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Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

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At least 433 records · Page 24
All sourcesNASA NTRSDOE OSTI
DOE OSTI2020

Materials Data on Na2InAgBr6 by Materials Project

(Na)2AgInBr6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one AgInBr6 framework. In the AgInBr6 framework, Ag1+ is bonded to six equivalent Br1- atoms to form AgBr6 octahedra that share corners with six equivalent InBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ag–Br bond lengths are 2.80 Å. In3+ is bonded to six equivalent Br1- atoms to form InBr6 octahedra that share corners with six equivalent AgBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–Br bond lengths are 2.71 Å. Br1- is bonded in a linear geometry to one Ag1+ and one In3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li2InCuF6 by Materials Project

(Li)2CuInF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight lithium molecules and one CuInF6 framework. In the CuInF6 framework, Cu1+ is bonded to six equivalent F1- atoms to form CuF6 octahedra that share corners with six equivalent InF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cu–F bond lengths are 2.11 Å. In3+ is bonded to six equivalent F1- atoms to form InF6 octahedra that share corners with six equivalent CuF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–F bond lengths are 2.11 Å. F1- is bonded in a linear geometry to one Cu1+ and one In3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na2AgAsBr6 by Materials Project

(Na)2AgAsBr6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one AgAsBr6 framework. In the AgAsBr6 framework, Ag1+ is bonded to six equivalent Br1- atoms to form AgBr6 octahedra that share corners with six equivalent AsBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ag–Br bond lengths are 2.78 Å. As3+ is bonded to six equivalent Br1- atoms to form AsBr6 octahedra that share corners with six equivalent AgBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All As–Br bond lengths are 2.66 Å. Br1- is bonded in a linear geometry to one Ag1+ and one As3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on ZrNiF6 by Materials Project

ZrNiF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Zr4+ is bonded to six equivalent F1- atoms to form ZrF6 octahedra that share corners with six equivalent NiF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Zr–F bond lengths are 2.04 Å. Ni2+ is bonded to six equivalent F1- atoms to form NiF6 octahedra that share corners with six equivalent ZrF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ni–F bond lengths are 2.02 Å. F1- is bonded in a linear geometry to one Zr4+ and one Ni2+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na3LuCl6 by Materials Project

(Na)2NaLuCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one NaLuCl6 framework. In the NaLuCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent LuCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.69 Å. Lu3+ is bonded to six equivalent Cl1- atoms to form LuCl6 octahedra that share corners with six equivalent NaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Lu–Cl bond lengths are 2.56 Å. Cl1- is bonded in a linear geometry to one Na1+ and one Lu3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na3CeCl6 by Materials Project

(Na)2NaCeCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one NaCeCl6 framework. In the NaCeCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent CeCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.71 Å. Ce3+ is bonded to six equivalent Cl1- atoms to form CeCl6 octahedra that share corners with six equivalent NaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ce–Cl bond lengths are 2.73 Å. Cl1- is bonded in a linear geometry to one Na1+ and one Ce3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na2PrCuCl6 by Materials Project

(Na)2PrCuCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight natrium molecules and one PrCuCl6 framework. In the PrCuCl6 framework, Pr3+ is bonded to six equivalent Cl1- atoms to form PrCl6 octahedra that share corners with six equivalent CuCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pr–Cl bond lengths are 2.73 Å. Cu1+ is bonded to six equivalent Cl1- atoms to form CuCl6 octahedra that share corners with six equivalent PrCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cu–Cl bond lengths are 2.51 Å. Cl1- is bonded in a linear geometry to one Pr3+ and one Cu1+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na3TmCl6 by Materials Project

(Na)2NaTmCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight natrium molecules and one NaTmCl6 framework. In the NaTmCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent TmCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.70 Å. Tm3+ is bonded to six equivalent Cl1- atoms to form TmCl6 octahedra that share corners with six equivalent NaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tm–Cl bond lengths are 2.58 Å. Cl1- is bonded in a linear geometry to one Na1+ and one Tm3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on K2TlSbCl6 by Materials Project

(K)2TlSbCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one TlSbCl6 framework. In the TlSbCl6 framework, Tl1+ is bonded to six equivalent Cl1- atoms to form TlCl6 octahedra that share corners with six equivalent SbCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–Cl bond lengths are 3.02 Å. Sb3+ is bonded to six equivalent Cl1- atoms to form SbCl6 octahedra that share corners with six equivalent TlCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–Cl bond lengths are 2.66 Å. Cl1- is bonded in a linear geometry to one Tl1+ and one Sb3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na2GaAgI6 by Materials Project

