cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1678050
title: Materials Data on Gd(Co5Mo)2 by Materials Project

description: Gd(MoCo5)2 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Gd is bonded in a 12-coordinate geometry to two equivalent Mo and eighteen Co atoms. Both Gd–Mo bond lengths are 3.04 Å. There are a spread of Gd–Co bond distances ranging from 2.96–3.22 Å. Mo is bonded in a 10-coordinate geometry to one Gd, one Mo, and twelve Co atoms. The Mo–Mo bond length is 2.41 Å. There are a spread of Mo–Co bond distances ranging from 2.59–2.90 Å. There are four inequivalent Co sites. In the first Co site, Co is bonded to two equivalent Gd, two equivalent Mo, and eight Co atoms to form a mixture of distorted edge, face, and corner-sharing CoGd2Co8Mo2 cuboctahedra. There are a spread of Co–Co bond distances ranging from 2.45–2.66 Å. In the second Co site, Co is bonded in a 12-coordinate geometry to two equivalent Gd, two equivalent Mo, and eight Co atoms. There are four shorter (2.44 Å) and two longer (2.66 Å) Co–Co bond lengths. In the third Co site, Co is bonded to two equivalent Gd, two equivalent Mo, and eight Co atoms to form a mixture of distorted edge, face, and corner-sharing CoGd2Co8Mo2 cuboctahedra. There are two shorter (2.35 Å) and two longer (2.60 Å) Co–Co bond lengths. In the fourth Co site, Co is bonded in a 2-coordinate geometry to one Gd, four equivalent Mo, and nine Co atoms. The Co–Co bond length is 2.39 Å.
DOI: 10.17188/1678051
title: Materials Data on ZrGeRh by Materials Project

description: ZrRhGe crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Zr is bonded in a 11-coordinate geometry to six equivalent Rh and five equivalent Ge atoms. There are a spread of Zr–Rh bond distances ranging from 2.98–3.15 Å. There are a spread of Zr–Ge bond distances ranging from 2.84–2.87 Å. Rh is bonded in a 12-coordinate geometry to six equivalent Zr and four equivalent Ge atoms. There are a spread of Rh–Ge bond distances ranging from 2.52–2.56 Å. Ge is bonded in a 9-coordinate geometry to five equivalent Zr and four equivalent Rh atoms.
DOI: 10.17188/1678052
title: Materials Data on Na2AgMoF6 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: 10.17188/1678054
title: Materials Data on Al(SiO3)2 by Materials Project

description: Al(SiO3)2 is Low Tridymite-derived structured and crystallizes in the tetragonal P4_32_12 space group. The structure is three-dimensional. Al is bonded to four O atoms to form AlO4 tetrahedra that share corners with four equivalent SiO4 tetrahedra. There is two shorter (1.74 Å) and two longer (1.75 Å) Al–O bond length. Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with two equivalent AlO4 tetrahedra and corners with two equivalent SiO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.62–1.64 Å. There are three inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to one Al and one Si atom. In the second O site, O is bonded in a linear geometry to one Al and one Si atom. In the third O site, O is bonded in a bent 150 degrees geometry to two equivalent Si atoms.
DOI: 10.17188/1678055
title: Materials Data on Nb2CrRe by Materials Project

description: Nb2CrRe crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Nb2CrRe ribbons oriented in the (1, 0, 0) direction. Nb is bonded in a linear geometry to one Cr and one Re atom. The Nb–Cr bond length is 2.63 Å. The Nb–Re bond length is 2.24 Å. Cr is bonded in a linear geometry to two equivalent Nb atoms. Re is bonded in a linear geometry to two equivalent Nb atoms.
DOI: 10.17188/1678056
title: Materials Data on NdSi3Rh by Materials Project

