cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1295920
title: Materials Data on LiAgF4 by Materials Project

description: LiAgF4 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to five F1- atoms to form distorted LiF5 trigonal bipyramids that share corners with six AgF6 octahedra. The corner-sharing octahedra tilt angles range from 45–67°. There are a spread of Li–F bond distances ranging from 1.96–2.08 Å. In the second Li1+ site, Li1+ is bonded in a 5-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.96–2.30 Å. There are two inequivalent Ag3+ sites. In the first Ag3+ site, Ag3+ is bonded to six F1- atoms to form AgF6 octahedra that share corners with four AgF6 octahedra and corners with four equivalent LiF5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 42–50°. There are a spread of Ag–F bond distances ranging from 1.94–2.24 Å. In the second Ag3+ site, Ag3+ is bonded to six F1- atoms to form AgF6 octahedra that share corners with four AgF6 octahedra and corners with two equivalent LiF5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 42–56°. There are a spread of Ag–F bond distances ranging from 2.00–2.30 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Li1+ and one Ag3+ atom. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Ag3+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent Ag3+ atoms. In the fourth F1- site, F1- is bonded in a trigonal planar geometry to one Li1+ and two equivalent Ag3+ atoms. In the fifth F1- site, F1- is bonded in a trigonal non-coplanar geometry to two Li1+ and one Ag3+ atom.
DOI: 10.17188/1295921
title: Materials Data on LiCuF4 by Materials Project

description: LiCuF4 is Hydrophilite-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.97–2.42 Å. Cu3+ is bonded to six F1- atoms to form corner-sharing CuF6 octahedra. The corner-sharing octahedral tilt angles are 46°. There are a spread of Cu–F bond distances ranging from 1.88–1.97 Å. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a trigonal planar geometry to two equivalent Li1+ and one Cu3+ atom. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to two equivalent Li1+ and one Cu3+ atom. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent Cu3+ atoms. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to one Li1+ and two equivalent Cu3+ atoms.
DOI: 10.17188/1295922
title: Materials Data on Li8NbNi3(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: 10.17188/1295923
title: Materials Data on V5F11 (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: 10.17188/1295924
title: Materials Data on LaHSe3O10 by Materials Project

description: LaHSe3O8O2 crystallizes in the orthorhombic Pbca space group. The structure is two-dimensional and consists of eight hydrogen peroxide molecules and two LaHSe3O8 sheets oriented in the (0, 0, 1) direction. In each LaHSe3O8 sheet, La3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of La–O bond distances ranging from 2.42–2.83 Å. H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.98 Å. There are three inequivalent Se+5.33+ sites. In the first Se+5.33+ site, Se+5.33+ is bonded in a trigonal non-coplanar geometry to three O2- atoms. There are a spread of Se–O bond distances ranging from 1.69–1.83 Å. In the second Se+5.33+ site, Se+5.33+ is bonded in a trigonal non-coplanar geometry to three O2- atoms. There are a spread of Se–O bond distances ranging from 1.68–1.88 Å. In the third Se+5.33+ site, Se+5.33+ is bonded in a distorted trigonal non-coplanar geometry to three O2- atoms. There are a spread of Se–O bond distances ranging from 1.68–1.90 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one La3+ and one Se+5.33+ atom. In the second O2- site, O2- is bonded in a distorted water-like geometry to one H1+ and one Se+5.33+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent La3+ and one Se+5.33+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one La3+ and two Se+5.33+ atoms. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one La3+ and one Se+5.33+ atom. In the sixth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one La3+ and one Se+5.33+ atom. In the seventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one La3+ and one Se+5.33+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one La3+ and one Se+5.33+ atom.
DOI: 10.17188/1295926
title: Materials Data on Li4V3P8O29 (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: 10.17188/1295927
title: Materials Data on Li2VF6 (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: 10.17188/1295928
title: Materials Data on Li3V2(OF)3 by Materials Project

