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At least 397 records · Page 22

Materials Data on CdHgO2 by Materials Project

CdO(HgO) crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Hg2+ is bonded in a linear geometry to two equivalent O2- atoms. Both Hg–O bond lengths are 2.02 Å. Cd2+ is bonded to six equivalent O2- atoms to form edge-sharing CdO6 octahedra. All Cd–O bond lengths are 2.36 Å. O2- is bonded to one Hg2+ and three equivalent Cd2+ atoms to form a mixture of distorted edge and corner-sharing OCd3Hg tetrahedra.

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Materials Data on AlAgO2 by Materials Project

AgAlO2 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ag1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Ag–O bond lengths are 2.14 Å. Al3+ is bonded to six equivalent O2- atoms to form edge-sharing AlO6 octahedra. All Al–O bond lengths are 1.94 Å. O2- is bonded to one Ag1+ and three equivalent Al3+ atoms to form a mixture of distorted edge and corner-sharing OAl3Ag tetrahedra.

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Materials Data on AgBiO2 by Materials Project

AgBiO2 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. Ag1+ is bonded in a linear geometry to two O2- atoms. There are one shorter (2.09 Å) and one longer (2.10 Å) Ag–O bond lengths. Bi3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Bi–O bond distances ranging from 2.20–2.80 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Ag1+ and three equivalent Bi3+ atoms. In the second O2- site, O2- is bonded to one Ag1+ and three equivalent Bi3+ atoms to form a mixture of distorted corner and edge-sharing OAgBi3 tetrahedra.

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Materials Data on PbAuO2 by Materials Project

AuPbO2 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Au2+ is bonded in a linear geometry to two equivalent O2- atoms. Both Au–O bond lengths are 2.01 Å. Pb2+ is bonded to six equivalent O2- atoms to form edge-sharing PbO6 octahedra. All Pb–O bond lengths are 2.44 Å. O2- is bonded to one Au2+ and three equivalent Pb2+ atoms to form a mixture of distorted edge and corner-sharing OPb3Au tetrahedra.

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Materials Data on TlCuO2 by Materials Project

CuTlO2 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Cu1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Cu–O bond lengths are 1.82 Å. Tl3+ is bonded to six equivalent O2- atoms to form edge-sharing TlO6 octahedra. All Tl–O bond lengths are 2.33 Å. O2- is bonded to one Cu1+ and three equivalent Tl3+ atoms to form a mixture of distorted corner and edge-sharing OTl3Cu tetrahedra.

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Materials Data on CuBiO2 by Materials Project

CuBiO2 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. Cu1+ is bonded in a linear geometry to two O2- atoms. Both Cu–O bond lengths are 1.84 Å. Bi3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Bi–O bond distances ranging from 2.21–2.72 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Cu1+ and three equivalent Bi3+ atoms. In the second O2- site, O2- is bonded to one Cu1+ and three equivalent Bi3+ atoms to form a mixture of distorted corner and edge-sharing OCuBi3 tetrahedra.

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Materials Data on BiAuO2 by Materials Project

AuBiO2 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. Au1+ is bonded in a linear geometry to two O2- atoms. Both Au–O bond lengths are 2.05 Å. Bi3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Bi–O bond distances ranging from 2.24–2.69 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to one Au1+ and three equivalent Bi3+ atoms to form a mixture of distorted edge and corner-sharing OBi3Au tetrahedra. In the second O2- site, O2- is bonded to one Au1+ and three equivalent Bi3+ atoms to form a mixture of distorted edge and corner-sharing OBi3Au tetrahedra.

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Materials Data on ReC2 by Materials Project

ReC2 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Re6+ is bonded in a linear geometry to two equivalent C3- atoms. Both Re–C bond lengths are 2.36 Å. C3- is bonded to one Re6+ and three equivalent C3- atoms to form corner-sharing CReC3 tetrahedra. All C–C bond lengths are 1.52 Å.

