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At least 667 records · Page 37

Materials Data on Ce4CdRu by Materials Project

Ce4RuCd crystallizes in the cubic F-43m space group. The structure is three-dimensional. there are three inequivalent Ce sites. In the first Ce site, Ce is bonded in a 4-coordinate geometry to two equivalent Ru and two equivalent Cd atoms. Both Ce–Ru bond lengths are 3.49 Å. Both Ce–Cd bond lengths are 3.34 Å. In the second Ce site, Ce is bonded in a distorted bent 150 degrees geometry to two equivalent Ru and two equivalent Cd atoms. Both Ce–Ru bond lengths are 2.75 Å. Both Ce–Cd bond lengths are 3.53 Å. In the third Ce site, Ce is bonded in a 3-coordinate geometry to three equivalent Ru and three equivalent Cd atoms. All Ce–Ru bond lengths are 2.92 Å. All Ce–Cd bond lengths are 3.50 Å. Ru is bonded in a 6-coordinate geometry to nine Ce atoms. Cd is bonded to nine Ce and three equivalent Cd atoms to form a mixture of face and corner-sharing CdCe9Cd3 cuboctahedra. All Cd–Cd bond lengths are 3.07 Å.

36 MATERIALS SCIENCE↗

Materials Data on Tb4MgRu by Materials Project

MgTb4Ru crystallizes in the cubic F-43m space group. The structure is three-dimensional. Mg is bonded to three equivalent Mg and nine Tb atoms to form a mixture of corner and face-sharing MgTb9Mg3 cuboctahedra. All Mg–Mg bond lengths are 3.08 Å. There are three shorter (3.34 Å) and six longer (3.58 Å) Mg–Tb bond lengths. There are three inequivalent Tb sites. In the first Tb site, Tb is bonded in a 3-coordinate geometry to three equivalent Mg and three equivalent Ru atoms. All Tb–Ru bond lengths are 2.84 Å. In the second Tb site, Tb is bonded in a bent 150 degrees geometry to two equivalent Mg and two equivalent Ru atoms. Both Tb–Ru bond lengths are 2.79 Å. In the third Tb site, Tb is bonded in a distorted rectangular see-saw-like geometry to two equivalent Mg and two equivalent Ru atoms. Both Tb–Ru bond lengths are 3.53 Å. Ru is bonded in a 6-coordinate geometry to nine Tb atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr4Fe3Si4Ru by Materials Project

Pr4RuFe3Si4 crystallizes in the tetragonal P-4m2 space group. The structure is three-dimensional. there are two inequivalent Pr sites. In the first Pr site, Pr is bonded in a 9-coordinate geometry to two equivalent Ru, two equivalent Fe, and five Si atoms. Both Pr–Ru bond lengths are 3.08 Å. Both Pr–Fe bond lengths are 3.08 Å. There are four shorter (3.13 Å) and one longer (3.67 Å) Pr–Si bond lengths. In the second Pr site, Pr is bonded in a 9-coordinate geometry to four equivalent Fe and five Si atoms. All Pr–Fe bond lengths are 3.02 Å. There are four shorter (3.12 Å) and one longer (3.68 Å) Pr–Si bond lengths. Ru is bonded in a 12-coordinate geometry to four equivalent Pr, four equivalent Fe, and four equivalent Si atoms. All Ru–Fe bond lengths are 2.93 Å. All Ru–Si bond lengths are 2.39 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded in a 8-coordinate geometry to four equivalent Pr and four equivalent Si atoms. All Fe–Si bond lengths are 2.35 Å. In the second Fe site, Fe is bonded to four equivalent Pr, four equivalent Ru, and four equivalent Si atoms to form a mixture of distorted corner and face-sharing FePr4Si4Ru4 cuboctahedra. All Fe–Si bond lengths are 2.39 Å. There are two inequivalent Si sites. In the first Si site, Si is bonded in a 9-coordinate geometry to five Pr and four equivalent Fe atoms. In the second Si site, Si is bonded in a 2-coordinate geometry to five Pr, two equivalent Ru, and two equivalent Fe atoms.

