cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1294086
title: Materials Data on Li2FeCo3O8 by Materials Project

description: Li2FeCo3O8 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent FeO6 octahedra, edges with two equivalent LiO6 octahedra, and edges with six CoO6 octahedra. The corner-sharing octahedra tilt angles range from 11–14°. All Li–O bond lengths are 2.14 Å. In the second Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent CoO6 octahedra, edges with two equivalent LiO6 octahedra, edges with two equivalent FeO6 octahedra, and edges with four equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 11–14°. There are two shorter (2.15 Å) and four longer (2.16 Å) Li–O bond lengths. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with two equivalent LiO6 octahedra, and edges with six CoO6 octahedra. The corner-sharing octahedra tilt angles range from 11–14°. There are four shorter (2.03 Å) and two longer (2.04 Å) Fe–O bond lengths. There are two inequivalent Co+3.67+ sites. In the first Co+3.67+ site, Co+3.67+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with two equivalent LiO6 octahedra, edges with two equivalent FeO6 octahedra, and edges with four equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 11–14°. There are four shorter (2.01 Å) and two longer (2.03 Å) Co–O bond lengths. In the second Co+3.67+ site, Co+3.67+ is bonded to six O2- atoms to form CoO6 octahedra that share edges with two equivalent FeO6 octahedra, edges with four LiO6 octahedra, and edges with four CoO6 octahedra. There is two shorter (1.89 Å) and four longer (1.90 Å) Co–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to two Li1+, one Fe3+, and two Co+3.67+ atoms to form a mixture of edge and corner-sharing OLi2FeCo2 square pyramids. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Co+3.67+ atoms. In the third O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+, one Fe3+, and two equivalent Co+3.67+ atoms.
DOI: 10.17188/1294087
title: Materials Data on Co3(OF2)2 by Materials Project

description: Co3(OF2)2 is zeta iron carbide-derived structured and crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are four inequivalent Co+2.67+ sites. In the first Co+2.67+ site, Co+2.67+ is bonded to three O2- and three F1- atoms to form CoO3F3 octahedra that share corners with eight CoOF5 octahedra and edges with two CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 48–53°. There are a spread of Co–O bond distances ranging from 1.84–1.99 Å. There are a spread of Co–F bond distances ranging from 2.07–2.13 Å. In the second Co+2.67+ site, Co+2.67+ is bonded to one O2- and five F1- atoms to form CoOF5 octahedra that share corners with eight CoO3F3 octahedra and edges with two CoOF5 octahedra. The corner-sharing octahedra tilt angles range from 48–60°. The Co–O bond length is 1.95 Å. There are a spread of Co–F bond distances ranging from 2.01–2.14 Å. In the third Co+2.67+ site, Co+2.67+ is bonded to two equivalent O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoOF5 octahedra and edges with two equivalent CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 45–60°. Both Co–O bond lengths are 1.91 Å. There are two shorter (1.98 Å) and two longer (2.11 Å) Co–F bond lengths. In the fourth Co+2.67+ site, Co+2.67+ is bonded to two O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoO3F3 octahedra and edges with two equivalent CoOF5 octahedra. The corner-sharing octahedra tilt angles range from 45–49°. There is one shorter (1.85 Å) and one longer (1.94 Å) Co–O bond length. There are two shorter (2.05 Å) and two longer (2.09 Å) Co–F bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three Co+2.67+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to three Co+2.67+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.67+ atoms. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.67+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.67+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.67+ atoms. In the fourth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.67+ atoms.
DOI: 10.17188/1294088
title: Materials Data on Li4Fe3CuO8 (SG:166) by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1294089
title: Materials Data on Mn6O7F5 (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: 10.17188/1294090
title: Materials Data on VOF2 (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: 10.17188/1294092
title: Materials Data on Co2OF3 (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: 10.17188/1294093
title: Materials Data on Ni3OF5 by Materials Project

