T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012MSHT...54...96T"><span>Effect of mechanical alloying and heat treatment on the behavior of <span class="hlt">fe</span> - 28% al - 5% <span class="hlt">cr</span> powder with nanocrystalline structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tang, W. M.; Liu, H. L.; Wang, Y. X.; Xu, G. O.; Zheng, Z. X.</p> <p>2012-05-01</p> <p>Nanocrystalline powders of alloy <span class="hlt">Fe</span> - 28% Al - 5% <span class="hlt">Cr</span> (at.%) obtained by mechanical alloying from powdered iron, aluminum, and preliminarily alloyed <span class="hlt">Fe</span> - 20% <span class="hlt">Cr</span> are studied. The chemical composition is shown to be homogenized. The changes in the structure and in the morphology of the particles in the process of ball milling and subsequent heat treatment are determined. The alloying is shown to occur by the mechanism of continuous diffusion mixing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JSSCh.237..225S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JSSCh.237..225S"><span>Design and syntheses of hybrid metal-organic materials based on K3[M(C2O4)3]·3H2O [M(III)=<span class="hlt">Fe</span>, Al, <span class="hlt">Cr</span>] metallotectons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sun, Yayong; Zong, Yingxia; Ma, Haoran; Zhang, Ao; Liu, Kang; Wang, Debao; Wang, Wenqiang; Wang, Lei</p> <p>2016-05-01</p> <p>By using K3[M(C2O4)3]·3H2O [M(III)=<span class="hlt">Fe</span>, Al, <span class="hlt">Cr</span>] (C2O42-=oxalate) metallotectons as the starting material, we have synthesized eight novel complexes with formulas [{<span class="hlt">Fe</span>(C2O4)2(H2O)2}2]·(H-L1)2·H2O 1, [<span class="hlt">Fe</span>(C2O4)Cl2]·(H2-L2)0.5·(L2)0.5·H2O 2, [{<span class="hlt">Fe</span>(C2O4)1.5Cl2}2]·(H-L3)43, [<span class="hlt">Fe</span>2(C2O4)Cl8]·(H2-L4)2·2H2O 4, K[Al(C2O4)3]·(H2-L5)·2H2O 5, K[Al(C2O4)3]·(H-L6)2·2H2O 6, K[<span class="hlt">Cr</span>(C2O4)3]·2H2O 7, Na[<span class="hlt">Fe</span>(C2O4)3]·(H-L6)2·2H2O 8 (with L1=4-dimethylaminopyridine, L2=2,3,5,6-tetramethylpyrazine, L3=2-aminobenzimidazole, L4=1,4-bis-(1H-imidazol-1-yl)benzene, L5=1,4-bis((2-methylimidazol-1-yl)methyl)benzene, L6=2-methylbenzimidazole). Their structures have been determined by single-crystal X-ray diffraction analyses, elemental analyses, IR spectra and thermogravimetric analyses. Compound 3 is a 2D H-bonded supramolecular architecture. Others are 3D supramolecular structures. Compound 1 shows a [<span class="hlt">Fe</span>(C2O4)2(H2O)2]- unit and 3D antionic H-bonded framework. Compound 2 features a [<span class="hlt">Fe</span>(C2O4)Cl2]- anion and 1D iron-oxalate-iron chain. Compound 3 features a [<span class="hlt">Fe</span>2(C2O4)3Cl4]4- unit. Compound 4 features distinct [<span class="hlt">Fe</span>2(C2O4)Cl8]4- units, which are mutual linked by water molecules to generated a 2D H-bonded network. Compound 5 features infinite ladder-like chains constructed by [Al(C2O4)3]3- units and K+ cations. The 1D chains are further extended into 3D antionic H-bonded framework through O-H···O H-bonds. Compounds 6-8 show 2D [KAl(C2O4)3]2- <span class="hlt">layer</span>, [KCr(C2O4)3]2- <span class="hlt">layer</span> and [Na<span class="hlt">Fe</span>(C2O4)3]2- <span class="hlt">layer</span>, respectively.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007PhyE...37...11A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007PhyE...37...11A"><span>Growth of carbon nanotubes by <span class="hlt">Fe</span>-catalyzed chemical vapor processes on <span class="hlt">silicon</span>-based substrates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Angelucci, Renato; Rizzoli, Rita; Vinciguerra, Vincenzo; Fortuna Bevilacqua, Maria; Guerri, Sergio; Corticelli, Franco; Passini, Mara</p> <p>2007-03-01</p> <p>In this paper, a site-selective catalytic chemical vapor deposition synthesis of carbon nanotubes on <span class="hlt">silicon</span>-based substrates has been developed in order to get horizontally oriented nanotubes for field effect transistors and other electronic devices. Properly micro-fabricated <span class="hlt">silicon</span> oxide and polysilicon structures have been used as substrates. Iron nanoparticles have been obtained both from a thin <span class="hlt">Fe</span> film evaporated by e-gun and from iron nitrate solutions accurately dispersed on the substrates. Single-walled nanotubes with diameters as small as 1 nm, bridging polysilicon and <span class="hlt">silicon</span> dioxide “pillars”, have been grown. The morphology and structure of CNTs have been characterized by SEM, AFM and Raman spectroscopy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMEP...26.2430S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMEP...26.2430S"><span>Microstructure and Mechanical Properties of <span class="hlt">Fe</span>-18Mn-18<span class="hlt">Cr</span>-0.5N Austenitic Nonmagnetic Stainless Steel in Asymmetric Hot Rolling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, Y. L.; Li, C. S.; Ma, B.; Han, Y. H.</p> <p>2017-05-01</p> <p>Asymmetric hot rolling (ASHR) with a mismatch speed ratio of 1.15 in a single pass was applied to <span class="hlt">Fe</span>-18Mn-18<span class="hlt">Cr</span>-0.5N steel and was compared with symmetric hot rolling (SHR). The results indicated that a through-thickness microstructure gradient was formed in the plate due to the shear strain (0.36) introduced by ASHR. A fine-grained <span class="hlt">layer</span> with the average size of 3 μm was achieved at the top surface of ASHR plate, while numerous elongated grains with a few recrystallized grains were presented at the center <span class="hlt">layer</span>. The texture was distributed randomly at the top surface of ASHR plate, and a weaker intensity of typical hot-rolled texture in austenitic steel was obtained at the center <span class="hlt">layer</span> of ASHR plate compared to SHR plate. An excellent combination of microhardness, strength and ductility was obtained in the ASHR plate, which was attributed to gradient microstructure induced by ASHR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AcSpe.101...46H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AcSpe.101...46H"><span>Ultrasonic slurry sampling electrothermal vaporization inductively coupled plasma mass spectrometry for the determination of <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Cu, Zn and Se in cereals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huang, Shih-Yi; Jiang, Shiuh-Jen; Sahayam, A. C.