cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1687822
title: Materials Data on ThU(CuSi)4 by Materials Project

description: UTh(CuSi)4 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. U6+ is bonded to eight equivalent Si4- atoms to form USi8 hexagonal bipyramids that share corners with sixteen equivalent CuSi4 tetrahedra, edges with four equivalent USi8 hexagonal bipyramids, edges with eight equivalent CuSi4 tetrahedra, and faces with four equivalent USi8 hexagonal bipyramids. All U–Si bond lengths are 3.09 Å. Th4+ is bonded in a distorted body-centered cubic geometry to eight equivalent Si4- atoms. All Th–Si bond lengths are 3.11 Å. Cu+1.50+ is bonded to four Si4- atoms to form CuSi4 tetrahedra that share corners with four equivalent USi8 hexagonal bipyramids, corners with four equivalent CuSi4 tetrahedra, edges with two equivalent USi8 hexagonal bipyramids, and edges with four equivalent CuSi4 tetrahedra. There are two shorter (2.40 Å) and two longer (2.41 Å) Cu–Si bond lengths. There are two inequivalent Si4- sites. In the first Si4- site, Si4- is bonded in a 9-coordinate geometry to four equivalent Th4+, four equivalent Cu+1.50+, and one Si4- atom. The Si–Si bond length is 2.42 Å. In the second Si4- site, Si4- is bonded in a 9-coordinate geometry to four equivalent U6+, four equivalent Cu+1.50+, and one Si4- atom. The Si–Si bond length is 2.33 Å.
DOI: 10.17188/1687823
title: Materials Data on LuB12 by Materials Project

description: LuB12 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Lu is bonded in a 1-coordinate geometry to twenty-four equivalent B atoms. All Lu–B bond lengths are 2.77 Å. B is bonded in a 7-coordinate geometry to two equivalent Lu and five equivalent B atoms. There is one shorter (1.71 Å) and four longer (1.78 Å) B–B bond length.
DOI: 10.17188/1687824
title: Materials Data on VO2 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: 10.17188/1687825
title: Materials Data on LuHSe by Materials Project

description: LuHSe crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Lu3+ is bonded in a distorted trigonal planar geometry to three equivalent H1- and six equivalent Se2- atoms. All Lu–H bond lengths are 2.17 Å. All Lu–Se bond lengths are 2.90 Å. H1- is bonded in a trigonal planar geometry to three equivalent Lu3+ atoms. Se2- is bonded to six equivalent Lu3+ atoms to form a mixture of distorted edge, corner, and face-sharing SeLu6 pentagonal pyramids.
DOI: 10.17188/1687826
title: Materials Data on Li6V3Ni(PO4)6 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: 10.17188/1687827
title: Materials Data on Hg2TeSe by Materials Project

description: Hg2TeSe is Lavarevi\'{c}ite-like structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. there are two inequivalent Hg2+ sites. In the first Hg2+ site, Hg2+ is bonded to three equivalent Te2- and one Se2- atom to form corner-sharing HgTe3Se tetrahedra. All Hg–Te bond lengths are 2.84 Å. The Hg–Se bond length is 2.70 Å. In the second Hg2+ site, Hg2+ is bonded to one Te2- and three equivalent Se2- atoms to form corner-sharing HgTeSe3 tetrahedra. The Hg–Te bond length is 2.88 Å. All Hg–Se bond lengths are 2.77 Å. Te2- is bonded to four Hg2+ atoms to form TeHg4 tetrahedra that share corners with six equivalent TeHg4 tetrahedra and corners with six equivalent SeHg4 tetrahedra. Se2- is bonded to four Hg2+ atoms to form SeHg4 tetrahedra that share corners with six equivalent TeHg4 tetrahedra and corners with six equivalent SeHg4 tetrahedra.
DOI: 10.17188/1687828
title: Materials Data on Mn3Al(SiO4)3 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: 10.17188/1687829
title: Materials Data on Si6Bi3N11 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: 10.17188/1687830
title: Materials Data on RbPr(SO6)2 by Materials Project

