cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1738117
title: Materials Data on CaSeO4 by Materials Project

description: CaSeO4 crystallizes in the monoclinic P2_1/c space group. The structure is two-dimensional and consists of one CaSeO4 sheet oriented in the (0, 0, 1) direction. Ca2+ is bonded to seven O2- atoms to form a mixture of distorted edge and corner-sharing CaO7 pentagonal bipyramids. There are a spread of Ca–O bond distances ranging from 2.30–2.55 Å. Se6+ is bonded in a trigonal non-coplanar geometry to three O2- atoms. There are a spread of Se–O bond distances ranging from 1.69–1.76 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Ca2+ and one Se6+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Ca2+ and one Se6+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to three equivalent Ca2+ and one Se6+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to one Ca2+ atom.
DOI: 10.17188/1738118
title: Materials Data on RbTaTiO5 by Materials Project

description: RbTiTaO5 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Rb1+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Rb–O bond distances ranging from 2.95–3.20 Å. Ti4+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ti–O bond distances ranging from 1.80–2.35 Å. Ta5+ is bonded to six O2- atoms to form distorted corner-sharing TaO6 octahedra. The corner-sharing octahedral tilt angles are 31°. There are a spread of Ta–O bond distances ranging from 1.81–2.33 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to two equivalent Rb1+, one Ti4+, and one Ta5+ atom. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Rb1+, one Ti4+, and one Ta5+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Ti4+ and two equivalent Ta5+ atoms. In the fourth O2- site, O2- is bonded to three equivalent Ti4+ and one Ta5+ atom to form a mixture of distorted edge and corner-sharing OTaTi3 trigonal pyramids. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to four equivalent Rb1+ and one Ta5+ atom.
DOI: 10.17188/1738119
title: Materials Data on Li2Mn2(SiO3)3 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: 10.17188/1738120
title: Materials Data on TlBi(WO4)2 by Materials Project

description: TlBi(WO4)2 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing WO6 octahedra. The corner-sharing octahedral tilt angles are 41°. There are a spread of W–O bond distances ranging from 1.84–2.16 Å. Tl1+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Tl–O bond distances ranging from 2.94–3.16 Å. Bi3+ is bonded in a 6-coordinate geometry to eight O2- atoms. There are a spread of Bi–O bond distances ranging from 2.33–2.91 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent W6+ and two equivalent Tl1+ atoms. In the second O2- site, O2- is bonded in a 1-coordinate geometry to one W6+, one Tl1+, and two equivalent Bi3+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent W6+, one Tl1+, and one Bi3+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to one W6+, one Tl1+, and one Bi3+ atom.
DOI: 10.17188/1738121
title: Materials Data on Mn7SnN6 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: 10.17188/1738122
title: Materials Data on SrO10 by Materials Project

description: SrO10 crystallizes in the tetragonal P4/mcc space group. The structure is two-dimensional and consists of two hydrogen peroxide molecules and two SrO8 sheets oriented in the (0, 0, 1) direction. In each SrO8 sheet, Sr is bonded in a distorted body-centered cubic geometry to eight equivalent O atoms. All Sr–O bond lengths are 2.64 Å. O is bonded in a distorted bent 120 degrees geometry to one Sr and one O atom. The O–O bond length is 1.28 Å.
DOI: 10.17188/1738124
title: Materials Data on Co(PdN)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: 10.17188/1738125
title: Materials Data on TlCSN by Materials Project

description: TlCNS is Potassium thiocyanate structured and crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. Tl1+ is bonded in a 8-coordinate geometry to four equivalent N3- and four equivalent S2- atoms. There are two shorter (3.08 Å) and two longer (3.18 Å) Tl–N bond lengths. There are two shorter (3.39 Å) and two longer (3.49 Å) Tl–S bond lengths. C4+ is bonded in a distorted linear geometry to one N3- and one S2- atom. The C–N bond length is 1.19 Å. The C–S bond length is 1.63 Å. N3- is bonded in a distorted single-bond geometry to four equivalent Tl1+ and one C4+ atom. S2- is bonded in a 1-coordinate geometry to four equivalent Tl1+ and one C4+ atom.
DOI: 10.17188/1738127
title: Materials Data on Nb6AlSb by Materials Project

