cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1311863
title: Materials Data on Sr2HgPb by Materials Project

description: Sr2HgPb is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sr is bonded in a body-centered cubic geometry to four equivalent Hg and four equivalent Pb atoms. All Sr–Hg bond lengths are 3.54 Å. All Sr–Pb bond lengths are 3.54 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Sr atoms. Pb is bonded in a body-centered cubic geometry to eight equivalent Sr atoms.
DOI: 10.17188/1311864
title: Materials Data on Sr2LiIn by Materials Project

description: LiSr2In 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 Sr atoms. All Li–Sr bond lengths are 3.56 Å. Sr is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent In atoms. All Sr–In bond lengths are 3.56 Å. In is bonded in a body-centered cubic geometry to eight equivalent Sr atoms.
DOI: 10.17188/1311874
title: Materials Data on LiCa2Hg by Materials Project

description: LiCa2Hg 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 Ca atoms. All Li–Ca bond lengths are 3.31 Å. Ca is bonded to four equivalent Li and four equivalent Hg atoms to form a mixture of distorted face, edge, and corner-sharing CaLi4Hg4 tetrahedra. All Ca–Hg bond lengths are 3.31 Å. Hg is bonded in a body-centered cubic geometry to eight equivalent Ca atoms.
DOI: 10.17188/1311875
title: Materials Data on LiCa2In by Materials Project

description: LiCa2In 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 Ca atoms. All Li–Ca bond lengths are 3.35 Å. Ca is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent In atoms. All Ca–In bond lengths are 3.35 Å. In is bonded in a body-centered cubic geometry to eight equivalent Ca atoms.
DOI: 10.17188/1311876
title: Materials Data on TcOs3 by Materials Project

description: TcOs3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Tc3- is bonded to twelve equivalent Os1+ atoms to form a mixture of face and corner-sharing TcOs12 cuboctahedra. There are six shorter (2.70 Å) and six longer (2.76 Å) Tc–Os bond lengths. Os1+ is bonded in a see-saw-like geometry to four equivalent Tc3- atoms.
DOI: 10.17188/1311877
title: Materials Data on Er2OsPd by Materials Project

description: Er2OsPd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Er is bonded in a body-centered cubic geometry to four equivalent Os and four equivalent Pd atoms. All Er–Os bond lengths are 2.96 Å. All Er–Pd bond lengths are 2.96 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Er atoms. Pd is bonded in a body-centered cubic geometry to eight equivalent Er atoms.
DOI: 10.17188/1311878
title: Materials Data on Er2IrRu by Materials Project

description: Er2RuIr is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Er is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Ir atoms. All Er–Ru bond lengths are 2.93 Å. All Er–Ir bond lengths are 2.93 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Er atoms. Ir is bonded in a body-centered cubic geometry to eight equivalent Er atoms.
DOI: 10.17188/1311879
title: Materials Data on Sc3OsC4 by Materials Project

