cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1720390
title: Materials Data on GdUAl4 by Materials Project

description: UGdAl4 is Hexagonal Laves-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. U is bonded in a 12-coordinate geometry to four equivalent Gd and twelve equivalent Al atoms. All U–Gd bond lengths are 3.39 Å. All U–Al bond lengths are 3.25 Å. Gd is bonded in a 12-coordinate geometry to four equivalent U and twelve equivalent Al atoms. All Gd–Al bond lengths are 3.25 Å. Al is bonded to three equivalent U, three equivalent Gd, and six equivalent Al atoms to form a mixture of face, edge, and corner-sharing AlGd3U3Al6 cuboctahedra. There are three shorter (2.76 Å) and three longer (2.78 Å) Al–Al bond lengths.
DOI: 10.17188/1720392
title: Materials Data on Ba2NaLi by Materials Project

description: NaLiBa2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two NaLiBa2 ribbons oriented in the (0, 1, 0) direction. Na is bonded in a linear geometry to two equivalent Ba atoms. Both Na–Ba bond lengths are 4.00 Å. Li is bonded in a linear geometry to two equivalent Ba atoms. Both Li–Ba bond lengths are 3.80 Å. Ba is bonded in a linear geometry to one Na and one Li atom.
DOI: 10.17188/1720395
title: Materials Data on YBiO12 by Materials Project

description: YO12Bi crystallizes in the cubic Fd-3m space group. The structure is three-dimensional and consists of eight bismuth molecules and one YO12 framework. In the YO12 framework, Y is bonded in a cuboctahedral geometry to twelve equivalent O atoms. All Y–O bond lengths are 2.55 Å. O is bonded in a 3-coordinate geometry to one Y and two equivalent O atoms. Both O–O bond lengths are 1.69 Å.
DOI: 10.17188/1720396
title: Materials Data on ZnO 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: 10.17188/1720397
title: Materials Data on Li3Al2VO6 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: 10.17188/1720398
title: Materials Data on Ce(BRh)4 by Materials Project

description: Ce(RhB)4 crystallizes in the tetragonal P4_2/nmc space group. The structure is three-dimensional. Ce is bonded in a 12-coordinate geometry to twelve equivalent Rh and twelve equivalent B atoms. There are four shorter (2.99 Å) and eight longer (3.18 Å) Ce–Rh bond lengths. There are eight shorter (3.04 Å) and four longer (3.17 Å) Ce–B bond lengths. Rh is bonded in a 5-coordinate geometry to three equivalent Ce and five equivalent B atoms. There are a spread of Rh–B bond distances ranging from 2.22–2.27 Å. B is bonded in a 6-coordinate geometry to three equivalent Ce, five equivalent Rh, and one B atom. The B–B bond length is 1.79 Å.
DOI: 10.6084/m9.figshare.13661315.v5
title: Acoustic diversity dataset

description: Dataset and code for "<i>A machine learning approach for classifying and quantifying acoustic diversity</i>"<br><b></b>
DOI: 10.17188/1720399
title: Materials Data on MgTi by Materials Project

