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Materials Data on HfGeOs by Materials Project

HfOsGe crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Hf is bonded in a 11-coordinate geometry to six equivalent Os and five Ge atoms. There are two shorter (2.96 Å) and four longer (3.10 Å) Hf–Os bond lengths. There are four shorter (2.78 Å) and one longer (2.81 Å) Hf–Ge bond lengths. Os is bonded in a 12-coordinate geometry to six equivalent Hf, two equivalent Os, and four Ge atoms. Both Os–Os bond lengths are 2.87 Å. There are two shorter (2.53 Å) and two longer (2.59 Å) Os–Ge bond lengths. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to six equivalent Hf and three equivalent Os atoms. In the second Ge site, Ge is bonded in a 9-coordinate geometry to three equivalent Hf and six equivalent Os atoms.

36 MATERIALS SCIENCE↗

Materials Data on Os2Xe(O3F5)2 by Materials Project

XeF5Os2O6F5 crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four Os2O6F5 clusters and four XeF5 clusters. In each Os2O6F5 cluster, Os is bonded to three O and three F atoms to form distorted corner-sharing OsO3F3 octahedra. The corner-sharing octahedral tilt angles are 24°. There is two shorter (1.71 Å) and one longer (1.72 Å) Os–O bond length. There are a spread of Os–F bond distances ranging from 2.00–2.17 Å. There are three inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Os atom. In the second O site, O is bonded in a single-bond geometry to one Os atom. In the third O site, O is bonded in a single-bond geometry to one Os atom. There are three inequivalent F sites. In the first F site, F is bonded in a bent 150 degrees geometry to two equivalent Os atoms. In the second F site, F is bonded in a single-bond geometry to one Os atom. In the third F site, F is bonded in a single-bond geometry to one Os atom. In each XeF5 cluster, Xe is bonded in a distorted square pyramidal geometry to five F atoms. There is three shorter (1.98 Å) and two longer (1.99 Å) Xe–F bond length. There are four inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Xe atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom. In the fourth F site, F is bonded in a single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Materials Data on Nd(Al5Os)2 by Materials Project

Nd(OsAl5)2 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Nd is bonded in a 10-coordinate geometry to four equivalent Os and sixteen Al atoms. All Nd–Os bond lengths are 3.49 Å. There are a spread of Nd–Al bond distances ranging from 3.19–3.70 Å. Os is bonded in a 10-coordinate geometry to two equivalent Nd and ten Al atoms. There are a spread of Os–Al bond distances ranging from 2.58–2.77 Å. There are five inequivalent Al sites. In the first Al site, Al is bonded in a 2-coordinate geometry to one Nd and two equivalent Os atoms. In the second Al site, Al is bonded in a distorted linear geometry to two equivalent Nd and two equivalent Os atoms. In the third Al site, Al is bonded in a 2-coordinate geometry to two equivalent Nd and two equivalent Os atoms. In the fourth Al site, Al is bonded in a distorted bent 120 degrees geometry to two equivalent Nd and two equivalent Os atoms. In the fifth Al site, Al is bonded in a 2-coordinate geometry to one Nd and two equivalent Os atoms.

36 MATERIALS SCIENCE↗

Artificial Neural Network Models for Octane Number and Octane Sensitivity: A Quantitative Structure Property Relationship Approach to Fuel Design

Octane sensitivity (OS), defined as the research octane number (RON) minus the motor octane number (MON) of a fuel, has gained interest among researchers due to its effect on knocking conditions in internal combustion engines. Compounds with a high OS enable higher efficiencies, especially within advanced compression ignition engines. RON/MON must be experimentally tested to determine OS, requiring time, funding, and specialized equipment. Thus, predictive models trained with existing experimental data and molecular descriptors (via quantitative structure-property relationships (QSPRs)) would allow for the preemptive screening of compounds prior to performing these experiments. Here, the present work proposes two methods for predicting the OS of a given compound: using artificial neural networks (ANNs) trained with QSPR descriptors to predict RON and MON individually to compute OS (derived octane sensitivity (dOS)), and using ANNs trained with QSPR descriptors to directly predict OS. Twenty-five ANNs were trained for both RON and MON and their test sets achieved an overall 6.4% and 5.2% error, respectively. Twenty-five additional ANNs were trained for both dOS and OS; dOS calculations were found to have 15.3% error while predicting OS directly resulted in 9.9% error. A chemical analysis of the top QSPR descriptors for RON/MON and OS is conducted, highlighting desirable structural features for high-performing molecules and offering insight into the inner mathematical workings of ANNs; such chemical interpretations study the interconnections between structural features, descriptors, and fuel performance showing that connectivity, structural diversity, and atomic hybridization consistently drive fuel performance.

