cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1301869
title: Materials Data on KMnPCO7 by Materials Project

description: KMnCPO7 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. K1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of K–O bond distances ranging from 2.57–3.41 Å. Mn4+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with four equivalent PO4 tetrahedra. There are a spread of Mn–O bond distances ranging from 1.90–2.02 Å. C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.24–1.33 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 28–44°. There are a spread of P–O bond distances ranging from 1.53–1.56 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one K1+ and one C4+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one K1+, one Mn4+, and one C4+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one K1+, one Mn4+, and one C4+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one K1+, one Mn4+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent K1+, one Mn4+, and one P5+ atom. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one K1+, one Mn4+, and one P5+ atom. In the seventh O2- site, O2- is bonded in a 2-coordinate geometry to one K1+, one Mn4+, and one P5+ atom.
DOI: 10.17188/1301870
title: Materials Data on TiNi5(PO4)6 (SG:146) 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: 10.17188/1301872
title: Materials Data on NaLi5Fe2P2(CO7)2 (SG:2) 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: 10.17188/1301874
title: Materials Data on Li3FeOF4 (SG:8) 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: 10.17188/1301875
title: Materials Data on Li2V3FeO8 (SG:166) 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: 10.17188/1301876
title: Materials Data on Li5Ni5(SnO6)2 (SG:5) 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: 10.17188/1301877
title: Materials Data on K2Li3MnO4 (SG:14) 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: 10.17188/1301878
title: Materials Data on V3O7 (SG:139) 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: 10.17188/1301879
title: Materials Data on MgV3O7 by Materials Project

description: MgV3O7 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Mg2+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Mg–O bond distances ranging from 2.07–2.52 Å. There are two inequivalent V4+ sites. In the first V4+ site, V4+ is bonded to five O2- atoms to form distorted edge-sharing VO5 trigonal bipyramids. There are a spread of V–O bond distances ranging from 1.66–2.01 Å. In the second V4+ site, V4+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of V–O bond distances ranging from 1.66–2.01 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Mg2+ and one V4+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Mg2+ and one V4+ atom. In the third O2- site, O2- is bonded to one Mg2+ and three V4+ atoms to form a mixture of distorted corner and edge-sharing OMgV3 tetrahedra. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to one Mg2+ and three V4+ atoms.
DOI: 10.17188/1301880
title: Materials Data on NaLi2MnPCO7 (SG:1) 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: 10.17188/1301881
title: Materials Data on Na5LiFe2P2(CO7)2 (SG:2) 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: 10.17188/1301882
title: Materials Data on Fe4OF7 (SG:38) 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: 10.17188/1301883
title: Materials Data on K2FePCO7 by Materials Project

description: K2FeCPO7 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. K1+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of K–O bond distances ranging from 2.58–3.03 Å. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with four equivalent PO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 1.97–2.15 Å. C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.25–1.33 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 29–38°. There are a spread of P–O bond distances ranging from 1.55–1.58 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent K1+ and one C4+ atom. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two equivalent K1+, one Fe3+, and one C4+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent K1+, one Fe3+, and one C4+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent K1+, one Fe3+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent K1+, one Fe3+, and one P5+ atom. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent K1+, one Fe3+, and one P5+ atom.
DOI: 10.17188/1301884
title: Materials Data on Li5CoO4 by Materials Project

description: Li5CoO4 crystallizes in the orthorhombic Pnnm space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with two equivalent CoO4 tetrahedra, corners with ten LiO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, edges with two equivalent LiO6 octahedra, edges with two equivalent CoO4 tetrahedra, edges with four LiO4 tetrahedra, and edges with two equivalent LiO4 trigonal pyramids. There are a spread of Li–O bond distances ranging from 2.01–2.56 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form distorted LiO4 tetrahedra that share corners with two equivalent LiO6 octahedra, corners with two equivalent CoO4 tetrahedra, corners with four equivalent LiO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, edges with two equivalent LiO6 octahedra, an edgeedge with one CoO4 tetrahedra, edges with two equivalent LiO4 tetrahedra, and an edgeedge with one LiO4 trigonal pyramid. The corner-sharing octahedral tilt angles are 56°. There are a spread of Li–O bond distances ranging from 1.90–2.18 Å. In the third Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent LiO6 octahedra, corners with two equivalent CoO4 tetrahedra, corners with four LiO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, an edgeedge with one LiO6 octahedra, an edgeedge with one CoO4 tetrahedra, edges with two LiO4 tetrahedra, and an edgeedge with one LiO4 trigonal pyramid. The corner-sharing octahedra tilt angles range from 16–52°. There are a spread of Li–O bond distances ranging from 1.93–2.00 Å. In the fourth Li1+ site, Li1+ is bonded to four O2- atoms to form distorted LiO4 trigonal pyramids that share corners with two equivalent LiO6 octahedra, corners with four equivalent CoO4 tetrahedra, corners with six LiO4 tetrahedra, edges with two equivalent LiO6 octahedra, and edges with three LiO4 tetrahedra. The corner-sharing octahedral tilt angles are 82°. There are a spread of Li–O bond distances ranging from 2.01–2.16 Å. Co3+ is bonded to four O2- atoms to form distorted CoO4 tetrahedra that share corners with two equivalent LiO6 octahedra, corners with six LiO4 tetrahedra, corners with four equivalent LiO4 trigonal pyramids, edges with two equivalent LiO6 octahedra, and edges with three LiO4 tetrahedra. The corner-sharing octahedral tilt angles are 58°. There are a spread of Co–O bond distances ranging from 1.85–1.96 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to five Li1+ and one Co3+ atom. In the second O2- site, O2- is bonded in a 7-coordinate geometry to six Li1+ and one Co3+ atom. In the third O2- site, O2- is bonded in a 5-coordinate geometry to six Li1+ and one Co3+ atom.
DOI: 10.17188/1301885
title: Materials Data on V2SnO7 by Materials Project