36 MATERIALS SCIENCE↗

Materials Data on Dy4MgRu by Materials Project

MgDy4Ru crystallizes in the cubic F-43m space group. The structure is three-dimensional. Mg is bonded to three equivalent Mg and nine Dy atoms to form a mixture of corner and face-sharing MgDy9Mg3 cuboctahedra. All Mg–Mg bond lengths are 3.07 Å. There are a spread of Mg–Dy bond distances ranging from 3.33–3.57 Å. There are three inequivalent Dy sites. In the first Dy site, Dy is bonded in a 3-coordinate geometry to three equivalent Mg, three equivalent Dy, and three equivalent Ru atoms. All Dy–Dy bond lengths are 3.52 Å. All Dy–Ru bond lengths are 2.83 Å. In the second Dy site, Dy is bonded in a bent 150 degrees geometry to two equivalent Mg, four equivalent Dy, and two equivalent Ru atoms. All Dy–Dy bond lengths are 3.65 Å. Both Dy–Ru bond lengths are 2.78 Å. In the third Dy site, Dy is bonded in a 4-coordinate geometry to two equivalent Mg, ten Dy, and two equivalent Ru atoms. All Dy–Dy bond lengths are 3.64 Å. Both Dy–Ru bond lengths are 3.51 Å. Ru is bonded in a 6-coordinate geometry to nine Dy atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sm4MgRu by Materials Project

MgSm4Ru crystallizes in the cubic F-43m space group. The structure is three-dimensional. Mg is bonded to three equivalent Mg and nine Sm atoms to form a mixture of corner and face-sharing MgSm9Mg3 cuboctahedra. All Mg–Mg bond lengths are 3.11 Å. There are a spread of Mg–Sm bond distances ranging from 3.39–3.63 Å. There are three inequivalent Sm sites. In the first Sm site, Sm is bonded in a 4-coordinate geometry to two equivalent Mg, ten Sm, and two equivalent Ru atoms. There are two shorter (3.57 Å) and eight longer (3.70 Å) Sm–Sm bond lengths. Both Sm–Ru bond lengths are 3.57 Å. In the second Sm site, Sm is bonded in a bent 150 degrees geometry to two equivalent Mg, four equivalent Sm, and two equivalent Ru atoms. Both Sm–Ru bond lengths are 2.82 Å. In the third Sm site, Sm is bonded in a 3-coordinate geometry to three equivalent Mg, three equivalent Sm, and three equivalent Ru atoms. All Sm–Ru bond lengths are 2.88 Å. Ru is bonded in a 6-coordinate geometry to nine Sm atoms.

36 MATERIALS SCIENCE↗

Materials Data on Pr3RuBr3 by Materials Project

Pr3RuBr3 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are three inequivalent Pr sites. In the first Pr site, Pr is bonded to two equivalent Ru and four Br atoms to form PrRu2Br4 octahedra that share corners with four equivalent PrRu3Br3 octahedra and edges with ten PrRu2Br4 octahedra. The corner-sharing octahedra tilt angles range from 2–6°. Both Pr–Ru bond lengths are 2.88 Å. There are a spread of Pr–Br bond distances ranging from 3.08–3.32 Å. In the second Pr site, Pr is bonded to three equivalent Ru and three Br atoms to form a mixture of corner and edge-sharing PrRu3Br3 octahedra. The corner-sharing octahedra tilt angles range from 0–6°. There are one shorter (2.82 Å) and two longer (2.92 Å) Pr–Ru bond lengths. There are one shorter (3.20 Å) and two longer (3.46 Å) Pr–Br bond lengths. In the third Pr site, Pr is bonded to one Ru and five Br atoms to form distorted PrRuBr5 octahedra that share corners with two equivalent PrRu3Br3 octahedra and edges with eight PrRu2Br4 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. The Pr–Ru bond length is 2.61 Å. There are a spread of Pr–Br bond distances ranging from 3.02–3.31 Å. Ru is bonded to six Pr atoms to form RuPr6 octahedra that share corners with four equivalent BrPr5 trigonal bipyramids, edges with four equivalent RuPr6 octahedra, and edges with four equivalent BrPr5 trigonal bipyramids. There are three inequivalent Br sites. In the first Br site, Br is bonded to five Pr atoms to form distorted BrPr5 trigonal bipyramids that share corners with four equivalent RuPr6 octahedra, edges with four equivalent RuPr6 octahedra, and edges with four equivalent BrPr5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 8–10°. In the second Br site, Br is bonded in a distorted see-saw-like geometry to four Pr atoms. In the third Br site, Br is bonded in a distorted T-shaped geometry to three Pr atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sc2FeB2Ru4Rh by Materials Project