09 BIOMASS FUELS↗

The causes for geographical variations in OS187/OS186 at the Cretaceous-Tertiary boundary

Researchers at Yale has approached the problem of the osmium isotopic composition of marine deposits formed in contact with both oxidized and reduced bottom waters. The measured (187) Os/(186) Os ratios of modern bulk sediment can be explained using mixing equations involving continental detrital, volcaniclastic, cosmogenic and hydrogeneous components. These studies show that sediments deposited under reducing marine conditions contain a hydrogenous component which is enriched in Re and has a radiogenic (187) Os/(186) Os ratio. The presence of such a hydrogenous component in the marine fish clay at Stevns Klint can account for the elevation of its (187) Os/(186) Os ration above the expected meteoritic value. Mass balance considerations require the Re/Os ratio of the phase precipitated from the terminal Cretaceous sea at Stevns Klint to have been about one tenth the value observed in contemporary deposits in the Black Sea, assuming Re has not been lost (or Os gained) subsequent to precipitation. In continental sections, the elevation of the (187) Os/(186) Os ratio in boundary layers may be due to precipitation from continental waters of crustally-derived radiogenic osmium either contemporaneous with the meteoritic (or mantle) osmium deposition or later during diagenesis.

Turekian, K. K.↗

Highly Siderophile Elements as Tracers for the Subcontinental Mantle Evolution Beneath the Southwestern USA: The San Carlos and Kilbourne Hole Peridotite Xenoliths Revisited

Peridotite xenoliths from San Carlos, Arizona, and Kilbourne Hole, New Mexico, have been studied since the 1970 s to give insights into melting and metasomatism in the subcontinental mantle beneath the southwestern USA. More recently, the highly siderophile elements (HSE; Os, Ir, Ru, Rh, Pt, Pd, and Re) and the included Re-Os isotope system have been established as powerful tools for the study of mantle processes because of their range in compatibility during mantle melting and their siderophile and chalcophile geochemical behavior. Model aluminachron Re-Os ages for San Carlos and Kilbourne Hole, as well as for the nearby Dish Hill and Vulcan's Throne sites, give consistent depletion ages of around 2.2 Ga. This age can be interpreted as a single large scale mantle melting event linked to crustal formation and continental growth under the southwestern USA. Highly siderophile elements, however, may be added to depleted peridotites via melt-rock interaction, especially the more incompatible and hence mobile Pt, Pd, and Re. This may result in overprinting of the signature of melt extraction, thus abating the usefulness of Re-Os mantle extraction model ages. A comprehensive characterization of the suite of mantle xenoliths from the SW USA in terms of HSE concentrations is thus necessary to re-assess the Re-Os system for dating purposes. San Carlos peridotites are depleted to moderately fertile, as indicated by their bulk Al2O3 contents between 0.66 wt% and 3.13 wt%. Bulk Os-187/Os-188 in San Carlos peridotites range from 0.1206 to 0.1357. In contrast, Kilbourne Hole peridotites tend to be more fertile with Al2O3 between 2.11 and 3.78 wt%, excluding one extremely depleted sample with 0.30 wt% Al2O3, and have Os-187/Os-188 between 0.1156 and 0.1272, typical for mantle peridotites. No large fractionation between the more compatible HSE Os, Ir, and Ru are observed. The more incompatible HSE Re, Pd, and to a minor extent, Pt, however, are depleted in a number of samples by factors of up to 4 for Pt, 6 for Pd, and 20 for Re, compared to primitive mantle estimates. This is in agreement with previous studies from the same locales, which demonstrated the presence of different populations of mantle xenoliths having undergone various degrees of melt extraction. The depletion of the more incompatible elements (Re, Pd, and Pt) also suggests that the HSE budgets of the SW USA peridotites were primarily established by extraction of basaltic melt, and reflect only minor influence from later episodes of metasomatism. Model Re-Os ages obtained from San Carlos and Kilbourne Hole xenoliths may thus reflect ages of crustal formation and mantle depletion in the SW USA region.

vanAcken, D.↗

A Transmission Electron Microscopy Study of a Refractory Metal Grain from a Calcium-Aluminum-Rich Inclusion in the Leoville CV3 Chondrite

