cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1687287
title: Materials Data on AlCu4SbPb6S2(Cl2O13)2 by Materials Project

description: Cu4AlPb6SbS2(O13Cl2)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Cu3+ sites. In the first Cu3+ site, Cu3+ is bonded in a square co-planar geometry to four O2- atoms. There is two shorter (1.84 Å) and two longer (1.95 Å) Cu–O bond length. In the second Cu3+ site, Cu3+ is bonded to six O2- atoms to form CuO6 octahedra that share a cornercorner with one SbO6 octahedra and an edgeedge with one AlO6 octahedra. The corner-sharing octahedral tilt angles are 42°. There are a spread of Cu–O bond distances ranging from 1.91–2.14 Å. Al3+ is bonded to six O2- atoms to form AlO6 octahedra that share edges with two equivalent CuO6 octahedra. There is four shorter (1.88 Å) and two longer (2.00 Å) Al–O bond length. There are two inequivalent Pb4+ sites. In the first Pb4+ site, Pb4+ is bonded in a 8-coordinate geometry to seven O2- and one Cl1- atom. There are a spread of Pb–O bond distances ranging from 2.28–2.63 Å. The Pb–Cl bond length is 2.61 Å. In the second Pb4+ site, Pb4+ is bonded in a 6-coordinate geometry to five O2- and one Cl1- atom. There are a spread of Pb–O bond distances ranging from 2.22–2.61 Å. The Pb–Cl bond length is 2.65 Å. Sb5+ is bonded to six O2- atoms to form SbO6 octahedra that share corners with two equivalent CuO6 octahedra. The corner-sharing octahedral tilt angles are 42°. There are two shorter (1.98 Å) and four longer (2.02 Å) Sb–O bond lengths. S6+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of S–O bond distances ranging from 1.46–1.54 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Cu3+, two equivalent Pb4+, and one Sb5+ atom. In the second O2- site, O2- is bonded in a distorted T-shaped geometry to three Cu3+ atoms. In the third O2- site, O2- is bonded in a single-bond geometry to one Pb4+ and one S6+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Al3+ and two equivalent Pb4+ atoms. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to two Pb4+ and one Sb5+ atom. In the sixth O2- site, O2- is bonded in a 2-coordinate geometry to one Cu3+, one Al3+, and one Pb4+ atom. In the seventh O2- site, O2- is bonded in a 2-coordinate geometry to two Cu3+ and one Pb4+ atom. In the eighth O2- site, O2- is bonded in a 1-coordinate geometry to one Pb4+ and one S6+ atom. In the ninth O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Pb4+ and one S6+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one Pb4+ atom. In the second Cl1- site, Cl1- is bonded in a distorted L-shaped geometry to two equivalent Pb4+ atoms.
DOI: 10.17188/1687288
title: Materials Data on SmAl3Ni by Materials Project

description: SmNiAl3 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Sm is bonded in a 10-coordinate geometry to two equivalent Sm, two equivalent Ni, and eleven Al atoms. Both Sm–Sm bond lengths are 3.66 Å. Both Sm–Ni bond lengths are 3.13 Å. There are a spread of Sm–Al bond distances ranging from 3.06–3.66 Å. Ni is bonded in a 9-coordinate geometry to two equivalent Sm and seven Al atoms. There are a spread of Ni–Al bond distances ranging from 2.35–2.52 Å. There are three inequivalent Al sites. In the first Al site, Al is bonded in a 2-coordinate geometry to four equivalent Sm, two equivalent Ni, and six Al atoms. There are a spread of Al–Al bond distances ranging from 2.63–2.94 Å. In the second Al site, Al is bonded in a 3-coordinate geometry to three equivalent Sm, three equivalent Ni, and two equivalent Al atoms. In the third Al site, Al is bonded in a 2-coordinate geometry to four equivalent Sm, two equivalent Ni, and four equivalent Al atoms.
DOI: 10.17188/1687289
title: Materials Data on MnH7C3NO6 by Materials Project

