cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1292819
title: Materials Data on LiFeSiO4 (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: 10.17188/1292820
title: Materials Data on LiFe(PO3)3 by Materials Project

description: LiFe(PO3)3 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Li1+ is bonded in a 2-coordinate geometry to three O2- atoms. There are a spread of Li–O bond distances ranging from 1.89–2.41 Å. Fe2+ is bonded to five O2- atoms to form distorted FeO5 square pyramids that share corners with five PO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 2.07–2.27 Å. There are three inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent FeO5 square pyramids and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.50–1.61 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one FeO5 square pyramid and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.49–1.62 Å. In the third P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent FeO5 square pyramids and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.49–1.61 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Fe2+ and one P5+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe2+, and one P5+ atom. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Fe2+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe2+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms. In the seventh O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two P5+ atoms. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one Fe2+ and one P5+ atom. In the ninth O2- site, O2- is bonded in a bent 150 degrees geometry to one Li1+ and one P5+ atom.
DOI: 10.17188/1292821
title: Materials Data on Li4Mn3Nb2Sn3O16 (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: 10.17188/1292822
title: Materials Data on Li2(NiO2)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: 10.17188/1292823
title: Materials Data on Li6V3P6WO24 (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: 10.17188/1292824
title: Materials Data on LiFe5P3O13 (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: 10.17188/1292825
title: Materials Data on LiFeP2O7 (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: 10.17188/1292826
title: Materials Data on Mn2(CO3)3 by Materials Project

description: Mn2(CO3)3 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent Mn3+ sites. In the first Mn3+ site, Mn3+ is bonded to six O2- atoms to form distorted face-sharing MnO6 octahedra. There are a spread of Mn–O bond distances ranging from 1.95–2.35 Å. In the second Mn3+ site, Mn3+ is bonded to six O2- atoms to form distorted face-sharing MnO6 octahedra. There are a spread of Mn–O bond distances ranging from 1.93–2.27 Å. There are three 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 1.28–1.31 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 1.26–1.32 Å. In the third 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 1.27–1.32 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn3+ and one C4+ atom. In the second O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn3+ and one C4+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two Mn3+ and one C4+ atom. In the fourth O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn3+ and one C4+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Mn3+ and one C4+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to two Mn3+ and one C4+ atom. In the seventh O2- site, O2- is bonded in a 3-coordinate geometry to two Mn3+ and one C4+ atom. In the eighth O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn3+ and one C4+ atom. In the ninth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Mn3+ and one C4+ atom.
DOI: 10.17188/1292827
title: Materials Data on Li2Mn2NiO6 (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: 10.17188/1292828
title: Materials Data on LiFe4(PO4)3 (SG:9) 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: 10.17188/1292831
title: Materials Data on Li8(NiO2)11 (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: 10.17188/1292832
title: Materials Data on LiFeSiO4 (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: 10.17188/1292833
title: Materials Data on V(TeO3)4 by Materials Project

description: V(TeO3)4 crystallizes in the triclinic P1 space group. The structure is three-dimensional. V4+ is bonded to six O2- atoms to form distorted VO6 octahedra that share edges with three TeO6 octahedra. There are a spread of V–O bond distances ranging from 1.87–2.20 Å. There are four inequivalent Te5+ sites. In the first Te5+ site, Te5+ is bonded to six O2- atoms to form TeO6 octahedra that share an edgeedge with one VO6 octahedra. There are a spread of Te–O bond distances ranging from 1.90–2.03 Å. In the second Te5+ site, Te5+ is bonded to six O2- atoms to form TeO6 octahedra that share edges with two equivalent VO6 octahedra. There are a spread of Te–O bond distances ranging from 1.93–1.99 Å. In the third Te5+ site, Te5+ is bonded in a 4-coordinate geometry to six O2- atoms. There are a spread of Te–O bond distances ranging from 1.91–2.80 Å. In the fourth Te5+ site, Te5+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Te–O bond distances ranging from 1.95–2.67 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted water-like geometry to one V4+ and two Te5+ atoms. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Te5+ atoms. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to two Te5+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to one V4+ and two Te5+ atoms. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to two Te5+ atoms. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to two Te5+ atoms. In the seventh O2- site, O2- is bonded in a water-like geometry to one V4+ and one Te5+ atom. In the eighth O2- site, O2- is bonded in a 2-coordinate geometry to one V4+ and two Te5+ atoms. In the ninth O2- site, O2- is bonded in a distorted T-shaped geometry to one V4+ and two Te5+ atoms. In the tenth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Te5+ atoms. In the eleventh O2- site, O2- is bonded in a distorted water-like geometry to one V4+ and two Te5+ atoms. In the twelfth O2- site, O2- is bonded in a bent 120 degrees geometry to two Te5+ atoms.
DOI: 10.17188/1292834
title: Materials Data on Li2Fe3P9O28 (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: 10.17188/1292835
title: Materials Data on LiFeSiO4 (SG:173) 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: 10.17188/1292836
title: Materials Data on Li4V2Fe5O12 (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: 10.17188/1292837
title: Materials Data on LiMnPO4F (SG:9) 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: 10.17188/1292838
title: Materials Data on Li2Ti(FeO3)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: 10.17188/1292839
title: Materials Data on Li3V3(FeO5)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: 10.17188/1292840
title: Materials Data on LiFeSiO4 (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: 10.17188/1292841
title: Materials Data on LiFeSiO4 (SG:95) 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: 10.17188/1292842
title: Materials Data on Li4Ti2Fe5O12 (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: 10.17188/1292843
title: Materials Data on Li7FeP4O14F (SG:9) 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: 10.17188/1292845
title: Materials Data on Li3TiFe3O8 (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: 10.17188/1292847
title: Materials Data on Li4Ti3(FeO4)3 (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: 10.17188/1292848
title: Materials Data on LiFeSiO4 (SG:61) 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: 10.17188/1292849
title: Materials Data on Li3Cr4P2O8F9 (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: 10.17188/1292850
title: Materials Data on LiMn(PO3)3 (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: 10.17188/1292851
title: Materials Data on Li5MnP2(O4F)2 (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: 10.17188/1292853
title: Materials Data on LiTiFeO4 (SG:74) by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1292854
title: Materials Data on Li3Ti2(FeO4)2 by Materials Project

