cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1708769
title: Materials Data on TbSi3Ni8 by Materials Project

description: TbNi8Si3 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Tb3+ is bonded in a 6-coordinate geometry to six Si4- atoms. There are a spread of Tb–Si bond distances ranging from 3.12–3.32 Å. There are five inequivalent Ni+1.12+ sites. In the first Ni+1.12+ site, Ni+1.12+ is bonded in a 3-coordinate geometry to three Si4- atoms. There are a spread of Ni–Si bond distances ranging from 2.35–2.54 Å. In the second Ni+1.12+ site, Ni+1.12+ is bonded in a trigonal non-coplanar geometry to three Si4- atoms. There are a spread of Ni–Si bond distances ranging from 2.33–2.36 Å. In the third Ni+1.12+ site, Ni+1.12+ is bonded to four Si4- atoms to form a mixture of edge and corner-sharing NiSi4 tetrahedra. There are a spread of Ni–Si bond distances ranging from 2.35–2.48 Å. In the fourth Ni+1.12+ site, Ni+1.12+ is bonded in a distorted rectangular see-saw-like geometry to four Si4- atoms. There are two shorter (2.57 Å) and two longer (2.66 Å) Ni–Si bond lengths. In the fifth Ni+1.12+ site, Ni+1.12+ is bonded in a distorted rectangular see-saw-like geometry to four equivalent Si4- atoms. There are two shorter (2.36 Å) and two longer (2.40 Å) Ni–Si bond lengths. There are two inequivalent Si4- sites. In the first Si4- site, Si4- is bonded in a 12-coordinate geometry to two equivalent Tb3+, nine Ni+1.12+, and one Si4- atom. The Si–Si bond length is 2.66 Å. In the second Si4- site, Si4- is bonded in a 12-coordinate geometry to two equivalent Tb3+ and ten Ni+1.12+ atoms.
DOI: 10.17188/1708770
title: Materials Data on MnFeO4 by Materials Project

description: FeMnO4 crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. Mn is bonded to six O atoms to form MnO6 octahedra that share corners with six equivalent FeO4 tetrahedra and edges with two equivalent MnO6 octahedra. There is two shorter (1.90 Å) and four longer (1.95 Å) Mn–O bond length. Fe is bonded to four O atoms to form FeO4 tetrahedra that share corners with six equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 51–57°. There is two shorter (1.83 Å) and two longer (1.91 Å) Fe–O bond length. There are two inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to one Mn and one Fe atom. In the second O site, O is bonded in a trigonal planar geometry to two equivalent Mn and one Fe atom.
DOI: 10.17188/1708771
title: Materials Data on Cr2HgS4 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: 10.6084/m9.figshare.13681828.v1
title: Database Lung Cancer

description: <b>The impact of Coping Styles on the Relationship between the Cognitive Appraisal of the Disease and Stress Level in Lung Cancer Patients</b>
DOI: 10.6084/m9.figshare.13681828
title: Database Lung Cancer

description: <b>The impact of Coping Styles on the Relationship between the Cognitive Appraisal of the Disease and Stress Level in Lung Cancer Patients</b>
DOI: 10.17188/1708772
title: Materials Data on Li2FePO5 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: 10.17188/1708773
title: Materials Data on La4Al2O9 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: 10.17188/1708774
title: Materials Data on LiFeSi3O8 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: 10.17188/1708775
title: Materials Data on K2H14Rh2N12O17 by Materials Project

