cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1283128
title: Materials Data on Lu4Hf3O12 by Materials Project

description: Lu4Hf3O12 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are four inequivalent Lu3+ sites. In the first Lu3+ site, Lu3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Lu–O bond distances ranging from 2.15–2.52 Å. In the second Lu3+ site, Lu3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Lu–O bond distances ranging from 2.15–2.64 Å. In the third Lu3+ site, Lu3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Lu–O bond distances ranging from 2.17–2.61 Å. In the fourth Lu3+ site, Lu3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Lu–O bond distances ranging from 2.19–2.61 Å. There are three inequivalent Hf4+ sites. In the first Hf4+ site, Hf4+ is bonded in an octahedral geometry to six O2- atoms. There are a spread of Hf–O bond distances ranging from 2.07–2.11 Å. In the second Hf4+ site, Hf4+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Hf–O bond distances ranging from 2.07–2.50 Å. In the third Hf4+ site, Hf4+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Hf–O bond distances ranging from 2.07–2.18 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two Lu3+ and two Hf4+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Lu3+ and two Hf4+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two Lu3+ and two Hf4+ atoms. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Lu3+ and two Hf4+ atoms. In the fifth O2- site, O2- is bonded to two Lu3+ and two equivalent Hf4+ atoms to form distorted OLu2Hf2 tetrahedra that share corners with six OLu3Hf tetrahedra and edges with three OLu2Hf2 tetrahedra. In the sixth O2- site, O2- is bonded to three Lu3+ and one Hf4+ atom to form a mixture of distorted corner and edge-sharing OLu3Hf tetrahedra. In the seventh O2- site, O2- is bonded to three Lu3+ and one Hf4+ atom to form a mixture of corner and edge-sharing OLu3Hf tetrahedra. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to three Lu3+ and one Hf4+ atom. In the ninth O2- site, O2- is bonded to three Lu3+ and one Hf4+ atom to form a mixture of distorted corner and edge-sharing OLu3Hf tetrahedra. In the tenth O2- site, O2- is bonded to two Lu3+ and two equivalent Hf4+ atoms to form a mixture of distorted corner and edge-sharing OLu2Hf2 tetrahedra. In the eleventh O2- site, O2- is bonded in a 4-coordinate geometry to two Lu3+ and two Hf4+ atoms. In the twelfth O2- site, O2- is bonded to three Lu3+ and one Hf4+ atom to form OLu3Hf tetrahedra that share corners with six OLu2Hf2 tetrahedra and edges with three OLu3Hf tetrahedra.
DOI: 10.17188/1283130
title: Materials Data on KBa2DyBi2O9 by Materials Project

description: K2Ba4Dy2(BiO6)3Bi crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional and consists of one bismuth molecule and one K2Ba4Dy2(BiO6)3 framework. In the K2Ba4Dy2(BiO6)3 framework, K1+ is bonded in a distorted hexagonal planar geometry to six O2- atoms. There are three shorter (2.59 Å) and three longer (3.18 Å) K–O bond lengths. There are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a distorted trigonal non-coplanar geometry to three equivalent O2- atoms. All Ba–O bond lengths are 2.48 Å. In the second Ba2+ site, Ba2+ is bonded in a distorted hexagonal planar geometry to six O2- atoms. There are three shorter (2.58 Å) and three longer (2.67 Å) Ba–O bond lengths. Dy3+ is bonded to six O2- atoms to form corner-sharing DyO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (2.27 Å) and three longer (2.43 Å) Dy–O bond lengths. There are two inequivalent Bi5+ sites. In the first Bi5+ site, Bi5+ is bonded in an octahedral geometry to six equivalent O2- atoms. All Bi–O bond lengths are 2.09 Å. In the second Bi5+ site, Bi5+ is bonded in a trigonal non-coplanar geometry to three equivalent O2- atoms. All Bi–O bond lengths are 2.17 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to two equivalent Dy3+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to two Ba2+ and one Bi5+ atom. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one K1+, one Ba2+, and one Dy3+ atom. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent K1+ and two equivalent Bi5+ atoms.
DOI: 10.17188/1283131
title: Materials Data on Ba4Ta2TiZnO12 by Materials Project