description: Nb6AlSb crystallizes in the cubic Pm-3 space group. The structure is three-dimensional. there are three inequivalent Nb sites. In the first Nb site, Nb is bonded in a 6-coordinate geometry to ten Nb, two equivalent Al, and two equivalent Sb atoms. There are a spread of Nb–Nb bond distances ranging from 2.63–3.22 Å. Both Nb–Al bond lengths are 2.94 Å. Both Nb–Sb bond lengths are 2.94 Å. In the second Nb site, Nb is bonded in a 6-coordinate geometry to ten Nb, two equivalent Al, and two equivalent Sb atoms. Both Nb–Nb bond lengths are 3.22 Å. Both Nb–Al bond lengths are 2.94 Å. Both Nb–Sb bond lengths are 2.94 Å. In the third Nb site, Nb is bonded in a 6-coordinate geometry to ten Nb, two equivalent Al, and two equivalent Sb atoms. Both Nb–Al bond lengths are 2.94 Å. Both Nb–Sb bond lengths are 2.94 Å. Al is bonded to twelve Nb atoms to form AlNb12 cuboctahedra that share edges with six equivalent AlNb12 cuboctahedra and faces with eight equivalent SbNb12 cuboctahedra. Sb is bonded to twelve Nb atoms to form SbNb12 cuboctahedra that share edges with six equivalent SbNb12 cuboctahedra and faces with eight equivalent AlNb12 cuboctahedra.
DOI: 10.5517/ccdc.csd.cc1mv6ym
title: CCDC 1514751: Experimental Crystal Structure Determination

description: Related Article: hui zhou|2020|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc1nhqlg
title: CCDC 1534456: Experimental Crystal Structure Determination

description: Related Article: Hui Zhou|2020|CSD Communication|||
DOI: 10.17188/1738128
title: Materials Data on K2Re3TeC3(SN)3 by Materials Project

description: K2(CN)3Re3TeS3 crystallizes in the cubic Ia-3 space group. The structure is three-dimensional and consists of eight Re3TeS3 clusters and one K2(CN)3 framework. In each Re3TeS3 cluster, Re+3.67+ is bonded in a distorted rectangular see-saw-like geometry to one Te2- and three equivalent S2- atoms. The Re–Te bond length is 2.73 Å. There are a spread of Re–S bond distances ranging from 2.41–2.43 Å. Te2- is bonded in a 6-coordinate geometry to three equivalent Re+3.67+ atoms. S2- is bonded in a 5-coordinate geometry to three equivalent Re+3.67+ atoms. In the K2(CN)3 framework, there are two inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a distorted octahedral geometry to six equivalent N3- atoms. All K–N bond lengths are 2.98 Å. In the second K1+ site, K1+ is bonded in a 2-coordinate geometry to two equivalent N3- atoms. Both K–N bond lengths are 2.92 Å. C+1.33+ is bonded in a single-bond geometry to one N3- atom. The C–N bond length is 1.18 Å. N3- is bonded in a 1-coordinate geometry to two K1+ and one C+1.33+ atom.
DOI: 10.5517/ccdc.csd.cc1nhqmh
title: CCDC 1534457: Experimental Crystal Structure Determination

description: Related Article: Hui Zhou|2020|CSD Communication|||
DOI: 10.17188/1738129
title: Materials Data on Tm2InCu2 by Materials Project

description: Tm2Cu2In crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Tm is bonded in a 6-coordinate geometry to six equivalent Cu and four equivalent In atoms. There are two shorter (2.85 Å) and four longer (2.87 Å) Tm–Cu bond lengths. All Tm–In bond lengths are 3.32 Å. Cu is bonded in a 9-coordinate geometry to six equivalent Tm, one Cu, and two equivalent In atoms. The Cu–Cu bond length is 2.60 Å. Both Cu–In bond lengths are 3.01 Å. In is bonded to eight equivalent Tm and four equivalent Cu atoms to form a mixture of face and corner-sharing InTm8Cu4 cuboctahedra.
DOI: 10.5517/ccdc.csd.cc1nhqnj
title: CCDC 1534458: Experimental Crystal Structure Determination

description: Related Article: Hui Zhou|2020|CSD Communication|||
DOI: 10.17188/1738130
title: Materials Data on Mg2ZnGa by Materials Project