description: RbPr(SO6)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Rb is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Rb–O bond distances ranging from 2.89–3.51 Å. Pr is bonded in a 8-coordinate geometry to eight O atoms. There are a spread of Pr–O bond distances ranging from 2.38–2.73 Å. There are two inequivalent S sites. In the first S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.46–1.52 Å. In the second S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.45–1.53 Å. There are twelve inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to one Rb and one O atom. The O–O bond length is 1.26 Å. In the second O site, O is bonded in a single-bond geometry to one Rb and one S atom. In the third O site, O is bonded in a distorted water-like geometry to one Pr and one S atom. In the fourth O site, O is bonded in a distorted linear geometry to one Pr and one S atom. In the fifth O site, O is bonded in a bent 150 degrees geometry to one Pr and one S atom. In the sixth O site, O is bonded in a bent 120 degrees geometry to one Rb and one Pr atom. In the seventh O site, O is bonded in a 1-coordinate geometry to two equivalent Rb, one Pr, and one S atom. In the eighth O site, O is bonded in a distorted water-like geometry to one Pr and one S atom. In the ninth O site, O is bonded in a single-bond geometry to one S atom. In the tenth O site, O is bonded in a distorted single-bond geometry to two equivalent Rb, one Pr, and one S atom. In the eleventh O site, O is bonded in a bent 120 degrees geometry to two O atoms. The O–O bond length is 1.32 Å. In the twelfth O site, O is bonded in a water-like geometry to one Pr and one O atom.
DOI: 10.17188/1687831
title: Materials Data on Yb2NiGe6 by Materials Project

description: Yb2NiGe6 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Yb sites. In the first Yb site, Yb is bonded in a 10-coordinate geometry to ten Ge atoms. There are a spread of Yb–Ge bond distances ranging from 3.04–3.31 Å. In the second Yb site, Yb is bonded in a 10-coordinate geometry to four equivalent Ni and ten Ge atoms. All Yb–Ni bond lengths are 3.09 Å. There are a spread of Yb–Ge bond distances ranging from 3.06–3.34 Å. Ni is bonded in a 9-coordinate geometry to four equivalent Yb and five Ge atoms. There are a spread of Ni–Ge bond distances ranging from 2.32–2.41 Å. There are six inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to two equivalent Yb, two equivalent Ni, and five Ge atoms. There are one shorter (2.48 Å) and four longer (2.85 Å) Ge–Ge bond lengths. In the second Ge site, Ge is bonded in a 7-coordinate geometry to two equivalent Yb and five Ge atoms. All Ge–Ge bond lengths are 2.85 Å. In the third Ge site, Ge is bonded in a 3-coordinate geometry to two equivalent Yb, two equivalent Ni, and five Ge atoms. The Ge–Ge bond length is 2.50 Å. In the fourth Ge site, Ge is bonded in a 7-coordinate geometry to two equivalent Yb and five Ge atoms. In the fifth Ge site, Ge is bonded in a 1-coordinate geometry to six Yb, one Ni, and two equivalent Ge atoms. Both Ge–Ge bond lengths are 2.47 Å. In the sixth Ge site, Ge is bonded in a 8-coordinate geometry to six Yb and two equivalent Ge atoms.
DOI: 10.17188/1687832
title: Materials Data on Li3Sc by Materials Project

description: Li3Sc is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Li sites. In the first Li site, Li is bonded in a 12-coordinate geometry to eight Li and four equivalent Sc atoms. There are a spread of Li–Li bond distances ranging from 3.01–3.22 Å. There are two shorter (3.09 Å) and two longer (3.12 Å) Li–Sc bond lengths. In the second Li site, Li is bonded in a 12-coordinate geometry to eight equivalent Li and four equivalent Sc atoms. There are two shorter (3.09 Å) and two longer (3.12 Å) Li–Sc bond lengths. Sc is bonded to twelve Li atoms to form a mixture of corner and face-sharing ScLi12 cuboctahedra.
DOI: 10.17188/1687833
title: Materials Data on Ho2MgTc by Materials Project

description: MgHo2Tc is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a distorted body-centered cubic geometry to eight equivalent Ho atoms. All Mg–Ho bond lengths are 3.07 Å. Ho is bonded in a distorted body-centered cubic geometry to four equivalent Mg and four equivalent Tc atoms. All Ho–Tc bond lengths are 3.07 Å. Tc is bonded in a body-centered cubic geometry to eight equivalent Ho atoms.
DOI: 10.17188/1687835
title: Materials Data on Yb2ZnIr by Materials Project