description: NdRhSi3 crystallizes in the tetragonal I4mm space group. The structure is three-dimensional. Nd is bonded in a 12-coordinate geometry to five equivalent Rh and twelve Si atoms. There are four shorter (3.37 Å) and one longer (3.41 Å) Nd–Rh bond lengths. There are a spread of Nd–Si bond distances ranging from 3.12–3.36 Å. Rh is bonded in a 5-coordinate geometry to five equivalent Nd and five Si atoms. There are four shorter (2.37 Å) and one longer (2.39 Å) Rh–Si bond lengths. There are two inequivalent Si sites. In the first Si site, Si is bonded in a distorted single-bond geometry to four equivalent Nd, one Rh, and four equivalent Si atoms. All Si–Si bond lengths are 2.60 Å. In the second Si site, Si is bonded in a distorted bent 120 degrees geometry to four equivalent Nd, two equivalent Rh, and two equivalent Si atoms.
DOI: 10.17188/1678057
title: Materials Data on K2PdN2(ClO2)2 by Materials Project

description: K2PdN2(O2Cl)2 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. K1+ is bonded to five O2- and three equivalent Cl1- atoms to form distorted edge-sharing KCl3O5 hexagonal bipyramids. There are a spread of K–O bond distances ranging from 2.88–3.12 Å. There are a spread of K–Cl bond distances ranging from 3.18–3.23 Å. Pd2+ is bonded in a distorted square co-planar geometry to two equivalent N3+ and two equivalent Cl1- atoms. Both Pd–N bond lengths are 2.06 Å. Both Pd–Cl bond lengths are 2.33 Å. N3+ is bonded in a distorted bent 120 degrees geometry to one Pd2+ and two O2- atoms. There is one shorter (1.25 Å) and one longer (1.26 Å) N–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to three equivalent K1+ and one N3+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent K1+ and one N3+ atom. Cl1- is bonded in a 4-coordinate geometry to three equivalent K1+ and one Pd2+ atom.
DOI: 10.17188/1678058
title: Materials Data on H5W by Materials Project

description: WH5 crystallizes in the orthorhombic Pma2 space group. The structure is two-dimensional and consists of one WH5 sheet oriented in the (0, 1, 0) direction. W3+ is bonded in a 12-coordinate geometry to ten H+0.60- atoms. There are a spread of W–H bond distances ranging from 1.76–2.05 Å. There are three inequivalent H+0.60- sites. In the first H+0.60- site, H+0.60- is bonded in a water-like geometry to two equivalent W3+ atoms. In the second H+0.60- site, H+0.60- is bonded in a water-like geometry to two equivalent W3+ atoms. In the third H+0.60- site, H+0.60- is bonded in a 1-coordinate geometry to two equivalent W3+ atoms.
DOI: 10.17188/1678059
title: Materials Data on Li3Cu(NiO2)4 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1678060
title: Materials Data on BaSrI4 by Materials Project

description: BaSrI4 is Hydrophilite-derived structured and crystallizes in the orthorhombic Pnna space group. The structure is three-dimensional. Ba2+ is bonded to six I1- atoms to form distorted BaI6 pentagonal pyramids that share corners with eight equivalent SrI6 octahedra and edges with two equivalent BaI6 pentagonal pyramids. The corner-sharing octahedra tilt angles range from 32–69°. There are a spread of Ba–I bond distances ranging from 3.39–3.56 Å. Sr2+ is bonded to six I1- atoms to form SrI6 octahedra that share corners with eight equivalent BaI6 pentagonal pyramids and edges with two equivalent SrI6 octahedra. There are a spread of Sr–I bond distances ranging from 3.26–3.37 Å. There are two inequivalent I1- sites. In the first I1- site, I1- is bonded in a 3-coordinate geometry to two equivalent Ba2+ and one Sr2+ atom. In the second I1- site, I1- is bonded in a distorted trigonal planar geometry to one Ba2+ and two equivalent Sr2+ atoms.
DOI: 10.17188/1678061
title: Materials Data on LiCoPO4 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: 10.17188/1678062
title: Materials Data on Li5Co5O9F 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: 10.17188/1678063
title: Materials Data on Li5Cr3NiO8 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: 10.17188/1678065
title: Materials Data on CoSnH12(OF)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: 10.17188/1678066
title: Materials Data on Sm(CrB3)2 by Materials Project

