cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1311107
title: Materials Data on Cd2PtRh by Materials Project

description: RhPtCd2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Rh is bonded in a body-centered cubic geometry to eight equivalent Cd atoms. All Rh–Cd bond lengths are 2.82 Å. Pt is bonded in a body-centered cubic geometry to eight equivalent Cd atoms. All Pt–Cd bond lengths are 2.82 Å. Cd is bonded in a body-centered cubic geometry to four equivalent Rh and four equivalent Pt atoms.
DOI: 10.17188/1311108
title: Materials Data on TiZnCu2 by Materials Project

description: Cu2TiZn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a body-centered cubic geometry to eight equivalent Cu atoms. All Ti–Cu bond lengths are 2.60 Å. Cu is bonded in a body-centered cubic geometry to four equivalent Ti and four equivalent Zn atoms. All Cu–Zn bond lengths are 2.60 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Cu atoms.
DOI: 10.17188/1311109
title: Materials Data on Ti2TcPd by Materials Project

description: Ti2TcPd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a body-centered cubic geometry to four equivalent Tc and four equivalent Pd atoms. All Ti–Tc bond lengths are 2.71 Å. All Ti–Pd bond lengths are 2.71 Å. Tc is bonded in a distorted body-centered cubic geometry to eight equivalent Ti atoms. Pd is bonded in a body-centered cubic geometry to eight equivalent Ti atoms.
DOI: 10.17188/1311110
title: Materials Data on Li2CePb by Materials Project

description: Li2CePb is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to four equivalent Ce and four equivalent Pb atoms. All Li–Ce bond lengths are 3.05 Å. All Li–Pb bond lengths are 3.05 Å. Ce is bonded in a 8-coordinate geometry to eight equivalent Li and six equivalent Pb atoms. All Ce–Pb bond lengths are 3.52 Å. Pb is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent Ce atoms.
DOI: 10.17188/1311111
title: Materials Data on LiSiIr2 by Materials Project

description: LiIr2Si is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Ir and six equivalent Si atoms. All Li–Ir bond lengths are 2.52 Å. All Li–Si bond lengths are 2.91 Å. Ir is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Si atoms. All Ir–Si bond lengths are 2.52 Å. Si is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Ir atoms.
DOI: 10.17188/1311112
title: Materials Data on YbF2 by Materials Project

description: YbF2 is Rutile structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Yb2+ is bonded to six equivalent F1- atoms to form a mixture of edge and corner-sharing YbF6 octahedra. The corner-sharing octahedral tilt angles are 51°. There are two shorter (2.23 Å) and four longer (2.25 Å) Yb–F bond lengths. F1- is bonded in a trigonal planar geometry to three equivalent Yb2+ atoms.
DOI: 10.17188/1311113
title: Materials Data on Li2MgSn by Materials Project

description: Li2MgSn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Sn atoms. All Li–Mg bond lengths are 2.89 Å. All Li–Sn bond lengths are 2.89 Å. Mg is bonded in a distorted body-centered cubic geometry to eight equivalent Li atoms. Sn is bonded in a body-centered cubic geometry to eight equivalent Li atoms.
DOI: 10.17188/1311114
title: Materials Data on LiSc2Tc by Materials Project

description: LiSc2Tc is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a distorted body-centered cubic geometry to eight equivalent Sc and six equivalent Tc atoms. All Li–Sc bond lengths are 2.85 Å. All Li–Tc bond lengths are 3.30 Å. Sc is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Tc atoms. All Sc–Tc bond lengths are 2.85 Å. Tc is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Sc atoms.
DOI: 10.17188/1311115
title: Materials Data on KNpAgS3 by Materials Project

