cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1727589
title: Materials Data on Ti3AgS6 by Materials Project

description: Ti3AgS6 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. there are two inequivalent Ti+3.67+ sites. In the first Ti+3.67+ site, Ti+3.67+ is bonded to six equivalent S2- atoms to form TiS6 octahedra that share corners with six equivalent AgS6 octahedra and edges with six equivalent TiS6 octahedra. The corner-sharing octahedral tilt angles are 46°. All Ti–S bond lengths are 2.44 Å. In the second Ti+3.67+ site, Ti+3.67+ is bonded to six equivalent S2- atoms to form TiS6 octahedra that share corners with three equivalent AgS6 octahedra, edges with six TiS6 octahedra, and a faceface with one AgS6 octahedra. The corner-sharing octahedral tilt angles are 47°. There are three shorter (2.43 Å) and three longer (2.48 Å) Ti–S bond lengths. Ag1+ is bonded to six equivalent S2- atoms to form AgS6 octahedra that share corners with twelve TiS6 octahedra and faces with two equivalent TiS6 octahedra. The corner-sharing octahedra tilt angles range from 46–47°. All Ag–S bond lengths are 2.69 Å. S2- is bonded in a rectangular see-saw-like geometry to three Ti+3.67+ and one Ag1+ atom.
DOI: 10.17188/1727590
title: Materials Data on ZrCrAgS4 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: 10.17188/1727591
title: Materials Data on Li2MnCr3O8 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: 10.17188/1727592
title: Materials Data on EuMgGa3 by Materials Project

description: MgEuGa3 crystallizes in the tetragonal I-4m2 space group. The structure is three-dimensional. Mg is bonded in a 4-coordinate geometry to four equivalent Eu and eight Ga atoms. All Mg–Eu bond lengths are 3.59 Å. There are four shorter (2.70 Å) and four longer (3.07 Å) Mg–Ga bond lengths. Eu is bonded in a 8-coordinate geometry to four equivalent Mg and twelve Ga atoms. There are eight shorter (3.32 Å) and four longer (3.59 Å) Eu–Ga bond lengths. There are two inequivalent Ga sites. In the first Ga site, Ga is bonded in a 2-coordinate geometry to two equivalent Mg, four equivalent Eu, and three Ga atoms. There are one shorter (2.50 Å) and two longer (2.70 Å) Ga–Ga bond lengths. In the second Ga site, Ga is bonded to four equivalent Mg, four equivalent Eu, and four equivalent Ga atoms to form a mixture of face and corner-sharing GaEu4Mg4Ga4 cuboctahedra.
DOI: 10.17188/1727593
title: Materials Data on SrU2Se5 by Materials Project

description: SrU2Se5 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Sr2+ is bonded to seven Se2- atoms to form distorted edge-sharing SrSe7 pentagonal bipyramids. There are a spread of Sr–Se bond distances ranging from 2.93–3.10 Å. U4+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of U–Se bond distances ranging from 2.80–3.16 Å. There are four inequivalent Se2- sites. In the first Se2- site, Se2- is bonded to two equivalent Sr2+ and two equivalent U4+ atoms to form distorted SeSr2U2 tetrahedra that share corners with six SeSrU4 square pyramids, corners with six equivalent SeSr2U2 tetrahedra, edges with three SeSrU4 square pyramids, and an edgeedge with one SeSr2U2 tetrahedra. In the second Se2- site, Se2- is bonded in a 5-coordinate geometry to one Sr2+ and four equivalent U4+ atoms. In the third Se2- site, Se2- is bonded to one Sr2+ and four equivalent U4+ atoms to form SeSrU4 square pyramids that share corners with four equivalent SeSrU4 square pyramids, corners with eight equivalent SeSr2U2 tetrahedra, edges with three SeSrU4 square pyramids, edges with two equivalent SeSr2U2 tetrahedra, and a faceface with one SeSrU4 square pyramid. In the fourth Se2- site, Se2- is bonded to one Sr2+ and four equivalent U4+ atoms to form distorted SeSrU4 square pyramids that share corners with eight SeSrU4 square pyramids, corners with four equivalent SeSr2U2 tetrahedra, an edgeedge with one SeSrU4 square pyramid, edges with four equivalent SeSr2U2 tetrahedra, and a faceface with one SeSrU4 square pyramid.
DOI: 10.17188/1727594
title: Materials Data on Ti2Cr3O12 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: 10.17188/1727596
title: Materials Data on Yb3Ge13Ir4 by Materials Project