Sc2Ru4FeRhB2 crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Sc is bonded in a 11-coordinate geometry to eight equivalent Ru, two equivalent Rh, and three equivalent B atoms. There are four shorter (2.83 Å) and four longer (2.94 Å) Sc–Ru bond lengths. Both Sc–Rh bond lengths are 2.77 Å. There are one shorter (2.60 Å) and two longer (2.87 Å) Sc–B bond lengths. Ru is bonded in a 8-coordinate geometry to four equivalent Sc, two equivalent Fe, and two equivalent B atoms. Both Ru–Fe bond lengths are 2.59 Å. Both Ru–B bond lengths are 2.19 Å. Fe is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. Rh is bonded in a distorted body-centered cubic geometry to four equivalent Sc and four equivalent B atoms. All Rh–B bond lengths are 2.26 Å. B is bonded in a 9-coordinate geometry to three equivalent Sc, four equivalent Ru, and two equivalent Rh atoms.

36 MATERIALS SCIENCE↗

Materials Data on Y4RuBr5 by Materials Project

Y4RuBr5 crystallizes in the tetragonal P4_2/nnm space group. The structure is three-dimensional. there are three inequivalent Y sites. In the first Y site, Y is bonded to one Ru and five Br atoms to form distorted YRuBr5 octahedra that share a cornercorner with one YRu3Br3 octahedra and edges with eight YRuBr5 octahedra. The corner-sharing octahedral tilt angles are 13°. The Y–Ru bond length is 2.72 Å. There are a spread of Y–Br bond distances ranging from 2.93–3.20 Å. In the second Y site, Y is bonded to three equivalent Ru and three Br atoms to form a mixture of edge and corner-sharing YRu3Br3 octahedra. The corner-sharing octahedra tilt angles range from 2–14°. There are two shorter (2.83 Å) and one longer (2.86 Å) Y–Ru bond lengths. There are one shorter (3.06 Å) and two longer (3.20 Å) Y–Br bond lengths. In the third Y site, Y is bonded to one Ru and five Br atoms to form distorted YRuBr5 octahedra that share corners with three YRu3Br3 octahedra and edges with eight YRuBr5 octahedra. The corner-sharing octahedra tilt angles range from 2–14°. The Y–Ru bond length is 2.69 Å. There are a spread of Y–Br bond distances ranging from 2.91–3.24 Å. Ru is bonded to six Y atoms to form edge-sharing RuY6 octahedra. There are four inequivalent Br sites. In the first Br site, Br is bonded in a 3-coordinate geometry to three Y atoms. In the second Br site, Br is bonded in a distorted see-saw-like geometry to four Y atoms. In the third Br site, Br is bonded in a distorted see-saw-like geometry to four Y atoms. In the fourth Br site, Br is bonded in a 3-coordinate geometry to three Y atoms.

36 MATERIALS SCIENCE↗

Materials Data on Mn2GeRu by Materials Project

Mn2RuGe crystallizes in the cubic F-43m space group. The structure is three-dimensional. there are two inequivalent Mn sites. In the first Mn site, Mn is bonded to four equivalent Mn and four equivalent Ru atoms to form distorted MnMn4Ru4 tetrahedra that share corners with twelve equivalent MnMn4Ge4Ru6 tetrahedra, edges with twelve equivalent MnMn4Ru4 tetrahedra, and faces with four equivalent MnMn4Ge4Ru6 tetrahedra. All Mn–Mn bond lengths are 2.56 Å. All Mn–Ru bond lengths are 2.56 Å. In the second Mn site, Mn is bonded to four equivalent Mn, six equivalent Ru, and four equivalent Ge atoms to form distorted MnMn4Ge4Ru6 tetrahedra that share corners with eighteen MnMn4Ru4 tetrahedra and faces with sixteen MnMn4Ge4Ru6 tetrahedra. All Mn–Ru bond lengths are 2.95 Å. All Mn–Ge bond lengths are 2.56 Å. Ru is bonded in a distorted body-centered cubic geometry to ten Mn and four equivalent Ge atoms. All Ru–Ge bond lengths are 2.56 Å. Ge is bonded in a distorted body-centered cubic geometry to four equivalent Mn and four equivalent Ru atoms.