description: Yb2IrZn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Yb is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Zn atoms. All Yb–Ir bond lengths are 2.98 Å. All Yb–Zn bond lengths are 2.98 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Yb atoms. Zn is bonded in a body-centered cubic geometry to eight equivalent Yb atoms.
DOI: 10.17188/1687836
title: Materials Data on KLiNiO2 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: 10.17188/1687837
title: Materials Data on SrLaCoO4 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: 10.17188/1687838
title: Materials Data on KAs3(PbO3)4 by Materials Project

description: KAs3(PbO3)4 crystallizes in the hexagonal P6_3 space group. The structure is three-dimensional. K1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of K–O bond distances ranging from 2.75–3.06 Å. There are two inequivalent Pb2+ sites. In the first Pb2+ site, Pb2+ is bonded to six O2- atoms to form distorted PbO6 pentagonal pyramids that share corners with four equivalent PbO6 pentagonal pyramids, corners with four equivalent AsO4 tetrahedra, and an edgeedge with one AsO4 tetrahedra. There are a spread of Pb–O bond distances ranging from 2.28–2.81 Å. In the second Pb2+ site, Pb2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Pb–O bond distances ranging from 2.46–3.09 Å. As5+ is bonded to four O2- atoms to form AsO4 tetrahedra that share corners with four equivalent PbO6 pentagonal pyramids and an edgeedge with one PbO6 pentagonal pyramid. There are a spread of As–O bond distances ranging from 1.72–1.74 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to one K1+, two Pb2+, and one As5+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to one K1+, two Pb2+, and one As5+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one K1+, two equivalent Pb2+, and one As5+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to three Pb2+ and one As5+ atom.
DOI: 10.17188/1687839
title: Materials Data on YNiGe by Materials Project

description: YNiGe crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Y is bonded in a 12-coordinate geometry to six equivalent Ni and six equivalent Ge atoms. There are a spread of Y–Ni bond distances ranging from 2.95–3.22 Å. There are a spread of Y–Ge bond distances ranging from 2.99–3.17 Å. Ni is bonded in a 10-coordinate geometry to six equivalent Y, one Ni, and three equivalent Ge atoms. The Ni–Ni bond length is 2.72 Å. There are two shorter (2.39 Å) and one longer (2.61 Å) Ni–Ge bond lengths. Ge is bonded in a 10-coordinate geometry to six equivalent Y, three equivalent Ni, and one Ge atom. The Ge–Ge bond length is 2.77 Å.
DOI: 10.17188/1687840
title: Materials Data on CoH2SeO4 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: 10.17188/1687841
title: Materials Data on Li3V6O16 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: 10.17188/1687842
title: Materials Data on LiFeCO4 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: 10.17188/1687843
title: Materials Data on TlMo2Cl7O2 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: 10.17188/1687844
title: Materials Data on MnGeRh by Materials Project

description: MnRhGe crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Mn is bonded in a 11-coordinate geometry to six equivalent Rh and five Ge atoms. There are two shorter (2.84 Å) and four longer (2.97 Å) Mn–Rh bond lengths. All Mn–Ge bond lengths are 2.69 Å. Rh is bonded in a 10-coordinate geometry to six equivalent Mn and four Ge atoms. There are two shorter (2.47 Å) and two longer (2.48 Å) Rh–Ge bond lengths. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to six equivalent Mn and three equivalent Rh atoms. In the second Ge site, Ge is bonded in a 9-coordinate geometry to three equivalent Mn and six equivalent Rh atoms.
DOI: 10.17188/1687845
title: Materials Data on CaSbPd by Materials Project

description: CaPdSb crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ca is bonded in a 12-coordinate geometry to six equivalent Pd and six equivalent Sb atoms. There are a spread of Ca–Pd bond distances ranging from 3.21–3.48 Å. There are a spread of Ca–Sb bond distances ranging from 3.22–3.44 Å. Pd is bonded in a 10-coordinate geometry to six equivalent Ca and four equivalent Sb atoms. There are a spread of Pd–Sb bond distances ranging from 2.72–2.84 Å. Sb is bonded in a 10-coordinate geometry to six equivalent Ca and four equivalent Pd atoms.
DOI: 10.17188/1687846
title: Materials Data on CrN by Materials Project