description: LiTiO2(LiFeO2)2TiO2 crystallizes in the triclinic P-1 space group. The structure is one-dimensional and consists of one titanium dihydroxide molecule; two LiFeO2 ribbons oriented in the (1, 1, 1) direction; and one LiTiO2 ribbon oriented in the (1, 1, 1) direction. In each LiFeO2 ribbon, Li1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.43 Å. Fe+2.50+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both Fe–O bond lengths are 1.68 Å. O2- is bonded in a 2-coordinate geometry to one Li1+ and one Fe+2.50+ atom. In the LiTiO2 ribbon, Li1+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.70 Å. Ti4+ is bonded in a linear geometry to two equivalent O2- atoms. Both Ti–O bond lengths are 1.36 Å. O2- is bonded in a distorted linear geometry to one Li1+ and one Ti4+ atom.
DOI: 10.17188/1292855
title: Materials Data on LiFeSiO4 (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: 10.17188/1292856
title: Materials Data on Li4Fe(SiO4)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: 10.17188/1292857
title: Materials Data on Li3FeSiO5 (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: 10.17188/1292858
title: Materials Data on Li5Mn4P4O16F (SG:82) 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: 10.17188/1292859
title: Materials Data on Li3Fe(PO4)2 (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: 10.17188/1292860
title: Materials Data on Li7MnP4O14F (SG:9) 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: 10.17188/1292861
title: Materials Data on LiTiFe2O5 (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: 10.17188/1292862
title: Materials Data on Li3VFe3O8 by Materials Project

description: LiVO2(LiFeO2)2FeO2 crystallizes in the triclinic P-1 space group. The structure is one-dimensional and consists of one iron dihydroxide molecule; two LiFeO2 ribbons oriented in the (0, 1, 1) direction; and one LiVO2 ribbon oriented in the (0, 1, 1) direction. In each LiFeO2 ribbon, Li1+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.61 Å. Fe+2.67+ is bonded in a linear geometry to two equivalent O2- atoms. Both Fe–O bond lengths are 1.44 Å. O2- is bonded in a distorted bent 150 degrees geometry to one Li1+ and one Fe+2.67+ atom. In the LiVO2 ribbon, Li1+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.60 Å. V5+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both V–O bond lengths are 1.41 Å. O2- is bonded in a linear geometry to one Li1+ and one V5+ atom.
DOI: 10.17188/1292863
title: Materials Data on Li2Fe(PO4)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: 10.17188/1292864
title: Materials Data on Li4Fe3P3O12F (SG:218) 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: 10.17188/1292865
title: Materials Data on LiMn(PO3)3 (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: 10.17188/1292866
title: Materials Data on Li2FeSi4O11 (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: 10.17188/1292867
title: Materials Data on Li2Mn3(P2O7)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
DOI: 10.17188/1292868
title: Materials Data on Li2Fe3(SiO4)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: 10.17188/1292869
title: Materials Data on LiMn2(PO4)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: 10.17188/1292870
title: Materials Data on Li2FeSi4O11 (SG:87) 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: 10.17188/1292871
title: Materials Data on Li2Mn2P2O9 (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