description: V2SnO7 crystallizes in the cubic Pa-3 space group. The structure is three-dimensional. V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with three equivalent SnO6 octahedra and a cornercorner with one VO4 tetrahedra. The corner-sharing octahedral tilt angles are 16°. There is three shorter (1.72 Å) and one longer (1.79 Å) V–O bond length. Sn4+ is bonded to six equivalent O2- atoms to form SnO6 octahedra that share corners with six equivalent VO4 tetrahedra. All Sn–O bond lengths are 2.06 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent V5+ atoms. In the second O2- site, O2- is bonded in a distorted linear geometry to one V5+ and one Sn4+ atom.
DOI: 10.17188/1301886
title: Materials Data on Li9Fe3(WO4)7 (SG:160) 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: 10.17188/1301887
title: Materials Data on Li2FeCuO4 (SG:10) 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: 10.17188/1301888
title: Materials Data on Li4MgCo3O8 (SG:166) 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: 10.17188/1301889
title: Materials Data on MnTeO4 (SG:10) 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: 10.17188/1301890
title: Materials Data on K2CoPCO7 by Materials Project

description: K2CoCPO7 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. K1+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of K–O bond distances ranging from 2.58–3.02 Å. Co3+ is bonded to six O2- atoms to form distorted CoO6 octahedra that share corners with four equivalent PO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.88–2.21 Å. C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.25–1.32 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 29–39°. There are a spread of P–O bond distances ranging from 1.54–1.59 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent K1+ and one C4+ atom. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two equivalent K1+, one Co3+, and one C4+ atom. In the third O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to two equivalent K1+, one Co3+, and one C4+ atom. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent K1+, one Co3+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent K1+, one Co3+, and one P5+ atom. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent K1+, one Co3+, and one P5+ atom.
DOI: 10.17188/1301891
title: Materials Data on Li4TiV3O10 (SG:115) 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: 10.17188/1301892
title: Materials Data on NaCu3O4 by Materials Project

description: NaCu3O4 crystallizes in the tetragonal P4_122 space group. The structure is three-dimensional. Na1+ is bonded to six O2- atoms to form NaO6 octahedra that share corners with six CuO6 octahedra, edges with two equivalent NaO6 octahedra, and edges with ten CuO6 octahedra. The corner-sharing octahedra tilt angles range from 10–15°. There are four shorter (2.35 Å) and two longer (2.41 Å) Na–O bond lengths. There are three inequivalent Cu+2.33+ sites. In the first Cu+2.33+ site, Cu+2.33+ is bonded to six O2- atoms to form CuO6 octahedra that share corners with six CuO6 octahedra, edges with four equivalent NaO6 octahedra, and edges with eight CuO6 octahedra. The corner-sharing octahedra tilt angles range from 10–19°. There are a spread of Cu–O bond distances ranging from 1.92–2.19 Å. In the second Cu+2.33+ site, Cu+2.33+ is bonded to six O2- atoms to form distorted CuO6 octahedra that share corners with two equivalent CuO6 octahedra, corners with four equivalent NaO6 octahedra, edges with two equivalent NaO6 octahedra, and edges with ten CuO6 octahedra. The corner-sharing octahedra tilt angles range from 10–15°. There are four shorter (1.95 Å) and two longer (2.49 Å) Cu–O bond lengths. In the third Cu+2.33+ site, Cu+2.33+ is bonded to six O2- atoms to form CuO6 octahedra that share corners with two equivalent NaO6 octahedra, corners with four equivalent CuO6 octahedra, edges with four equivalent NaO6 octahedra, and edges with eight CuO6 octahedra. The corner-sharing octahedra tilt angles range from 10–19°. There are a spread of Cu–O bond distances ranging from 2.01–2.15 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to one Na1+ and five Cu+2.33+ atoms. In the second O2- site, O2- is bonded to two equivalent Na1+ and four Cu+2.33+ atoms to form a mixture of corner and edge-sharing ONa2Cu4 octahedra. The corner-sharing octahedra tilt angles range from 6–7°.
DOI: 10.17188/1301893
title: Materials Data on Li2Ni3WO8 (SG:166) 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: 10.17188/1301894
title: Materials Data on LiFeSiO4 (SG:74) 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: 10.17188/1301896
title: Materials Data on Li5Mn2V3O10 (SG:2) 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: 10.17188/1301897
title: Materials Data on RbH2SNO3 by Materials Project