</p> <p>2014-11-01</p> <p>Ultrasonic slurry sampling electrothermal vaporization inductively coupled plasma mass spectrometry (USS-ETV-ICP-MS) has been applied to determine <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Cu, Zn and Se in several cereal samples. Thioacetamide was used as the modifier to enhance the ion signals. The background ions at the masses of interest were reduced in intensity significantly by using 1.0 mL min- 1 methane (CH4) as reaction cell gas in the dynamic reaction cell (DRC). Since the sensitivities of <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Cu, Zn and Se in different matrices were quite different, standard addition and isotope dilution methods were used for the determination of <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Cu, Zn and Se in these cereal samples. The method detection limits estimated from standard addition curves were about 1, 10, 4, 12 and 2 ng g- 1 for <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Cu, Zn and Se, respectively, in original cereal samples. This procedure has been applied to the determination of <span class="hlt">Cr</span>, <span class="hlt">Fe</span>, Cu, Zn and Se whose concentrations are in μg g- 1 (except <span class="hlt">Cr</span> and Se) in standard reference materials (SRM) of National institute of standards and technology (NIST), NIST SRM 1568a Rice Flour and NIST SRM 1567a Wheat Flour and two cereal samples purchased from a local market. The analysis results of reference materials agreed with certified values at 95% confidence level according to Student's T-test. The results for the real world cereal samples were also found to be in good agreement with the pneumatic nebulization DRC ICP-MS results of the sample solutions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1321882','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1321882"><span>Atomistic clustering-ordering and high-strain deformation of an Al 0.1<span class="hlt">CrCoFe</span>Ni high-entropy alloy</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>Sharma, Aayush; Singh, Prashant; Johnson, Duane D.</p> <p>2016-08-08</p> <p>Here, computational investigations of structural, chemical, and deformation behavior in high-entropy alloys (HEAs), which possess notable mechanical strength, have been limited due to the absence of applicable force fields. To extend investigations, we propose a set of intermolecular potential parameters for a quinary Al-<span class="hlt">Cr-Co-Fe</span>-Ni alloy, using the available ternary Embedded Atom Method and Lennard-Jones potential in classical molecular-dynamics simulations. The simulation results are validated by a comparison to first-principles Korringa-Kohn-Rostoker (KKR) - Coherent Potential Approximation (CPA) [KKR-CPA] calculations for the HEA structural properties (lattice constants and bulk moduli), relative stability, pair probabilities, and high-temperature short-range ordering. The simulation (MD)-derived propertiesmore » are in quantitative agreement with KKR-CPA calculations (first-principles) and experiments. We study Al x<span class="hlt">CrCoFe</span>Ni for Al ranging from 0 ≤ x ≤2 mole fractions, and find that the HEA shows large chemical clustering over a wide temperature range for x < 0.5. At various temperatures high-strain compression promotes atomistic rearrangements in Al 0.1<span class="hlt">CrCoFe</span>Ni, resulting in a clustering-to-ordering transition that is absent for tensile loading. Large fluctuations under stress, and at higher temperatures, are attributed to the thermo-plastic instability in Al 0.1<span class="hlt">CrCoFe</span>Ni.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4976365','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4976365"><span>Atomistic clustering-ordering and high-strain deformation of an Al0.1<span class="hlt">CrCoFe</span>Ni high-entropy alloy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sharma, Aayush; Singh, Prashant; Johnson, Duane D.; Liaw, Peter K.; Balasubramanian, Ganesh</p> <p>2016-01-01</p> <p>Computational investigations of structural, chemical, and deformation behavior in high-entropy alloys (HEAs), which possess notable mechanical strength, have been limited due to the absence of applicable force fields. To extend investigations, we propose a set of intermolecular potential parameters for a quinary Al-<span class="hlt">Cr-Co-Fe</span>-Ni alloy, using the available ternary Embedded Atom Method and Lennard-Jones potential in classical molecular-dynamics simulations. The simulation results are validated by a comparison to first-principles Korringa-Kohn-Rostoker (KKR) - Coherent Potential Approximation (CPA) [KKR-CPA] calculations for the HEA structural properties (lattice constants and bulk moduli), relative stability, pair probabilities, and high-temperature short-range ordering. The simulation (MD)-derived properties are in quantitative agreement with KKR-CPA calculations (first-principles) and experiments. We study Alx<span class="hlt">CrCoFe</span>Ni for Al ranging from 0 ≤ x ≤2 mole fractions, and find that the HEA shows large chemical clustering over a wide temperature range for x < 0.5. At various temperatures high-strain compression promotes atomistic rearrangements in Al0.1<span class="hlt">CrCoFe</span>Ni, resulting in a clustering-to-ordering transition that is absent for tensile loading. Large fluctuations under stress, and at higher temperatures, are attributed to the thermo-plastic instability in Al0.1<span class="hlt">CrCoFe</span>Ni. PMID:27498807</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22163174-twin-nucleation-migration-fecr-single-crystals','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22163174-twin-nucleation-migration-fecr-single-crystals"><span>Twin nucleation and migration in <span class="hlt">FeCr</span> single crystals</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>Patriarca, L.; Abuzaid, Wael; Sehitoglu, Huseyin, E-mail: huseyin@illinois.edu</p> <p>2013-01-15</p> <p>Tension and compression experiments were conducted on body-centered cubic <span class="hlt">Fe</span> -47.8 at pct. <span class="hlt">Cr</span> single crystals. The critical resolved shear stress (CRSS) magnitudes for slip nucleation, twin nucleation and twin migration were established. We show that the nucleation of slip occurs at a CRSS of about 88 MPa, while twinning nucleates at a CRSS of about 191 MPa with an associated load drop. Following twin nucleation, twin migration proceeds at a CRSS that is lower than the initiation stress ( Almost-Equal-To 114-153 MPa). The experimental results of the nucleation stresses indicate that the Schmid law holds to a first approximationmore » for the slip and twin nucleation cases, but to a lesser extent for twin migration particularly when considerable slip strains preceded twinning. The CRSSs were determined experimentally using digital image correlation (DIC) in conjunction with electron back scattering diffraction (EBSD). The DIC measurements enabled pinpointing the precise stress on the stress-strain curves where twins or slip were activated. The crystal orientations were obtained using EBSD and used to determine the activated twin and slip systems through trace analysis. - Highlights: Black-Right-Pointing-Pointer Digital image correlation allows to capture slip/twin initiation for bcc <span class="hlt">FeCr</span>. Black-Right-Pointing-Pointer Crystal orientations from EBSD allow slip/twin system indexing. Black-Right-Pointing-Pointer Nucleation of slip always precedes twinning. Black-Right-Pointing-Pointer Twin growth is sustained with a lower stress than required for nucleation. Black-Right-Pointing-Pointer Twin-slip interactions provide high hardening at the onset of plasticity.