cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1307118
title: Materials Data on Ti(FeO2)2 by Materials Project

description: Fe2TiO4 is Spinel-like structured and 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 six equivalent FeO4 tetrahedra, edges with two equivalent TiO6 octahedra, and edges with four FeO6 octahedra. There are a spread of Ti–O bond distances ranging from 1.90–2.10 Å. In the second Ti4+ site, Ti4+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with six equivalent FeO4 tetrahedra, edges with two equivalent TiO6 octahedra, and edges with four FeO6 octahedra. There are a spread of Ti–O bond distances ranging from 1.97–2.01 Å. There are three inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent FeO4 tetrahedra, edges with two equivalent FeO6 octahedra, and edges with four TiO6 octahedra. There are a spread of Fe–O bond distances ranging from 2.11–2.20 Å. In the second Fe2+ site, Fe2+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with six TiO6 octahedra and corners with six FeO6 octahedra. The corner-sharing octahedra tilt angles range from 51–66°. There are three shorter (2.04 Å) and one longer (2.06 Å) Fe–O bond lengths. In the third Fe2+ site, Fe2+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent FeO4 tetrahedra, edges with two equivalent FeO6 octahedra, and edges with four TiO6 octahedra. There are a spread of Fe–O bond distances ranging from 2.09–2.24 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Ti4+ and three Fe2+ atoms. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Ti4+ and two Fe2+ atoms. In the third O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Ti4+ and three Fe2+ atoms. In the fourth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Ti4+ and two Fe2+ atoms.
DOI: 10.17188/1307120
title: Materials Data on Li3MnCr3O8 (SG:12) 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: 10.17188/1307121
title: Materials Data on Fe3O5F (SG:12) 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: 10.17188/1307123
title: Materials Data on Fe4O7F (SG:7) 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: 10.17188/1307124
title: Materials Data on Fe4O7F (SG:15) 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: 10.17188/1307125
title: Materials Data on VO2F (SG:19) 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: 10.17188/1307126
title: Materials Data on Na3VBPO7 (SG:11) 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: 10.17188/1307127
title: Materials Data on V2(OF)3 (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: 10.17188/1307128
title: Materials Data on Mn3Cr3(SbO8)2 (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: 10.17188/1307129
title: Materials Data on Cr3P by Materials Project

description: Cr3P crystallizes in the tetragonal I-4 space group. The structure is three-dimensional. there are three inequivalent Cr sites. In the first Cr site, Cr is bonded in a 4-coordinate geometry to four equivalent P atoms. There are a spread of Cr–P bond distances ranging from 2.32–2.36 Å. In the second Cr site, Cr is bonded in a 2-coordinate geometry to two equivalent P atoms. Both Cr–P bond lengths are 2.35 Å. In the third Cr site, Cr is bonded in a 3-coordinate geometry to three equivalent P atoms. There are a spread of Cr–P bond distances ranging from 2.30–2.40 Å. P is bonded in a 9-coordinate geometry to nine Cr atoms.
DOI: 10.17188/1307130
title: Materials Data on Na2BiO3 by Materials Project

description: Na2BiO3 is Caswellsilverite-like structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Na sites. In the first Na site, Na is bonded to six O atoms to form NaO6 octahedra that share corners with two equivalent BiO6 octahedra, corners with four NaO6 octahedra, edges with five equivalent BiO6 octahedra, and edges with seven NaO6 octahedra. The corner-sharing octahedra tilt angles range from 2–13°. There are a spread of Na–O bond distances ranging from 2.37–2.59 Å. In the second Na site, Na is bonded to six O atoms to form NaO6 octahedra that share corners with six NaO6 octahedra, edges with five equivalent BiO6 octahedra, and edges with seven NaO6 octahedra. The corner-sharing octahedra tilt angles range from 1–13°. There are a spread of Na–O bond distances ranging from 2.36–2.44 Å. Bi is bonded to six O atoms to form BiO6 octahedra that share corners with two equivalent NaO6 octahedra, corners with four equivalent BiO6 octahedra, edges with two equivalent BiO6 octahedra, and edges with ten NaO6 octahedra. The corner-sharing octahedra tilt angles range from 2–14°. There are a spread of Bi–O bond distances ranging from 2.08–2.53 Å. There are three inequivalent O sites. In the first O site, O is bonded to three Na and three equivalent Bi atoms to form a mixture of edge and corner-sharing ONa3Bi3 octahedra. The corner-sharing octahedra tilt angles range from 1–14°. In the second O site, O is bonded to five Na and one Bi atom to form a mixture of edge and corner-sharing ONa5Bi octahedra. The corner-sharing octahedra tilt angles range from 6–12°. In the third O site, O is bonded to four Na and two equivalent Bi atoms to form a mixture of edge and corner-sharing ONa4Bi2 octahedra. The corner-sharing octahedra tilt angles range from 1–7°.
DOI: 10.17188/1307131
title: Materials Data on RbTaO3 by Materials Project