description: Li3V2(OF)3 is Aluminum carbonitride-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 5-coordinate geometry to one O2- and four F1- atoms. The Li–O bond length is 2.35 Å. There are a spread of Li–F bond distances ranging from 1.91–1.93 Å. In the second Li1+ site, Li1+ is bonded to one O2- and three equivalent F1- atoms to form LiOF3 tetrahedra that share corners with three equivalent VO6 octahedra and corners with nine LiOF3 tetrahedra. The corner-sharing octahedra tilt angles range from 65–67°. The Li–O bond length is 2.02 Å. There are a spread of Li–F bond distances ranging from 1.93–1.95 Å. In the third Li1+ site, Li1+ is bonded to four F1- atoms to form corner-sharing LiF4 tetrahedra. There are a spread of Li–F bond distances ranging from 1.90–1.95 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to six O2- atoms to form VO6 octahedra that share corners with three equivalent LiOF3 tetrahedra, corners with three equivalent VO4F trigonal bipyramids, and edges with six equivalent VO6 octahedra. There are a spread of V–O bond distances ranging from 2.00–2.23 Å. In the second V3+ site, V3+ is bonded to four O2- and one F1- atom to form distorted VO4F trigonal bipyramids that share corners with three equivalent VO6 octahedra and corners with six equivalent VO4F trigonal bipyramids. The corner-sharing octahedra tilt angles range from 57–60°. There are a spread of V–O bond distances ranging from 1.89–1.94 Å. The V–F bond length is 2.28 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Li1+ and three equivalent V3+ atoms. In the second O2- site, O2- is bonded to one Li1+ and three equivalent V3+ atoms to form OLiV3 tetrahedra that share corners with three equivalent FLi4 tetrahedra, corners with six equivalent OLiV3 tetrahedra, corners with three equivalent OV4 trigonal pyramids, and edges with three equivalent OV4 trigonal pyramids. In the third O2- site, O2- is bonded to four V3+ atoms to form distorted OV4 trigonal pyramids that share a cornercorner with one FLi3V tetrahedra, corners with three equivalent OLiV3 tetrahedra, corners with six equivalent OV4 trigonal pyramids, and edges with three equivalent OLiV3 tetrahedra. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded to four Li1+ atoms to form corner-sharing FLi4 tetrahedra. In the second F1- site, F1- is bonded to three equivalent Li1+ and one V3+ atom to form distorted FLi3V tetrahedra that share corners with nine FLi4 tetrahedra and a cornercorner with one OV4 trigonal pyramid. In the third F1- site, F1- is bonded to four Li1+ atoms to form FLi4 tetrahedra that share corners with three equivalent OLiV3 tetrahedra and corners with nine FLi4 tetrahedra.
DOI: 10.17188/1295929
title: Materials Data on Li3VOF5 by Materials Project

description: Li3VOF5 crystallizes in the monoclinic Pc space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to one O2- and five F1- atoms to form LiOF5 octahedra that share corners with six equivalent VOF5 octahedra. The corner-sharing octahedra tilt angles range from 39–51°. The Li–O bond length is 2.10 Å. There are a spread of Li–F bond distances ranging from 2.00–2.23 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to one O2- and three F1- atoms. The Li–O bond length is 2.12 Å. There are a spread of Li–F bond distances ranging from 1.93–2.13 Å. In the third Li1+ site, Li1+ is bonded in a 7-coordinate geometry to two equivalent O2- and five F1- atoms. There are one shorter (2.61 Å) and one longer (2.65 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.97–2.45 Å. V4+ is bonded to one O2- and five F1- atoms to form VOF5 octahedra that share corners with six equivalent LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 39–51°. The V–O bond length is 1.67 Å. There are a spread of V–F bond distances ranging from 1.96–2.04 Å. O2- is bonded in a 3-coordinate geometry to four Li1+ and one V4+ atom. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded to three Li1+ and one V4+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the second F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V4+ atom. In the third F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V4+ atom. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V4+ atom. In the fifth F1- site, F1- is bonded to three Li1+ and one V4+ atom to form distorted corner-sharing FLi3V tetrahedra.
DOI: 10.17188/1295930
title: Materials Data on Li5VO4F (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: 10.17188/1295931
title: Materials Data on Ni(Pt3O4)4 by Materials Project

