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At least 577 records · Page 32

Non-Neutron Transmutation of Used Nuclear Fuel (Final Report)

The primary goal of this study is to develop a national facility concept for transmuting long-lived fission products (LLFP) to substantially reduce the disposal impact by minimizing the need for a geologic-timescale repository. As a charter for this study, the national transmutation facility was required to reduce the radiotoxicity and decay heat of LLFP isotopes by at least 90% relative to their values at discharge from a commercial LWR, while consuming less than 10% of the reactor's energy. The identified LLFP isotopes are Se-79, Zr-93, Tc-99, I-129, Sn-126, and Cs-135, whose radiotoxicity is about 99% of the total radiotoxicity of all fission products at 1,000 years. Approximately ~72 kg of LLFPs is discharged every year from a 1,000 MWe commercial or advanced nuclear reactor. First, LLFP transmutation options with non-neutron beams (photons and protons) were explored. The study concluded that LLFP transmutation is feasible with high-energy, high-intensity photons or protons, but impractical on an engineering scale due to low transmutation rates and the high energy requirements to produce the desired photon or proton beams. As alternatives, LLFP transmutation options with neutrons from fission, fusion, and spallation reactions were additionally explored. The transmutation options using advanced critical reactors are attractive only for selective LLFP isotopes because the production rates of several LLFP isotopes (Zr-93, Sn-126, and Cs-135) from fission reactions are larger than the transmutation rates. The transmutation options with only spallation neutrons are favorable to transmute all LLFP isotopes, but as a tradeoff, the net transmutation rates are reduced. The national transmutation facility concept was developed following an exploration of transmutation options using various incident particles. The proposed national LLFP transmutation comprises a dedicated molten-salt reactor (MSR), a proton accelerator, and a spallation neutron-based transmuter. The MSR power was set at 300 MWt and 120 MWe, with the thermal power approximately 10% of that of a commercial 1,000 MWe PWR. The electricity generated by the MSR powers the accelerator and transmuter. The accelerator produces 1 GeV, 30 mA protons, which are introduced into the spallation neutron-based transmuter. The spallation neutron-based transmuter consists of a central spallation target and LLFP target pins merged in a heavy water tank. The six LLFP isotopes are separated into two groups. Tc-99, I-129, and Se-79, having larger neutron cross sections, belong to group A, while Zr-93, Sn126, and Cs-135, having smaller neutron cross sections, belong to group B. Then, for effective transmutation, LLFPs in groups A and B are transmuted in the dedicated MSR and in a spallation neutron-based transmuter, respectively. The estimated capital cost of the national transmutation facility is approximately $\$$3.1B, and its annual O&M cost is expected to be ~$\$$182M. Radiotoxicity and decay heat of LLFPs were calculated and compared with those of the original LLFPs. It was assumed that the targets were made with elementwise LLFP rather than isotopic LLFP, owing to the potentially high cost of isotopic separation from used nuclear fuels. The decay heat of LLFPs can be reduced by more than 90% using a single national transmutation facility. However, radiotoxicity decreases by 79–84%, which does not meet the transmutation performance requirement, primarily because Cs-135 is produced rather than depleted. Thus, to meet the design requirement, Cs-135 should be separated from other Cs isotopes and irradiated in a spallation neutron-based transmuter. Then, radiotoxicity decreases by ~92%.

11 NUCLEAR FUEL CYCLE AND FUEL MATERIALS↗

Wash Penalty Factors: Insight into the Effects of Water Wash Down of Building Materials for Radionuclide/Nuclear (Rn) Decontamination - 20153

