cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1311906
title: Materials Data on Sc2ZnGa by Materials Project

description: Sc2ZnGa 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 Zn and four equivalent Ga atoms. All Sc–Zn bond lengths are 2.91 Å. All Sc–Ga bond lengths are 2.91 Å. Zn is bonded in a body-centered cubic geometry to eight equivalent Sc atoms. Ga is bonded in a body-centered cubic geometry to eight equivalent Sc atoms.
DOI: 10.17188/1311907
title: Materials Data on Sc2ZnOs by Materials Project

description: Sc2OsZn 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 Os and four equivalent Zn atoms. All Sc–Os bond lengths are 2.83 Å. All Sc–Zn bond lengths are 2.83 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Sc atoms. Zn is bonded in a distorted body-centered cubic geometry to eight equivalent Sc atoms.
DOI: 10.17188/1311908
title: Materials Data on LiGdAu2 by Materials Project

description: LiGdAu2 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 2.99 Å. Gd is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Gd–Au bond lengths are 2.99 Å. Au is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Gd atoms.
DOI: 10.17188/1311909
title: Materials Data on LaAgHg2 by Materials Project

description: LaAgHg2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. La is bonded in a distorted body-centered cubic geometry to six equivalent Ag and eight equivalent Hg atoms. All La–Ag bond lengths are 3.68 Å. All La–Hg bond lengths are 3.19 Å. Ag is bonded in a 8-coordinate geometry to six equivalent La and eight equivalent Hg atoms. All Ag–Hg bond lengths are 3.19 Å. Hg is bonded in a body-centered cubic geometry to four equivalent La and four equivalent Ag atoms.
DOI: 10.17188/1311910
title: Materials Data on TbGa3 by Materials Project

description: TbGa3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Tb is bonded to twelve equivalent Ga atoms to form a mixture of distorted corner and face-sharing TbGa12 cuboctahedra. There are six shorter (3.05 Å) and six longer (3.16 Å) Tb–Ga bond lengths. Ga is bonded in a 10-coordinate geometry to four equivalent Tb and six equivalent Ga atoms. All Ga–Ga bond lengths are 2.80 Å.
DOI: 10.17188/1311911
title: Materials Data on TbBr3 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: 10.17188/1311912
title: Materials Data on LaBi3 by Materials Project

description: LaBi3 is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. La is bonded to twelve equivalent Bi atoms to form a mixture of corner and face-sharing LaBi12 cuboctahedra. All La–Bi bond lengths are 3.55 Å. Bi is bonded in a distorted square co-planar geometry to four equivalent La atoms.
DOI: 10.17188/1311913
title: Materials Data on TaAlFe2 by Materials Project

description: Fe2Ta(Al) 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 Fe atoms. All Ta–Fe bond lengths are 2.56 Å. Fe is bonded in a body-centered cubic geometry to four equivalent Ta and four equivalent Al atoms. All Fe–Al bond lengths are 2.56 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Fe atoms.
DOI: 10.17188/1311918
title: Materials Data on LiZn2Pd by Materials Project

description: LiPdZn2 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 Pd and eight equivalent Zn atoms. All Li–Pd bond lengths are 3.06 Å. All Li–Zn bond lengths are 2.65 Å. Pd is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Zn atoms. All Pd–Zn bond lengths are 2.65 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Pd atoms.
DOI: 10.17188/1311919
title: Materials Data on LiZn2Pt by Materials Project

description: LiPtZn2 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 Pt and eight equivalent Zn atoms. All Li–Pt bond lengths are 3.06 Å. All Li–Zn bond lengths are 2.65 Å. Pt is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Zn atoms. All Pt–Zn bond lengths are 2.65 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Pt atoms.
DOI: 10.17188/1311920
title: Materials Data on LiZn2Ni by Materials Project

description: LiNiZn2 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 Zn atoms. All Li–Ni bond lengths are 2.94 Å. All Li–Zn bond lengths are 2.54 Å. Ni is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Zn atoms. All Ni–Zn bond lengths are 2.54 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ni atoms.
DOI: 10.17188/1311921
title: Materials Data on LiZn2Ir by Materials Project

description: LiIrZn2 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 Ir and eight equivalent Zn atoms. All Li–Ir bond lengths are 3.03 Å. All Li–Zn bond lengths are 2.62 Å. Ir is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Zn atoms. All Ir–Zn bond lengths are 2.62 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ir atoms.
DOI: 10.17188/1311922
title: Materials Data on SmAgAu2 by Materials Project