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Materials Data on CeSi2Mo2C by Materials Project

CeMo2Si2C crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Ce3+ is bonded in a distorted linear geometry to eight equivalent Si4- and two equivalent C4- atoms. All Ce–Si bond lengths are 3.21 Å. Both Ce–C bond lengths are 2.68 Å. Mo+4.50+ is bonded to four equivalent Si4- and two equivalent C4- atoms to form a mixture of distorted corner, edge, and face-sharing MoSi4C2 octahedra. The corner-sharing octahedral tilt angles are 0°. All Mo–Si bond lengths are 2.59 Å. Both Mo–C bond lengths are 2.11 Å. Si4- is bonded in a 9-coordinate geometry to four equivalent Ce3+, four equivalent Mo+4.50+, and one Si4- atom. The Si–Si bond length is 2.35 Å. C4- is bonded to two equivalent Ce3+ and four equivalent Mo+4.50+ atoms to form corner-sharing CCe2Mo4 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on LaAl2BRu2 by Materials Project

LaRu2Al2B crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. La is bonded in a distorted linear geometry to two equivalent B atoms. Both La–B bond lengths are 2.84 Å. Ru is bonded to four equivalent Al and two equivalent B atoms to form a mixture of corner, edge, and face-sharing RuAl4B2 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ru–Al bond lengths are 2.56 Å. Both Ru–B bond lengths are 2.11 Å. Al is bonded in a 4-coordinate geometry to four equivalent Ru atoms. B is bonded to two equivalent La and four equivalent Ru atoms to form corner-sharing BLa2Ru4 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on HoCr2Si2C by Materials Project

HoCr2Si2C crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Ho3+ is bonded in a distorted linear geometry to eight equivalent Si4- and two equivalent C4- atoms. All Ho–Si bond lengths are 3.04 Å. Both Ho–C bond lengths are 2.61 Å. Cr+4.50+ is bonded in a distorted linear geometry to four equivalent Si4- and two equivalent C4- atoms. All Cr–Si bond lengths are 2.43 Å. Both Cr–C bond lengths are 1.98 Å. Si4- is bonded in a 9-coordinate geometry to four equivalent Ho3+, four equivalent Cr+4.50+, and one Si4- atom. The Si–Si bond length is 2.39 Å. C4- is bonded to two equivalent Ho3+ and four equivalent Cr+4.50+ atoms to form corner-sharing CHo2Cr4 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on CuAgS by Materials Project

AgCuS crystallizes in the orthorhombic Cmc2_1 space group. The structure is three-dimensional. Ag1+ is bonded in a linear geometry to two equivalent S2- atoms. There are one shorter (2.47 Å) and one longer (2.49 Å) Ag–S bond lengths. Cu1+ is bonded in a trigonal planar geometry to three equivalent S2- atoms. There are two shorter (2.25 Å) and one longer (2.36 Å) Cu–S bond lengths. S2- is bonded in a 5-coordinate geometry to two equivalent Ag1+ and three equivalent Cu1+ atoms.

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Materials Data on LiCa2CuN2 by Materials Project

LiCa2CuN2 crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Li1+ is bonded in a linear geometry to two equivalent N3- atoms. Both Li–N bond lengths are 1.89 Å. Ca2+ is bonded to four equivalent N3- atoms to form a mixture of edge and corner-sharing CaN4 tetrahedra. All Ca–N bond lengths are 2.50 Å. Cu1+ is bonded in a linear geometry to two equivalent N3- atoms. Both Cu–N bond lengths are 1.86 Å. N3- is bonded to one Li1+, four equivalent Ca2+, and one Cu1+ atom to form a mixture of edge and corner-sharing NLiCa4Cu octahedra. The corner-sharing octahedra tilt angles range from 0–64°.