description: Sc3OsC4 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are four inequivalent Sc3+ sites. In the first Sc3+ site, Sc3+ is bonded to eight C2- atoms to form distorted ScC8 hexagonal bipyramids that share corners with eight CSc5OsC pentagonal bipyramids and faces with two equivalent ScOs4C8 cuboctahedra. There are four shorter (2.42 Å) and four longer (2.43 Å) Sc–C bond lengths. In the second Sc3+ site, Sc3+ is bonded to four equivalent Os1- and eight C2- atoms to form ScOs4C8 cuboctahedra that share corners with eight CSc5OsC pentagonal bipyramids, edges with two equivalent ScOs4C8 cuboctahedra, edges with eight CSc5OsC pentagonal bipyramids, and faces with two equivalent ScC8 hexagonal bipyramids. All Sc–Os bond lengths are 2.75 Å. There are four shorter (2.41 Å) and four longer (2.42 Å) Sc–C bond lengths. In the third Sc3+ site, Sc3+ is bonded in a 6-coordinate geometry to six C2- atoms. There are a spread of Sc–C bond distances ranging from 2.37–2.40 Å. In the fourth Sc3+ site, Sc3+ is bonded in a 6-coordinate geometry to six C2- atoms. There are a spread of Sc–C bond distances ranging from 2.36–2.40 Å. Os1- is bonded in a distorted square co-planar geometry to two equivalent Sc3+ and four C2- atoms. All Os–C bond lengths are 2.20 Å. There are two inequivalent C2- sites. In the first C2- site, C2- is bonded to five Sc3+, one Os1-, and one C2- atom to form distorted CSc5OsC pentagonal bipyramids that share a cornercorner with one ScOs4C8 cuboctahedra, a cornercorner with one ScC8 hexagonal bipyramid, corners with thirteen CSc5OsC pentagonal bipyramids, an edgeedge with one ScOs4C8 cuboctahedra, edges with five CSc5OsC pentagonal bipyramids, and faces with three CSc5OsC pentagonal bipyramids. The C–C bond length is 1.44 Å. In the second C2- site, C2- is bonded to five Sc3+, one Os1-, and one C2- atom to form distorted CSc5OsC pentagonal bipyramids that share a cornercorner with one ScOs4C8 cuboctahedra, a cornercorner with one ScC8 hexagonal bipyramid, corners with thirteen CSc5OsC pentagonal bipyramids, an edgeedge with one ScOs4C8 cuboctahedra, edges with five CSc5OsC pentagonal bipyramids, and faces with three CSc5OsC pentagonal bipyramids. The C–C bond length is 1.44 Å.
DOI: 10.17188/1311880
title: Materials Data on TaFeRu2 by Materials Project

description: TaRu2Fe is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ta is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ta–Ru bond lengths are 2.68 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Ta and four equivalent Fe atoms. All Ru–Fe bond lengths are 2.68 Å. Fe is bonded in a distorted body-centered cubic geometry to eight equivalent Ru atoms.
DOI: 10.17188/1311881
title: Materials Data on CaPrHg2 by Materials Project

description: CaPrHg2 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 3.32 Å. Pr is bonded in a body-centered cubic geometry to eight equivalent Hg atoms. All Pr–Hg bond lengths are 3.32 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent Pr atoms.
DOI: 10.17188/1311882
title: Materials Data on SmAgHg2 by Materials Project

description: SmAgHg2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sm is bonded in a distorted body-centered cubic geometry to six equivalent Ag and eight equivalent Hg atoms. All Sm–Ag bond lengths are 3.60 Å. All Sm–Hg bond lengths are 3.12 Å. Ag is bonded in a 8-coordinate geometry to six equivalent Sm and eight equivalent Hg atoms. All Ag–Hg bond lengths are 3.12 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Sm and four equivalent Ag atoms.
DOI: 10.17188/1311883
title: Materials Data on Sr2GaGeN by Materials Project

description: Sr2GaGeN crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are two inequivalent Sr sites. In the first Sr site, Sr is bonded in a 3-coordinate geometry to two equivalent Ge and three equivalent N atoms. Both Sr–Ge bond lengths are 3.41 Å. There are one shorter (2.52 Å) and two longer (2.78 Å) Sr–N bond lengths. In the second Sr site, Sr is bonded in a 2-coordinate geometry to three equivalent Ge and two equivalent N atoms. All Sr–Ge bond lengths are 3.38 Å. Both Sr–N bond lengths are 2.73 Å. Ga is bonded in a distorted single-bond geometry to two equivalent Ge and one N atom. Both Ga–Ge bond lengths are 2.49 Å. The Ga–N bond length is 1.89 Å. Ge is bonded in a 7-coordinate geometry to five Sr and two equivalent Ga atoms. N is bonded to five Sr and one Ga atom to form distorted edge-sharing NSr5Ga octahedra.
DOI: 10.17188/1311884
title: Materials Data on LiTm2Ir by Materials Project

description: LiTm2Ir 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 Tm atoms. All Li–Tm bond lengths are 2.97 Å. Tm is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ir atoms. All Tm–Ir bond lengths are 2.97 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Tm atoms.
DOI: 10.17188/1311885
title: Materials Data on Ce3(TaN3)2 by Materials Project