description: SmAu2Ag is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sm is bonded in a body-centered cubic geometry to eight equivalent Au atoms. All Sm–Au bond lengths are 3.04 Å. Au is bonded in a body-centered cubic geometry to four equivalent Sm and four equivalent Ag atoms. All Au–Ag bond lengths are 3.04 Å. Ag is bonded in a distorted body-centered cubic geometry to eight equivalent Au atoms.
DOI: 10.17188/1311923
title: Materials Data on LiZn2Au by Materials Project

description: LiAuZn2 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 Au and eight equivalent Zn atoms. All Li–Au bond lengths are 3.13 Å. All Li–Zn bond lengths are 2.71 Å. Au is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Zn atoms. All Au–Zn bond lengths are 2.71 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Au atoms.
DOI: 10.17188/1311924
title: Materials Data on DyCdAg2 by Materials Project

description: DyAg2Cd 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 Ag atoms. All Dy–Ag bond lengths are 3.03 Å. Ag is bonded in a body-centered cubic geometry to four equivalent Dy and four equivalent Cd atoms. All Ag–Cd bond lengths are 3.03 Å. Cd is bonded in a distorted body-centered cubic geometry to eight equivalent Ag atoms.
DOI: 10.17188/1311925
title: Materials Data on CaPrCd2 by Materials Project

description: CaPrCd2 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 3.35 Å. Pr is bonded in a body-centered cubic geometry to eight equivalent Cd atoms. All Pr–Cd bond lengths are 3.35 Å. Cd is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent Pr atoms.
DOI: 10.17188/1311926
title: Materials Data on LiZnPd2 by Materials Project

description: LiPd2Zn 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 atoms. All Li–Pd bond lengths are 2.63 Å. Pd is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Zn atoms. All Pd–Zn bond lengths are 2.63 Å. Zn is bonded in a distorted body-centered cubic geometry to eight equivalent Pd atoms.
DOI: 10.17188/1311927
title: Materials Data on RhCl2 by Materials Project

description: RhCl2 is Rutile structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Rh is bonded to six equivalent Cl atoms to form a mixture of edge and corner-sharing RhCl6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are two shorter (2.44 Å) and four longer (2.45 Å) Rh–Cl bond lengths. Cl is bonded in a distorted trigonal planar geometry to three equivalent Rh atoms.
DOI: 10.17188/1311928
title: Materials Data on CdAgPd2 by Materials Project

description: Pd2AgCd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pd is bonded in a body-centered cubic geometry to four equivalent Ag and four equivalent Cd atoms. All Pd–Ag bond lengths are 2.81 Å. All Pd–Cd bond lengths are 2.81 Å. Ag is bonded in a distorted body-centered cubic geometry to eight equivalent Pd atoms. Cd is bonded in a body-centered cubic geometry to eight equivalent Pd atoms.
DOI: 10.17188/1311929
title: Materials Data on RbSrCO3F (SG:187) 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: 10.17188/1311930
title: Materials Data on ScTc3 by Materials Project

description: ScTc3 is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sc3+ is bonded in a distorted body-centered cubic geometry to fourteen Tc1- atoms. There are eight shorter (2.72 Å) and six longer (3.14 Å) Sc–Tc bond lengths. There are two inequivalent Tc1- sites. In the first Tc1- site, Tc1- is bonded to four equivalent Sc3+ and four equivalent Tc1- atoms to form a mixture of distorted corner, edge, and face-sharing TcSc4Tc4 tetrahedra. All Tc–Tc bond lengths are 2.72 Å. In the second Tc1- site, Tc1- is bonded in a 8-coordinate geometry to six equivalent Sc3+ and eight equivalent Tc1- atoms.
DOI: 10.17188/1311931
title: Materials Data on ScCdHg2 by Materials Project

description: ScHg2Cd 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 eight equivalent Hg atoms. All Sc–Hg bond lengths are 3.05 Å. Hg is bonded in a body-centered cubic geometry to four equivalent Sc and four equivalent Cd atoms. All Hg–Cd bond lengths are 3.05 Å. Cd is bonded in a distorted body-centered cubic geometry to eight equivalent Hg atoms.
DOI: 10.17188/1311932
title: Materials Data on Re3Os by Materials Project

