cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1285370
title: Materials Data on SiHC3O by Materials Project

description: SiC3HO crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four (dimethylsilyl)methanol molecules and eight SiC3HO clusters. In four of the SiC3HO clusters, Si4+ is bonded in a 4-coordinate geometry to three C1- and one H1+ atom. There are a spread of Si–C bond distances ranging from 1.80–1.86 Å. The Si–H bond length is 1.48 Å. There are three inequivalent C1- sites. In the first C1- site, C1- is bonded in a 2-coordinate geometry to one Si4+ and one C1- atom. The C–C bond length is 1.29 Å. In the second C1- site, C1- is bonded in a 2-coordinate geometry to one Si4+ and one C1- atom. In the third C1- site, C1- is bonded in a linear geometry to one Si4+ and one O2- atom. The C–O bond length is 1.17 Å. H1+ is bonded in a single-bond geometry to one Si4+ atom. O2- is bonded in a single-bond geometry to one C1- atom. In four of the SiC3HO clusters, Si4+ is bonded in a rectangular see-saw-like geometry to three C1- and one H1+ atom. There are a spread of Si–C bond distances ranging from 1.83–1.85 Å. The Si–H bond length is 1.48 Å. There are three inequivalent C1- sites. In the first C1- site, C1- is bonded in a 2-coordinate geometry to one Si4+ and one C1- atom. The C–C bond length is 1.29 Å. In the second C1- site, C1- is bonded in a 2-coordinate geometry to one Si4+ and one C1- atom. In the third C1- site, C1- is bonded in a distorted linear geometry to one Si4+ and one O2- atom. The C–O bond length is 1.16 Å. H1+ is bonded in a single-bond geometry to one Si4+ atom. O2- is bonded in a single-bond geometry to one C1- atom.
DOI: 10.17188/1285371
title: Materials Data on Ni3(BiO2)10 (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: 10.17188/1285372
title: Materials Data on Fe2SiO4 (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: 10.17188/1285373
title: Materials Data on La7Mn8O24 (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: 10.17188/1285375
title: Materials Data on Li21Mo11O32 (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: 10.17188/1285378
title: Materials Data on La6Mn5O18 (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: 10.17188/1285379
title: Materials Data on Fe21O32 (SG:155) 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: 10.17188/1285380
title: Materials Data on Co5Te4(BrO6)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: 10.17188/1285382
title: Materials Data on Li5Mn7O16 (SG:58) 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: 10.17188/1285383
title: Materials Data on Sr24Ni19O54 (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: 10.17188/1285386
title: Materials Data on Li10Mn21O48 (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: 10.17188/1285388
title: Materials Data on Co9Ru3O16 (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: 10.17188/1285389
title: Materials Data on Ta by Materials Project

description: Ta is Copper structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ta is bonded to twelve equivalent Ta atoms to form a mixture of corner, edge, and face-sharing TaTa12 cuboctahedra. All Ta–Ta bond lengths are 2.99 Å.
DOI: 10.17188/1285390
title: Materials Data on Li11Mn13O32 (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: 10.17188/1285392
title: Materials Data on CaGaBiB2O7 by Materials Project

description: CaGaBBiO6BO crystallizes in the tetragonal P-42_1m space group. The structure is three-dimensional and consists of four boron monoxide molecules and one CaGaBBiO6 framework. In the CaGaBBiO6 framework, Ca2+ is bonded to six O2- atoms to form distorted CaO6 octahedra that share a cornercorner with one CaO6 octahedra, a cornercorner with one BO4 tetrahedra, corners with two equivalent GaO4 tetrahedra, and edges with two equivalent BO4 tetrahedra. The corner-sharing octahedral tilt angles are 74°. There are a spread of Ca–O bond distances ranging from 2.24–2.66 Å. There are two inequivalent Ga3+ sites. In the first Ga3+ site, Ga3+ is bonded to four equivalent O2- atoms to form GaO4 tetrahedra that share corners with four equivalent CaO6 octahedra and corners with four equivalent BO4 tetrahedra. The corner-sharing octahedral tilt angles are 67°. All Ga–O bond lengths are 1.91 Å. In the second Ga3+ site, Ga3+ is bonded in a 4-coordinate geometry to four equivalent O2- atoms. All Ga–O bond lengths are 1.89 Å. B3+ is bonded to four O2- atoms to form BO4 tetrahedra that share a cornercorner with one CaO6 octahedra, a cornercorner with one BO4 tetrahedra, corners with two equivalent GaO4 tetrahedra, and edges with two equivalent CaO6 octahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of B–O bond distances ranging from 1.43–1.55 Å. Bi3+ is bonded in a 1-coordinate geometry to seven O2- atoms. There are a spread of Bi–O bond distances ranging from 2.13–2.90 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to one Ca2+, one Ga3+, one Bi3+, and one O2- atom. The O–O bond length is 1.59 Å. In the second O2- site, O2- is bonded in a water-like geometry to two equivalent Bi3+ atoms. In the third O2- site, O2- is bonded in a 1-coordinate geometry to one Ca2+, one B3+, and two equivalent Bi3+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to one Ca2+, one Ga3+, one B3+, and one Bi3+ atom. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ca2+ and two equivalent B3+ atoms.
DOI: 10.17188/1285393
title: Materials Data on La10Mn9O30 (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: 10.17188/1285394
title: Materials Data on Ti5Fe11O24 (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: 10.17188/1285396
title: Materials Data on Rb(WO3)6 by Materials Project