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JAP...116b3907B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JAP...116b3907B"><span>Iron silicide formation at different <span class="hlt">layers</span> of (<span class="hlt">Fe</span>/Si)3 multilayered structures determined by conversion electron Mössbauer spectroscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Badía-Romano, L.; Rubín, J.; Magén, C.; Bürgler, D. E.; Bartolomé, J.</p> <p>2014-07-01</p> <p>The morphology and the quantitative composition of the <span class="hlt">Fe</span>-Si interface <span class="hlt">layer</span> forming at each <span class="hlt">Fe</span> <span class="hlt">layer</span> of a (<span class="hlt">Fe</span>/Si)3 multilayer have been determined by means of conversion electron Mössbauer spectroscopy (CEMS) and high-resolution transmission electron microscopy (HRTEM). For the CEMS measurements, each <span class="hlt">layer</span> was selected by depositing the Mössbauer active 57<span class="hlt">Fe</span> isotope with 95% enrichment. Samples with <span class="hlt">Fe</span> <span class="hlt">layers</span> of nominal thickness d<span class="hlt">Fe</span> = 2.6 nm and Si spacers of dSi = 1.5 nm were prepared by thermal evaporation onto a GaAs(001) substrate with an intermediate Ag(001) buffer <span class="hlt">layer</span>. HRTEM images showed that Si <span class="hlt">layers</span> grow amorphous and the epitaxial growth of the <span class="hlt">Fe</span> is good only for the first deposited <span class="hlt">layer</span>. The CEMS spectra show that at all <span class="hlt">Fe</span>/Si and Si/<span class="hlt">Fe</span> interfaces a paramagnetic c-<span class="hlt">Fe</span>1-xSi phase is formed, which contains 16% of the nominal <span class="hlt">Fe</span> deposited in the <span class="hlt">Fe</span> <span class="hlt">layer</span>. The bottom <span class="hlt">Fe</span> <span class="hlt">layer</span>, which is in contact with the Ag buffer, also contains α-<span class="hlt">Fe</span> and an <span class="hlt">Fe</span>1-xSix alloy that cannot be attributed to a single phase. In contrast, the other two <span class="hlt">layers</span> only comprise an <span class="hlt">Fe</span>1-xSix alloy with a Si concentration of ≃0.15, but no α-<span class="hlt">Fe</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1435600-dose-dependence-radiation-damage-nano-structured-amorphous-sioc-crystalline-fe-composite','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1435600-dose-dependence-radiation-damage-nano-structured-amorphous-sioc-crystalline-fe-composite"><span>Dose dependence of radiation damage in nano-structured amorphous SiOC/crystalline <span class="hlt">Fe</span> composite</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Su, Qing; Price, Lloyd; Shao, Lin; ...</p> <p>2015-10-29</p> <p>Here, through examination of radiation tolerance properties of amorphous <span class="hlt">silicon</span> oxycarbide (SiOC) and crystalline <span class="hlt">Fe</span> composite to averaged damage levels, from approximately 8 to 30 displacements per atom (dpa), we demonstrated that the <span class="hlt">Fe</span>/SiOC interface and the <span class="hlt">Fe</span>/amorphous <span class="hlt">Fe</span> xSi yO z interface act as efficient defect sinks and promote the recombination of vacancies and interstitials. For thick <span class="hlt">Fe</span>/SiOC multilayers, a clear <span class="hlt">Fe</span>/SiOC interface remained and no irradiation-induced mixing was observed even after 32 dpa. For thin <span class="hlt">Fe</span>/SiOC multilayers, an amorphous <span class="hlt">Fe</span> xSi yO z intermixed <span class="hlt">layer</span> was observed to form at 8 dpa, but no further <span class="hlt">layer</span> growth wasmore » observed for higher dpa levels.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29256738','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29256738"><span>Retinal <span class="hlt">Layers</span> Measurements following <span class="hlt">Silicone</span> Oil Tamponade for Retinal Detachment Surgery.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jurišić, Darija; Geber, Mia Zorić; Ćavar, Ivan; Utrobičić, Dobrila Karlica</p> <p>2017-12-19</p> <p>This study aimed to investigate the influence of <span class="hlt">silicone</span> oil on the retinal nerve fiber <span class="hlt">layer</span> (RNFL) thickness in patients with primary rhegmatogenous retinal detachment who underwent vitreoretinal surgery. The study included 47 patients (eyes), who underwent a pars plana vitrectomy with the <span class="hlt">silicone</span> oil tamponade. The control group included unoperated eye of all participants. Spectral-domain optical coherence tomography (SD-OCT) was used for the measurements of peripapilar and macular RNFL thickness. The average peripapillary RNFL thickness was significantly higher in the <span class="hlt">silicone</span> oil filled eyes during endotamponade and after its removal. The eyes with elevated IOP had less thickening of the RNFL in comparison to the eyes with normal IOP. Central macular thickness and macular volume were decreased in the <span class="hlt">silicone</span> oil filled eyes in comparison to the control eyes. In conclusion, <span class="hlt">silicone</span> oil caused peripapilar RNFL thickening in the vitrectomized eyes during endotamponade and after <span class="hlt">silicone</span> oil removal.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JNuM..497...37R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JNuM..497...37R"><span>Effects of iron content in Ni-<span class="hlt">Cr-xFe</span> alloys and immersion time on the oxide films formed in a simulated PWR water environment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ru, Xiangkun; Lu, Zhanpeng; Chen, Junjie; Han, Guangdong; Zhang, Jinlong; Hu, Pengfei; Liang, Xue</p> <p>2017-12-01</p> <p>The iron content in Ni-<span class="hlt">Cr-xFe</span> (x = 0-9 at.