description: Re3Os is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Re sites. In the first Re site, Re is bonded to eight Re and four equivalent Os atoms to form distorted ReRe8Os4 cuboctahedra that share corners with four equivalent OsRe12 cuboctahedra, corners with fourteen equivalent ReRe8Os4 cuboctahedra, edges with six equivalent OsRe12 cuboctahedra, edges with twelve ReRe8Os4 cuboctahedra, faces with four equivalent OsRe12 cuboctahedra, and faces with sixteen ReRe8Os4 cuboctahedra. There are a spread of Re–Re bond distances ranging from 2.73–2.80 Å. There are two shorter (2.75 Å) and two longer (2.78 Å) Re–Os bond lengths. In the second Re site, Re is bonded to eight equivalent Re and four equivalent Os atoms to form distorted ReRe8Os4 cuboctahedra that share corners with four equivalent OsRe12 cuboctahedra, corners with fourteen ReRe8Os4 cuboctahedra, edges with six equivalent OsRe12 cuboctahedra, edges with twelve equivalent ReRe8Os4 cuboctahedra, faces with four equivalent OsRe12 cuboctahedra, and faces with sixteen ReRe8Os4 cuboctahedra. There are two shorter (2.75 Å) and two longer (2.78 Å) Re–Os bond lengths. Os is bonded to twelve Re atoms to form OsRe12 cuboctahedra that share corners with six equivalent OsRe12 cuboctahedra, corners with twelve ReRe8Os4 cuboctahedra, edges with eighteen ReRe8Os4 cuboctahedra, faces with eight equivalent OsRe12 cuboctahedra, and faces with twelve ReRe8Os4 cuboctahedra.
DOI: 10.17188/1311933
title: Materials Data on LiTm2Os by Materials Project

description: LiTm2Os 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 Tm atoms. All Li–Tm bond lengths are 2.96 Å. Tm is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Os atoms. All Tm–Os bond lengths are 2.96 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Tm atoms.
DOI: 10.17188/1311934
title: Materials Data on CaMgTl2 by Materials Project

description: CaMgTl2 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 Tl atoms. All Ca–Tl bond lengths are 3.27 Å. Mg is bonded in a body-centered cubic geometry to eight equivalent Tl atoms. All Mg–Tl bond lengths are 3.27 Å. Tl is bonded in a body-centered cubic geometry to four equivalent Ca and four equivalent Mg atoms.
DOI: 10.17188/1311935
title: Materials Data on LiHo2Pt by Materials Project

description: LiHo2Pt is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Ho atoms. All Li–Ho bond lengths are 3.03 Å. Ho is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Pt atoms. All Ho–Pt bond lengths are 3.03 Å. Pt is bonded in a body-centered cubic geometry to eight equivalent Ho atoms.
DOI: 10.17188/1311936
title: Materials Data on K4P2PdS8 (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: 10.17188/1311937
title: Materials Data on LiHo2Os by Materials Project

description: LiHo2Os is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Ho atoms. All Li–Ho bond lengths are 2.99 Å. Ho is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Os atoms. All Ho–Os bond lengths are 2.99 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Ho atoms.
DOI: 10.17188/1311938
title: Materials Data on Be2CoPt by Materials Project

description: Be2CoPt is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a body-centered cubic geometry to four equivalent Co and four equivalent Pt atoms. All Be–Co bond lengths are 2.36 Å. All Be–Pt bond lengths are 2.36 Å. Co is bonded in a distorted body-centered cubic geometry to eight equivalent Be atoms. Pt is bonded in a body-centered cubic geometry to eight equivalent Be atoms.
DOI: 10.17188/1311939
title: Materials Data on Be2CoNi by Materials Project

description: Be2CoNi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a body-centered cubic geometry to four equivalent Co and four equivalent Ni atoms. All Be–Co bond lengths are 2.25 Å. All Be–Ni bond lengths are 2.25 Å. Co is bonded in a body-centered cubic geometry to eight equivalent Be atoms. Ni is bonded in a body-centered cubic geometry to eight equivalent Be atoms.
DOI: 10.17188/1311940
title: Materials Data on LiAlCu2 by Materials Project

description: LiCu2Al 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 Cu and six equivalent Al atoms. All Li–Cu bond lengths are 2.55 Å. All Li–Al bond lengths are 2.94 Å. Cu is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Al atoms. All Cu–Al bond lengths are 2.55 Å. Al is bonded in a distorted body-centered cubic geometry to six equivalent Li and eight equivalent Cu atoms.
DOI: 10.17188/1311941
title: Materials Data on Be2CuIr by Materials Project

description: Be2IrCu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Cu atoms. All Be–Ir bond lengths are 2.38 Å. All Be–Cu bond lengths are 2.38 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Be atoms. Cu is bonded in a distorted body-centered cubic geometry to eight equivalent Be atoms.
DOI: 10.17188/1311942
title: Materials Data on Be2CoIr by Materials Project

description: Be2IrCo is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Co atoms. All Be–Ir bond lengths are 2.35 Å. All Be–Co bond lengths are 2.35 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Be atoms. Co is bonded in a distorted body-centered cubic geometry to eight equivalent Be atoms.
DOI: 10.17188/1311943
title: Materials Data on BeVOs2 by Materials Project

