cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1711034
title: Materials Data on Dy3GaNiSe7 by Materials Project

description: Dy3NiGaSe7 crystallizes in the hexagonal P6_3 space group. The structure is three-dimensional. Dy3+ is bonded in a 7-coordinate geometry to seven Se2- atoms. There are a spread of Dy–Se bond distances ranging from 2.86–3.17 Å. Ni2+ is bonded to six equivalent Se2- atoms to form face-sharing NiSe6 octahedra. There are three shorter (2.54 Å) and three longer (2.67 Å) Ni–Se bond lengths. Ga3+ is bonded in a tetrahedral geometry to four Se2- atoms. There are one shorter (2.41 Å) and three longer (2.42 Å) Ga–Se bond lengths. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a distorted rectangular see-saw-like geometry to three equivalent Dy3+ and one Ga3+ atom. In the second Se2- site, Se2- is bonded to three equivalent Dy3+ and one Ga3+ atom to form distorted corner-sharing SeDy3Ga tetrahedra. In the third Se2- site, Se2- is bonded to three equivalent Dy3+ and two equivalent Ni2+ atoms to form distorted SeDy3Ni2 square pyramids that share corners with two equivalent SeDy3Ni2 square pyramids, corners with three equivalent SeDy3Ga tetrahedra, edges with four equivalent SeDy3Ni2 square pyramids, and faces with two equivalent SeDy3Ni2 square pyramids.
DOI: 10.17188/1711035
title: Materials Data on KFeS2O9 by Materials Project

description: KFeS2O9 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. K is bonded in a 10-coordinate geometry to ten O atoms. There are a spread of K–O bond distances ranging from 2.82–3.11 Å. Fe is bonded to six O atoms to form FeO6 octahedra that share corners with five SO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 2.00–2.08 Å. There are two inequivalent S sites. In the first S site, S is bonded to four O atoms to form SO4 tetrahedra that share corners with two equivalent FeO6 octahedra. The corner-sharing octahedral tilt angles are 40°. There are a spread of S–O bond distances ranging from 1.46–1.52 Å. In the second S site, S is bonded to four O atoms to form SO4 tetrahedra that share corners with three equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 35–45°. There are a spread of S–O bond distances ranging from 1.46–1.50 Å. There are seven inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to one K and one S atom. In the second O site, O is bonded in a single-bond geometry to two equivalent K and one S atom. In the third O site, O is bonded in a 2-coordinate geometry to one K, one Fe, and one S atom. In the fourth O site, O is bonded in a bent 150 degrees geometry to one Fe and one S atom. In the fifth O site, O is bonded in a distorted single-bond geometry to three equivalent K and one S atom. In the sixth O site, O is bonded in a 3-coordinate geometry to one K, one Fe, and one S atom. In the seventh O site, O is bonded in a single-bond geometry to one Fe atom.
DOI: 10.17188/1711036
title: Materials Data on FeH18(NO6)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: 10.17188/1711038
title: Materials Data on Cs by Materials Project

description: Cs is Magnesium structured and crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. Cs is bonded in a 12-coordinate geometry to eight equivalent Cs atoms. There are a spread of Cs–Cs bond distances ranging from 5.24–5.53 Å.
DOI: 10.17188/1711039
title: Materials Data on LiGa2Co by Materials Project

description: LiCoGa2 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 Co and eight equivalent Ga atoms. All Li–Co bond lengths are 2.95 Å. All Li–Ga bond lengths are 2.55 Å. Co is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Ga atoms. All Co–Ga bond lengths are 2.55 Å. Ga is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent Co atoms.
DOI: 10.17188/1711040
title: Materials Data on Sm(Cd10Ni)2 by Materials Project