Introduction: Calcium-aluminum-rich inclusions (CAIs) are an important component of chondritic meteorites. They can contain materials that are thermodynamically predicted and isotopically age dated to be among the first-formed solids in our solar system [1-5]. Observed in some CAIs are micron to sub-micron sized inclusions rich in Fe, Ni, and high-Z elements such as Pt, Os, Ir and W, in the form of refractory metal nuggets (RMNs), fremdlinges, and ‘nugget like objects’ (NLOs) [1,6]. Refractory siderophile elements such as Os, Ir and Ru are thermodynamically predicted to condense at temperatures well in excess of the major CAI phases such as melilite, perovskite, spinel and hibonite [2,7-9]. These refractory metal inclusions in CAIs can therefore serve as probes into the thermodynamic landscape of the early solar protoplanetary disk. Here we report on a refractory grain identified in a CAI of the Leoville CV3 chondrite. This work is part of an ongoing effort to gain insight into the thermochemistry of the early solar system through systematic analyses of the structure and chemistry of various components in CAIs [10-13]. Sample and Analytical Techniques: A fluffy type A CAI (Fig. 1A) was identified in a section of the Leoville, CV3 chondrite (Center for Meteorite Studies, Arizona State University collection, #821_C_3) using a JOEL-JXA 8530F electron microprobe at Arizona State University. Backscattered electron (BSE) imaging and energy-dispersive X-ray spectroscopy (EDS) were used to identify refractory metal grains in the CAI using a Thermo Fisher (formerly FEI) Helios NanoLab 660 G3 focused-ion-beam scanning-electron microscope (FIBSEM) located at the Kuiper Materials Imaging and Characterization Facility (KMICF) at the Lunar and Planetary Laboratory, University of Arizona. The FIB is equipped with an EDAX EDS system. We selected one of the larger (micron-sized) refractory metal grains, designated as ‘Spud’ (Fig. 1B) for further analysis. ‘Spud’ was extracted and thinned to electron transparency (<100 nm) using the FIB-SEM located in KMICF, following methods described by [14- 15]. The FIB section was analyzed using a 200 keV Hitachi HF5000 scanning transmission electron microscope (S/TEM) located at KMICF. The HF5000 is equipped with cold-field emission gun, 3rd-order spherical aberration corrector for STEM imaging, and an Oxford Instruments X-Max N 100 TLE energydispersive spectroscopy (EDS) system with dual 100 mm2 windowless silicon-drift detectors (Ω = 2.0 sr). Selected-area electron-diffraction (SAED) patterns were acquired to aid in determination of crystallinity and phase. Results: The mineralogy, texture, and morphology of the CAI are consistent with that of a fluffy type A (FTA) CAI [16]. BSE imaging at high magnifications revealed grains with high contrast, indicative of compositions rich in elements of higher atomic number relative to surrounding material. These high-Z grains have sizes that range from ∼250 nm to 4 µm. EDS analyses confirm that the bright grains are metal-rich inclusions. A minor fraction of the grains are composed of only Fe and Ni, but the majority (∼60%) of the identified inclusions also contained various refractory siderophiles including Os, Ru, Zr, Ir and Mo. EDS analysis on the FIB-SEM of Spud shows that it contains Fe, Ni, Mo and Ru. High-angle annular dark-field (HAAFD) imaging and EDS mapping in the TEM (Fig. 2) show that Spud occurs in melilite (Ca1.9Al1.99Si1.06O7). Spud contains a subhedral to anhedral morphology and is compositionally heterogenous (polyphasic, Fig. 2). Local spatial correlation occurs among Fe, Ni, and Pt, and also among Os, Ru, and Mo. SAED patterns show that the Fe-Ni-Pt, Fe-Os-Mo-Ru and Fe-Pt regions are crystalline. Discussion: CAIs can contain various types of inclusions rich in Fe, Ni and refractory siderophiles such as Os, Ru, W and Pt [1]. RMNs are micron-sized, single phase alloy grains and can contain Os, Ir, Ru and Rh [1,7,17]. NLOs are also micron-sized inclusions, but contain two phases, a refractory metal, and an oxide [6]. Fremdlinge are the largest of such inclusions (tens of microns in size) and are complex aggregates of Fe-Ni alloy, silicates, oxides, and sulfides [1,17]. While the size of Spud matches previous descriptions of RMNs and NLOs, Spud is neither a single-phase alloy like RMNs, nor does it contain one metal phase and one oxide like NLOs. Spud does not match the above described categories of refractory metal inclusions. The presence of refractory siderophiles such as Mo, Os, Ru, and Pt suggests a high-temperature origin. Thermodynamic modelling by [7] indicates condensation temperatures of 1917 K, 1693 K, 1613 K and 1415 K for Os, Mo, Ru and Pt respectively. These models also show that following the initial condensation of a refractory metal, alloying of solutes such as Fe, Ni and W, occurs in levels proportional to their partial pressures in the surrounding gas. Such alloying occurs at temperatures above the condensation temperatures of common CAI phases such as melilite (1529 K), perovskite (1441 K), spinel (197 K) and forsterite (1354 K) [2]. The polyphasic nature of Spud could be the result of such high-temperature alloying, possibly shortly after the condensation of Mo and Ru at 1693 K and 1613 K respectively. That Spud occurs as an inclusion is consistent with it having formed prior to and at temperature above that of its host melilite in this FTA CAI, which is qualitatively consistent with such prior thermodynamic modeling. Further, the polyphasic nature of Spud is similar to refractory grains from a FTA CAI in the Northwest Africa (NWA) 8323, CV3 chondrite [11-13]. These data suggest that such refractory metal grains could have been widespread in the inner and early solar protoplanetary disk and represent some of the earliest formed solids to have condensed. Acknowledgments: Research and instrumentation supported by NASA grants #NNX12AL47G, #NNX15AJ22G and #80NSSC19K0509, and NSF grants #1531243 and #0619599. Fig 2. STEM data on ‘Spud’. HAADF Image (Top) False-color EDS Maps (Bottom) References: [1] MacPherson G. J. (2014) T. of Geochem. Vol I: Met. And Cosmochem. Processes, 139-179. [2] Lodders K. (2003) ApJ, 591, 1220-1247. [3] Ebel D. S. (2006) Met. & the Early S. Sys. II., 253- 277. [4] Amelin Y. (2002) Science, 297, 1678-1683. [5] Connelly J.N. et.al. (2012) Science, 338, 651-655. [6] Schwander D. et al. (2015) GCA, 18, 70-87. [7] Palme H. and Wlotzka F. (1976) EPSL, 33, 45-60. [8] Berg T. et al. (2009) ApJ, 702, 172-176. [9] Liffman K. et al. (2021) Icarus, 221, 89-105. [10] Zega T.J. et al. (2021) PSJ, 2, 115. [11] Ramprasad T. et al. (2020) LPSC LI, Abstract #2472. [12] Ramprasad T. et al. (2021) Microscopy & Microanalysis, S1, 2792-2794. [13] Ramprasad T. et al. (2021) 84th MetSoc, Abstract #6123. [14] Zega T.J. et al. (2007) MAPS, 42, 1373-1386. [15] Ramprasad T. et al. (2022) MAPS, in revision. [16] Grossman L. (1975), GCA, 39, 433-454. [17] El Goresy A. et al. (1978) LPSC IX, Abstract#1100