description: Ce3(TaN3)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are two inequivalent Ce3+ sites. In the first Ce3+ site, Ce3+ is bonded in a body-centered cubic geometry to eight equivalent N3- atoms. All Ce–N bond lengths are 2.60 Å. In the second Ce3+ site, Ce3+ is bonded in a 1-coordinate geometry to nine N3- atoms. There are a spread of Ce–N bond distances ranging from 2.30–2.89 Å. Ta+4.50+ is bonded to five N3- atoms to form corner-sharing TaN5 square pyramids. There are one shorter (1.98 Å) and four longer (2.05 Å) Ta–N bond lengths. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded to four Ce3+ and two equivalent Ta+4.50+ atoms to form a mixture of distorted face, edge, and corner-sharing NCe4Ta2 octahedra. The corner-sharing octahedra tilt angles range from 0–67°. In the second N3- site, N3- is bonded in a distorted linear geometry to five equivalent Ce3+ and one Ta+4.50+ atom.
DOI: 10.17188/1311886
title: Materials Data on LiCa2Ir by Materials Project

description: LiCa2Ir 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 Ca atoms. All Li–Ca bond lengths are 3.06 Å. Ca is bonded to four equivalent Li and four equivalent Ir atoms to form a mixture of distorted edge, face, and corner-sharing CaLi4Ir4 tetrahedra. All Ca–Ir bond lengths are 3.06 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Ca atoms.
DOI: 10.17188/1311887
title: Materials Data on LiGa2Ni by Materials Project

description: LiNiGa2 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 Ni and eight equivalent Ga atoms. All Li–Ni bond lengths are 2.96 Å. All Li–Ga bond lengths are 2.57 Å. Ni is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Ga atoms. All Ni–Ga bond lengths are 2.57 Å. Ga is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Ni atoms.
DOI: 10.17188/1311888
title: Materials Data on CaNdCd2 by Materials Project

description: CaNdCd2 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 Cd atoms. All Ca–Cd bond lengths are 3.34 Å. Nd is bonded in a body-centered cubic geometry to eight equivalent Cd atoms. All Nd–Cd bond lengths are 3.34 Å. Cd is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent Nd atoms.
DOI: 10.17188/1311889
title: Materials Data on LaCdAg2 by Materials Project

description: LaAg2Cd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. La is bonded in a body-centered cubic geometry to eight equivalent Ag and six equivalent Cd atoms. All La–Ag bond lengths are 3.15 Å. All La–Cd bond lengths are 3.63 Å. Ag is bonded in a body-centered cubic geometry to four equivalent La and four equivalent Cd atoms. All Ag–Cd bond lengths are 3.15 Å. Cd is bonded in a distorted body-centered cubic geometry to six equivalent La and eight equivalent Ag atoms.
DOI: 10.17188/1311890
title: Materials Data on Li3In by Materials Project

description: Li3In is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Li sites. In the first Li site, Li is bonded to four equivalent Li and four equivalent In atoms to form a mixture of distorted face, edge, and corner-sharing LiLi4In4 tetrahedra. All Li–Li bond lengths are 2.88 Å. All Li–In bond lengths are 2.88 Å. In the second Li site, Li is bonded in a 8-coordinate geometry to eight equivalent Li and six equivalent In atoms. All Li–In bond lengths are 3.33 Å. In is bonded in a body-centered cubic geometry to fourteen Li atoms.
DOI: 10.17188/1311891
title: Materials Data on Li3Pt by Materials Project

description: Li3Pt is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent Li sites. In the first Li site, Li is bonded to four equivalent Li and four equivalent Pt atoms to form a mixture of distorted edge, corner, and face-sharing LiLi4Pt4 tetrahedra. All Li–Li bond lengths are 2.63 Å. All Li–Pt bond lengths are 2.63 Å. In the second Li site, Li is bonded in a 8-coordinate geometry to eight equivalent Li and six equivalent Pt atoms. All Li–Pt bond lengths are 3.04 Å. Pt is bonded in a distorted body-centered cubic geometry to fourteen Li atoms.
DOI: 10.17188/1311892
title: Materials Data on K2Mn(PSe3)2 (SG:14) 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: 10.17188/1311893
title: Materials Data on RbSn3 by Materials Project