description: MnH3(CO2)3NH4 crystallizes in the monoclinic C2 space group. The structure is three-dimensional and consists of four ammonium molecules and one MnH3(CO2)3 framework. In the MnH3(CO2)3 framework, Mn2+ is bonded in an octahedral geometry to six O2- atoms. There are a spread of Mn–O bond distances ranging from 2.19–2.28 Å. There are four inequivalent C2+ sites. In the first C2+ site, C2+ is bonded in a trigonal planar geometry to one H1+ and two O2- atoms. The C–H bond length is 1.11 Å. There is one shorter (1.27 Å) and one longer (1.28 Å) C–O bond length. In the second C2+ site, C2+ is bonded in a trigonal planar geometry to one H1+ and two equivalent O2- atoms. The C–H bond length is 1.11 Å. Both C–O bond lengths are 1.27 Å. In the third C2+ site, C2+ is bonded in a trigonal planar geometry to one H1+ and two O2- atoms. The C–H bond length is 1.11 Å. There is one shorter (1.27 Å) and one longer (1.28 Å) C–O bond length. In the fourth C2+ site, C2+ is bonded in a trigonal planar geometry to one H1+ and two equivalent O2- atoms. The C–H bond length is 1.11 Å. Both C–O bond lengths are 1.27 Å. There are four inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one C2+ atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one C2+ atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one C2+ atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one C2+ atom. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C2+ atom. In the second O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C2+ atom. In the third O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C2+ atom. In the fourth O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C2+ atom. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C2+ atom. In the sixth O2- site, O2- is bonded in a bent 120 degrees geometry to one Mn2+ and one C2+ atom.
DOI: 10.17188/1687290
title: Materials Data on La5P12Ru19 by Materials Project

description: La5Ru19P12 crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. there are two inequivalent La sites. In the first La site, La is bonded in a 2-coordinate geometry to ten Ru and six P atoms. There are a spread of La–Ru bond distances ranging from 3.08–3.40 Å. There are four shorter (3.11 Å) and two longer (3.17 Å) La–P bond lengths. In the second La site, La is bonded in a 6-coordinate geometry to nine Ru and six equivalent P atoms. There are three shorter (3.17 Å) and six longer (3.19 Å) La–Ru bond lengths. All La–P bond lengths are 3.04 Å. There are five inequivalent Ru sites. In the first Ru site, Ru is bonded in a 9-coordinate geometry to six equivalent La and three equivalent P atoms. All Ru–P bond lengths are 2.39 Å. In the second Ru site, Ru is bonded in a distorted single-bond geometry to six Ru and five P atoms. There are two shorter (2.86 Å) and four longer (2.92 Å) Ru–Ru bond lengths. There are one shorter (2.27 Å) and four longer (2.83 Å) Ru–P bond lengths. In the third Ru site, Ru is bonded in a 12-coordinate geometry to two equivalent La, four equivalent Ru, and four P atoms. All Ru–Ru bond lengths are 2.86 Å. There are two shorter (2.29 Å) and two longer (2.36 Å) Ru–P bond lengths. In the fourth Ru site, Ru is bonded in a 12-coordinate geometry to three La, five Ru, and four P atoms. Both Ru–Ru bond lengths are 2.85 Å. There are a spread of Ru–P bond distances ranging from 2.37–2.45 Å. In the fifth Ru site, Ru is bonded in a 12-coordinate geometry to three La, five Ru, and four P atoms. The Ru–Ru bond length is 2.74 Å. There are a spread of Ru–P bond distances ranging from 2.35–2.53 Å. There are three inequivalent P sites. In the first P site, P is bonded in a 9-coordinate geometry to four equivalent La and five Ru atoms. In the second P site, P is bonded in a 9-coordinate geometry to two equivalent La and seven Ru atoms. In the third P site, P is bonded in a 9-coordinate geometry to two equivalent La and seven Ru atoms.
DOI: 10.17188/1687291
title: Materials Data on Ba4B10Cl2O19 by Materials Project

