cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1652162
title: Materials Data on Ce6Mg23Sn by Materials Project

description: Mg23Ce6Sn crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are four inequivalent Mg sites. In the first Mg site, Mg is bonded in a 10-coordinate geometry to seven Mg and three equivalent Ce atoms. There are a spread of Mg–Mg bond distances ranging from 3.05–3.19 Å. All Mg–Ce bond lengths are 3.41 Å. In the second Mg site, Mg is bonded to eight Mg and four equivalent Ce atoms to form MgCe4Mg8 cuboctahedra that share corners with four equivalent MgCe4Mg8 cuboctahedra, edges with two equivalent SnCe6 octahedra, and faces with eight equivalent MgCe4Mg8 cuboctahedra. All Mg–Mg bond lengths are 2.96 Å. All Mg–Ce bond lengths are 3.65 Å. In the third Mg site, Mg is bonded in a body-centered cubic geometry to eight equivalent Mg atoms. In the fourth Mg site, Mg is bonded in a 12-coordinate geometry to nine Mg and three equivalent Ce atoms. All Mg–Mg bond lengths are 3.31 Å. All Mg–Ce bond lengths are 3.54 Å. Ce is bonded in a distorted single-bond geometry to twelve Mg and one Sn atom. The Ce–Sn bond length is 3.15 Å. Sn is bonded to six equivalent Ce atoms to form SnCe6 octahedra that share edges with twelve equivalent MgCe4Mg8 cuboctahedra.
DOI: 10.17188/1652163
title: Materials Data on Cd(PO5)2 by Materials Project

description: Cd(PO3)2(O2)2 crystallizes in the trigonal P-3 space group. The structure is three-dimensional and consists of six hydrogen peroxide molecules and one Cd(PO3)2 framework. In the Cd(PO3)2 framework, Cd is bonded in a square co-planar geometry to four O atoms. There are two shorter (2.21 Å) and two longer (2.23 Å) Cd–O bond lengths. P is bonded to four O atoms to form corner-sharing PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.50–1.63 Å. There are three inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to two equivalent P atoms. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one Cd and one P atom. In the third O site, O is bonded in a 2-coordinate geometry to one Cd and one P atom.
DOI: 10.17188/1652164
title: Materials Data on V4O7F5 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: 10.17188/1652165
title: Materials Data on Cs2NdAgCl6 by Materials Project

description: Cs2NdAgCl6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs1+ is bonded to twelve equivalent Cl1- atoms to form CsCl12 cuboctahedra that share corners with twelve equivalent CsCl12 cuboctahedra, faces with six equivalent CsCl12 cuboctahedra, faces with four equivalent NdCl6 octahedra, and faces with four equivalent AgCl6 octahedra. All Cs–Cl bond lengths are 3.90 Å. Nd3+ is bonded to six equivalent Cl1- atoms to form NdCl6 octahedra that share corners with six equivalent AgCl6 octahedra and faces with eight equivalent CsCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Nd–Cl bond lengths are 2.74 Å. Ag1+ is bonded to six equivalent Cl1- atoms to form AgCl6 octahedra that share corners with six equivalent NdCl6 octahedra and faces with eight equivalent CsCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ag–Cl bond lengths are 2.78 Å. Cl1- is bonded in a distorted linear geometry to four equivalent Cs1+, one Nd3+, and one Ag1+ atom.
DOI: 10.17188/1652166
title: Materials Data on PHPbO4 by Materials Project

description: PbHPO4 crystallizes in the monoclinic P2/c space group. The structure is three-dimensional. Pb2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Pb–O bond distances ranging from 2.40–2.93 Å. P5+ is bonded in a tetrahedral geometry to four O2- atoms. There is two shorter (1.55 Å) and two longer (1.56 Å) P–O bond length. H1+ is bonded in a linear geometry to two equivalent O2- atoms. Both H–O bond lengths are 1.21 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Pb2+ and one P5+ atom. In the second O2- site, O2- is bonded in a bent 120 degrees geometry to one Pb2+, one P5+, and one H1+ atom.
DOI: 10.17188/1652167
title: Materials Data on Pr4CdIr by Materials Project

description: Pr4IrCd crystallizes in the cubic F-43m space group. The structure is three-dimensional. there are three inequivalent Pr sites. In the first Pr site, Pr is bonded in a 3-coordinate geometry to three equivalent Ir and three equivalent Cd atoms. All Pr–Ir bond lengths are 2.93 Å. All Pr–Cd bond lengths are 3.60 Å. In the second Pr site, Pr is bonded in a distorted bent 150 degrees geometry to two equivalent Ir and two equivalent Cd atoms. Both Pr–Ir bond lengths are 2.92 Å. Both Pr–Cd bond lengths are 3.64 Å. In the third Pr site, Pr is bonded in a 4-coordinate geometry to two equivalent Ir and two equivalent Cd atoms. Both Pr–Ir bond lengths are 3.61 Å. Both Pr–Cd bond lengths are 3.43 Å. Ir is bonded in a 6-coordinate geometry to nine Pr atoms. Cd is bonded to nine Pr and three equivalent Cd atoms to form a mixture of distorted face and corner-sharing CdPr9Cd3 cuboctahedra. All Cd–Cd bond lengths are 3.19 Å.
DOI: 10.17188/1652168
title: Materials Data on Ho5BiPt2 by Materials Project

