cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1757735
title: Materials Data on RbCrF5 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: 10.17188/1757737
title: Materials Data on Tm5Ga3 by Materials Project

description: Tm5Ga3 crystallizes in the hexagonal P6_3/mcm space group. The structure is three-dimensional. there are two inequivalent Tm sites. In the first Tm site, Tm is bonded in a 6-coordinate geometry to six equivalent Ga atoms. All Tm–Ga bond lengths are 3.06 Å. In the second Tm site, Tm is bonded in a 3-coordinate geometry to five equivalent Ga atoms. There are a spread of Tm–Ga bond distances ranging from 2.95–3.50 Å. Ga is bonded in a 9-coordinate geometry to nine Tm atoms.
DOI: 10.17188/1757738
title: Materials Data on Ti3V2O9 by Materials Project

description: Ti3V2O9 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are two inequivalent Ti4+ sites. In the first Ti4+ site, Ti4+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with two equivalent TiO6 octahedra and corners with two equivalent TiO5 trigonal bipyramids. The corner-sharing octahedral tilt angles are 60°. There are a spread of Ti–O bond distances ranging from 1.86–2.12 Å. In the second Ti4+ site, Ti4+ is bonded to five O2- atoms to form TiO5 trigonal bipyramids that share a cornercorner with one TiO6 octahedra, corners with two equivalent TiO5 trigonal bipyramids, and an edgeedge with one TiO5 trigonal bipyramid. The corner-sharing octahedral tilt angles are 33°. There are a spread of Ti–O bond distances ranging from 1.85–2.00 Å. V3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.92–2.44 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to two equivalent Ti4+ atoms. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Ti4+ and two equivalent V3+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two Ti4+ and one V3+ atom. In the fourth O2- site, O2- is bonded in a distorted T-shaped geometry to two equivalent Ti4+ and one V3+ atom. In the fifth O2- site, O2- is bonded to one Ti4+ and three equivalent V3+ atoms to form a mixture of distorted corner and edge-sharing OTiV3 trigonal pyramids.
DOI: 10.17188/1757739
title: Materials Data on DyMn4(CuO4)3 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: 10.17188/1757740
title: Materials Data on Li2Cr3P9O28 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: 10.17188/1757741
title: Materials Data on KRb2CuF6 by Materials Project

description: Rb2KCuF6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Rb1+ is bonded to twelve equivalent F1- atoms to form RbF12 cuboctahedra that share corners with twelve equivalent RbF12 cuboctahedra, faces with six equivalent RbF12 cuboctahedra, faces with four equivalent KF6 octahedra, and faces with four equivalent CuF6 octahedra. All Rb–F bond lengths are 3.16 Å. K1+ is bonded to six equivalent F1- atoms to form KF6 octahedra that share corners with six equivalent CuF6 octahedra and faces with eight equivalent RbF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All K–F bond lengths are 2.52 Å. Cu3+ is bonded to six equivalent F1- atoms to form CuF6 octahedra that share corners with six equivalent KF6 octahedra and faces with eight equivalent RbF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Cu–F bond lengths are 1.93 Å. F1- is bonded in a distorted linear geometry to four equivalent Rb1+, one K1+, and one Cu3+ atom.
DOI: 10.17188/1757742
title: Materials Data on FePH5CO8 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: 10.17188/1757743
title: Materials Data on BaMn4AlO7 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: 10.17188/1757744
title: Materials Data on LiFe2(BO3)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: 10.17188/1757745
title: Materials Data on Cs2RbSbBr6 by Materials Project