description: Sm(NiCd10)2 crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Sm is bonded in a 4-coordinate geometry to sixteen Cd atoms. There are four shorter (3.41 Å) and twelve longer (3.45 Å) Sm–Cd bond lengths. Ni is bonded to twelve Cd atoms to form NiCd12 cuboctahedra that share corners with six equivalent NiCd12 cuboctahedra, edges with eighteen equivalent CdSmCd10Ni cuboctahedra, and faces with six equivalent CdSmCd10Ni cuboctahedra. There are six shorter (2.79 Å) and six longer (3.08 Å) Ni–Cd bond lengths. There are three inequivalent Cd sites. In the first Cd site, Cd is bonded in a distorted linear geometry to two equivalent Ni and ten Cd atoms. There are a spread of Cd–Cd bond distances ranging from 2.97–3.12 Å. In the second Cd site, Cd is bonded to one Sm, one Ni, and ten Cd atoms to form distorted CdSmCd10Ni cuboctahedra that share corners with fifteen equivalent CdSmCd10Ni cuboctahedra, edges with two equivalent CdSmCd10Ni cuboctahedra, edges with three equivalent NiCd12 cuboctahedra, a faceface with one NiCd12 cuboctahedra, and faces with fifteen equivalent CdSmCd10Ni cuboctahedra. There are a spread of Cd–Cd bond distances ranging from 2.90–3.35 Å. In the third Cd site, Cd is bonded in a distorted linear geometry to two equivalent Sm and twelve equivalent Cd atoms.
DOI: 10.17188/1711041
title: Materials Data on Mg16PaAl12 by Materials Project

description: Mg16PaAl12 crystallizes in the cubic I-43m space group. The structure is three-dimensional. there are two inequivalent Mg sites. In the first Mg site, Mg is bonded in a 12-coordinate geometry to seven Mg and five equivalent Al atoms. There are a spread of Mg–Mg bond distances ranging from 3.02–3.16 Å. There are a spread of Mg–Al bond distances ranging from 2.86–3.19 Å. In the second Mg site, Mg is bonded in a 10-coordinate geometry to three equivalent Mg, one Pa, and six equivalent Al atoms. The Mg–Pa bond length is 3.30 Å. All Mg–Al bond lengths are 3.18 Å. Pa is bonded in a 4-coordinate geometry to four equivalent Mg and twelve equivalent Al atoms. All Pa–Al bond lengths are 3.21 Å. Al is bonded in a 11-coordinate geometry to seven Mg, one Pa, and three equivalent Al atoms. There are one shorter (2.70 Å) and two longer (2.76 Å) Al–Al bond lengths.
DOI: 10.17188/1711042
title: Materials Data on Mn3(PO4)4 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: 10.17188/1711043
title: Materials Data on Sr5(MnN3)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: 10.17188/1711044
title: Materials Data on MgAsPd2 by Materials Project

description: MgPd2As crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two MgPd2As ribbons oriented in the (1, 0, 0) direction. Mg is bonded in a linear geometry to two equivalent Pd atoms. Both Mg–Pd bond lengths are 2.63 Å. Pd is bonded in a linear geometry to one Mg and one As atom. The Pd–As bond length is 2.28 Å. As is bonded in a linear geometry to two equivalent Pd atoms.
DOI: 10.17188/1711045
title: Materials Data on MgSb by Materials Project

description: MgSb crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are two inequivalent Mg2+ sites. In the first Mg2+ site, Mg2+ is bonded to eight Sb2- atoms to form distorted MgSb8 hexagonal bipyramids that share corners with two equivalent MgSb8 hexagonal bipyramids, corners with four equivalent MgSb4 trigonal pyramids, edges with six equivalent MgSb8 hexagonal bipyramids, and edges with eight equivalent MgSb4 trigonal pyramids. There are a spread of Mg–Sb bond distances ranging from 2.91–3.32 Å. In the second Mg2+ site, Mg2+ is bonded to four Sb2- atoms to form distorted MgSb4 trigonal pyramids that share corners with two equivalent MgSb8 hexagonal bipyramids, corners with eight equivalent MgSb4 trigonal pyramids, and edges with four equivalent MgSb8 hexagonal bipyramids. There are a spread of Mg–Sb bond distances ranging from 2.98–3.08 Å. There are two inequivalent Sb2- sites. In the first Sb2- site, Sb2- is bonded in a 8-coordinate geometry to five Mg2+ and three equivalent Sb2- atoms. There are one shorter (3.01 Å) and two longer (3.35 Å) Sb–Sb bond lengths. In the second Sb2- site, Sb2- is bonded to six Mg2+ atoms to form distorted corner-sharing SbMg6 pentagonal pyramids.
DOI: 10.17188/1711047
title: Materials Data on KH2C4N3O4 by Materials Project