description: CrN is Tungsten Carbide structured and crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Cr3+ is bonded to six equivalent N3- atoms to form a mixture of distorted edge, corner, and face-sharing CrN6 pentagonal pyramids. All Cr–N bond lengths are 2.02 Å. N3- is bonded to six equivalent Cr3+ atoms to form a mixture of distorted edge, corner, and face-sharing NCr6 pentagonal pyramids.
DOI: 10.17188/1687847
title: Materials Data on Mg16Al12Hg by Materials Project

description: Mg16HgAl12 crystallizes in the trigonal R3m space group. The structure is three-dimensional. there are five inequivalent Mg sites. In the first Mg site, Mg is bonded in a 10-coordinate geometry to four Mg and six Al atoms. There are a spread of Mg–Mg bond distances ranging from 3.05–3.16 Å. There are a spread of Mg–Al bond distances ranging from 3.07–3.12 Å. In the second Mg site, Mg is bonded in a 12-coordinate geometry to seven Mg and five Al atoms. There are a spread of Mg–Mg bond distances ranging from 3.11–3.16 Å. There are a spread of Mg–Al bond distances ranging from 2.99–3.14 Å. In the third Mg site, Mg is bonded in a 1-coordinate geometry to three equivalent Mg, one Hg, and twelve Al atoms. The Mg–Hg bond length is 3.07 Å. There are a spread of Mg–Al bond distances ranging from 3.20–3.24 Å. In the fourth Mg site, Mg is bonded in a 12-coordinate geometry to six Mg, one Hg, and five Al atoms. There are two shorter (3.17 Å) and two longer (3.21 Å) Mg–Mg bond lengths. The Mg–Hg bond length is 2.98 Å. There are a spread of Mg–Al bond distances ranging from 2.97–3.25 Å. In the fifth Mg site, Mg is bonded in a 12-coordinate geometry to seven Mg and five Al atoms. Both Mg–Mg bond lengths are 3.23 Å. There are a spread of Mg–Al bond distances ranging from 2.88–3.17 Å. Hg is bonded in a 10-coordinate geometry to four Mg and six equivalent Al atoms. All Hg–Al bond lengths are 3.12 Å. There are three inequivalent Al sites. In the first Al site, Al is bonded in a 11-coordinate geometry to eight Mg and three Al atoms. There are one shorter (2.69 Å) and two longer (2.75 Å) Al–Al bond lengths. In the second Al site, Al is bonded in a 11-coordinate geometry to eight Mg and three Al atoms. Both Al–Al bond lengths are 2.78 Å. In the third Al site, Al is bonded in a 11-coordinate geometry to seven Mg, one Hg, and three Al atoms. There are one shorter (2.73 Å) and one longer (2.78 Å) Al–Al bond lengths.
DOI: 10.17188/1687848
title: Materials Data on HoGa2Ni3 by Materials Project

