cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1738669
title: Materials Data on LiY2Tc by Materials Project

description: LiY2Tc crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two LiY2Tc ribbons oriented in the (1, 0, 0) direction. Li is bonded in a linear geometry to two equivalent Y atoms. Both Li–Y bond lengths are 3.32 Å. Y is bonded in a linear geometry to one Li and one Tc atom. The Y–Tc bond length is 2.27 Å. Tc is bonded in a linear geometry to two equivalent Y atoms.
DOI: 10.17188/1738670
title: Materials Data on Li5Mn6(BO3)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: 10.17188/1738671
title: Materials Data on Sr4SiAs4 by Materials Project

description: Sr4SiAs4 crystallizes in the cubic P-43n space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded to six As3- atoms to form distorted SrAs6 octahedra that share corners with six SrAs6 octahedra, corners with three SiAs4 tetrahedra, edges with twelve SrAs6 octahedra, and a faceface with one SiAs4 tetrahedra. The corner-sharing octahedra tilt angles range from 14–18°. There are a spread of Sr–As bond distances ranging from 3.18–3.33 Å. In the second Sr2+ site, Sr2+ is bonded to six As3- atoms to form distorted SrAs6 octahedra that share corners with six equivalent SrAs6 octahedra, corners with three equivalent SiAs4 tetrahedra, edges with twelve SrAs6 octahedra, and a faceface with one SiAs4 tetrahedra. The corner-sharing octahedra tilt angles range from 15–17°. There are three shorter (3.22 Å) and three longer (3.32 Å) Sr–As bond lengths. There are two inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four equivalent As3- atoms to form SiAs4 tetrahedra that share corners with twelve SrAs6 octahedra and faces with four equivalent SrAs6 octahedra. The corner-sharing octahedra tilt angles range from 48–53°. All Si–As bond lengths are 2.40 Å. In the second Si4+ site, Si4+ is bonded to four equivalent As3- atoms to form SiAs4 tetrahedra that share corners with twelve equivalent SrAs6 octahedra and faces with four equivalent SrAs6 octahedra. The corner-sharing octahedral tilt angles are 53°. All Si–As bond lengths are 2.39 Å. There are two inequivalent As3- sites. In the first As3- site, As3- is bonded in a 7-coordinate geometry to six Sr2+ and one Si4+ atom. In the second As3- site, As3- is bonded in a 7-coordinate geometry to six Sr2+ and one Si4+ atom.
DOI: 10.17188/1738672
title: Materials Data on Cr10Sb3Te7 by Materials Project

