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At least 631 records · Page 35

Materials Data on Li3InCl6 by Materials Project

Li3InCl6 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 LiInCl6 framework. In the LiInCl6 framework, Li1+ is bonded to six equivalent Cl1- atoms to form LiCl6 octahedra that share corners with six equivalent InCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Li–Cl bond lengths are 2.50 Å. In3+ is bonded to six equivalent Cl1- atoms to form InCl6 octahedra that share corners with six equivalent LiCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–Cl bond lengths are 2.52 Å. Cl1- is bonded in a linear geometry to one Li1+ and one In3+ atom.

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Materials Data on Cs3BiI6 by Materials Project

(Cs)2CsBiI6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsBiI6 framework. In the CsBiI6 framework, Cs1+ is bonded to six equivalent I1- atoms to form CsI6 octahedra that share corners with six equivalent BiI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–I bond lengths are 3.63 Å. Bi3+ is bonded to six equivalent I1- atoms to form BiI6 octahedra that share corners with six equivalent CsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Bi–I bond lengths are 3.09 Å. I1- is bonded in a linear geometry to one Cs1+ and one Bi3+ atom.

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Materials Data on Na2LiNdCl6 by Materials Project

(Na)2LiNdCl6 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 LiNdCl6 framework. In the LiNdCl6 framework, Li1+ is bonded to six equivalent Cl1- atoms to form LiCl6 octahedra that share corners with six equivalent NdCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Li–Cl bond lengths are 2.53 Å. Nd3+ is bonded to six equivalent Cl1- atoms to form NdCl6 octahedra that share corners with six equivalent LiCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Nd–Cl bond lengths are 2.71 Å. Cl1- is bonded in a linear geometry to one Li1+ and one Nd3+ atom.

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Materials Data on K2TlSbBr6 by Materials Project

(K)2TlSbBr6 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 TlSbBr6 framework. In the TlSbBr6 framework, Tl1+ is bonded to six equivalent Br1- atoms to form TlBr6 octahedra that share corners with six equivalent SbBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–Br bond lengths are 3.12 Å. Sb3+ is bonded to six equivalent Br1- atoms to form SbBr6 octahedra that share corners with six equivalent TlBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–Br bond lengths are 2.81 Å. Br1- is bonded in a linear geometry to one Tl1+ and one Sb3+ atom.

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Materials Data on Na2AgAsCl6 by Materials Project

(Na)2AgAsCl6 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 AgAsCl6 framework. In the AgAsCl6 framework, Ag1+ is bonded to six equivalent Cl1- atoms to form AgCl6 octahedra that share corners with six equivalent AsCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ag–Cl bond lengths are 2.66 Å. As3+ is bonded to six equivalent Cl1- atoms to form AsCl6 octahedra that share corners with six equivalent AgCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All As–Cl bond lengths are 2.50 Å. Cl1- is bonded in a linear geometry to one Ag1+ and one As3+ atom.

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Materials Data on Na2TlHgF6 by Materials Project

(Na)2HgTlF6 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 HgTlF6 framework. In the HgTlF6 framework, Hg1+ is bonded to six equivalent F1- atoms to form HgF6 octahedra that share corners with six equivalent TlF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Hg–F bond lengths are 2.31 Å. Tl3+ is bonded to six equivalent F1- atoms to form TlF6 octahedra that share corners with six equivalent HgF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–F bond lengths are 2.29 Å. F1- is bonded in a linear geometry to one Hg1+ and one Tl3+ atom.

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Materials Data on Na3TbCl6 by Materials Project

(Na)2NaTbCl6 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 NaTbCl6 framework. In the NaTbCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent TbCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.70 Å. Tb3+ is bonded to six equivalent Cl1- atoms to form TbCl6 octahedra that share corners with six equivalent NaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tb–Cl bond lengths are 2.63 Å. Cl1- is bonded in a linear geometry to one Na1+ and one Tb3+ atom.

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Materials Data on Na2LiEuCl6 by Materials Project

(Na)2LiEuCl6 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 LiEuCl6 framework. In the LiEuCl6 framework, Li1+ is bonded to six equivalent Cl1- atoms to form LiCl6 octahedra that share corners with six equivalent EuCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Li–Cl bond lengths are 2.51 Å. Eu3+ is bonded to six equivalent Cl1- atoms to form EuCl6 octahedra that share corners with six equivalent LiCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Eu–Cl bond lengths are 2.68 Å. Cl1- is bonded in a linear geometry to one Li1+ and one Eu3+ atom.

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Materials Data on K2RbDyCl6 by Materials Project

(K)2RbDyCl6 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 RbDyCl6 framework. In the RbDyCl6 framework, Rb1+ is bonded to six equivalent Cl1- atoms to form RbCl6 octahedra that share corners with six equivalent DyCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–Cl bond lengths are 3.10 Å. Dy3+ is bonded to six equivalent Cl1- atoms to form DyCl6 octahedra that share corners with six equivalent RbCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Dy–Cl bond lengths are 2.63 Å. Cl1- is bonded in a linear geometry to one Rb1+ and one Dy3+ atom.

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Materials Data on HfMnF6 by Materials Project

HfMnF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Hf4+ is bonded to six equivalent F1- atoms to form HfF6 octahedra that share corners with six equivalent MnF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Hf–F bond lengths are 2.01 Å. Mn2+ is bonded to six equivalent F1- atoms to form MnF6 octahedra that share corners with six equivalent HfF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Mn–F bond lengths are 2.14 Å. F1- is bonded in a linear geometry to one Hf4+ and one Mn2+ atom.

