cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1310880
title: Materials Data on Y2MgAl by Materials Project

description: MgY2Al is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Y atoms. All Mg–Y bond lengths are 3.19 Å. Y is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Al atoms. All Y–Al bond lengths are 3.19 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310881
title: Materials Data on Y2IrRh by Materials Project

description: Y2IrRh is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Y is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Rh atoms. All Y–Ir bond lengths are 2.98 Å. All Y–Rh bond lengths are 2.98 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Rh is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310882
title: Materials Data on Li5Mg by Materials Project

description: Li5Mg crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. there are two inequivalent Li sites. In the first Li site, Li is bonded to ten Li and two equivalent Mg atoms to form LiLi10Mg2 cuboctahedra that share corners with eighteen equivalent LiLi10Mg2 cuboctahedra, edges with four equivalent MgLi12 cuboctahedra, edges with fourteen LiLi10Mg2 cuboctahedra, faces with four equivalent MgLi12 cuboctahedra, and faces with sixteen LiLi10Mg2 cuboctahedra. There are a spread of Li–Li bond distances ranging from 3.04–3.06 Å. Both Li–Mg bond lengths are 3.05 Å. In the second Li site, Li is bonded to nine Li and three equivalent Mg atoms to form LiLi9Mg3 cuboctahedra that share corners with nine equivalent LiLi9Mg3 cuboctahedra, corners with nine equivalent MgLi12 cuboctahedra, edges with eighteen LiLi10Mg2 cuboctahedra, faces with three equivalent MgLi12 cuboctahedra, and faces with seventeen LiLi10Mg2 cuboctahedra. All Li–Li bond lengths are 3.04 Å. All Li–Mg bond lengths are 3.04 Å. Mg is bonded to twelve Li atoms to form MgLi12 cuboctahedra that share corners with eighteen equivalent LiLi9Mg3 cuboctahedra, edges with six equivalent MgLi12 cuboctahedra, edges with twelve equivalent LiLi10Mg2 cuboctahedra, faces with two equivalent MgLi12 cuboctahedra, and faces with eighteen LiLi10Mg2 cuboctahedra.
DOI: 10.17188/1310883
title: Materials Data on YBr3 by Materials Project

description: YBr3 crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two YBr3 ribbons oriented in the (0, 0, 1) direction. Y3+ is bonded to six equivalent Br1- atoms to form distorted face-sharing YBr6 pentagonal pyramids. All Y–Br bond lengths are 2.83 Å. Br1- is bonded in an L-shaped geometry to two equivalent Y3+ atoms.
DOI: 10.17188/1310884
title: Materials Data on CsTaGeS5 by Materials Project

description: CsTaGeS5 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Cs1+ is bonded in a 10-coordinate geometry to ten S2- atoms. There are a spread of Cs–S bond distances ranging from 3.58–4.16 Å. Ta5+ is bonded to six S2- atoms to form TaS6 octahedra that share corners with two equivalent GeS4 tetrahedra and edges with two equivalent TaS6 octahedra. There are a spread of Ta–S bond distances ranging from 2.34–2.57 Å. Ge4+ is bonded to four S2- atoms to form GeS4 tetrahedra that share corners with two equivalent TaS6 octahedra and an edgeedge with one GeS4 tetrahedra. The corner-sharing octahedra tilt angles range from 71–74°. There are a spread of Ge–S bond distances ranging from 2.21–2.29 Å. There are five inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted L-shaped geometry to one Cs1+ and two equivalent Ta5+ atoms. In the second S2- site, S2- is bonded in a 2-coordinate geometry to two equivalent Cs1+ and two equivalent Ta5+ atoms. In the third S2- site, S2- is bonded in a distorted water-like geometry to three equivalent Cs1+, one Ta5+, and one Ge4+ atom. In the fourth S2- site, S2- is bonded in a distorted water-like geometry to two equivalent Cs1+, one Ta5+, and one Ge4+ atom. In the fifth S2- site, S2- is bonded in a 2-coordinate geometry to two equivalent Cs1+ and two equivalent Ge4+ atoms.
DOI: 10.17188/1310885
title: Materials Data on LuGaPd2 by Materials Project

description: LuPd2Ga 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 Pd atoms. All Lu–Pd bond lengths are 2.83 Å. Pd is bonded in a body-centered cubic geometry to four equivalent Lu and four equivalent Ga atoms. All Pd–Ga bond lengths are 2.83 Å. Ga is bonded in a distorted body-centered cubic geometry to eight equivalent Pd atoms.
DOI: 10.17188/1310887
title: Materials Data on LuPaOs2 by Materials Project

description: PaLuOs2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Os atoms. All Pa–Os bond lengths are 2.96 Å. Lu is bonded in a body-centered cubic geometry to eight equivalent Os atoms. All Lu–Os bond lengths are 2.96 Å. Os is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Lu atoms.
DOI: 10.17188/1310888
title: Materials Data on LuGaRh2 by Materials Project