description: Cr10Sb3Te7 is Caswellsilverite-like structured and crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are five inequivalent Cr+2.30+ sites. In the first Cr+2.30+ site, Cr+2.30+ is bonded to one Sb3- and five Te2- atoms to form CrSbTe5 octahedra that share corners with twelve CrSbTe5 octahedra, edges with six CrSb2Te4 octahedra, and faces with two CrSbTe5 octahedra. The corner-sharing octahedra tilt angles range from 49–50°. The Cr–Sb bond length is 2.81 Å. There are a spread of Cr–Te bond distances ranging from 2.82–2.84 Å. In the second Cr+2.30+ site, Cr+2.30+ is bonded to two Sb3- and four Te2- atoms to form a mixture of corner, edge, and face-sharing CrSb2Te4 octahedra. The corner-sharing octahedra tilt angles range from 49–50°. Both Cr–Sb bond lengths are 2.80 Å. There are two shorter (2.82 Å) and two longer (2.85 Å) Cr–Te bond lengths. In the third Cr+2.30+ site, Cr+2.30+ is bonded to two equivalent Sb3- and four Te2- atoms to form CrSb2Te4 octahedra that share corners with twelve CrSbTe5 octahedra, edges with six CrSbTe5 octahedra, and faces with two CrSb2Te4 octahedra. The corner-sharing octahedra tilt angles range from 49–50°. There are one shorter (2.80 Å) and one longer (2.81 Å) Cr–Sb bond lengths. There are two shorter (2.82 Å) and two longer (2.84 Å) Cr–Te bond lengths. In the fourth Cr+2.30+ site, Cr+2.30+ is bonded to two equivalent Sb3- and four Te2- atoms to form CrSb2Te4 octahedra that share corners with twelve CrSbTe5 octahedra, edges with six CrSbTe5 octahedra, and faces with two CrSb2Te4 octahedra. The corner-sharing octahedra tilt angles range from 49–50°. Both Cr–Sb bond lengths are 2.80 Å. There are a spread of Cr–Te bond distances ranging from 2.82–2.85 Å. In the fifth Cr+2.30+ site, Cr+2.30+ is bonded to two Sb3- and four Te2- atoms to form CrSb2Te4 octahedra that share corners with twelve CrSbTe5 octahedra, edges with six CrSbTe5 octahedra, and faces with two CrSb2Te4 octahedra. The corner-sharing octahedra tilt angles range from 49–50°. There are one shorter (2.80 Å) and one longer (2.81 Å) Cr–Sb bond lengths. There are a spread of Cr–Te bond distances ranging from 2.82–2.85 Å. There are two inequivalent Sb3- sites. In the first Sb3- site, Sb3- is bonded in a 6-coordinate geometry to six Cr+2.30+ atoms. In the second Sb3- site, Sb3- is bonded in a 6-coordinate geometry to six Cr+2.30+ atoms. There are four inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 6-coordinate geometry to six Cr+2.30+ atoms. In the second Te2- site, Te2- is bonded in a 6-coordinate geometry to six Cr+2.30+ atoms. In the third Te2- site, Te2- is bonded in a 6-coordinate geometry to six Cr+2.30+ atoms. In the fourth Te2- site, Te2- is bonded in a 6-coordinate geometry to six Cr+2.30+ atoms.
DOI: 10.17188/1738673
title: Materials Data on YbH2ClO2 by Materials Project

description: YbH2O2Cl crystallizes in the orthorhombic Pnma space group. The structure is two-dimensional and consists of two YbH2O2Cl sheets oriented in the (0, 0, 1) direction. Yb3+ is bonded in a 6-coordinate geometry to six O2- and two equivalent Cl1- atoms. There are a spread of Yb–O bond distances ranging from 2.31–2.53 Å. Both Yb–Cl bond lengths are 2.95 Å. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.98 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.98 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to three equivalent Yb3+, one H1+, and one Cl1- atom. The O–Cl bond length is 2.43 Å. In the second O2- site, O2- is bonded in a distorted single-bond geometry to three equivalent Yb3+ and one H1+ atom. Cl1- is bonded in a 3-coordinate geometry to two equivalent Yb3+ and one O2- atom.
DOI: 10.17188/1738674
title: Materials Data on KRbMnV2O7 by Materials Project

description: RbKV2MnO7 crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Rb1+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are four shorter (2.98 Å) and four longer (3.04 Å) Rb–O bond lengths. K1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of K–O bond distances ranging from 2.77–3.21 Å. V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share a cornercorner with one VO4 tetrahedra and corners with two equivalent MnO4 tetrahedra. There are a spread of V–O bond distances ranging from 1.68–1.84 Å. Mn2+ is bonded to four equivalent O2- atoms to form MnO4 tetrahedra that share corners with four equivalent VO4 tetrahedra. All Mn–O bond lengths are 2.06 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Rb1+, one K1+, and one V5+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent K1+ and two equivalent V5+ atoms. In the third O2- site, O2- is bonded in a 2-coordinate geometry to one Rb1+, one K1+, one V5+, and one Mn2+ atom.
DOI: 10.17188/1738675
title: Materials Data on Sr10CaY4(CoO3)10 by Materials Project