%) alloys strongly affected the properties of oxide films after 978 h of immersion in the simulated PWR primary water environment at 310 °C. Increasing the iron content in the alloys increased the amount of iron-bearing polyhedral spinel oxide particles in the outer oxide <span class="hlt">layer</span> and increased the local oxidation penetrations into the alloy matrix from the chromium-rich inner oxide <span class="hlt">layer</span>. The effects of iron content in the alloys on the oxide film properties after 500 h of immersion were less significant than those after 978 h. Iron content increased, and chromium content decreased, in the outer oxide <span class="hlt">layer</span> with increasing iron content in the alloys. Increasing the immersion time facilitated the formation of the local oxidation penetrations along the matrix/film interface and the nickel-bearing spinel oxides in the outer oxide <span class="hlt">layer</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AIPC.1731e0016A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AIPC.1731e0016A"><span>Microstructural, optical and electrical properties of La<span class="hlt">Fe</span>0.5<span class="hlt">Cr</span>0.5O3 perovskite nanostructures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ali, S. Asad; Naseem, Swaleha; Khan, Wasi; Sharma, A.; Naqvi, A. H.</p> <p>2016-05-01</p> <p>Perovskite nanocrystalline powder of La<span class="hlt">Fe</span>0.5<span class="hlt">Cr</span>0.5O3 was synthesized by sol-gel combustion route and characterized by x-ray diffractometer (XRD), scanning electron microscopy (SEM) equipped with EDS, UV-visible and LCR meter at room temperature Rietveld refinement of the XRD data confirms that the sample is in single phase-rhombohedral structure with space group R-3C. SEM micrograph shows clear nanostructure of the sample and EDS ensures the presence of all elements in good stoichiometric. The optical absorption indicates the maximum absorption at 315 nm and optical band gap of 2.94 eV was estimated using Tauc's relation. Dielectric constant (ɛ') and loss were found to decrease with increase in frequencies. The dielectric behavior was explained on the basis of Maxwell-Wagner's two <span class="hlt">layer</span> model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22492962-magnetic-characteristics-high-layer-number-nife-femn-multilayer','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22492962-magnetic-characteristics-high-layer-number-nife-femn-multilayer"><span>Magnetic characteristics of a high-<span class="hlt">layer</span>-number Ni<span class="hlt">Fe/Fe</span>Mn multilayer</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>Paterson, G. W., E-mail: gary.paterson@glasgow.ac.uk; Gonçalves, F. J. T.; McFadzean, S.</p> <p>2015-11-28</p> <p>We report the static and dynamic magnetic characteristics of a high-<span class="hlt">layer</span>-number Ni<span class="hlt">Fe/Fe</span>Mn multilayer test structure with potential applications in broadband absorber and filter devices. To allow fine control over the absorption linewidths and to understand the mechanisms governing the resonances in a tailored structure similar to that expected to be used in real world applications, the multilayer was intentionally designed to have <span class="hlt">layer</span> thickness and interface roughness variations. Magnetometry measurements show that the sample has complex hysteresis loops with features consistent with single ferromagnetic film reversals. Characterisation by transmission electron microscopy allows us to correlate the magnetic properties with structuralmore » features, including the film widths and interface roughnesses. Analysis of resonance frequencies from broadband ferromagnetic resonance measurements as a function of field magnitude and orientation provide values of the local exchange bias, rotatable anisotropy, and uniaxial anisotropy fields for specific <span class="hlt">layers</span> in the stack and explain the observed mode softening. The linewidths of the multilayer are adjustable around the bias field, approaching twice that seen at larger fields, allowing control over the bandwidth of devices formed from the structure.« 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 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('https://www.osti.gov/servlets/purl/1237412','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1237412"><span>A defect density-based constitutive crystal plasticity framework for modeling the plastic deformation of <span class="hlt">Fe-Cr</span>-Al cladding alloys subsequent to irradiation</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>Patra, Anirban; Wen, Wei; Martinez Saez, Enrique</p> <p>2016-02-05</p> <p>It is essential to understand the deformation behavior of these <span class="hlt">Fe-Cr</span>-Al alloys, in order to be able to develop models for predicting their mechanical response under varied loading conditions. Interaction of dislocations with the radiation-induced defects governs the crystallographic deformation mechanisms. A crystal plasticity framework is employed to model these mechanisms in <span class="hlt">Fe-Cr</span>-Al alloys. This work builds on a previously developed defect density-based crystal plasticity model for bcc metals and alloys, with necessary modifications made to account for the defect substructure observed in <span class="hlt">Fe-Cr</span>-Al alloys. The model is implemented in a Visco-Plastic Self Consistent (VPSC) framework, to predict the mechanicalmore » behavior under quasi-static loading.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApSS..416..470W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApSS..416..470W"><span>Investigation into nanoscratching mechanical response of Al<span class="hlt">CrCuFe</span>Ni high-entropy alloys using atomic simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Zining; Li, Jia; Fang, QiHong; Liu, Bin; Zhang, Liangchi</p> <p>2017-09-01</p> <p>The mechanical behaviors and deformation mechanisms of scratched Al<span class="hlt">CrCuFe</span>Ni high entropy alloys (HEAs) have been studied by molecular dynamics (MD) simulations, in terms of the scratching forces, atomic strain, atomic displacement, microstructural evolution and dislocation density. The results show that the larger tangential and normal forces and higher friction coefficient take place in Al<span class="hlt">CrCuFe</span>Ni HEA due to its outstanding strength and hardness, and high adhesion and fracture toughness over the pure metal materials. Moreover, the stacking fault energy (SFE) in HEA increases the probability to initiate dislocation and twinning, which is conducive to the formation of complex deformation modes. Compared to the single element metal workpieces, the segregation potency of solutes into twinning boundary (TB) is raised due to the decreasing segregation energy of TB, resulting in the