description: K2(NO2)7(Rh)2(NH3)4NO2H2O crystallizes in the triclinic P-1 space group. The structure is two-dimensional and consists of eight ammonia molecules; two hydroxylamine, n-hydroxy- molecules; four rhodium molecules; two water molecules; and one K2(NO2)7 sheet oriented in the (0, 0, 1) direction. In the K2(NO2)7 sheet, there are two inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of K–O bond distances ranging from 2.66–3.30 Å. In the second K1+ site, K1+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of K–O bond distances ranging from 2.84–3.33 Å. There are seven inequivalent N1+ sites. In the first N1+ site, N1+ is bonded in a bent 120 degrees geometry to two O2- atoms. There is one shorter (1.24 Å) and one longer (1.26 Å) N–O bond length. In the second N1+ site, N1+ is bonded in a bent 120 degrees geometry to two O2- atoms. Both N–O bond lengths are 1.25 Å. In the third N1+ site, N1+ is bonded in a bent 120 degrees geometry to two O2- atoms. Both N–O bond lengths are 1.25 Å. In the fourth N1+ site, N1+ is bonded in a bent 120 degrees geometry to two O2- atoms. Both N–O bond lengths are 1.25 Å. In the fifth N1+ site, N1+ is bonded in a bent 120 degrees geometry to two O2- atoms. Both N–O bond lengths are 1.25 Å. In the sixth N1+ site, N1+ is bonded in a bent 120 degrees geometry to two O2- atoms. Both N–O bond lengths are 1.25 Å. In the seventh N1+ site, N1+ is bonded in a bent 120 degrees geometry to two O2- atoms. Both N–O bond lengths are 1.25 Å. There are fourteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to two K1+ and one N1+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one K1+ and one N1+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one K1+ and one N1+ atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one N1+ atom. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent K1+ and one N1+ atom. In the sixth O2- site, O2- is bonded in a single-bond geometry to one N1+ atom. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to two K1+ and one N1+ atom. In the eighth O2- site, O2- is bonded in a distorted single-bond geometry to three K1+ and one N1+ atom. In the ninth O2- site, O2- is bonded in a single-bond geometry to one K1+ and one N1+ atom. In the tenth O2- site, O2- is bonded in a distorted single-bond geometry to one K1+ and one N1+ atom. In the eleventh O2- site, O2- is bonded in a distorted single-bond geometry to two K1+ and one N1+ atom. In the twelfth O2- site, O2- is bonded in a single-bond geometry to one K1+ and one N1+ atom. In the thirteenth O2- site, O2- is bonded in a distorted single-bond geometry to two K1+ and one N1+ atom. In the fourteenth O2- site, O2- is bonded in a distorted single-bond geometry to one K1+ and one N1+ atom.
DOI: 10.17188/1708776
title: Materials Data on LaNO5 by Materials Project

description: LaNO5 crystallizes in the monoclinic P2_1 space group. The structure is two-dimensional and consists of one LaNO5 sheet oriented in the (0, 0, 1) direction. La is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of La–O bond distances ranging from 2.34–2.78 Å. N is bonded in a trigonal planar geometry to three O atoms. There are a spread of N–O bond distances ranging from 1.22–1.33 Å. There are five inequivalent O sites. In the first O site, O is bonded in a 1-coordinate geometry to two equivalent La and one N atom. In the second O site, O is bonded in a single-bond geometry to one N atom. In the third O site, O is bonded in a distorted single-bond geometry to three equivalent La atoms. In the fourth O site, O is bonded in a trigonal planar geometry to three equivalent La atoms. In the fifth O site, O is bonded in a distorted single-bond geometry to one La and one N atom.
DOI: 10.17188/1708777
title: Materials Data on Er2TiCuO6 by Materials Project

description: Er2TiCuO6 crystallizes in the trigonal P3m1 space group. The structure is three-dimensional. there are two inequivalent Er3+ sites. In the first Er3+ site, Er3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Er–O bond distances ranging from 2.17–2.55 Å. In the second Er3+ site, Er3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Er–O bond distances ranging from 2.17–2.55 Å. Ti4+ is bonded to five O2- atoms to form corner-sharing TiO5 trigonal bipyramids. There are a spread of Ti–O bond distances ranging from 1.87–2.07 Å. Cu2+ is bonded to five O2- atoms to form corner-sharing CuO5 trigonal bipyramids. There is two shorter (1.92 Å) and three longer (2.07 Å) Cu–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to three equivalent Er3+ and one Ti4+ atom. In the second O2- site, O2- is bonded to three equivalent Er3+ and one Cu2+ atom to form OEr3Cu tetrahedra that share corners with seven OEr3Cu tetrahedra and edges with three equivalent OEr2Cu3 trigonal bipyramids. In the third O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Ti4+ atoms. In the fourth O2- site, O2- is bonded to two Er3+ and three equivalent Cu2+ atoms to form OEr2Cu3 trigonal bipyramids that share corners with six equivalent OEr2Cu3 trigonal bipyramids and edges with six OEr3Cu tetrahedra. In the fifth O2- site, O2- is bonded to three equivalent Er3+ and one Cu2+ atom to form OEr3Cu tetrahedra that share corners with seven OEr3Cu tetrahedra and edges with three equivalent OEr2Cu3 trigonal bipyramids. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to three equivalent Er3+ and one Ti4+ atom.
DOI: 10.17188/1708778
title: Materials Data on Sm3(Al3Os)4 by Materials Project