description: Ho5Pt2Bi crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. there are two inequivalent Ho sites. In the first Ho site, Ho is bonded to four equivalent Pt and two equivalent Bi atoms to form distorted corner-sharing HoBi2Pt4 octahedra. The corner-sharing octahedra tilt angles range from 0–48°. All Ho–Pt bond lengths are 3.01 Å. Both Ho–Bi bond lengths are 3.47 Å. In the second Ho site, Ho is bonded in a 5-coordinate geometry to three equivalent Pt and two equivalent Bi atoms. There are one shorter (2.93 Å) and two longer (2.97 Å) Ho–Pt bond lengths. Both Ho–Bi bond lengths are 3.33 Å. Pt is bonded in a 8-coordinate geometry to eight Ho atoms. Bi is bonded in a 10-coordinate geometry to ten Ho atoms.
DOI: 10.17188/1652169
title: Materials Data on K2GaAuF6 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: 10.17188/1652170
title: Materials Data on Na2UI6 by Materials Project

description: Na2UI6 is beta Vanadium nitride-derived structured and crystallizes in the trigonal R3 space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded to six I1- atoms to form NaI6 octahedra that share corners with three equivalent NaI6 octahedra, corners with six equivalent UI6 octahedra, and a faceface with one NaI6 octahedra. The corner-sharing octahedra tilt angles range from 43–58°. There are three shorter (3.25 Å) and three longer (3.28 Å) Na–I bond lengths. In the second Na1+ site, Na1+ is bonded to six I1- atoms to form NaI6 octahedra that share corners with three equivalent NaI6 octahedra, edges with three equivalent UI6 octahedra, and a faceface with one NaI6 octahedra. The corner-sharing octahedral tilt angles are 58°. There are three shorter (3.18 Å) and three longer (3.36 Å) Na–I bond lengths. U4+ is bonded to six I1- atoms to form UI6 octahedra that share corners with six equivalent NaI6 octahedra and edges with three equivalent NaI6 octahedra. The corner-sharing octahedral tilt angles are 43°. There are three shorter (3.01 Å) and three longer (3.03 Å) U–I bond lengths. There are two inequivalent I1- sites. In the first I1- site, I1- is bonded in a distorted trigonal planar geometry to two Na1+ and one U4+ atom. In the second I1- site, I1- is bonded in a distorted T-shaped geometry to two Na1+ and one U4+ atom.
DOI: 10.17188/1652171
title: Materials Data on Ta6Br12ClO15 by Materials Project

description: (TaO)6(O2)3ClO3(Br)12 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of twenty-four hydrobromic acid molecules, six hydrogen peroxide molecules, twelve oxotantalum molecules, and two ClO3 clusters. In each ClO3 cluster, there are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a water-like geometry to one O2- and one Cl1- atom. The O–O bond length is 1.31 Å. The O–Cl bond length is 2.47 Å. In the second O2- site, O2- is bonded in a single-bond geometry to one O2- atom. The O–O bond length is 1.33 Å. In the third O2- site, O2- is bonded in a bent 120 degrees geometry to two O2- atoms. Cl1- is bonded in a distorted single-bond geometry to one O2- atom.
DOI: 10.17188/1652172
title: Materials Data on Li5Mn3O8 by Materials Project