description: Sr10CaY4(CoO3)10 crystallizes in the tetragonal I4/m space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.60–2.83 Å. In the second Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.43–2.99 Å. Ca2+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Ca–O bond lengths are 2.46 Å. Y3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Y–O bond distances ranging from 2.38–2.41 Å. There are two inequivalent Co+2.60+ sites. In the first Co+2.60+ site, Co+2.60+ is bonded to five O2- atoms to form distorted corner-sharing CoO5 trigonal bipyramids. There is one shorter (1.78 Å) and four longer (1.98 Å) Co–O bond length. In the second Co+2.60+ site, Co+2.60+ is bonded to five O2- atoms to form corner-sharing CoO5 square pyramids. There are a spread of Co–O bond distances ranging from 1.94–2.08 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded to five Sr2+ and one Co+2.60+ atom to form a mixture of distorted edge and corner-sharing OSr5Co octahedra. The corner-sharing octahedral tilt angles are 9°. In the second O2- site, O2- is bonded to five Sr2+ and one Co+2.60+ atom to form a mixture of distorted edge and corner-sharing OSr5Co octahedra. The corner-sharing octahedra tilt angles range from 9–14°. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Sr2+, two equivalent Y3+, and two Co+2.60+ atoms. In the fourth O2- site, O2- is bonded in a 6-coordinate geometry to two equivalent Sr2+, two equivalent Y3+, and two equivalent Co+2.60+ atoms. In the fifth O2- site, O2- is bonded in a 6-coordinate geometry to two Sr2+, one Ca2+, one Y3+, and two equivalent Co+2.60+ atoms.
DOI: 10.17188/1738676
title: Materials Data on Al2Cd3(GeO4)3 by Materials Project

description: Cd3Al2(GeO4)3 crystallizes in the cubic Ia-3d space group. The structure is three-dimensional. Cd2+ is bonded in a distorted body-centered cubic geometry to eight equivalent O2- atoms. There are four shorter (2.36 Å) and four longer (2.54 Å) Cd–O bond lengths. Al3+ is bonded to six equivalent O2- atoms to form AlO6 octahedra that share corners with six equivalent GeO4 tetrahedra. All Al–O bond lengths are 1.94 Å. Ge4+ is bonded to four equivalent O2- atoms to form GeO4 tetrahedra that share corners with four equivalent AlO6 octahedra. The corner-sharing octahedral tilt angles are 46°. All Ge–O bond lengths are 1.78 Å. O2- is bonded in a 4-coordinate geometry to two equivalent Cd2+, one Al3+, and one Ge4+ atom.
DOI: 10.17188/1738677
title: Materials Data on Dy6Ag(GeS7)2 by Materials Project

description: Dy6Ag(GeS7)2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Dy–S bond distances ranging from 2.74–3.22 Å. In the second Dy3+ site, Dy3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Dy–S bond distances ranging from 2.74–3.22 Å. In the third Dy3+ site, Dy3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Dy–S bond distances ranging from 2.74–3.23 Å. In the fourth Dy3+ site, Dy3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Dy–S bond distances ranging from 2.74–3.23 Å. In the fifth Dy3+ site, Dy3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Dy–S bond distances ranging from 2.74–3.23 Å. In the sixth Dy3+ site, Dy3+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of Dy–S bond distances ranging from 2.74–3.23 Å. Ag2+ is bonded in an octahedral geometry to six S2- atoms. There are a spread of Ag–S bond distances ranging from 2.60–2.74 Å. There are two inequivalent Ge4+ sites. In the first Ge4+ site, Ge4+ is bonded in a tetrahedral geometry to four S2- atoms. There are one shorter (2.20 Å) and three longer (2.25 Å) Ge–S bond lengths. In the second Ge4+ site, Ge4+ is bonded in a tetrahedral geometry to four S2- atoms. There are one shorter (2.20 Å) and three longer (2.24 Å) Ge–S bond lengths. There are fourteen inequivalent S2- sites. In the first S2- site, S2- is bonded in a 5-coordinate geometry to four Dy3+ and one Ag2+ atom. In the second S2- site, S2- is bonded in a 5-coordinate geometry to four Dy3+ and one Ag2+ atom. In the third S2- site, S2- is bonded in a 5-coordinate geometry to four Dy3+ and one Ag2+ atom. In the fourth S2- site, S2- is bonded in a 5-coordinate geometry to four Dy3+ and one Ag2+ atom. In the fifth S2- site, S2- is bonded in a 5-coordinate geometry to four Dy3+ and one Ag2+ atom. In the sixth S2- site, S2- is bonded in a 5-coordinate geometry to four Dy3+ and one Ag2+ atom. In the seventh S2- site, S2- is bonded in a tetrahedral geometry to three Dy3+ and one Ge4+ atom. In the eighth S2- site, S2- is bonded in a tetrahedral geometry to three Dy3+ and one Ge4+ atom. In the ninth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Dy3+ and one Ge4+ atom. In the tenth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Dy3+ and one Ge4+ atom. In the eleventh S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Dy3+ and one Ge4+ atom. In the twelfth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Dy3+ and one Ge4+ atom. In the thirteenth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Dy3+ and one Ge4+ atom. In the fourteenth S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Dy3+ and one Ge4+ atom.
DOI: 10.17188/1738678
title: Materials Data on Ho4Ge6Ir7 by Materials Project