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Materials Data on TiOF2 by Materials Project

TiOF2 is High-temperature superconductor-derived structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Ti4+ is bonded to two equivalent O2- and four equivalent F1- atoms to form corner-sharing TiO2F4 octahedra. The corner-sharing octahedral tilt angles are 0°. Both Ti–O bond lengths are 1.85 Å. All Ti–F bond lengths are 1.97 Å. O2- is bonded in a linear geometry to two equivalent Ti4+ atoms. F1- is bonded in a linear geometry to two equivalent Ti4+ atoms.

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Materials Data on Na2LiSmCl6 by Materials Project

(Na)2LiSmCl6 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 LiSmCl6 framework. In the LiSmCl6 framework, Li1+ is bonded to six equivalent Cl1- atoms to form LiCl6 octahedra that share corners with six equivalent SmCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Li–Cl bond lengths are 2.53 Å. Sm3+ is bonded to six equivalent Cl1- atoms to form SmCl6 octahedra that share corners with six equivalent LiCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sm–Cl bond lengths are 2.67 Å. Cl1- is bonded in a linear geometry to one Li1+ and one Sm3+ atom.

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Materials Data on NaAsF6 by Materials Project

NaAsF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Na1+ is bonded to six equivalent F1- atoms to form NaF6 octahedra that share corners with six equivalent AsF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–F bond lengths are 2.30 Å. As5+ is bonded to six equivalent F1- atoms to form AsF6 octahedra that share corners with six equivalent NaF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All As–F bond lengths are 1.77 Å. F1- is bonded in a linear geometry to one Na1+ and one As5+ atom.

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Materials Data on Cu23PdN8 by Materials Project

PdCu23N8 is High-temperature superconductor-derived structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Pd is bonded in a linear geometry to two equivalent N atoms. Both Pd–N bond lengths are 2.04 Å. There are fifteen inequivalent Cu sites. In the first Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the second Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the third Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the fourth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the fifth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the sixth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the seventh Cu site, Cu is bonded in a linear geometry to two N atoms. There is one shorter (1.90 Å) and one longer (1.91 Å) Cu–N bond length. In the eighth Cu site, Cu is bonded in a linear geometry to two equivalent N atoms. Both Cu–N bond lengths are 1.93 Å. In the ninth Cu site, Cu is bonded in a linear geometry to two equivalent N atoms. Both Cu–N bond lengths are 1.93 Å. In the tenth Cu site, Cu is bonded in a linear geometry to two equivalent N atoms. Both Cu–N bond lengths are 1.83 Å. In the eleventh Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the twelfth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the thirteenth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the fourteenth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the fifteenth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. There are three inequivalent N sites. In the first N site, N is bonded to one Pd and five Cu atoms to form corner-sharing NCu5Pd octahedra. The corner-sharing octahedra tilt angles range from 0–2°. In the second N site, N is bonded to six Cu atoms to form corner-sharing NCu6 octahedra. The corner-sharing octahedra tilt angles range from 0–2°. In the third N site, N is bonded to six Cu atoms to form corner-sharing NCu6 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on K3LaCl6 by Materials Project

(K)2KLaCl6 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 KLaCl6 framework. In the KLaCl6 framework, K1+ is bonded to six equivalent Cl1- atoms to form KCl6 octahedra that share corners with six equivalent LaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All K–Cl bond lengths are 2.99 Å. La3+ is bonded to six equivalent Cl1- atoms to form LaCl6 octahedra that share corners with six equivalent KCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All La–Cl bond lengths are 2.77 Å. Cl1- is bonded in a linear geometry to one K1+ and one La3+ atom.

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Materials Data on LiTaF6 by Materials Project

LiTaF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li1+ is bonded to six equivalent F1- atoms to form LiF6 octahedra that share corners with six equivalent TaF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Li–F bond lengths are 2.07 Å. Ta5+ is bonded to six equivalent F1- atoms to form TaF6 octahedra that share corners with six equivalent LiF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ta–F bond lengths are 1.92 Å. F1- is bonded in a linear geometry to one Li1+ and one Ta5+ atom.

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Materials Data on ZrMnF6 by Materials Project

MnZrF6 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 MnF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Zr–F bond lengths are 2.04 Å. Mn2+ is bonded to six equivalent F1- atoms to form MnF6 octahedra that share corners with six equivalent ZrF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Mn–F bond lengths are 2.14 Å. F1- is bonded in a linear geometry to one Zr4+ and one Mn2+ atom.

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Materials Data on Cu11PdN4 by Materials Project

PdCu11N4 is High-temperature superconductor-derived structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Pd is bonded in a linear geometry to two equivalent N atoms. Both Pd–N bond lengths are 1.96 Å. There are eight inequivalent Cu sites. In the first Cu site, Cu is bonded in a linear geometry to two equivalent N atoms. Both Cu–N bond lengths are 1.96 Å. In the second Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the third Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the fourth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the fifth Cu site, Cu is bonded in a linear geometry to two N atoms. Both Cu–N bond lengths are 1.90 Å. In the sixth Cu site, Cu is bonded in a linear geometry to two equivalent N atoms. Both Cu–N bond lengths are 1.96 Å. In the seventh Cu site, Cu is bonded in a linear geometry to two N atoms. There is one shorter (1.90 Å) and one longer (1.91 Å) Cu–N bond length. In the eighth Cu site, Cu is bonded in a linear geometry to two N atoms. There is one shorter (1.90 Å) and one longer (1.91 Å) Cu–N bond length. There are three inequivalent N sites. In the first N site, N is bonded to two equivalent Pd and four Cu atoms to form corner-sharing NCu4Pd2 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second N site, N is bonded to six Cu atoms to form corner-sharing NCu6 octahedra. The corner-sharing octahedral tilt angles are 0°. In the third N site, N is bonded to six Cu atoms to form corner-sharing NCu6 octahedra. The corner-sharing octahedral tilt angles are 0°.

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