description: Ba4TiTa2ZnO12 is (Cubic) Perovskite-derived structured and crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve equivalent BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, faces with two equivalent TiO6 octahedra, faces with two equivalent ZnO6 octahedra, and faces with four equivalent TaO6 octahedra. There are a spread of Ba–O bond distances ranging from 2.85–2.95 Å. Ti4+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with six equivalent TaO6 octahedra and faces with eight equivalent BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–3°. There are two shorter (1.98 Å) and four longer (2.04 Å) Ti–O bond lengths. Ta5+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with three equivalent TiO6 octahedra, corners with three equivalent ZnO6 octahedra, and faces with eight equivalent BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–4°. There are a spread of Ta–O bond distances ranging from 1.94–2.14 Å. Zn2+ is bonded to six O2- atoms to form ZnO6 octahedra that share corners with six equivalent TaO6 octahedra and faces with eight equivalent BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–4°. There are four shorter (2.13 Å) and two longer (2.22 Å) Zn–O bond lengths. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to four equivalent Ba2+, one Ta5+, and one Zn2+ atom. In the second O2- site, O2- is bonded in a distorted linear geometry to four equivalent Ba2+, one Ta5+, and one Zn2+ atom. In the third O2- site, O2- is bonded in a distorted linear geometry to four equivalent Ba2+, one Ti4+, and one Ta5+ atom. In the fourth O2- site, O2- is bonded in a distorted linear geometry to four equivalent Ba2+, one Ti4+, and one Ta5+ atom.
DOI: 10.17188/1283132
title: Materials Data on Rb2CeO3 by Materials Project

description: Rb2CeO3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are three inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded to six O2- atoms to form distorted RbO6 octahedra that share corners with two equivalent RbO6 octahedra, corners with four equivalent CeO6 octahedra, edges with two equivalent RbO6 octahedra, and edges with four equivalent CeO6 octahedra. The corner-sharing octahedra tilt angles range from 18–25°. There are two shorter (2.73 Å) and four longer (3.15 Å) Rb–O bond lengths. In the second Rb1+ site, Rb1+ is bonded to six O2- atoms to form distorted RbO6 octahedra that share corners with two equivalent RbO6 octahedra, edges with two equivalent RbO6 octahedra, and edges with six equivalent CeO6 octahedra. The corner-sharing octahedral tilt angles are 25°. There are two shorter (2.83 Å) and four longer (2.84 Å) Rb–O bond lengths. In the third Rb1+ site, Rb1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Rb–O bond distances ranging from 2.75–3.18 Å. Ce4+ is bonded to six O2- atoms to form distorted CeO6 octahedra that share corners with two equivalent RbO6 octahedra, edges with three equivalent CeO6 octahedra, and edges with five RbO6 octahedra. The corner-sharing octahedral tilt angles are 18°. There are two shorter (2.31 Å) and four longer (2.32 Å) Ce–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to four Rb1+ and two equivalent Ce4+ atoms. In the second O2- site, O2- is bonded in a 6-coordinate geometry to four Rb1+ and two equivalent Ce4+ atoms.
DOI: 10.17188/1283134
title: Materials Data on NaClO2 by Materials Project