stronger solute effects on improving twinning properties for HEA workpiece. The higher dislocation density and the more activated slipping planes lead to the outstanding plasticity of Al<span class="hlt">CrCuFe</span>Ni HEA. The solute atoms as barriers to hinder the motion of dislocation and the severe lattice distortion to suppress the free slipping of dislocation are significantly stronger obstacles to strengthen HEA. The excellent comprehensive scratching properties of the bulk Al<span class="hlt">CrCuFe</span>Ni HEAs are associated with the combined effects of multiple strengthening mechanisms, such as dislocation strengthening, deformation twinning strengthening as well as solute strengthening. This work provides a basis for further understanding and tailoring SFE in mechanical properties and deformation mechanism of HEAs, which maybe facilitate the design and preparation of new HEAs with high performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22304472-epitaxial-ferromagnetic-oxide-thin-films-silicon-atomically-sharp-interfaces','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22304472-epitaxial-ferromagnetic-oxide-thin-films-silicon-atomically-sharp-interfaces"><span>Epitaxial ferromagnetic oxide thin films on <span class="hlt">silicon</span> with atomically sharp interfaces</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>Coux, P. de; CEMES-CNRS, 29 rue Jeanne Marvig, BP 94347, Toulouse Cedex 4; Bachelet, R.</p> <p></p> <p>A bottleneck in the integration of functional oxides with <span class="hlt">silicon</span>, either directly grown or using a buffer, is the usual formation of an amorphous interfacial <span class="hlt">layer</span>. Here, we demonstrate that ferromagnetic Co<span class="hlt">Fe</span>{sub 2}O{sub 4} films can be grown epitaxially on Si(111) using a Y{sub 2}O{sub 3} buffer <span class="hlt">layer</span>, and remarkably the Y{sub 2}O{sub 3}/Si(111) interface is stable and remains atomically sharp. Co<span class="hlt">Fe</span>{sub 2}O{sub 4} films present high crystal quality and high saturation magnetization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011APS..MARY26006G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011APS..MARY26006G"><span>High Resolution X-ray Scattering Studies of Structural Phase Transitions in Ba<span class="hlt">Fe</span>2-x <span class="hlt">Cr</span> x As 2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gaulin, B. D.; Clancy, J. P.; Wagman, J. J.; Sefat, A. S.</p> <p>2011-03-01</p> <p>While the effects of electron-doping on the parent compounds of the 122 family of <span class="hlt">Fe</span>-based superconductors have been extremely well-studied in recent years, far less is known about the influence of hole-doping in compounds such as Ba<span class="hlt">Fe</span> 2-x <span class="hlt">Cr</span> x As 2 . In contrast to the electron-doped 122 systems, the hole-doped compounds do not become superconducting. Furthermore, while the hole-doped compounds exhibit similar structural and magnetic phase transitions, they appear to be much less sensitive to dopant concentration. We have performed high resolution x-ray scattering and magnetic susceptibility measurements on single crystal samples of Ba<span class="hlt">Fe</span> 2-x <span class="hlt">Cr</span> x As 2 for <span class="hlt">Cr</span> concentrations ranging from 0 <= x <= 0.67 . These measurements allow us to determine the magnetic and structural phase transitions for this series and map out the low temperature phase diagram as a function of doping. In particular, we have carried out detailed measurements of the tetragonal (I4/mmm) to orthorhombic (Fmmm) structural phase transition which reveal how the orthorhombicity of the system evolves with increasing <span class="hlt">Cr</span> concentration and how this correlates with the values of Ts and Tm .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4770426','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4770426"><span>Effect of one-step recrystallization on the grain boundary evolution of Co<span class="hlt">CrFe</span>MnNi high entropy alloy and its subsystems</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chen, Bo-Ru; Yeh, An-Chou; Yeh, Jien-Wei</p> <p>2016-01-01</p> <p>In this study, the grain boundary evolution of equiatomic Co<span class="hlt">CrFe</span>MnNi, Co<span class="hlt">CrFe</span>Ni, and <span class="hlt">Fe</span>CoNi alloys after one-step recrystallization were investigated. The special boundary fraction and twin density of these alloys were evaluated by electron backscatter diffraction analysis. Among the three alloys tested, <span class="hlt">Fe</span>CoNi exhibited the highest special boundary fraction and twin density after one-step recrystallization. The special boundary increment after one-step recrystallization was mainly affected by grain boundary velocity, while twin density was mainly affected by average grain boundary energy and twin boundary energy. PMID:26923713</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26923713','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26923713"><span>Effect of one-step recrystallization on the grain boundary evolution of Co<span class="hlt">CrFe</span>MnNi high entropy alloy and its subsystems.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Bo-Ru; Yeh, An-Chou; Yeh, Jien-Wei</p> <p>2016-02-29</p> <p>In this study, the grain boundary evolution of equiatomic Co<span class="hlt">CrFe</span>MnNi, Co<span class="hlt">CrFe</span>Ni, and <span class="hlt">Fe</span>CoNi alloys after one-step recrystallization were investigated. The special boundary fraction and twin density of these alloys were evaluated by electron backscatter diffraction analysis. Among the three alloys tested, <span class="hlt">Fe</span>CoNi exhibited the highest special boundary fraction and twin density after one-step recrystallization. The special boundary increment after one-step recrystallization was mainly affected by grain boundary velocity, while twin density was mainly affected by average grain boundary energy and twin boundary energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70010960','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70010960"><span>Evidence of the impacting body of the Ries crater - the discovery of <span class="hlt">Fe-Cr</span>-Ni veinlets below the crater bottom</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>El, Goresy A.; Chao, E.C.T.