The release of radiological material to the urban environment can have a devastating socio-economic impact. In an urban release scenario, areas around the dispersal epicenter and any areas contaminated via atmospheric deposition may require extensive decontamination. Most recently, our group reported the decontamination efficacy of pressurized water washing of common porous building materials, and compared the penetration depth of the contaminations before and after exposure to pressurized tap water. Here, we continue evaluation of the decontamination efficacy of wash solutions based on potassium (K{sup +}) salt for cesium (Cs), strontium (Sr), and europium (Eu) contaminations on common building surfaces. The surfaces included: the cement used in concrete, the aggregate used in concrete, intact concrete, roadway asphalt, asphalt shingles, and latex paint. We deposited solutions of {sup 137}Cs, {sup 85}Sr, and {sup 152}Eu onto numerous common building materials and exposed these materials to a static bath or low-pressure flow of tap water, 0.1 M potassium chloride (KCl), and 0.5 M KCl. The decontamination efficacy and the depth profile for residual contamination were measured to determine the conditions under which applying a wash solution has benefit compared to physically removing the surface material. To aid in these analyses, we introduced a 'wash penalty factor' to quantify the degree to which contamination migrated into the bulk material by the action of the wash method. On asphalt, 70-80% of the radionuclides were found to be within 0.02 mm of the surface. Cs{sup +} bonded to negative charge sites on the surface of the mineral aggregate (used in concrete) so decontamination was improved by ion exchange with K{sup +}. Sr{sup 2+} is soluble and removed by water, while not bonding to aggregate or demonstrating solubility in the liquid asphalt. Eu{sup 3+} is precipitated and not removed in gentle wash but displays mobility within the pore space that suggests its presence as a colloid. Concrete is more porous than asphalt, and 80% of the radionuclides were within 0.2 mm of the surface for {sup 137}Cs and {sup 152}Eu and 50- 80% for {sup 85}Sr. On concrete, Cs{sup +} bonds similarly to asphalt. Sr{sup 2+} bonds to the cement or precipitates from the alkaline pore water. Eu{sup 3+} sorbs to the cement and then precipitates. In brick, the results for Cs{sup +} and Sr{sup 2+} suggested that diffusion of ions from deeper in the coupon was important. Eu{sup 3+} is removed poorly due to precipitation. We will explain and report example wash penalty factors that vary from 0 to > 1 for the various methods and the implications for deciding when to implement wash down methods. (authors)

12 MANAGEMENT OF RADIOACTIVE AND NON-RADIOACTIVE W↗

GeoMelt{sup R} In-Container Vitrification (ICV){sup TM} for Fukushima Daiichi Water Treatment Secondary Wastes - 20212

The Japanese government is supporting development work implemented jointly by Veolia subsidiaries Kurion Japan, K.K., Veolia Nuclear Solutions (VNS), Inc., and Veolia Nuclear Solutions Federal Services, LLC for treating radioactive waste generated from Fukushima Daiichi Nuclear Power Station (NPS) water treatment using the GeoMelt{sup TM} In-Container Vitrification (ICV){sup TM} technology. The initial work consisted of glass formulation and engineering-scale testing which was completed in 2018, in the frame of an IRID (International Research Institute for Nuclear Decommissioning) program as part of a project subsidized by Japan's Ministry of Economy, Trade and Industry (METI). The Fukushima Daiichi NPS Mid- and Long-Term Road-map requires investigation of methods to stabilize solid wastes (and to immobilize radioisotopes in the wastes) generated as a result of emergency response and decommissioning activities. Cooling water treatment has resulted in a significant amount of solid and slurry secondary wastes (mostly adsorbents and ion-exchange materials) which will require processing at some point. GeoMelt{sup R} ICV{sup TM} is a joule-heated melter technology which uses a refractory-lined single-use container combining the melter and disposal container. There is no pouring required nor concerns with refractory corrosion which allows the process to accommodate a wide range of waste chemistries and high waste loadings. The testing described here consisted of three engineering-scale melts, each processing between 212 kg and 240 kg of waste simulants, glass formers, and non-radioactive cesium (Cs) and strontium (Sr) tracers. Continuous isokinetic stack sampling of off-gas emissions was performed for each test in order to calculate Cs and Sr retention in the glass wasteform. Single-pass retention of Cs in the final glass wasteform ranged from 91.46 to 99.30%, and single-pass retention of Sr ranged from 99.76 to 100%. Planned particulate recycle will increase these retention levels. Melt 1 processed a mixture of KUR-EH (a zeolite-based ion-exchange material), simulated Advanced Liquid Processing System (ALPS) Carbonate and Iron Slurries, and glass additives. Melt 2 processed a mixture of KUR-EH, KUR-TSG (a titanate-based adsorbent), and glass additives. Melt 3 processed a mixture of KUR-EH, simulated barium sulfate/iron ferrocyanide sludge (AREVA sludge), and glass additives. Waste loadings for these melts ranged from 70 weight percent (wt%) to 82 wt%. Vitrification produces a waste form much denser than the stored water treatment secondary waste wastes, resulting in significant volume reduction. Volume reductions for the three tests ranged from 74 to 79 vol%. Vitrification produces a chemically durable wasteform. Pacific Northwest National Laboratory (PNNL) tested three glass samples from each engineering-scale melt) by the Materials Characterization Center 1 (MCC-1) test, an international standard leach test of the chemical durability of nuclear waste glasses. PNNL also obtained one U.S. reference glass (EA Glass) and two Japan reference glasses P0798) and tested these under the same MCC-1 conditions (90 deg. C, 10 m-1, DIW, and 7, 14, 28-day) as the GeoMelt{sup R} ICV{sup TM} glasses. The GeoMelt{sup R} ICV{sup TM} glasses exhibited lower total normalized releases and 14- to 28-day normalized release rates than the three reference glasses. These results suggest that the GeoMelt{sup R} ICV{sup TM} glasses have durabilities on par with high-level waste glasses under standard test conditions. Post-melt process sampling and analysis indicated no Cs migration into the melter refractory materials and very little deposition of Cs or Sr onto the melter hood or off-gas piping internals. The results of the testing indicated good Cs retention in the glass, high volume reduction and waste loadings, and excellent chemical durability. These factors are important to minimize treatment costs and to protect workers and the environment. (authors)