description: Ho4Ir7Ge6 crystallizes in the cubic Im-3m space group. The structure is three-dimensional. Ho is bonded to six equivalent Ir and six equivalent Ge atoms to form HoGe6Ir6 cuboctahedra that share corners with twelve equivalent HoGe6Ir6 cuboctahedra, faces with six equivalent HoGe6Ir6 cuboctahedra, and faces with two equivalent IrGe6 octahedra. All Ho–Ir bond lengths are 2.97 Å. All Ho–Ge bond lengths are 3.02 Å. There are two inequivalent Ir sites. In the first Ir site, Ir is bonded to six equivalent Ge atoms to form IrGe6 octahedra that share faces with eight equivalent HoGe6Ir6 cuboctahedra. All Ir–Ge bond lengths are 2.67 Å. In the second Ir site, Ir is bonded in a 12-coordinate geometry to four equivalent Ho and four equivalent Ge atoms. All Ir–Ge bond lengths are 2.60 Å. Ge is bonded in a 9-coordinate geometry to four equivalent Ho and five Ir atoms.
DOI: 10.17188/1738679
title: Materials Data on Li2Cr3TeO8 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: 10.17188/1738680
title: Materials Data on Na2Al2(SiO4)3 by Materials Project

description: Na2Al2(SiO4)3 crystallizes in the orthorhombic Fdd2 space group. The structure is three-dimensional. Na is bonded to six O atoms to form distorted NaO6 pentagonal pyramids that share corners with two equivalent AlO4 tetrahedra, corners with two equivalent SiO4 tetrahedra, edges with two equivalent NaO6 pentagonal pyramids, an edgeedge with one AlO4 tetrahedra, and an edgeedge with one SiO4 tetrahedra. There are a spread of Na–O bond distances ranging from 2.37–2.53 Å. Al is bonded to four O atoms to form AlO4 tetrahedra that share corners with two equivalent NaO6 pentagonal pyramids, corners with four SiO4 tetrahedra, and an edgeedge with one NaO6 pentagonal pyramid. There are a spread of Al–O bond distances ranging from 1.75–1.78 Å. There are two inequivalent Si sites. In the first Si site, 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 is two shorter (1.63 Å) and two longer (1.65 Å) Si–O bond length. In the second Si site, Si is bonded to four O atoms to form SiO4 tetrahedra that share corners with two equivalent NaO6 pentagonal pyramids, a cornercorner with one SiO4 tetrahedra, corners with three equivalent AlO4 tetrahedra, and an edgeedge with one NaO6 pentagonal pyramid. There is two shorter (1.63 Å) and two longer (1.65 Å) Si–O bond length. There are six inequivalent O sites. In the first O site, O is bonded in a 3-coordinate geometry to one Na, one Al, and one Si atom. In the second O site, O is bonded in a 3-coordinate geometry to one Na, one Al, and one Si atom. In the third O site, O is bonded in a bent 150 degrees geometry to two Si atoms. In the fourth O site, O is bonded in an L-shaped geometry to two equivalent Na atoms. In the fifth O site, O is bonded in a bent 150 degrees geometry to one Al and one Si atom. In the sixth O site, O is bonded in a 4-coordinate geometry to two equivalent Na, one Al, and one Si atom.
DOI: 10.17188/1738681
title: Materials Data on SnPb7N6 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: 10.17188/1738682
title: Materials Data on ThTi3 by Materials Project