description: MgTi crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. there are three inequivalent Mg sites. In the first Mg site, Mg is bonded to seven Mg and five Ti atoms to form distorted MgMg7Ti5 cuboctahedra that share corners with four equivalent TiMg4Ti8 cuboctahedra, corners with eight MgMg7Ti5 cuboctahedra, edges with seven equivalent TiMg4Ti8 cuboctahedra, edges with eight MgMg7Ti5 cuboctahedra, a faceface with one TiMg4Ti8 cuboctahedra, and faces with eleven MgMg7Ti5 cuboctahedra. There are a spread of Mg–Mg bond distances ranging from 3.01–3.18 Å. There are a spread of Mg–Ti bond distances ranging from 3.07–3.33 Å. In the second Mg site, Mg is bonded to seven Mg and five Ti atoms to form distorted MgMg7Ti5 cuboctahedra that share corners with two equivalent TiMg4Ti8 cuboctahedra, corners with ten MgMg7Ti5 cuboctahedra, edges with four equivalent TiMg4Ti8 cuboctahedra, edges with eleven MgMg7Ti5 cuboctahedra, faces with three equivalent TiMg4Ti8 cuboctahedra, and faces with nine MgMg7Ti5 cuboctahedra. There are two shorter (2.98 Å) and one longer (3.04 Å) Mg–Mg bond lengths. There are a spread of Mg–Ti bond distances ranging from 3.08–3.20 Å. In the third Mg site, Mg is bonded to four Mg and eight Ti atoms to form distorted MgMg4Ti8 cuboctahedra that share corners with four equivalent TiMg4Ti8 cuboctahedra, corners with eight MgMg7Ti5 cuboctahedra, edges with eleven MgMg7Ti5 cuboctahedra, faces with six equivalent TiMg4Ti8 cuboctahedra, and faces with eight MgMg7Ti5 cuboctahedra. Both Mg–Mg bond lengths are 3.00 Å. There are a spread of Mg–Ti bond distances ranging from 3.01–3.15 Å. There are three inequivalent Ti sites. In the first Ti site, Ti is bonded in a 12-coordinate geometry to seven Mg and four Ti atoms. There are a spread of Ti–Ti bond distances ranging from 2.73–2.87 Å. In the second Ti site, Ti is bonded in a 12-coordinate geometry to seven Mg and four Ti atoms. There are one shorter (2.71 Å) and two longer (2.87 Å) Ti–Ti bond lengths. In the third Ti site, Ti is bonded to four Mg and eight Ti atoms to form TiMg4Ti8 cuboctahedra that share corners with two equivalent TiMg4Ti8 cuboctahedra, corners with ten MgMg7Ti5 cuboctahedra, edges with eleven MgMg7Ti5 cuboctahedra, faces with four equivalent TiMg4Ti8 cuboctahedra, and faces with ten MgMg7Ti5 cuboctahedra. Both Ti–Ti bond lengths are 2.87 Å.
DOI: 10.17188/1720400
title: Materials Data on Mg2Nb2VO8 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: 10.17188/1720401
title: Materials Data on Li2CrO3 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: 10.17188/1720402
title: Materials Data on MnH16C4S4(N4Cl)2 by Materials Project

description: MnC4H16S4(N4Cl)2 is Tungsten structured and crystallizes in the tetragonal P4_2/n space group. The structure is zero-dimensional and consists of four MnC4H16S4(N4Cl)2 clusters. Mn2+ is bonded in an octahedral geometry to four S2- and two equivalent Cl1- atoms. There are two shorter (2.56 Å) and two longer (2.66 Å) Mn–S bond lengths. Both Mn–Cl bond lengths are 2.58 Å. There are two inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a distorted trigonal planar geometry to two N3- and one S2- atom. Both C–N bond lengths are 1.34 Å. The C–S bond length is 1.71 Å. In the second C4+ site, C4+ is bonded in a distorted trigonal planar geometry to two N3- and one S2- atom. Both C–N bond lengths are 1.34 Å. The C–S bond length is 1.72 Å. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded in a trigonal planar geometry to one C4+ and two H1+ atoms. Both N–H bond lengths are 1.02 Å. In the second N3- site, N3- is bonded in a trigonal planar geometry to one C4+ and two H1+ atoms. There is one shorter (1.01 Å) and one longer (1.02 Å) N–H bond length. In the third N3- site, N3- is bonded in a trigonal planar geometry to one C4+ and two H1+ atoms. Both N–H bond lengths are 1.02 Å. In the fourth N3- site, N3- is bonded in a trigonal planar geometry to one C4+ and two H1+ atoms. Both N–H bond lengths are 1.02 Å. There are eight inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the eighth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C4+ atom. In the second S2- site, S2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C4+ atom. Cl1- is bonded in a single-bond geometry to one Mn2+ atom.
DOI: 10.17188/1720403
title: Materials Data on Bi(W3O10)6 by Materials Project