description: RbNH2SO3 crystallizes in the orthorhombic Pbca space group. The structure is three-dimensional. Rb1+ is bonded in a 8-coordinate geometry to one H1+ and seven O2- atoms. The Rb–H bond length is 3.09 Å. There are a spread of Rb–O bond distances ranging from 3.00–3.18 Å. N5+ is bonded in a distorted trigonal non-coplanar geometry to two H1+ and one S2- atom. Both N–H bond lengths are 1.03 Å. The N–S bond length is 1.68 Å. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N5+ atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one Rb1+ and one N5+ atom. S2- is bonded in a tetrahedral geometry to one N5+ and three O2- atoms. There is two shorter (1.47 Å) and one longer (1.48 Å) S–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to three equivalent Rb1+ and one S2- atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to three equivalent Rb1+ and one S2- atom. In the third O2- site, O2- is bonded in a single-bond geometry to one Rb1+ and one S2- atom.
DOI: 10.17188/1301898
title: Materials Data on CsH5S2(NO3)2 by Materials Project

description: CsH5S2(NO3)2 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is two-dimensional and consists of two CsH5S2(NO3)2 sheets oriented in the (0, 0, 1) direction. Cs1+ is bonded to eight O2- atoms to form distorted CsO8 hexagonal bipyramids that share corners with two equivalent CsO8 hexagonal bipyramids, corners with six SNO3 tetrahedra, edges with two equivalent CsO8 hexagonal bipyramids, and an edgeedge with one SNO3 tetrahedra. There are a spread of Cs–O bond distances ranging from 3.14–3.45 Å. There are two inequivalent N5+ sites. In the first N5+ site, N5+ is bonded in a trigonal non-coplanar geometry to two H1+ and one S2- atom. Both N–H bond lengths are 1.03 Å. The N–S bond length is 1.67 Å. In the second N5+ site, N5+ is bonded in a distorted trigonal non-coplanar geometry to three H1+ and one S2- atom. There is two shorter (1.04 Å) and one longer (1.06 Å) N–H bond length. The N–S bond length is 1.80 Å. There are five inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N5+ atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N5+ atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N5+ atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one N5+ atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one N5+ atom. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to one N5+ and three O2- atoms to form SNO3 tetrahedra that share corners with four equivalent CsO8 hexagonal bipyramids and an edgeedge with one CsO8 hexagonal bipyramid. There is two shorter (1.47 Å) and one longer (1.49 Å) S–O bond length. In the second S2- site, S2- is bonded to one N5+ and three O2- atoms to form distorted SNO3 tetrahedra that share corners with two equivalent CsO8 hexagonal bipyramids. There is one shorter (1.44 Å) and two longer (1.46 Å) S–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to two equivalent Cs1+ and one S2- atom. In the second O2- site, O2- is bonded in a single-bond geometry to two equivalent Cs1+ and one S2- atom. In the third O2- site, O2- is bonded in a single-bond geometry to one Cs1+ and one S2- atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one Cs1+ and one S2- atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Cs1+ and one S2- atom.
DOI: 10.17188/1301900
title: Materials Data on Pr5(CoB3)2 by Materials Project

description: Pr(Pr2CoB3)2 crystallizes in the trigonal R-3m space group. The structure is two-dimensional and consists of three praseodymium molecules and three Pr2CoB3 sheets oriented in the (0, 0, 1) direction. In each Pr2CoB3 sheet, there are two inequivalent Pr3+ sites. In the first Pr3+ site, Pr3+ is bonded in a 6-coordinate geometry to six equivalent B3- atoms. All Pr–B bond lengths are 2.76 Å. In the second Pr3+ site, Pr3+ is bonded in a 6-coordinate geometry to six equivalent B3- atoms. All Pr–B bond lengths are 2.79 Å. Co+1.50+ is bonded in a 6-coordinate geometry to six equivalent B3- atoms. All Co–B bond lengths are 2.12 Å. B3- is bonded in a 9-coordinate geometry to four Pr3+, two equivalent Co+1.50+, and three equivalent B3- atoms. All B–B bond lengths are 1.83 Å.