cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1297525
title: Materials Data on Li4Mn3Fe3(CuO8)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: 10.17188/1297526
title: Materials Data on Li3MnPCO7 (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: 10.17188/1297527
title: Materials Data on Li4Mn(OF)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: 10.17188/1297528
title: Materials Data on Li6MnCoP2(CO7)2 (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: 10.17188/1297530
title: Materials Data on Li7(SbS)2 by Materials Project

description: Li7(SbS)2 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are seven inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to three Sb+1.50- and one S2- atom. There are two shorter (2.91 Å) and one longer (3.15 Å) Li–Sb bond lengths. The Li–S bond length is 2.40 Å. In the second Li1+ site, Li1+ is bonded in a 3-coordinate geometry to one Sb+1.50- and two S2- atoms. The Li–Sb bond length is 2.82 Å. There are one shorter (2.36 Å) and one longer (2.45 Å) Li–S bond lengths. In the third Li1+ site, Li1+ is bonded to one Sb+1.50- and three S2- atoms to form a mixture of distorted corner and edge-sharing LiSbS3 tetrahedra. The Li–Sb bond length is 3.02 Å. There are a spread of Li–S bond distances ranging from 2.39–2.45 Å. In the fourth Li1+ site, Li1+ is bonded to one Sb+1.50- and three S2- atoms to form a mixture of distorted corner and edge-sharing LiSbS3 tetrahedra. The Li–Sb bond length is 3.02 Å. There are a spread of Li–S bond distances ranging from 2.46–2.48 Å. In the fifth Li1+ site, Li1+ is bonded in a 3-coordinate geometry to one Sb+1.50- and two equivalent S2- atoms. The Li–Sb bond length is 2.78 Å. There are one shorter (2.33 Å) and one longer (2.43 Å) Li–S bond lengths. In the sixth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to three equivalent Sb+1.50- and one S2- atom. There are a spread of Li–Sb bond distances ranging from 2.89–3.21 Å. The Li–S bond length is 2.47 Å. In the seventh Li1+ site, Li1+ is bonded in a 4-coordinate geometry to two equivalent Sb+1.50- and two S2- atoms. There are one shorter (2.84 Å) and one longer (2.92 Å) Li–Sb bond lengths. There are one shorter (2.37 Å) and one longer (2.42 Å) Li–S bond lengths. There are two inequivalent Sb+1.50- sites. In the first Sb+1.50- site, Sb+1.50- is bonded in a 6-coordinate geometry to four Li1+ and one Sb+1.50- atom. The Sb–Sb bond length is 2.92 Å. In the second Sb+1.50- site, Sb+1.50- is bonded in a 9-coordinate geometry to eight Li1+ and one Sb+1.50- atom. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to seven Li1+ atoms to form distorted edge-sharing SLi7 pentagonal bipyramids. In the second S2- site, S2- is bonded in a 7-coordinate geometry to seven Li1+ atoms.
DOI: 10.17188/1297531
title: Materials Data on V6F13 (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: 10.17188/1297532
title: Materials Data on LiVSi3O8 (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: 10.17188/1297533
title: Materials Data on MnOF2 (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: 10.17188/1297534
title: Materials Data on Li3NiPCO7 (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: 10.17188/1297535
title: Materials Data on Li4Mn3Sn(PO4)4 (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: 10.17188/1297537
title: Materials Data on Li3TiCr3O8 (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: 10.17188/1297538
title: Materials Data on Mn3(OF)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: 10.17188/1297539
title: Materials Data on Li2Si2Ni2O7 (SG:40) 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: 10.17188/1297540
title: Materials Data on LiCoPO4 (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: 10.17188/1297541
title: Materials Data on Li2Si3NiO8 (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: 10.17188/1297542
title: Materials Data on Li2TiCr2O6 (SG:64) 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: 10.17188/1297543
title: Materials Data on Li3MnPCO7 (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: 10.17188/1297544
title: Materials Data on Li2SiNiO4 (SG:144) 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: 10.17188/1297545
title: Materials Data on V(SiO3)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: 10.17188/1297546
title: Materials Data on LiMnO2 (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: 10.17188/1297547
title: Materials Data on Li2ScPCO7 by Materials Project

description: Li2ScCPO7 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. Li1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Li–O bond distances ranging from 1.98–2.59 Å. Sc3+ is bonded to six O2- atoms to form distorted ScO6 octahedra that share corners with four equivalent PO4 tetrahedra. There are a spread of Sc–O bond distances ranging from 2.06–2.21 Å. 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. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four equivalent ScO6 octahedra. The corner-sharing octahedra tilt angles range from 42–64°. There are a spread of P–O bond distances ranging from 1.54–1.57 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to two equivalent Li1+ and one C4+ atom. In the second O2- site, O2- is bonded to two equivalent Li1+, one Sc3+, and one C4+ atom to form distorted edge-sharing OLi2ScC trigonal pyramids. In the third O2- site, O2- is bonded to two equivalent Li1+, one Sc3+, and one C4+ atom to form distorted edge-sharing OLi2ScC trigonal pyramids. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Sc3+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two equivalent Li1+, one Sc3+, and one P5+ atom. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Li1+, one Sc3+, and one P5+ atom.
DOI: 10.17188/1297548
title: Materials Data on Li3CoPCO7 (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: 10.17188/1297549
title: Materials Data on Li3CrPCO7 (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: 10.17188/1297550
title: Materials Data on Mn2Si2O7 (SG:63) 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: 10.17188/1297551
title: Materials Data on Cr5(Si2O7)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: 10.17188/1297552
title: Materials Data on Mn5(Si2O7)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: 10.17188/1297553
title: Materials Data on Li3FePCO7 (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: 10.17188/1297554
title: Materials Data on LiMn5(CuO6)2 (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: 10.17188/1297555
title: Materials Data on LiVF5 (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: 10.17188/1297556
title: Materials Data on LiVF3 (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: 10.17188/1297558
title: Materials Data on Mn5O5F (SG:156) 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: 10.17188/1297559
title: Materials Data on Li6CrCoP2(CO7)2 (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: 10.17188/1297560
title: Materials Data on Li3Cr2P4HO14 (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: 10.17188/1297561
title: Materials Data on CoPO4 (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: 10.17188/1297562
title: Materials Data on LiCo(SiO3)2 (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: 10.17188/1297563
title: Materials Data on NiH12SO9 (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: 10.17188/1297564
title: Materials Data on MnV3Sb2(PO4)6 by Materials Project