description: Bi(W3O10)6 is beta Polonium structured and crystallizes in the trigonal R3 space group. The structure is zero-dimensional and consists of three Bi(W3O10)6 clusters. there are six inequivalent W sites. In the first W site, W is bonded in a 5-coordinate geometry to six O atoms. There are a spread of W–O bond distances ranging from 1.72–2.64 Å. In the second W site, W is bonded in a 6-coordinate geometry to six O atoms. There are a spread of W–O bond distances ranging from 1.73–2.40 Å. In the third W site, W is bonded in a 6-coordinate geometry to six O atoms. There are a spread of W–O bond distances ranging from 1.73–2.38 Å. In the fourth W site, W is bonded in a 6-coordinate geometry to six O atoms. There are a spread of W–O bond distances ranging from 1.73–2.27 Å. In the fifth W site, W is bonded in a 6-coordinate geometry to six O atoms. There are a spread of W–O bond distances ranging from 1.73–2.35 Å. In the sixth W site, W is bonded in a 6-coordinate geometry to six O atoms. There are a spread of W–O bond distances ranging from 1.73–2.25 Å. Bi is bonded in a distorted T-shaped geometry to three equivalent O atoms. All Bi–O bond lengths are 2.18 Å. There are twenty inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one W atom. In the second O site, O is bonded in a single-bond geometry to one W atom. In the third O site, O is bonded in a bent 120 degrees geometry to two W atoms. In the fourth O site, O is bonded in a bent 120 degrees geometry to two W atoms. In the fifth O site, O is bonded in a bent 120 degrees geometry to two W atoms. In the sixth O site, O is bonded in a bent 120 degrees geometry to two W atoms. In the seventh O site, O is bonded in a single-bond geometry to one W atom. In the eighth O site, O is bonded in a single-bond geometry to one W atom. In the ninth O site, O is bonded in a single-bond geometry to one W atom. In the tenth O site, O is bonded in a single-bond geometry to one W atom. In the eleventh O site, O is bonded in a bent 120 degrees geometry to two W atoms. In the twelfth O site, O is bonded in a bent 120 degrees geometry to two W atoms. In the thirteenth O site, O is bonded in a bent 150 degrees geometry to two W atoms. In the fourteenth O site, O is bonded in a bent 150 degrees geometry to two W atoms. In the fifteenth O site, O is bonded in a bent 150 degrees geometry to two equivalent W atoms. In the sixteenth O site, O is bonded in a bent 150 degrees geometry to two equivalent W atoms. In the seventeenth O site, O is bonded in a bent 150 degrees geometry to two W atoms. In the eighteenth O site, O is bonded in a bent 150 degrees geometry to two W atoms. In the nineteenth O site, O is bonded in a 4-coordinate geometry to three W and one Bi atom. In the twentieth O site, O is bonded in a distorted trigonal non-coplanar geometry to three W atoms.
DOI: 10.17188/1720404
title: Materials Data on Y2Cu3(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: 10.17188/1720405
title: Materials Data on ZrCrCuS4 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: 10.17188/1720406
title: Materials Data on Eu2GaHg by Materials Project

description: Eu2HgGa is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Eu is bonded in a body-centered cubic geometry to four equivalent Hg and four equivalent Ga atoms. All Eu–Hg bond lengths are 3.33 Å. All Eu–Ga bond lengths are 3.33 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Eu atoms. Ga is bonded in a body-centered cubic geometry to eight equivalent Eu atoms.
DOI: 10.17188/1720407
title: Materials Data on CrPO4 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: 10.17188/1720408
title: Materials Data on Li2Mg by Materials Project

description: MgLi2 is beta-derived structured and crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. there are three inequivalent Li sites. In the first Li site, Li is bonded to twelve Li atoms to form LiLi12 cuboctahedra that share corners with six equivalent MgLi3Mg9 cuboctahedra, corners with twelve LiLi12 cuboctahedra, edges with eighteen LiLi12 cuboctahedra, a faceface with one MgLi3Mg9 cuboctahedra, and faces with nineteen LiLi12 cuboctahedra. There are a spread of Li–Li bond distances ranging from 3.01–3.16 Å. In the second Li site, Li is bonded to nine Li and three equivalent Mg atoms to form distorted LiLi9Mg3 cuboctahedra that share corners with six equivalent MgLi3Mg9 cuboctahedra, corners with twelve LiLi9Mg3 cuboctahedra, edges with six equivalent MgLi3Mg9 cuboctahedra, edges with twelve LiLi12 cuboctahedra, faces with seven equivalent MgLi3Mg9 cuboctahedra, and faces with thirteen LiLi12 cuboctahedra. All Li–Li bond lengths are 3.16 Å. All Li–Mg bond lengths are 3.05 Å. In the third Li site, Li is bonded to twelve Li atoms to form LiLi12 cuboctahedra that share corners with six equivalent MgLi3Mg9 cuboctahedra, corners with twelve LiLi9Mg3 cuboctahedra, edges with eighteen LiLi12 cuboctahedra, a faceface with one MgLi3Mg9 cuboctahedra, and faces with nineteen LiLi12 cuboctahedra. There are three shorter (3.01 Å) and six longer (3.16 Å) Li–Li bond lengths. Mg is bonded to three equivalent Li and nine equivalent Mg atoms to form distorted MgLi3Mg9 cuboctahedra that share corners with six equivalent MgLi3Mg9 cuboctahedra, corners with twelve LiLi12 cuboctahedra, edges with six equivalent LiLi9Mg3 cuboctahedra, edges with twelve equivalent MgLi3Mg9 cuboctahedra, faces with eight LiLi12 cuboctahedra, and faces with twelve equivalent MgLi3Mg9 cuboctahedra. All Mg–Mg bond lengths are 3.16 Å.
DOI: 10.17188/1720409
title: Materials Data on Li2NiGeO4 by Materials Project