description: Yb3Ir4Ge13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Yb is bonded in a 8-coordinate geometry to four equivalent Ir and twelve equivalent Ge atoms. All Yb–Ir bond lengths are 3.20 Å. There are eight shorter (3.15 Å) and four longer (3.26 Å) Yb–Ge bond lengths. Ir is bonded in a 9-coordinate geometry to three equivalent Yb and six equivalent Ge atoms. All Ir–Ge bond lengths are 2.51 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 6-coordinate geometry to three equivalent Yb, two equivalent Ir, and two Ge atoms. There are one shorter (2.62 Å) and one longer (3.07 Å) Ge–Ge bond lengths. In the second Ge site, Ge is bonded in a cuboctahedral geometry to twelve equivalent Ge atoms.
DOI: 10.17188/1727597
title: Materials Data on Hf2ZnFe by Materials Project

description: Hf2FeZn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Hf2FeZn ribbons oriented in the (1, 0, 0) direction. Hf is bonded in a linear geometry to one Fe and one Zn atom. The Hf–Fe bond length is 2.09 Å. The Hf–Zn bond length is 2.98 Å. Fe is bonded in a linear geometry to two equivalent Hf atoms. Zn is bonded in a linear geometry to two equivalent Hf atoms.
DOI: 10.17188/1727598
title: Materials Data on GdGaPd2 by Materials Project

description: GdPd2Ga is delta Molybdenum Boride-derived structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Gd is bonded in a 11-coordinate geometry to eight equivalent Pd and three equivalent Ga atoms. There are a spread of Gd–Pd bond distances ranging from 3.07–3.30 Å. There are a spread of Gd–Ga bond distances ranging from 3.07–3.11 Å. Pd is bonded in a 12-coordinate geometry to four equivalent Gd and three equivalent Ga atoms. There are a spread of Pd–Ga bond distances ranging from 2.55–2.66 Å. Ga is bonded in a 9-coordinate geometry to three equivalent Gd and six equivalent Pd atoms.
DOI: 10.17188/1727600
title: Materials Data on LiH2N by Materials Project

description: LiNH2 crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. Li1+ is bonded in a 8-coordinate geometry to four equivalent N3- and four H1+ atoms. There are two shorter (2.10 Å) and two longer (2.23 Å) Li–N bond lengths. There are two shorter (2.05 Å) and two longer (2.11 Å) Li–H bond lengths. N3- is bonded in a 1-coordinate geometry to four equivalent Li1+ and three H1+ atoms. There is one shorter (1.03 Å) and two longer (1.38 Å) N–H bond length. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to two equivalent Li1+ and one N3- atom. In the second H1+ site, H1+ is bonded in a distorted linear geometry to two equivalent Li1+ and two equivalent N3- atoms.
DOI: 10.17188/1727602
title: Materials Data on BaLaMn2O6 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: 10.17188/1727603
title: Materials Data on KI by Materials Project

description: IK1 is Molybdenum Carbide MAX Phase-like structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. K1+ is bonded to six equivalent I1- atoms to form a mixture of corner, edge, and face-sharing KI6 octahedra. The corner-sharing octahedra tilt angles range from 45–48°. There are a spread of K–I bond distances ranging from 3.58–3.63 Å. I1- is bonded to six equivalent K1+ atoms to form a mixture of distorted corner and edge-sharing IK6 pentagonal pyramids.
DOI: 10.17188/1727604
title: Materials Data on Ba5Y2ZrAl2O13 by Materials Project

