cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1295418
title: Materials Data on Fe4O7F by Materials Project

description: Fe4O7F is Hydrophilite-derived structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are four inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with eight FeO6 octahedra and edges with two equivalent FeO5F octahedra. The corner-sharing octahedra tilt angles range from 48–53°. There are a spread of Fe–O bond distances ranging from 1.94–2.09 Å. In the second Fe site, Fe is bonded to five O and one F atom to form a mixture of edge and corner-sharing FeO5F octahedra. The corner-sharing octahedra tilt angles range from 47–52°. There is four shorter (1.94 Å) and one longer (1.97 Å) Fe–O bond length. The Fe–F bond length is 2.12 Å. In the third Fe site, Fe is bonded to five O and one F atom to form FeO5F octahedra that share corners with eight FeO6 octahedra and edges with two equivalent FeO5F octahedra. The corner-sharing octahedra tilt angles range from 47–54°. There are a spread of Fe–O bond distances ranging from 1.94–1.98 Å. The Fe–F bond length is 2.09 Å. In the fourth Fe site, Fe is bonded to five O and one F atom to form FeO5F octahedra that share corners with eight FeO6 octahedra and edges with two equivalent FeO5F octahedra. The corner-sharing octahedra tilt angles range from 47–54°. There are a spread of Fe–O bond distances ranging from 1.94–2.02 Å. The Fe–F bond length is 2.05 Å. There are seven inequivalent O sites. In the first O site, O is bonded in a distorted trigonal planar geometry to three Fe atoms. In the second O site, O is bonded in a trigonal planar geometry to three Fe atoms. In the third O site, O is bonded in a distorted trigonal planar geometry to three Fe atoms. In the fourth O site, O is bonded in a trigonal planar geometry to three Fe atoms. In the fifth O site, O is bonded in a distorted trigonal planar geometry to three Fe atoms. In the sixth O site, O is bonded in a trigonal planar geometry to three Fe atoms. In the seventh O site, O is bonded in a trigonal planar geometry to three Fe atoms. F is bonded in a distorted trigonal planar geometry to three Fe atoms.
DOI: 10.17188/1295419
title: Materials Data on Fe4O7F by Materials Project

description: Fe4O7F is Hydrophilite-derived structured and crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. there are three inequivalent Fe sites. In the first Fe site, Fe is bonded to five O and one F atom to form FeO5F octahedra that share corners with eight FeO6 octahedra and edges with two equivalent FeO5F octahedra. The corner-sharing octahedra tilt angles range from 46–54°. There are a spread of Fe–O bond distances ranging from 1.94–1.97 Å. The Fe–F bond length is 2.09 Å. In the second Fe site, Fe is bonded to six O atoms to form a mixture of corner and edge-sharing FeO6 octahedra. The corner-sharing octahedra tilt angles range from 46–52°. There is four shorter (1.95 Å) and two longer (2.02 Å) Fe–O bond length. In the third Fe site, Fe is bonded to five O and one F atom to form FeO5F octahedra that share corners with eight equivalent FeO5F octahedra and edges with two equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 48–54°. There is four shorter (1.95 Å) and one longer (1.98 Å) Fe–O bond length. The Fe–F bond length is 2.11 Å. There are three inequivalent O sites. In the first O site, O is bonded in a distorted trigonal planar geometry to three Fe atoms. In the second O site, O is bonded in a trigonal planar geometry to three Fe atoms. In the third O site, O is bonded in a trigonal planar geometry to three Fe atoms. F is bonded in a distorted trigonal planar geometry to three Fe atoms.
DOI: 10.17188/1295422
title: Materials Data on Li3Fe4(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: 10.17188/1295426
title: Materials Data on Li2Mn5F17 by Materials Project