description: Ni3OF5 is Hydrophilite-derived structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are three inequivalent Ni+2.33+ sites. In the first Ni+2.33+ site, Ni+2.33+ is bonded to one O2- and five F1- atoms to form a mixture of edge and corner-sharing NiOF5 octahedra. The corner-sharing octahedra tilt angles range from 47–51°. The Ni–O bond length is 1.96 Å. There are a spread of Ni–F bond distances ranging from 2.01–2.05 Å. In the second Ni+2.33+ site, Ni+2.33+ is bonded to one O2- and five F1- atoms to form a mixture of edge and corner-sharing NiOF5 octahedra. The corner-sharing octahedra tilt angles range from 48–52°. The Ni–O bond length is 1.95 Å. There are a spread of Ni–F bond distances ranging from 2.03–2.05 Å. In the third Ni+2.33+ site, Ni+2.33+ is bonded to one O2- and five F1- atoms to form a mixture of edge and corner-sharing NiOF5 octahedra. The corner-sharing octahedra tilt angles range from 47–52°. The Ni–O bond length is 1.96 Å. There are a spread of Ni–F bond distances ranging from 2.02–2.07 Å. O2- is bonded in a distorted trigonal planar geometry to three Ni+2.33+ atoms. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three Ni+2.33+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Ni+2.33+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to three Ni+2.33+ atoms. In the fourth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Ni+2.33+ atoms. In the fifth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Ni+2.33+ atoms.
DOI: 10.17188/1294094
title: Materials Data on LiCo5O3F5 (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: 10.17188/1294095
title: Materials Data on CoOF by Materials Project

description: CoOF is zeta iron carbide-derived structured and crystallizes in the monoclinic P2/m space group. The structure is three-dimensional. there are four inequivalent Co3+ sites. In the first Co3+ site, Co3+ is bonded to four equivalent O2- and two equivalent F1- atoms to form CoO4F2 octahedra that share corners with eight equivalent CoO3F3 octahedra and edges with two equivalent CoO4F2 octahedra. The corner-sharing octahedra tilt angles range from 49–51°. All Co–O bond lengths are 1.89 Å. Both Co–F bond lengths are 2.19 Å. In the second Co3+ site, Co3+ is bonded to two O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoO3F3 octahedra and edges with two equivalent CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 47–52°. There is one shorter (1.84 Å) and one longer (1.85 Å) Co–O bond length. There are two shorter (2.01 Å) and two longer (2.03 Å) Co–F bond lengths. In the third Co3+ site, Co3+ is bonded to three O2- and three F1- atoms to form CoO3F3 octahedra that share corners with eight CoO4F2 octahedra and edges with two equivalent CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 47–52°. There is one shorter (1.81 Å) and two longer (1.87 Å) Co–O bond length. There is two shorter (1.97 Å) and one longer (2.01 Å) Co–F bond length. In the fourth Co3+ site, Co3+ is bonded to four equivalent O2- and two equivalent F1- atoms to form CoO4F2 octahedra that share corners with eight equivalent CoO2F4 octahedra and edges with two equivalent CoO4F2 octahedra. The corner-sharing octahedra tilt angles range from 47–51°. All Co–O bond lengths are 1.89 Å. Both Co–F bond lengths are 2.14 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co3+ atoms. In the second O2- site, O2- is bonded in a trigonal planar geometry to three Co3+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co3+ atoms. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to three Co3+ atoms. In the second F1- site, F1- is bonded in a 3-coordinate geometry to three Co3+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three Co3+ atoms.
DOI: 10.17188/1294096
title: Materials Data on Li4Ti3Fe2Ni3O16 (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: 10.17188/1294097
title: Materials Data on Li3CrFe3O8 (SG:186) 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: 10.17188/1294098
title: Materials Data on Mn3OF5 by Materials Project