description: Sm3(OsAl3)4 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Sm is bonded in a 1-coordinate geometry to four equivalent Os and eleven Al atoms. All Sm–Os bond lengths are 3.40 Å. There are a spread of Sm–Al bond distances ranging from 2.96–3.24 Å. There are two inequivalent Os sites. In the first Os site, Os is bonded in a body-centered cubic geometry to eight Al atoms. There are two shorter (2.41 Å) and six longer (2.61 Å) Os–Al bond lengths. In the second Os site, Os is bonded in a 12-coordinate geometry to four equivalent Sm and eight Al atoms. There are a spread of Os–Al bond distances ranging from 2.57–2.70 Å. There are four inequivalent Al sites. In the first Al site, Al is bonded in a 3-coordinate geometry to three equivalent Sm and three equivalent Os atoms. In the second Al site, Al is bonded in a 3-coordinate geometry to three equivalent Sm and three Os atoms. In the third Al site, Al is bonded in a 2-coordinate geometry to two equivalent Sm and two equivalent Os atoms. In the fourth Al site, Al is bonded to three equivalent Sm and two equivalent Os atoms to form distorted corner-sharing AlSm3Os2 trigonal bipyramids.
DOI: 10.17188/1708779
title: Materials Data on Cu3MoH24C8S3I3N2O 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: 10.17188/1708780
title: Materials Data on Y2(B2Rh3)3 by Materials Project

description: Y2(Rh3B2)3 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Y is bonded in a 6-coordinate geometry to six equivalent Rh atoms. All Y–Rh bond lengths are 3.02 Å. There are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 4-coordinate geometry to two equivalent Y and four B atoms. There are two shorter (2.15 Å) and two longer (2.17 Å) Rh–B bond lengths. In the second Rh site, Rh is bonded in a distorted square co-planar geometry to four equivalent B atoms. All Rh–B bond lengths are 2.17 Å. There are two inequivalent B sites. In the first B site, B is bonded to six equivalent Rh atoms to form distorted edge-sharing BRh6 pentagonal pyramids. In the second B site, B is bonded in a 6-coordinate geometry to six Rh atoms.
DOI: 10.17188/1708782
title: Materials Data on ZrVW by Materials Project

description: ZrVW crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. Zr is bonded in a 12-coordinate geometry to six equivalent V and six equivalent W atoms. There are two shorter (3.11 Å) and four longer (3.12 Å) Zr–V bond lengths. There are two shorter (3.11 Å) and four longer (3.12 Å) Zr–W bond lengths. V is bonded to six equivalent Zr, two equivalent V, and four equivalent W atoms to form distorted VZr6V2W4 cuboctahedra that share corners with eight equivalent WZr6V4W2 cuboctahedra, corners with ten equivalent VZr6V2W4 cuboctahedra, edges with six equivalent VZr6V2W4 cuboctahedra, faces with six equivalent VZr6V2W4 cuboctahedra, and faces with twelve equivalent WZr6V4W2 cuboctahedra. Both V–V bond lengths are 2.66 Å. All V–W bond lengths are 2.66 Å. W is bonded to six equivalent Zr, four equivalent V, and two equivalent W atoms to form distorted WZr6V4W2 cuboctahedra that share corners with eight equivalent VZr6V2W4 cuboctahedra, corners with ten equivalent WZr6V4W2 cuboctahedra, edges with six equivalent WZr6V4W2 cuboctahedra, faces with six equivalent WZr6V4W2 cuboctahedra, and faces with twelve equivalent VZr6V2W4 cuboctahedra. Both W–W bond lengths are 2.66 Å.
DOI: 10.17188/1708783
title: Materials Data on Co(N3O4)3 by Materials Project