description: KNpAgS3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. K1+ is bonded in a 8-coordinate geometry to eight S2- atoms. There are a spread of K–S bond distances ranging from 3.24–3.58 Å. Np4+ is bonded to six S2- atoms to form NpS6 octahedra that share corners with two equivalent NpS6 octahedra, edges with two equivalent NpS6 octahedra, and edges with four equivalent AgS4 tetrahedra. The corner-sharing octahedral tilt angles are 37°. There are four shorter (2.73 Å) and two longer (2.75 Å) Np–S bond lengths. Ag1+ is bonded to four S2- atoms to form AgS4 tetrahedra that share corners with two equivalent AgS4 tetrahedra and edges with four equivalent NpS6 octahedra. There are two shorter (2.47 Å) and two longer (2.56 Å) Ag–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a 6-coordinate geometry to three equivalent K1+, two equivalent Np4+, and one Ag1+ atom. In the second S2- site, S2- is bonded to two equivalent K1+, two equivalent Np4+, and two equivalent Ag1+ atoms to form a mixture of distorted edge and corner-sharing SK2Np2Ag2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1311116
title: Materials Data on LiMg2 by Materials Project

description: LiMg2 crystallizes in the monoclinic C2/m space group. The structure is two-dimensional and consists of two LiMg2 sheets oriented in the (1, 0, 0) direction. Li is bonded in a body-centered cubic geometry to eight equivalent Mg atoms. There are four shorter (2.95 Å) and four longer (2.96 Å) Li–Mg bond lengths. Mg is bonded in a 8-coordinate geometry to four equivalent Li atoms.
DOI: 10.17188/1311117
title: Materials Data on LiThAu2 by Materials Project

description: LiThAu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Li–Au bond lengths are 3.07 Å. Th is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Th–Au bond lengths are 3.07 Å. Au is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Th atoms.
DOI: 10.17188/1311118
title: Materials Data on ThSnRu2 by Materials Project

description: ThRu2Sn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Th is bonded in a body-centered cubic geometry to eight equivalent Ru and six equivalent Sn atoms. All Th–Ru bond lengths are 2.95 Å. All Th–Sn bond lengths are 3.40 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Th and four equivalent Sn atoms. All Ru–Sn bond lengths are 2.95 Å. Sn is bonded in a distorted body-centered cubic geometry to six equivalent Th and eight equivalent Ru atoms.
DOI: 10.17188/1311119
title: Materials Data on LuInNi2 by Materials Project

description: LuNi2In is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Lu is bonded in a body-centered cubic geometry to eight equivalent Ni and six equivalent In atoms. All Lu–Ni bond lengths are 2.76 Å. All Lu–In bond lengths are 3.19 Å. Ni is bonded in a body-centered cubic geometry to four equivalent Lu and four equivalent In atoms. All Ni–In bond lengths are 2.76 Å. In is bonded in a distorted body-centered cubic geometry to six equivalent Lu and eight equivalent Ni atoms.
DOI: 10.17188/1311120
title: Materials Data on YbPrAg2 by Materials Project

description: YbPrAg2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Yb is bonded in a body-centered cubic geometry to eight equivalent Ag atoms. All Yb–Ag bond lengths are 3.23 Å. Pr is bonded in a body-centered cubic geometry to eight equivalent Ag atoms. All Pr–Ag bond lengths are 3.23 Å. Ag is bonded in a body-centered cubic geometry to four equivalent Yb and four equivalent Pr atoms.
DOI: 10.17188/1311121
title: Materials Data on Ti2ReRh by Materials Project

description: Ti2ReRh is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a body-centered cubic geometry to four equivalent Re and four equivalent Rh atoms. All Ti–Re bond lengths are 2.69 Å. All Ti–Rh bond lengths are 2.69 Å. Re is bonded in a distorted body-centered cubic geometry to eight equivalent Ti atoms. Rh is bonded in a body-centered cubic geometry to eight equivalent Ti atoms.
DOI: 10.17188/1311122
title: Materials Data on TmNpRu2 by Materials Project

description: NpTmRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Np is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Np–Ru bond lengths are 2.92 Å. Tm is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Tm–Ru bond lengths are 2.92 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Np and four equivalent Tm atoms.
DOI: 10.17188/1311123
title: Materials Data on AcAg3 by Materials Project