description: V3MnSb2(PO4)6 crystallizes in the trigonal R3 space group. The structure is three-dimensional. there are three inequivalent V5+ sites. In the first V5+ site, V5+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six PO4 tetrahedra. There is three shorter (1.90 Å) and three longer (2.05 Å) V–O bond length. In the second V5+ site, V5+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.99 Å) and three longer (2.09 Å) V–O bond lengths. In the third V5+ site, V5+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (1.97 Å) and three longer (2.09 Å) V–O bond lengths. Mn2+ is bonded to six O2- atoms to form distorted MnO6 octahedra that share corners with six PO4 tetrahedra. There are three shorter (2.04 Å) and three longer (2.26 Å) Mn–O bond lengths. There are two inequivalent Sb+0.50+ sites. In the first Sb+0.50+ site, Sb+0.50+ is bonded in a 6-coordinate geometry to six O2- atoms. There are three shorter (2.25 Å) and three longer (2.42 Å) Sb–O bond lengths. In the second Sb+0.50+ site, Sb+0.50+ is bonded in a distorted hexagonal planar geometry to six O2- atoms. There are three shorter (2.35 Å) and three longer (2.42 Å) Sb–O bond lengths. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one MnO6 octahedra and corners with three VO6 octahedra. The corner-sharing octahedra tilt angles range from 27–45°. There are a spread of P–O bond distances ranging from 1.50–1.60 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one MnO6 octahedra and corners with three VO6 octahedra. The corner-sharing octahedra tilt angles range from 26–50°. There are a spread of P–O bond distances ranging from 1.52–1.57 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one V5+ and one P5+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one V5+, one Sb+0.50+, and one P5+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Mn2+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one V5+, one Sb+0.50+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one V5+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a 1-coordinate geometry to one Mn2+, one Sb+0.50+, and one P5+ atom. In the seventh O2- site, O2- is bonded in a 3-coordinate geometry to one V5+, one Sb+0.50+, and one P5+ atom. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one V5+ and one P5+ atom.
DOI: 10.17188/1297565
title: Materials Data on LiMn(SiO3)2 (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: 10.17188/1297566
title: Materials Data on LiNiPO4 (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: 10.17188/1297567
title: Materials Data on Li3Mn2(FeO4)2 by Materials Project

description: (LiMnO2)2LiFeO2FeO2 crystallizes in the triclinic P-1 space group. The structure is one-dimensional and consists of one iron dihydroxide molecule; one LiFeO2 ribbon oriented in the (0, 1, 1) direction; and two LiMnO2 ribbons oriented in the (0, 1, 1) direction. In the LiFeO2 ribbon, Li1+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.63 Å. Fe3+ is bonded in a linear geometry to two equivalent O2- atoms. Both Fe–O bond lengths are 1.41 Å. O2- is bonded in a distorted linear geometry to one Li1+ and one Fe3+ atom. In each LiMnO2 ribbon, Li1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.41 Å. Mn+3.50+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both Mn–O bond lengths are 1.66 Å. O2- is bonded in a 2-coordinate geometry to one Li1+ and one Mn+3.50+ atom.
DOI: 10.17188/1297568
title: Materials Data on Li2Mn2Si2O7 (SG:40) 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: 10.17188/1297570
title: Materials Data on VOF (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: 10.17188/1297576
title: Materials Data on Gd3AsO7 by Materials Project

description: Gd3AsO7 crystallizes in the orthorhombic C222_1 space group. The structure is three-dimensional. there are two inequivalent Gd3+ sites. In the first Gd3+ site, Gd3+ is bonded to seven O2- atoms to form distorted GdO7 pentagonal bipyramids that share corners with two equivalent AsO6 octahedra, a cornercorner with one GdO7 pentagonal bipyramid, edges with two equivalent AsO6 octahedra, and edges with three equivalent GdO7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 43–45°. There are a spread of Gd–O bond distances ranging from 2.23–2.52 Å. In the second Gd3+ site, Gd3+ is bonded in a distorted body-centered cubic geometry to eight O2- atoms. There are a spread of Gd–O bond distances ranging from 2.31–2.80 Å. As5+ is bonded to six O2- atoms to form AsO6 octahedra that share corners with two equivalent AsO6 octahedra, corners with four equivalent GdO7 pentagonal bipyramids, and edges with four equivalent GdO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 36°. There are a spread of As–O bond distances ranging from 1.85–1.96 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Gd3+ and two equivalent As5+ atoms. In the second O2- site, O2- is bonded to four Gd3+ atoms to form a mixture of corner and edge-sharing OGd4 tetrahedra. In the third O2- site, O2- is bonded in a 4-coordinate geometry to three Gd3+ and one As5+ atom. In the fourth O2- site, O2- is bonded to four Gd3+ atoms to form a mixture of corner and edge-sharing OGd4 tetrahedra. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to three Gd3+ and one As5+ atom.