description: Ba5Y2ZrAl2O13 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are three inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 12-coordinate geometry to nine equivalent O2- atoms. There are three shorter (2.93 Å) and six longer (3.03 Å) Ba–O bond lengths. In the second Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are three shorter (2.78 Å) and six longer (3.08 Å) Ba–O bond lengths. In the third Ba2+ site, Ba2+ is bonded in a 6-coordinate geometry to six equivalent O2- atoms. All Ba–O bond lengths are 2.93 Å. Y3+ is bonded to six O2- atoms to form YO6 octahedra that share corners with three equivalent ZrO6 octahedra and corners with three equivalent AlO4 tetrahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (2.26 Å) and three longer (2.27 Å) Y–O bond lengths. Zr4+ is bonded to six equivalent O2- atoms to form ZrO6 octahedra that share corners with six equivalent YO6 octahedra. The corner-sharing octahedral tilt angles are 1°. All Zr–O bond lengths are 2.12 Å. Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with three equivalent YO6 octahedra and a cornercorner with one AlO4 tetrahedra. The corner-sharing octahedral tilt angles are 19°. There is one shorter (1.74 Å) and three longer (1.78 Å) Al–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four Ba2+, one Y3+, and one Zr4+ atom to form a mixture of distorted face, edge, and corner-sharing OBa4YZr octahedra. The corner-sharing octahedra tilt angles range from 0–61°. In the second O2- site, O2- is bonded in a linear geometry to two equivalent Al3+ atoms. In the third O2- site, O2- is bonded in a 2-coordinate geometry to three Ba2+, one Y3+, and one Al3+ atom.
DOI: 10.17188/1727605
title: Materials Data on YZnPd2 by Materials Project

description: YPd2Zn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two YPd2Zn ribbons oriented in the (1, 0, 0) direction. Y is bonded in a linear geometry to two equivalent Pd atoms. Both Y–Pd bond lengths are 2.41 Å. Pd is bonded in a linear geometry to one Y and one Zn atom. The Pd–Zn bond length is 2.54 Å. Zn is bonded in a linear geometry to two equivalent Pd atoms.
DOI: 10.17188/1727606
title: Materials Data on CaAlPt by Materials Project

description: CaPtAl crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ca is bonded in a 5-coordinate geometry to five equivalent Pt and six equivalent Al atoms. There are a spread of Ca–Pt bond distances ranging from 3.00–3.16 Å. There are a spread of Ca–Al bond distances ranging from 3.17–3.35 Å. Pt is bonded in a 9-coordinate geometry to five equivalent Ca and four equivalent Al atoms. There are a spread of Pt–Al bond distances ranging from 2.60–2.71 Å. Al is bonded in a 4-coordinate geometry to six equivalent Ca and four equivalent Pt atoms.
DOI: 10.17188/1727608
title: Materials Data on Rb2LuAuCl6 by Materials Project

description: Rb2LuAuCl6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Rb1+ is bonded to twelve equivalent Cl1- atoms to form RbCl12 cuboctahedra that share corners with twelve equivalent RbCl12 cuboctahedra, faces with six equivalent RbCl12 cuboctahedra, faces with four equivalent LuCl6 octahedra, and faces with four equivalent AuCl6 octahedra. All Rb–Cl bond lengths are 3.78 Å. Lu3+ is bonded to six equivalent Cl1- atoms to form LuCl6 octahedra that share corners with six equivalent AuCl6 octahedra and faces with eight equivalent RbCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Lu–Cl bond lengths are 2.58 Å. Au1+ is bonded to six equivalent Cl1- atoms to form AuCl6 octahedra that share corners with six equivalent LuCl6 octahedra and faces with eight equivalent RbCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Au–Cl bond lengths are 2.76 Å. Cl1- is bonded in a 6-coordinate geometry to four equivalent Rb1+, one Lu3+, and one Au1+ atom.
DOI: 10.17188/1727609
title: Materials Data on CoTeMo by Materials Project

description: MoCoTe crystallizes in the orthorhombic Pmmn space group. The structure is three-dimensional. Mo is bonded in a 4-coordinate geometry to four equivalent Co and two equivalent Te atoms. There are two shorter (2.55 Å) and two longer (2.56 Å) Mo–Co bond lengths. There are one shorter (2.77 Å) and one longer (2.78 Å) Mo–Te bond lengths. Co is bonded in a body-centered cubic geometry to four equivalent Mo and four equivalent Te atoms. There are two shorter (2.68 Å) and two longer (2.72 Å) Co–Te bond lengths. Te is bonded in a 4-coordinate geometry to two equivalent Mo and four equivalent Co atoms.
DOI: 10.17188/1727610
title: Materials Data on Gd2Al4CoGe2 by Materials Project