36 MATERIALS SCIENCE↗

Spectroscopic and Theoretical Studies of Ruthenium Complexes with a Noninnocent N 2 S 2 Ligand in Different Redox States

Herein we report an electronic structure investigation of neutral and oxidized Ru complexes containing a redox noninnocent N 2 S 2 ligand derived from o-phenylenediamide (L1). UV–vis spectroelectrochemistry (SEC) studies were conducted on the square pyramidal complex [Ru I I(L1)(PPh 3 )] (1) and the six-coordinate complexes [Ru I I(μ-BH 3 )(L1)(PPh 3 )] (2) – which has BH 3 bound in a metal–ligand cooperative (MLC) fashion across Ru and L1 – and [Ru II (L1)(PPh 3 )(MeCN)] (3). The SEC results yielded spectra assigned to singly and doubly oxidized 1 and 3, revealing electronic structure changes as a function of oxidation state and in response to the presence and absence of bound MeCN. By contrast, the SEC results of 2 showed that it rapidly loses MLC-bound BH 3 upon oxidation. The SEC results for 1 and 3 were compared to single-crystal XRD data and UV–vis, EPR, and P K-edge, S K-edge, and Ru L 3 -edge X-ray absorption spectroscopy (XAS) data collected on isolated samples of chemically oxidized 3. The data revealed that the first two oxidations are primarily localized on the ligand, which was supported by DFT and TDDFT calculations. DFT calculations for the doubly oxidized species revealed a singlet ground state with a singlet–triplet gap of 8.9 kcal/mol. CASPT2 calculations corroborated the DFT calculations and further revealed that the singlet ground state is multiconfigurational with 21% radical character. Collectively, the results establish redox formalisms and the underlying electronic structure of Ru complexes containing a noninnocent tetradentate ligand in different oxidation states.

electronic structure↗

Photochemical CO 2 Reduction by a Postsynthetically Modified Zr-MOF

Metal–organic frameworks are an excellent platform for photochemical CO 2 reduction into valuable chemicals. Herein, we report the synthesis and photocatalytic behavior of Ru@MOF-808, a Zr-based MOF, modified with a Ru-polypyridyl complex. The postsynthetic modification was achieved using solvent-assisted incorporation of bipyridine–carboxylate ligands onto the nodes of the MOF-808, followed by the coordination of Ru­(II)-terpyridine moiety. A thorough characterization including 1 H NMR, diffuse reflectance UV/vis, X-ray absorption spectroscopy and gas adsorption studies, combined with DFT calculations, provides strong support for efficient incorporation of the molecular Ru-complex at the loading of one Ru center per node. In the presence of a strong sacrificial reductant BIH, Ru@MOF-808 was found to catalyze the photochemical reduction of CO 2 into a mixture of CO and formate ion. When compared to the homogeneous model catalyst Ru­(tpy)­(bpy) 2+ , Ru@MOF-808 was found to exhibit higher formate yields. Additionally, to explain these formate enhancements, we propose a mechanism that involves CO 2 capture at the MOF nodes to form Zr-bicarbonate species, which further react in a hydride transfer reaction with photogenerated Ru–H donor, thereby outperforming molecular catalysts in HCOO – production. Overall, the results presented in this work indicate the potential of Zr-based MOFs in integrating CO 2 capture with its photochemical conversion to desired products.