description: Sm(CrB3)2 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Sm2+ is bonded in a 12-coordinate geometry to sixteen B1- atoms. There are a spread of Sm–B bond distances ranging from 2.81–2.96 Å. Cr2+ is bonded in a 10-coordinate geometry to ten B1- atoms. There are a spread of Cr–B bond distances ranging from 2.12–2.22 Å. There are two inequivalent B1- sites. In the first B1- site, B1- is bonded in a 6-coordinate geometry to three equivalent Sm2+, three equivalent Cr2+, and three B1- atoms. There is one shorter (1.76 Å) and two longer (1.79 Å) B–B bond length. In the second B1- site, B1- is bonded in a 9-coordinate geometry to two equivalent Sm2+, four equivalent Cr2+, and three B1- atoms. The B–B bond length is 1.84 Å.
DOI: 10.17188/1678068
title: Materials Data on Li3Cr3(PO4)4 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1678069
title: Materials Data on PaSb3 by Materials Project

description: PaSb3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Pa3+ is bonded to twelve equivalent Sb1- atoms to form a mixture of face and corner-sharing PaSb12 cuboctahedra. There are six shorter (3.18 Å) and six longer (3.49 Å) Pa–Sb bond lengths. Sb1- is bonded in a 2-coordinate geometry to four equivalent Pa3+ and four equivalent Sb1- atoms. There are two shorter (3.09 Å) and two longer (3.27 Å) Sb–Sb bond lengths.
DOI: 10.17188/1678070
title: Materials Data on La2(MoO4)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: 10.17188/1678071
title: Materials Data on CsBa2Cr2F11 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: 10.17188/1678072
title: Materials Data on Cs2AlAuBr6 by Materials Project

description: Cs2AuAlBr6 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 AuBr6 octahedra, and faces with four equivalent AlBr6 octahedra. All Cs–Br bond lengths are 3.87 Å. Au1+ is bonded to six equivalent Br1- atoms to form AuBr6 octahedra that share corners with six equivalent AlBr6 octahedra and faces with eight equivalent CsBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Au–Br bond lengths are 2.90 Å. Al3+ is bonded to six equivalent Br1- atoms to form AlBr6 octahedra that share corners with six equivalent AuBr6 octahedra and faces with eight equivalent CsBr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Al–Br bond lengths are 2.57 Å. Br1- is bonded in a 6-coordinate geometry to four equivalent Cs1+, one Au1+, and one Al3+ atom.
DOI: 10.17188/1678074
title: Materials Data on Sn(ClO)2 by Materials Project

description: SnCl2O2 crystallizes in the monoclinic P2_1/c space group. The structure is two-dimensional and consists of four hydrogen peroxide molecules and one SnCl2 sheet oriented in the (1, 0, 0) direction. In the SnCl2 sheet, Sn is bonded in a rectangular see-saw-like geometry to four Cl atoms. There are a spread of Sn–Cl bond distances ranging from 2.62–2.97 Å. There are two inequivalent Cl sites. In the first Cl site, Cl is bonded in a water-like geometry to two equivalent Sn atoms. In the second Cl site, Cl is bonded in a bent 120 degrees geometry to two equivalent Sn atoms.
DOI: 10.17188/1678075
title: Materials Data on LiMnVP2(HO5)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: 10.17188/1678076
title: Materials Data on Ba3V2(PO5)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: 10.17188/1678077
title: Materials Data on Li3NiF6 by Materials Project

