cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1684601
title: Materials Data on ScNiBO4 by Materials Project

description: ScNiBO4 crystallizes in the orthorhombic Pmc2_1 space group. The structure is three-dimensional. there are two inequivalent Sc3+ sites. In the first Sc3+ site, Sc3+ is bonded to six O2- atoms to form ScO6 octahedra that share a cornercorner with one ScO6 octahedra, corners with two equivalent NiO6 octahedra, edges with two equivalent ScO6 octahedra, and edges with four NiO6 octahedra. The corner-sharing octahedra tilt angles range from 52–65°. There are a spread of Sc–O bond distances ranging from 2.01–2.28 Å. In the second Sc3+ site, Sc3+ is bonded to six O2- atoms to form ScO6 octahedra that share a cornercorner with one ScO6 octahedra, corners with two equivalent NiO6 octahedra, edges with two equivalent ScO6 octahedra, and edges with two equivalent NiO6 octahedra. The corner-sharing octahedra tilt angles range from 52–62°. There are a spread of Sc–O bond distances ranging from 1.99–2.22 Å. There are two inequivalent Ni2+ sites. In the first Ni2+ site, Ni2+ is bonded to six O2- atoms to form NiO6 octahedra that share a cornercorner with one NiO6 octahedra, corners with two equivalent ScO6 octahedra, edges with two equivalent NiO6 octahedra, and edges with four ScO6 octahedra. The corner-sharing octahedra tilt angles range from 57–62°. There are a spread of Ni–O bond distances ranging from 2.04–2.18 Å. In the second Ni2+ site, Ni2+ is bonded to six O2- atoms to form NiO6 octahedra that share a cornercorner with one NiO6 octahedra, corners with two equivalent ScO6 octahedra, edges with two equivalent ScO6 octahedra, and edges with two equivalent NiO6 octahedra. The corner-sharing octahedra tilt angles range from 57–65°. There are a spread of Ni–O bond distances ranging from 1.99–2.19 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 1.37–1.40 Å. In the second 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 1.37–1.41 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two equivalent Sc3+, one Ni2+, and one B3+ atom. In the second O2- site, O2- is bonded to one Sc3+, two equivalent Ni2+, and one B3+ atom to form distorted corner-sharing OScNi2B tetrahedra. In the third O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Sc3+, one Ni2+, and one B3+ atom. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to one Sc3+, two equivalent Ni2+, and one B3+ atom. In the fifth O2- site, O2- is bonded to two equivalent Sc3+ and two Ni2+ atoms to form corner-sharing OSc2Ni2 tetrahedra. In the sixth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Sc3+ and two equivalent Ni2+ atoms. In the seventh O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Sc3+ and one B3+ atom. In the eighth O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Ni2+ and one B3+ atom.
DOI: 10.17188/1684602
title: Materials Data on YCoC by Materials Project

description: YCoC crystallizes in the orthorhombic Pmmm space group. The structure is three-dimensional. Y3+ is bonded in a square co-planar geometry to four equivalent C4- atoms. All Y–C bond lengths are 2.52 Å. Co1+ is bonded in a linear geometry to two equivalent C4- atoms. Both Co–C bond lengths are 1.81 Å. C4- is bonded to four equivalent Y3+ and two equivalent Co1+ atoms to form a mixture of edge and corner-sharing CY4Co2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1684603
title: Materials Data on Cr2PO5 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: 10.17188/1684604
title: Materials Data on LiV2(SiO4)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: 10.17188/1684605
title: Materials Data on Tm4Ni2C5 by Materials Project

