cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1698524
title: Materials Data on Nd(SiPt)2 by Materials Project

description: Nd(PtSi)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Nd2+ is bonded in a 8-coordinate geometry to eight equivalent Si4- atoms. All Nd–Si bond lengths are 3.29 Å. Pt3+ is bonded in a 4-coordinate geometry to four equivalent Si4- atoms. All Pt–Si bond lengths are 2.43 Å. Si4- is bonded in a 4-coordinate geometry to four equivalent Nd2+ and four equivalent Pt3+ atoms.
DOI: 10.17188/1698525
title: Materials Data on Li2NbCr3O8 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.cc25p99h
title: CCDC 2016466: Experimental Crystal Structure Determination

description: Related Article: Guangwu Zhang|2020|CSD Communication|||
description: Related Article: Saisai Zhang, Xun-Yong Liu, Zhenbang Chang, Xinxin Qiao, Heng-Ying Xiong, Guangwu Zhang|2020|iScience|23|101705|doi:10.1016/j.isci.2020.101705
DOI: 10.5517/ccdc.csd.cc268g87
title: CCDC 2033918: Experimental Crystal Structure Determination

description: Related Article: Guangwu Zhang|2020|CSD Communication|||
description: Related Article: Saisai Zhang, Xun-Yong Liu, Zhenbang Chang, Xinxin Qiao, Heng-Ying Xiong, Guangwu Zhang|2020|iScience|23|101705|doi:10.1016/j.isci.2020.101705
DOI: 10.17188/1698526
title: Materials Data on Li(DySe2)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: 10.17188/1698527
title: Materials Data on Li4Cr3Ni2Sb3O16 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: 10.17188/1698528
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 eight Si atoms. There are a spread of Mg–Si bond distances ranging from 2.86–3.20 Å. In the second Mg site, Mg is bonded in a 5-coordinate geometry to five Si atoms. There are a spread of Mg–Si bond distances ranging from 2.64–2.99 Å. In the third Mg site, Mg is bonded in a 8-coordinate geometry to nine Si atoms. There are a spread of Mg–Si bond distances ranging from 2.77–3.24 Å. In the fourth Mg site, Mg is bonded in a 9-coordinate geometry to nine Si atoms. There are a spread of Mg–Si bond distances ranging from 2.70–2.94 Å. In the fifth Mg site, Mg is bonded in a 6-coordinate geometry to seven Si atoms. There are a spread of Mg–Si bond distances ranging from 2.75–3.24 Å. In the sixth Mg site, Mg is bonded in a distorted rectangular see-saw-like geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.77–3.23 Å. There are eight inequivalent Si sites. In the first Si site, Si is bonded in a 10-coordinate geometry to five Mg and five Si atoms. There are a spread of Si–Si bond distances ranging from 2.45–2.61 Å. In the second Si site, Si is bonded in a 8-coordinate geometry to four Mg and four Si atoms. There are one shorter (2.43 Å) and two longer (2.44 Å) Si–Si bond lengths. In the third Si site, Si is bonded in a 8-coordinate geometry to six Mg and three Si atoms. There are one shorter (2.47 Å) and one longer (2.90 Å) Si–Si bond lengths. In the fourth Si site, Si is bonded in a 10-coordinate geometry to six Mg and four Si atoms. The Si–Si bond length is 2.45 Å. In the fifth Si site, Si is bonded in a 9-coordinate geometry to seven Mg and two Si atoms. In the sixth Si site, Si is bonded in a 7-coordinate geometry to five Mg and two Si atoms. The Si–Si bond length is 2.38 Å. In the seventh Si site, Si is bonded in a 8-coordinate geometry to six Mg and two Si atoms. In the eighth Si site, Si is bonded in a 7-coordinate geometry to five Mg and two Si atoms.
DOI: 10.17188/1698530
title: Materials Data on TlSbAs2PbS6 by Materials Project