description: Cs2RbSbBr6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs1+ is bonded to twelve equivalent Br1- atoms to form CsBr12 cuboctahedra that share corners with twelve equivalent CsBr12 cuboctahedra, faces with six equivalent CsBr12 cuboctahedra, faces with four equivalent RbBr6 octahedra, and faces with four equivalent SbBr6 octahedra. All Cs–Br bond lengths are 4.32 Å. Rb1+ is bonded to six equivalent Br1- atoms to form RbBr6 octahedra that share corners with six equivalent SbBr6 octahedra and faces with eight equivalent CsBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–Br bond lengths are 3.28 Å. Sb3+ is bonded to six equivalent Br1- atoms to form SbBr6 octahedra that share corners with six equivalent RbBr6 octahedra and faces with eight equivalent CsBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–Br bond lengths are 2.82 Å. Br1- is bonded in a linear geometry to four equivalent Cs1+, one Rb1+, and one Sb3+ atom.
DOI: 10.17188/1757746
title: Materials Data on Mn4P4O13 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: 10.17188/1757747
title: Materials Data on Ca3Si4(SnO7)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: 10.17188/1757748
title: Materials Data on Mn6OF11 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: 10.17188/1757750
title: Materials Data on Fe2BO4 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: 10.17188/1757751
title: Materials Data on In2SbAs by Materials Project

description: In2SbAs is Enargite-like structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. there are two inequivalent In3+ sites. In the first In3+ site, In3+ is bonded to three equivalent Sb3- and one As3- atom to form corner-sharing InSb3As tetrahedra. All In–Sb bond lengths are 2.82 Å. The In–As bond length is 2.67 Å. In the second In3+ site, In3+ is bonded to one Sb3- and three equivalent As3- atoms to form corner-sharing InSbAs3 tetrahedra. The In–Sb bond length is 2.88 Å. All In–As bond lengths are 2.74 Å. Sb3- is bonded to four In3+ atoms to form SbIn4 tetrahedra that share corners with six equivalent SbIn4 tetrahedra and corners with six equivalent AsIn4 tetrahedra. As3- is bonded to four In3+ atoms to form AsIn4 tetrahedra that share corners with six equivalent SbIn4 tetrahedra and corners with six equivalent AsIn4 tetrahedra.
DOI: 10.17188/1757752
title: Materials Data on Li2MnCSO7 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: 10.17188/1757753
title: Materials Data on ReN2 by Materials Project

description: ReN2 crystallizes in the monoclinic Cm space group. The structure is two-dimensional and consists of one ReN2 sheet oriented in the (0, 0, 1) direction. Re6+ is bonded to six N3- atoms to form distorted edge-sharing ReN6 pentagonal pyramids. There are a spread of Re–N bond distances ranging from 2.04–2.10 Å. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded in a rectangular see-saw-like geometry to three equivalent Re6+ and one N3- atom. The N–N bond length is 1.40 Å. In the second N3- site, N3- is bonded in a distorted T-shaped geometry to three equivalent Re6+ atoms.
DOI: 10.17188/1757754
title: Materials Data on Mg3Si4 by Materials Project

description: Mg3Si4 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Mg sites. In the first Mg site, Mg is bonded in a 6-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.88–3.07 Å. In the second Mg site, Mg is bonded in a 4-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.73–3.05 Å. In the third Mg site, Mg is bonded in a 9-coordinate geometry to ten Si atoms. There are a spread of Mg–Si bond distances ranging from 2.78–3.19 Å. In the fourth Mg site, Mg is bonded in a 6-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.68–2.97 Å. In the fifth Mg site, Mg is bonded in a 7-coordinate geometry to seven Si atoms. There are a spread of Mg–Si bond distances ranging from 2.73–3.05 Å. In the sixth Mg site, Mg is bonded in a 6-coordinate geometry to seven Si atoms. There are a spread of Mg–Si bond distances ranging from 2.78–3.10 Å. There are eight inequivalent Si sites. In the first Si site, Si is bonded in a 6-coordinate geometry to six Mg and two Si atoms. There are one shorter (2.48 Å) and one longer (2.59 Å) Si–Si bond lengths. In the second Si site, Si is bonded in a 9-coordinate geometry to six Mg and three Si atoms. Both Si–Si bond lengths are 2.51 Å. In the third Si site, Si is bonded in a 10-coordinate geometry to six Mg and four Si atoms. There are a spread of Si–Si bond distances ranging from 2.46–2.61 Å. In the fourth Si site, Si is bonded in a 9-coordinate geometry to six Mg and three Si atoms. The Si–Si bond length is 2.42 Å. In the fifth Si site, Si is bonded in a 8-coordinate geometry to four Mg and four Si atoms. Both Si–Si bond lengths are 2.48 Å. In the sixth Si site, Si is bonded in a 7-coordinate geometry to three Mg and four Si atoms. Both Si–Si bond lengths are 2.55 Å. In the seventh Si site, Si is bonded in a 9-coordinate geometry to seven Mg and two equivalent Si atoms. In the eighth Si site, Si is bonded in a 8-coordinate geometry to four Mg and four Si atoms.
DOI: 10.17188/1757755
title: Materials Data on Ba2LiAl(CN2)4 by Materials Project