description: Ba4B10O19Cl2 crystallizes in the orthorhombic Pnn2 space group. The structure is three-dimensional. there are two inequivalent Ba sites. In the first Ba site, Ba is bonded in a 10-coordinate geometry to eight O and two Cl atoms. There are a spread of Ba–O bond distances ranging from 2.70–3.16 Å. There are one shorter (3.14 Å) and one longer (3.19 Å) Ba–Cl bond lengths. In the second Ba site, Ba is bonded in a 9-coordinate geometry to seven O and two Cl atoms. There are a spread of Ba–O bond distances ranging from 2.68–3.08 Å. There are one shorter (3.06 Å) and one longer (3.22 Å) Ba–Cl bond lengths. There are five inequivalent B sites. In the first B site, B is bonded in a trigonal planar geometry to three O atoms. There is two shorter (1.37 Å) and one longer (1.40 Å) B–O bond length. In the second B site, B is bonded in a trigonal planar geometry to three O atoms. All B–O bond lengths are 1.38 Å. In the third B site, B is bonded to four O atoms to form corner-sharing BO4 tetrahedra. There is three shorter (1.49 Å) and one longer (1.50 Å) B–O bond length. In the fourth B site, B is bonded to four O atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.47–1.50 Å. In the fifth B site, B is bonded to four O atoms to form corner-sharing BO4 tetrahedra. There are a spread of B–O bond distances ranging from 1.46–1.53 Å. There are ten inequivalent O sites. In the first O site, O is bonded in a distorted bent 150 degrees geometry to two equivalent Ba and one Cl atom. The O–Cl bond length is 2.45 Å. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one Ba and two B atoms. In the third O site, O is bonded in a bent 120 degrees geometry to two Ba and two B atoms. In the fourth O site, O is bonded in a distorted bent 120 degrees geometry to one Ba and two B atoms. In the fifth O site, O is bonded in a distorted bent 120 degrees geometry to one Ba and two B atoms. In the sixth O site, O is bonded in a bent 120 degrees geometry to two Ba and two B atoms. In the seventh O site, O is bonded in a distorted bent 120 degrees geometry to two Ba and two B atoms. In the eighth O site, O is bonded in a distorted bent 150 degrees geometry to two Ba and two B atoms. In the ninth O site, O is bonded in a distorted bent 150 degrees geometry to one Ba and two B atoms. In the tenth O site, O is bonded in a distorted bent 120 degrees geometry to two Ba and two B atoms. There are two inequivalent Cl sites. In the first Cl site, Cl is bonded in a rectangular see-saw-like geometry to four Ba atoms. In the second Cl site, Cl is bonded in a 5-coordinate geometry to four Ba and one O atom.
DOI: 10.17188/1687292
title: Materials Data on MnV4O12 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: 10.17188/1687293
title: Materials Data on FeGe7N10 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: 10.17188/1687294
title: Materials Data on CsSe by Materials Project

description: CsSe is Tetraauricupride structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Cs1+ is bonded in a body-centered cubic geometry to eight equivalent Se1- atoms. All Cs–Se bond lengths are 3.77 Å. Se1- is bonded in a body-centered cubic geometry to eight equivalent Cs1+ atoms.
DOI: 10.17188/1687295
title: Materials Data on VCu2BiO6 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: 10.17188/1687296
title: Materials Data on GeO2 by Materials Project

description: GeO2 is Rutile structured and crystallizes in the orthorhombic Pnnm space group. The structure is three-dimensional. Ge4+ is bonded to six equivalent O2- atoms to form a mixture of corner and edge-sharing GeO6 octahedra. The corner-sharing octahedral tilt angles are 50°. There is four shorter (1.90 Å) and two longer (1.95 Å) Ge–O bond length. O2- is bonded in a distorted trigonal planar geometry to three equivalent Ge4+ atoms.
DOI: 10.17188/1687297
title: Materials Data on FeBPbO4 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: 10.17188/1687298
title: Materials Data on LiVF4 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: 10.17188/1687299
title: Materials Data on NiP2O7 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: 10.17188/1687300
title: Materials Data on Mn3V(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: 10.17188/1687301
title: Materials Data on K7(FeTe2)4 by Materials Project

