cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1310822
title: Materials Data on CeCdAg2 by Materials Project

description: CeAg2Cd 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 and six equivalent Cd atoms. All Ce–Ag bond lengths are 3.09 Å. All Ce–Cd bond lengths are 3.57 Å. Ag is bonded in a body-centered cubic geometry to four equivalent Ce and four equivalent Cd atoms. All Ag–Cd bond lengths are 3.09 Å. Cd is bonded in a distorted body-centered cubic geometry to six equivalent Ce and eight equivalent Ag atoms.
DOI: 10.17188/1310823
title: Materials Data on CaEuIn2 by Materials Project

description: CaEuIn2 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 In atoms. All Ca–In bond lengths are 3.44 Å. Eu is bonded in a body-centered cubic geometry to eight equivalent In atoms. All Eu–In bond lengths are 3.44 Å. In is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent Eu atoms.
DOI: 10.17188/1310824
title: Materials Data on Mn2VGe by Materials Project

description: VMn2Ge is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. V is bonded in a distorted body-centered cubic geometry to eight equivalent Mn and six equivalent Ge atoms. All V–Mn bond lengths are 2.50 Å. All V–Ge bond lengths are 2.88 Å. Mn is bonded in a body-centered cubic geometry to four equivalent V and four equivalent Ge atoms. All Mn–Ge bond lengths are 2.50 Å. Ge is bonded in a distorted body-centered cubic geometry to six equivalent V and eight equivalent Mn atoms.
DOI: 10.17188/1310825
title: Materials Data on AcTe3 by Materials Project

description: AcTe3 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ac3+ is bonded to twelve Te1- atoms to form AcTe12 cuboctahedra that share corners with four equivalent AcTe12 cuboctahedra, edges with eight equivalent AcTe12 cuboctahedra, edges with sixteen equivalent TeAc4Te8 cuboctahedra, faces with four equivalent AcTe12 cuboctahedra, and faces with eight equivalent TeAc4Te8 cuboctahedra. There are four shorter (3.32 Å) and eight longer (3.74 Å) Ac–Te bond lengths. There are two inequivalent Te1- sites. In the first Te1- site, Te1- is bonded to four equivalent Ac3+ and eight Te1- atoms to form distorted TeAc4Te8 cuboctahedra that share corners with twelve equivalent TeAc4Te8 cuboctahedra, edges with eight equivalent AcTe12 cuboctahedra, edges with eight equivalent TeAc4Te8 cuboctahedra, faces with four equivalent AcTe12 cuboctahedra, and faces with ten equivalent TeAc4Te8 cuboctahedra. There are four shorter (3.32 Å) and four longer (3.74 Å) Te–Te bond lengths. In the second Te1- site, Te1- is bonded in a square co-planar geometry to four equivalent Ac3+ and eight equivalent Te1- atoms.
DOI: 10.17188/1310826
title: Materials Data on Y2AlZn by Materials Project

description: Y2ZnAl 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 Al atoms. All Y–Zn bond lengths are 3.12 Å. All Y–Al bond lengths are 3.12 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Al is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310846
title: Materials Data on Y2AgRu by Materials Project

description: Y2RuAg 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 Ag atoms. All Y–Ru bond lengths are 3.05 Å. All Y–Ag bond lengths are 3.05 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Ag is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310847
title: Materials Data on Be3Ru by Materials Project

description: Be3Ru is Uranium Silicide-like structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are two inequivalent Be sites. In the first Be site, Be is bonded to eight Be and four equivalent Ru atoms to form distorted BeBe8Ru4 cuboctahedra that share corners with twelve equivalent BeBe8Ru4 cuboctahedra, edges with eight equivalent BeBe8Ru4 cuboctahedra, edges with eight equivalent RuBe12 cuboctahedra, faces with four equivalent RuBe12 cuboctahedra, and faces with ten equivalent BeBe8Ru4 cuboctahedra. There are four shorter (2.25 Å) and four longer (2.46 Å) Be–Be bond lengths. All Be–Ru bond lengths are 2.46 Å. In the second Be site, Be is bonded in a square co-planar geometry to eight equivalent Be and four equivalent Ru atoms. All Be–Ru bond lengths are 2.25 Å. Ru is bonded to twelve Be atoms to form RuBe12 cuboctahedra that share corners with four equivalent RuBe12 cuboctahedra, edges with eight equivalent RuBe12 cuboctahedra, edges with sixteen equivalent BeBe8Ru4 cuboctahedra, faces with four equivalent RuBe12 cuboctahedra, and faces with eight equivalent BeBe8Ru4 cuboctahedra.
DOI: 10.17188/1310848
title: Materials Data on LuZnPd2 by Materials Project