description: RbSn3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Rb is bonded in a 12-coordinate geometry to twelve equivalent Sn atoms. There are six shorter (3.94 Å) and six longer (4.01 Å) Rb–Sn bond lengths. Sn is bonded in a 10-coordinate geometry to four equivalent Rb and six equivalent Sn atoms. There are two shorter (3.07 Å) and four longer (3.27 Å) Sn–Sn bond lengths.
DOI: 10.17188/1311894
title: Materials Data on TbB4Ru by Materials Project

description: TbRuB4 crystallizes in the orthorhombic Pbam space group. The structure is three-dimensional. Tb3+ is bonded in a 2-coordinate geometry to fourteen B+1.50- atoms. There are a spread of Tb–B bond distances ranging from 2.65–2.78 Å. Ru3+ is bonded in a 10-coordinate geometry to ten B+1.50- atoms. There are a spread of Ru–B bond distances ranging from 2.27–2.41 Å. There are four inequivalent B+1.50- sites. In the first B+1.50- site, B+1.50- is bonded in a 9-coordinate geometry to four equivalent Tb3+, two equivalent Ru3+, and three B+1.50- atoms. There are a spread of B–B bond distances ranging from 1.76–1.87 Å. In the second B+1.50- site, B+1.50- is bonded in a 9-coordinate geometry to four equivalent Tb3+, two equivalent Ru3+, and three B+1.50- atoms. The B–B bond length is 1.84 Å. In the third B+1.50- site, B+1.50- is bonded in a 9-coordinate geometry to four equivalent Tb3+, two equivalent Ru3+, and three B+1.50- atoms. There is one shorter (1.75 Å) and one longer (1.78 Å) B–B bond length. In the fourth B+1.50- site, B+1.50- is bonded in a 9-coordinate geometry to two equivalent Tb3+, four equivalent Ru3+, and three B+1.50- atoms. The B–B bond length is 1.72 Å.
DOI: 10.17188/1311895
title: Materials Data on TbI3 (SG:194) 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: 10.17188/1311896
title: Materials Data on TbAl3 by Materials Project

description: TbAl3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Tb is bonded to twelve equivalent Al atoms to form a mixture of distorted corner and face-sharing TbAl12 cuboctahedra. There are six shorter (3.08 Å) and six longer (3.16 Å) Tb–Al bond lengths. Al is bonded in a 10-coordinate geometry to four equivalent Tb and six equivalent Al atoms. There are two shorter (2.76 Å) and four longer (2.81 Å) Al–Al bond lengths.
DOI: 10.17188/1311897
title: Materials Data on Sc2ZnIr by Materials Project

description: Sc2IrZn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sc is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Zn atoms. All Sc–Ir bond lengths are 2.84 Å. All Sc–Zn bond lengths are 2.84 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Sc atoms. Zn is bonded in a body-centered cubic geometry to eight equivalent Sc atoms.
DOI: 10.17188/1311898
title: Materials Data on TbMgHg2 by Materials Project

description: MgTbHg2 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 Hg atoms. All Mg–Hg bond lengths are 3.12 Å. Tb is bonded in a body-centered cubic geometry to eight equivalent Hg atoms. All Tb–Hg bond lengths are 3.12 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Tb atoms.
DOI: 10.17188/1311899
title: Materials Data on LiY2Ir by Materials Project

description: LiY2Ir 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 Y atoms. All Li–Y bond lengths are 3.02 Å. Y is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ir atoms. All Y–Ir bond lengths are 3.02 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1311900
title: Materials Data on Tb2IrPd by Materials Project

description: Tb2IrPd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Tb is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Pd atoms. All Tb–Ir bond lengths are 3.01 Å. All Tb–Pd bond lengths are 3.01 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Tb atoms. Pd is bonded in a body-centered cubic geometry to eight equivalent Tb atoms.
DOI: 10.17188/1311901
title: Materials Data on KB6(HO)6 by Materials Project