description: Li2NiGeO4 is Stannite-like structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with two equivalent LiO4 tetrahedra, corners with four equivalent NiO4 tetrahedra, corners with four equivalent GeO4 tetrahedra, and an edgeedge with one LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.02 Å. Ni2+ is bonded to four O2- atoms to form NiO4 tetrahedra that share corners with four equivalent GeO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. There is two shorter (1.99 Å) and two longer (2.00 Å) Ni–O bond length. Ge4+ is bonded to four O2- atoms to form GeO4 tetrahedra that share corners with four equivalent NiO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. There is two shorter (1.78 Å) and two longer (1.79 Å) Ge–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Li1+, one Ni2+, and one Ge4+ atom to form a mixture of distorted edge and corner-sharing OLi2NiGe tetrahedra. In the second O2- site, O2- is bonded to two equivalent Li1+, one Ni2+, and one Ge4+ atom to form corner-sharing OLi2NiGe tetrahedra. In the third O2- site, O2- is bonded to two equivalent Li1+, one Ni2+, and one Ge4+ atom to form corner-sharing OLi2NiGe tetrahedra.
DOI: 10.17188/1720410
title: Materials Data on Zr6FeS2 by Materials Project

description: Zr6FeS2 crystallizes in the orthorhombic Pnnm space group. The structure is three-dimensional. there are six inequivalent Zr sites. In the first Zr site, Zr is bonded in a 3-coordinate geometry to one Fe and two S atoms. The Zr–Fe bond length is 2.97 Å. There are one shorter (2.80 Å) and one longer (2.94 Å) Zr–S bond lengths. In the second Zr site, Zr is bonded in a 4-coordinate geometry to one Fe and four S atoms. The Zr–Fe bond length is 3.23 Å. All Zr–S bond lengths are 2.65 Å. In the third Zr site, Zr is bonded in a 3-coordinate geometry to two equivalent Fe and one S atom. Both Zr–Fe bond lengths are 2.60 Å. The Zr–S bond length is 2.84 Å. In the fourth Zr site, Zr is bonded in a 4-coordinate geometry to two equivalent Fe and two equivalent S atoms. Both Zr–Fe bond lengths are 2.64 Å. Both Zr–S bond lengths are 2.76 Å. In the fifth Zr site, Zr is bonded to two equivalent Fe and three S atoms to form distorted edge-sharing ZrFe2S3 trigonal bipyramids. Both Zr–Fe bond lengths are 2.63 Å. There are one shorter (2.68 Å) and two longer (2.74 Å) Zr–S bond lengths. In the sixth Zr site, Zr is bonded in a 3-coordinate geometry to one Fe and three S atoms. The Zr–Fe bond length is 3.13 Å. There are one shorter (2.66 Å) and two longer (2.70 Å) Zr–S bond lengths. Fe is bonded in a 6-coordinate geometry to nine Zr atoms. There are two inequivalent S sites. In the first S site, S is bonded in a 7-coordinate geometry to seven Zr atoms. In the second S site, S is bonded in a 8-coordinate geometry to eight Zr atoms.
DOI: 10.17188/1720411
title: Materials Data on SmSbTe3 by Materials Project