description: TlPbSbAs2S6 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Tl1+ is bonded in a 9-coordinate geometry to nine S2- atoms. There are a spread of Tl–S bond distances ranging from 3.29–3.98 Å. Pb2+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Pb–S bond distances ranging from 2.83–3.55 Å. Sb1- is bonded in a 3-coordinate geometry to three S2- atoms. There are a spread of Sb–S bond distances ranging from 2.49–2.54 Å. There are two inequivalent As5+ sites. In the first As5+ site, As5+ is bonded in a 3-coordinate geometry to three S2- atoms. There are one shorter (2.26 Å) and two longer (2.32 Å) As–S bond lengths. In the second As5+ site, As5+ is bonded in a trigonal non-coplanar geometry to three S2- atoms. There are a spread of As–S bond distances ranging from 2.26–2.36 Å. There are six inequivalent S2- sites. In the first S2- site, S2- is bonded in a 1-coordinate geometry to three equivalent Pb2+ and one As5+ atom. In the second S2- site, S2- is bonded in a 3-coordinate geometry to one Tl1+, one Sb1-, and one As5+ atom. In the third S2- site, S2- is bonded in a 2-coordinate geometry to three equivalent Tl1+ and two As5+ atoms. In the fourth S2- site, S2- is bonded in a 2-coordinate geometry to three equivalent Tl1+ and two equivalent Sb1- atoms. In the fifth S2- site, S2- is bonded in a 1-coordinate geometry to one Tl1+, two equivalent Pb2+, and one As5+ atom. In the sixth S2- site, S2- is bonded in a 1-coordinate geometry to one Tl1+, two equivalent Pb2+, and one As5+ atom.
DOI: 10.5517/ccdc.csd.cc26b0n7
title: CCDC 2035418: Experimental Crystal Structure Determination

description: Related Article: zhenlang Xie|2020|CSD Communication|||
DOI: 10.17188/1698531
title: Materials Data on Sc2V2O7 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.cc269xm2
title: CCDC 2035324: Experimental Crystal Structure Determination

description: Related Article: Huong Dau, Anthony Keyes, Hatice E. Basbug Alhan, Estela Ordonez, Enkhjargal Tsogtgerel, Anthony P. Gies, Evelyn Auyeung, Zhe Zhou, Asim Maity, Anuvab Das, David C. Powers, Dain B. Beezer, Eva Harth|2020|J.Am.Chem.Soc.|142|21469|doi:10.1021/jacs.0c10588
description: Related Article: Huong Dau|2020|CSD Communication|||
DOI: 10.17188/1698532
title: Materials Data on K2LiPrCl6 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.cc26b5j8
title: CCDC 2035569: Experimental Crystal Structure Determination

description: Related Article: Li Tian|2020|CSD Communication|||
description: Related Article: Meng Chen Wang, Jian Yun Shi, Zhi Long Ma, Li Tian|2020|Polyhedron|194|114928|doi:10.1016/j.poly.2020.114928
DOI: 10.5517/ccdc.csd.cc26b5k9
title: CCDC 2035570: Experimental Crystal Structure Determination

description: Related Article: Li Tian|2020|CSD Communication|||
description: Related Article: Meng Chen Wang, Jian Yun Shi, Zhi Long Ma, Li Tian|2020|Polyhedron|194|114928|doi:10.1016/j.poly.2020.114928
DOI: 10.5517/ccdc.csd.cc26b5lb
title: CCDC 2035571: Experimental Crystal Structure Determination

description: Related Article: Li Tian|2020|CSD Communication|||
description: Related Article: Meng Chen Wang, Jian Yun Shi, Zhi Long Ma, Li Tian|2020|Polyhedron|194|114928|doi:10.1016/j.poly.2020.114928
DOI: 10.5517/ccdc.csd.cc26bcmk
title: CCDC 2035758: Experimental Crystal Structure Determination

description: Related Article: Mustapha Tiouabi, Raphael Tabacchi and Helen Stoeckli-Evans|2020|CSD Communication|||
DOI: 10.5517/ccdc.csd.cc26bdcb
title: CCDC 2035781: Experimental Crystal Structure Determination

description: Related Article: Jonathan M. White, Sadegh Shabanibalajadeh, C. Hutton|2020|CSD Communication|||
DOI: 10.17188/1698534
title: Materials Data on Li3Cr5O8 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: 10.17188/1698535
title: Materials Data on Tm2Fe17C3 by Materials Project