</p> <p>1976-01-01</p> <p><span class="hlt">Fe-Cr</span>-Ni particles and veinlets have been discovered in the top 15 m of the compressed zone with abundant shatter cones below the bottom of the Ries crater. The metallic particles are less than a few microns across. They occur in various minerals along healed intergranular and locally in intragranular microfractures in quartz diorite, amphibolite and chloritized granite of the basement crystalline rocks. The particles consist of major <span class="hlt">Fe</span>, <span class="hlt">Cr</span>, and Ni with minor Si and Ca. Origin due to contamination is absolutely ruled out. We believe that these <span class="hlt">Fe-Cr</span>-Ni particles are probably condensed from the vaporized impacting body which produced the Ries crater. These particles were injected with high velocity into microfractures near the top of the compressed zone, implanted in and across various minerals before these microfractures were resealed. The presence of Si and Ca as well as the fact that the <span class="hlt">Cr</span> content is nearly twice that of Ni, led us to conclude that the Ries impacting body is very likely not an iron meteorite but a stony meteorite. ?? 1976.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhLB..772..599A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhLB..772..599A"><span>Enhanced collectivity along the N = Z line: Lifetime measurements in 44Ti, 48<span class="hlt">Cr</span>, and 52<span class="hlt">Fe</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arnswald, K.; Braunroth, T.; Seidlitz, M.; Coraggio, L.; Reiter, P.; Birkenbach, B.; Blazhev, A.; Dewald, A.; Fransen, C.; Fu, B.; Gargano, A.; Hess, H.; Hirsch, R.; Itaco, N.; Lenzi, S. M.; Lewandowski, L.; Litzinger, J.; Müller-Gatermann, C.; Queiser, M.; Rosiak, D.; Schneiders, D.; Siebeck, B.; Steinbach, T.; Vogt, A.; Wolf, K.; Zell, K. O.</p> <p>2017-09-01</p> <p>Lifetimes of the 21+ states in 44Ti, 48,50<span class="hlt">Cr</span>, and 52<span class="hlt">Fe</span> were determined with high accuracy exploiting the recoil distance Doppler-shift method. The reduced E2 transition strengths of 44Ti and 52<span class="hlt">Fe</span> differ considerably from previously known values. A systematic increase in collectivity is found for the N = Z nuclei compared to neighboring isotopes. The B (E2) values along the Ti, <span class="hlt">Cr</span>, and <span class="hlt">Fe</span> isotopic chains are compared to shell-model calculations employing established interactions for the 0 f 1 p shell, as well as a novel effective shell-model Hamiltonian starting from a realistic nucleon-nucleon potential. The theoretical approaches underestimate the B (E2) values for the lower-mass Ti isotopes. Strong indication is found for particle-hole cross-shell configurations, recently corroborated by similar results for the neighboring isotone 42Ca.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMMM..449..493B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMMM..449..493B"><span>First-principles study of high spin-polarization and thermoelectric efficiency of ferromagnetic Co<span class="hlt">FeCr</span>As quaternary Heusler alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bhat, Tahir Mohiuddin; Gupta, Dinesh C.</p> <p>2018-03-01</p> <p>The ground state properties along with thermodynamic and thermoelectric properties of quaternary Co<span class="hlt">FeCr</span>As alloy within the ordered LiMgPdSn-type structure have been investigated by employing first-principles calculations. The alloy offers half-metallic ferromagnet character with an indirect band gap of 1.12 eV in the minority spin state with total spin magnetic moment of 4μB and follows Slater-Pauling relation. Effects on various properties of the material has been studied by the variation of the pressure and temperature. Co<span class="hlt">FeCr</span>As tenders large value of the Grüneisen parameter and small value for the thermal expansion coefficient. The materials present high Seebeck coefficient and huge power factor with the room temperature value of ∼-40 μV/K and 18 (1014 μWcm-1 K-2 s-1) respectively, which make Co<span class="hlt">FeCr</span>As promising candidate for efficient thermoelectric material.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/350043-recent-progress-study-protective-rust-layer-formation-weathering-steel','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/350043-recent-progress-study-protective-rust-layer-formation-weathering-steel"><span>Recent progress in the study of protective rust-<span class="hlt">layer</span> formation on weathering steel</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>Yamashita, M.; Misawa, T.</p> <p></p> <p>Latest understanding of protective rust <span class="hlt">layer</span> on weathering steel and its application for structural steels is discussed. Phase transformation of the weathering steel rust <span class="hlt">layer</span> during long-time exposure brings {alpha}-(<span class="hlt">Fe</span>{sub 1{minus}x},<span class="hlt">Cr</span>{sub x})OOH, <span class="hlt">Cr</span>-substituted goethite, as the final protective rust <span class="hlt">layer</span>. It is said that the <span class="hlt">Cr</span> content in the <span class="hlt">Cr</span>-substituted goethite <span class="hlt">layer</span> increases gradiently with reaching the rust-steel interface. This increase in the <span class="hlt">Cr</span> content gives densely packed fine crystal structure end cation selective ability, which impedes the penetration of aggressive corrosives including anions such as Cl{sup {minus}} and SO{sub 4}{sup 2{minus}}. Quite recently, new surface-treatment technique employing <span class="hlt">Cr</span>{sub 2}(SO{submore » 4}){sub 3}, was proposed, which provides a possibility for obtaining the protective rust <span class="hlt">layer</span> in a relatively short period even in the severe environment such as coastal region.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JNuM..431..125C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JNuM..431..125C"><span>Impedance spectroscopy and microstructural characterization of the corrosion behavior of <span class="hlt">FeCr</span>Al alloy in lead-bismuth eutectic</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Xiang; Haasch, Rick; Stubbins, James F.