description: Mg2ZnGa crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Mg2ZnGa ribbons oriented in the (1, 0, 0) direction. Mg is bonded in a linear geometry to one Zn and one Ga atom. The Mg–Zn bond length is 2.69 Å. The Mg–Ga bond length is 2.64 Å. Zn is bonded in a linear geometry to two equivalent Mg atoms. Ga is bonded in a linear geometry to two equivalent Mg atoms.
DOI: 10.17188/1738131
title: Materials Data on YMg2 by Materials Project

description: Mg2Y is Bergman Structure: Mg32(Al,Zn)49 Bergman-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Mg sites. In the first Mg site, Mg is bonded to seven Mg and five equivalent Y atoms to form a mixture of corner, edge, and face-sharing MgY5Mg7 cuboctahedra. There are a spread of Mg–Mg bond distances ranging from 3.16–3.39 Å. There are a spread of Mg–Y bond distances ranging from 3.42–3.63 Å. In the second Mg site, Mg is bonded in a 11-coordinate geometry to seven Mg and four equivalent Y atoms. There are two shorter (3.07 Å) and two longer (3.39 Å) Mg–Mg bond lengths. All Mg–Y bond lengths are 3.30 Å. Y is bonded in a 12-coordinate geometry to nine Mg and three equivalent Y atoms. There are two shorter (3.39 Å) and one longer (3.48 Å) Y–Y bond lengths.
DOI: 10.17188/1738132
title: Materials Data on Mo4C3 by Materials Project

description: Mo4C3 crystallizes in the trigonal R-3m space group. The structure is two-dimensional and consists of three Mo4C3 sheets oriented in the (0, 0, 1) direction. there are two inequivalent Mo3+ sites. In the first Mo3+ site, Mo3+ is bonded to six C4- atoms to form a mixture of edge and corner-sharing MoC6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (2.21 Å) and three longer (2.22 Å) Mo–C bond lengths. In the second Mo3+ site, Mo3+ is bonded in a distorted T-shaped geometry to three equivalent C4- atoms. All Mo–C bond lengths are 2.06 Å. There are two inequivalent C4- sites. In the first C4- site, C4- is bonded to six Mo3+ atoms to form a mixture of edge and corner-sharing CMo6 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second C4- site, C4- is bonded to six equivalent Mo3+ atoms to form a mixture of edge and corner-sharing CMo6 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.5517/ccdc.csd.cc21zszt
title: CCDC 1906437: Experimental Crystal Structure Determination

description: Related Article: R. Doi, T. Okano, I. Abdullah, Y. Sato|2020|CSD Communication|||
DOI: 10.17188/1738133
title: Materials Data on InHO2 by Materials Project

description: InOOH crystallizes in the cubic Pa-3 space group. The structure is three-dimensional. In3+ is bonded to six equivalent O2- atoms to form corner-sharing InO6 octahedra. The corner-sharing octahedral tilt angles are 62°. All In–O bond lengths are 2.23 Å. H1+ is bonded in a linear geometry to two equivalent O2- atoms. Both H–O bond lengths are 1.21 Å. O2- is bonded in a distorted single-bond geometry to three equivalent In3+ and one H1+ atom.
DOI: 10.17188/1738134
title: Materials Data on Sr2ZnSb2 by Materials Project

description: Sr2ZnSb2 crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Sr2+ is bonded to six Sb3- atoms to form a mixture of distorted edge, corner, and face-sharing SrSb6 octahedra. The corner-sharing octahedra tilt angles range from 43–49°. There are three shorter (3.29 Å) and three longer (3.71 Å) Sr–Sb bond lengths. Zn2+ is bonded in a trigonal planar geometry to three equivalent Sb3- atoms. All Zn–Sb bond lengths are 2.71 Å. There are two inequivalent Sb3- sites. In the first Sb3- site, Sb3- is bonded in a 6-coordinate geometry to six equivalent Sr2+ atoms. In the second Sb3- site, Sb3- is bonded in a distorted trigonal planar geometry to six equivalent Sr2+ and three equivalent Zn2+ atoms.
DOI: 10.17188/1738135
title: Materials Data on SnWO4 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: 10.17188/1738136
title: Materials Data on Co2H21I7(N2O)3 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: 10.17188/1738137
title: Materials Data on Mg3Si4 by Materials Project