T. Ramprasad↗

Materials Data on Ho2Ge2Os by Materials Project

Ho2OsGe2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ho sites. In the first Ho site, Ho is bonded in a 8-coordinate geometry to two equivalent Os and six Ge atoms. Both Ho–Os bond lengths are 3.19 Å. There are a spread of Ho–Ge bond distances ranging from 2.90–3.22 Å. In the second Ho site, Ho is bonded in a 2-coordinate geometry to four equivalent Os and six Ge atoms. There are a spread of Ho–Os bond distances ranging from 3.09–3.18 Å. There are a spread of Ho–Ge bond distances ranging from 2.93–3.12 Å. Os is bonded in a 10-coordinate geometry to six Ho and four Ge atoms. There are a spread of Os–Ge bond distances ranging from 2.47–2.61 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to seven Ho, one Os, and one Ge atom. The Ge–Ge bond length is 2.66 Å. In the second Ge site, Ge is bonded in a 9-coordinate geometry to five Ho, three equivalent Os, and one Ge atom. The Ge–Ge bond length is 2.71 Å.

36 MATERIALS SCIENCE↗

Materials Data on OsXe(O2F3)2 by Materials Project

XeOF4OsO3F2 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of one OsO3F2 cluster and two XeOF4 clusters. In the OsO3F2 cluster, Os is bonded in a 6-coordinate geometry to three O and three F atoms. All Os–O bond lengths are 1.71 Å. There are a spread of Os–F bond distances ranging from 1.96–2.16 Å. There are three inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Os atom. In the second O site, O is bonded in a single-bond geometry to one Os atom. In the third O site, O is bonded in a single-bond geometry to one Os atom. There are two inequivalent F sites. In the first F site, F is bonded in a water-like geometry to two equivalent Os atoms. In the second F site, F is bonded in a single-bond geometry to one Os atom. In each XeOF4 cluster, Xe is bonded in a square pyramidal geometry to one O and four F atoms. The Xe–O bond length is 1.83 Å. There are two shorter (2.03 Å) and two longer (2.04 Å) Xe–F bond lengths. O is bonded in a single-bond geometry to one Xe atom. There are four inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Xe atom. In the second F site, F is bonded in a single-bond geometry to one Xe atom. In the third F site, F is bonded in a single-bond geometry to one Xe atom. In the fourth F site, F is bonded in a single-bond geometry to one Xe atom.