description: Tm4Ni2C5 crystallizes in the orthorhombic Pmm2 space group. The structure is three-dimensional. there are three inequivalent Tm3+ sites. In the first Tm3+ site, Tm3+ is bonded to seven C+3.20- atoms to form distorted TmC7 pentagonal bipyramids that share corners with two equivalent CTm5NiC pentagonal bipyramids, corners with five equivalent TmC7 pentagonal bipyramids, edges with four equivalent TmC6 octahedra, edges with two equivalent TmC7 pentagonal bipyramids, and faces with two equivalent TmC7 pentagonal bipyramids. There are a spread of Tm–C bond distances ranging from 2.32–2.58 Å. In the second Tm3+ site, Tm3+ is bonded in a square co-planar geometry to four equivalent C+3.20- atoms. All Tm–C bond lengths are 2.62 Å. In the third Tm3+ site, Tm3+ is bonded to six C+3.20- atoms to form TmC6 octahedra that share corners with four equivalent TmC6 octahedra, edges with four equivalent TmC6 octahedra, and edges with eight equivalent TmC7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 1°. There are a spread of Tm–C bond distances ranging from 2.53–2.62 Å. Ni2+ is bonded in a 3-coordinate geometry to three C+3.20- atoms. There are two shorter (1.93 Å) and one longer (2.11 Å) Ni–C bond lengths. There are three inequivalent C+3.20- sites. In the first C+3.20- site, C+3.20- is bonded to five Tm3+, one Ni2+, and one C+3.20- atom to form distorted CTm5NiC pentagonal bipyramids that share corners with two equivalent TmC7 pentagonal bipyramids, corners with five equivalent CTm5NiC pentagonal bipyramids, edges with four equivalent CTm6 octahedra, and edges with four equivalent CTm5NiC pentagonal bipyramids. The C–C bond length is 1.39 Å. In the second C+3.20- site, C+3.20- is bonded in a 7-coordinate geometry to four Tm3+, two equivalent Ni2+, and one C+3.20- atom. In the third C+3.20- site, C+3.20- is bonded to six Tm3+ atoms to form CTm6 octahedra that share corners with four equivalent CTm6 octahedra, edges with four equivalent CTm6 octahedra, and edges with eight equivalent CTm5NiC pentagonal bipyramids. The corner-sharing octahedral tilt angles are 1°.
DOI: 10.17188/1684606
title: Materials Data on GaNi10P3 by Materials Project

description: Ni10GaP3 crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. there are seven inequivalent Ni sites. In the first Ni site, Ni is bonded in a distorted bent 150 degrees geometry to two equivalent Ni and two equivalent P atoms. Both Ni–Ni bond lengths are 2.71 Å. Both Ni–P bond lengths are 2.22 Å. In the second Ni site, Ni is bonded in a 4-coordinate geometry to one Ni and three equivalent P atoms. The Ni–Ni bond length is 2.26 Å. All Ni–P bond lengths are 2.28 Å. In the third Ni site, Ni is bonded in a 3-coordinate geometry to two equivalent Ni, one Ga, and three P atoms. Both Ni–Ni bond lengths are 2.63 Å. The Ni–Ga bond length is 2.52 Å. There are two shorter (2.18 Å) and one longer (2.29 Å) Ni–P bond lengths. In the fourth Ni site, Ni is bonded in a 4-coordinate geometry to three equivalent Ni, one Ga, and three equivalent P atoms. All Ni–Ni bond lengths are 2.64 Å. The Ni–Ga bond length is 2.44 Å. All Ni–P bond lengths are 2.40 Å. In the fifth Ni site, Ni is bonded in a 12-coordinate geometry to eight Ni, one Ga, and three P atoms. There are two shorter (2.50 Å) and one longer (2.53 Å) Ni–Ni bond lengths. The Ni–Ga bond length is 2.53 Å. There are two shorter (2.26 Å) and one longer (2.30 Å) Ni–P bond lengths. In the sixth Ni site, Ni is bonded in a distorted tetrahedral geometry to three equivalent Ni, one Ga, and three equivalent P atoms. The Ni–Ga bond length is 2.35 Å. All Ni–P bond lengths are 2.34 Å. In the seventh Ni site, Ni is bonded in a 2-coordinate geometry to two equivalent Ni, one Ga, and two equivalent P atoms. The Ni–Ga bond length is 2.59 Å. Both Ni–P bond lengths are 2.27 Å. There are two inequivalent Ga sites. In the first Ga site, Ga is bonded in a 5-coordinate geometry to five Ni atoms. In the second Ga site, Ga is bonded in a cuboctahedral geometry to twelve Ni atoms. There are two inequivalent P sites. In the first P site, P is bonded in a body-centered cubic geometry to eight Ni atoms. In the second P site, P is bonded in a 9-coordinate geometry to nine Ni atoms.
DOI: 10.17188/1684607
title: Materials Data on LaTa2AgO7 by Materials Project