description: Mg3Si4 is Magnesium tetraboride-like structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Mg sites. In the first Mg site, Mg is bonded in a 6-coordinate geometry to two Mg and six Si atoms. There are one shorter (2.92 Å) and one longer (3.13 Å) Mg–Mg bond lengths. There are a spread of Mg–Si bond distances ranging from 2.76–2.92 Å. In the second Mg site, Mg is bonded in a distorted trigonal pyramidal geometry to two Mg and five Si atoms. There are one shorter (2.89 Å) and one longer (3.11 Å) Mg–Mg bond lengths. There are a spread of Mg–Si bond distances ranging from 2.73–3.20 Å. In the third Mg site, Mg is bonded in a 12-coordinate geometry to five Mg and seven Si atoms. There are a spread of Mg–Mg bond distances ranging from 2.97–3.19 Å. There are a spread of Mg–Si bond distances ranging from 2.72–3.24 Å. In the fourth Mg site, Mg is bonded in a 8-coordinate geometry to five Mg and eight Si atoms. There are one shorter (2.97 Å) and one longer (3.09 Å) Mg–Mg bond lengths. There are a spread of Mg–Si bond distances ranging from 2.79–3.08 Å. In the fifth Mg site, Mg is bonded in a 12-coordinate geometry to two Mg and six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.78–3.06 Å. In the sixth Mg site, Mg is bonded in a 6-coordinate geometry to two Mg and seven Si atoms. There are a spread of Mg–Si bond distances ranging from 2.84–3.13 Å. There are eight inequivalent Si sites. In the first Si site, Si is bonded in a 6-coordinate geometry to two Mg and four Si atoms. There are a spread of Si–Si bond distances ranging from 2.47–2.60 Å. In the second Si site, Si is bonded in a 8-coordinate geometry to four Mg and four Si atoms. There are a spread of Si–Si bond distances ranging from 2.48–2.56 Å. In the third Si site, Si is bonded in a 9-coordinate geometry to five Mg and three Si atoms. There are a spread of Si–Si bond distances ranging from 2.45–2.62 Å. In the fourth Si site, Si is bonded in a 9-coordinate geometry to six Mg and three Si atoms. In the fifth Si site, Si is bonded in a 8-coordinate geometry to four Mg and four Si atoms. The Si–Si bond length is 2.61 Å. In the sixth Si site, Si is bonded in a 8-coordinate geometry to six Mg and two Si atoms. In the seventh Si site, Si is bonded in a 9-coordinate geometry to six Mg and three Si atoms. In the eighth Si site, Si is bonded in a 7-coordinate geometry to six Mg and one Si atom.
DOI: 10.17188/1738138
title: Materials Data on La2CuO4 by Materials Project

description: La2CuO4 is (La,Ba)CuO4-like structured and crystallizes in the orthorhombic Cmce space group. The structure is three-dimensional. La3+ is bonded in a 1-coordinate geometry to nine O2- atoms. There are a spread of La–O bond distances ranging from 2.31–2.87 Å. Cu2+ is bonded to six O2- atoms to form corner-sharing CuO6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are four shorter (1.91 Å) and two longer (2.44 Å) Cu–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to five equivalent La3+ and one Cu2+ atom. In the second O2- site, O2- is bonded to four equivalent La3+ and two equivalent Cu2+ atoms to form a mixture of distorted corner, edge, and face-sharing OLa4Cu2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1738139
title: Materials Data on LiMnCo3O8 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: 10.17188/1738141
title: Materials Data on InOF2 by Materials Project

description: InOF2 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. In is bonded to two equivalent O and four equivalent F atoms to form distorted corner-sharing InO2F4 pentagonal pyramids. Both In–O bond lengths are 2.14 Å. There are two shorter (2.13 Å) and two longer (2.17 Å) In–F bond lengths. O is bonded in a bent 150 degrees geometry to two equivalent In atoms. F is bonded in a bent 150 degrees geometry to two equivalent In atoms.
DOI: 10.5517/ccdc.csd.cc251n41
title: CCDC 1997582: Experimental Crystal Structure Determination