12 MANAGEMENT OF RADIOACTIVE AND NON-RADIOACTIVE W↗

Modeling Cost of Offshore Carbon Storage in Saline Reservoirs

Poster presentation to the AAPG-SEG-SPE CCUS 2024 Conference. Offshore saline reservoirs provide a significant and accessible resource for geologic carbon storage (CS). The offshore environment requires distinct approaches to site selection, operations, monitoring, and risk that affect the technoeconomic assessment of offshore CS projects. The National Energy Technology Laboratory (NETL) has developed a CS cost model for offshore saline reservoirs known as CO2_S_COM_Offshore. Based on NETL’s widely used CO2_S_COM cost model for onshore saline CS, CO2_S_COM_Offshore enables technoeconomic analysis of CS in offshore areas. This model comprehensively incorporates multiple facets of offshore CS projects, from regional evaluation and site selection to permitting, transport, operations, monitoring, site closure, and decommissioning. Developed to model cost for offshore United States (US) Exclusive Economic Zones, aspects of this model can be adapted to international projects. Presented at the SPE/AAPG/SEG Carbon Capture Utilization and Storage Conference in Houston, TX, March 11-13, 2024.

Mark-Moser, Mackenzie K.↗

Materials Data on CsI3 by Materials Project

CsI3 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Cs is bonded in a 10-coordinate geometry to ten I atoms. There are a spread of Cs–I bond distances ranging from 3.95–4.55 Å. There are three inequivalent I sites. In the first I site, I is bonded in a distorted rectangular see-saw-like geometry to two equivalent Cs and two I atoms. There are one shorter (2.90 Å) and one longer (3.02 Å) I–I bond lengths. In the second I site, I is bonded in a 5-coordinate geometry to four equivalent Cs and one I atom. In the third I site, I is bonded in a 3-coordinate geometry to four equivalent Cs and one I atom.

36 MATERIALS SCIENCE↗

Materials Data on CsBrF by Materials Project

CsBrF crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Cs is bonded to four equivalent Br and five equivalent F atoms to form distorted CsBr4F5 square pyramids that share corners with four equivalent FCs5Br octahedra, edges with eight equivalent CsBr4F5 square pyramids, and faces with four equivalent CsBr4F5 square pyramids. The corner-sharing octahedral tilt angles are 125°. All Cs–Br bond lengths are 3.81 Å. There are one shorter (2.97 Å) and four longer (3.12 Å) Cs–F bond lengths. Br is bonded in a 1-coordinate geometry to four equivalent Cs, one Br, and one F atom. The Br–Br bond length is 2.41 Å. The Br–F bond length is 2.49 Å. F is bonded to five equivalent Cs and one Br atom to form FCs5Br octahedra that share corners with four equivalent FCs5Br octahedra, corners with four equivalent CsBr4F5 square pyramids, and edges with eight equivalent FCs5Br octahedra. The corner-sharing octahedral tilt angles are 10°.

