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At least 415 records · Page 23

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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Materials Data on Na2LiGdCl6 by Materials Project

(Na)2LiGdCl6 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 LiGdCl6 framework. In the LiGdCl6 framework, Li1+ is bonded to six equivalent Cl1- atoms to form LiCl6 octahedra that share corners with six equivalent GdCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Li–Cl bond lengths are 2.52 Å. Gd3+ is bonded to six equivalent Cl1- atoms to form GdCl6 octahedra that share corners with six equivalent LiCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Gd–Cl bond lengths are 2.64 Å. Cl1- is bonded in a linear geometry to one Li1+ and one Gd3+ atom.

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Materials Data on Na3PrCl6 by Materials Project

(Na)2NaPrCl6 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 NaPrCl6 framework. In the NaPrCl6 framework, Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent PrCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.71 Å. Pr3+ is bonded to six equivalent Cl1- atoms to form PrCl6 octahedra that share corners with six equivalent NaCl6 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 Na1+ and one Pr3+ atom.

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Materials Data on Cs3BiBr6 by Materials Project

(Cs)2CsBiBr6 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 CsBiBr6 framework. In the CsBiBr6 framework, Cs1+ is bonded to six equivalent Br1- atoms to form CsBr6 octahedra that share corners with six equivalent BiBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Br bond lengths are 3.42 Å. Bi3+ is bonded to six equivalent Br1- atoms to form BiBr6 octahedra that share corners with six equivalent CsBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Bi–Br bond lengths are 2.87 Å. Br1- is bonded in a linear geometry to one Cs1+ and one Bi3+ atom.

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Materials Data on K3AsI6 by Materials Project

(K)2KAsI6 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 KAsI6 framework. In the KAsI6 framework, K1+ is bonded to six equivalent I1- atoms to form KI6 octahedra that share corners with six equivalent AsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All K–I bond lengths are 3.35 Å. As3+ is bonded to six equivalent I1- atoms to form AsI6 octahedra that share corners with six equivalent KI6 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 K1+ and one As3+ atom.

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Materials Data on CsK2InCl6 by Materials Project

(K)2CsInCl6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight kalium molecules and one CsInCl6 framework. In the CsInCl6 framework, Cs1+ is bonded to six equivalent Cl1- atoms to form CsCl6 octahedra that share corners with six equivalent InCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Cl bond lengths are 3.22 Å. In3+ is bonded to six equivalent Cl1- atoms to form InCl6 octahedra that share corners with six equivalent CsCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–Cl bond lengths are 2.54 Å. Cl1- is bonded in a linear geometry to one Cs1+ and one In3+ atom.

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Materials Data on WO3 by Materials Project

WO3 is High-temperature superconductor-like structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form corner-sharing WO6 octahedra. The corner-sharing octahedra tilt angles range from 4–7°. There are a spread of W–O bond distances ranging from 1.85–2.04 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the third O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. There is one shorter (1.86 Å) and one longer (2.02 Å) O–W bond length. In the fifth O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the sixth O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms.

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Materials Data on NaLi2TiF6 by Materials Project

(Li)2NaTiF6 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 NaTiF6 framework. In the NaTiF6 framework, Na1+ is bonded to six equivalent F1- atoms to form NaF6 octahedra that share corners with six equivalent TiF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Na–F bond lengths are 2.17 Å. Ti3+ is bonded to six equivalent F1- atoms to form TiF6 octahedra that share corners with six equivalent NaF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ti–F bond lengths are 1.96 Å. F1- is bonded in a linear geometry to one Na1+ and one Ti3+ atom.

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Materials Data on Na2GaHgBr6 by Materials Project

(Na)2HgGaBr6 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 HgGaBr6 framework. In the HgGaBr6 framework, Hg1+ is bonded to six equivalent Br1- atoms to form HgBr6 octahedra that share corners with six equivalent GaBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Hg–Br bond lengths are 2.87 Å. Ga3+ is bonded to six equivalent Br1- atoms to form GaBr6 octahedra that share corners with six equivalent HgBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ga–Br bond lengths are 2.61 Å. Br1- is bonded in a linear geometry to one Hg1+ and one Ga3+ atom.

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Materials Data on K2InSbI6 by Materials Project

(K)2InSbI6 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 InSbI6 framework. In the InSbI6 framework, In1+ is bonded to six equivalent I1- atoms to form InI6 octahedra that share corners with six equivalent SbI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–I bond lengths are 3.20 Å. Sb3+ is bonded to six equivalent I1- atoms to form SbI6 octahedra that share corners with six equivalent InI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–I bond lengths are 3.04 Å. I1- is bonded in a linear geometry to one In1+ and one Sb3+ atom.

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Materials Data on HfFeF6 by Materials Project

HfFeF6 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 FeF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Hf–F bond lengths are 2.01 Å. Fe2+ is bonded to six equivalent F1- atoms to form FeF6 octahedra that share corners with six equivalent HfF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Fe–F bond lengths are 2.08 Å. F1- is bonded in a linear geometry to one Hf4+ and one Fe2+ atom.

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Materials Data on Cs3TlI6 by Materials Project

(Cs)2CsTlI6 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 CsTlI6 framework. In the CsTlI6 framework, Cs1+ is bonded to six equivalent I1- atoms to form CsI6 octahedra that share corners with six equivalent TlI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–I bond lengths are 3.61 Å. Tl3+ is bonded to six equivalent I1- atoms to form TlI6 octahedra that share corners with six equivalent CsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–I bond lengths are 3.02 Å. I1- is bonded in a linear geometry to one Cs1+ and one Tl3+ atom.

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