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Materials Data on SmCr2Si2C by Materials Project

SmCr2Si2C crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Sm3+ is bonded in a distorted linear geometry to eight equivalent Si4- and two equivalent C4- atoms. All Sm–Si bond lengths are 3.07 Å. Both Sm–C bond lengths are 2.66 Å. Cr+4.50+ is bonded in a distorted linear geometry to four equivalent Si4- and two equivalent C4- atoms. All Cr–Si bond lengths are 2.45 Å. Both Cr–C bond lengths are 1.99 Å. Si4- is bonded in a 9-coordinate geometry to four equivalent Sm3+, four equivalent Cr+4.50+, and one Si4- atom. The Si–Si bond length is 2.46 Å. C4- is bonded to two equivalent Sm3+ and four equivalent Cr+4.50+ atoms to form corner-sharing CSm2Cr4 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on DyTiFe11C by Materials Project

DyTiFe11C crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. Dy is bonded in a distorted linear geometry to one Ti, ten Fe, and two equivalent C atoms. The Dy–Ti bond length is 3.18 Å. There are a spread of Dy–Fe bond distances ranging from 3.07–3.30 Å. Both Dy–C bond lengths are 2.43 Å. Ti is bonded in a 1-coordinate geometry to one Dy and thirteen Fe atoms. There are a spread of Ti–Fe bond distances ranging from 2.35–2.94 Å. There are six inequivalent Fe sites. In the first Fe site, Fe is bonded in a single-bond geometry to six Fe and one C atom. There are four shorter (2.46 Å) and two longer (2.63 Å) Fe–Fe bond lengths. The Fe–C bond length is 1.90 Å. In the second Fe site, Fe is bonded in a single-bond geometry to two equivalent Ti, six Fe, and one C atom. There are four shorter (2.48 Å) and two longer (2.65 Å) Fe–Fe bond lengths. The Fe–C bond length is 1.91 Å. In the third Fe site, Fe is bonded in a single-bond geometry to one Ti, six Fe, and one C atom. There are a spread of Fe–Fe bond distances ranging from 2.44–2.70 Å. The Fe–C bond length is 1.89 Å. In the fourth Fe site, Fe is bonded to two equivalent Dy, one Ti, and nine Fe atoms to form distorted FeDy2TiFe9 cuboctahedra that share corners with ten equivalent FeDy2TiFe9 cuboctahedra, corners with two equivalent CDy2Fe4 octahedra, edges with four equivalent FeDy2TiFe9 cuboctahedra, faces with six equivalent FeDy2TiFe9 cuboctahedra, and faces with two equivalent CDy2Fe4 octahedra. The corner-sharing octahedra tilt angles range from 67–69°. There are a spread of Fe–Fe bond distances ranging from 2.42–2.63 Å. In the fifth Fe site, Fe is bonded in a 1-coordinate geometry to one Ti and eight Fe atoms. All Fe–Fe bond lengths are 2.97 Å. In the sixth Fe site, Fe is bonded in a 12-coordinate geometry to one Dy, two equivalent Ti, and eleven Fe atoms. The Fe–Fe bond length is 2.42 Å. C is bonded to two equivalent Dy and four Fe atoms to form CDy2Fe4 octahedra that share corners with eight equivalent FeDy2TiFe9 cuboctahedra, corners with two equivalent CDy2Fe4 octahedra, and faces with eight equivalent FeDy2TiFe9 cuboctahedra. The corner-sharing octahedral tilt angles are 2°.

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Materials Data on LaGa3Fe10C by Materials Project