description: AcAg3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Ac is bonded to twelve Ag atoms to form a mixture of distorted corner and face-sharing AcAg12 cuboctahedra. There are a spread of Ac–Ag bond distances ranging from 3.36–3.51 Å. There are two inequivalent Ag sites. In the first Ag site, Ag is bonded in a 10-coordinate geometry to four equivalent Ac and six Ag atoms. There are a spread of Ag–Ag bond distances ranging from 2.94–2.97 Å. In the second Ag site, Ag is bonded in a 10-coordinate geometry to four equivalent Ac and six equivalent Ag atoms.
DOI: 10.17188/1311124
title: Materials Data on Ac2IrAu by Materials Project

description: Ac2IrAu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ac is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Au atoms. All Ac–Ir bond lengths are 3.30 Å. All Ac–Au bond lengths are 3.30 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Ac atoms. Au is bonded in a body-centered cubic geometry to eight equivalent Ac atoms.
DOI: 10.17188/1311125
title: Materials Data on AcTlAu2 by Materials Project

description: AcAu2Tl is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ac is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Ac–Au bond lengths are 3.25 Å. Au is bonded in a body-centered cubic geometry to four equivalent Ac and four equivalent Tl atoms. All Au–Tl bond lengths are 3.25 Å. Tl is bonded in a body-centered cubic geometry to eight equivalent Au atoms.
DOI: 10.17188/1311126
title: Materials Data on AcYbZn2 by Materials Project

description: AcYbZn2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ac is bonded in a body-centered cubic geometry to eight equivalent Zn atoms. All Ac–Zn bond lengths are 3.28 Å. Yb is bonded in a body-centered cubic geometry to eight equivalent Zn atoms. All Yb–Zn bond lengths are 3.28 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Ac and four equivalent Yb atoms.
DOI: 10.17188/1311127
title: Materials Data on LiHo2Rh by Materials Project

description: LiHo2Rh is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Ho atoms. All Li–Ho bond lengths are 3.01 Å. Ho is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Rh atoms. All Ho–Rh bond lengths are 3.01 Å. Rh is bonded in a body-centered cubic geometry to eight equivalent Ho atoms.
DOI: 10.17188/1311128
title: Materials Data on CaNdHg2 by Materials Project

description: CaNdHg2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ca is bonded in a body-centered cubic geometry to eight equivalent Hg atoms. All Ca–Hg bond lengths are 3.30 Å. Nd is bonded in a body-centered cubic geometry to eight equivalent Hg atoms. All Nd–Hg bond lengths are 3.30 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent Nd atoms.
DOI: 10.17188/1311129
title: Materials Data on IrCl3 by Materials Project

description: IrCl3 crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two IrCl3 ribbons oriented in the (0, 0, 1) direction. Ir3+ is bonded to six equivalent Cl1- atoms to form distorted face-sharing IrCl6 pentagonal pyramids. All Ir–Cl bond lengths are 2.41 Å. Cl1- is bonded in an L-shaped geometry to two equivalent Ir3+ atoms.
DOI: 10.17188/1311130
title: Materials Data on AcSnAu2 by Materials Project

description: AcAu2Sn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ac is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Ac–Au bond lengths are 3.22 Å. Au is bonded in a body-centered cubic geometry to four equivalent Ac and four equivalent Sn atoms. All Au–Sn bond lengths are 3.22 Å. Sn is bonded in a distorted body-centered cubic geometry to eight equivalent Au atoms.
DOI: 10.17188/1311131
title: Materials Data on AcTlAg2 by Materials Project

description: AcAg2Tl is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ac is bonded in a body-centered cubic geometry to eight equivalent Ag atoms. All Ac–Ag bond lengths are 3.25 Å. Ag is bonded in a body-centered cubic geometry to four equivalent Ac and four equivalent Tl atoms. All Ag–Tl bond lengths are 3.25 Å. Tl is bonded in a distorted body-centered cubic geometry to eight equivalent Ag atoms.
DOI: 10.17188/1311132
title: Materials Data on LiHo2Ru by Materials Project

description: LiHo2Ru is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Ho atoms. All Li–Ho bond lengths are 2.99 Å. Ho is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ru atoms. All Ho–Ru bond lengths are 2.99 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Ho atoms.
DOI: 10.17188/1311133
title: Materials Data on CoRe3 by Materials Project