description: LuPd2Zn 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 Zn atoms. All Pd–Zn bond lengths are 2.83 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Pd atoms.
DOI: 10.17188/1310849
title: Materials Data on Tl2CoP4(HO2)8 (SG:2) 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: 10.17188/1310850
title: Materials Data on CsSn3 by Materials Project

description: CsSn3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Cs is bonded in a 12-coordinate geometry to twelve equivalent Sn atoms. There are six shorter (4.03 Å) and six longer (4.13 Å) Cs–Sn bond lengths. Sn is bonded in a 10-coordinate geometry to four equivalent Cs and six equivalent Sn atoms. There are two shorter (3.07 Å) and four longer (3.27 Å) Sn–Sn bond lengths.
DOI: 10.17188/1310851
title: Materials Data on LuZnRh2 by Materials Project

description: LuRh2Zn 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 2.77 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Lu and four equivalent Zn atoms. All Rh–Zn bond lengths are 2.77 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Rh atoms.
DOI: 10.17188/1310852
title: Materials Data on ThScTc2 by Materials Project

description: ThScTc2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Th4+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Th–Tc bond lengths are 2.93 Å. Sc2+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Sc–Tc bond lengths are 2.93 Å. Tc3- is bonded in a body-centered cubic geometry to four equivalent Th4+ and four equivalent Sc2+ atoms.
DOI: 10.17188/1310853
title: Materials Data on Ti2MnIr by Materials Project

description: Ti2MnIr 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 four equivalent Mn and four equivalent Ir atoms. All Ti–Mn bond lengths are 2.64 Å. All Ti–Ir bond lengths are 2.64 Å. Mn is bonded in a 8-coordinate geometry to eight equivalent Ti and six equivalent Ir atoms. All Mn–Ir bond lengths are 3.05 Å. Ir is bonded in a distorted body-centered cubic geometry to eight equivalent Ti and six equivalent Mn atoms.
DOI: 10.17188/1310854
title: Materials Data on CeAu3 by Materials Project

description: CeAu3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ce3+ is bonded to twelve equivalent Au1- atoms to form a mixture of corner and face-sharing CeAu12 cuboctahedra. There are six shorter (3.11 Å) and six longer (3.24 Å) Ce–Au bond lengths. Au1- is bonded in a 4-coordinate geometry to four equivalent Ce3+ atoms.
DOI: 10.17188/1310855
title: Materials Data on Li2ErTl by Materials Project

description: Li2ErTl 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 Er and four equivalent Tl atoms. All Li–Er bond lengths are 2.96 Å. All Li–Tl bond lengths are 2.96 Å. Er 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: 10.17188/1310856
title: Materials Data on Li2CdAu by Materials Project

description: Li2AuCd 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 Au and four equivalent Cd atoms. All Li–Au bond lengths are 2.78 Å. All Li–Cd bond lengths are 2.78 Å. Au is bonded in a body-centered cubic geometry to eight equivalent Li atoms. Cd is bonded in a distorted body-centered cubic geometry to eight equivalent Li atoms.
DOI: 10.17188/1310857
title: Materials Data on LiNd2Ga by Materials Project

description: LiNd2Ga 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 Nd atoms. All Li–Nd bond lengths are 3.22 Å. Nd is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ga atoms. All Nd–Ga bond lengths are 3.22 Å. Ga is bonded in a body-centered cubic geometry to eight equivalent Nd atoms.
DOI: 10.17188/1310858
title: Materials Data on Li2ErIn by Materials Project

description: Li2ErIn 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 Er and four equivalent In atoms. All Li–Er bond lengths are 2.96 Å. All Li–In bond lengths are 2.96 Å. Er is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent In atoms. All Er–In bond lengths are 3.42 Å. In is bonded in a body-centered cubic geometry to eight equivalent Li and six equivalent Er atoms.
DOI: 10.17188/1310859
title: Materials Data on Li2DyIn by Materials Project

description: Li2DyIn 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 Dy and four equivalent In atoms. All Li–Dy bond lengths are 2.97 Å. All Li–In bond lengths are 2.97 Å. Dy is bonded in a distorted body-centered cubic geometry to eight equivalent Li and six equivalent In atoms. All Dy–In bond lengths are 3.43 Å. In is bonded in a body-centered cubic geometry to eight equivalent Li and six equivalent Dy atoms.
DOI: 10.17188/1310860
title: Materials Data on Li2DyTl by Materials Project

description: Li2DyTl 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 Dy and four equivalent Tl atoms. All Li–Dy bond lengths are 2.97 Å. All Li–Tl bond lengths are 2.97 Å. Dy 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: 10.17188/1310861
title: Materials Data on Li2CdPd by Materials Project