description: K7(FeTe2)4 crystallizes in the tetragonal P4_2/nmc space group. The structure is three-dimensional. there are three inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 8-coordinate geometry to eight Te2- atoms. There are four shorter (3.59 Å) and four longer (3.82 Å) K–Te bond lengths. In the second K1+ site, K1+ is bonded to four equivalent Te2- atoms to form KTe4 tetrahedra that share corners with four equivalent FeTe4 tetrahedra and edges with two equivalent KTe4 tetrahedra. There are two shorter (3.50 Å) and two longer (3.56 Å) K–Te bond lengths. In the third K1+ site, K1+ is bonded in a 8-coordinate geometry to eight Te2- atoms. There are a spread of K–Te bond distances ranging from 3.51–4.16 Å. Fe+2.25+ is bonded to four Te2- atoms to form FeTe4 tetrahedra that share corners with two equivalent KTe4 tetrahedra and edges with three equivalent FeTe4 tetrahedra. There are a spread of Fe–Te bond distances ranging from 2.59–2.63 Å. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 6-coordinate geometry to five K1+ and three equivalent Fe+2.25+ atoms. In the second Te2- site, Te2- is bonded in a 8-coordinate geometry to seven K1+ and one Fe+2.25+ atom.
DOI: 10.17188/1687302
title: Materials Data on VPH7N2O5 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: 10.17188/1687303
title: Materials Data on Ti3Fe9O16 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: 10.17188/1687304
title: Materials Data on Cr2FeSeS3 by Materials Project

description: Cr2FeSeS3 is Spinel-derived structured and crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. there are two inequivalent Cr3+ sites. In the first Cr3+ site, Cr3+ is bonded to one Se2- and five S2- atoms to form CrSeS5 octahedra that share corners with six FeSe2S2 tetrahedra and edges with six CrSeS5 octahedra. The Cr–Se bond length is 2.52 Å. There are one shorter (2.42 Å) and four longer (2.44 Å) Cr–S bond lengths. In the second Cr3+ site, Cr3+ is bonded to two equivalent Se2- and four S2- atoms to form CrSe2S4 octahedra that share corners with six FeSe2S2 tetrahedra and edges with six CrSeS5 octahedra. Both Cr–Se bond lengths are 2.53 Å. There are one shorter (2.42 Å) and three longer (2.43 Å) Cr–S bond lengths. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to two equivalent Se2- and two equivalent S2- atoms to form FeSe2S2 tetrahedra that share corners with twelve CrSeS5 octahedra. The corner-sharing octahedra tilt angles range from 54–63°. Both Fe–Se bond lengths are 2.40 Å. Both Fe–S bond lengths are 2.29 Å. In the second Fe2+ site, Fe2+ is bonded to four S2- atoms to form FeS4 tetrahedra that share corners with twelve CrSeS5 octahedra. The corner-sharing octahedra tilt angles range from 56–57°. There are two shorter (2.34 Å) and two longer (2.36 Å) Fe–S bond lengths. Se2- is bonded in a rectangular see-saw-like geometry to three Cr3+ and one Fe2+ atom. There are three inequivalent S2- sites. In the first S2- site, S2- is bonded to three Cr3+ and one Fe2+ atom to form a mixture of distorted edge and corner-sharing SCr3Fe trigonal pyramids. In the second S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Cr3+ and one Fe2+ atom. In the third S2- site, S2- is bonded in a distorted rectangular see-saw-like geometry to three Cr3+ and one Fe2+ atom.
DOI: 10.17188/1687305
title: Materials Data on Zr3TiZn8 by Materials Project