description: LiLi3Mn10F34 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional and consists of four litio molecules and one Li3Mn10F34 framework. In the Li3Mn10F34 framework, there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a water-like geometry to two equivalent F1- atoms. Both Li–F bond lengths are 1.92 Å. In the second Li1+ site, Li1+ is bonded in a distorted rectangular see-saw-like geometry to four F1- atoms. There are two shorter (1.99 Å) and two longer (2.09 Å) Li–F bond lengths. There are three inequivalent Mn3+ sites. In the first Mn3+ site, Mn3+ is bonded to six F1- atoms to form corner-sharing MnF6 octahedra. The corner-sharing octahedra tilt angles range from 34–47°. There are a spread of Mn–F bond distances ranging from 1.82–2.00 Å. In the second Mn3+ site, Mn3+ is bonded to six F1- atoms to form corner-sharing MnF6 octahedra. The corner-sharing octahedra tilt angles range from 25–39°. There are a spread of Mn–F bond distances ranging from 1.94–2.07 Å. In the third Mn3+ site, Mn3+ is bonded to six F1- atoms to form corner-sharing MnF6 octahedra. The corner-sharing octahedra tilt angles range from 34–47°. There are a spread of Mn–F bond distances ranging from 1.82–2.11 Å. There are thirteen inequivalent F1- sites. In the first F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one Mn3+ atom. In the second F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Mn3+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent Mn3+ atoms. In the fourth F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Mn3+ atoms. In the fifth F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Mn3+ atoms. In the sixth F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Mn3+ atoms. In the seventh F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Mn3+ atoms. In the eighth F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Mn3+ atoms. In the ninth F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Mn3+ atoms. In the tenth F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one Mn3+ atom. In the eleventh F1- site, F1- is bonded in a bent 150 degrees geometry to two Mn3+ atoms. In the twelfth F1- site, F1- is bonded in a distorted bent 120 degrees geometry to two Mn3+ atoms. In the thirteenth F1- site, F1- is bonded in a bent 150 degrees geometry to two Mn3+ atoms.
DOI: 10.17188/1295427
title: Materials Data on Li2MnV(P2O7)2 (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: 10.17188/1295428
title: Materials Data on Li6Fe5WO12 (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: 10.17188/1295429
title: Materials Data on LiVF4 (SG:4) 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: 10.17188/1295431
title: Materials Data on Li8NiO5F (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: 10.17188/1295432
title: Materials Data on V3O5F (SG:65) 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: 10.17188/1295433
title: Materials Data on Li2FeOF3 (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: 10.17188/1295434
title: Materials Data on VOF by Materials Project

description: VOF is beta Vanadium nitride-derived structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are three inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to three O2- and three F1- atoms to form a mixture of corner and edge-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 48–52°. There is one shorter (1.93 Å) and two longer (1.99 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.10–2.15 Å. In the second V3+ site, V3+ is bonded to three O2- and three F1- atoms to form a mixture of corner and edge-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 47–54°. There are a spread of V–O bond distances ranging from 1.92–2.00 Å. There are a spread of V–F bond distances ranging from 2.10–2.14 Å. In the third V3+ site, V3+ is bonded to three O2- and three F1- atoms to form a mixture of corner and edge-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 47–54°. There is one shorter (1.91 Å) and two longer (1.97 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.13–2.15 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three V3+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three V3+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three V3+ atoms. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to three V3+ atoms. In the second F1- site, F1- is bonded in a 3-coordinate geometry to three V3+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three V3+ atoms.
DOI: 10.17188/1295435
title: Materials Data on Li3Ni3O3F5 (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: 10.17188/1295436
title: Materials Data on Li4Fe2Co3Sb3O16 (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: 10.17188/1295439
title: Materials Data on Li2Mn3F8 by Materials Project

description: Li2Mn3F8 crystallizes in the orthorhombic Cmce space group. The structure is three-dimensional. Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with nine MnF6 octahedra. The corner-sharing octahedra tilt angles range from 53–57°. There are a spread of Li–F bond distances ranging from 1.91–2.05 Å. There are two inequivalent Mn2+ sites. In the first Mn2+ site, Mn2+ is bonded to six F1- atoms to form MnF6 octahedra that share corners with six equivalent LiF4 tetrahedra and edges with four MnF6 octahedra. There are a spread of Mn–F bond distances ranging from 2.10–2.28 Å. In the second Mn2+ site, Mn2+ is bonded to six F1- atoms to form MnF6 octahedra that share corners with six equivalent LiF4 tetrahedra and edges with four equivalent MnF6 octahedra. There are four shorter (2.15 Å) and two longer (2.18 Å) Mn–F bond lengths. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Mn2+ atoms. In the second F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to one Li1+ and three Mn2+ atoms. In the third F1- site, F1- is bonded in a trigonal planar geometry to one Li1+ and two equivalent Mn2+ atoms.
DOI: 10.17188/1295440
title: Materials Data on LiV2O4 (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: 10.17188/1295441
title: Materials Data on Li3Fe3OF7 (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: 10.17188/1295442
title: Materials Data on Li3VO3F (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: 10.17188/1295443
title: Materials Data on Li5Mn3Cr(PO4)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: 10.17188/1295444
title: Materials Data on Ni3OF5 (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: 10.17188/1295447
title: Materials Data on Li3Ti4VO8 (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: 10.17188/1295448
title: Materials Data on LiFe4(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: 10.17188/1295453
title: Materials Data on Co3(O2F)2 (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: 10.17188/1295454
title: Materials Data on LiVF5 (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: 10.17188/1295455
title: Materials Data on VF5 (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: 10.17188/1295456
title: Materials Data on VF4 (SG:55) 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: 10.17188/1295457
title: Materials Data on Mn6OF11 (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: 10.17188/1295462
title: Materials Data on Na(NiO2)2 by Materials Project