description: LaTa2AgO7 crystallizes in the tetragonal I-4m2 space group. The structure is three-dimensional. La3+ is bonded to twelve O2- atoms to form a mixture of corner and face-sharing LaO12 cuboctahedra. There are a spread of La–O bond distances ranging from 2.69–2.76 Å. Ta5+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ta–O bond distances ranging from 1.81–2.28 Å. Ag1+ is bonded to four equivalent O2- atoms to form corner-sharing AgO4 tetrahedra. All Ag–O bond lengths are 2.39 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent La3+ and two equivalent Ta5+ atoms. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two equivalent La3+ and two equivalent Ta5+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one Ta5+ and two equivalent Ag1+ atoms. In the fourth O2- site, O2- is bonded to four equivalent La3+ and two equivalent Ta5+ atoms to form a mixture of distorted corner and edge-sharing OLa4Ta2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1684608
title: Materials Data on TaPb2N3 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: 10.17188/1684609
title: Materials Data on Cs3InCl6 by Materials Project

description: Cs3InCl6 is (Cubic) Perovskite-like structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Cs1+ sites. In the first Cs1+ site, 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 CsCl6 octahedra, and faces with four equivalent InCl6 octahedra. All Cs–Cl bond lengths are 4.13 Å. In the second Cs1+ site, Cs1+ is bonded to six equivalent Cl1- atoms to form CsCl6 octahedra that share corners with six equivalent InCl6 octahedra and faces with eight equivalent CsCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Cl bond lengths are 3.27 Å. In3+ is bonded to six equivalent Cl1- atoms to form InCl6 octahedra that share corners with six equivalent CsCl6 octahedra and faces with eight equivalent CsCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All In–Cl bond lengths are 2.55 Å. Cl1- is bonded in a distorted linear geometry to five Cs1+ and one In3+ atom.
DOI: 10.17188/1684610
title: Materials Data on NaMg4(SiO3)6 by Materials Project

description: NaMg4(SiO3)6 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Na is bonded in a 8-coordinate geometry to eight O atoms. There are a spread of Na–O bond distances ranging from 2.43–2.93 Å. There are four inequivalent Mg sites. In the first Mg site, Mg is bonded to six O atoms to form distorted MgO6 octahedra that share corners with four equivalent SiO4 tetrahedra and edges with six MgO6 octahedra. There are a spread of Mg–O bond distances ranging from 1.98–2.15 Å. In the second Mg site, Mg is bonded to six O atoms to form distorted MgO6 octahedra that share corners with four SiO4 tetrahedra and edges with five MgO6 octahedra. There are a spread of Mg–O bond distances ranging from 1.97–2.17 Å. In the third Mg site, Mg is bonded to six O atoms to form distorted MgO6 octahedra that share corners with four SiO4 tetrahedra and edges with six MgO6 octahedra. There are a spread of Mg–O bond distances ranging from 2.07–2.29 Å. In the fourth Mg site, Mg is bonded to six O atoms to form MgO6 octahedra that share corners with six SiO4 tetrahedra and edges with three MgO6 octahedra. There are a spread of Mg–O bond distances ranging from 2.02–2.19 Å. There are three inequivalent Si sites. In the first Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with three MgO6 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 56–60°. There are a spread of Si–O bond distances ranging from 1.63–1.65 Å. In the second Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with three MgO6 octahedra and corners with three SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 56–61°. There are a spread of Si–O bond distances ranging from 1.63–1.65 Å. In the third Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with three MgO6 octahedra and corners with two equivalent SiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 25–56°. There are a spread of Si–O bond distances ranging from 1.63–1.67 Å. There are nine inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to two equivalent Si atoms. In the second O site, O is bonded in a bent 150 degrees geometry to two Si atoms. In the third O site, O is bonded in a 2-coordinate geometry to one Na and two Si atoms. In the fourth O site, O is bonded in a rectangular see-saw-like geometry to three Mg and one Si atom. In the fifth O site, O is bonded in a distorted bent 150 degrees geometry to one Na and two Si atoms. In the sixth O site, O is bonded in a distorted T-shaped geometry to one Na, one Mg, and one Si atom. In the seventh O site, O is bonded to three Mg and one Si atom to form a mixture of distorted corner and edge-sharing OMg3Si tetrahedra. In the eighth O site, O is bonded in a 4-coordinate geometry to three Mg and one O atom. The O–O bond length is 1.51 Å. In the ninth O site, O is bonded in a distorted rectangular see-saw-like geometry to one Na, two Mg, and one Si atom.
DOI: 10.17188/1684611
title: Materials Data on Ba4Pd by Materials Project