description: Tm2Fe17C3 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Tm is bonded in a distorted trigonal planar geometry to four Fe and three equivalent C atoms. There are one shorter (3.07 Å) and three longer (3.31 Å) Tm–Fe bond lengths. All Tm–C bond lengths are 2.48 Å. There are four inequivalent Fe sites. In the first Fe site, Fe is bonded to two equivalent Tm and ten Fe atoms to form distorted FeTm2Fe10 cuboctahedra that share corners with four equivalent FeTm2Fe10 cuboctahedra, corners with two equivalent CTm2Fe4 octahedra, faces with four equivalent FeTm2Fe10 cuboctahedra, and faces with four equivalent CTm2Fe4 octahedra. The corner-sharing octahedral tilt angles are 44°. There are a spread of Fe–Fe bond distances ranging from 2.44–2.63 Å. In the second Fe site, Fe is bonded in a single-bond geometry to four Fe and one C atom. Both Fe–Fe bond lengths are 2.72 Å. The Fe–C bond length is 1.86 Å. In the third Fe site, Fe is bonded in a single-bond geometry to three Fe and one C atom. The Fe–Fe bond length is 2.65 Å. The Fe–C bond length is 1.91 Å. In the fourth Fe site, Fe is bonded in a 2-coordinate geometry to one Tm and thirteen Fe atoms. The Fe–Fe bond length is 2.40 Å. C is bonded to two equivalent Tm and four Fe atoms to form CTm2Fe4 octahedra that share corners with two equivalent FeTm2Fe10 cuboctahedra, corners with four equivalent CTm2Fe4 octahedra, and faces with four equivalent FeTm2Fe10 cuboctahedra. The corner-sharing octahedral tilt angles are 60°.
DOI: 10.5517/ccdc.csd.cc26bjvy
title: CCDC 2035920: Experimental Crystal Structure Determination

description: Related Article: Guangwu Zhang|2020|CSD Communication|||
description: Related Article: Saisai Zhang, Xun-Yong Liu, Zhenbang Chang, Xinxin Qiao, Heng-Ying Xiong, Guangwu Zhang|2020|iScience|23|101705|doi:10.1016/j.isci.2020.101705
DOI: 10.5517/ccdc.csd.cc25p9jq
title: CCDC 2016473: Experimental Crystal Structure Determination

description: Related Article: Guangwu Zhang|2020|CSD Communication|||
description: Related Article: Saisai Zhang, Xun-Yong Liu, Zhenbang Chang, Xinxin Qiao, Heng-Ying Xiong, Guangwu Zhang|2020|iScience|23|101705|doi:10.1016/j.isci.2020.101705
DOI: 10.17188/1698536
title: Materials Data on Ba2Sr2Y2Cu6O13 by Materials Project

description: Ba2Sr2Y2Cu6O13 crystallizes in the orthorhombic Fmm2 space group. The structure is three-dimensional. Ba2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Ba–O bond distances ranging from 2.69–3.02 Å. Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.65–2.90 Å. Y3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are a spread of Y–O bond distances ranging from 2.38–2.46 Å. There are three inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded to five O2- atoms to form distorted corner-sharing CuO5 square pyramids. There are a spread of Cu–O bond distances ranging from 1.93–2.49 Å. In the second Cu2+ site, Cu2+ is bonded to five O2- atoms to form corner-sharing CuO5 square pyramids. There are a spread of Cu–O bond distances ranging from 1.93–2.31 Å. In the third Cu2+ site, Cu2+ is bonded in a T-shaped geometry to three O2- atoms. There are a spread of Cu–O bond distances ranging from 1.83–1.92 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to two equivalent Sr2+, two equivalent Y3+, and two equivalent Cu2+ atoms. In the second O2- site, O2- is bonded in a 6-coordinate geometry to two equivalent Sr2+, two equivalent Y3+, and two equivalent Cu2+ atoms. In the third O2- site, O2- is bonded in a distorted linear geometry to two equivalent Ba2+, two equivalent Sr2+, and two equivalent Cu2+ atoms. In the fourth O2- site, O2- is bonded in a 6-coordinate geometry to four equivalent Ba2+ and two Cu2+ atoms. In the fifth O2- site, O2- is bonded in a 6-coordinate geometry to four equivalent Sr2+ and two Cu2+ atoms. In the sixth O2- site, O2- is bonded in a 6-coordinate geometry to two equivalent Ba2+, two equivalent Y3+, and two equivalent Cu2+ atoms. In the seventh O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+, two equivalent Y3+, and two equivalent Cu2+ atoms. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+, two equivalent Y3+, and two equivalent Cu2+ atoms. In the ninth O2- site, O2- is bonded in a distorted octahedral geometry to two equivalent Sr2+, two equivalent Y3+, and two equivalent Cu2+ atoms.
DOI: 10.5517/ccdc.csd.cc26h70z
title: CCDC 2040420: Experimental Crystal Structure Determination