CO2 reduction↗

Oxygen Atom Transfer as an Alternative Pathway for Oxygen–Oxygen Bond Formation

Fundamental understanding of catalytic mechanisms of water oxidation is a prerequisite for the design and development of efficient and rugged water oxidation catalysts. In this work, a detailed mechanistic study of the water oxidation mechanism of the [Ru II (npm)(4-pic) 2 (H 2 O)] 2+ (npm = 4-t-butyl-2,6-di(1',8'-naphthyrid-2'-yl)-pyridine, pic = 4-picoline) complex, [Ru II –OH 2 ] 2+ , reveals oxygen atom transfer from highly reactive ruthenium oxo intermediates to noncoordinating nitrogen atoms of the ligand as a novel route for oxygen evolution via storage of oxidizing equivalents as N-oxide groups on the ligand framework. Theoretical calculations show that the initial complex, [RuII–OH 2 ] 2+ , is transformed to a di-N-oxide [Ru II –OH 2 ,(-NO) 2 ] 2+ complex upon oxidation via facile OAT steps from Ru V =O species and that [Ru V =O,(-NO) 2 ] 3+ represents the most likely reactive species for the critical O–O bond formation. Furthermore, a new stepwise mechanism for oxygen evolution is introduced, which proceeds via coupling of Ru–O and N–O moieties producing a peroxide intermediate, [Ru V –OO–N,(-NO)] 3+ , and can compete with the water nucleophilic attack pathway for the oxygen evolution reaction. In this mechanism, a water molecule is oxidatively activated to an “oxygen atom” which is “stored” at a noncoordinating pyridine. Oxidative activation of a second water molecule, facilitated by coordination expansion of the intermediate N-oxide, generates the second oxygen atom required to produce a dioxygen molecule.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Hybrid Quantum Mechanical, Molecular Mechanical, and Machine Learning Potential for Computing Aqueous-Phase Adsorption Free Energies on Metal Surfaces

Performing reliable computer simulations of elementary processes occurring at metal–water interfaces is pivotal for novel catalyst design in sustainable energy applications. Computational catalyst design hinges on the ability to reliably and efficiently compute the potential energy surface (PES) of the system. Here, due to the large system sizes needed for studying processes at liquid water–metal interfaces, these systems can currently not be described using density functional theory (DFT). In this work, we used a hybrid quantum mechanical, molecular mechanical, and machine learning potential for studying the adsorption behavior of phenol, atomic hydrogen, 2-butanol, and 2-butanone on the (0001) facet of Ru under reducing conditions when Ru is not oxidized. Specifically, we describe the adsorbate and the surrounding metal atoms at the DFT level of theory. Here, we also considered the electrostatic field effect of the water molecules on adsorbate–metal interactions. Next, for the water–water and water–adsorbate interactions, we used established classical force fields. Finally, for the water–Ru surface interaction, for which no reliable force fields have been published, we used Behler–Parrinello high-dimensional neural network potentials (HDNNPs). Employing this setup, we used our explicit solvation for metal surface (eSMS) approach to compute the aqueous-phase effect on the low-coverage adsorption of selected molecules and atoms on the (0001) facet of Ru. In agreement with previous experimental and computational studies of oxygenated molecules over transition metal facets, we found that liquid water destabilizes the tested adsorbates on Ru(0001). Interestingly, our findings indicate that adsorbates on Ru are less affected by the presence of an aqueous phase than on other transition metals (e.g., Pt), highlighting the necessity of experimental investigations of Ru-based catalytic systems in liquid water.

Adsorption↗

Atomic Layer Deposition of Ruthenium Films Using Ruthenium Diketonates and O 2 , H 2 , or N 2 O: The Role of Ruthenium Etching

