cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1279352
title: Materials Data on KH4F5 by Materials Project

description: KH4F5 crystallizes in the tetragonal I4_1/a space group. The structure is three-dimensional. K1+ is bonded to eight equivalent F1- atoms to form distorted edge-sharing KF8 hexagonal bipyramids. There are four shorter (2.70 Å) and four longer (3.12 Å) K–F bond lengths. H1+ is bonded in a linear geometry to two F1- atoms. There is one shorter (0.98 Å) and one longer (1.49 Å) H–F bond length. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a rectangular see-saw-like geometry to four equivalent H1+ atoms. In the second F1- site, F1- is bonded in a distorted single-bond geometry to two equivalent K1+ and one H1+ atom.
DOI: 10.17188/1279354
title: Materials Data on Li5B4 by Materials Project

description: Li5B4 is beta Plutonium-derived structured and crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are four inequivalent Li sites. In the first Li site, Li is bonded in a 4-coordinate geometry to two equivalent Li and six B atoms. There are one shorter (2.27 Å) and one longer (2.35 Å) Li–Li bond lengths. There are a spread of Li–B bond distances ranging from 2.20–2.45 Å. In the second Li site, Li is bonded in a 5-coordinate geometry to two equivalent Li and seven B atoms. There are one shorter (2.37 Å) and one longer (2.41 Å) Li–Li bond lengths. There are a spread of Li–B bond distances ranging from 2.37–2.81 Å. In the third Li site, Li is bonded to eight Li and four equivalent B atoms to form a mixture of face and corner-sharing LiLi8B4 cuboctahedra. There are one shorter (2.30 Å) and one longer (2.41 Å) Li–Li bond lengths. There are two shorter (2.72 Å) and two longer (2.80 Å) Li–B bond lengths. In the fourth Li site, Li is bonded in a 4-coordinate geometry to two equivalent Li and six B atoms. There are a spread of Li–B bond distances ranging from 2.17–2.47 Å. There are three inequivalent B sites. In the first B site, B is bonded in a 8-coordinate geometry to four Li and four B atoms. There are a spread of B–B bond distances ranging from 1.72–1.97 Å. In the second B site, B is bonded in a 12-coordinate geometry to ten Li and two B atoms. The B–B bond length is 1.73 Å. In the third B site, B is bonded in a 10-coordinate geometry to six Li and four B atoms.
DOI: 10.17188/1279355
title: Materials Data on LiNiO2 by Materials Project

description: LiNiO2 crystallizes in the hexagonal P6/mmm space group. The structure is one-dimensional and consists of one LiNiO2 ribbon oriented in the (0, 0, 1) direction. Li1+ is bonded in a linear geometry to two equivalent O2- atoms. Both Li–O bond lengths are 1.77 Å. Ni3+ is bonded in a linear geometry to two equivalent O2- atoms. Both Ni–O bond lengths are 1.69 Å. O2- is bonded in a linear geometry to one Li1+ and one Ni3+ atom.
DOI: 10.17188/1279356
title: Materials Data on CaUO4 by Materials Project

description: CaUO4 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Ca2+ is bonded in a distorted body-centered cubic geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.17–2.55 Å. U6+ is bonded in a distorted square co-planar geometry to eight O2- atoms. There are a spread of U–O bond distances ranging from 1.97–2.46 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to three equivalent Ca2+ and one U6+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to one Ca2+ and three equivalent U6+ atoms.
DOI: 10.17188/1279357
title: Materials Data on Li2PWO4F (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: 10.17188/1279358
title: Materials Data on LaSn3 by Materials Project

description: LaSn3 is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. La is bonded to twelve equivalent Sn atoms to form a mixture of corner and face-sharing LaSn12 cuboctahedra. All La–Sn bond lengths are 3.41 Å. Sn is bonded in a distorted square co-planar geometry to four equivalent La atoms.
DOI: 10.17188/1279359
title: Materials Data on RbUN3O11 by Materials Project

description: RbUN3O11 crystallizes in the trigonal R-3c space group. The structure is three-dimensional. Rb1+ is bonded in a 2-coordinate geometry to fourteen O2- atoms. There are a spread of Rb–O bond distances ranging from 3.01–3.50 Å. U6+ is bonded in a distorted linear geometry to two equivalent O2- atoms. Both U–O bond lengths are 1.80 Å. N5+ is bonded in a trigonal planar geometry to three O2- atoms. There is one shorter (1.23 Å) and two longer (1.29 Å) N–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one Rb1+ and one N5+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to two equivalent Rb1+ and one N5+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one Rb1+ and one U6+ atom.
DOI: 10.17188/1279360
title: Materials Data on Sb2Pb2O7 by Materials Project