36 MATERIALS SCIENCE↗

Materials Data on CsIO4 by Materials Project

CsIO4 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Cs is bonded in a 8-coordinate geometry to eight O atoms. There are a spread of Cs–O bond distances ranging from 3.16–3.40 Å. There are three inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to two equivalent Cs and one I atom. The O–I bond length is 1.80 Å. In the second O site, O is bonded in a distorted single-bond geometry to three equivalent Cs and one I atom. The O–I bond length is 1.80 Å. In the third O site, O is bonded in a distorted linear geometry to one Cs and one I atom. The O–I bond length is 1.80 Å. I is bonded in a tetrahedral geometry to four O atoms.

36 MATERIALS SCIENCE↗

Materials Data on CsH18RuN6(ClO2)4 by Materials Project

Cs(O2Cl)4Ru(NH3)6 crystallizes in the trigonal R-3 space group. The structure is two-dimensional and consists of three Ru(NH3)6 clusters and three Cs(O2Cl)4 sheets oriented in the (0, 0, 1) direction. In each Ru(NH3)6 cluster, Ru5+ is bonded in an octahedral geometry to six equivalent N+0.67- atoms. All Ru–N bond lengths are 2.13 Å. N+0.67- is bonded in a distorted trigonal non-coplanar geometry to one Ru5+ and three H1+ atoms. All N–H bond lengths are 1.03 Å. There are three inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N+0.67- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N+0.67- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N+0.67- atom. In each Cs(O2Cl)4 sheet, Cs1+ is bonded in a distorted body-centered cubic geometry to six equivalent O2- and two equivalent Cl1- atoms. All Cs–O bond lengths are 3.16 Å. Both Cs–Cl bond lengths are 3.69 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one Cs1+ and one Cl1- atom. The O–Cl bond length is 1.46 Å. In the second O2- site, O2- is bonded in a single-bond geometry to one Cl1- atom. The O–Cl bond length is 1.47 Å. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a tetrahedral geometry to four O2- atoms. In the second Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one Cs1+ atom.

36 MATERIALS SCIENCE↗

Materials Data on CsBr3 by Materials Project

CsBr3 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Cs is bonded in a 10-coordinate geometry to ten Br atoms. There are a spread of Cs–Br bond distances ranging from 3.69–4.29 Å. There are three inequivalent Br sites. In the first Br site, Br is bonded in a 5-coordinate geometry to four equivalent Cs and one Br atom. The Br–Br bond length is 2.66 Å. In the second Br site, Br is bonded to four equivalent Cs and one Br atom to form distorted BrCs4Br trigonal bipyramids that share corners with six equivalent BrCs2Br2 tetrahedra, corners with eight equivalent BrCs4Br trigonal bipyramids, an edgeedge with one BrCs2Br2 tetrahedra, and edges with two equivalent BrCs4Br trigonal bipyramids. The Br–Br bond length is 2.52 Å. In the third Br site, Br is bonded to two equivalent Cs and two Br atoms to form distorted BrCs2Br2 tetrahedra that share corners with two equivalent BrCs2Br2 tetrahedra, corners with six equivalent BrCs4Br trigonal bipyramids, and an edgeedge with one BrCs4Br trigonal bipyramid.

36 MATERIALS SCIENCE↗

Materials Data on CsXeF7 by Materials Project

XeCsF7 crystallizes in the cubic P2_13 space group. The structure is three-dimensional. Xe is bonded in a 7-coordinate geometry to seven F atoms. There are a spread of Xe–F bond distances ranging from 2.06–2.14 Å. Cs is bonded in a 9-coordinate geometry to fifteen F atoms. There are a spread of Cs–F bond distances ranging from 3.19–3.59 Å. There are three inequivalent F sites. In the first F site, F is bonded in a distorted single-bond geometry to one Xe and two equivalent Cs atoms. In the second F site, F is bonded in a distorted single-bond geometry to one Xe and two equivalent Cs atoms. In the third F site, F is bonded in a distorted single-bond geometry to one Xe and three equivalent Cs atoms.