(Na)2AgGaI6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one AgGaI6 framework. In the AgGaI6 framework, Ag1+ is bonded to six equivalent I1- atoms to form AgI6 octahedra that share corners with six equivalent GaI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ag–I bond lengths are 2.96 Å. Ga3+ is bonded to six equivalent I1- atoms to form GaI6 octahedra that share corners with six equivalent AgI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ga–I bond lengths are 2.84 Å. I1- is bonded in a linear geometry to one Ag1+ and one Ga3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on LaMg2TiO6 by Materials Project

(Mg)2LaTiO6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight magnesium molecules and one LaTiO6 framework. In the LaTiO6 framework, La is bonded to six equivalent O atoms to form LaO6 octahedra that share corners with six equivalent TiO6 octahedra. The corner-sharing octahedral tilt angles are 0°. All La–O bond lengths are 2.28 Å. Ti is bonded to six equivalent O atoms to form TiO6 octahedra that share corners with six equivalent LaO6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ti–O bond lengths are 1.94 Å. O is bonded in a linear geometry to one La and one Ti atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na3SmCl6 by Materials Project

(Na)2NaSmCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one NaSmCl6 framework. In the NaSmCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent SmCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.70 Å. Sm3+ is bonded to six equivalent Cl1- atoms to form SmCl6 octahedra that share corners with six equivalent NaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sm–Cl bond lengths are 2.68 Å. Cl1- is bonded in a linear geometry to one Na1+ and one Sm3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on NaIn(NF3)2 by Materials Project

NaInF6N2 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight ammonia molecules and one NaInF6 framework. In the NaInF6 framework, Na1+ is bonded to six equivalent F1- atoms to form NaF6 octahedra that share corners with six equivalent InF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–F bond lengths are 2.25 Å. In3+ is bonded to six equivalent F1- atoms to form InF6 octahedra that share corners with six equivalent NaF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–F bond lengths are 2.10 Å. F1- is bonded in a linear geometry to one Na1+ and one In3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Na2LiPrCl6 by Materials Project

(Na)2LiPrCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight sodium molecules and one LiPrCl6 framework. In the LiPrCl6 framework, Li1+ is bonded to six equivalent Cl1- atoms to form LiCl6 octahedra that share corners with six equivalent PrCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Li–Cl bond lengths are 2.53 Å. Pr3+ is bonded to six equivalent Cl1- atoms to form PrCl6 octahedra that share corners with six equivalent LiCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Pr–Cl bond lengths are 2.73 Å. Cl1- is bonded in a linear geometry to one Li1+ and one Pr3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on K2RbAsI6 by Materials Project

(K)2RbAsI6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one RbAsI6 framework. In the RbAsI6 framework, Rb1+ is bonded to six equivalent I1- atoms to form RbI6 octahedra that share corners with six equivalent AsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–I bond lengths are 3.45 Å. As3+ is bonded to six equivalent I1- atoms to form AsI6 octahedra that share corners with six equivalent RbI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All As–I bond lengths are 2.87 Å. I1- is bonded in a linear geometry to one Rb1+ and one As3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li2CuSbF6 by Materials Project

(Li)2CuSbF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight lithium molecules and one CuSbF6 framework. In the CuSbF6 framework, Cu1+ is bonded to six equivalent F1- atoms to form CuF6 octahedra that share corners with six equivalent SbF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cu–F bond lengths are 2.14 Å. Sb3+ is bonded to six equivalent F1- atoms to form SbF6 octahedra that share corners with six equivalent CuF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–F bond lengths are 2.19 Å. F1- is bonded in a linear geometry to one Cu1+ and one Sb3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on K2RbInBr6 by Materials Project

(K)2RbInBr6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one RbInBr6 framework. In the RbInBr6 framework, Rb1+ is bonded to six equivalent Br1- atoms to form RbBr6 octahedra that share corners with six equivalent InBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–Br bond lengths are 3.23 Å. In3+ is bonded to six equivalent Br1- atoms to form InBr6 octahedra that share corners with six equivalent RbBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–Br bond lengths are 2.70 Å. Br1- is bonded in a linear geometry to one Rb1+ and one In3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on K2RbTlBr6 by Materials Project

(K)2RbTlBr6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one RbTlBr6 framework. In the RbTlBr6 framework, Rb1+ is bonded to six equivalent Br1- atoms to form RbBr6 octahedra that share corners with six equivalent TlBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–Br bond lengths are 3.23 Å. Tl3+ is bonded to six equivalent Br1- atoms to form TlBr6 octahedra that share corners with six equivalent RbBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–Br bond lengths are 2.77 Å. Br1- is bonded in a linear geometry to one Rb1+ and one Tl3+ atom.

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