description: Pb2Sb2O7 crystallizes in the orthorhombic Ima2 space group. The structure is three-dimensional. there are two inequivalent Pb2+ sites. In the first Pb2+ site, Pb2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Pb–O bond distances ranging from 2.45–2.73 Å. In the second Pb2+ site, Pb2+ is bonded to eight O2- atoms to form distorted PbO8 hexagonal bipyramids that share corners with two equivalent PbO8 hexagonal bipyramids, corners with two equivalent SbO6 octahedra, and edges with six SbO6 octahedra. The corner-sharing octahedral tilt angles are 52°. There are a spread of Pb–O bond distances ranging from 2.47–2.93 Å. There are two inequivalent Sb5+ sites. In the first Sb5+ site, Sb5+ is bonded to six O2- atoms to form SbO6 octahedra that share corners with six SbO6 octahedra and edges with four equivalent PbO8 hexagonal bipyramids. The corner-sharing octahedra tilt angles range from 41–43°. There are a spread of Sb–O bond distances ranging from 2.01–2.04 Å. In the second Sb5+ site, Sb5+ is bonded to six O2- atoms to form SbO6 octahedra that share corners with two equivalent PbO8 hexagonal bipyramids, corners with four equivalent SbO6 octahedra, and edges with two equivalent PbO8 hexagonal bipyramids. The corner-sharing octahedral tilt angles are 41°. There are a spread of Sb–O bond distances ranging from 1.96–2.08 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two Pb2+ and two Sb5+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to three Pb2+ and one Sb5+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Pb2+ and two Sb5+ atoms. In the fourth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent Pb2+ and two equivalent Sb5+ atoms.
DOI: 10.17188/1279361
title: Materials Data on Na2Y2B2O7 by Materials Project

description: Na2Y2B2O7 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a 5-coordinate geometry to seven O2- atoms. There are a spread of Na–O bond distances ranging from 2.36–3.01 Å. In the second Na1+ site, Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.34–2.62 Å. There are two inequivalent Y3+ sites. In the first Y3+ site, Y3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Y–O bond distances ranging from 2.27–2.52 Å. In the second Y3+ site, Y3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Y–O bond distances ranging from 2.27–2.65 Å. There are two inequivalent B3+ sites. In the first B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.36–1.40 Å. In the second B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There is two shorter (1.38 Å) and one longer (1.42 Å) B–O bond length. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded to four Y3+ atoms to form a mixture of corner and edge-sharing OY4 tetrahedra. In the second O2- site, O2- is bonded in a distorted single-bond geometry to four Na1+, one Y3+, and one B3+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to three Y3+ and one B3+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to three Y3+ and one B3+ atom. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to four Na1+, one Y3+, and one B3+ atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to four Na1+, one Y3+, and one B3+ atom. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to one Na1+, three Y3+, and one B3+ atom.
DOI: 10.17188/1279362
title: Materials Data on GdBO3 (SG:194) 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: 10.17188/1279363
title: Materials Data on H8W3Se(NO6)2 (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: 10.17188/1279364
title: Materials Data on NaTeH6O6F by Materials Project

description: NaH6TeO6F crystallizes in the trigonal R3 space group. The structure is three-dimensional. Na1+ is bonded in a 7-coordinate geometry to six O2- and one F1- atom. There are three shorter (2.39 Å) and three longer (2.66 Å) Na–O bond lengths. The Na–F bond length is 2.42 Å. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 1.00 Å. In the second H1+ site, H1+ is bonded in a linear geometry to one O2- and one F1- atom. The H–O bond length is 1.03 Å. The H–F bond length is 1.51 Å. Te6+ is bonded in an octahedral geometry to six O2- atoms. There is three shorter (1.95 Å) and three longer (1.96 Å) Te–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one Na1+, one H1+, and one Te6+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one Na1+, one H1+, and one Te6+ atom. F1- is bonded in a 4-coordinate geometry to one Na1+ and three equivalent H1+ atoms.
DOI: 10.17188/1279365
title: Materials Data on Li2TiSiO5 by Materials Project