description: RbTaO3 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 4-coordinate geometry to six O2- atoms. There are a spread of Rb–O bond distances ranging from 2.85–3.39 Å. In the second Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Rb–O bond distances ranging from 2.90–3.37 Å. 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 2.82–3.21 Å. There are two inequivalent Ta5+ sites. In the first Ta5+ site, Ta5+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ta–O bond distances ranging from 1.81–2.39 Å. In the second Ta5+ site, Ta5+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ta–O bond distances ranging from 1.82–2.47 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to four Ta5+ atoms. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two Rb1+ and two Ta5+ atoms. In the third O2- site, O2- is bonded in a distorted single-bond geometry to four Rb1+ and one Ta5+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to three Rb1+ and one Ta5+ atom. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to two Rb1+ and two Ta5+ atoms. In the sixth O2- site, O2- is bonded in a distorted water-like geometry to three Rb1+ and two Ta5+ atoms.
DOI: 10.17188/1307132
title: Materials Data on Tb5O9 by Materials Project

description: Tb5O9 crystallizes in the tetragonal I-4 space group. The structure is three-dimensional. there are two inequivalent Tb+3.60+ sites. In the first Tb+3.60+ site, Tb+3.60+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Tb–O bond distances ranging from 2.30–2.45 Å. In the second Tb+3.60+ site, Tb+3.60+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are four shorter (2.31 Å) and four longer (2.52 Å) Tb–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Tb+3.60+ atoms to form a mixture of edge and corner-sharing OTb4 tetrahedra. In the second O2- site, O2- is bonded to four Tb+3.60+ atoms to form a mixture of edge and corner-sharing OTb4 tetrahedra. In the third O2- site, O2- is bonded to four Tb+3.60+ atoms to form a mixture of distorted edge and corner-sharing OTb4 tetrahedra.
DOI: 10.17188/1307135
title: Materials Data on Li3Mn2Fe(BO3)3 (SG:6) 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: 10.17188/1307136
title: Materials Data on Li10Fe2Co3Ni3O16 (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: 10.17188/1307137
title: Materials Data on Ni3OF5 (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: 10.17188/1307138
title: Materials Data on Li6MnFe5(BO3)6 (SG:6) 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: 10.17188/1307139
title: Materials Data on Li4MnFe3(BO3)4 (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: 10.17188/1307140
title: Materials Data on Mn3O5F by Materials Project

description: Mn3O5F is zeta iron carbide-derived structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are four inequivalent Mn+3.67+ sites. In the first Mn+3.67+ site, Mn+3.67+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with eight MnO4F2 octahedra and edges with two MnO6 octahedra. The corner-sharing octahedra tilt angles range from 44–53°. There are a spread of Mn–O bond distances ranging from 1.93–2.05 Å. In the second Mn+3.67+ site, Mn+3.67+ is bonded to four O2- and two equivalent F1- atoms to form MnO4F2 octahedra that share corners with eight MnO4F2 octahedra and edges with two equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 43–57°. There is two shorter (1.95 Å) and two longer (1.96 Å) Mn–O bond length. Both Mn–F bond lengths are 2.08 Å. In the third Mn+3.67+ site, Mn+3.67+ is bonded to four O2- and two equivalent F1- atoms to form MnO4F2 octahedra that share corners with eight MnO6 octahedra and edges with two equivalent MnO5F octahedra. The corner-sharing octahedra tilt angles range from 50–57°. There is two shorter (1.92 Å) and two longer (2.02 Å) Mn–O bond length. Both Mn–F bond lengths are 2.04 Å. In the fourth Mn+3.67+ site, Mn+3.67+ is bonded to five O2- and one F1- atom to form MnO5F octahedra that share corners with eight MnO6 octahedra and edges with two MnO4F2 octahedra. The corner-sharing octahedra tilt angles range from 43–53°. There are a spread of Mn–O bond distances ranging from 1.84–1.97 Å. The Mn–F bond length is 1.97 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Mn+3.67+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three Mn+3.67+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three Mn+3.67+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Mn+3.67+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Mn+3.67+ atoms. F1- is bonded in a distorted trigonal planar geometry to three Mn+3.67+ atoms.
DOI: 10.17188/1307141
title: Materials Data on Li3MnSiO5 (SG:33) 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: 10.17188/1307142
title: Materials Data on Fe3O5F (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: 10.17188/1307143
title: Materials Data on MnCrO4 (SG:62) 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: 10.17188/1307144
title: Materials Data on Li2Co2OF6 (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: 10.17188/1307145
title: Materials Data on Li3MnCu3O8 (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: 10.17188/1307146
title: Materials Data on Fe2O3F (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: 10.17188/1307147
title: Materials Data on Fe3O5F (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: 10.17188/1307148
title: Materials Data on LiMnPO4 (SG:33) 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: 10.17188/1307149
title: Materials Data on V3O5F (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: 10.17188/1307150
title: Materials Data on Fe2O3F (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: 10.17188/1307151
title: Materials Data on V2O3F (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: 10.17188/1307153
title: Materials Data on CaSb2H2F14 by Materials Project