description: Li3NiF6 crystallizes in the orthorhombic Pna2_1 space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.90–2.47 Å. In the second Li1+ site, Li1+ is bonded to six F1- atoms to form distorted LiF6 octahedra that share corners with two equivalent LiF6 octahedra, corners with two equivalent NiF6 octahedra, and edges with two equivalent NiF6 octahedra. The corner-sharing octahedra tilt angles range from 46–56°. There are a spread of Li–F bond distances ranging from 1.95–2.26 Å. In the third Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.91–2.48 Å. Ni3+ is bonded to six F1- atoms to form NiF6 octahedra that share corners with two equivalent LiF6 octahedra and edges with two equivalent LiF6 octahedra. The corner-sharing octahedra tilt angles range from 54–56°. There are a spread of Ni–F bond distances ranging from 1.91–1.95 Å. There are six inequivalent F1- sites. In the first F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one Ni3+ atom. In the second F1- site, F1- is bonded to three Li1+ and one Ni3+ atom to form a mixture of distorted corner and edge-sharing FLi3Ni trigonal pyramids. In the third F1- site, F1- is bonded in a 5-coordinate geometry to four Li1+ and one Ni3+ atom. In the fourth F1- site, F1- is bonded to three Li1+ and one Ni3+ atom to form a mixture of distorted corner and edge-sharing FLi3Ni trigonal pyramids. In the fifth F1- site, F1- is bonded in a trigonal planar geometry to two equivalent Li1+ and one Ni3+ atom. In the sixth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one Ni3+ atom.
DOI: 10.17188/1678078
title: Materials Data on Zr6Ga2Fe by Materials Project

description: Zr6FeGa2 crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. there are two inequivalent Zr sites. In the first Zr site, Zr is bonded in a 2-coordinate geometry to two equivalent Fe and two equivalent Ga atoms. Both Zr–Fe bond lengths are 2.58 Å. Both Zr–Ga bond lengths are 3.02 Å. In the second Zr site, Zr is bonded in a 5-coordinate geometry to one Fe and four equivalent Ga atoms. The Zr–Fe bond length is 3.16 Å. All Zr–Ga bond lengths are 2.94 Å. Fe is bonded in a 6-coordinate geometry to nine Zr atoms. Ga is bonded in a 9-coordinate geometry to nine Zr atoms.
DOI: 10.17188/1678081
title: Materials Data on Ba2VP2O9 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: 10.17188/1678082
title: Materials Data on Li3MnV(PO4)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: 10.17188/1678083
title: Materials Data on TmMnO3 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: 10.17188/1678084
title: Materials Data on Pr2FeAs2RuO2 by Materials Project

description: Pr2RuFeAs2O2 crystallizes in the tetragonal P-4m2 space group. The structure is three-dimensional. Pr3+ is bonded in a 4-coordinate geometry to four equivalent As3- and four equivalent O2- atoms. All Pr–As bond lengths are 3.36 Å. All Pr–O bond lengths are 2.36 Å. Ru2+ is bonded to four equivalent As3- atoms to form RuAs4 tetrahedra that share corners with four equivalent RuAs4 tetrahedra and edges with four equivalent FeAs4 tetrahedra. All Ru–As bond lengths are 2.53 Å. Fe2+ is bonded to four equivalent As3- atoms to form FeAs4 tetrahedra that share corners with four equivalent FeAs4 tetrahedra and edges with four equivalent RuAs4 tetrahedra. All Fe–As bond lengths are 2.53 Å. As3- is bonded in a 2-coordinate geometry to four equivalent Pr3+, two equivalent Ru2+, and two equivalent Fe2+ atoms. O2- is bonded to four equivalent Pr3+ atoms to form a mixture of corner and edge-sharing OPr4 tetrahedra.
DOI: 10.17188/1678085
title: Materials Data on AgS8N9(ClO6)2 by Materials Project