description: NaClO2 crystallizes in the triclinic P1 space group. The structure is two-dimensional and consists of one NaClO2 sheet oriented in the (1, 1, 0) direction. there are two inequivalent Na sites. In the first Na site, Na is bonded in a 4-coordinate geometry to four O atoms. There are a spread of Na–O bond distances ranging from 2.33–2.48 Å. In the second Na site, Na is bonded in a 4-coordinate geometry to four O atoms. There are a spread of Na–O bond distances ranging from 2.34–2.47 Å. There are four inequivalent O sites. In the first O site, O is bonded in a distorted T-shaped geometry to two Na and one Cl atom. The O–Cl bond length is 1.58 Å. In the second O site, O is bonded in a distorted T-shaped geometry to two Na and one Cl atom. The O–Cl bond length is 1.58 Å. In the third O site, O is bonded in a distorted T-shaped geometry to two Na and one Cl atom. The O–Cl bond length is 1.58 Å. In the fourth O site, O is bonded in a distorted T-shaped geometry to two Na and one Cl atom. The O–Cl bond length is 1.58 Å. There are two inequivalent Cl sites. In the first Cl site, Cl is bonded in a water-like geometry to two O atoms. In the second Cl site, Cl is bonded in a water-like geometry to two O atoms.
DOI: 10.17188/1283135
title: Materials Data on In2AsSe by Materials Project

description: In2AsSe is Chalcopyrite structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent In+2.50+ sites. In the first In+2.50+ site, In+2.50+ is bonded to two As3- and two Se2- atoms to form corner-sharing InAs2Se2 tetrahedra. Both In–As bond lengths are 2.73 Å. Both In–Se bond lengths are 2.82 Å. In the second In+2.50+ site, In+2.50+ is bonded to two As3- and two Se2- atoms to form corner-sharing InAs2Se2 tetrahedra. There are one shorter (2.72 Å) and one longer (2.73 Å) In–As bond lengths. Both In–Se bond lengths are 2.82 Å. In the third In+2.50+ site, In+2.50+ is bonded to two As3- and two Se2- atoms to form corner-sharing InAs2Se2 tetrahedra. Both In–As bond lengths are 2.72 Å. Both In–Se bond lengths are 2.81 Å. In the fourth In+2.50+ site, In+2.50+ is bonded to two As3- and two Se2- atoms to form corner-sharing InAs2Se2 tetrahedra. Both In–As bond lengths are 2.73 Å. There are one shorter (2.81 Å) and one longer (2.82 Å) In–Se bond lengths. There are two inequivalent As3- sites. In the first As3- site, As3- is bonded to four In+2.50+ atoms to form AsIn4 tetrahedra that share corners with four equivalent AsIn4 tetrahedra and corners with eight SeIn4 tetrahedra. In the second As3- site, As3- is bonded to four In+2.50+ atoms to form AsIn4 tetrahedra that share corners with four equivalent AsIn4 tetrahedra and corners with eight SeIn4 tetrahedra. There are two inequivalent Se2- sites. In the first Se2- site, Se2- is bonded to four In+2.50+ atoms to form SeIn4 tetrahedra that share corners with four equivalent SeIn4 tetrahedra and corners with eight AsIn4 tetrahedra. In the second Se2- site, Se2- is bonded to four In+2.50+ atoms to form SeIn4 tetrahedra that share corners with four equivalent SeIn4 tetrahedra and corners with eight AsIn4 tetrahedra.
DOI: 10.17188/1283140
title: Materials Data on KCN by Materials Project

description: KCN crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 5-coordinate geometry to five N3- atoms. There are a spread of K–N bond distances ranging from 2.85–3.02 Å. In the second K1+ site, K1+ is bonded in a distorted single-bond geometry to one N3- atom. The K–N bond length is 2.81 Å. In the third K1+ site, K1+ is bonded in a 1-coordinate geometry to six N3- atoms. There are a spread of K–N bond distances ranging from 2.82–3.30 Å. In the fourth K1+ site, K1+ is bonded in a 2-coordinate geometry to two N3- atoms. There are one shorter (2.81 Å) and one longer (2.96 Å) K–N bond lengths. There are four inequivalent C2+ sites. In the first C2+ site, C2+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.36 Å. In the second C2+ site, C2+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.41 Å. In the third C2+ site, C2+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.42 Å. In the fourth C2+ site, C2+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.37 Å. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded in a distorted single-bond geometry to three K1+ and one C2+ atom. In the second N3- site, N3- is bonded in a 1-coordinate geometry to four K1+ and one C2+ atom. In the third N3- site, N3- is bonded in a 1-coordinate geometry to four K1+ and one C2+ atom. In the fourth N3- site, N3- is bonded in a distorted single-bond geometry to three K1+ and one C2+ atom.
DOI: 10.17188/1283142
title: Materials Data on Li3MnAs2 (SG:137) by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1283144
title: Materials Data on CIF5 by Materials Project