36 MATERIALS SCIENCE↗

Materials Data on Os2C6SO6 by Materials Project

Os2C6SO6 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two Os2C6SO6 clusters. there are four inequivalent Os1- sites. In the first Os1- site, Os1- is bonded in a distorted rectangular see-saw-like geometry to three C+2.67+ and one S2- atom. There are a spread of Os–C bond distances ranging from 1.89–1.91 Å. The Os–S bond length is 2.40 Å. In the second Os1- site, Os1- is bonded in a distorted rectangular see-saw-like geometry to three C+2.67+ and one S2- atom. There is one shorter (1.89 Å) and two longer (1.90 Å) Os–C bond length. The Os–S bond length is 2.40 Å. In the third Os1- site, Os1- is bonded to three C+2.67+ and two S2- atoms to form distorted edge-sharing OsC3S2 square pyramids. There is two shorter (1.91 Å) and one longer (1.92 Å) Os–C bond length. There are one shorter (2.45 Å) and one longer (2.47 Å) Os–S bond lengths. In the fourth Os1- site, Os1- is bonded to three C+2.67+ and two S2- atoms to form distorted edge-sharing OsC3S2 square pyramids. There are a spread of Os–C bond distances ranging from 1.90–1.93 Å. There are one shorter (2.44 Å) and one longer (2.47 Å) Os–S bond lengths. There are twelve inequivalent C+2.67+ sites. In the first C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the second C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the third C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the fourth C+2.67+ site, C+2.67+ is bonded in a distorted linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the fifth C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the sixth C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the seventh C+2.67+ site, C+2.67+ is bonded in a distorted linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the eighth C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the ninth C+2.67+ site, C+2.67+ is bonded in a distorted linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the tenth C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the eleventh C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. In the twelfth C+2.67+ site, C+2.67+ is bonded in a linear geometry to one Os1- and one O2- atom. The C–O bond length is 1.16 Å. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a 3-coordinate geometry to three Os1- atoms. In the second S2- site, S2- is bonded in a 3-coordinate geometry to three Os1- atoms. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the sixth O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the seventh O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the eighth O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the ninth O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the tenth O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the eleventh O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the twelfth O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Os4C13(SO6)2 by Materials Project

Os4C13(SO6)2 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two Os4C13(SO6)2 clusters. there are four inequivalent Os2- sites. In the first Os2- site, Os2- is bonded in a 5-coordinate geometry to four C+2.77+ and one S2- atom. There are a spread of Os–C bond distances ranging from 1.90–2.16 Å. The Os–S bond length is 2.49 Å. In the second Os2- site, Os2- is bonded to four C+2.77+ and one S2- atom to form distorted edge-sharing OsC4S trigonal bipyramids. There are a spread of Os–C bond distances ranging from 1.91–2.19 Å. The Os–S bond length is 2.44 Å. In the third Os2- site, Os2- is bonded to four C+2.77+ and one S2- atom to form distorted edge-sharing OsC4S trigonal bipyramids. There are a spread of Os–C bond distances ranging from 1.91–2.23 Å. The Os–S bond length is 2.47 Å. In the fourth Os2- site, Os2- is bonded to four C+2.77+ and one S2- atom to form distorted edge-sharing OsC4S trigonal bipyramids. There are a spread of Os–C bond distances ranging from 1.91–2.23 Å. The Os–S bond length is 2.47 Å. There are thirteen inequivalent C+2.77+ sites. In the first C+2.77+ site, C+2.77+ is bonded in a distorted linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the second C+2.77+ site, C+2.77+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the third C+2.77+ site, C+2.77+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the fourth C+2.77+ site, C+2.77+ is bonded in a distorted linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the fifth C+2.77+ site, C+2.77+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the sixth C+2.77+ site, C+2.77+ is bonded in a distorted linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the seventh C+2.77+ site, C+2.77+ is bonded in a distorted linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the eighth C+2.77+ site, C+2.77+ is bonded in a distorted trigonal bipyramidal geometry to four Os2- and one S2- atom. The C–S bond length is 1.75 Å. In the ninth C+2.77+ site, C+2.77+ is bonded in a distorted linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the tenth C+2.77+ site, C+2.77+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the eleventh C+2.77+ site, C+2.77+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the twelfth C+2.77+ site, C+2.77+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. In the thirteenth C+2.77+ site, C+2.77+ is bonded in a linear geometry to one Os2- and one O2- atom. The C–O bond length is 1.16 Å. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a 3-coordinate geometry to three Os2- atoms. In the second S2- site, S2- is bonded in a 1-coordinate geometry to one Os2- and one C+2.77+ atom. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the sixth O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the seventh O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the eighth O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the ninth O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the tenth O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the eleventh O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom. In the twelfth O2- site, O2- is bonded in a single-bond geometry to one C+2.77+ atom.