description: HoNi3Ga2 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Ho sites. In the first Ho site, Ho is bonded in a 9-coordinate geometry to nine Ni and nine Ga atoms. There are a spread of Ho–Ni bond distances ranging from 3.03–3.10 Å. There are a spread of Ho–Ga bond distances ranging from 3.21–3.26 Å. In the second Ho site, Ho is bonded in a 6-coordinate geometry to twelve Ni atoms. There are a spread of Ho–Ni bond distances ranging from 2.81–3.30 Å. There are five inequivalent Ni sites. In the first Ni site, Ni is bonded in a 11-coordinate geometry to three Ho, four Ni, and four Ga atoms. There are a spread of Ni–Ni bond distances ranging from 2.53–2.94 Å. There are a spread of Ni–Ga bond distances ranging from 2.36–2.45 Å. In the second Ni site, Ni is bonded in a 11-coordinate geometry to three Ho, four Ni, and four Ga atoms. There are two shorter (2.53 Å) and one longer (2.68 Å) Ni–Ni bond lengths. There are a spread of Ni–Ga bond distances ranging from 2.37–2.45 Å. In the third Ni site, Ni is bonded in a 11-coordinate geometry to three Ho, four Ni, and four Ga atoms. There are two shorter (2.53 Å) and one longer (2.95 Å) Ni–Ni bond lengths. There are a spread of Ni–Ga bond distances ranging from 2.36–2.45 Å. In the fourth Ni site, Ni is bonded to four Ho, four equivalent Ni, and four Ga atoms to form a mixture of distorted corner and face-sharing NiHo4Ga4Ni4 cuboctahedra. There are two shorter (2.49 Å) and two longer (2.64 Å) Ni–Ga bond lengths. In the fifth Ni site, Ni is bonded to four Ho, four Ni, and four Ga atoms to form a mixture of distorted corner and face-sharing NiHo4Ga4Ni4 cuboctahedra. There are a spread of Ni–Ga bond distances ranging from 2.48–2.63 Å. There are four inequivalent Ga sites. In the first Ga site, Ga is bonded in a 12-coordinate geometry to four equivalent Ho and six Ni atoms. In the second Ga site, Ga is bonded in a 12-coordinate geometry to four equivalent Ho and six Ni atoms. In the third Ga site, Ga is bonded in a 12-coordinate geometry to two equivalent Ho and six Ni atoms. In the fourth Ga site, Ga is bonded in a 12-coordinate geometry to two equivalent Ho and six Ni atoms.
DOI: 10.17188/1687849
title: Materials Data on Ca3Tb by Materials Project

description: Ca3Tb is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ca is bonded to eight equivalent Ca and four equivalent Tb atoms to form CaCa8Tb4 cuboctahedra that share corners with four equivalent TbCa12 cuboctahedra, corners with fourteen equivalent CaCa8Tb4 cuboctahedra, edges with six equivalent TbCa12 cuboctahedra, edges with twelve equivalent CaCa8Tb4 cuboctahedra, faces with four equivalent TbCa12 cuboctahedra, and faces with sixteen equivalent CaCa8Tb4 cuboctahedra. There are a spread of Ca–Ca bond distances ranging from 3.71–3.87 Å. All Ca–Tb bond lengths are 3.79 Å. Tb is bonded to twelve equivalent Ca atoms to form TbCa12 cuboctahedra that share corners with six equivalent TbCa12 cuboctahedra, corners with twelve equivalent CaCa8Tb4 cuboctahedra, edges with eighteen equivalent CaCa8Tb4 cuboctahedra, faces with eight equivalent TbCa12 cuboctahedra, and faces with twelve equivalent CaCa8Tb4 cuboctahedra.
DOI: 10.17188/1687850
title: Materials Data on Li4TiNi3O8 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: 10.17188/1687851
title: Materials Data on Rb3Y by Materials Project

description: Rb3Y is Uranium Silicide-like structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are two inequivalent Rb sites. In the first Rb site, Rb is bonded to eight Rb and four equivalent Y atoms to form distorted RbRb8Y4 cuboctahedra that share corners with twelve equivalent RbRb8Y4 cuboctahedra, edges with eight equivalent YRb12 cuboctahedra, edges with sixteen RbRb8Y4 cuboctahedra, faces with four equivalent YRb12 cuboctahedra, and faces with fourteen RbRb8Y4 cuboctahedra. There are four shorter (4.45 Å) and four longer (4.59 Å) Rb–Rb bond lengths. All Rb–Y bond lengths are 4.59 Å. In the second Rb site, Rb is bonded to eight equivalent Rb and four equivalent Y atoms to form distorted RbRb8Y4 cuboctahedra that share corners with four equivalent RbRb8Y4 cuboctahedra, corners with eight equivalent YRb12 cuboctahedra, edges with twenty-four RbRb8Y4 cuboctahedra, faces with six equivalent YRb12 cuboctahedra, and faces with twelve RbRb8Y4 cuboctahedra. All Rb–Y bond lengths are 4.45 Å. Y is bonded to twelve Rb atoms to form YRb12 cuboctahedra that share corners with four equivalent YRb12 cuboctahedra, corners with eight equivalent RbRb8Y4 cuboctahedra, edges with eight equivalent YRb12 cuboctahedra, edges with sixteen equivalent RbRb8Y4 cuboctahedra, faces with four equivalent YRb12 cuboctahedra, and faces with fourteen RbRb8Y4 cuboctahedra.