</p> <p>2012-12-01</p> <p>The corrosion behavior of <span class="hlt">FeCr</span>Al alloy in Lead-Bismuth Eutectic (LBE) saturated with oxygen at 550 °C was investigated. Impedance Spectroscopy (IS) measurement was made continuously on one specimen during the entire LBE exposure test to characterize the corrosion kinetics. Various microanalysis techniques, including SEM, EDS, XRD, AES, and XPS were used to analyze the corrosion products of post-exposure specimens. It was found that a very thin, adherent alumina oxide <span class="hlt">layer</span> formed on the specimen surface and was able to protect the alloy from the corrosion attack in LBE. The thickness of the alumina surface <span class="hlt">layer</span> increased very slowly with time reaching about 837 nm in average thickness after exposure for 3600-h in LBE. The IS measurements match the microanalysis results in three respects: first, a non-zero impedance measurement agrees with the existence of a continuous surface oxide <span class="hlt">layer</span>; second, a general increase of the impedance was observed during the real-time IS measurement which means that the IS measurements reflect the growth rate of the oxide <span class="hlt">layer</span>; and third, the oxide film thickness derived from the IS data compares favorably with the SEM film thickness measurements which establishes the validity of using IS to monitor the real-time corrosion kinetics of alloys in LBE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JSSCh.212..218P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JSSCh.212..218P"><span>Magnetic and low temperature phonon studies of Co<span class="hlt">Cr</span>2O4 powders doped with <span class="hlt">Fe</span>(III) and Ni(II) ions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ptak, M.; Mączka, M.; Pikul, A.; Tomaszewski, P. E.; Hanuza, J.</p> <p>2014-04-01</p> <p>Extensive temperature-dependent phonon studies and low-temperature magnetic measurements of Co<span class="hlt">Cr</span>2-xFexO4 (for x=0.5, 1 and 2) and Co0.9Ni0.1<span class="hlt">Cr</span>2O4 polycrystalline powders are presented. The main aim of these studies was to obtain information on phonon and structural properties of these compounds as well as strength of spin-phonon coupling in the magnetically ordered phases. IR and Raman spectra show that doping of Co<span class="hlt">Cr</span>2O4 with <span class="hlt">Fe</span>(III) ions leads to broadening of bands and appearance of new bands due to the formation of inverted spinel structure. In contrast to this behavior, doping with 10 mol% of Ni(II) ions leads to weak increase of band width only. Magnetization measured as a function of temperature and external magnetic field showed that magnetic properties of Co0.9Ni0.1<span class="hlt">Cr</span>2O4 sample are similar to those reported for pure Co<span class="hlt">Cr</span>2O4, i.e., partial substitution of Ni(II) for Co(II) leads to slight shift of the ferrimagnetic phase transition at TC and spiral spin order transition at TS towards lower values. The change of crystallization preference induced by incorporation of increasing concentration of <span class="hlt">Fe</span>(III) ions in the spinel lattice causes significant increase of TC and decrease of TS. The latter transition disappears completely for higher concentrations of <span class="hlt">Fe</span>(III). The performed temperature-dependent IR studies revealed interesting anomalous behavior of phonons below TC for Co<span class="hlt">Cr</span>1.5<span class="hlt">Fe</span>0.5O4 and Co0.9Ni0.1<span class="hlt">Cr</span>2O4, which was attributed to spin-phonon coupling.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22962795','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22962795"><span>Effect of ultraviolet illumination and ambient gases on the photoluminescence and electrical properties of nanoporous <span class="hlt">silicon</span> <span class="hlt">layer</span> for organic vapor sensor.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Atiwongsangthong, Narin</p> <p>2012-08-01</p> <p>The purpose of this research, the nanoporous <span class="hlt">silicon</span> <span class="hlt">layer</span> were fabricated and investigated the physical properties such as photoluminescence and the electrical properties in order to develop organic vapor sensor by using nanoporous <span class="hlt">silicon</span>. The Changes in the photoluminescence intensity of nanoporous <span class="hlt">silicon</span> samples are studied during ultraviolet illumination in various ambient gases such as nitrogen, oxigen and vacuum. In this paper, the nanoporous <span class="hlt">silicon</span> <span class="hlt">layer</span> was used as organic vapor adsorption and sensing element. The advantage of this device are simple process compatible in <span class="hlt">silicon</span> technology and usable in room temperature. The structure of this device consists of nanoporous <span class="hlt">silicon</span> <span class="hlt">layer</span> which is formed by anodization of <span class="hlt">silicon</span> wafer in hydrofluoric acid solution and aluminum electrode which deposited on the top of nanoporous <span class="hlt">silicon</span> <span class="hlt">layer</span> by evaporator. The nanoporous <span class="hlt">silicon</span> sensors were placed in a gas chamber with various organic vapor such as ethanol, methanol and isopropyl alcohol. From studying on electrical characteristics of this device, it is found that the nanoporous <span class="hlt">silicon</span> <span class="hlt">layer</span> can detect the different organic vapor. Therefore, the nanoporous <span class="hlt">silicon</span> is important material for organic vapor sensor and it can develop to other applications about gas sensors in the future.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780016679','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780016679"><span><span class="hlt">Silicon</span> materials task of the low cost solar array project, phase 2</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hopkins, R. H.; Davis, J. R., Jr.; Blais, P. D.; Rohatgi, A.; Rai-Choudhury, P.; Hanes, M. H.; Mccormick, J. R.</p> <p>1977-01-01</p> <p>The object of phase 2 of this program is to investigate and define the effects of various processes, contaminants and process-contaminant interactions in the performance of terrestrial solar cells. The major effort this quarter was in the areas of crystal growth and thermal processing, comparison of impurity effects in low and high resistivity <span class="hlt">silicon</span>, modeling the behavior of p-type ingots containing Mo, and C and, quantitative analysis of bulk lifetime and junction degradation effects in contaminated solar cells. The performance of solar cells fabricated on <span class="hlt">silicon</span> web crystals grown from melts containing about 10 to the 18th power/cu cm of <span class="hlt">Cr</span>, Mn, <span class="hlt">Fe</span>, Ni, Ti, and V, respectively were measured. Deep level spectroscopy of metal-contaminated ingots was employed to determine the level and density of recombination centers due to Ti, V, Ni, and <span class="hlt">Cr</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1324177','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1324177"><span>Enhanced damage resistance and novel defect structure of <span class="hlt">CrFe</span>CoNi under in situ electron irradiation</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>He, Mo -Rigen; Wang, Shuai; Jin, Ke</p> <p></p> <p>Defect production and growth in <span class="hlt">CrFe</span>CoNi, a