36 MATERIALS SCIENCE↗

Materials Data on CsRe2OsSe4Cl3 by Materials Project

CsRe2OsSe4Cl3 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are two inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 6-coordinate geometry to six Cl1- atoms. There are a spread of Cs–Cl bond distances ranging from 3.81–3.84 Å. In the second Cs1+ site, Cs1+ is bonded in a distorted cuboctahedral geometry to six Se2- and six Cl1- atoms. There are a spread of Cs–Se bond distances ranging from 3.97–4.01 Å. There are a spread of Cs–Cl bond distances ranging from 4.20–4.24 Å. There are four inequivalent Re6+ sites. In the first Re6+ site, Re6+ is bonded in a 5-coordinate geometry to two Os2-, four Se2-, and one Cl1- atom. Both Re–Os bond lengths are 2.65 Å. There are three shorter (2.54 Å) and one longer (2.55 Å) Re–Se bond lengths. The Re–Cl bond length is 2.41 Å. In the second Re6+ site, Re6+ is bonded in a 5-coordinate geometry to two Os2-, four Se2-, and one Cl1- atom. There are one shorter (2.65 Å) and one longer (2.66 Å) Re–Os bond lengths. There are three shorter (2.54 Å) and one longer (2.55 Å) Re–Se bond lengths. The Re–Cl bond length is 2.41 Å. In the third Re6+ site, Re6+ is bonded in a 5-coordinate geometry to two Os2-, four Se2-, and one Cl1- atom. There are one shorter (2.65 Å) and one longer (2.66 Å) Re–Os bond lengths. There are three shorter (2.54 Å) and one longer (2.55 Å) Re–Se bond lengths. The Re–Cl bond length is 2.41 Å. In the fourth Re6+ site, Re6+ is bonded in a 5-coordinate geometry to two Os2-, four Se2-, and one Cl1- atom. Both Re–Os bond lengths are 2.65 Å. There are three shorter (2.54 Å) and one longer (2.55 Å) Re–Se bond lengths. The Re–Cl bond length is 2.41 Å. There are two inequivalent Os2- sites. In the first Os2- site, Os2- is bonded in a 1-coordinate geometry to four Re6+, four Se2-, and one Cl1- atom. There are a spread of Os–Se bond distances ranging from 2.51–2.53 Å. The Os–Cl bond length is 2.41 Å. In the second Os2- site, Os2- is bonded in a 1-coordinate geometry to four Re6+, four Se2-, and one Cl1- atom. There are a spread of Os–Se bond distances ranging from 2.51–2.53 Å. The Os–Cl bond length is 2.41 Å. There are eight inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 9-coordinate geometry to two Re6+ and one Os2- atom. In the second Se2- site, Se2- is bonded in a 9-coordinate geometry to two Re6+ and one Os2- atom. In the third Se2- site, Se2- is bonded in a 7-coordinate geometry to one Cs1+, two Re6+, and one Os2- atom. In the fourth Se2- site, Se2- is bonded in a 4-coordinate geometry to one Cs1+, two Re6+, and one Os2- atom. In the fifth Se2- site, Se2- is bonded in a 7-coordinate geometry to one Cs1+, two Re6+, and one Os2- atom. In the sixth Se2- site, Se2- is bonded in a 7-coordinate geometry to one Cs1+, two Re6+, and one Os2- atom. In the seventh Se2- site, Se2- is bonded in a 7-coordinate geometry to one Cs1+, two Re6+, and one Os2- atom. In the eighth Se2- site, Se2- is bonded in a 7-coordinate geometry to one Cs1+, two Re6+, and one Os2- atom. There are six inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted single-bond geometry to two Cs1+ and one Os2- atom. In the second Cl1- site, Cl1- is bonded in a distorted single-bond geometry to two Cs1+ and one Re6+ atom. In the third Cl1- site, Cl1- is bonded in a distorted single-bond geometry to two Cs1+ and one Re6+ atom. In the fourth Cl1- site, Cl1- is bonded in a distorted single-bond geometry to two Cs1+ and one Re6+ atom. In the fifth Cl1- site, Cl1- is bonded in a distorted single-bond geometry to two Cs1+ and one Os2- atom. In the sixth Cl1- site, Cl1- is bonded in a distorted single-bond geometry to two Cs1+ and one Re6+ atom.

36 MATERIALS SCIENCE↗

Materials Data on LaCeOs4 by Materials Project

CeLaOs4 is Cubic Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Ce3+ is bonded in a 12-coordinate geometry to twelve equivalent Os+1.50- atoms. All Ce–Os bond lengths are 3.19 Å. La3+ is bonded in a 12-coordinate geometry to twelve equivalent Os+1.50- atoms. All La–Os bond lengths are 3.19 Å. Os+1.50- is bonded to three equivalent Ce3+, three equivalent La3+, and six equivalent Os+1.50- atoms to form a mixture of edge, face, and corner-sharing OsLa3Ce3Os6 cuboctahedra. There are three shorter (2.71 Å) and three longer (2.72 Å) Os–Os bond lengths.