description: CF2(CIF5)2CIF4IF4 crystallizes in the triclinic P1 space group. The structure is zero-dimensional and consists of one difluoromethane molecule, one CIF4 cluster, two CIF5 clusters, and one IF4 cluster. In the CIF4 cluster, C is bonded in a water-like geometry to one I and two F atoms. The C–I bond length is 2.21 Å. There is one shorter (1.32 Å) and one longer (1.33 Å) C–F bond length. I is bonded in a distorted T-shaped geometry to one C and two F atoms. There are one shorter (2.00 Å) and one longer (2.02 Å) I–F bond lengths. There are four inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one I atom. In the second F site, F is bonded in a single-bond geometry to one I atom. In the third F site, F is bonded in a single-bond geometry to one C atom. In the fourth F site, F is bonded in a single-bond geometry to one C atom. In each CIF5 cluster, C is bonded in a trigonal non-coplanar geometry to one I and three F atoms. The C–I bond length is 2.22 Å. All C–F bond lengths are 1.34 Å. I is bonded in a distorted T-shaped geometry to one C and two F atoms. There are one shorter (2.01 Å) and one longer (2.04 Å) I–F bond lengths. There are five inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one C atom. In the second F site, F is bonded in a single-bond geometry to one I atom. In the third F site, F is bonded in a single-bond geometry to one C atom. In the fourth F site, F is bonded in a single-bond geometry to one C atom. In the fifth F site, F is bonded in a single-bond geometry to one I atom. In the IF4 cluster, I is bonded in a distorted rectangular see-saw-like geometry to four F atoms. There are a spread of I–F bond distances ranging from 1.95–1.97 Å. There are four inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one I atom. In the second F site, F is bonded in a single-bond geometry to one I atom. In the third F site, F is bonded in a single-bond geometry to one I atom. In the fourth F site, F is bonded in a single-bond geometry to one I atom.
DOI: 10.17188/1283148
title: Materials Data on ReSeCl by Materials Project

description: ReSeCl crystallizes in the orthorhombic C222_1 space group. The structure is two-dimensional and consists of two ReSeCl sheets oriented in the (0, 1, 0) direction. there are four inequivalent Re3+ sites. In the first Re3+ site, Re3+ is bonded to two equivalent Se2- and three Cl1- atoms to form edge-sharing ReSe2Cl3 square pyramids. Both Re–Se bond lengths are 2.55 Å. There are one shorter (2.36 Å) and two longer (2.44 Å) Re–Cl bond lengths. In the second Re3+ site, Re3+ is bonded to three Se2- and two Cl1- atoms to form ReSe3Cl2 square pyramids that share a cornercorner with one ReSe3Cl2 square pyramid and edges with four ReSe4Cl square pyramids. There are one shorter (2.51 Å) and two longer (2.53 Å) Re–Se bond lengths. There are one shorter (2.50 Å) and one longer (2.51 Å) Re–Cl bond lengths. In the third Re3+ site, Re3+ is bonded to three Se2- and two Cl1- atoms to form ReSe3Cl2 square pyramids that share a cornercorner with one ReSe3Cl2 square pyramid and edges with four ReSe4Cl square pyramids. There are a spread of Re–Se bond distances ranging from 2.50–2.55 Å. There are one shorter (2.53 Å) and one longer (2.55 Å) Re–Cl bond lengths. In the fourth Re3+ site, Re3+ is bonded to four Se2- and one Cl1- atom to form edge-sharing ReSe4Cl square pyramids. All Re–Se bond lengths are 2.54 Å. The Re–Cl bond length is 2.40 Å. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 4-coordinate geometry to three Re3+ atoms. In the second Se2- site, Se2- is bonded in a 8-coordinate geometry to three Re3+ atoms. In the third Se2- site, Se2- is bonded in a 5-coordinate geometry to three Re3+ atoms. There are four inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one Re3+ atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Re3+ atom. In the third Cl1- site, Cl1- is bonded in a 4-coordinate geometry to three Re3+ atoms. In the fourth Cl1- site, Cl1- is bonded in a distorted bent 120 degrees geometry to two Re3+ atoms.
DOI: 10.17188/1283149
title: Materials Data on Hf8PbO24 by Materials Project