description: LuRh2Ga 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 Rh atoms. All Lu–Rh bond lengths are 2.76 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Lu and four equivalent Ga atoms. All Rh–Ga bond lengths are 2.76 Å. Ga is bonded in a distorted body-centered cubic geometry to eight equivalent Rh atoms.
DOI: 10.17188/1310889
title: Materials Data on LuH3 by Materials Project

description: LuH3 is alpha bismuth trifluoride structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Lu3+ is bonded to twelve H1- atoms to form a mixture of distorted corner, edge, and face-sharing LuH12 cuboctahedra. There are eight shorter (2.18 Å) and four longer (2.37 Å) Lu–H bond lengths. There are two inequivalent H1- sites. In the first H1- site, H1- is bonded to four equivalent Lu3+ atoms to form a mixture of corner and edge-sharing HLu4 tetrahedra. In the second H1- site, H1- is bonded in a square co-planar geometry to four equivalent Lu3+ atoms.
DOI: 10.17188/1310890
title: Materials Data on MgRh3 by Materials Project

description: MgRh3 crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. Mg is bonded in a 12-coordinate geometry to ten Rh atoms. There are a spread of Mg–Rh bond distances ranging from 2.68–2.81 Å. There are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 12-coordinate geometry to three equivalent Mg atoms. In the second Rh site, Rh is bonded to four equivalent Mg atoms to form a mixture of distorted edge and corner-sharing RhMg4 cuboctahedra.
DOI: 10.17188/1310891
title: Materials Data on LiCd3 by Materials Project

description: LiCd3 is Uranium Silicide-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Li is bonded to twelve equivalent Cd atoms to form a mixture of face and corner-sharing LiCd12 cuboctahedra. There are six shorter (3.03 Å) and six longer (3.09 Å) Li–Cd bond lengths. Cd is bonded in a distorted see-saw-like geometry to four equivalent Li atoms.
DOI: 10.17188/1310892
title: Materials Data on GaSiRu2 by Materials Project

description: Ru2GaSi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ru is bonded in a body-centered cubic geometry to four equivalent Ga and four equivalent Si atoms. All Ru–Ga bond lengths are 2.58 Å. All Ru–Si bond lengths are 2.58 Å. Ga is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. Si is bonded in a body-centered cubic geometry to eight equivalent Ru atoms.
DOI: 10.17188/1310893
title: Materials Data on Yb2AgIr by Materials Project

description: Yb2IrAg 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 four equivalent Ir and four equivalent Ag atoms. All Yb–Ir bond lengths are 3.01 Å. All Yb–Ag bond lengths are 3.01 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Yb atoms. Ag is bonded in a body-centered cubic geometry to eight equivalent Yb atoms.
DOI: 10.17188/1310894
title: Materials Data on Li2HoIn by Materials Project

description: Li2HoIn 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 Ho and four equivalent In atoms. All Li–Ho bond lengths are 2.96 Å. All Li–In bond lengths are 2.96 Å. Ho is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent In atoms. All Ho–In bond lengths are 3.42 Å. In is bonded in a body-centered cubic geometry to eight equivalent Li and six equivalent Ho atoms.
DOI: 10.17188/1310895
title: Materials Data on Lu2IrRh by Materials Project

description: Lu2IrRh 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 four equivalent Ir and four equivalent Rh atoms. All Lu–Ir bond lengths are 2.91 Å. All Lu–Rh bond lengths are 2.91 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Lu atoms. Rh is bonded in a body-centered cubic geometry to eight equivalent Lu atoms.
DOI: 10.17188/1310896
title: Materials Data on Li2HoTl by Materials Project

description: Li2HoTl 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 Ho and four equivalent Tl atoms. All Li–Ho bond lengths are 2.96 Å. All Li–Tl bond lengths are 2.96 Å. Ho is bonded in a distorted body-centered cubic geometry to eight equivalent Li atoms. Tl is bonded in a body-centered cubic geometry to eight equivalent Li atoms.
DOI: 10.17188/1310897
title: Materials Data on Na2MgSn by Materials Project

description: Na2MgSn crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Na is bonded in a 11-coordinate geometry to four equivalent Na, three equivalent Mg, and four equivalent Sn atoms. There are three shorter (3.34 Å) and one longer (3.43 Å) Na–Na bond lengths. All Na–Mg bond lengths are 3.40 Å. There are one shorter (3.32 Å) and three longer (3.40 Å) Na–Sn bond lengths. Mg is bonded in a distorted trigonal planar geometry to six equivalent Na and three equivalent Sn atoms. All Mg–Sn bond lengths are 2.93 Å. Sn is bonded in a 11-coordinate geometry to eight equivalent Na and three equivalent Mg atoms.
DOI: 10.17188/1310898
title: Materials Data on Li2CeAl by Materials Project

description: Li2CeAl 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 Al atoms. All Li–Ce bond lengths are 2.96 Å. All Li–Al bond lengths are 2.96 Å. Ce is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent Al atoms. All Ce–Al bond lengths are 3.42 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Li and six equivalent Ce atoms.
DOI: 10.17188/1310899
title: Materials Data on Yb2AgGe by Materials Project

description: Yb2AgGe 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 four equivalent Ag and four equivalent Ge atoms. All Yb–Ag bond lengths are 3.12 Å. All Yb–Ge bond lengths are 3.12 Å. Ag is bonded in a body-centered cubic geometry to eight equivalent Yb atoms. Ge is bonded in a body-centered cubic geometry to eight equivalent Yb atoms.
DOI: 10.17188/1310900
title: Materials Data on LuPaRu2 by Materials Project

description: PaLuRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Pa–Ru bond lengths are 2.94 Å. Lu is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Lu–Ru bond lengths are 2.94 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Lu atoms.
DOI: 10.17188/1310901
title: Materials Data on TiGeRu2 by Materials Project

description: Ru2TiGe 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 Ru and six equivalent Ge atoms. All Ti–Ru bond lengths are 2.66 Å. All Ti–Ge bond lengths are 3.07 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Ti and four equivalent Ge atoms. All Ru–Ge bond lengths are 2.66 Å. Ge is bonded in a distorted body-centered cubic geometry to six equivalent Ti and eight equivalent Ru atoms.
DOI: 10.17188/1310902
title: Materials Data on Y2NiRu by Materials Project

description: Y2RuNi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Y is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Ni atoms. All Y–Ru bond lengths are 2.96 Å. All Y–Ni bond lengths are 2.96 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Ni is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310903
title: Materials Data on Yb2CdPb by Materials Project

description: Yb2CdPb 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 four equivalent Cd and four equivalent Pb atoms. All Yb–Cd bond lengths are 3.33 Å. All Yb–Pb bond lengths are 3.33 Å. Cd is bonded in a body-centered cubic geometry to eight equivalent Yb atoms. Pb is bonded in a body-centered cubic geometry to eight equivalent Yb atoms.
DOI: 10.17188/1310904
title: Materials Data on Ti2TcRh by Materials Project

description: Ti2TcRh 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 Rh atoms. All Ti–Tc bond lengths are 2.69 Å. All Ti–Rh bond lengths are 2.69 Å. Tc 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: 10.17188/1310905
title: Materials Data on Ti2TcRu by Materials Project

description: Ti2TcRu 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 Ru atoms. All Ti–Tc bond lengths are 2.68 Å. All Ti–Ru bond lengths are 2.68 Å. Tc is bonded in a distorted body-centered cubic geometry to eight equivalent Ti atoms. Ru is bonded in a body-centered cubic geometry to eight equivalent Ti atoms.
DOI: 10.17188/1310906
title: Materials Data on Y2TlCd by Materials Project

description: Y2CdTl is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Y is bonded in a body-centered cubic geometry to four equivalent Cd and four equivalent Tl atoms. All Y–Cd bond lengths are 3.27 Å. All Y–Tl bond lengths are 3.27 Å. Cd is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Tl is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310907
title: Materials Data on TiMn2Si by Materials Project

description: TiMn2Si is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a 8-coordinate geometry to eight equivalent Mn and six equivalent Si atoms. All Ti–Mn bond lengths are 2.51 Å. All Ti–Si bond lengths are 2.90 Å. Mn is bonded in a distorted body-centered cubic geometry to four equivalent Ti and four equivalent Si atoms. All Mn–Si bond lengths are 2.51 Å. Si is bonded in a distorted body-centered cubic geometry to six equivalent Ti and eight equivalent Mn atoms.
DOI: 10.17188/1310908
title: Materials Data on TiNbRe2 by Materials Project

description: TiNbRe2 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 Re atoms. All Ti–Re bond lengths are 2.75 Å. Nb is bonded in a body-centered cubic geometry to eight equivalent Re atoms. All Nb–Re bond lengths are 2.75 Å. Re is bonded in a body-centered cubic geometry to four equivalent Ti and four equivalent Nb atoms.
DOI: 10.17188/1310909
title: Materials Data on Y2TlAg by Materials Project

description: Y2AgTl is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Y is bonded in a body-centered cubic geometry to four equivalent Ag and four equivalent Tl atoms. All Y–Ag bond lengths are 3.23 Å. All Y–Tl bond lengths are 3.23 Å. Ag is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Tl is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310910
title: Materials Data on TiNbTc2 by Materials Project

description: TiNbTc2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti4+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Ti–Tc bond lengths are 2.73 Å. Nb2+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Nb–Tc bond lengths are 2.73 Å. Tc3- is bonded in a body-centered cubic geometry to four equivalent Ti4+ and four equivalent Nb2+ atoms.
DOI: 10.17188/1310911
title: Materials Data on TiMn2W by Materials Project

description: TiWMn2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a 8-coordinate geometry to six equivalent W and eight equivalent Mn atoms. All Ti–W bond lengths are 2.98 Å. All Ti–Mn bond lengths are 2.58 Å. W is bonded in a distorted body-centered cubic geometry to six equivalent Ti and eight equivalent Mn atoms. All W–Mn bond lengths are 2.58 Å. Mn is bonded to four equivalent Ti and four equivalent W atoms to form a mixture of distorted corner, edge, and face-sharing MnTi4W4 tetrahedra.
DOI: 10.17188/1310912
title: Materials Data on LiPrGe2 by Materials Project

description: LiPrGe2 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Li is bonded in a 5-coordinate geometry to five Ge atoms. There are a spread of Li–Ge bond distances ranging from 2.58–2.73 Å. Pr is bonded in a 6-coordinate geometry to nine Ge atoms. There are a spread of Pr–Ge bond distances ranging from 3.12–3.43 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to three equivalent Li, four equivalent Pr, and two equivalent Ge atoms. Both Ge–Ge bond lengths are 2.55 Å. In the second Ge site, Ge is bonded in a 1-coordinate geometry to two equivalent Li, five equivalent Pr, and two equivalent Ge atoms.
DOI: 10.17188/1310913
title: Materials Data on Y2ZnIr by Materials Project

description: Y2IrZn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Y is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Zn atoms. All Y–Ir bond lengths are 3.03 Å. All Y–Zn bond lengths are 3.03 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Zn is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310914
title: Materials Data on Yb2AgPt by Materials Project

description: Yb2PtAg 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 four equivalent Pt and four equivalent Ag atoms. All Yb–Pt bond lengths are 3.06 Å. All Yb–Ag bond lengths are 3.06 Å. Pt is bonded in a body-centered cubic geometry to eight equivalent Yb atoms. Ag is bonded in a body-centered cubic geometry to eight equivalent Yb atoms.
DOI: 10.17188/1310915
title: Materials Data on Yb2AgPb by Materials Project

description: Yb2AgPb 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 four equivalent Ag and four equivalent Pb atoms. All Yb–Ag bond lengths are 3.27 Å. All Yb–Pb bond lengths are 3.27 Å. Ag is bonded in a body-centered cubic geometry to eight equivalent Yb atoms. Pb is bonded in a body-centered cubic geometry to eight equivalent Yb atoms.
DOI: 10.17188/1310916
title: Materials Data on YbLuRh2 by Materials Project

description: LuYbRh2 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 Rh atoms. All Lu–Rh bond lengths are 2.89 Å. Yb is bonded in a body-centered cubic geometry to eight equivalent Rh atoms. All Yb–Rh bond lengths are 2.89 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Lu and four equivalent Yb atoms.
DOI: 10.17188/1310917
title: Materials Data on TiRe2W by Materials Project

description: TiWRe2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a distorted body-centered cubic geometry to six equivalent W and eight equivalent Re atoms. All Ti–W bond lengths are 3.14 Å. All Ti–Re bond lengths are 2.72 Å. W is bonded in a distorted body-centered cubic geometry to six equivalent Ti and eight equivalent Re atoms. All W–Re bond lengths are 2.72 Å. Re is bonded in a body-centered cubic geometry to four equivalent Ti and four equivalent W atoms.
DOI: 10.17188/1310918
title: Materials Data on Li2TlAg by Materials Project

description: Li2AgTl 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 Ag and four equivalent Tl atoms. All Li–Ag bond lengths are 2.87 Å. All Li–Tl bond lengths are 2.87 Å. Ag is bonded in a body-centered cubic geometry to eight equivalent Li atoms. Tl is bonded in a body-centered cubic geometry to eight equivalent Li atoms.
DOI: 10.17188/1310919
title: Materials Data on TiSiTc2 by Materials Project

description: TiTc2Si is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti2+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Ti–Tc bond lengths are 2.63 Å. Tc3- is bonded in a 8-coordinate geometry to four equivalent Ti2+ and four equivalent Si4+ atoms. All Tc–Si bond lengths are 2.63 Å. Si4+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms.
DOI: 10.17188/1310920
title: Materials Data on Y2ZnIn by Materials Project

description: Y2ZnIn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Y is bonded in a body-centered cubic geometry to four equivalent Zn and four equivalent In atoms. All Y–Zn bond lengths are 3.19 Å. All Y–In bond lengths are 3.19 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Y atoms. In is bonded in a body-centered cubic geometry to eight equivalent Y atoms.