36 MATERIALS SCIENCE↗

Materials Data on IrOsRu by Materials Project

OsRuIr is Copper-derived structured and crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. Os is bonded to six equivalent Os, three equivalent Ru, and three equivalent Ir atoms to form OsIr3Os6Ru3 cuboctahedra that share corners with three equivalent RuIr3Os3Ru6 cuboctahedra, corners with three equivalent IrIr6Os3Ru3 cuboctahedra, corners with six equivalent OsIr3Os6Ru3 cuboctahedra, edges with six equivalent OsIr3Os6Ru3 cuboctahedra, edges with nine equivalent RuIr3Os3Ru6 cuboctahedra, edges with nine equivalent IrIr6Os3Ru3 cuboctahedra, faces with six equivalent OsIr3Os6Ru3 cuboctahedra, faces with six equivalent RuIr3Os3Ru6 cuboctahedra, and faces with six equivalent IrIr6Os3Ru3 cuboctahedra. All Os–Os bond lengths are 2.73 Å. All Os–Ru bond lengths are 2.67 Å. All Os–Ir bond lengths are 2.75 Å. Ru is bonded to three equivalent Os, six equivalent Ru, and three equivalent Ir atoms to form RuIr3Os3Ru6 cuboctahedra that share corners with three equivalent OsIr3Os6Ru3 cuboctahedra, corners with three equivalent IrIr6Os3Ru3 cuboctahedra, corners with six equivalent RuIr3Os3Ru6 cuboctahedra, edges with six equivalent RuIr3Os3Ru6 cuboctahedra, edges with nine equivalent OsIr3Os6Ru3 cuboctahedra, edges with nine equivalent IrIr6Os3Ru3 cuboctahedra, faces with six equivalent OsIr3Os6Ru3 cuboctahedra, faces with six equivalent RuIr3Os3Ru6 cuboctahedra, and faces with six equivalent IrIr6Os3Ru3 cuboctahedra. All Ru–Ru bond lengths are 2.73 Å. All Ru–Ir bond lengths are 2.76 Å. Ir is bonded to three equivalent Os, three equivalent Ru, and six equivalent Ir atoms to form IrIr6Os3Ru3 cuboctahedra that share corners with three equivalent OsIr3Os6Ru3 cuboctahedra, corners with three equivalent RuIr3Os3Ru6 cuboctahedra, corners with six equivalent IrIr6Os3Ru3 cuboctahedra, edges with six equivalent IrIr6Os3Ru3 cuboctahedra, edges with nine equivalent OsIr3Os6Ru3 cuboctahedra, edges with nine equivalent RuIr3Os3Ru6 cuboctahedra, faces with six equivalent OsIr3Os6Ru3 cuboctahedra, faces with six equivalent RuIr3Os3Ru6 cuboctahedra, and faces with six equivalent IrIr6Os3Ru3 cuboctahedra. All Ir–Ir bond lengths are 2.73 Å.

36 MATERIALS SCIENCE↗

Materials Data on CeIrOs by Materials Project

CeOsIr is Cubic Laves-derived structured and crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. Ce is bonded in a 12-coordinate geometry to six equivalent Os and six equivalent Ir atoms. There are four shorter (3.18 Å) and two longer (3.24 Å) Ce–Os bond lengths. There are four shorter (3.07 Å) and two longer (3.28 Å) Ce–Ir bond lengths. Os is bonded to six equivalent Ce, two equivalent Os, and four equivalent Ir atoms to form OsCe6Ir4Os2 cuboctahedra that share corners with eight equivalent IrCe6Ir2Os4 cuboctahedra, corners with ten equivalent OsCe6Ir4Os2 cuboctahedra, edges with six equivalent OsCe6Ir4Os2 cuboctahedra, faces with six equivalent OsCe6Ir4Os2 cuboctahedra, and faces with twelve equivalent IrCe6Ir2Os4 cuboctahedra. Both Os–Os bond lengths are 2.56 Å. All Os–Ir bond lengths are 2.73 Å. Ir is bonded to six equivalent Ce, four equivalent Os, and two equivalent Ir atoms to form IrCe6Ir2Os4 cuboctahedra that share corners with eight equivalent OsCe6Ir4Os2 cuboctahedra, corners with ten equivalent IrCe6Ir2Os4 cuboctahedra, edges with six equivalent IrCe6Ir2Os4 cuboctahedra, faces with six equivalent IrCe6Ir2Os4 cuboctahedra, and faces with twelve equivalent OsCe6Ir4Os2 cuboctahedra. Both Ir–Ir bond lengths are 2.74 Å.