description: Li2TiSiO5 crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with two equivalent LiO6 octahedra, corners with four equivalent SiO4 tetrahedra, and edges with four equivalent LiO6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are four shorter (2.09 Å) and two longer (2.48 Å) Li–O bond lengths. Ti4+ is bonded in a 5-coordinate geometry to five O2- atoms. There is one shorter (1.72 Å) and four longer (1.99 Å) Ti–O bond length. Si4+ is bonded to four equivalent O2- atoms to form SiO4 tetrahedra that share corners with eight equivalent LiO6 octahedra. The corner-sharing octahedral tilt angles are 62°. All Si–O bond lengths are 1.65 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to four equivalent Li1+ and one Ti4+ atom. In the second O2- site, O2- is bonded to two equivalent Li1+, one Ti4+, and one Si4+ atom to form a mixture of distorted edge and corner-sharing OLi2TiSi trigonal pyramids.
DOI: 10.17188/1279366
title: Materials Data on NaIn(SiO3)2 by Materials Project

description: NaInSi2O6 is Esseneite structured and crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Na1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Na–O bond distances ranging from 2.39–2.98 Å. In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with six equivalent SiO4 tetrahedra and edges with two equivalent InO6 octahedra. There are a spread of In–O bond distances ranging from 2.11–2.26 Å. Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share corners with three equivalent InO6 octahedra and corners with two equivalent SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 36–59°. There are a spread of Si–O bond distances ranging from 1.61–1.67 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted T-shaped geometry to one Na1+, one In3+, and one Si4+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Na1+ and two equivalent Si4+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one Na1+, two equivalent In3+, and one Si4+ atom.
DOI: 10.17188/1279367
title: Materials Data on Cu3As4 by Materials Project

description: Cu3As4 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Cu3As4 ribbons oriented in the (1, 0, 0) direction. there are two inequivalent Cu+1.33+ sites. In the first Cu+1.33+ site, Cu+1.33+ is bonded in a 4-coordinate geometry to four As1- atoms. There are two shorter (2.44 Å) and two longer (2.51 Å) Cu–As bond lengths. In the second Cu+1.33+ site, Cu+1.33+ is bonded in a 6-coordinate geometry to six As1- atoms. There are two shorter (2.45 Å) and four longer (2.52 Å) Cu–As bond lengths. There are three inequivalent As1- sites. In the first As1- site, As1- is bonded in a 4-coordinate geometry to four Cu+1.33+ atoms. In the second As1- site, As1- is bonded in a 4-coordinate geometry to four equivalent Cu+1.33+ atoms. In the third As1- site, As1- is bonded in a distorted L-shaped geometry to two equivalent Cu+1.33+ atoms.
DOI: 10.17188/1279368
title: Materials Data on Mn2H2SO6 (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: 10.17188/1279369
title: Materials Data on LiCoPCO7 (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: 10.17188/1279370
title: Materials Data on Rb2CoH12(SeO7)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: 10.17188/1279371
title: Materials Data on VCuHPbO5 (SG:62) by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1279372
title: Materials Data on B9C by Materials Project

description: B9C crystallizes in the triclinic P1 space group. The structure is zero-dimensional and consists of ten boron molecules, one tetraborylmethane molecule, and one B4C cluster. In the B4C cluster, there are four inequivalent B+0.33+ sites. In the first B+0.33+ site, B+0.33+ is bonded in a single-bond geometry to one C3- atom. The B–C bond length is 1.85 Å. In the second B+0.33+ site, B+0.33+ is bonded in a single-bond geometry to one C3- atom. The B–C bond length is 1.58 Å. In the third B+0.33+ site, B+0.33+ is bonded in a single-bond geometry to one C3- atom. The B–C bond length is 1.52 Å. In the fourth B+0.33+ site, B+0.33+ is bonded in a single-bond geometry to one C3- atom. The B–C bond length is 1.59 Å. C3- is bonded in a 4-coordinate geometry to four B+0.33+ atoms.
DOI: 10.17188/1279373
title: Materials Data on Cs2NiH12(SO7)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: 10.17188/1279374
title: Materials Data on Na3In(PO4)2 by Materials Project