description: (NAgN)2N2(NS2)4(N2S2O6Cl)4 crystallizes in the tetragonal I-42d space group. The structure is zero-dimensional and consists of four ammonia molecules, eight N2S2O6Cl clusters, four NAgN clusters, and eight NS2 clusters. In each N2S2O6Cl cluster, N+4.56+ is bonded in a distorted bent 150 degrees geometry to one S2- and one Cl1- atom. The N–S bond length is 1.80 Å. The N–Cl bond length is 1.55 Å. S2- is bonded in a distorted tetrahedral geometry to one N+4.56+ and three O2- atoms. There is two shorter (1.45 Å) and one longer (1.46 Å) S–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the second O2- site, O2- is bonded in a single-bond geometry to one S2- atom. In the third O2- site, O2- is bonded in a single-bond geometry to one S2- atom. Cl1- is bonded in a bent 150 degrees geometry to two equivalent N+4.56+ atoms. In each NAgN cluster, Ag1+ is bonded in a linear geometry to two equivalent N+4.56+ atoms. Both Ag–N bond lengths are 2.09 Å. N+4.56+ is bonded in a single-bond geometry to one Ag1+ atom. In each NS2 cluster, N+4.56+ is bonded in a linear geometry to two equivalent S2- atoms. Both N–S bond lengths are 1.50 Å. S2- is bonded in a distorted single-bond geometry to one N+4.56+ atom.
DOI: 10.17188/1678086
title: Materials Data on ErTc2 by Materials Project

description: ErTc2 is Hexagonal Laves structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Er is bonded in a 12-coordinate geometry to twelve Tc atoms. There are a spread of Er–Tc bond distances ranging from 3.14–3.16 Å. There are two inequivalent Tc sites. In the first Tc site, Tc is bonded to six equivalent Er and six equivalent Tc atoms to form a mixture of edge, corner, and face-sharing TcEr6Tc6 cuboctahedra. All Tc–Tc bond lengths are 2.73 Å. In the second Tc site, Tc is bonded to six equivalent Er and six Tc atoms to form a mixture of edge, corner, and face-sharing TcEr6Tc6 cuboctahedra. There are two shorter (2.60 Å) and two longer (2.76 Å) Tc–Tc bond lengths.
DOI: 10.17188/1678087
title: Materials Data on Al4CdO7 by Materials Project

description: CdAl4O7 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Cd2+ is bonded to five O2- atoms to form CdO5 trigonal bipyramids that share corners with ten AlO4 tetrahedra. There are a spread of Cd–O bond distances ranging from 2.29–2.38 Å. There are two inequivalent Al3+ sites. In the first Al3+ site, Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with five AlO4 tetrahedra and corners with three equivalent CdO5 trigonal bipyramids. There are a spread of Al–O bond distances ranging from 1.76–1.82 Å. In the second Al3+ site, Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with six AlO4 tetrahedra and corners with two equivalent CdO5 trigonal bipyramids. There are a spread of Al–O bond distances ranging from 1.75–1.82 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to one Cd2+ and two equivalent Al3+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to one Cd2+ and two equivalent Al3+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one Cd2+ and two Al3+ atoms. In the fourth O2- site, O2- is bonded in a trigonal planar geometry to three Al3+ atoms.
DOI: 10.17188/1678088
title: Materials Data on Dy3Ni11Ge4 by Materials Project

description: Dy3Ni11Ge4 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Dy is bonded in a 1-coordinate geometry to ten Ni and five Ge atoms. There are a spread of Dy–Ni bond distances ranging from 2.91–3.00 Å. There are one shorter (2.82 Å) and four longer (3.09 Å) Dy–Ge bond lengths. There are three inequivalent Ni sites. In the first Ni site, Ni is bonded in a 12-coordinate geometry to three equivalent Dy, six Ni, and three Ge atoms. There are a spread of Ni–Ni bond distances ranging from 2.56–2.80 Å. There are two shorter (2.59 Å) and one longer (2.64 Å) Ni–Ge bond lengths. In the second Ni site, Ni is bonded in a 12-coordinate geometry to two equivalent Dy, eight Ni, and two equivalent Ge atoms. There are two shorter (2.52 Å) and two longer (2.56 Å) Ni–Ni bond lengths. Both Ni–Ge bond lengths are 2.34 Å. In the third Ni site, Ni is bonded in a 12-coordinate geometry to three equivalent Dy, six Ni, and three equivalent Ge atoms. All Ni–Ge bond lengths are 2.40 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to three equivalent Dy and six equivalent Ni atoms. In the second Ge site, Ge is bonded to four equivalent Dy and eight Ni atoms to form a mixture of distorted corner and face-sharing GeDy4Ni8 cuboctahedra.