description: Mn3OF5 is Hydrophilite-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are four inequivalent Mn+2.33+ sites. In the first Mn+2.33+ site, Mn+2.33+ is bonded to six F1- atoms to form MnF6 octahedra that share corners with eight MnO2F4 octahedra and edges with two equivalent MnOF5 octahedra. The corner-sharing octahedra tilt angles range from 46–59°. There are four shorter (2.13 Å) and two longer (2.17 Å) Mn–F bond lengths. In the second Mn+2.33+ site, Mn+2.33+ is bonded to two equivalent O2- and four F1- atoms to form MnO2F4 octahedra that share corners with eight MnF6 octahedra and edges with two MnO2F4 octahedra. The corner-sharing octahedra tilt angles range from 46–54°. There is one shorter (1.92 Å) and one longer (1.94 Å) Mn–O bond length. There are a spread of Mn–F bond distances ranging from 2.05–2.21 Å. In the third Mn+2.33+ site, Mn+2.33+ is bonded to six F1- atoms to form MnF6 octahedra that share corners with eight MnF6 octahedra and edges with two equivalent MnO2F4 octahedra. The corner-sharing octahedra tilt angles range from 48–59°. There are a spread of Mn–F bond distances ranging from 2.13–2.23 Å. In the fourth Mn+2.33+ site, Mn+2.33+ is bonded to one O2- and five F1- atoms to form MnOF5 octahedra that share corners with eight MnO2F4 octahedra and edges with two MnF6 octahedra. The corner-sharing octahedra tilt angles range from 46–56°. The Mn–O bond length is 2.02 Å. There are a spread of Mn–F bond distances ranging from 2.12–2.22 Å. O2- is bonded in a distorted trigonal planar geometry to three Mn+2.33+ atoms. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three Mn+2.33+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Mn+2.33+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to three Mn+2.33+ atoms. In the fourth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Mn+2.33+ atoms.
DOI: 10.17188/1294100
title: Materials Data on MnOF (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: 10.17188/1294101
title: Materials Data on VO2F (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: 10.17188/1294102
title: Materials Data on CoOF (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: 10.17188/1294103
title: Materials Data on VOF (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: 10.17188/1294104
title: Materials Data on Co2OF3 (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: 10.17188/1294105
title: Materials Data on Li4Co3OF8 (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: 10.17188/1294107
title: Materials Data on Li5CoOF5 (SG:123) 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: 10.17188/1294108
title: Materials Data on V4O5F7 (SG:3) 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: 10.17188/1294109
title: Materials Data on NaFePO4 (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: 10.17188/1294110
title: Materials Data on V2O3F (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: 10.17188/1294111
title: Materials Data on Co3(OF2)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: 10.17188/1294112
title: Materials Data on Co6O7F5 (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: 10.17188/1294113
title: Materials Data on V3O5F by Materials Project

description: V3O5F is beta Vanadium nitride-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are four inequivalent V+3.67+ sites. In the first V+3.67+ site, V+3.67+ is bonded to five O2- and one F1- atom to form VO5F octahedra that share corners with eight VO6 octahedra and edges with two VO5F octahedra. The corner-sharing octahedra tilt angles range from 41–55°. There are a spread of V–O bond distances ranging from 1.87–2.00 Å. The V–F bond length is 2.27 Å. In the second V+3.67+ site, V+3.67+ is bonded to six O2- atoms to form VO6 octahedra that share corners with eight VO5F octahedra and edges with two equivalent VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 49–50°. There are a spread of V–O bond distances ranging from 1.95–2.06 Å. In the third V+3.67+ site, V+3.67+ is bonded to four O2- and two equivalent F1- atoms to form VO4F2 octahedra that share corners with eight VO5F octahedra and edges with two VO6 octahedra. The corner-sharing octahedra tilt angles range from 41–55°. There are a spread of V–O bond distances ranging from 1.81–1.96 Å. There are one shorter (2.05 Å) and one longer (2.12 Å) V–F bond lengths. In the fourth V+3.67+ site, V+3.67+ is bonded to six O2- atoms to form VO6 octahedra that share corners with eight VO6 octahedra and edges with two equivalent VO5F octahedra. The corner-sharing octahedra tilt angles range from 43–49°. There is four shorter (1.95 Å) and two longer (2.00 Å) V–O bond length. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three V+3.67+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three V+3.67+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to three V+3.67+ atoms. In the fourth O2- site, O2- is bonded in a distorted T-shaped geometry to three V+3.67+ atoms. F1- is bonded in a distorted trigonal planar geometry to three V+3.67+ atoms.
DOI: 10.17188/1294114
title: Materials Data on VO2F (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: 10.17188/1294115
title: Materials Data on Co3OF5 (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: 10.17188/1294116
title: Materials Data on V6O5F19 (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