description: KB6(H2O3)2H2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional and consists of four dihydrogen molecules and one KB6(H2O3)2 framework. In the KB6(H2O3)2 framework, K is bonded in a 6-coordinate geometry to six O atoms. There are a spread of K–O bond distances ranging from 2.72–2.99 Å. There are six inequivalent B sites. In the first B site, B is bonded in a single-bond geometry to one B and one O atom. The B–B bond length is 1.63 Å. The B–O bond length is 1.24 Å. In the second B site, B is bonded in a 5-coordinate geometry to five B atoms. There are a spread of B–B bond distances ranging from 1.69–1.86 Å. In the third B site, B is bonded in a distorted bent 120 degrees geometry to two O atoms. There is one shorter (1.29 Å) and one longer (1.41 Å) B–O bond length. In the fourth B site, B is bonded in a distorted single-bond geometry to two equivalent B and one H atom. The B–H bond length is 1.21 Å. In the fifth B site, B is bonded in a bent 120 degrees geometry to one B and two O atoms. There is one shorter (1.35 Å) and one longer (1.45 Å) B–O bond length. In the sixth B site, B is bonded in a bent 120 degrees geometry to two O atoms. There is one shorter (1.28 Å) and one longer (1.55 Å) B–O bond length. There are four inequivalent H sites. In the first H site, H is bonded in a linear geometry to two O atoms. There is one shorter (1.05 Å) and one longer (1.44 Å) H–O bond length. In the second H site, H is bonded in a single-bond geometry to one B atom. In the third H site, H is bonded in a single-bond geometry to one O atom. The H–O bond length is 0.99 Å. In the fourth H site, H is bonded in a single-bond geometry to one O atom. The H–O bond length is 0.98 Å. There are six inequivalent O sites. In the first O site, O is bonded in a water-like geometry to one B and one H atom. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one K, one B, and one H atom. In the third O site, O is bonded in a trigonal non-coplanar geometry to two B and one H atom. In the fourth O site, O is bonded in a distorted single-bond geometry to two equivalent K and one B atom. In the fifth O site, O is bonded in a distorted bent 150 degrees geometry to one K, one B, and one H atom. In the sixth O site, O is bonded in a distorted single-bond geometry to two equivalent K and one B atom.
DOI: 10.17188/1311902
title: Materials Data on SmPb3 by Materials Project

description: SmPb3 is Uranium Silicide structured and crystallizes in the monoclinic Pm space group. The structure is three-dimensional. Sm is bonded to twelve Pb atoms to form a mixture of face and corner-sharing SmPb12 cuboctahedra. There are a spread of Sm–Pb bond distances ranging from 3.52–3.54 Å. There are three inequivalent Pb sites. In the first Pb site, Pb is bonded in a distorted rectangular see-saw-like geometry to four equivalent Sm atoms. In the second Pb site, Pb is bonded in a distorted rectangular see-saw-like geometry to four equivalent Sm atoms. In the third Pb site, Pb is bonded in a distorted square co-planar geometry to four equivalent Sm atoms.
DOI: 10.17188/1311903
title: Materials Data on Ce2AgPb by Materials Project

description: Ce2AgPb 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 four equivalent Ag and four equivalent Pb atoms. All Ce–Ag bond lengths are 3.34 Å. All Ce–Pb bond lengths are 3.34 Å. Ag is bonded in a body-centered cubic geometry to eight equivalent Ce atoms. Pb is bonded in a body-centered cubic geometry to eight equivalent Ce atoms.
DOI: 10.17188/1311904
title: Materials Data on SmMgRh2 by Materials Project

description: MgSmRh2 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 Rh atoms. All Mg–Rh bond lengths are 2.89 Å. Sm is bonded in a body-centered cubic geometry to eight equivalent Rh atoms. All Sm–Rh bond lengths are 2.89 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Sm atoms.
DOI: 10.17188/1311905
title: Materials Data on Ac2GePd by Materials Project

description: Ac2PdGe 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 Pd and four equivalent Ge atoms. All Ac–Pd bond lengths are 3.35 Å. All Ac–Ge bond lengths are 3.35 Å. Pd 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.