description: Zr3TiZn8 is Hexagonal Laves-derived structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. there are three inequivalent Zr sites. In the first Zr site, Zr is bonded in a 12-coordinate geometry to four Zr and twelve Zn atoms. All Zr–Zr bond lengths are 3.21 Å. There are nine shorter (3.05 Å) and three longer (3.07 Å) Zr–Zn bond lengths. In the second Zr site, Zr is bonded in a 12-coordinate geometry to three equivalent Zr, one Ti, and twelve Zn atoms. The Zr–Ti bond length is 3.14 Å. There are a spread of Zr–Zn bond distances ranging from 3.03–3.11 Å. In the third Zr site, Zr is bonded in a 12-coordinate geometry to one Zr, three equivalent Ti, and twelve Zn atoms. All Zr–Ti bond lengths are 3.17 Å. There are a spread of Zr–Zn bond distances ranging from 2.99–3.07 Å. Ti is bonded in a 1-coordinate geometry to four Zr and twelve Zn atoms. There are three shorter (3.02 Å) and nine longer (3.05 Å) Ti–Zn bond lengths. There are four inequivalent Zn sites. In the first Zn site, Zn is bonded to four Zr, two equivalent Ti, and six Zn atoms to form a mixture of edge, corner, and face-sharing ZnZr4Ti2Zn6 cuboctahedra. There are a spread of Zn–Zn bond distances ranging from 2.59–2.61 Å. In the second Zn site, Zn is bonded to five Zr, one Ti, and six Zn atoms to form a mixture of edge, corner, and face-sharing ZnZr5TiZn6 cuboctahedra. There are a spread of Zn–Zn bond distances ranging from 2.59–2.61 Å. In the third Zn site, Zn is bonded to three equivalent Zr, three equivalent Ti, and six Zn atoms to form ZnZr3Ti3Zn6 cuboctahedra that share corners with eighteen ZnZr4Ti2Zn6 cuboctahedra, edges with six equivalent ZnZr3Ti3Zn6 cuboctahedra, and faces with eighteen ZnZr4Ti2Zn6 cuboctahedra. In the fourth Zn site, Zn is bonded to six Zr and six Zn atoms to form ZnZr6Zn6 cuboctahedra that share corners with eighteen ZnZr4Ti2Zn6 cuboctahedra, edges with six equivalent ZnZr6Zn6 cuboctahedra, and faces with eighteen ZnZr4Ti2Zn6 cuboctahedra.
DOI: 10.17188/1687306
title: Materials Data on HgGe3 by Materials Project

description: HgGe3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Hg is bonded to twelve equivalent Ge atoms to form a mixture of face and corner-sharing HgGe12 cuboctahedra. There are six shorter (3.13 Å) and six longer (3.14 Å) Hg–Ge bond lengths. Ge is bonded in a 10-coordinate geometry to four equivalent Hg and six equivalent Ge atoms. There are two shorter (3.02 Å) and four longer (3.07 Å) Ge–Ge bond lengths.
DOI: 10.17188/1687307
title: Materials Data on Bi3As by Materials Project

description: Bi3As crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two Bi3As ribbons oriented in the (0, 0, 1) direction. Bi1+ is bonded in a distorted water-like geometry to two equivalent As3- atoms. Both Bi–As bond lengths are 3.32 Å. As3- is bonded in a 12-coordinate geometry to six equivalent Bi1+ atoms.
DOI: 10.17188/1687308
title: Materials Data on Ti3Cr2Sb(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: 10.17188/1687309
title: Materials Data on Cs3ScF6 by Materials Project

description: Cs3ScF6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded to twelve equivalent F1- atoms to form CsF12 cuboctahedra that share corners with twelve equivalent CsF12 cuboctahedra, faces with six equivalent CsF12 cuboctahedra, faces with four equivalent CsF6 octahedra, and faces with four equivalent ScF6 octahedra. All Cs–F bond lengths are 3.48 Å. In the second Cs1+ site, Cs1+ is bonded to six equivalent F1- atoms to form CsF6 octahedra that share corners with six equivalent ScF6 octahedra and faces with eight equivalent CsF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–F bond lengths are 2.85 Å. Sc3+ is bonded to six equivalent F1- atoms to form ScF6 octahedra that share corners with six equivalent CsF6 octahedra and faces with eight equivalent CsF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Sc–F bond lengths are 2.04 Å. F1- is bonded in a 2-coordinate geometry to five Cs1+ and one Sc3+ atom.
DOI: 10.17188/1687310
title: Materials Data on EuIn3 by Materials Project

description: EuIn3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Eu is bonded to twelve In atoms to form a mixture of face and corner-sharing EuIn12 cuboctahedra. There are a spread of Eu–In bond distances ranging from 3.38–3.43 Å. There are two inequivalent In sites. In the first In site, In is bonded in a 4-coordinate geometry to four equivalent Eu and six equivalent In atoms. There are two shorter (3.24 Å) and four longer (3.25 Å) In–In bond lengths. In the second In site, In is bonded in a 4-coordinate geometry to four equivalent Eu and six In atoms. There are one shorter (3.24 Å) and two longer (3.25 Å) In–In bond lengths.