description: Gd2CoAl4Ge2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Gd is bonded in a 5-coordinate geometry to four equivalent Al and five equivalent Ge atoms. All Gd–Al bond lengths are 3.11 Å. There are four shorter (2.97 Å) and one longer (3.04 Å) Gd–Ge bond lengths. Co is bonded in a body-centered cubic geometry to eight Al atoms. All Co–Al bond lengths are 2.44 Å. There are three inequivalent Al sites. In the first Al site, Al is bonded in a 4-coordinate geometry to two equivalent Gd, two equivalent Co, five equivalent Al, and two equivalent Ge atoms. Both Al–Co bond lengths are 2.44 Å. There are one shorter (2.57 Å) and four longer (2.93 Å) Al–Al bond lengths. Both Al–Ge bond lengths are 2.80 Å. In the second Al site, Al is bonded in a 4-coordinate geometry to two equivalent Gd, two equivalent Co, five Al, and two equivalent Ge atoms. Both Al–Gd bond lengths are 3.11 Å. There are one shorter (2.57 Å) and four longer (2.93 Å) Al–Al bond lengths. Both Al–Ge bond lengths are 2.80 Å. In the third Al site, Al is bonded in a 4-coordinate geometry to two equivalent Gd, two equivalent Co, five Al, and two equivalent Ge atoms. Both Al–Gd bond lengths are 3.11 Å. All Al–Al bond lengths are 2.93 Å. Both Al–Ge bond lengths are 2.80 Å. Ge is bonded in a 9-coordinate geometry to five equivalent Gd and four equivalent Al atoms.
DOI: 10.17188/1727612
title: Materials Data on BaLa3Sc4HO12 by Materials Project

description: BaLa3Sc4HO12 crystallizes in the monoclinic Pm space group. The structure is three-dimensional. Ba2+ is bonded in a 10-coordinate geometry to one H1+ and nine O2- atoms. The Ba–H bond length is 2.59 Å. There are a spread of Ba–O bond distances ranging from 2.60–3.16 Å. There are three inequivalent La3+ sites. In the first La3+ site, La3+ is bonded in a 9-coordinate geometry to one H1+ and eight O2- atoms. The La–H bond length is 2.62 Å. There are a spread of La–O bond distances ranging from 2.39–3.06 Å. In the second La3+ site, La3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of La–O bond distances ranging from 2.41–2.94 Å. In the third La3+ site, La3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of La–O bond distances ranging from 2.40–3.01 Å. There are two inequivalent Sc3+ sites. In the first Sc3+ site, Sc3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Sc–O bond distances ranging from 2.03–2.25 Å. In the second Sc3+ site, Sc3+ is bonded to six O2- atoms to form corner-sharing ScO6 octahedra. The corner-sharing octahedra tilt angles range from 32–35°. There are a spread of Sc–O bond distances ranging from 2.13–2.18 Å. H1+ is bonded in a single-bond geometry to one Ba2+, one La3+, and one O2- atom. The H–O bond length is 0.99 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Ba2+, one La3+, and two equivalent Sc3+ atoms. In the second O2- site, O2- is bonded in a single-bond geometry to one Ba2+, one La3+, two equivalent Sc3+, and one H1+ atom. In the third O2- site, O2- is bonded in a distorted tetrahedral geometry to two La3+ and two equivalent Sc3+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two La3+ and two equivalent Sc3+ atoms. In the fifth O2- site, O2- is bonded in a 5-coordinate geometry to one Ba2+, two La3+, and two Sc3+ atoms. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Ba2+, two La3+, and two Sc3+ atoms. In the seventh O2- site, O2- is bonded in a 5-coordinate geometry to one Ba2+, two La3+, and two Sc3+ atoms. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to three La3+ and two Sc3+ atoms.
DOI: 10.17188/1727615
title: Materials Data on TbCuGe by Materials Project

description: TbCuGe is hexagonal omega structure-derived structured and crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Tb is bonded to six equivalent Cu and six equivalent Ge atoms to form a mixture of edge and face-sharing TbCu6Ge6 cuboctahedra. All Tb–Cu bond lengths are 3.08 Å. All Tb–Ge bond lengths are 3.08 Å. Cu is bonded in a 9-coordinate geometry to six equivalent Tb and three equivalent Ge atoms. All Cu–Ge bond lengths are 2.45 Å. Ge is bonded in a 9-coordinate geometry to six equivalent Tb and three equivalent Cu atoms.
DOI: 10.17188/1727616
title: Materials Data on ZrSn by Materials Project