description: Li5Mn3O8 is Caswellsilverite-like structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are four 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 MnO6 octahedra, edges with four MnO6 octahedra, and edges with eight LiO6 octahedra. The corner-sharing octahedra tilt angles range from 5–8°. There are a spread of Li–O bond distances ranging from 2.14–2.31 Å. In the second Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with six LiO6 octahedra, and edges with six MnO6 octahedra. The corner-sharing octahedra tilt angles range from 7–12°. There are four shorter (2.07 Å) and two longer (2.12 Å) Li–O bond lengths. In the third Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent MnO6 octahedra, edges with four equivalent MnO6 octahedra, and edges with eight LiO6 octahedra. The corner-sharing octahedra tilt angles range from 7–10°. There are two shorter (2.03 Å) and four longer (2.16 Å) Li–O bond lengths. In the fourth Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with six LiO6 octahedra, and edges with six MnO6 octahedra. The corner-sharing octahedra tilt angles range from 7–12°. There are four shorter (2.05 Å) and two longer (2.14 Å) Li–O bond lengths. There are two inequivalent Mn+3.67+ sites. In the first Mn+3.67+ site, Mn+3.67+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with four equivalent MnO6 octahedra, and edges with eight LiO6 octahedra. The corner-sharing octahedra tilt angles range from 7–10°. There are four shorter (1.95 Å) and two longer (2.23 Å) Mn–O bond lengths. In the second Mn+3.67+ site, Mn+3.67+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with four MnO6 octahedra, and edges with eight LiO6 octahedra. The corner-sharing octahedra tilt angles range from 5–8°. There is four shorter (1.95 Å) and two longer (1.96 Å) Mn–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four Li1+ and two Mn+3.67+ atoms to form a mixture of corner and edge-sharing OLi4Mn2 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second O2- site, O2- is bonded to four Li1+ and two equivalent Mn+3.67+ atoms to form a mixture of corner and edge-sharing OLi4Mn2 octahedra. The corner-sharing octahedral tilt angles are 0°. In the third O2- site, O2- is bonded to three Li1+ and three Mn+3.67+ atoms to form OLi3Mn3 octahedra that share corners with six equivalent OLi3Mn3 octahedra and edges with twelve OLi4Mn2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1652173
title: Materials Data on LiFeSiO4 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: 10.17188/1652174
title: Materials Data on BPt by Materials Project

description: PtB is Caswellsilverite-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pt is bonded to six equivalent B atoms to form a mixture of edge, face, and corner-sharing PtB6 octahedra. The corner-sharing octahedral tilt angles are 48°. All Pt–B bond lengths are 2.28 Å. B is bonded to six equivalent Pt atoms to form a mixture of distorted edge and corner-sharing BPt6 pentagonal pyramids.
DOI: 10.17188/1652175
title: Materials Data on Cs2NaNdBr6 by Materials Project

description: Cs2NaNdBr6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs1+ is bonded to twelve equivalent Br1- atoms to form CsBr12 cuboctahedra that share corners with twelve equivalent CsBr12 cuboctahedra, faces with six equivalent CsBr12 cuboctahedra, faces with four equivalent NaBr6 octahedra, and faces with four equivalent NdBr6 octahedra. All Cs–Br bond lengths are 4.13 Å. Na1+ is bonded to six equivalent Br1- atoms to form NaBr6 octahedra that share corners with six equivalent NdBr6 octahedra and faces with eight equivalent CsBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Br bond lengths are 2.95 Å. Nd3+ is bonded to six equivalent Br1- atoms to form NdBr6 octahedra that share corners with six equivalent NaBr6 octahedra and faces with eight equivalent CsBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Nd–Br bond lengths are 2.89 Å. Br1- is bonded in a distorted linear geometry to four equivalent Cs1+, one Na1+, and one Nd3+ atom.
DOI: 10.17188/1652176
title: Materials Data on BaMgAl3P2(HO7)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: 10.17188/1652177
title: Materials Data on Li5Fe11O16 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: 10.17188/1652178
title: Materials Data on Sm2CuGe6 by Materials Project

description: Sm2CuGe6 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Sm sites. In the first Sm site, Sm is bonded in a 10-coordinate geometry to ten Ge atoms. There are eight shorter (3.06 Å) and two longer (3.23 Å) Sm–Ge bond lengths. In the second Sm site, Sm is bonded in a 4-coordinate geometry to four equivalent Cu and ten Ge atoms. All Sm–Cu bond lengths are 3.16 Å. There are a spread of Sm–Ge bond distances ranging from 3.13–3.38 Å. Cu is bonded in a 9-coordinate geometry to four equivalent Sm and five Ge atoms. There are a spread of Cu–Ge bond distances ranging from 2.35–2.44 Å. There are six inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to two equivalent Sm, two equivalent Cu, and five Ge atoms. There are one shorter (2.49 Å) and four longer (2.92 Å) Ge–Ge bond lengths. In the second Ge site, Ge is bonded in a 7-coordinate geometry to two equivalent Sm and five Ge atoms. All Ge–Ge bond lengths are 2.92 Å. In the third Ge site, Ge is bonded in a 2-coordinate geometry to two equivalent Sm, two equivalent Cu, and five Ge atoms. The Ge–Ge bond length is 2.51 Å. In the fourth Ge site, Ge is bonded in a 7-coordinate geometry to two equivalent Sm and five Ge atoms. In the fifth Ge site, Ge is bonded in a 1-coordinate geometry to six Sm, one Cu, and two equivalent Ge atoms. Both Ge–Ge bond lengths are 2.56 Å. In the sixth Ge site, Ge is bonded in a 8-coordinate geometry to six Sm and two equivalent Ge atoms.
DOI: 10.17188/1652180
title: Materials Data on In3Pb3N5 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: 10.17188/1652181
title: Materials Data on Li4Nb3V3(SnO8)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: 10.17188/1652182
title: Materials Data on RbYb(WO4)2 by Materials Project