description: BeVOs2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be2+ is bonded in a body-centered cubic geometry to eight equivalent Os2- atoms. All Be–Os bond lengths are 2.54 Å. V2+ is bonded in a body-centered cubic geometry to eight equivalent Os2- atoms. All V–Os bond lengths are 2.54 Å. Os2- is bonded in a body-centered cubic geometry to four equivalent Be2+ and four equivalent V2+ atoms.
DOI: 10.17188/1311944
title: Materials Data on DyCdPd2 by Materials Project

description: DyPd2Cd 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 Pd atoms. All Dy–Pd bond lengths are 2.94 Å. Pd is bonded in a body-centered cubic geometry to four equivalent Dy and four equivalent Cd atoms. All Pd–Cd bond lengths are 2.94 Å. Cd is bonded in a distorted body-centered cubic geometry to eight equivalent Pd atoms.
DOI: 10.17188/1311945
title: Materials Data on Ho2MgAl by Materials Project

description: MgHo2Al 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 Ho atoms. All Mg–Ho bond lengths are 3.17 Å. Ho is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Al atoms. All Ho–Al bond lengths are 3.17 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Ho atoms.
DOI: 10.17188/1311946
title: Materials Data on DyPaTc2 by Materials Project

description: PaDyTc2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa3+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Pa–Tc bond lengths are 2.96 Å. Dy3+ is bonded in a body-centered cubic geometry to eight equivalent Tc3- atoms. All Dy–Tc bond lengths are 2.96 Å. Tc3- is bonded in a body-centered cubic geometry to four equivalent Pa3+ and four equivalent Dy3+ atoms.
DOI: 10.17188/1311947
title: Materials Data on DyPaRu2 by Materials Project

description: PaDyRu2 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 2.96 Å. Dy is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Dy–Ru bond lengths are 2.96 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Dy atoms.
DOI: 10.17188/1311948
title: Materials Data on Be2IrPt by Materials Project

description: Be2IrPt is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Pt atoms. All Be–Ir bond lengths are 2.44 Å. All Be–Pt bond lengths are 2.44 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent Be atoms. Pt is bonded in a body-centered cubic geometry to eight equivalent Be atoms.
DOI: 10.17188/1311949
title: Materials Data on Tc3Pt by Materials Project

description: Tc3Pt is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Tc+1.67- sites. In the first Tc+1.67- site, Tc+1.67- is bonded to eight Tc+1.67- and four equivalent Pt5+ atoms to form distorted TcTc8Pt4 cuboctahedra that share corners with four equivalent PtTc12 cuboctahedra, corners with fourteen TcTc8Pt4 cuboctahedra, edges with six equivalent PtTc12 cuboctahedra, edges with twelve TcTc8Pt4 cuboctahedra, faces with four equivalent PtTc12 cuboctahedra, and faces with sixteen TcTc8Pt4 cuboctahedra. There are a spread of Tc–Tc bond distances ranging from 2.65–2.91 Å. There are two shorter (2.77 Å) and two longer (2.78 Å) Tc–Pt bond lengths. In the second Tc+1.67- site, Tc+1.67- is bonded to eight Tc+1.67- and four equivalent Pt5+ atoms to form distorted TcTc8Pt4 cuboctahedra that share corners with four equivalent PtTc12 cuboctahedra, corners with fourteen TcTc8Pt4 cuboctahedra, edges with six equivalent PtTc12 cuboctahedra, edges with twelve TcTc8Pt4 cuboctahedra, faces with four equivalent PtTc12 cuboctahedra, and faces with sixteen TcTc8Pt4 cuboctahedra. Both Tc–Tc bond lengths are 2.68 Å. There are two shorter (2.77 Å) and two longer (2.78 Å) Tc–Pt bond lengths. Pt5+ is bonded to twelve Tc+1.67- atoms to form PtTc12 cuboctahedra that share corners with six equivalent PtTc12 cuboctahedra, corners with twelve TcTc8Pt4 cuboctahedra, edges with eighteen TcTc8Pt4 cuboctahedra, faces with eight equivalent PtTc12 cuboctahedra, and faces with twelve TcTc8Pt4 cuboctahedra.
DOI: 10.17632/wyx92rzw6k.1
title: Data for: Safety of thyroid surgery in the elderly: a propensity-score matched cohort study.

description: raw data with patient demographics and complications
DOI: 10.17632/634zdghj48.2
title: Data for: Increasing reoperation rates and inferior outcome with prolonged symptom duration in lumbar disc herniation surgery - A prospective cohort study

description: Patients with lumbar disc herniation who underwent surgery with discectomy.
DOI: 10.17632/krkvbm28wx.1
title: Data for: Coaxiality evaluation based on double material condition

description: Measurements of considered shaft and its datum shaft of a stepped shaft.