description: Li2PdCd 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 Pd and four equivalent Cd atoms. All Li–Pd bond lengths are 2.73 Å. All Li–Cd bond lengths are 2.73 Å. Pd is bonded in a body-centered cubic geometry to eight equivalent Li atoms. Cd is bonded in a body-centered cubic geometry to eight equivalent Li atoms.
DOI: 10.17188/1310862
title: Materials Data on Y2Mg by Materials Project

description: MgY2 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight Y atoms. There are a spread of Mg–Y bond distances ranging from 3.29–3.34 Å. There are two inequivalent Y sites. In the first Y site, Y is bonded in a 12-coordinate geometry to six equivalent Mg and four equivalent Y atoms. There are two shorter (3.60 Å) and two longer (3.65 Å) Y–Y bond lengths. In the second Y site, Y is bonded to two equivalent Mg and ten Y atoms to form a mixture of distorted corner, edge, and face-sharing YY10Mg2 cuboctahedra. There are four shorter (3.41 Å) and two longer (3.70 Å) Y–Y bond lengths.
DOI: 10.17188/1310863
title: Materials Data on VGeRu2 by Materials Project

description: Ru2VGe is Heusler structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. V is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. There are six shorter (2.62 Å) and two longer (2.63 Å) V–Ru bond lengths. Ru is bonded in a body-centered cubic geometry to four equivalent V and four equivalent Ge atoms. There are three shorter (2.62 Å) and one longer (2.63 Å) Ru–Ge bond lengths. Ge is bonded in a distorted body-centered cubic geometry to eight equivalent Ru atoms.
DOI: 10.17188/1310864
title: Materials Data on VGaRu2 by Materials Project

description: Ru2VGa is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. V is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All V–Ru bond lengths are 2.61 Å. Ru is bonded in a body-centered cubic geometry to four equivalent V and four equivalent Ga atoms. All Ru–Ga bond lengths are 2.61 Å. Ga is bonded in a body-centered cubic geometry to eight equivalent Ru atoms.
DOI: 10.17188/1310865
title: Materials Data on Y2CuRh by Materials Project

description: Y2RhCu 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 Rh and four equivalent Cu atoms. All Y–Rh bond lengths are 3.00 Å. All Y–Cu bond lengths are 3.00 Å. Rh is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310866
title: Materials Data on Y2CuRu by Materials Project

description: Y2RuCu 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 Cu atoms. All Y–Ru bond lengths are 2.98 Å. All Y–Cu bond lengths are 2.98 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310867
title: Materials Data on Lu2IrPd by Materials Project

description: Lu2IrPd 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 Pd atoms. All Lu–Ir bond lengths are 2.94 Å. All Lu–Pd bond lengths are 2.94 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Lu atoms. Pd is bonded in a body-centered cubic geometry to eight equivalent Lu atoms.
DOI: 10.17188/1310868
title: Materials Data on GdMgCd2 by Materials Project

description: MgGdCd2 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 Cd atoms. All Mg–Cd bond lengths are 3.14 Å. Gd is bonded in a body-centered cubic geometry to eight equivalent Cd atoms. All Gd–Cd bond lengths are 3.14 Å. Cd is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Gd atoms.
DOI: 10.17188/1310869
title: Materials Data on Ti2NiMo by Materials Project

description: Ti2MoNi 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 Mo and four equivalent Ni atoms. All Ti–Mo bond lengths are 2.67 Å. All Ti–Ni bond lengths are 2.67 Å. Mo is bonded in a body-centered cubic geometry to eight equivalent Ti atoms. Ni is bonded in a body-centered cubic geometry to eight equivalent Ti atoms.
DOI: 10.17188/1310870
title: Materials Data on Y2ZnRu by Materials Project

description: Y2RuZn 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 Zn atoms. All Y–Ru bond lengths are 3.02 Å. All Y–Zn bond lengths are 3.02 Å. Ru 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: 10.17188/1310871
title: Materials Data on Lu2GaTc by Materials Project

description: Lu2TcGa 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 Tc and four equivalent Ga atoms. All Lu–Tc bond lengths are 2.97 Å. All Lu–Ga bond lengths are 2.97 Å. Tc is bonded in a body-centered cubic geometry to eight equivalent Lu atoms. Ga is bonded in a body-centered cubic geometry to eight equivalent Lu atoms.
DOI: 10.17188/1310872
title: Materials Data on Y2CuIr by Materials Project

description: Y2IrCu 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 Cu atoms. All Y–Ir bond lengths are 3.00 Å. All Y–Cu bond lengths are 3.00 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310873
title: Materials Data on Lu2CuRu by Materials Project