description: Na3In(PO4)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Na–O bond distances ranging from 2.35–2.87 Å. In the second Na1+ site, Na1+ is bonded to six O2- atoms to form distorted NaO6 octahedra that share corners with six PO4 tetrahedra and edges with two equivalent InO6 octahedra. There are a spread of Na–O bond distances ranging from 2.25–2.83 Å. In the third Na1+ site, Na1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Na–O bond distances ranging from 2.37–3.01 Å. In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with six PO4 tetrahedra and edges with two equivalent NaO6 octahedra. There are a spread of In–O bond distances ranging from 2.18–2.22 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with three equivalent NaO6 octahedra and corners with three equivalent InO6 octahedra. The corner-sharing octahedra tilt angles range from 36–56°. There are a spread of P–O bond distances ranging from 1.52–1.58 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with three equivalent NaO6 octahedra and corners with three equivalent InO6 octahedra. The corner-sharing octahedra tilt angles range from 43–66°. There are a spread of P–O bond distances ranging from 1.52–1.58 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to three Na1+, one In3+, and one P5+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to three Na1+, one In3+, and one P5+ atom. In the third O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Na1+, one In3+, and one P5+ atom. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to three Na1+, one In3+, and one P5+ atom. In the fifth O2- site, O2- is bonded in a 1-coordinate geometry to three Na1+, one In3+, and one P5+ atom. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to three Na1+ and one P5+ atom. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to four Na1+ and one P5+ atom. In the eighth O2- site, O2- is bonded in a 1-coordinate geometry to one Na1+, one In3+, and one P5+ atom.
DOI: 10.17188/1279375
title: Materials Data on Rb5Si2NiO8 (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: 10.17188/1279376
title: Materials Data on K23Na8(CdIn4)12 by Materials Project

description: Na8K23Cd12In48 is Bergman Structure: Mg32(Al,Zn)49 Bergman-derived structured and crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. there are four inequivalent K sites. In the first K site, K is bonded in a 12-coordinate geometry to four K, one Na, two equivalent Cd, and nine In atoms. There are a spread of K–K bond distances ranging from 3.93–4.18 Å. The K–Na bond length is 3.89 Å. Both K–Cd bond lengths are 3.91 Å. There are a spread of K–In bond distances ranging from 3.66–3.90 Å. In the second K site, K is bonded in a 10-coordinate geometry to four equivalent K and ten In atoms. There are a spread of K–In bond distances ranging from 3.78–4.03 Å. In the third K site, K is bonded in a 12-coordinate geometry to three equivalent K and twelve In atoms. There are three shorter (3.58 Å) and nine longer (3.71 Å) K–In bond lengths. In the fourth K site, K is bonded in a 2-coordinate geometry to eight Na atoms. There are two shorter (3.70 Å) and six longer (4.22 Å) K–Na bond lengths. There are two inequivalent Na sites. In the first Na site, Na is bonded in a 10-coordinate geometry to three K, four equivalent Cd, and six In atoms. All Na–Cd bond lengths are 3.46 Å. There are two shorter (3.63 Å) and four longer (3.66 Å) Na–In bond lengths. In the second Na site, Na is bonded in a 6-coordinate geometry to one K, one Na, six equivalent Cd, and six equivalent In atoms. The Na–Na bond length is 3.29 Å. All Na–Cd bond lengths are 3.44 Å. All Na–In bond lengths are 3.64 Å. Cd is bonded in a 12-coordinate geometry to two equivalent K, three Na, and three In atoms. There are one shorter (3.11 Å) and two longer (3.13 Å) Cd–In bond lengths. There are five inequivalent In sites. In the first In site, In is bonded in a 11-coordinate geometry to three K, two equivalent Na, one Cd, and five In atoms. There are a spread of In–In bond distances ranging from 3.10–3.21 Å. In the second In site, In is bonded in a distorted q6 geometry to four K, one Na, and six In atoms. There are a spread of In–In bond distances ranging from 3.04–3.21 Å. In the third In site, In is bonded in a 11-coordinate geometry to five K and six In atoms. There are one shorter (3.07 Å) and one longer (3.16 Å) In–In bond lengths. In the fourth In site, In is bonded to eight K and four In atoms to form a mixture of edge and face-sharing InK8In4 cuboctahedra. Both In–In bond lengths are 3.19 Å. In the fifth In site, In is bonded in a distorted q6 geometry to four K, two equivalent Na, four equivalent Cd, and two equivalent In atoms. Both In–In bond lengths are 3.24 Å.
DOI: 10.17188/1279377
title: Materials Data on Mn3AgAs3(HO6)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: 10.17188/1279378
title: Materials Data on Cs2CrH2Cl5O (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: 10.17188/1279379
title: Materials Data on CoSiO4 (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