description: Rb(WO3)6 crystallizes in the orthorhombic Pnnm space group. The structure is three-dimensional. Rb1+ is bonded to twelve O2- atoms to form RbO12 cuboctahedra that share edges with twelve WO6 octahedra. All Rb–O bond lengths are 3.36 Å. There are two inequivalent W+5.83+ sites. In the first W+5.83+ site, W+5.83+ is bonded to six O2- atoms to form WO6 octahedra that share corners with six WO6 octahedra and edges with two equivalent RbO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–30°. There are a spread of W–O bond distances ranging from 1.92–1.97 Å. In the second W+5.83+ site, W+5.83+ is bonded to six O2- atoms to form WO6 octahedra that share corners with six WO6 octahedra and edges with two equivalent RbO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–30°. There are a spread of W–O bond distances ranging from 1.92–1.97 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent W+5.83+ atoms. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Rb1+ and two W+5.83+ atoms. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Rb1+ and two W+5.83+ atoms. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to one Rb1+ and two equivalent W+5.83+ atoms. In the fifth O2- site, O2- is bonded in a linear geometry to two equivalent W+5.83+ atoms. In the sixth O2- site, O2- is bonded in a linear geometry to two equivalent W+5.83+ atoms.
DOI: 10.17188/1285399
title: Materials Data on Rb3FeF3 by Materials Project

description: Rb3FeF3 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Rb sites. In the first Rb site, Rb is bonded in a 5-coordinate geometry to five F atoms. There are a spread of Rb–F bond distances ranging from 2.95–3.35 Å. In the second Rb site, Rb is bonded in a T-shaped geometry to three F atoms. There are a spread of Rb–F bond distances ranging from 2.64–2.80 Å. In the third Rb site, Rb is bonded in a 6-coordinate geometry to six F atoms. There are a spread of Rb–F bond distances ranging from 2.87–3.38 Å. In the fourth Rb site, Rb is bonded in a T-shaped geometry to three F atoms. There are a spread of Rb–F bond distances ranging from 2.64–2.76 Å. In the fifth Rb site, Rb is bonded in a 5-coordinate geometry to five F atoms. There are a spread of Rb–F bond distances ranging from 2.92–3.24 Å. In the sixth Rb site, Rb is bonded in a 5-coordinate geometry to five F atoms. There are a spread of Rb–F bond distances ranging from 2.99–3.28 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded in a T-shaped geometry to three F atoms. There are a spread of Fe–F bond distances ranging from 2.12–2.14 Å. In the second Fe site, Fe is bonded in a T-shaped geometry to three F atoms. There are a spread of Fe–F bond distances ranging from 2.13–2.16 Å. There are six inequivalent F sites. In the first F site, F is bonded to five Rb and one Fe atom to form distorted corner-sharing FRb5Fe octahedra. The corner-sharing octahedral tilt angles are 8°. In the second F site, F is bonded in a 6-coordinate geometry to five Rb and one Fe atom. In the third F site, F is bonded in a 5-coordinate geometry to four Rb and one Fe atom. In the fourth F site, F is bonded in a 6-coordinate geometry to five Rb and one Fe atom. In the fifth F site, F is bonded in a 4-coordinate geometry to three Rb and one Fe atom. In the sixth F site, F is bonded in a 6-coordinate geometry to five Rb and one Fe atom.
DOI: 10.17188/1285404
title: Materials Data on La8Mn7O24 (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: 10.17188/1285405
title: Materials Data on Li9Ni23O32 (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: 10.17188/1285406
title: Materials Data on K3Sc(HO)6 by Materials Project

description: K3Sc(H2O3)2H2 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional and consists of four hydrogen molecules and one K3Sc(H2O3)2 framework. In the K3Sc(H2O3)2 framework, there are two inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 2-coordinate geometry to four H1+ and six O2- atoms. There are two shorter (2.82 Å) and two longer (2.85 Å) K–H bond lengths. There are a spread of K–O bond distances ranging from 2.61–3.08 Å. In the second K1+ site, K1+ is bonded in a 2-coordinate geometry to three O2- atoms. There are a spread of K–O bond distances ranging from 2.52–2.65 Å. Sc3+ is bonded in an octahedral geometry to six O2- atoms. There are a spread of Sc–O bond distances ranging from 2.07–2.20 Å. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one K1+ and one O2- atom. The H–O bond length is 0.97 Å. In the second H1+ site, H1+ is bonded in a distorted single-bond geometry to one K1+ and one H1+ atom. The H–H bond length is 0.76 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to two K1+, one Sc3+, and one O2- atom. The O–O bond length is 1.53 Å. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two K1+, one Sc3+, and one O2- atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two K1+, one Sc3+, and one H1+ atom.
DOI: 10.17188/1285407
title: Materials Data on La17Mn18O54 (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: 10.17188/1285408
title: Materials Data on Ga2NiO4 (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: 10.17188/1285413
title: Materials Data on Al2NiO4 (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: 10.17188/1285415
title: Materials Data on NaMgFe(SO4)3 by Materials Project