LaFe10Ga3C crystallizes in the orthorhombic Fmm2 space group. The structure is three-dimensional. La is bonded in a distorted linear geometry to ten Fe, six Ga, and two equivalent C atoms. There are a spread of La–Fe bond distances ranging from 3.46–3.51 Å. There are a spread of La–Ga bond distances ranging from 3.38–3.43 Å. There are one shorter (2.88 Å) and one longer (2.89 Å) La–C bond lengths. There are nine inequivalent Fe sites. In the first Fe site, Fe is bonded in a single-bond geometry to four Fe, three Ga, and one C atom. There are a spread of Fe–Fe bond distances ranging from 2.48–2.60 Å. There are two shorter (2.57 Å) and one longer (2.66 Å) Fe–Ga bond lengths. The Fe–C bond length is 1.85 Å. In the second Fe site, Fe is bonded in a single-bond geometry to four Fe, three Ga, and one C atom. There are a spread of Fe–Fe bond distances ranging from 2.47–2.63 Å. There are a spread of Fe–Ga bond distances ranging from 2.55–2.67 Å. The Fe–C bond length is 1.86 Å. In the third Fe site, Fe is bonded to ten Fe and two equivalent Ga atoms to form FeGa2Fe10 cuboctahedra that share corners with four FeLa2Ga3Fe7 cuboctahedra, corners with four equivalent CLa2Fe4 octahedra, and faces with ten FeLa2Ga3Fe7 cuboctahedra. The corner-sharing octahedral tilt angles are 29°. There are a spread of Fe–Fe bond distances ranging from 2.39–2.49 Å. Both Fe–Ga bond lengths are 2.58 Å. In the fourth Fe site, Fe is bonded to eight Fe and four Ga atoms to form FeGa4Fe8 cuboctahedra that share corners with six FeLa2Ga4Fe6 cuboctahedra, corners with four equivalent CLa2Fe4 octahedra, and faces with ten FeLa2Ga3Fe7 cuboctahedra. The corner-sharing octahedral tilt angles are 30°. There are two shorter (2.42 Å) and two longer (2.43 Å) Fe–Fe bond lengths. There are two shorter (2.58 Å) and two longer (2.59 Å) Fe–Ga bond lengths. In the fifth Fe site, Fe is bonded to two equivalent La, seven Fe, and three Ga atoms to form distorted FeLa2Ga3Fe7 cuboctahedra that share corners with ten FeGa2Fe10 cuboctahedra, corners with two equivalent CLa2Fe4 octahedra, edges with four equivalent FeLa2Ga4Fe6 cuboctahedra, edges with two equivalent CLa2Fe4 octahedra, and faces with ten FeGa2Fe10 cuboctahedra. The corner-sharing octahedral tilt angles are 76°. There are a spread of Fe–Fe bond distances ranging from 2.49–2.55 Å. There are one shorter (2.55 Å) and two longer (2.61 Å) Fe–Ga bond lengths. In the sixth Fe site, Fe is bonded to two equivalent La, six Fe, and four Ga atoms to form distorted FeLa2Ga4Fe6 cuboctahedra that share corners with ten FeGa4Fe8 cuboctahedra, corners with two equivalent CLa2Fe4 octahedra, edges with six FeLa2Ga3Fe7 cuboctahedra, edges with two equivalent CLa2Fe4 octahedra, and faces with nine FeGa2Fe10 cuboctahedra. The corner-sharing octahedral tilt angles are 75°. There are two shorter (2.57 Å) and one longer (2.60 Å) Fe–Fe bond lengths. There are a spread of Fe–Ga bond distances ranging from 2.51–2.59 Å. In the seventh Fe site, Fe is bonded to two equivalent La, seven Fe, and three Ga atoms to form distorted FeLa2Ga3Fe7 cuboctahedra that share corners with twelve FeGa2Fe10 cuboctahedra, corners with two equivalent CLa2Fe4 octahedra, edges with four equivalent FeLa2Ga2Fe8 cuboctahedra, edges with two equivalent CLa2Fe4 octahedra, and faces with eight FeGa4Fe8 cuboctahedra. The corner-sharing octahedral tilt angles are 76°. There are one shorter (2.55 Å) and one longer (2.65 Å) Fe–Fe bond lengths. There are one shorter (2.52 Å) and two longer (2.60 Å) Fe–Ga bond lengths. In the eighth Fe site, Fe is bonded to two equivalent La, eight Fe, and two Ga atoms to form distorted FeLa2Ga2Fe8 cuboctahedra that share corners with ten FeGa4Fe8 cuboctahedra, corners with two equivalent CLa2Fe4 octahedra, edges with four equivalent FeLa2Ga3Fe7 cuboctahedra, edges with two equivalent CLa2Fe4 octahedra, and faces with nine FeGa2Fe10 cuboctahedra. The corner-sharing octahedral tilt angles are 76°. There are two shorter (2.59 Å) and one longer (2.65 Å) Fe–Fe bond lengths. There are one shorter (2.51 Å) and one longer (2.54 Å) Fe–Ga bond lengths. In the ninth Fe site, Fe is bonded to two equivalent La, nine Fe, and one Ga atom to form distorted FeLa2GaFe9 cuboctahedra that share corners with thirteen FeGa4Fe8 cuboctahedra, corners with two equivalent CLa2Fe4 octahedra, edges with two equivalent FeLa2Ga4Fe6 cuboctahedra, faces with eleven FeGa4Fe8 cuboctahedra, and faces with two equivalent CLa2Fe4 octahedra. The corner-sharing octahedral tilt angles are 63°. The Fe–Ga bond length is 2.72 Å. There are three inequivalent Ga sites. In the first Ga site, Ga is bonded in a 12-coordinate geometry to two equivalent La, nine Fe, and one Ga atom. The Ga–Ga bond length is 2.83 Å. In the second Ga site, Ga is bonded in a 12-coordinate geometry to two equivalent La and ten Fe atoms. In the third Ga site, Ga is bonded in a 12-coordinate geometry to two equivalent La, nine Fe, and one Ga atom. C is bonded to two equivalent La and four Fe atoms to form distorted CLa2Fe4 octahedra that share corners with fourteen FeGa2Fe10 cuboctahedra, corners with two equivalent CLa2Fe4 octahedra, edges with eight FeLa2Ga2Fe8 cuboctahedra, and faces with two equivalent FeLa2GaFe9 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on Nb3Al2Mo3 by Materials Project