description: KC3N2O3CNOH2 crystallizes in the monoclinic P2_1/c space group. The structure is two-dimensional and consists of eight hydrogen molecules; one KC3N2O3 sheet oriented in the (0, 0, 1) direction; and four ~{n}-methylidenehydroxylamine molecules. In the KC3N2O3 sheet, K1+ is bonded in a distorted trigonal pyramidal geometry to one N3- and three O2- atoms. The K–N bond length is 2.79 Å. There are one shorter (2.64 Å) and two longer (2.69 Å) K–O bond lengths. There are three inequivalent C+3.50+ sites. In the first C+3.50+ site, C+3.50+ is bonded in a distorted bent 150 degrees geometry to one N3- and one O2- atom. The C–N bond length is 1.30 Å. The C–O bond length is 1.23 Å. In the second C+3.50+ site, C+3.50+ is bonded in a trigonal planar geometry to two N3- and one O2- atom. Both C–N bond lengths are 1.38 Å. The C–O bond length is 1.25 Å. In the third C+3.50+ site, C+3.50+ is bonded in a bent 120 degrees geometry to one N3- and one O2- atom. The C–N bond length is 1.31 Å. The C–O bond length is 1.24 Å. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded in a 2-coordinate geometry to one K1+ and two C+3.50+ atoms. In the second N3- site, N3- is bonded in a bent 120 degrees geometry to two C+3.50+ atoms. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one K1+ and one C+3.50+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one K1+ and one C+3.50+ atom. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one K1+ and one C+3.50+ atom.
DOI: 10.17188/1711048
title: Materials Data on MnNF3 by Materials Project

description: (MnF3)2N2 is (Cubic) Perovskite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional and consists of four ammonia molecules and one MnF3 framework. In the MnF3 framework, Mn2+ is bonded to six F1- atoms to form corner-sharing MnF6 octahedra. The corner-sharing octahedra tilt angles range from 3–4°. There are a spread of Mn–F bond distances ranging from 1.92–2.06 Å. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a linear geometry to two equivalent Mn2+ atoms. In the second F1- site, F1- is bonded in a linear geometry to two equivalent Mn2+ atoms.
DOI: 10.17188/1711049
title: Materials Data on Sr2La2MnZnO8 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: 10.17188/1711050
title: Materials Data on RbHfCu3Se4 by Materials Project

description: RbHfCu3Se4 crystallizes in the cubic P-43m space group. The structure is three-dimensional. Rb1+ is bonded to four equivalent Se2- atoms to form RbSe4 tetrahedra that share corners with four equivalent HfSe4 tetrahedra and corners with twelve equivalent CuSe4 tetrahedra. All Rb–Se bond lengths are 3.00 Å. Hf4+ is bonded to four equivalent Se2- atoms to form HfSe4 tetrahedra that share corners with four equivalent RbSe4 tetrahedra and edges with six equivalent CuSe4 tetrahedra. All Hf–Se bond lengths are 2.47 Å. Cu1+ is bonded to four equivalent Se2- atoms to form CuSe4 tetrahedra that share corners with four equivalent RbSe4 tetrahedra, corners with eight equivalent CuSe4 tetrahedra, and edges with two equivalent HfSe4 tetrahedra. All Cu–Se bond lengths are 2.66 Å. Se2- is bonded to one Rb1+, one Hf4+, and three equivalent Cu1+ atoms to form a mixture of distorted edge and corner-sharing SeRbHfCu3 trigonal bipyramids.
DOI: 10.17188/1711052
title: Materials Data on LaIr3 by Materials Project

description: Ir3La crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent La sites. In the first La site, La is bonded in a 12-coordinate geometry to twelve Ir atoms. There are a spread of La–Ir bond distances ranging from 3.15–3.41 Å. In the second La site, La is bonded in a 6-coordinate geometry to eighteen Ir atoms. There are six shorter (3.14 Å) and twelve longer (3.45 Å) La–Ir bond lengths. There are three inequivalent Ir sites. In the first Ir site, Ir is bonded to five La and seven Ir atoms to form a mixture of corner, edge, and face-sharing IrLa5Ir7 cuboctahedra. There are a spread of Ir–Ir bond distances ranging from 2.62–2.77 Å. In the second Ir site, Ir is bonded in a 12-coordinate geometry to three equivalent La and six equivalent Ir atoms. In the third Ir site, Ir is bonded to six equivalent La and six equivalent Ir atoms to form IrLa6Ir6 cuboctahedra that share corners with twelve equivalent IrLa5Ir7 cuboctahedra, edges with six equivalent IrLa6Ir6 cuboctahedra, and faces with eighteen equivalent IrLa5Ir7 cuboctahedra.
DOI: 10.17188/1711053
title: Materials Data on Si14H89C30O by Materials Project