description: NaMgFe(SO4)3 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a distorted hexagonal planar geometry to six equivalent O2- atoms. All Na–O bond lengths are 2.45 Å. In the second Na1+ site, Na1+ is bonded in a distorted hexagonal planar geometry to six equivalent O2- atoms. All Na–O bond lengths are 2.56 Å. Mg2+ is bonded to six O2- atoms to form MgO6 octahedra that share corners with six equivalent SO4 tetrahedra. There are three shorter (2.04 Å) and three longer (2.09 Å) Mg–O bond lengths. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent SO4 tetrahedra. There are three shorter (1.99 Å) and three longer (2.07 Å) Fe–O bond lengths. S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with two equivalent MgO6 octahedra and corners with two equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 24–40°. There are a spread of S–O bond distances ranging from 1.46–1.51 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Fe3+ and one S6+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Mg2+, and one S6+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Fe3+, and one S6+ atom. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to one Mg2+ and one S6+ atom.
DOI: 10.17188/1285419
title: Materials Data on Nd2(MoO4)3 by Materials Project

description: Nd2(MoO4)3 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent Nd3+ sites. In the first Nd3+ site, Nd3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Nd–O bond distances ranging from 2.44–2.57 Å. In the second Nd3+ site, Nd3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Nd–O bond distances ranging from 2.44–2.56 Å. There are three inequivalent Mo6+ sites. In the first Mo6+ site, Mo6+ is bonded in a tetrahedral geometry to four O2- atoms. There is two shorter (1.77 Å) and two longer (1.84 Å) Mo–O bond length. In the second Mo6+ site, Mo6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of Mo–O bond distances ranging from 1.78–1.86 Å. In the third Mo6+ site, Mo6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of Mo–O bond distances ranging from 1.78–1.86 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Nd3+ and one Mo6+ atom. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Nd3+ and one Mo6+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Nd3+ and one Mo6+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Nd3+ and one Mo6+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Nd3+ and one Mo6+ atom. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Nd3+ and one Mo6+ atom. In the seventh O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Nd3+ and one Mo6+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Nd3+ and one Mo6+ atom. In the ninth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Nd3+ and one Mo6+ atom. In the tenth O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Nd3+ and one Mo6+ atom. In the eleventh O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Nd3+ and one Mo6+ atom. In the twelfth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Nd3+ and one Mo6+ atom.
DOI: 10.17188/1285423
title: Materials Data on V2Bi4O11 (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: 10.17188/1285426
title: Materials Data on NaCaGaSi2O7 by Materials Project

description: NaCaGaSi2O7 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Na1+ is bonded in a distorted see-saw-like geometry to four O2- atoms. There are a spread of Na–O bond distances ranging from 2.30–2.49 Å. Ca2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ca–O bond distances ranging from 2.23–2.73 Å. Ga3+ is bonded in an L-shaped geometry to two O2- atoms. There are one shorter (1.95 Å) and one longer (2.35 Å) Ga–O bond lengths. There are two inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.61–1.69 Å. In the second Si4+ site, Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.60–1.69 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Ca2+ and two Si4+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one Na1+, one Ca2+, one Ga3+, and one Si4+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Ca2+, and one Si4+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Na1+, one Ca2+, and one O2- atom. The O–O bond length is 1.49 Å. In the fifth O2- site, O2- is bonded in a 2-coordinate geometry to one Ca2+, one Si4+, and one O2- atom. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Ca2+ and two Si4+ atoms. In the seventh O2- site, O2- is bonded in a 3-coordinate geometry to one Na1+, one Ga3+, and one Si4+ atom.
DOI: 10.17188/1285429
title: Materials Data on CaFe2Sb2(PO4)6 by Materials Project

description: CaFe2Sb2(PO4)6 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. Ca2+ is bonded in a distorted hexagonal planar geometry to six equivalent O2- atoms. All Ca–O bond lengths are 2.44 Å. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent PO4 tetrahedra. There are three shorter (1.96 Å) and three longer (2.08 Å) Fe–O bond lengths. Sb5+ is bonded to six O2- atoms to form SbO6 octahedra that share corners with six equivalent PO4 tetrahedra. There is three shorter (1.98 Å) and three longer (1.99 Å) Sb–O bond length. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent FeO6 octahedra and corners with two equivalent SbO6 octahedra. The corner-sharing octahedra tilt angles range from 28–48°. There are a spread of P–O bond distances ranging from 1.51–1.59 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Sb5+ and one P5+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Sb5+ and one P5+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Fe3+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Ca2+, one Fe3+, and one P5+ atom.