description: Re3Co is Magnesium-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Re is bonded to eight equivalent Re and four equivalent Co atoms to form ReCo4Re8 cuboctahedra that share corners with four equivalent CoRe12 cuboctahedra, corners with fourteen equivalent ReCo4Re8 cuboctahedra, edges with six equivalent CoRe12 cuboctahedra, edges with twelve equivalent ReCo4Re8 cuboctahedra, faces with four equivalent CoRe12 cuboctahedra, and faces with sixteen equivalent ReCo4Re8 cuboctahedra. There are a spread of Re–Re bond distances ranging from 2.68–2.72 Å. There are two shorter (2.69 Å) and two longer (2.71 Å) Re–Co bond lengths. Co is bonded to twelve equivalent Re atoms to form CoRe12 cuboctahedra that share corners with six equivalent CoRe12 cuboctahedra, corners with twelve equivalent ReCo4Re8 cuboctahedra, edges with eighteen equivalent ReCo4Re8 cuboctahedra, faces with eight equivalent CoRe12 cuboctahedra, and faces with twelve equivalent ReCo4Re8 cuboctahedra.
DOI: 10.17188/1311134
title: Materials Data on K3Bi(AsSe2)6 by Materials Project

description: K3BiAs6Se12 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent K1+ sites. In the first K1+ site, K1+ is bonded to six Se2- atoms to form KSe6 octahedra that share faces with two equivalent BiSe6 octahedra. All K–Se bond lengths are 3.37 Å. In the second K1+ site, K1+ is bonded in a distorted q6 geometry to nine Se2- atoms. There are a spread of K–Se bond distances ranging from 3.54–3.78 Å. Bi3+ is bonded to six Se2- atoms to form BiSe6 octahedra that share faces with two equivalent KSe6 octahedra. There are two shorter (3.00 Å) and four longer (3.01 Å) Bi–Se bond lengths. There are three inequivalent As3+ sites. In the first As3+ site, As3+ is bonded in a distorted trigonal non-coplanar geometry to three Se2- atoms. There are a spread of As–Se bond distances ranging from 2.38–2.49 Å. In the second As3+ site, As3+ is bonded in a distorted trigonal non-coplanar geometry to three Se2- atoms. There are a spread of As–Se bond distances ranging from 2.38–2.49 Å. In the third As3+ site, As3+ is bonded in a distorted trigonal non-coplanar geometry to three Se2- atoms. There are a spread of As–Se bond distances ranging from 2.38–2.49 Å. There are six inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 4-coordinate geometry to two K1+, one Bi3+, and one As3+ atom. In the second Se2- site, Se2- is bonded in a 4-coordinate geometry to two K1+, one Bi3+, and one As3+ atom. In the third Se2- site, Se2- is bonded in a 4-coordinate geometry to two K1+, one Bi3+, and one As3+ atom. In the fourth Se2- site, Se2- is bonded in a 4-coordinate geometry to two equivalent K1+ and two As3+ atoms. In the fifth Se2- site, Se2- is bonded in a 4-coordinate geometry to two equivalent K1+ and two As3+ atoms. In the sixth Se2- site, Se2- is bonded in a 2-coordinate geometry to two equivalent K1+ and two As3+ atoms.
DOI: 10.17188/1311135
title: Materials Data on LiGaAg2 by Materials Project

description: LiAg2Ga is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Ag atoms. All Li–Ag bond lengths are 2.77 Å. Ag is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Ga atoms. All Ag–Ga bond lengths are 2.77 Å. Ga is bonded in a distorted body-centered cubic geometry to eight equivalent Ag atoms.
DOI: 10.17188/1311136
title: Materials Data on Li2CaSn by Materials Project

description: Li2CaSn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a distorted body-centered cubic geometry to four equivalent Ca and four equivalent Sn atoms. All Li–Ca bond lengths are 3.00 Å. All Li–Sn bond lengths are 3.00 Å. Ca is bonded in a 8-coordinate geometry to eight equivalent Li and six equivalent Sn atoms. All Ca–Sn bond lengths are 3.47 Å. Sn is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent Ca atoms.
DOI: 10.17188/1311137
title: Materials Data on Li2CaSi by Materials Project