description: (Co)2(N2)3(NO2)12 crystallizes in the cubic Fm-3 space group. The structure is zero-dimensional and consists of twelve ammonia molecules, four cobalt molecules, and twenty-four nitrous acid molecules.
DOI: 10.17188/1708784
title: Materials Data on BaErCuSe3 by Materials Project

description: BaErCuSe3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Ba2+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of Ba–Se bond distances ranging from 3.27–3.64 Å. Er3+ is bonded to six Se2- atoms to form ErSe6 octahedra that share corners with two equivalent ErSe6 octahedra, edges with two equivalent ErSe6 octahedra, and edges with four equivalent CuSe4 tetrahedra. The corner-sharing octahedral tilt angles are 40°. There are two shorter (2.81 Å) and four longer (2.87 Å) Er–Se bond lengths. Cu1+ is bonded to four Se2- atoms to form CuSe4 tetrahedra that share corners with two equivalent CuSe4 tetrahedra and edges with four equivalent ErSe6 octahedra. There are two shorter (2.46 Å) and two longer (2.52 Å) Cu–Se bond lengths. There are two inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a 6-coordinate geometry to three equivalent Ba2+, two equivalent Er3+, and one Cu1+ atom. In the second Se2- site, Se2- is bonded in a 6-coordinate geometry to two equivalent Ba2+, two equivalent Er3+, and two equivalent Cu1+ atoms.
DOI: 10.17188/1708785
title: Materials Data on Dy(VCo5)2 by Materials Project

description: DyCo10V2 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Dy is bonded in a 12-coordinate geometry to two equivalent V and eighteen Co atoms. Both Dy–V bond lengths are 3.01 Å. There are a spread of Dy–Co bond distances ranging from 2.95–3.17 Å. V is bonded in a 9-coordinate geometry to one Dy, one V, and twelve Co atoms. The V–V bond length is 2.32 Å. There are a spread of V–Co bond distances ranging from 2.56–2.86 Å. There are four inequivalent Co sites. In the first Co site, Co is bonded to two equivalent Dy, two equivalent V, and eight Co atoms to form a mixture of distorted edge, face, and corner-sharing CoDy2V2Co8 cuboctahedra. There are a spread of Co–Co bond distances ranging from 2.40–2.61 Å. In the second Co site, Co is bonded to two equivalent Dy, two equivalent V, and eight Co atoms to form a mixture of distorted edge, face, and corner-sharing CoDy2V2Co8 cuboctahedra. There are four shorter (2.40 Å) and two longer (2.61 Å) Co–Co bond lengths. In the third Co site, Co is bonded to two equivalent Dy, two equivalent V, and eight Co atoms to form a mixture of distorted edge, face, and corner-sharing CoDy2V2Co8 cuboctahedra. There are two shorter (2.33 Å) and two longer (2.56 Å) Co–Co bond lengths. In the fourth Co site, Co is bonded in a 2-coordinate geometry to one Dy, four equivalent V, and nine Co atoms. The Co–Co bond length is 2.34 Å.
DOI: 10.17188/1708787
title: Materials Data on Cr2FeNO8 by Materials Project

description: (Cr2FeO8)2N2 crystallizes in the monoclinic P2_1/c space group. The structure is two-dimensional and consists of four ammonia molecules and two Cr2FeO8 sheets oriented in the (0, 1, 0) direction. In each Cr2FeO8 sheet, there are two inequivalent Cr4+ sites. In the first Cr4+ site, Cr4+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with three equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 32–47°. There are a spread of Cr–O bond distances ranging from 1.61–1.70 Å. In the second Cr4+ site, Cr4+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with three equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 13–45°. There are a spread of Cr–O bond distances ranging from 1.61–1.69 Å. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six CrO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 2.00–2.04 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr4+ and one Fe3+ atom. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Cr4+ and one Fe3+ atom. In the third O2- site, O2- is bonded in a linear geometry to one Cr4+ and one Fe3+ atom. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr4+ and one Fe3+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one Cr4+ atom. In the sixth O2- site, O2- is bonded in a single-bond geometry to one Cr4+ atom. In the seventh O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr4+ and one Fe3+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr4+ and one Fe3+ atom.
DOI: 10.17188/1708789
title: Materials Data on Ga2(TeO3)3 by Materials Project