36 MATERIALS SCIENCE↗

Materials Data on CsClO4 by Materials Project

CsClO4 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Cs is bonded in a 12-coordinate geometry to twelve O atoms. There are a spread of Cs–O bond distances ranging from 3.24–3.69 Å. There are three inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to three equivalent Cs and one Cl atom. The O–Cl bond length is 1.46 Å. In the second O site, O is bonded in a distorted single-bond geometry to three equivalent Cs and one Cl atom. The O–Cl bond length is 1.47 Å. In the third O site, O is bonded in a distorted single-bond geometry to three equivalent Cs and one Cl atom. The O–Cl bond length is 1.46 Å. Cl is bonded in a tetrahedral geometry to four O atoms.

36 MATERIALS SCIENCE↗

Materials Data on CsGa7 by Materials Project

CsGa7 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Cs is bonded in a 12-coordinate geometry to fifteen Ga atoms. There are a spread of Cs–Ga bond distances ranging from 3.85–3.94 Å. There are three inequivalent Ga sites. In the first Ga site, Ga is bonded in a 7-coordinate geometry to three equivalent Cs and four Ga atoms. There are one shorter (2.62 Å) and three longer (2.64 Å) Ga–Ga bond lengths. In the second Ga site, Ga is bonded in a 8-coordinate geometry to one Cs and seven Ga atoms. There are a spread of Ga–Ga bond distances ranging from 2.57–2.83 Å. In the third Ga site, Ga is bonded in a 9-coordinate geometry to three equivalent Cs and six Ga atoms. Both Ga–Ga bond lengths are 2.83 Å.

36 MATERIALS SCIENCE↗

Materials Data on Cs4Pr6C2I13 by Materials Project

Cs4Pr6C2I13 crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. Cs is bonded in a 7-coordinate geometry to seven I atoms. There are a spread of Cs–I bond distances ranging from 3.98–4.27 Å. There are two inequivalent Pr sites. In the first Pr site, Pr is bonded to one C and five I atoms to form distorted PrCI5 octahedra that share a cornercorner with one PrCI5 octahedra, corners with two equivalent PrC2I5 pentagonal bipyramids, and edges with four equivalent PrC2I5 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 0°. The Pr–C bond length is 2.31 Å. There are a spread of Pr–I bond distances ranging from 3.18–3.42 Å. In the second Pr site, Pr is bonded to two equivalent C and five I atoms to form distorted PrC2I5 pentagonal bipyramids that share a cornercorner with one PrCI5 octahedra, edges with two equivalent PrCI5 octahedra, edges with two equivalent PrC2I5 pentagonal bipyramids, and faces with two equivalent PrC2I5 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 7°. There are one shorter (2.63 Å) and one longer (2.64 Å) Pr–C bond lengths. There are a spread of Pr–I bond distances ranging from 3.20–3.46 Å. C is bonded in a 6-coordinate geometry to five Pr and one C atom. The C–C bond length is 1.39 Å. There are four inequivalent I sites. In the first I site, I is bonded to two equivalent Cs and three Pr atoms to form distorted ICs2Pr3 trigonal bipyramids that share corners with three equivalent ICs2Pr3 trigonal bipyramids, an edgeedge with one ICs2Pr3 trigonal bipyramid, and a faceface with one ICs4Pr2 octahedra. In the second I site, I is bonded to four equivalent Cs and two equivalent Pr atoms to form face-sharing ICs4Pr2 octahedra. In the third I site, I is bonded in a 5-coordinate geometry to two equivalent Pr atoms. In the fourth I site, I is bonded in a 6-coordinate geometry to four equivalent Cs and two Pr atoms.