description: RbYb(WO4)2 crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. Rb1+ is bonded to twelve O2- atoms to form RbO12 cuboctahedra that share edges with six equivalent RbO12 cuboctahedra, edges with six equivalent WO4 tetrahedra, and faces with two equivalent YbO6 octahedra. There are six shorter (3.30 Å) and six longer (3.59 Å) Rb–O bond lengths. Yb3+ is bonded to six equivalent O2- atoms to form YbO6 octahedra that share corners with six equivalent WO4 tetrahedra and faces with two equivalent RbO12 cuboctahedra. All Yb–O bond lengths are 2.29 Å. W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with three equivalent YbO6 octahedra and edges with three equivalent RbO12 cuboctahedra. The corner-sharing octahedral tilt angles are 18°. There is one shorter (1.80 Å) and three longer (1.82 Å) W–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one Rb1+, one Yb3+, and one W6+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to three equivalent Rb1+ and one W6+ atom.
DOI: 10.17188/1652183
title: Materials Data on CoH20C22(N5O3)2 by Materials Project

description: (C)4CoC6H8(N4O3)2(CH)8(C2NH2)2 crystallizes in the monoclinic P2/c space group. The structure is zero-dimensional and consists of eight medicinal charcoal molecules, sixteen medicinal charcoal molecules, four n-methyl methanimine molecules, and two CoC6H8(N4O3)2 clusters. In each CoC6H8(N4O3)2 cluster, Co2+ is bonded in an octahedral geometry to four N3- and two equivalent O2- atoms. There are a spread of Co–N bond distances ranging from 2.09–2.23 Å. Both Co–O bond lengths are 2.14 Å. There are three inequivalent C+0.91+ sites. In the first C+0.91+ site, C+0.91+ is bonded in a bent 120 degrees geometry to one N3- and one H1+ atom. The C–N bond length is 1.35 Å. The C–H bond length is 1.09 Å. In the second C+0.91+ site, C+0.91+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.18 Å) and one longer (1.31 Å) C–N bond length. In the third C+0.91+ site, C+0.91+ is bonded in a bent 120 degrees geometry to one N3- and one H1+ atom. The C–N bond length is 1.35 Å. The C–H bond length is 1.09 Å. There are five inequivalent N3- sites. In the first N3- site, N3- is bonded in a trigonal planar geometry to one Co2+ and two equivalent C+0.91+ atoms. In the second N3- site, N3- is bonded in a trigonal planar geometry to one Co2+ and two equivalent C+0.91+ atoms. In the third N3- site, N3- is bonded in a distorted bent 150 degrees geometry to one Co2+ and one C+0.91+ atom. In the fourth N3- site, N3- is bonded in a distorted trigonal planar geometry to one N3- and two O2- atoms. The N–N bond length is 1.38 Å. Both N–O bond lengths are 1.25 Å. In the fifth N3- site, N3- is bonded in a distorted bent 120 degrees geometry to one C+0.91+ and one N3- atom. There are four 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 1.01 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.98 Å. In the third H1+ site, H1+ is bonded in a single-bond geometry to one C+0.91+ atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one C+0.91+ atom. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one N3- atom. In the second O2- site, O2- is bonded in a single-bond geometry to one N3- atom. In the third O2- site, O2- is bonded in a distorted water-like geometry to one Co2+ and two H1+ atoms.
DOI: 10.17188/1652185
title: Materials Data on GaAgSnSe4 by Materials Project

description: AgGaSnSe4 crystallizes in the tetragonal I-4 space group. The structure is three-dimensional. Ag1+ is bonded to four equivalent Se2- atoms to form AgSe4 tetrahedra that share corners with four equivalent GaSe4 tetrahedra and corners with four equivalent SnSe4 tetrahedra. All Ag–Se bond lengths are 2.68 Å. Ga3+ is bonded to four equivalent Se2- atoms to form GaSe4 tetrahedra that share corners with four equivalent AgSe4 tetrahedra and corners with four equivalent SnSe4 tetrahedra. All Ga–Se bond lengths are 2.45 Å. Sn4+ is bonded to four equivalent Se2- atoms to form SnSe4 tetrahedra that share corners with four equivalent AgSe4 tetrahedra and corners with four equivalent GaSe4 tetrahedra. All Sn–Se bond lengths are 2.59 Å. Se2- is bonded in a trigonal non-coplanar geometry to one Ag1+, one Ga3+, and one Sn4+ atom.