description: Ga2(TeO3)3 crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. Ga3+ is bonded to six O2- atoms to form face-sharing GaO6 octahedra. There are three shorter (1.95 Å) and three longer (2.08 Å) Ga–O bond lengths. Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. There is two shorter (1.92 Å) and one longer (1.94 Å) Te–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to one Ga3+ and one Te4+ atom. In the second O2- site, O2- is bonded in a trigonal non-coplanar geometry to two equivalent Ga3+ and one Te4+ atom.
DOI: 10.17188/1708791
title: Materials Data on Hf2BIr6 by Materials Project

description: Hf2Ir6B crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Hf is bonded to twelve Ir atoms to form HfIr12 cuboctahedra that share corners with twelve equivalent HfIr12 cuboctahedra, faces with six equivalent HfIr12 cuboctahedra, and faces with four equivalent BIr6 octahedra. There are a spread of Hf–Ir bond distances ranging from 2.79–2.93 Å. There are three inequivalent Ir sites. In the first Ir site, Ir is bonded to four equivalent Hf and two equivalent B atoms to form a mixture of distorted edge, corner, and face-sharing IrHf4B2 octahedra. The corner-sharing octahedral tilt angles are 0°. Both Ir–B bond lengths are 2.05 Å. In the second Ir site, Ir is bonded in a distorted square co-planar geometry to four equivalent Hf atoms. In the third Ir site, Ir is bonded in a 5-coordinate geometry to four equivalent Hf and one B atom. The Ir–B bond length is 2.08 Å. B is bonded to six Ir atoms to form BIr6 octahedra that share corners with four equivalent BIr6 octahedra and faces with eight equivalent HfIr12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1708792
title: Materials Data on Sc2Te3 by Materials Project

description: Sc2Te3 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Sc3+ is bonded to six Te2- atoms to form a mixture of edge and corner-sharing ScTe6 octahedra. The corner-sharing octahedra tilt angles range from 0–3°. There are a spread of Sc–Te bond distances ranging from 2.92–2.94 Å. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a square co-planar geometry to four equivalent Sc3+ atoms. In the second Te2- site, Te2- is bonded in a rectangular see-saw-like geometry to four equivalent Sc3+ atoms.
DOI: 10.17188/1708793
title: Materials Data on U2Cu(GeO9)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: 10.17188/1708795
title: Materials Data on MgTi by Materials Project

description: MgTi is TlF-II structured and crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. Mg is bonded to six equivalent Mg and six equivalent Ti atoms to form distorted MgMg6Ti6 cuboctahedra that share corners with six equivalent MgMg6Ti6 cuboctahedra, corners with twelve equivalent TiMg6Ti6 cuboctahedra, edges with eight equivalent MgMg6Ti6 cuboctahedra, edges with ten equivalent TiMg6Ti6 cuboctahedra, faces with ten equivalent MgMg6Ti6 cuboctahedra, and faces with ten equivalent TiMg6Ti6 cuboctahedra. There are four shorter (3.03 Å) and two longer (3.08 Å) Mg–Mg bond lengths. There are a spread of Mg–Ti bond distances ranging from 3.00–3.47 Å. Ti is bonded to six equivalent Mg and six equivalent Ti atoms to form distorted TiMg6Ti6 cuboctahedra that share corners with six equivalent TiMg6Ti6 cuboctahedra, corners with twelve equivalent MgMg6Ti6 cuboctahedra, edges with eight equivalent TiMg6Ti6 cuboctahedra, edges with ten equivalent MgMg6Ti6 cuboctahedra, faces with ten equivalent MgMg6Ti6 cuboctahedra, and faces with ten equivalent TiMg6Ti6 cuboctahedra. There are four shorter (2.83 Å) and two longer (2.94 Å) Ti–Ti bond lengths.
DOI: 10.17188/1708798
title: Materials Data on DyHg2 by Materials Project

description: DyHg2 crystallizes in the trigonal P-3m1 space group. The structure is two-dimensional and consists of one DyHg2 sheet oriented in the (0, 0, 1) direction. Dy is bonded in a distorted hexagonal planar geometry to six equivalent Hg atoms. All Dy–Hg bond lengths are 3.10 Å. Hg is bonded in a distorted trigonal planar geometry to three equivalent Dy atoms.