description: Lu2RuCu 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 Ru and four equivalent Cu atoms. All Lu–Ru bond lengths are 2.90 Å. All Lu–Cu bond lengths are 2.90 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Lu atoms. Cu is bonded in a body-centered cubic geometry to eight equivalent Lu atoms.
DOI: 10.17188/1310874
title: Materials Data on YLu3 by Materials Project

description: Lu3Y is Magnesium-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are three inequivalent Lu sites. In the first Lu site, Lu is bonded to eight Lu and four equivalent Y atoms to form LuY4Lu8 cuboctahedra that share corners with four equivalent YLu12 cuboctahedra, corners with fourteen equivalent LuY4Lu8 cuboctahedra, edges with six equivalent YLu12 cuboctahedra, edges with twelve LuY4Lu8 cuboctahedra, faces with four equivalent YLu12 cuboctahedra, and faces with sixteen LuY4Lu8 cuboctahedra. There are a spread of Lu–Lu bond distances ranging from 3.45–3.59 Å. There are two shorter (3.47 Å) and two longer (3.56 Å) Lu–Y bond lengths. In the second Lu site, Lu is bonded to eight Lu and four equivalent Y atoms to form LuY4Lu8 cuboctahedra that share corners with four equivalent YLu12 cuboctahedra, corners with fourteen LuY4Lu8 cuboctahedra, edges with six equivalent YLu12 cuboctahedra, edges with twelve LuY4Lu8 cuboctahedra, faces with four equivalent YLu12 cuboctahedra, and faces with sixteen LuY4Lu8 cuboctahedra. There are a spread of Lu–Lu bond distances ranging from 3.45–3.59 Å. There are two shorter (3.47 Å) and two longer (3.56 Å) Lu–Y bond lengths. In the third Lu site, Lu is bonded to eight Lu and four equivalent Y atoms to form LuY4Lu8 cuboctahedra that share corners with four equivalent YLu12 cuboctahedra, corners with fourteen LuY4Lu8 cuboctahedra, edges with six equivalent YLu12 cuboctahedra, edges with twelve LuY4Lu8 cuboctahedra, faces with four equivalent YLu12 cuboctahedra, and faces with sixteen LuY4Lu8 cuboctahedra. There are two shorter (3.47 Å) and two longer (3.56 Å) Lu–Y bond lengths. Y is bonded to twelve Lu atoms to form YLu12 cuboctahedra that share corners with six equivalent YLu12 cuboctahedra, corners with twelve LuY4Lu8 cuboctahedra, edges with eighteen LuY4Lu8 cuboctahedra, faces with eight equivalent YLu12 cuboctahedra, and faces with twelve LuY4Lu8 cuboctahedra.
DOI: 10.17188/1310875
title: Materials Data on NdPbAu2 by Materials Project

description: NdAu2Pb is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Nd is bonded in a distorted body-centered cubic geometry to eight equivalent Au and six equivalent Pb atoms. All Nd–Au bond lengths are 3.16 Å. All Nd–Pb bond lengths are 3.65 Å. Au is bonded in a body-centered cubic geometry to four equivalent Nd and four equivalent Pb atoms. All Au–Pb bond lengths are 3.16 Å. Pb is bonded in a 8-coordinate geometry to six equivalent Nd and eight equivalent Au atoms.
DOI: 10.17188/1310876
title: Materials Data on YGa3 by Materials Project

description: YGa3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Y is bonded to twelve equivalent Ga atoms to form a mixture of distorted face and corner-sharing YGa12 cuboctahedra. There are six shorter (3.06 Å) and six longer (3.16 Å) Y–Ga bond lengths. Ga is bonded in a 10-coordinate geometry to four equivalent Y and six equivalent Ga atoms. There are two shorter (2.79 Å) and four longer (2.80 Å) Ga–Ga bond lengths.
DOI: 10.17188/1310877
title: Materials Data on Lu2RuPt by Materials Project

description: Lu2RuPt 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 Ru and four equivalent Pt atoms. All Lu–Ru bond lengths are 2.92 Å. All Lu–Pt bond lengths are 2.92 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Lu atoms. Pt is bonded in a body-centered cubic geometry to eight equivalent Lu atoms.
DOI: 10.17188/1310878
title: Materials Data on Y2IrPd by Materials Project

description: Y2IrPd 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 Pd atoms. All Y–Ir bond lengths are 3.01 Å. All Y–Pd bond lengths are 3.01 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Y atoms. Pd is bonded in a body-centered cubic geometry to eight equivalent Y atoms.
DOI: 10.17188/1310879
title: Materials Data on Lu2RuRh by Materials Project

description: Lu2RuRh 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 Ru and four equivalent Rh atoms. All Lu–Ru bond lengths are 2.89 Å. All Lu–Rh bond lengths are 2.89 Å. Ru 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.