description: Related Article: Carlos E. Puerto Galvis, Cristian C. Granados, Vladimir V. Kouznetsov, Mario A. Macías|2021|New J.Chem.|45|1565|doi:10.1039/D0NJ05235C
DOI: 10.17188/1698537
title: Materials Data on MnCr(Ni2Sn)2 by Materials Project

description: CrMn(Ni2Sn)2 is Tungsten-derived structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Cr is bonded in a distorted body-centered cubic geometry to eight Ni and six equivalent Sn atoms. There are six shorter (2.63 Å) and two longer (2.64 Å) Cr–Ni bond lengths. All Cr–Sn bond lengths are 3.03 Å. Mn is bonded in a distorted body-centered cubic geometry to eight Ni and six equivalent Sn atoms. There are two shorter (2.62 Å) and six longer (2.63 Å) Mn–Ni bond lengths. All Mn–Sn bond lengths are 3.04 Å. There are five inequivalent Ni sites. In the first Ni site, Ni is bonded in a distorted body-centered cubic geometry to three equivalent Cr, one Mn, and four equivalent Sn atoms. There are three shorter (2.62 Å) and one longer (2.63 Å) Ni–Sn bond lengths. In the second Ni site, Ni is bonded in a distorted body-centered cubic geometry to one Cr, three equivalent Mn, and four equivalent Sn atoms. The Ni–Cr bond length is 2.64 Å. There are one shorter (2.63 Å) and three longer (2.64 Å) Ni–Sn bond lengths. In the third Ni site, Ni is bonded in a distorted body-centered cubic geometry to one Cr, three equivalent Mn, and four equivalent Sn atoms. There are one shorter (2.63 Å) and three longer (2.64 Å) Ni–Sn bond lengths. In the fourth Ni site, Ni is bonded in a distorted body-centered cubic geometry to three equivalent Cr, one Mn, and four equivalent Sn atoms. There are three shorter (2.62 Å) and one longer (2.63 Å) Ni–Sn bond lengths. In the fifth Ni site, Ni is bonded in a distorted body-centered cubic geometry to three equivalent Cr, one Mn, and four equivalent Sn atoms. All Ni–Cr bond lengths are 2.63 Å. The Ni–Mn bond length is 2.62 Å. There are three shorter (2.62 Å) and one longer (2.63 Å) Ni–Sn bond lengths. Sn is bonded in a 8-coordinate geometry to three equivalent Cr, three equivalent Mn, and eight Ni atoms.
DOI: 10.5517/ccdc.csd.cc26h710
title: CCDC 2040421: Experimental Crystal Structure Determination

description: Related Article: Carlos E. Puerto Galvis, Cristian C. Granados, Vladimir V. Kouznetsov, Mario A. Macías|2021|New J.Chem.|45|1565|doi:10.1039/D0NJ05235C
DOI: 10.5517/ccdc.csd.cc26hn9p
title: CCDC 2040832: Experimental Crystal Structure Determination

description: Related Article: Christophe Kahlfuss, Eliot Starck, Elsa Tufenkjian, Nathalie Kyritsakas, Abdelaziz Jouaiti, Stéphane A. Baudron, Mir Wais Hosseini, Véronique Bulach|2021|CrystEngComm|23|944|doi:10.1039/D0CE01661F
DOI: 10.5517/ccdc.csd.cc26hnbq
title: CCDC 2040833: Experimental Crystal Structure Determination

description: Related Article: Christophe Kahlfuss, Eliot Starck, Elsa Tufenkjian, Nathalie Kyritsakas, Abdelaziz Jouaiti, Stéphane A. Baudron, Mir Wais Hosseini, Véronique Bulach|2021|CrystEngComm|23|944|doi:10.1039/D0CE01661F
DOI: 10.17188/1698538
title: Materials Data on HgPt2Se3 by Materials Project

description: Pt2HgSe3 crystallizes in the trigonal P-3m1 space group. The structure is two-dimensional and consists of one Pt2HgSe3 sheet oriented in the (0, 0, 1) direction. there are two inequivalent Pt2+ sites. In the first Pt2+ site, Pt2+ is bonded in an octahedral geometry to six equivalent Se2- atoms. All Pt–Se bond lengths are 2.57 Å. In the second Pt2+ site, Pt2+ is bonded in a square co-planar geometry to four equivalent Se2- atoms. All Pt–Se bond lengths are 2.49 Å. Hg2+ is bonded in a 6-coordinate geometry to three equivalent Se2- atoms. All Hg–Se bond lengths are 3.16 Å. Se2- is bonded in a 4-coordinate geometry to three Pt2+ and one Hg2+ atom.
DOI: 10.17188/1698539
title: Materials Data on PmYCu2 by Materials Project