description: Related Article: wei chen|2020|CSD Communication|||
description: Related Article: Hui Zhou, Wei Chen, Ji-Hong Liu, Wen-Zhen Zhang, Xiao-Bing Lu|2020|Green Chemistry|22|7832|doi:10.1039/D0GC03009K
DOI: 10.17188/1738142
title: Materials Data on KHg5Cl11 by Materials Project

description: KHg5Cl11 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. K1+ is bonded in a 10-coordinate geometry to ten Cl1- atoms. There are a spread of K–Cl bond distances ranging from 3.33–3.89 Å. There are two inequivalent Hg2+ sites. In the first Hg2+ site, Hg2+ is bonded in a distorted linear geometry to seven Cl1- atoms. There are a spread of Hg–Cl bond distances ranging from 2.33–3.43 Å. In the second Hg2+ site, Hg2+ is bonded in a distorted linear geometry to six Cl1- atoms. There are two shorter (2.34 Å) and four longer (3.38 Å) Hg–Cl bond lengths. There are four inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted single-bond geometry to three Hg2+ atoms. In the second Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one K1+ and three equivalent Hg2+ atoms. In the third Cl1- site, Cl1- is bonded to two equivalent K1+ and four equivalent Hg2+ atoms to form corner-sharing ClK2Hg4 octahedra. The corner-sharing octahedral tilt angles are 0°. In the fourth Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one K1+ and three Hg2+ atoms.
DOI: 10.5517/ccdc.csd.cc251n74
title: CCDC 1997585: Experimental Crystal Structure Determination

description: Related Article: wei chen|2020|CSD Communication|||
description: Related Article: Hui Zhou, Wei Chen, Ji-Hong Liu, Wen-Zhen Zhang, Xiao-Bing Lu|2020|Green Chemistry|22|7832|doi:10.1039/D0GC03009K
DOI: 10.5517/ccdc.csd.cc251n52
title: CCDC 1997583: Experimental Crystal Structure Determination

description: Related Article: wei chen|2020|CSD Communication|||
description: Related Article: Hui Zhou, Wei Chen, Ji-Hong Liu, Wen-Zhen Zhang, Xiao-Bing Lu|2020|Green Chemistry|22|7832|doi:10.1039/D0GC03009K
DOI: 10.17188/1738143
title: Materials Data on MnH4(BrO)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: 10.5517/ccdc.csd.cc251n63
title: CCDC 1997584: Experimental Crystal Structure Determination

description: Related Article: wei chen|2020|CSD Communication|||
description: Related Article: Hui Zhou, Wei Chen, Ji-Hong Liu, Wen-Zhen Zhang, Xiao-Bing Lu|2020|Green Chemistry|22|7832|doi:10.1039/D0GC03009K
DOI: 10.5517/ccdc.csd.cc26fdqs
title: CCDC 2038675: Experimental Crystal Structure Determination

description: Related Article: Inga Kholod, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc26fdrt
title: CCDC 2038676: Experimental Crystal Structure Determination

description: Related Article: Inga Kholod, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.17188/1738144
title: Materials Data on Co(IO3)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: 10.5517/ccdc.csd.cc26fdsv
title: CCDC 2038677: Experimental Crystal Structure Determination

description: Related Article: Inga Kholod, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc26fdtw
title: CCDC 2038678: Experimental Crystal Structure Determination

description: Related Article: Inga Kholod, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.17188/1738145
title: Materials Data on Y2ZnRh by Materials Project

description: Y2RhZn 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 Zn atoms. All Y–Rh bond lengths are 3.03 Å. All Y–Zn bond lengths are 3.03 Å. Rh 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: 10.5517/ccdc.csd.cc26fdvx
title: CCDC 2038679: Experimental Crystal Structure Determination

description: Related Article: Inga Kholod, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc26fdwy
title: CCDC 2038680: Experimental Crystal Structure Determination

description: Related Article: Inga Kholod, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc26fdxz
title: CCDC 2038681: Experimental Crystal Structure Determination

description: Related Article: Inga Kholod, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc26ff36
title: CCDC 2038687: Experimental Crystal Structure Determination

description: Related Article: Ana-Maria Buciumas, Reinhard Neier and Helen Stoeckli-Evans|2020|CSD Communication|||