description: LiBa2Al(CN2)4 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Li1+ is bonded in a tetrahedral geometry to four N3- atoms. There are a spread of Li–N bond distances ranging from 2.07–2.14 Å. There are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight N3- atoms. There are a spread of Ba–N bond distances ranging from 2.92–2.99 Å. In the second Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight N3- atoms. There are a spread of Ba–N bond distances ranging from 2.83–3.13 Å. Al3+ is bonded in a tetrahedral geometry to four N3- atoms. There is two shorter (1.85 Å) and two longer (1.86 Å) Al–N bond length. There are four inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.22 Å) and one longer (1.26 Å) C–N bond length. In the second C4+ site, C4+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.21 Å) and one longer (1.26 Å) C–N bond length. In the third C4+ site, C4+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.22 Å) and one longer (1.26 Å) C–N bond length. In the fourth C4+ site, C4+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.22 Å) and one longer (1.26 Å) C–N bond length. There are eight inequivalent N3- sites. In the first N3- site, N3- is bonded in a 2-coordinate geometry to two equivalent Ba2+, one Al3+, and one C4+ atom. In the second N3- site, N3- is bonded in a distorted bent 120 degrees geometry to two Ba2+, one Al3+, and one C4+ atom. In the third N3- site, N3- is bonded in a distorted bent 120 degrees geometry to two Ba2+, one Al3+, and one C4+ atom. In the fourth N3- site, N3- is bonded in a distorted bent 120 degrees geometry to two Ba2+, one Al3+, and one C4+ atom. In the fifth N3- site, N3- is bonded in a 4-coordinate geometry to one Li1+, two Ba2+, and one C4+ atom. In the sixth N3- site, N3- is bonded in a 2-coordinate geometry to one Li1+, two equivalent Ba2+, and one C4+ atom. In the seventh N3- site, N3- is bonded in a 2-coordinate geometry to one Li1+, two Ba2+, and one C4+ atom. In the eighth N3- site, N3- is bonded in a 2-coordinate geometry to one Li1+, two Ba2+, and one C4+ atom.
DOI: 10.17188/1757756
title: Materials Data on Tm2(B2Rh3)3 by Materials Project

description: Tm2(Rh3B2)3 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Tm is bonded in a 12-coordinate geometry to one Tm, twelve Rh, and six equivalent B atoms. The Tm–Tm bond length is 3.51 Å. There are six shorter (3.01 Å) and six longer (3.30 Å) Tm–Rh bond lengths. All Tm–B bond lengths are 3.24 Å. There are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 4-coordinate geometry to two equivalent Tm and four B atoms. There are two shorter (2.15 Å) and two longer (2.16 Å) Rh–B bond lengths. In the second Rh site, Rh is bonded in a distorted square co-planar geometry to four equivalent Tm and four equivalent B atoms. All Rh–B bond lengths are 2.16 Å. There are two inequivalent B sites. In the first B site, B is bonded to six equivalent Rh atoms to form distorted edge-sharing BRh6 pentagonal pyramids. In the second B site, B is bonded in a 6-coordinate geometry to three equivalent Tm and six Rh atoms.
DOI: 10.17188/1757757
title: Materials Data on LiCrPO4 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: 10.17188/1757758
title: Materials Data on Pr7(IO6)3 by Materials Project