description: (SiCH3)4(Si(CH3)3)8Si2C2H5O crystallizes in the triclinic P1 space group. The structure is zero-dimensional and consists of one hydroxy(2-$l^{1}-silanylethyl)silicon molecule; four silane, methyl- molecules; and eight trimethylsilyl radical molecules.
DOI: 10.17188/1711054
title: Materials Data on Tm2I2F by Materials Project

description: Tm2I2F is Cyanogen Chloride-like structured and crystallizes in the tetragonal P4/mmm space group. The structure is zero-dimensional and consists of one Tm2I2F cluster. Tm is bonded in a distorted linear geometry to one I and one F atom. The Tm–I bond length is 2.74 Å. The Tm–F bond length is 2.15 Å. I is bonded in a single-bond geometry to one Tm atom. F is bonded in a linear geometry to two equivalent Tm atoms.
DOI: 10.17188/1711055
title: Materials Data on La2MgZn by Materials Project

description: MgLa2Zn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two MgLa2Zn ribbons oriented in the (1, 0, 0) direction. Mg is bonded in a linear geometry to two equivalent La atoms. Both Mg–La bond lengths are 3.30 Å. La is bonded in a linear geometry to one Mg and one Zn atom. The La–Zn bond length is 2.92 Å. Zn is bonded in a linear geometry to two equivalent La atoms.
DOI: 10.17188/1711056
title: Materials Data on Ni(AuF4)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: 10.17188/1711058
title: Materials Data on HfNbRu2 by Materials Project

description: HfNbRu2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two HfNbRu2 ribbons oriented in the (1, 0, 0) direction. Hf is bonded in a linear geometry to two equivalent Ru atoms. Both Hf–Ru bond lengths are 2.32 Å. Nb is bonded in a linear geometry to two equivalent Ru atoms. Both Nb–Ru bond lengths are 2.21 Å. Ru is bonded in a linear geometry to one Hf and one Nb atom.
DOI: 10.17188/1711060
title: Materials Data on LiFeF3 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: 10.17188/1711061
title: Materials Data on La4Co by Materials Project

description: La4Co is Iron carbide-like structured and crystallizes in the cubic Fd-3m space group. The structure is zero-dimensional and consists of eight La4Co clusters. La is bonded in a single-bond geometry to one Co atom. The La–Co bond length is 2.56 Å. Co is bonded in a tetrahedral geometry to four equivalent La atoms.
DOI: 10.17188/1711062
title: Materials Data on Nd6Nb4Al43 by Materials Project

description: Nd6Nb4Al43 crystallizes in the hexagonal P6_3/mcm space group. The structure is three-dimensional. Nd is bonded in a 6-coordinate geometry to one Nd, one Nb, and fifteen Al atoms. The Nd–Nd bond length is 3.50 Å. The Nd–Nb bond length is 3.56 Å. There are a spread of Nd–Al bond distances ranging from 3.10–3.53 Å. There are two inequivalent Nb sites. In the first Nb site, Nb is bonded to twelve Al atoms to form NbAl12 cuboctahedra that share corners with six equivalent NbNd2Al10 cuboctahedra and edges with six equivalent AlNb2Al10 cuboctahedra. There are six shorter (2.73 Å) and six longer (2.90 Å) Nb–Al bond lengths. In the second Nb site, Nb is bonded to two equivalent Nd and ten Al atoms to form distorted NbNd2Al10 cuboctahedra that share corners with four NbAl12 cuboctahedra, an edgeedge with one AlNb2Al10 cuboctahedra, and faces with six AlNb2Al10 cuboctahedra. There are a spread of Nb–Al bond distances ranging from 2.65–2.76 Å. There are seven inequivalent Al sites. In the first Al site, Al is bonded in a 12-coordinate geometry to one Nd, two Nb, and nine Al atoms. There are a spread of Al–Al bond distances ranging from 2.79–3.07 Å. In the second Al site, Al is bonded in a 12-coordinate geometry to two equivalent Nd, one Nb, and nine Al atoms. There are a spread of Al–Al bond distances ranging from 2.79–3.05 Å. In the third Al site, Al is bonded in a 10-coordinate geometry to four equivalent Nd and eight Al atoms. There are a spread of Al–Al bond distances ranging from 2.83–3.16 Å. In the fourth Al site, Al is bonded in a 12-coordinate geometry to two equivalent Nd, one Nb, and nine Al atoms. There are a spread of Al–Al bond distances ranging from 2.77–3.05 Å. In the fifth Al site, Al is bonded in a 10-coordinate geometry to two equivalent Nd, one Nb, and seven Al atoms. There are two shorter (2.85 Å) and one longer (2.91 Å) Al–Al bond lengths. In the sixth Al site, Al is bonded to two equivalent Nb and ten Al atoms to form distorted AlNb2Al10 cuboctahedra that share corners with four equivalent AlNd3Al9 cuboctahedra, edges with three NbAl12 cuboctahedra, faces with two equivalent NbNd2Al10 cuboctahedra, and faces with two equivalent AlNb2Al10 cuboctahedra. Both Al–Al bond lengths are 2.84 Å. In the seventh Al site, Al is bonded to three equivalent Nd and nine Al atoms to form AlNd3Al9 cuboctahedra that share corners with six AlNb2Al10 cuboctahedra, faces with two equivalent AlNd3Al9 cuboctahedra, and faces with three equivalent NbNd2Al10 cuboctahedra.
DOI: 10.17188/1711063
title: Materials Data on Gd2B6Os by Materials Project