description: Ba4Pd is Iron carbide-like structured and crystallizes in the cubic Fd-3m space group. The structure is zero-dimensional and consists of eight Ba4Pd clusters. Ba is bonded in a single-bond geometry to one Pd atom. The Ba–Pd bond length is 2.98 Å. Pd is bonded in a tetrahedral geometry to four equivalent Ba atoms.
DOI: 10.17188/1684612
title: Materials Data on Nb2B2Mo by Materials Project

description: Nb2MoB2 crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Nb2+ is bonded in a hexagonal planar geometry to six equivalent B3- atoms. There are four shorter (2.45 Å) and two longer (2.48 Å) Nb–B bond lengths. Mo2+ is bonded in a square co-planar geometry to four equivalent B3- atoms. All Mo–B bond lengths are 2.49 Å. B3- is bonded in a 9-coordinate geometry to six equivalent Nb2+, two equivalent Mo2+, and one B3- atom. The B–B bond length is 1.88 Å.
DOI: 10.17188/1684613
title: Materials Data on Mo2N2O7 by Materials Project

description: (Mo2NO7)2N2 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two ammonia molecules and one Mo2NO7 cluster. In the Mo2NO7 cluster, there are two inequivalent Mo6+ sites. In the first Mo6+ site, Mo6+ is bonded in a 4-coordinate geometry to five O2- atoms. There are a spread of Mo–O bond distances ranging from 1.71–2.28 Å. 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 1.72–2.01 Å. N1+ is bonded in a single-bond geometry to one O2- atom. The N–O bond length is 1.26 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to two Mo6+ atoms. In the second O2- site, O2- is bonded in a single-bond geometry to one Mo6+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one Mo6+ atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one Mo6+ atom. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to one Mo6+ and one N1+ atom. In the sixth O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Mo6+ and one O2- atom. The O–O bond length is 1.54 Å. In the seventh O2- site, O2- is bonded in a single-bond geometry to one Mo6+ atom.
DOI: 10.17188/1685059
title: Materials Data on Li2CoHgF6 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: 10.17188/1685062
title: Materials Data on C4NCl2 by Materials Project

description: CCN(CCl)2 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of sixteen chloromethane molecules, eight hydrogen cyanide molecules, and eight methane molecules.
DOI: 10.17188/1685063
title: Materials Data on GeI2 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: 10.17188/1685064
title: Materials Data on FeSO7 by Materials Project