In this work, the evolution of the surface during the steps that comprise the atomic layer deposition (ALD) of ruthenium films on a nickel substrate using tris(2,2,6,6-tetramethyl-3,5-heptanedionato)ruthenium(III) (Ru(tmhd) 3 ) and molecular oxygen was characterized using a combination of X-ray photoelectron (XPS) and reflection–absorption infrared (RAIRS) spectroscopies. The uptake of the Ru metalorganic precursor was determined to be activated, involving the average loss of two out of the three ligands (and the retention of the third, in molecular form, at the surface–vacuum interface), and self-limited, as required in ALD. The reaction of the resulting layer from that first half of the ALD cycle with O 2 proved to be more complex: in addition to the desired removal of the carbon-containing material, the Ni substrate becomes oxidized, and some Ru is etched away in the form of the volatile RuO 4 gas. By testing different combinations of exposures and temperatures it was determined that Ru film growth was possible, but tuning and optimizing the ALD or atomic layer etching (ALE) process conditions for maximum film growth or removal rate per cycle proved difficult. Replacing O 2 with H 2 was shown not to be viable either, as such an agent can reduce the nickel oxide formed after O 2 treatments (in fact, Ru(tmhd) 3 can do this as well) but not remove the carbonaceous material deposited on the surface by the Ru precursor. The use of N 2 O, on the other hand, showed much promise, being capable of removing most of the surface carbon without affecting the Ru film or the Ni substrate.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

A Mesopore-Confined and Graphene Oxide-Localized Ruthenium Catalyst Increases Rates of Mid-Chain Polyolefin Hydrogenolysis

A catalyst architecture with mesoporous silica coating Ru nanoparticles on reduced graphene oxide (mSiO 2 /Ru/rGO) localizes the 2 nm Ru solely at the closed bottoms of 2.9 nm diameter mesopores. mSiO 2 /Ru/rGO catalyzes the rapid, selective hydrogenolysis of polyolefins at wax formation rates (ν wax ) up to 1700 g wax ·g Ru –1 ·h –1 and a turnover frequency (TOF) for C–C bond cleavage of 130 ± 8 min –1 . The ν wax and TOF for mSiO 2 /Ru/rGO are 23× and 16× those of nonporous Ru/rGO, respectively, indicating that faster chain cleavage is also more selective inside mesopores. The methane yield from mSiO 2 /Ru/rGO is ca. 30% of the value obtained from Ru/rGO. Methane decreases, and wax selectivity improves with narrow-pore (2.3 nm) mSiO 2 /Ru/rGO. The reaction rate decreases at lower and higher H 2 pressures from its maximum at 37 bar. Log(TOF)-log(P H2 ) plots reveal rates ∝ [P H2 ] 2.8 or [P H2 ] −2.0 in the lower or higher pressure ranges, respectively. Corresponding plots for Ru/C give rates ∝ [P H2 ] 1 or [P H2 ] −2.4 . Ru is hydrocarbon-covered at low pressure; thus, the higher H 2 order for mSiO 2 /Ru/rGO indicates that mesopores increase the density of cleavable unsaturated moieties on the Ru surface. The lower H 2 order on Ru/C implies a lower density of cleavable groups because saturated segments occupy a larger fraction of the Ru surface. Higher surface occupancy by the hydrocarbon reactant correlates with more methane formation. Therefore, pore confinement, narrower pore diameter in mSiO 2 /Ru/rGO, or higher H 2 pressure leads to lower methane yields. Ru nanoparticles in mSiO 2 /Ru/rGO maintain equivalent activity and selectivity over five recycling tests.

Catalysts↗

Mechanisms of Retention and Transport of Fission Products in Virgin and Irradiated Nuclear Graphite