description: CaSb2H2F14 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ca2+ is bonded in a 8-coordinate geometry to eight F1- atoms. There are a spread of Ca–F bond distances ranging from 2.31–2.48 Å. There are three inequivalent Sb5+ sites. In the first Sb5+ site, Sb5+ is bonded in an octahedral geometry to six F1- atoms. There are a spread of Sb–F bond distances ranging from 1.89–1.95 Å. In the second Sb5+ site, Sb5+ is bonded in an octahedral geometry to six F1- atoms. There is two shorter (1.89 Å) and four longer (1.94 Å) Sb–F bond length. In the third Sb5+ site, Sb5+ is bonded in an octahedral geometry to six F1- atoms. There are a spread of Sb–F bond distances ranging from 1.89–1.95 Å. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a distorted linear geometry to two F1- atoms. There is one shorter (0.97 Å) and one longer (1.57 Å) H–F bond length. In the second H1+ site, H1+ is bonded in a distorted linear geometry to two F1- atoms. There is one shorter (0.97 Å) and one longer (1.54 Å) H–F bond length. There are fourteen inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ca2+ and one Sb5+ atom. In the second F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ca2+ and one Sb5+ atom. In the third F1- site, F1- is bonded in a linear geometry to one Ca2+ and one Sb5+ atom. In the fourth F1- site, F1- is bonded in a single-bond geometry to one Sb5+ atom. In the fifth F1- site, F1- is bonded in a distorted single-bond geometry to one Ca2+ and one H1+ atom. In the sixth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Sb5+ and one H1+ atom. In the seventh F1- site, F1- is bonded in a single-bond geometry to one Sb5+ atom. In the eighth F1- site, F1- is bonded in a single-bond geometry to one Sb5+ atom. In the ninth F1- site, F1- is bonded in a distorted bent 120 degrees geometry to one Sb5+ and one H1+ atom. In the tenth F1- site, F1- is bonded in a bent 150 degrees geometry to one Ca2+ and one Sb5+ atom. In the eleventh F1- site, F1- is bonded in a single-bond geometry to one Sb5+ atom. In the twelfth F1- site, F1- is bonded in a distorted single-bond geometry to one Ca2+ and one H1+ atom. In the thirteenth F1- site, F1- is bonded in a distorted linear geometry to one Ca2+ and one Sb5+ atom. In the fourteenth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ca2+ and one Sb5+ atom.
DOI: 10.17188/1307154
title: Materials Data on SrTaNO2 by Materials Project

description: SrTaO2N crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 12-coordinate geometry to four N3- and eight O2- atoms. There are a spread of Sr–N bond distances ranging from 2.74–2.96 Å. There are a spread of Sr–O bond distances ranging from 2.72–3.22 Å. In the second Sr2+ site, Sr2+ is bonded to four N3- and eight O2- atoms to form distorted SrN4O8 cuboctahedra that share corners with four equivalent SrN4O8 cuboctahedra, faces with two equivalent SrN4O8 cuboctahedra, and faces with eight TaN2O4 octahedra. There are a spread of Sr–N bond distances ranging from 2.72–3.02 Å. There are a spread of Sr–O bond distances ranging from 2.64–3.08 Å. There are two inequivalent Ta5+ sites. In the first Ta5+ site, Ta5+ is bonded to two N3- and four O2- atoms to form TaN2O4 octahedra that share corners with six TaN2O4 octahedra and faces with four equivalent SrN4O8 cuboctahedra. The corner-sharing octahedra tilt angles range from 10–16°. There is one shorter (1.98 Å) and one longer (1.99 Å) Ta–N bond length. There are a spread of Ta–O bond distances ranging from 2.03–2.13 Å. In the second Ta5+ site, Ta5+ is bonded to two N3- and four O2- atoms to form TaN2O4 octahedra that share corners with six TaN2O4 octahedra and faces with four equivalent SrN4O8 cuboctahedra. The corner-sharing octahedra tilt angles range from 9–16°. There is one shorter (1.98 Å) and one longer (1.99 Å) Ta–N bond length. There are a spread of Ta–O bond distances ranging from 2.02–2.14 Å. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a 2-coordinate geometry to four Sr2+ and two equivalent Ta5+ atoms. In the second N3- site, N3- is bonded in a 2-coordinate geometry to four Sr2+ and two Ta5+ atoms. In the third N3- site, N3- is bonded in a 2-coordinate geometry to four Sr2+ and two equivalent Ta5+ atoms. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two equivalent Ta5+ atoms. In the second O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two Ta5+ atoms. In the third O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two equivalent Ta5+ atoms. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two equivalent Ta5+ atoms. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two equivalent Ta5+ atoms.