description: Pr7(O6I)3 crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. there are three inequivalent Pr3+ sites. In the first Pr3+ site, Pr3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Pr–O bond distances ranging from 2.14–2.45 Å. In the second Pr3+ site, Pr3+ is bonded to four O2- atoms to form corner-sharing PrO4 trigonal pyramids. There are a spread of Pr–O bond distances ranging from 2.25–2.33 Å. In the third Pr3+ site, Pr3+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are three shorter (2.45 Å) and six longer (2.73 Å) Pr–O bond lengths. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three equivalent Pr3+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to three Pr3+ and one O2- atom. The O–O bond length is 1.51 Å. In the third O2- site, O2- is bonded in a water-like geometry to one Pr3+ and one I5+ atom. The O–I bond length is 1.90 Å. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Pr3+ and one I5+ atom. The O–I bond length is 1.96 Å. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Pr3+ and one O2- atom. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to two Pr3+ atoms. I5+ is bonded in a water-like geometry to two O2- atoms.
DOI: 10.17188/1757759
title: Materials Data on BaNa4Ti2(Si2O5)6 by Materials Project

description: Na4BaTi2(Si2O5)6 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Na–O bond distances ranging from 2.25–2.94 Å. In the second Na1+ site, Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.23–2.64 Å. Ba2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ba–O bond distances ranging from 2.85–3.25 Å. Ti3+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with four SiO4 tetrahedra and an edgeedge with one TiO6 octahedra. There are a spread of Ti–O bond distances ranging from 1.94–2.17 Å. There are three inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 46°. There are a spread of Si–O bond distances ranging from 1.58–1.70 Å. In the second Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one TiO6 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedral tilt angles are 41°. There are a spread of Si–O bond distances ranging from 1.59–1.70 Å. In the third Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.60–1.66 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Na1+, one Ba2+, and two equivalent Ti3+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+ and two equivalent Si4+ atoms. In the third O2- site, O2- is bonded in a linear geometry to two equivalent Si4+ atoms. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Ti3+, and one Si4+ atom. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+ and two Si4+ atoms. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to one Na1+, one Ba2+, one Ti3+, and one Si4+ atom. In the seventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Na1+ and two Si4+ atoms. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one Ba2+ and two Si4+ atoms. In the ninth O2- site, O2- is bonded in a 2-coordinate geometry to two Na1+ and two Si4+ atoms.
DOI: 10.17188/1757760
title: Materials Data on SrCa7Ti3Mn5O24 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: 10.17188/1757761
title: Materials Data on Cs2AlCuCl6 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: 10.17188/1757762
title: Materials Data on ScCrO4 by Materials Project

description: ScCrO4 is Zircon structured and crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. Sc3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Sc–O bond distances ranging from 2.16–2.44 Å. Cr5+ is bonded in a tetrahedral geometry to four O2- atoms. There is two shorter (1.70 Å) and two longer (1.74 Å) Cr–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Sc3+ and one Cr5+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Sc3+ and one Cr5+ atom.
DOI: 10.17188/1757763
title: Materials Data on BaMn4O8 by Materials Project

description: BaMn4O8 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Ba2+ is bonded in a 8-coordinate geometry to eight O2- atoms. All Ba–O bond lengths are 2.88 Å. There are two inequivalent Mn+3.50+ sites. In the first Mn+3.50+ site, Mn+3.50+ is bonded to six O2- atoms to form a mixture of corner and edge-sharing MnO6 octahedra. The corner-sharing octahedra tilt angles range from 53–54°. There are a spread of Mn–O bond distances ranging from 1.91–2.10 Å. In the second Mn+3.50+ site, Mn+3.50+ is bonded to six O2- atoms to form a mixture of corner and edge-sharing MnO6 octahedra. The corner-sharing octahedra tilt angles range from 53–54°. There are a spread of Mn–O bond distances ranging from 1.90–2.10 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Ba2+ and three equivalent Mn+3.50+ atoms. In the second O2- site, O2- is bonded in a trigonal planar geometry to three Mn+3.50+ atoms. In the third O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Ba2+ and three equivalent Mn+3.50+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Mn+3.50+ atoms.