description: Na(NiO2)2 crystallizes in the monoclinic P2/c space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first 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 2.35–2.46 Å. In the second Na1+ site, Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are two shorter (2.35 Å) and four longer (2.44 Å) Na–O bond lengths. There are three inequivalent Ni+3.50+ sites. In the first Ni+3.50+ site, Ni+3.50+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There are a spread of Ni–O bond distances ranging from 1.86–1.98 Å. In the second Ni+3.50+ site, Ni+3.50+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There are a spread of Ni–O bond distances ranging from 1.88–1.98 Å. In the third Ni+3.50+ site, Ni+3.50+ is bonded to six O2- atoms to form edge-sharing NiO6 octahedra. There is two shorter (1.87 Å) and four longer (1.88 Å) Ni–O bond length. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to two Na1+ and three Ni+3.50+ atoms to form distorted ONa2Ni3 trigonal bipyramids that share corners with five ONa2Ni3 trigonal bipyramids, corners with four ONaNi3 trigonal pyramids, edges with four ONa2Ni3 trigonal bipyramids, and edges with four ONaNi3 trigonal pyramids. In the second O2- site, O2- is bonded to two Na1+ and three Ni+3.50+ atoms to form distorted ONa2Ni3 trigonal bipyramids that share corners with five ONa2Ni3 trigonal bipyramids, corners with four ONaNi3 trigonal pyramids, edges with four ONa2Ni3 trigonal bipyramids, and edges with four ONaNi3 trigonal pyramids. In the third O2- site, O2- is bonded to one Na1+ and three Ni+3.50+ atoms to form distorted ONaNi3 trigonal pyramids that share corners with four ONa2Ni3 trigonal bipyramids, corners with six ONaNi3 trigonal pyramids, edges with four ONa2Ni3 trigonal bipyramids, and an edgeedge with one ONaNi3 trigonal pyramid. In the fourth O2- site, O2- is bonded to one Na1+ and three Ni+3.50+ atoms to form distorted ONaNi3 trigonal pyramids that share corners with four ONa2Ni3 trigonal bipyramids, corners with six ONaNi3 trigonal pyramids, edges with four ONa2Ni3 trigonal bipyramids, and an edgeedge with one ONaNi3 trigonal pyramid.
DOI: 10.17188/1295463
title: Materials Data on Li(CoO2)2 by Materials Project

description: Li(CoO2)2 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with twelve CoO6 octahedra, edges with two equivalent LiO6 octahedra, and faces with two CoO6 octahedra. The corner-sharing octahedra tilt angles range from 38–59°. There are a spread of Li–O bond distances ranging from 2.01–2.36 Å. There are two inequivalent Co+3.50+ sites. In the first Co+3.50+ site, Co+3.50+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with six CoO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 39–53°. There are a spread of Co–O bond distances ranging from 1.89–1.93 Å. In the second Co+3.50+ site, Co+3.50+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with six CoO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 38–59°. There are a spread of Co–O bond distances ranging from 1.85–2.08 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Co+3.50+ atoms. In the second O2- site, O2- is bonded to two equivalent Li1+ and three Co+3.50+ atoms to form distorted OLi2Co3 trigonal bipyramids that share corners with four equivalent OLi2Co3 trigonal bipyramids, corners with two equivalent OLiCo3 trigonal pyramids, edges with four OLi2Co3 trigonal bipyramids, and edges with two equivalent OLiCo3 trigonal pyramids. In the third O2- site, O2- is bonded to two equivalent Li1+ and three Co+3.50+ atoms to form distorted OLi2Co3 trigonal bipyramids that share corners with four equivalent OLi2Co3 trigonal bipyramids, corners with three equivalent OLiCo3 trigonal pyramids, edges with four OLi2Co3 trigonal bipyramids, and edges with two equivalent OLiCo3 trigonal pyramids. In the fourth O2- site, O2- is bonded to one Li1+ and three Co+3.50+ atoms to form OLiCo3 trigonal pyramids that share corners with five OLi2Co3 trigonal bipyramids, edges with four OLi2Co3 trigonal bipyramids, and an edgeedge with one OLiCo3 trigonal pyramid.
DOI: 10.17188/1295465
title: Materials Data on Mn12O5F19 (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: 10.17188/1295467
title: Materials Data on FeOF (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: 10.17188/1295469
title: Materials Data on Li5Mn2Co5O12 (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: 10.17188/1295470
title: Materials Data on Fe4O3F5 (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: 10.17188/1295471
title: Materials Data on LiMn(CO3)2 (SG:4) 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