36 MATERIALS SCIENCE↗

Materials Data on Dy5(Sn3Os)6 by Materials Project

Dy5Os6Sn17Sn crystallizes in the cubic F-43m space group. The structure is three-dimensional and consists of four 7440-31-5 molecules and one Dy5Os6Sn17 framework. In the Dy5Os6Sn17 framework, there are two inequivalent Dy sites. In the first Dy site, Dy is bonded in a 12-coordinate geometry to six equivalent Os and twelve equivalent Sn atoms. All Dy–Os bond lengths are 3.55 Å. All Dy–Sn bond lengths are 3.46 Å. In the second Dy site, Dy is bonded in a 1-coordinate geometry to three equivalent Os and ten Sn atoms. All Dy–Os bond lengths are 3.03 Å. There are a spread of Dy–Sn bond distances ranging from 2.95–3.37 Å. Os is bonded in a 9-coordinate geometry to three Dy and six Sn atoms. There are four shorter (2.68 Å) and two longer (2.83 Å) Os–Sn bond lengths. There are three inequivalent Sn sites. In the first Sn site, Sn is bonded in a tetrahedral geometry to four equivalent Dy atoms. In the second Sn site, Sn is bonded in a hexagonal planar geometry to three equivalent Dy and three equivalent Os atoms. In the third Sn site, Sn is bonded in a 2-coordinate geometry to three Dy and two equivalent Os atoms.

36 MATERIALS SCIENCE↗

Materials Data on CeOsRu by Materials Project

CeOsRu is Cubic Laves-derived structured and crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. Ce is bonded in a 12-coordinate geometry to six equivalent Os and six equivalent Ru atoms. There are two shorter (3.14 Å) and four longer (3.21 Å) Ce–Os bond lengths. There are four shorter (3.10 Å) and two longer (3.19 Å) Ce–Ru bond lengths. Os is bonded to six equivalent Ce, two equivalent Os, and four equivalent Ru atoms to form OsCe6Os2Ru4 cuboctahedra that share corners with eight equivalent RuCe6Os4Ru2 cuboctahedra, corners with ten equivalent OsCe6Os2Ru4 cuboctahedra, edges with six equivalent OsCe6Os2Ru4 cuboctahedra, faces with six equivalent OsCe6Os2Ru4 cuboctahedra, and faces with twelve equivalent RuCe6Os4Ru2 cuboctahedra. Both Os–Os bond lengths are 2.61 Å. All Os–Ru bond lengths are 2.70 Å. Ru is bonded to six equivalent Ce, four equivalent Os, and two equivalent Ru atoms to form RuCe6Os4Ru2 cuboctahedra that share corners with eight equivalent OsCe6Os2Ru4 cuboctahedra, corners with ten equivalent RuCe6Os4Ru2 cuboctahedra, edges with six equivalent RuCe6Os4Ru2 cuboctahedra, faces with six equivalent RuCe6Os4Ru2 cuboctahedra, and faces with twelve equivalent OsCe6Os2Ru4 cuboctahedra. Both Ru–Ru bond lengths are 2.77 Å.

36 MATERIALS SCIENCE↗

Materials Data on ThIrOs by Materials Project

ThOsIr is Cubic Laves-derived structured and crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. Th is bonded in a 12-coordinate geometry to six equivalent Os and six equivalent Ir atoms. There are four shorter (3.23 Å) and two longer (3.24 Å) Th–Os bond lengths. There are four shorter (3.12 Å) and two longer (3.31 Å) Th–Ir bond lengths. Os is bonded to six equivalent Th, two equivalent Os, and four equivalent Ir atoms to form OsTh6Ir4Os2 cuboctahedra that share corners with eight equivalent IrTh6Ir2Os4 cuboctahedra, corners with ten equivalent OsTh6Ir4Os2 cuboctahedra, edges with six equivalent OsTh6Ir4Os2 cuboctahedra, faces with six equivalent OsTh6Ir4Os2 cuboctahedra, and faces with twelve equivalent IrTh6Ir2Os4 cuboctahedra. Both Os–Os bond lengths are 2.61 Å. All Os–Ir bond lengths are 2.76 Å. Ir is bonded to six equivalent Th, four equivalent Os, and two equivalent Ir atoms to form IrTh6Ir2Os4 cuboctahedra that share corners with eight equivalent OsTh6Ir4Os2 cuboctahedra, corners with ten equivalent IrTh6Ir2Os4 cuboctahedra, edges with six equivalent IrTh6Ir2Os4 cuboctahedra, faces with six equivalent IrTh6Ir2Os4 cuboctahedra, and faces with twelve equivalent OsTh6Ir4Os2 cuboctahedra. Both Ir–Ir bond lengths are 2.77 Å.

36 MATERIALS SCIENCE↗