36 MATERIALS SCIENCE↗

Materials Data on Cs5Si3AgO9 by Materials Project

Cs5AgSi3O9 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are five inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Cs–O bond distances ranging from 3.03–3.57 Å. In the second Cs1+ site, Cs1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Cs–O bond distances ranging from 3.18–3.60 Å. In the third Cs1+ site, Cs1+ is bonded in a 2-coordinate geometry to two equivalent O2- atoms. Both Cs–O bond lengths are 2.86 Å. In the fourth Cs1+ site, Cs1+ is bonded in a 2-coordinate geometry to two equivalent O2- atoms. Both Cs–O bond lengths are 2.80 Å. In the fifth Cs1+ site, Cs1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Cs–O bond distances ranging from 3.12–3.48 Å. Ag1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Ag–O bond lengths are 2.07 Å. There are three inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.64–1.67 Å. In the second Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.62–1.72 Å. In the third Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.62–1.71 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to five Cs1+ and one Si4+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two Cs1+, one Ag1+, and one Si4+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to four Cs1+ and one Si4+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Cs1+ and two Si4+ atoms. In the fifth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to three equivalent Cs1+ and two Si4+ atoms. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to three equivalent Cs1+ and two Si4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Cs2Lu7CCl18 by Materials Project

Cs2Lu7CCl18 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. Cs is bonded to twelve Cl atoms to form CsCl12 cuboctahedra that share corners with nine LuCl6 octahedra, edges with three equivalent CsCl12 cuboctahedra, edges with three equivalent LuCCl5 octahedra, and faces with three equivalent LuCCl5 octahedra. The corner-sharing octahedra tilt angles range from 45–48°. There are a spread of Cs–Cl bond distances ranging from 3.73–3.87 Å. There are two inequivalent Lu sites. In the first Lu site, Lu is bonded to one C and five Cl atoms to form LuCCl5 octahedra that share corners with two equivalent CsCl12 cuboctahedra, corners with two LuCl6 octahedra, an edgeedge with one CsCl12 cuboctahedra, edges with four equivalent LuCCl5 octahedra, and a faceface with one CsCl12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–45°. The Lu–C bond length is 2.49 Å. There are a spread of Lu–Cl bond distances ranging from 2.59–2.73 Å. In the second Lu site, Lu is bonded to six equivalent Cl atoms to form LuCl6 octahedra that share corners with six equivalent CsCl12 cuboctahedra and corners with six equivalent LuCCl5 octahedra. The corner-sharing octahedral tilt angles are 45°. All Lu–Cl bond lengths are 2.62 Å. C is bonded in an octahedral geometry to six equivalent Lu atoms. There are three inequivalent Cl sites. In the first Cl site, Cl is bonded in a distorted L-shaped geometry to two equivalent Cs and two equivalent Lu atoms. In the second Cl site, Cl is bonded in a distorted L-shaped geometry to one Cs and two equivalent Lu atoms. In the third Cl site, Cl is bonded in a 2-coordinate geometry to one Cs and two Lu atoms.

36 MATERIALS SCIENCE↗

Materials Data on Cs2Ta6PbCl18 by Materials Project

Cs2PbTa6Cl18 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. Cs is bonded to twelve Cl atoms to form CsCl12 cuboctahedra that share corners with three equivalent PbCl6 octahedra, corners with six equivalent TaCl5 square pyramids, edges with three equivalent CsCl12 cuboctahedra, edges with three equivalent TaCl5 square pyramids, and faces with three equivalent TaCl5 square pyramids. The corner-sharing octahedral tilt angles are 56°. There are a spread of Cs–Cl bond distances ranging from 3.59–3.78 Å. Ta is bonded to five Cl atoms to form distorted TaCl5 square pyramids that share corners with two equivalent CsCl12 cuboctahedra, a cornercorner with one PbCl6 octahedra, corners with four equivalent TaCl5 square pyramids, an edgeedge with one CsCl12 cuboctahedra, and a faceface with one CsCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 44°. There are a spread of Ta–Cl bond distances ranging from 2.47–2.65 Å. Pb is bonded to six equivalent Cl atoms to form PbCl6 octahedra that share corners with six equivalent CsCl12 cuboctahedra and corners with six equivalent TaCl5 square pyramids. All Pb–Cl bond lengths are 2.97 Å. There are three inequivalent Cl sites. In the first Cl site, Cl is bonded in a 3-coordinate geometry to one Cs and two equivalent Ta atoms. In the second Cl site, Cl is bonded in a 3-coordinate geometry to one Cs, one Ta, and one Pb atom. In the third Cl site, Cl is bonded in a 4-coordinate geometry to two equivalent Cs and two equivalent Ta atoms.