description: ZrSn is beta-prime cadmium gold structured and crystallizes in the orthorhombic Pmma space group. The structure is three-dimensional. Zr is bonded in a 12-coordinate geometry to eight equivalent Sn atoms. There are a spread of Zr–Sn bond distances ranging from 3.08–3.22 Å. Sn is bonded in a 8-coordinate geometry to eight equivalent Zr atoms.
DOI: 10.17188/1727617
title: Materials Data on ErThRu2 by Materials Project

description: ThErRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Th is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Th–Ru bond lengths are 3.01 Å. Er is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Er–Ru bond lengths are 3.01 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Th and four equivalent Er atoms.
DOI: 10.17188/1727618
title: Materials Data on CrMoW2 by Materials Project

description: W2MoCr crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two W2MoCr ribbons oriented in the (1, 0, 0) direction. W is bonded in a linear geometry to one Mo and one Cr atom. The W–Mo bond length is 2.22 Å. The W–Cr bond length is 2.59 Å. Mo is bonded in a linear geometry to two equivalent W atoms. Cr is bonded in a linear geometry to two equivalent W atoms.
DOI: 10.17188/1727619
title: Materials Data on Ho2NiRuO6 by Materials Project

description: Ho2RuNiO6 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ho3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Ho–O bond distances ranging from 2.23–2.78 Å. Ru4+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with six equivalent NiO6 octahedra. The corner-sharing octahedra tilt angles range from 37–41°. There are four shorter (2.02 Å) and two longer (2.04 Å) Ru–O bond lengths. Ni2+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with six equivalent RuO6 octahedra. The corner-sharing octahedra tilt angles range from 37–41°. There are two shorter (2.07 Å) and four longer (2.08 Å) Ni–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Ho3+, one Ru4+, and one Ni2+ atom to form distorted corner-sharing OHo2NiRu trigonal pyramids. In the second O2- site, O2- is bonded in a 5-coordinate geometry to three equivalent Ho3+, one Ru4+, and one Ni2+ atom. In the third O2- site, O2- is bonded in a 5-coordinate geometry to three equivalent Ho3+, one Ru4+, and one Ni2+ atom.
DOI: 10.17188/1727620
title: Materials Data on AcTh3 by Materials Project

description: Th3Ac is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are three inequivalent Th sites. In the first Th site, Th is bonded to eight Th and four equivalent Ac atoms to form ThAc4Th8 cuboctahedra that share corners with four equivalent AcTh12 cuboctahedra, corners with fourteen ThAc4Th8 cuboctahedra, edges with six equivalent AcTh12 cuboctahedra, edges with twelve ThAc4Th8 cuboctahedra, faces with four equivalent AcTh12 cuboctahedra, and faces with sixteen ThAc4Th8 cuboctahedra. There are a spread of Th–Th bond distances ranging from 3.54–3.78 Å. There are two shorter (3.66 Å) and two longer (3.72 Å) Th–Ac bond lengths. In the second Th site, Th is bonded to eight equivalent Th and four equivalent Ac atoms to form ThAc4Th8 cuboctahedra that share corners with four equivalent AcTh12 cuboctahedra, corners with fourteen ThAc4Th8 cuboctahedra, edges with six equivalent AcTh12 cuboctahedra, edges with twelve equivalent ThAc4Th8 cuboctahedra, faces with four equivalent AcTh12 cuboctahedra, and faces with sixteen ThAc4Th8 cuboctahedra. There are two shorter (3.66 Å) and two longer (3.72 Å) Th–Ac bond lengths. In the third Th site, Th is bonded to eight equivalent Th and four equivalent Ac atoms to form ThAc4Th8 cuboctahedra that share corners with four equivalent AcTh12 cuboctahedra, corners with fourteen ThAc4Th8 cuboctahedra, edges with six equivalent AcTh12 cuboctahedra, edges with twelve equivalent ThAc4Th8 cuboctahedra, faces with four equivalent AcTh12 cuboctahedra, and faces with sixteen ThAc4Th8 cuboctahedra. There are two shorter (3.66 Å) and two longer (3.72 Å) Th–Ac bond lengths. Ac is bonded to twelve Th atoms to form AcTh12 cuboctahedra that share corners with six equivalent AcTh12 cuboctahedra, corners with twelve ThAc4Th8 cuboctahedra, edges with eighteen ThAc4Th8 cuboctahedra, faces with eight equivalent AcTh12 cuboctahedra, and faces with twelve ThAc4Th8 cuboctahedra.