description: ThTi3 is alpha bismuth trifluoride structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Th is bonded in a distorted body-centered cubic geometry to twelve Ti atoms. There are eight shorter (2.98 Å) and four longer (3.34 Å) Th–Ti bond lengths. There are two inequivalent Ti sites. In the first Ti site, Ti is bonded in a 8-coordinate geometry to four equivalent Th and four equivalent Ti atoms. All Ti–Ti bond lengths are 2.98 Å. In the second Ti site, Ti is bonded to four equivalent Th and eight equivalent Ti atoms to form a mixture of distorted edge, face, and corner-sharing TiTh4Ti8 cuboctahedra.
DOI: 10.17188/1738683
title: Materials Data on Sr3OsN3 by Materials Project

description: Sr3OsN3 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are three inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded to five N3- atoms to form a mixture of distorted edge and corner-sharing SrN5 trigonal bipyramids. There are a spread of Sr–N bond distances ranging from 2.70–2.93 Å. In the second Sr2+ site, Sr2+ is bonded to five N3- atoms to form a mixture of distorted edge and corner-sharing SrN5 trigonal bipyramids. There are a spread of Sr–N bond distances ranging from 2.71–2.93 Å. In the third Sr2+ site, Sr2+ is bonded to five N3- atoms to form a mixture of distorted edge and corner-sharing SrN5 trigonal bipyramids. There are a spread of Sr–N bond distances ranging from 2.70–2.92 Å. Os3+ is bonded in a trigonal planar geometry to three N3- atoms. All Os–N bond lengths are 1.87 Å. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded to five Sr2+ and one Os3+ atom to form a mixture of distorted edge and corner-sharing NSr5Os octahedra. The corner-sharing octahedra tilt angles range from 17–45°. In the second N3- site, N3- is bonded to five Sr2+ and one Os3+ atom to form a mixture of distorted edge and corner-sharing NSr5Os octahedra. The corner-sharing octahedra tilt angles range from 18–45°. In the third N3- site, N3- is bonded to five Sr2+ and one Os3+ atom to form a mixture of distorted edge and corner-sharing NSr5Os octahedra. The corner-sharing octahedra tilt angles range from 18–45°.
DOI: 10.17188/1738684
title: Materials Data on Li3MnF6 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: 10.17188/1738685
title: Materials Data on Sr(FeN)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: 10.17188/1738686
title: Materials Data on Mn3OF5 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: 10.17188/1738687
title: Materials Data on Pr2FeSn4 by Materials Project

description: Pr2FeSn4 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Pr sites. In the first Pr site, Pr is bonded in a 11-coordinate geometry to one Fe and ten Sn atoms. The Pr–Fe bond length is 3.34 Å. There are a spread of Pr–Sn bond distances ranging from 3.32–3.45 Å. In the second Pr site, Pr is bonded in a 10-coordinate geometry to ten Sn atoms. There are a spread of Pr–Sn bond distances ranging from 3.39–3.69 Å. Fe is bonded in a 5-coordinate geometry to one Pr and five Sn atoms. There are a spread of Fe–Sn bond distances ranging from 2.49–2.52 Å. There are four inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to four Pr and two equivalent Fe atoms. In the second Sn site, Sn is bonded in a 2-coordinate geometry to four Pr and two equivalent Fe atoms. In the third Sn site, Sn is bonded in a 1-coordinate geometry to six Pr, one Fe, and two equivalent Sn atoms. Both Sn–Sn bond lengths are 3.06 Å. In the fourth Sn site, Sn is bonded in a 4-coordinate geometry to six Pr and two equivalent Sn atoms.
DOI: 10.17188/1738688
title: Materials Data on EuZnIn by Materials Project

description: EuZnIn crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Eu is bonded in a 12-coordinate geometry to six equivalent Zn and six equivalent In atoms. There are a spread of Eu–Zn bond distances ranging from 3.29–3.53 Å. There are a spread of Eu–In bond distances ranging from 3.36–3.56 Å. Zn is bonded in a 10-coordinate geometry to six equivalent Eu, one Zn, and three equivalent In atoms. The Zn–Zn bond length is 2.75 Å. There are two shorter (2.80 Å) and one longer (3.10 Å) Zn–In bond lengths. In is bonded in a 10-coordinate geometry to six equivalent Eu, three equivalent Zn, and one In atom. The In–In bond length is 2.94 Å.