description: PmYCu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pm is bonded in a body-centered cubic geometry to eight equivalent Cu atoms. All Pm–Cu bond lengths are 3.05 Å. Y is bonded in a body-centered cubic geometry to eight equivalent Cu atoms. All Y–Cu bond lengths are 3.05 Å. Cu is bonded in a body-centered cubic geometry to four equivalent Pm and four equivalent Y atoms.
DOI: 10.5517/ccdc.csd.cc26hnft
title: CCDC 2040836: Experimental Crystal Structure Determination

description: Related Article: Christophe Kahlfuss, Eliot Starck, Elsa Tufenkjian, Nathalie Kyritsakas, Abdelaziz Jouaiti, Stéphane A. Baudron, Mir Wais Hosseini, Véronique Bulach|2021|CrystEngComm|23|944|doi:10.1039/D0CE01661F
DOI: 10.17188/1698540
title: Materials Data on Li2VCr(P2O7)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: 10.17188/1698541
title: Materials Data on GaCoN2 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: 10.17188/1698542
title: Materials Data on La2Cu2SeSO2 by Materials Project

description: La2Cu2SeSO2 crystallizes in the tetragonal P4mm space group. The structure is two-dimensional and consists of one La2Cu2SeSO2 sheet oriented in the (0, 0, 1) direction. there are two inequivalent La3+ sites. In the first La3+ site, La3+ is bonded in a 4-coordinate geometry to four equivalent Se2- and four equivalent O2- atoms. All La–Se bond lengths are 3.30 Å. All La–O bond lengths are 2.38 Å. In the second La3+ site, La3+ is bonded in a 4-coordinate geometry to four equivalent O2- atoms. All La–O bond lengths are 2.37 Å. Cu1+ is bonded to two equivalent Se2- and two equivalent S2- atoms to form a mixture of edge and corner-sharing CuSe2S2 tetrahedra. Both Cu–Se bond lengths are 2.54 Å. Both Cu–S bond lengths are 2.42 Å. Se2- is bonded in a 12-coordinate geometry to four equivalent La3+ and four equivalent Cu1+ atoms. S2- is bonded in a 4-coordinate geometry to four equivalent Cu1+ atoms. O2- is bonded to four La3+ atoms to form a mixture of edge and corner-sharing OLa4 tetrahedra.
DOI: 10.17188/1698543
title: Materials Data on CeNiO3 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: 10.17188/1698544
title: Materials Data on LiAlO3 by Materials Project

description: LiAlO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Li is bonded to twelve equivalent O atoms to form LiO12 cuboctahedra that share corners with twelve equivalent LiO12 cuboctahedra, faces with six equivalent LiO12 cuboctahedra, and faces with eight equivalent AlO6 octahedra. All Li–O bond lengths are 2.62 Å. Al is bonded to six equivalent O atoms to form AlO6 octahedra that share corners with six equivalent AlO6 octahedra and faces with eight equivalent LiO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Al–O bond lengths are 1.85 Å. O is bonded in a linear geometry to four equivalent Li and two equivalent Al atoms.
DOI: 10.5517/ccdc.csd.cc26jtvf
title: CCDC 2041965: Experimental Crystal Structure Determination

description: Related Article: André Schumann, Jonas Bresien, Malte Fischer, Christian Hering-Junghans|2021|Chem.Commun.|57|1014|doi:10.1039/D0CC07533G
DOI: 10.5517/ccdc.csd.cc26jtwg
title: CCDC 2041966: Experimental Crystal Structure Determination

description: Related Article: André Schumann, Jonas Bresien, Malte Fischer, Christian Hering-Junghans|2021|Chem.Commun.|57|1014|doi:10.1039/D0CC07533G
DOI: 10.5517/ccdc.csd.cc26jtxh
title: CCDC 2041967: Experimental Crystal Structure Determination

description: Related Article: André Schumann, Jonas Bresien, Malte Fischer, Christian Hering-Junghans|2021|Chem.Commun.|57|1014|doi:10.1039/D0CC07533G
DOI: 10.5517/ccdc.csd.cc26jtyj
title: CCDC 2041968: Experimental Crystal Structure Determination

description: Related Article: André Schumann, Jonas Bresien, Malte Fischer, Christian Hering-Junghans|2021|Chem.Commun.|57|1014|doi:10.1039/D0CC07533G