description: Gd2OsB6 crystallizes in the orthorhombic Pbam space group. The structure is three-dimensional. there are two inequivalent Gd3+ sites. In the first Gd3+ site, Gd3+ is bonded in a 6-coordinate geometry to fourteen B2- atoms. There are a spread of Gd–B bond distances ranging from 2.77–2.85 Å. In the second Gd3+ site, Gd3+ is bonded to twelve B2- atoms to form a mixture of edge and face-sharing GdB12 cuboctahedra. There are a spread of Gd–B bond distances ranging from 2.65–2.69 Å. Os6+ is bonded in a 10-coordinate geometry to ten B2- atoms. There are a spread of Os–B bond distances ranging from 2.39–2.46 Å. There are six inequivalent B2- sites. In the first B2- site, B2- is bonded in a 3-coordinate geometry to four equivalent Gd3+, two equivalent Os6+, and three B2- atoms. There are a spread of B–B bond distances ranging from 1.77–1.85 Å. In the second B2- site, B2- is bonded in a 9-coordinate geometry to four Gd3+, two equivalent Os6+, and three B2- atoms. Both B–B bond lengths are 1.81 Å. In the third B2- site, B2- is bonded in a 9-coordinate geometry to four Gd3+, two equivalent Os6+, and three B2- atoms. There is one shorter (1.72 Å) and one longer (1.89 Å) B–B bond length. In the fourth B2- site, B2- is bonded in a 9-coordinate geometry to four Gd3+, two equivalent Os6+, and three B2- atoms. There is one shorter (1.79 Å) and one longer (1.81 Å) B–B bond length. In the fifth B2- site, B2- is bonded in a 9-coordinate geometry to four Gd3+, two equivalent Os6+, and three B2- atoms. In the sixth B2- site, B2- is bonded in a 9-coordinate geometry to six Gd3+ and three B2- atoms. The B–B bond length is 2.18 Å.
DOI: 10.17188/1711064
title: Materials Data on CaCr3F6 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: 10.17188/1711067
title: Materials Data on NaIn2Sn by Materials Project

description: NaIn2Sn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two NaIn2Sn ribbons oriented in the (1, 0, 0) direction. Na is bonded in a linear geometry to two equivalent In atoms. Both Na–In bond lengths are 3.10 Å. In is bonded in a linear geometry to one Na and one Sn atom. The In–Sn bond length is 2.74 Å. Sn is bonded in a linear geometry to two equivalent In atoms.
DOI: 10.17188/1711068
title: Materials Data on Rb2CoH12(SO7)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: 10.17188/1711070
title: Materials Data on KCoO3 by Materials Project

description: KCoO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. K is bonded to twelve equivalent O atoms to form KO12 cuboctahedra that share corners with twelve equivalent KO12 cuboctahedra, faces with six equivalent KO12 cuboctahedra, and faces with eight equivalent CoO6 octahedra. All K–O bond lengths are 2.74 Å. Co is bonded to six equivalent O atoms to form CoO6 octahedra that share corners with six equivalent CoO6 octahedra and faces with eight equivalent KO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Co–O bond lengths are 1.94 Å. O is bonded to four equivalent K and two equivalent Co atoms to form a mixture of distorted face, edge, and corner-sharing OK4Co2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°.