description: Hf8PbO24 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Hf sites. In the first Hf site, Hf is bonded to six O atoms to form HfO6 octahedra that share corners with six HfO6 octahedra and a faceface with one PbO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 3–11°. There are a spread of Hf–O bond distances ranging from 2.03–2.12 Å. In the second Hf site, Hf is bonded to six O atoms to form HfO6 octahedra that share corners with six HfO6 octahedra and a faceface with one PbO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–11°. There are a spread of Hf–O bond distances ranging from 2.03–2.12 Å. Pb is bonded to twelve O atoms to form PbO12 cuboctahedra that share faces with eight HfO6 octahedra. There are a spread of Pb–O bond distances ranging from 2.77–2.79 Å. There are nine inequivalent O sites. In the first O site, O is bonded in a linear geometry to two equivalent Hf atoms. In the second O site, O is bonded in a linear geometry to two equivalent Hf atoms. In the third O site, O is bonded in a distorted linear geometry to two Hf and one Pb atom. In the fourth O site, O is bonded in a distorted linear geometry to two equivalent Hf and one Pb atom. In the fifth O site, O is bonded in a linear geometry to two equivalent Hf and one Pb atom. In the sixth O site, O is bonded in a linear geometry to two equivalent Hf atoms. In the seventh O site, O is bonded in a linear geometry to two equivalent Hf atoms. In the eighth O site, O is bonded in a distorted linear geometry to two Hf and one Pb atom. In the ninth O site, O is bonded in a linear geometry to two Hf atoms.
DOI: 10.17188/1283150
title: Materials Data on Li2SO4 by Materials Project

description: Li2SO4 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.99–2.17 Å. In the second Li1+ site, Li1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Li–O bond distances ranging from 1.97–2.56 Å. In the third Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.97–2.13 Å. In the fourth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 2.02–2.14 Å. There are two inequivalent S6+ sites. In the first S6+ site, S6+ is bonded in a tetrahedral geometry to four O2- atoms. All S–O bond lengths are 1.49 Å. In the second S6+ site, S6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of S–O bond distances ranging from 1.48–1.50 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted T-shaped geometry to two Li1+ and one S6+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to two Li1+ and one S6+ atom. In the third O2- site, O2- is bonded in a distorted T-shaped geometry to two Li1+ and one S6+ atom. In the fourth O2- site, O2- is bonded in a distorted T-shaped geometry to two Li1+ and one S6+ atom. In the fifth O2- site, O2- is bonded in a distorted T-shaped geometry to two Li1+ and one S6+ atom. In the sixth O2- site, O2- is bonded in a distorted T-shaped geometry to two Li1+ and one S6+ atom. In the seventh O2- site, O2- is bonded in a distorted T-shaped geometry to two Li1+ and one S6+ atom. In the eighth O2- site, O2- is bonded in a 3-coordinate geometry to three Li1+ and one S6+ atom.
DOI: 10.17188/1283153
title: Materials Data on Sr18ThCl40 (SG:0) by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations