cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1309258
title: Materials Data on LiRu2W by Materials Project

description: LiWRu2 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 six equivalent W and eight equivalent Ru atoms. All Li–W bond lengths are 3.03 Å. All Li–Ru bond lengths are 2.62 Å. W is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Ru atoms. All W–Ru bond lengths are 2.62 Å. Ru is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent W atoms.
DOI: 10.17188/1309259
title: Materials Data on LiSbRh2 by Materials Project

description: LiRh2Sb 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 Rh and six equivalent Sb atoms. All Li–Rh bond lengths are 2.68 Å. All Li–Sb bond lengths are 3.10 Å. Rh is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Sb atoms. All Rh–Sb bond lengths are 2.68 Å. Sb is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Rh atoms.
DOI: 10.17188/1309260
title: Materials Data on Ti2FeIr by Materials Project

description: Ti2FeIr 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 Fe and four equivalent Ir atoms. All Ti–Fe bond lengths are 2.65 Å. All Ti–Ir bond lengths are 2.65 Å. Fe is bonded in a distorted body-centered cubic geometry to eight equivalent Ti atoms. Ir is bonded in a body-centered cubic geometry to eight equivalent Ti atoms.
DOI: 10.17188/1309261
title: Materials Data on Ac2AgIr by Materials Project

description: Ac2IrAg 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 Ag atoms. All Ac–Ir bond lengths are 3.31 Å. All Ac–Ag bond lengths are 3.31 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Ac atoms. Ag is bonded in a body-centered cubic geometry to eight equivalent Ac atoms.
DOI: 10.17188/1309262
title: Materials Data on LiTl2Rh by Materials Project

description: LiRhTl2 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 Tl atoms. All Li–Tl bond lengths are 2.92 Å. Rh is bonded in a body-centered cubic geometry to eight equivalent Tl atoms. All Rh–Tl bond lengths are 2.92 Å. Tl is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Rh atoms.
DOI: 10.17188/1309263
title: Materials Data on PuBiPd2 by Materials Project

description: PuPd2Bi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pu is bonded in a body-centered cubic geometry to eight equivalent Pd and six equivalent Bi atoms. All Pu–Pd bond lengths are 3.00 Å. All Pu–Bi bond lengths are 3.46 Å. Pd is bonded in a body-centered cubic geometry to four equivalent Pu and four equivalent Bi atoms. All Pd–Bi bond lengths are 3.00 Å. Bi is bonded in a distorted body-centered cubic geometry to six equivalent Pu and eight equivalent Pd atoms.
DOI: 10.17188/1309264
title: Materials Data on PuBr2 by Materials Project

description: PuBr2 is Rutile structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Pu is bonded to six equivalent Br atoms to form a mixture of edge and corner-sharing PuBr6 octahedra. The corner-sharing octahedral tilt angles are 45°. There are four shorter (2.99 Å) and two longer (3.02 Å) Pu–Br bond lengths. Br is bonded in a distorted T-shaped geometry to three equivalent Pu atoms.
DOI: 10.17188/1309265
title: Materials Data on PuSbPd2 by Materials Project

description: PuPd2Sb is Heusler structured and crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Pu is bonded in a distorted body-centered cubic geometry to eight equivalent Pd and six equivalent Sb atoms. There are four shorter (2.95 Å) and four longer (2.96 Å) Pu–Pd bond lengths. There are four shorter (3.41 Å) and two longer (3.42 Å) Pu–Sb bond lengths. Pd is bonded in a body-centered cubic geometry to four equivalent Pu and four equivalent Sb atoms. There are two shorter (2.95 Å) and two longer (2.96 Å) Pd–Sb bond lengths. Sb is bonded in a 8-coordinate geometry to six equivalent Pu and eight equivalent Pd atoms.
DOI: 10.17188/1309266
title: Materials Data on LiTePd2 by Materials Project

description: LiPd2Te 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 Pd and six equivalent Te atoms. All Li–Pd bond lengths are 2.80 Å. All Li–Te bond lengths are 3.23 Å. Pd is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Te atoms. All Pd–Te bond lengths are 2.80 Å. Te is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Pd atoms.
DOI: 10.17188/1309267
title: Materials Data on AcZnAu2 by Materials Project

description: AcAu2Zn 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 3.17 Å. Au is bonded in a body-centered cubic geometry to four equivalent Ac and four equivalent Zn atoms. All Au–Zn bond lengths are 3.17 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Au atoms.
DOI: 10.17188/1309268
title: Materials Data on AcMgTl2 by Materials Project

description: MgAcTl2 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 Tl atoms. All Mg–Tl bond lengths are 3.40 Å. Ac is bonded in a body-centered cubic geometry to eight equivalent Tl atoms. All Ac–Tl bond lengths are 3.40 Å. Tl is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Ac atoms.
DOI: 10.17188/1309269
title: Materials Data on LiSbPd2 by Materials Project

description: LiPd2Sb 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 Pd and six equivalent Sb atoms. All Li–Pd bond lengths are 2.76 Å. All Li–Sb bond lengths are 3.19 Å. Pd is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Sb atoms. All Pd–Sb bond lengths are 2.76 Å. Sb is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Pd atoms.
DOI: 10.17188/1309270
title: Materials Data on CaMgPb by Materials Project

description: CaMgPb crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Ca is bonded in a 5-coordinate geometry to five equivalent Pb atoms. There are a spread of Ca–Pb bond distances ranging from 3.32–3.44 Å. Mg is bonded to four equivalent Pb atoms to form a mixture of distorted edge and corner-sharing MgPb4 tetrahedra. There are a spread of Mg–Pb bond distances ranging from 2.96–3.07 Å. Pb is bonded in a 9-coordinate geometry to five equivalent Ca and four equivalent Mg atoms.
DOI: 10.17188/1309271
title: Materials Data on Pu2HgBi by Materials Project

description: Pu2HgBi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pu is bonded in a body-centered cubic geometry to four equivalent Hg and four equivalent Bi atoms. All Pu–Hg bond lengths are 3.32 Å. All Pu–Bi bond lengths are 3.32 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Pu atoms. Bi is bonded in a body-centered cubic geometry to eight equivalent Pu atoms.
DOI: 10.17188/1309273
title: Materials Data on AcI3 by Materials Project

description: AcI3 crystallizes in the hexagonal P6_3/mmc space group. The structure is one-dimensional and consists of two AcI3 ribbons oriented in the (0, 0, 1) direction. Ac3+ is bonded to six equivalent I1- atoms to form distorted face-sharing AcI6 pentagonal pyramids. All Ac–I bond lengths are 3.29 Å. I1- is bonded in an L-shaped geometry to two equivalent Ac3+ atoms.
DOI: 10.17188/1309274
title: Materials Data on KNaLaTaO5 by Materials Project

description: LaKNaTaO5 crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. K1+ is bonded in a distorted square co-planar geometry to four equivalent O2- atoms. All K–O bond lengths are 2.94 Å. Na1+ is bonded to five O2- atoms to form distorted NaO5 trigonal bipyramids that share corners with five equivalent TaO5 trigonal bipyramids. There are one shorter (2.28 Å) and four longer (2.35 Å) Na–O bond lengths. La3+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All La–O bond lengths are 2.54 Å. Ta5+ is bonded to five O2- atoms to form distorted TaO5 trigonal bipyramids that share corners with five equivalent NaO5 trigonal bipyramids. There is one shorter (1.86 Å) and four longer (1.98 Å) Ta–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent K1+, one Na1+, and one Ta5+ atom to form a mixture of distorted edge and corner-sharing OK4NaTa octahedra. The corner-sharing octahedral tilt angles are 10°. In the second O2- site, O2- is bonded in a 4-coordinate geometry to one Na1+, two equivalent La3+, and one Ta5+ atom.
DOI: 10.17188/1309275
title: Materials Data on CaLuRh2 by Materials Project

description: CaLuRh2 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 Rh atoms. All Ca–Rh bond lengths are 2.93 Å. Lu is bonded in a body-centered cubic geometry to eight equivalent Rh atoms. All Lu–Rh bond lengths are 2.93 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent Lu atoms.
DOI: 10.17188/1309276
title: Materials Data on SeI2 by Materials Project

description: SeI2 crystallizes in the tetragonal P4_2/mnm space group. The structure is one-dimensional and consists of two SeI2 ribbons oriented in the (0, 0, 1) direction. Se is bonded in a square co-planar geometry to four equivalent I atoms. All Se–I bond lengths are 2.82 Å. I is bonded in an L-shaped geometry to two equivalent Se atoms.
DOI: 10.17188/1309277
title: Materials Data on Ac2HgGe by Materials Project

description: Ac2HgGe 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 Hg and four equivalent Ge atoms. All Ac–Hg bond lengths are 3.44 Å. All Ac–Ge bond lengths are 3.44 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Ac atoms. Ge is bonded in a body-centered cubic geometry to eight equivalent Ac atoms.
DOI: 10.17188/1309278
title: Materials Data on TaTlO3 by Materials Project

description: TlTaO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Ta5+ is bonded to six equivalent O2- atoms to form TaO6 octahedra that share corners with six equivalent TaO6 octahedra and faces with eight equivalent TlO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ta–O bond lengths are 2.04 Å. Tl1+ is bonded to twelve equivalent O2- atoms to form TlO12 cuboctahedra that share corners with twelve equivalent TlO12 cuboctahedra, faces with six equivalent TlO12 cuboctahedra, and faces with eight equivalent TaO6 octahedra. All Tl–O bond lengths are 2.89 Å. O2- is bonded in a distorted linear geometry to two equivalent Ta5+ and four equivalent Tl1+ atoms.
DOI: 10.17188/1309279
title: Materials Data on LiHoHg2 by Materials Project

description: LiHoHg2 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 Hg atoms. All Li–Hg bond lengths are 3.07 Å. Ho is bonded in a body-centered cubic geometry to eight equivalent Hg atoms. All Ho–Hg bond lengths are 3.07 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ho atoms.
DOI: 10.17188/1309280
title: Materials Data on LiHf2Re by Materials Project

description: LiHf2Re 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 Hf and six equivalent Re atoms. All Li–Hf bond lengths are 2.84 Å. All Li–Re bond lengths are 3.28 Å. Hf is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Re atoms. All Hf–Re bond lengths are 2.84 Å. Re is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Hf atoms.
DOI: 10.17188/1309281
title: Materials Data on LiAc2Si by Materials Project

description: LiAc2Si 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 Ac atoms. All Li–Ac bond lengths are 3.37 Å. Ac is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Si atoms. All Ac–Si bond lengths are 3.37 Å. Si is bonded in a body-centered cubic geometry to eight equivalent Ac atoms.
DOI: 10.17188/1309282
title: Materials Data on CdSnRh2 by Materials Project

description: Rh2CdSn 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 four equivalent Cd and four equivalent Sn atoms. All Rh–Cd bond lengths are 2.80 Å. All Rh–Sn bond lengths are 2.80 Å. Cd is bonded in a body-centered cubic geometry to eight equivalent Rh atoms. Sn is bonded in a distorted body-centered cubic geometry to eight equivalent Rh atoms.
DOI: 10.17188/1309283
title: Materials Data on Cd2AgRh by Materials Project

description: RhAgCd2 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 2.87 Å. Ag is bonded in a distorted body-centered cubic geometry to eight equivalent Cd atoms. All Ag–Cd bond lengths are 2.87 Å. Cd is bonded in a body-centered cubic geometry to four equivalent Rh and four equivalent Ag atoms.
DOI: 10.17188/1309284
title: Materials Data on AcCdRh2 by Materials Project

description: AcRh2Cd 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 Rh atoms. All Ac–Rh bond lengths are 3.01 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Ac and four equivalent Cd atoms. All Rh–Cd bond lengths are 3.01 Å. Cd is bonded in a distorted body-centered cubic geometry to eight equivalent Rh atoms.
DOI: 10.17188/1309285
title: Materials Data on LiGeAu2 by Materials Project

description: LiAu2Ge 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 2.80 Å. Au is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ge atoms. All Au–Ge bond lengths are 2.80 Å. Ge is bonded in a body-centered cubic geometry to eight equivalent Au atoms.
DOI: 10.17188/1309286
title: Materials Data on LiGeIr2 by Materials Project

description: LiIr2Ge 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 Ge atoms. All Li–Ir bond lengths are 2.57 Å. All Li–Ge bond lengths are 2.97 Å. Ir is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Ge atoms. All Ir–Ge bond lengths are 2.57 Å. Ge is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Ir atoms.
DOI: 10.17188/1309287
title: Materials Data on Ac2CuIr by Materials Project

description: Ac2IrCu 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 Cu atoms. All Ac–Ir bond lengths are 3.24 Å. All Ac–Cu bond lengths are 3.24 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Ac atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Ac atoms.
DOI: 10.17188/1309288
title: Materials Data on AcGaTe2 by Materials Project

description: AcTe2Ga is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of four gallium molecules and one AcTe2 framework. In the AcTe2 framework, Ac is bonded in a body-centered cubic geometry to eight equivalent Te atoms. All Ac–Te bond lengths are 3.46 Å. Te is bonded to four equivalent Ac atoms to form a mixture of corner and edge-sharing TeAc4 tetrahedra.
DOI: 10.17188/1309289
title: Materials Data on LiDyAu2 by Materials Project

description: LiDyAu2 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 2.98 Å. Dy is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Dy–Au bond lengths are 2.98 Å. Au is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Dy atoms.
DOI: 10.17188/1309290
title: Materials Data on LiDyHg2 by Materials Project

description: LiDyHg2 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 Hg atoms. All Li–Hg bond lengths are 3.08 Å. Dy is bonded in a body-centered cubic geometry to eight equivalent Hg atoms. All Dy–Hg bond lengths are 3.08 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Dy atoms.
DOI: 10.17188/1309291
title: Materials Data on CeBiAu2 by Materials Project

description: CeAu2Bi 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 Au atoms. All Ce–Au bond lengths are 3.16 Å. Au is bonded in a body-centered cubic geometry to four equivalent Ce and four equivalent Bi atoms. All Au–Bi bond lengths are 3.16 Å. Bi is bonded in a distorted body-centered cubic geometry to eight equivalent Au atoms.
DOI: 10.17188/1309292
title: Materials Data on Sc3Tc by Materials Project

description: Sc3Tc is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Sc is bonded to eight equivalent Sc and four equivalent Tc atoms to form distorted ScSc8Tc4 cuboctahedra that share corners with four equivalent TcSc12 cuboctahedra, corners with fourteen equivalent ScSc8Tc4 cuboctahedra, edges with six equivalent TcSc12 cuboctahedra, edges with twelve equivalent ScSc8Tc4 cuboctahedra, faces with four equivalent TcSc12 cuboctahedra, and faces with sixteen equivalent ScSc8Tc4 cuboctahedra. There are six shorter (3.03 Å) and two longer (3.22 Å) Sc–Sc bond lengths. There are two shorter (2.96 Å) and two longer (3.13 Å) Sc–Tc bond lengths. Tc is bonded to twelve equivalent Sc atoms to form TcSc12 cuboctahedra that share corners with six equivalent TcSc12 cuboctahedra, corners with twelve equivalent ScSc8Tc4 cuboctahedra, edges with eighteen equivalent ScSc8Tc4 cuboctahedra, faces with eight equivalent TcSc12 cuboctahedra, and faces with twelve equivalent ScSc8Tc4 cuboctahedra.
DOI: 10.17188/1309293
title: Materials Data on SeBr2 by Materials Project

description: SeBr2 crystallizes in the tetragonal P4_2/mnm space group. The structure is one-dimensional and consists of two SeBr2 ribbons oriented in the (0, 0, 1) direction. Se is bonded in a square co-planar geometry to four equivalent Br atoms. All Se–Br bond lengths are 2.62 Å. Br is bonded in an L-shaped geometry to two equivalent Se atoms.
DOI: 10.17188/1309294
title: Materials Data on DyInRh2 by Materials Project

description: DyRh2In is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to eight equivalent Rh atoms. All Dy–Rh bond lengths are 2.88 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Dy and four equivalent In atoms. All Rh–In bond lengths are 2.88 Å. In is bonded in a distorted body-centered cubic geometry to eight equivalent Rh atoms.
DOI: 10.17188/1309295
title: Materials Data on Li2LaPb by Materials Project

description: Li2LaPb 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 La and four equivalent Pb atoms. All Li–La bond lengths are 3.09 Å. All Li–Pb bond lengths are 3.09 Å. La is bonded in a 8-coordinate geometry to eight equivalent Li and six equivalent Pb atoms. All La–Pb bond lengths are 3.57 Å. Pb is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent La atoms.
DOI: 10.17188/1309296
title: Materials Data on Li2LaSn by Materials Project

description: Li2LaSn 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 La and four equivalent Sn atoms. All Li–La bond lengths are 3.05 Å. All Li–Sn bond lengths are 3.05 Å. La is bonded in a 8-coordinate geometry to eight equivalent Li and six equivalent Sn atoms. All La–Sn bond lengths are 3.52 Å. Sn is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent La atoms.
DOI: 10.17188/1309297
title: Materials Data on LiHg2Pd by Materials Project

description: LiPdHg2 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 six equivalent Pd and eight equivalent Hg atoms. All Li–Pd bond lengths are 3.32 Å. All Li–Hg bond lengths are 2.88 Å. Pd is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Hg atoms. All Pd–Hg bond lengths are 2.88 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Pd atoms.