description: FeSO7 crystallizes in the monoclinic P2_1/m space group. The structure is one-dimensional and consists of one FeSO7 ribbon oriented in the (0, 1, 0) direction. Fe is bonded to six O atoms to form FeO6 octahedra that share corners with two equivalent FeO6 octahedra and corners with two equivalent SO4 tetrahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of Fe–O bond distances ranging from 1.83–2.31 Å. S is bonded to four O atoms to form SO4 tetrahedra that share corners with two equivalent FeO6 octahedra. The corner-sharing octahedral tilt angles are 44°. There are a spread of S–O bond distances ranging from 1.44–1.55 Å. There are five inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to one Fe and one S atom. In the second O site, O is bonded in a single-bond geometry to one S atom. In the third O site, O is bonded in a single-bond geometry to one S atom. In the fourth O site, O is bonded in a bent 120 degrees geometry to two equivalent Fe atoms. In the fifth O site, O is bonded in a bent 120 degrees geometry to one Fe and one O atom. The O–O bond length is 1.25 Å.
DOI: 10.17188/1685066
title: Materials Data on KP by Materials Project

description: PK1 is Halite, Rock Salt structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. K1+ is bonded to six equivalent P1- atoms to form a mixture of edge and corner-sharing KP6 octahedra. The corner-sharing octahedral tilt angles are 0°. All K–P bond lengths are 3.36 Å. P1- is bonded to six equivalent K1+ atoms to form a mixture of edge and corner-sharing PK6 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1685068
title: Materials Data on BrO3 by Materials Project

description: BrO3 crystallizes in the orthorhombic Aea2 space group. The structure is one-dimensional and consists of four hydrogen peroxide molecules and four BrO ribbons oriented in the (0, 0, 1) direction. In each BrO ribbon, O is bonded in a distorted bent 120 degrees geometry to two equivalent Br atoms. Both O–Br bond lengths are 1.94 Å. Br is bonded in a distorted bent 120 degrees geometry to two equivalent O atoms.
DOI: 10.17188/1685069
title: Materials Data on Li2P8W3O29 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: 10.17188/1685071
title: Materials Data on HPtN5Cl4 by Materials Project

description: PtN3ClNHCl2NCl crystallizes in the trigonal R3m space group. The structure is zero-dimensional and consists of nine chloramine molecules; nine chloramine hydrochloride molecules; and nine platinum(1+), chloride molecules.
DOI: 10.17188/1685072
title: Materials Data on GaN 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: 10.17188/1685073
title: Materials Data on Sr2Ti2O5 by Materials Project

description: Sr2Ti2O5 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Sr–O bond distances ranging from 2.60–3.03 Å. In the second Sr2+ site, Sr2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Sr–O bond distances ranging from 2.60–3.04 Å. There are three inequivalent Ti3+ sites. In the first Ti3+ site, Ti3+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with four equivalent TiO6 octahedra and a cornercorner with one TiO4 trigonal pyramid. The corner-sharing octahedra tilt angles range from 6–8°. There are a spread of Ti–O bond distances ranging from 1.99–2.04 Å. In the second Ti3+ site, Ti3+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There is two shorter (1.92 Å) and two longer (1.93 Å) Ti–O bond length. In the third Ti3+ site, Ti3+ is bonded to four O2- atoms to form corner-sharing TiO4 trigonal pyramids. The corner-sharing octahedral tilt angles are 15°. There are a spread of Ti–O bond distances ranging from 1.91–1.93 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded to four Sr2+ and two equivalent Ti3+ atoms to form a mixture of distorted corner and edge-sharing OSr4Ti2 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+ and two equivalent Ti3+ atoms. In the third O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two Ti3+ atoms. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two Ti3+ atoms. In the fifth O2- site, O2- is bonded in a distorted linear geometry to four Sr2+ and two Ti3+ atoms. In the sixth O2- site, O2- is bonded in a distorted linear geometry to four Sr2+ and two Ti3+ atoms.
DOI: 10.17188/1685074
title: Materials Data on PmRh3 by Materials Project

description: PmRh3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pm is bonded to twelve equivalent Rh atoms to form a mixture of face and corner-sharing PmRh12 cuboctahedra. There are six shorter (2.96 Å) and six longer (2.97 Å) Pm–Rh bond lengths. Rh is bonded in a distorted see-saw-like geometry to four equivalent Pm atoms.