description: Li2CaSi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li1+ is bonded to four equivalent Ca2+ and four equivalent Si4- atoms to form a mixture of corner, edge, and face-sharing LiCa4Si4 tetrahedra. All Li–Ca bond lengths are 2.84 Å. All Li–Si bond lengths are 2.84 Å. Ca2+ is bonded in a 6-coordinate geometry to eight equivalent Li1+ and six equivalent Si4- atoms. All Ca–Si bond lengths are 3.28 Å. Si4- is bonded in a distorted body-centered cubic geometry to eight equivalent Li1+ and six equivalent Ca2+ atoms.
DOI: 10.17188/1311138
title: Materials Data on BeAlIr2 by Materials Project

description: BeIr2Al is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a body-centered cubic geometry to eight equivalent Ir atoms. All Be–Ir bond lengths are 2.53 Å. Ir is bonded in a body-centered cubic geometry to four equivalent Be and four equivalent Al atoms. All Ir–Al bond lengths are 2.53 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Ir atoms.
DOI: 10.17188/1311139
title: Materials Data on Ce5Al2Ru3 by Materials Project

description: Ce5Ru3Al2 crystallizes in the trigonal R3 space group. The structure is three-dimensional. there are four inequivalent Ce sites. In the first Ce site, Ce is bonded to three equivalent Ru and one Al atom to form distorted corner-sharing CeAlRu3 tetrahedra. All Ce–Ru bond lengths are 2.81 Å. The Ce–Al bond length is 3.24 Å. In the second Ce site, Ce is bonded in a 2-coordinate geometry to four Ru and four Al atoms. There are two shorter (2.77 Å) and two longer (3.28 Å) Ce–Ru bond lengths. There are a spread of Ce–Al bond distances ranging from 3.20–3.25 Å. In the third Ce site, Ce is bonded to three Ru and one Al atom to form distorted corner-sharing CeAlRu3 tetrahedra. There are two shorter (2.81 Å) and one longer (2.82 Å) Ce–Ru bond lengths. The Ce–Al bond length is 3.24 Å. In the fourth Ce site, Ce is bonded in a 2-coordinate geometry to four Ru and four Al atoms. There are a spread of Ce–Ru bond distances ranging from 2.76–3.29 Å. There are two shorter (3.21 Å) and two longer (3.24 Å) Ce–Al bond lengths. There are two inequivalent Ru sites. In the first Ru site, Ru is bonded in a 8-coordinate geometry to six Ce and two equivalent Al atoms. Both Ru–Al bond lengths are 2.62 Å. In the second Ru site, Ru is bonded in a 8-coordinate geometry to six Ce and two Al atoms. Both Ru–Al bond lengths are 2.62 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded in a 3-coordinate geometry to seven Ce and three equivalent Ru atoms. In the second Al site, Al is bonded in a 3-coordinate geometry to seven Ce and three Ru atoms.
DOI: 10.17188/1311140
title: Materials Data on CeAlAg2 by Materials Project

description: Ag2CeAl is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ce is bonded in a body-centered cubic geometry to eight equivalent Ag atoms. All Ce–Ag bond lengths are 3.03 Å. Ag is bonded in a body-centered cubic geometry to four equivalent Ce and four equivalent Al atoms. All Ag–Al bond lengths are 3.03 Å. Al is bonded in a distorted body-centered cubic geometry to eight equivalent Ag atoms.
DOI: 10.17188/1311141
title: Materials Data on LuReTc2 by Materials Project

description: LuReTc2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Lu3+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Lu–Tc bond lengths are 2.77 Å. Re3+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Re–Tc bond lengths are 2.77 Å. Tc3- is bonded to four equivalent Lu3+ and four equivalent Re3+ atoms to form a mixture of distorted edge, face, and corner-sharing TcLu4Re4 tetrahedra.