To fulfill the design and licensing requirements for advanced reactors, the U.S. Department of Energy (DOE) is specifically interested in targeted research to quantify the mechanisms of fission product transport and retention in graphitic grades that will likely be used in next-generation very/high temperature reactors, fluoride salt-cooled high temperature reactors and molten salt reactors. We have examined an integrated experimental-computational approach to determine the diffusivities of selected fission products – ruthenium (Ru) and silver (Ag) in five nuclear graphite grades – POCO AXF-5Q, POCO ZXF-5Q, PCEA, IG110, and NBG-18. Experimental investigation for diffusion of other fission products (iodine, cesium, and krypton) in graphite could not be carried out due to extreme evaporation due to high vapor pressure, despite several attempts incorporating various experimental schemes. Experimental investigation with irradiated graphite could not be carried out because necessary approval to transport irradiated graphite could not be obtained due to procedural reasons at ORNL and national policy change in UK. An effort was made to “produce” by ion sputtering, but it was discontinued because the outcome did not adequately represent irradiated graphite. Thin film and “cup-and-cap” methods were employed to deposit fission products, diffusion annealed were carried out in an argon atmosphere, and concentration profiles were determined by dynamic secondary ion mass spectroscopy depth profiling technique. Regardless of graphite type, anomalous diffusion behavior of Ru (i.e., lower than expected based on Arrhenius temperature dependence) at an intermediate temperature, around 600 to 700 °C, was observed. Diffusion behavior of silver on the other hand agreed well to the Arrhenius temperature dependence although the excessive evaporation of silver hampered the accurate determination of diffusivities at temperature higher than 900 °C. In general, silver was observed to diffuse faster than Ru in the temperature range compared from 500 to 900 °C, had consistently had higher pre-exponential factor corresponding to higher jump frequency. To understand the abnormal diffusional behavior of Ru in graphite in intermediate temperature range, a detailed microstructural analysis was carried out. Clustering of Ru into particles on the surface of graphite was observed around 700 °C corresponding to de-wetting and spheroidization. This change would influence the boundary condition of diffusion, although features of clustering was much smaller (<1 mm) than the SIMS raster size (120 x 120 mm). Raman spectroscopy also demonstrated that Raman peak intensity for Ru decreased significantly for samples annealed higher than 700 °C and presence of Ru in graphite altered the crystallinity of graphite. To further elucidate the abnormal diffusion behavior observed in intermediate temperature investigated, the vibrational properties of graphene, bilayer graphene and Kr atoms in bilayer graphene were investigated with molecular dynamics. Krypton, which is a fission product, was introduced between a bilayer graphene system to evaluate (i) whether the phonon dispersion curves change with high temperature in bilayer graphene (ii) whether the addition of Kr atoms between the bilayer introduces any significant change in the vibrational properties, and (iii) whether any change in the vibrational properties can be correlated to the diffusive behavior of Kr atoms. The results show that the Kr atoms indeed exhibit an anomalous diffusive behavior at 550°C. Phonon analysis shows that a few phonon frequencies are enhanced as much as 20 to 30 % with the addition of just 0.2 at.% Kr. So, this may explain the unexpected self-diffusivity of fission products.

11 NUCLEAR FUEL CYCLE AND FUEL MATERIALS↗

Trace element geochemistry and the early lunar differentiation

The results are considered of experiments in which thermal neutron activation analysis was used to measure the halogens, U, Te, Ru, Os, and Hg in lunar samples. A calorimetric method was used for P2O5. Three Apollo 17 basalts, one Apollo 11 basalt, and one Apollo 15 basalt were used for the Ru-Os study. Os and Ru were measured in seven samples of breccia 14305 in a series of experiments to check an apparent anomaly in the isotopic composition of the Hg which it contains. A lunar model for Ru-Os partition is discussed. It is suggested that Ru and Os were partitioned and fractionated in the original differentiation of the lunar surface ocean. Fractionation among near-surface materials was less than a factor of 2 according to the lithic breccia data. Fractionations among basaltic sources were very large, exceeding 100, and primarily due to Ru. A clue to Ru and Os distributions at the depths from which mare basalts were derived may be provided by the relative ages of the basalts. These are interpreted as being related to partial melting in response to temperature increases at depth with time.

Jovanovic, S.↗

Materials Data on MnAsRu by Materials Project

MnRuAs crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Mn is bonded in a 11-coordinate geometry to six equivalent Ru and five As atoms. There are two shorter (2.86 Å) and four longer (2.94 Å) Mn–Ru bond lengths. There are one shorter (2.65 Å) and four longer (2.69 Å) Mn–As bond lengths. Ru is bonded in a 10-coordinate geometry to six equivalent Mn and four As atoms. All Ru–As bond lengths are 2.47 Å. There are two inequivalent As sites. In the first As site, As is bonded in a 9-coordinate geometry to six equivalent Mn and three equivalent Ru atoms. In the second As site, As is bonded in a 9-coordinate geometry to three equivalent Mn and six equivalent Ru atoms.

36 MATERIALS SCIENCE↗