single-phase concentrated solid solution alloy, is characterized using in situ electron irradiation inside a transmission electron microscope operated at 400–1250 kV and 400 °C. All observed defects are interstitial-type, either elliptical Frank loops or polygonal (mostly rhombus) perfect loops. Both forms of loops in <span class="hlt">CrFe</span>CoNi exhibit a sublinear power law of growth that is > 40 times slower than the linear defect growth in pure Ni. Lastly, this result shows how compositional complexity impacts the production of Frenkel pairs and the agglomeration of interstitials into loops, and, thus, enhances the radiation tolerance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1324177-enhanced-damage-resistance-novel-defect-structure-crfeconi-under-situ-electron-irradiation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1324177-enhanced-damage-resistance-novel-defect-structure-crfeconi-under-situ-electron-irradiation"><span>Enhanced damage resistance and novel defect structure of <span class="hlt">CrFe</span>CoNi under in situ electron irradiation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>He, Mo -Rigen; Wang, Shuai; Jin, Ke; ...</p> <p>2016-07-25</p> <p>Defect production and growth in <span class="hlt">CrFe</span>CoNi, a single-phase concentrated solid solution alloy, is characterized using in situ electron irradiation inside a transmission electron microscope operated at 400–1250 kV and 400 °C. All observed defects are interstitial-type, either elliptical Frank loops or polygonal (mostly rhombus) perfect loops. Both forms of loops in <span class="hlt">CrFe</span>CoNi exhibit a sublinear power law of growth that is > 40 times slower than the linear defect growth in pure Ni. Lastly, this result shows how compositional complexity impacts the production of Frenkel pairs and the agglomeration of interstitials into loops, and, thus, enhances the radiation tolerance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1175464','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1175464"><span>Hafnium nitride buffer <span class="hlt">layers</span> for growth of GaN on <span class="hlt">silicon</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Armitage, Robert D.; Weber, Eicke R.</p> <p>2005-08-16</p> <p>Gallium nitride is grown by plasma-assisted molecular-beam epitaxy on (111) and (001) <span class="hlt">silicon</span> substrates using hafnium nitride buffer <span class="hlt">layers</span>. Wurtzite GaN epitaxial <span class="hlt">layers</span> are obtained on both the (111) and (001) HfN/Si surfaces, with crack-free thickness up to 1.2 {character pullout}m. However, growth on the (001) surface results in nearly stress-free films, suggesting that much thicker crack-free <span class="hlt">layers</span> could be obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22258754-influence-hydrogen-effusion-from-hydrogenated-silicon-nitride-layers-regeneration-boron-oxygen-related-defects-crystalline-silicon','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22258754-influence-hydrogen-effusion-from-hydrogenated-silicon-nitride-layers-regeneration-boron-oxygen-related-defects-crystalline-silicon"><span>Influence of hydrogen effusion from hydrogenated <span class="hlt">silicon</span> nitride <span class="hlt">layers</span> on the regeneration of boron-oxygen related defects in crystalline <span class="hlt">silicon</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>Wilking, S., E-mail: Svenja.Wilking@uni-konstanz.de; Ebert, S.; Herguth, A.</p> <p></p> <p>The degradation effect boron doped and oxygen-rich crystalline <span class="hlt">silicon</span> materials suffer from under illumination can be neutralized in hydrogenated <span class="hlt">silicon</span> by the application of a regeneration process consisting of a combination of slightly elevated temperature and carrier injection. In this paper, the influence of variations in short high temperature steps on the kinetics of the regeneration process is investigated. It is found that hotter and longer firing steps allowing an effective hydrogenation from a hydrogen-rich <span class="hlt">silicon</span> nitride passivation <span class="hlt">layer</span> result in an acceleration of the regeneration process. Additionally, a fast cool down from high temperature to around 550 °C seems tomore » be crucial for a fast regeneration process. It is suggested that high cooling rates suppress hydrogen effusion from the <span class="hlt">silicon</span> bulk in a temperature range where the hydrogenated passivation <span class="hlt">layer</span> cannot release hydrogen in considerable amounts. Thus, the hydrogen content of the <span class="hlt">silicon</span> bulk after the complete high temperature step can be increased resulting in a faster regeneration process. Hence, the data presented here back up the theory that the regeneration process might be a hydrogen passivation of boron-oxygen related defects.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/907982','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/907982"><span><span class="hlt">Silicone</span> metalization</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Maghribi, Mariam N [Livermore, CA; Krulevitch, Peter [Pleasanton, CA; Hamilton, Julie [Tracy, CA</p> <p>2006-12-05</p> <p>A system for providing metal features on <span class="hlt">silicone</span> comprising providing a <span class="hlt">silicone</span> <span class="hlt">layer</span> on a matrix and providing a metal <span class="hlt">layer</span> on the <span class="hlt">silicone</span> <span class="hlt">layer</span>. An electronic apparatus can be produced by the system. The electronic apparatus comprises a <span class="hlt">silicone</span> body and metal features on the <span class="hlt">silicone</span> body that provide an electronic device.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/958721','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/958721"><span><span class="hlt">Silicone</span> metalization</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Maghribi, Mariam N.; Krulevitch, Peter; Hamilton, Julie</p> <p>2008-12-09</p> <p>A system for providing metal features on <span class="hlt">silicone</span> comprising providing a <span class="hlt">silicone</span> <span class="hlt">layer</span> on a matrix and providing a metal <span class="hlt">layer</span> on the <span class="hlt">silicone</span> <span class="hlt">layer</span>. An electronic apparatus can be produced by the system. The electronic apparatus comprises a <span class="hlt">silicone</span> body and metal features on the <span class="hlt">silicone</span> body that provide an electronic device.</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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