Nb3Mo3Al2 crystallizes in the trigonal R32 space group. The structure is three-dimensional. Nb is bonded in a distorted linear geometry to two equivalent Mo and four equivalent Al atoms. Both Nb–Mo bond lengths are 2.55 Å. There are two shorter (2.83 Å) and two longer (2.87 Å) Nb–Al bond lengths. Mo is bonded in a 2-coordinate geometry to two equivalent Nb and four equivalent Al atoms. There are two shorter (2.83 Å) and two longer (2.86 Å) Mo–Al bond lengths. Al is bonded to six equivalent Nb and six equivalent Mo atoms to form a mixture of edge and face-sharing AlNb6Mo6 cuboctahedra.

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Materials Data on Cu11PdN4 by Materials Project

PdCu11N4 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Pd is bonded in a distorted linear geometry to four equivalent Cu and two equivalent N atoms. All Pd–Cu bond lengths are 2.62 Å. Both Pd–N bond lengths are 1.87 Å. There are four inequivalent Cu sites. In the first Cu site, Cu is bonded in a linear geometry to four equivalent Cu and two equivalent N atoms. All Cu–Cu bond lengths are 2.65 Å. Both Cu–N bond lengths are 1.87 Å. In the second Cu site, Cu is bonded in a linear geometry to four equivalent Cu and two N atoms. All Cu–Cu bond lengths are 2.65 Å. There is one shorter (1.81 Å) and one longer (1.92 Å) Cu–N bond length. In the third Cu site, Cu is bonded in a linear geometry to four equivalent Cu and two equivalent N atoms. All Cu–Cu bond lengths are 2.64 Å. Both Cu–N bond lengths are 1.87 Å. In the fourth Cu site, Cu is bonded in a distorted single-bond geometry to one Pd and seven Cu atoms. There are three inequivalent N sites. In the first N site, N is bonded in a linear geometry to two equivalent Pd atoms. 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 in a square co-planar geometry to four Cu atoms.

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