description: SmSbTe3 is Calaverite-derived structured and crystallizes in the trigonal R3m space group. The structure is two-dimensional and consists of three SmSbTe3 sheets oriented in the (0, 0, 1) direction. Sm3+ is bonded to six Te2- atoms to form SmTe6 octahedra that share corners with three equivalent SbTe6 octahedra, edges with three equivalent SbTe6 octahedra, and edges with six equivalent SmTe6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (3.06 Å) and three longer (3.25 Å) Sm–Te bond lengths. Sb3+ is bonded to six Te2- atoms to form SbTe6 octahedra that share corners with three equivalent SmTe6 octahedra, edges with three equivalent SmTe6 octahedra, and edges with six equivalent SbTe6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (3.02 Å) and three longer (3.29 Å) Sb–Te bond lengths. There are three inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Sm3+ atoms. In the second Te2- site, Te2- is bonded in a 3-coordinate geometry to three equivalent Sb3+ atoms. In the third Te2- site, Te2- is bonded to three equivalent Sm3+ and three equivalent Sb3+ atoms to form distorted edge-sharing TeSm3Sb3 octahedra.
DOI: 10.17188/1720412
title: Materials Data on Mn3Co2Sb(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: 10.17188/1720413
title: Materials Data on Ti3N4 by Materials Project

description: Ti3N4 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are two inequivalent Ti4+ sites. In the first Ti4+ site, Ti4+ is bonded to six N3- atoms to form a mixture of edge and corner-sharing TiN6 octahedra. The corner-sharing octahedra tilt angles range from 0–5°. There are four shorter (2.08 Å) and two longer (2.10 Å) Ti–N bond lengths. In the second Ti4+ site, Ti4+ is bonded to six N3- atoms to form a mixture of edge and corner-sharing TiN6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are two shorter (2.01 Å) and four longer (2.08 Å) Ti–N bond lengths. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded in a square co-planar geometry to four Ti4+ atoms. In the second N3- site, N3- is bonded to five Ti4+ atoms to form a mixture of edge and corner-sharing NTi5 square pyramids.
DOI: 10.17188/1720414
title: Materials Data on CaTbMn2O6 by Materials Project

description: CaTbMn2O6 is Orthorhombic Perovskite-derived structured and crystallizes in the orthorhombic Pmn2_1 space group. The structure is three-dimensional. Ca2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.33–2.66 Å. Tb4+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Tb–O bond distances ranging from 2.29–2.68 Å. Mn3+ is bonded to six O2- atoms to form corner-sharing MnO6 octahedra. The corner-sharing octahedra tilt angles range from 27–32°. There are a spread of Mn–O bond distances ranging from 1.96–2.01 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Ca2+, one Tb4+, and two equivalent Mn3+ atoms. In the second O2- site, O2- is bonded in a 5-coordinate geometry to one Ca2+, two equivalent Tb4+, and two equivalent Mn3+ atoms. In the third O2- site, O2- is bonded to one Ca2+, one Tb4+, and two equivalent Mn3+ atoms to form distorted corner-sharing OCaTbMn2 tetrahedra. In the fourth O2- site, O2- is bonded to one Ca2+, one Tb4+, and two equivalent Mn3+ atoms to form distorted corner-sharing OCaTbMn2 tetrahedra.
DOI: 10.17188/1720415
title: Materials Data on CeGe2Pt by Materials Project

description: CePtGe2 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. there are two inequivalent Ce sites. In the first Ce site, Ce is bonded in a 12-coordinate geometry to four equivalent Pt and ten Ge atoms. All Ce–Pt bond lengths are 3.33 Å. There are a spread of Ce–Ge bond distances ranging from 3.33–3.41 Å. In the second Ce site, Ce is bonded in a 8-coordinate geometry to six equivalent Pt and eight Ge atoms. There are four shorter (3.26 Å) and two longer (3.29 Å) Ce–Pt bond lengths. There are a spread of Ce–Ge bond distances ranging from 3.06–3.10 Å. Pt is bonded in a 10-coordinate geometry to five Ce and five Ge atoms. There are a spread of Pt–Ge bond distances ranging from 2.51–2.71 Å. There are three inequivalent Ge sites. In the first Ge site, Ge is bonded in a 2-coordinate geometry to four equivalent Ce, two equivalent Pt, and one Ge atom. The Ge–Ge bond length is 2.44 Å. In the second Ge site, Ge is bonded in a 9-coordinate geometry to six Ce, two equivalent Pt, and one Ge atom. The Ge–Ge bond length is 2.46 Å. In the third Ge site, Ge is bonded in a 8-coordinate geometry to four Ce, three equivalent Pt, and one Ge atom. The Ge–Ge bond length is 2.65 Å.