36 MATERIALS SCIENCE↗

Materials Data on Cs2YSi4O10F by Materials Project

Cs2YSi4O10F crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are four inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 9-coordinate geometry to eight O2- and one F1- atom. There are a spread of Cs–O bond distances ranging from 3.15–3.46 Å. The Cs–F bond length is 3.66 Å. In the second Cs1+ site, Cs1+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Cs–O bond distances ranging from 3.24–3.46 Å. In the third Cs1+ site, Cs1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are two shorter (3.18 Å) and two longer (3.19 Å) Cs–O bond lengths. In the fourth Cs1+ site, Cs1+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Cs–O bond distances ranging from 3.20–3.56 Å. Y3+ is bonded to four O2- and two F1- atoms to form YO4F2 octahedra that share corners with two equivalent YO4F2 octahedra and corners with four SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 10–11°. There are a spread of Y–O bond distances ranging from 2.25–2.28 Å. Both Y–F bond lengths are 2.26 Å. There are four inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one YO4F2 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 35°. There are a spread of Si–O bond distances ranging from 1.60–1.66 Å. In the second Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one YO4F2 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of Si–O bond distances ranging from 1.60–1.66 Å. In the third Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one YO4F2 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 46°. There are a spread of Si–O bond distances ranging from 1.60–1.66 Å. In the fourth Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one YO4F2 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 31°. There are a spread of Si–O bond distances ranging from 1.60–1.66 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Cs1+ and two Si4+ atoms. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two Cs1+, one Y3+, and one Si4+ atom. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Cs1+ and two Si4+ atoms. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Cs1+, one Y3+, and one Si4+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Cs1+ and two Si4+ atoms. In the sixth O2- site, O2- is bonded in a 2-coordinate geometry to two Cs1+ and two Si4+ atoms. In the seventh O2- site, O2- is bonded in a linear geometry to two equivalent Si4+ atoms. In the eighth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Cs1+, one Y3+, and one Si4+ atom. In the ninth O2- site, O2- is bonded in a 2-coordinate geometry to one Cs1+, one Y3+, and one Si4+ atom. In the tenth O2- site, O2- is bonded in a linear geometry to one Cs1+ and two equivalent Si4+ atoms. In the eleventh O2- site, O2- is bonded in a bent 150 degrees geometry to one Cs1+ and two equivalent Si4+ atoms. In the twelfth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cs1+ and two equivalent Si4+ atoms. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a linear geometry to two equivalent Y3+ atoms. In the second F1- site, F1- is bonded in a linear geometry to one Cs1+ and two equivalent Y3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Cs5SiP3 by Materials Project

Cs5SiP3 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are five inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a 3-coordinate geometry to three P+0.33- atoms. There are one shorter (3.68 Å) and two longer (3.75 Å) Cs–P bond lengths. In the second Cs1+ site, Cs1+ is bonded in a 4-coordinate geometry to four P+0.33- atoms. There are a spread of Cs–P bond distances ranging from 3.83–3.93 Å. In the third Cs1+ site, Cs1+ is bonded in a 3-coordinate geometry to three P+0.33- atoms. There are one shorter (3.56 Å) and two longer (3.66 Å) Cs–P bond lengths. In the fourth Cs1+ site, Cs1+ is bonded in a 5-coordinate geometry to five P+0.33- atoms. There are a spread of Cs–P bond distances ranging from 3.68–3.82 Å. In the fifth Cs1+ site, Cs1+ is bonded in a 4-coordinate geometry to four P+0.33- atoms. There are a spread of Cs–P bond distances ranging from 3.56–3.72 Å. Si4- is bonded in a trigonal planar geometry to three P+0.33- atoms. All Si–P bond lengths are 2.22 Å. There are three inequivalent P+0.33- sites. In the first P+0.33- site, P+0.33- is bonded in a 1-coordinate geometry to five Cs1+ and one Si4- atom. In the second P+0.33- site, P+0.33- is bonded in a 1-coordinate geometry to seven Cs1+ and one Si4- atom. In the third P+0.33- site, P+0.33- is bonded in a 1-coordinate geometry to seven Cs1+ and one Si4- atom.

36 MATERIALS SCIENCE↗