description: Ni(Pt3O4)4 crystallizes in the cubic Fm-3 space group. The structure is three-dimensional. Pt+2.50+ is bonded in a square co-planar geometry to four O2- atoms. There are two shorter (2.00 Å) and two longer (2.03 Å) Pt–O bond lengths. Ni2+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Ni–O bond lengths are 2.23 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Pt+2.50+ atoms. In the second O2- site, O2- is bonded to three equivalent Pt+2.50+ and one Ni2+ atom to form a mixture of edge and corner-sharing ONiPt3 trigonal pyramids.
DOI: 10.17188/1295932
title: Materials Data on LiV2O3F (SG:44) 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: 10.17188/1295933
title: Materials Data on Li2VF4 (SG:148) 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: 10.17188/1295934
title: Materials Data on Li10Mn2V3Cr3O16 (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: 10.17188/1295935
title: Materials Data on LiVF4 (SG:31) 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: 10.17188/1295936
title: Materials Data on LiVOF2 (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: 10.17188/1295937
title: Materials Data on LiVF4 (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: 10.17188/1295938
title: Materials Data on LiVF5 (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: 10.17188/1295939
title: Materials Data on Li7V3P8O29 (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: 10.17188/1295940
title: Materials Data on Li5V3Cu(PO4)4 (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: 10.17188/1295941
title: Materials Data on Li5V3P8O29 (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: 10.17188/1295994
title: Materials Data on Li5Ni3O5F3 (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: 10.17188/1295995
title: Materials Data on Li6Ni11(OF12)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: 10.17188/1295996
title: Materials Data on Li3V4O7F5 (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: 10.17188/1295997
title: Materials Data on Mn3CoSn2(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: 10.17188/1295998
title: Materials Data on Li2VFeP2(HO5)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: 10.17188/1295999
title: Materials Data on LiMnVP2(HO5)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: 10.17188/1296000
title: Materials Data on LiV5F11 (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: 10.17188/1296001
title: Materials Data on Li9Ti7Cr6O30 (SG:143) 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: 10.17188/1296002
title: Materials Data on Li15Mn8P8(O4F)8 (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: 10.17188/1296003
title: Materials Data on LiV3O5F3 (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: 10.17188/1296004
title: Materials Data on LiMn2F7 (SG:13) 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: 10.17188/1296005
title: Materials Data on LiV(CO3)2 by Materials Project

description: LiV(CO3)2 is Calcite-derived structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with two equivalent LiO6 octahedra, corners with two equivalent VO6 octahedra, and an edgeedge with one VO6 octahedra. The corner-sharing octahedra tilt angles range from 50–70°. There are a spread of Li–O bond distances ranging from 2.01–2.52 Å. V3+ is bonded to six O2- atoms to form VO6 octahedra that share corners with two equivalent LiO6 octahedra, corners with two equivalent VO6 octahedra, and an edgeedge with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 50–61°. There are a spread of V–O bond distances ranging from 2.00–2.22 Å. There are two inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.26–1.33 Å. In the second C4+ site, C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.27–1.33 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Li1+ and one C4+ atom. In the second O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one V3+, and one C4+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one V3+, and one C4+ atom. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to one Li1+, one V3+, and one C4+ atom. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+, one V3+, and one C4+ atom. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent V3+ and one C4+ atom.
DOI: 10.17188/1296006
title: Materials Data on Li5NiO3F (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: 10.17188/1296007
title: Materials Data on LiV(CO3)2 (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: 10.17188/1296008
title: Materials Data on LiNiPO4 (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: 10.17188/1296010
title: Materials Data on LiNiPO4 (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: 10.17188/1296012
title: Materials Data on Li10Cr3P6(O4F)6 (SG:143) 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