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Materials Data on Co3(OF2)2 by Materials Project

Co3(OF2)2 is zeta iron carbide-derived structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are four inequivalent Co+2.67+ sites. In the first Co+2.67+ site, Co+2.67+ is bonded to two O2- and four F1- atoms to form a mixture of edge and corner-sharing CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 47–58°. There is one shorter (1.82 Å) and one longer (1.87 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 2.02–2.14 Å. In the second Co+2.67+ site, Co+2.67+ is bonded to two O2- and four F1- atoms to form a mixture of edge and corner-sharing CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 45–57°. There is one shorter (1.91 Å) and one longer (1.97 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 2.04–2.09 Å. In the third Co+2.67+ site, Co+2.67+ is bonded to two equivalent O2- and four F1- atoms to form a mixture of edge and corner-sharing CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 45–51°. Both Co–O bond lengths are 1.90 Å. There are two shorter (1.95 Å) and two longer (2.05 Å) Co–F bond lengths. In the fourth Co+2.67+ site, Co+2.67+ is bonded to two equivalent O2- and four F1- atoms to form a mixture of edge and corner-sharing CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 48–58°. Both Co–O bond lengths are 1.93 Å. There are two shorter (2.00 Å) and two longer (2.01 Å) Co–F bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three Co+2.67+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.67+ atoms. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.67+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.67+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.67+ atoms. In the fourth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.67+ atoms.

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Materials Data on Co3(TeO4)2 by Materials Project

(Co6Te4O15)2O2 crystallizes in the orthorhombic Cmc2_1 space group. The structure is three-dimensional and consists of two O2 ribbons oriented in the (0, 0, 1) direction and one Co6Te4O15 framework. In each O2 ribbon, O2- is bonded in a linear geometry to two equivalent O2- atoms. Both O–O bond lengths are 2.50 Å. In the Co6Te4O15 framework, there are three inequivalent Co+2.67+ sites. In the first Co+2.67+ site, Co+2.67+ is bonded to six O2- atoms to form a mixture of edge, face, and corner-sharing CoO6 octahedra. The corner-sharing octahedra tilt angles range from 28–57°. There are a spread of Co–O bond distances ranging from 1.95–2.19 Å. In the second Co+2.67+ site, Co+2.67+ is bonded to six O2- atoms to form a mixture of edge, face, and corner-sharing CoO6 octahedra. The corner-sharing octahedra tilt angles range from 28–57°. There are a spread of Co–O bond distances ranging from 1.95–2.19 Å. In the third Co+2.67+ site, Co+2.67+ is bonded to six O2- atoms to form a mixture of edge, face, and corner-sharing CoO6 octahedra. The corner-sharing octahedra tilt angles range from 28–57°. There are a spread of Co–O bond distances ranging from 1.95–2.19 Å. There are three inequivalent Te4+ sites. In the first Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. There is one shorter (1.92 Å) and two longer (1.93 Å) Te–O bond length. In the second Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. There is one shorter (1.92 Å) and two longer (1.93 Å) Te–O bond length. In the third Te4+ site, Te4+ is bonded in a 3-coordinate geometry to three O2- atoms. All Te–O bond lengths are 1.91 Å. There are nine inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted square co-planar geometry to four equivalent Co+2.67+ atoms. In the second O2- site, O2- is bonded in a distorted square co-planar geometry to four Co+2.67+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to two equivalent Co+2.67+ and one Te4+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to two Co+2.67+ and one Te4+ atom. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to two Co+2.67+ and one Te4+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Co+2.67+ and one Te4+ atom. In the seventh O2- site, O2- is bonded in a 3-coordinate geometry to two Co+2.67+ and one Te4+ atom. In the eighth O2- site, O2- is bonded in a trigonal non-coplanar geometry to two equivalent Co+2.67+ and one Te4+ atom. In the ninth O2- site, O2- is bonded in a trigonal non-coplanar geometry to two Co+2.67+ and one Te4+ atom.

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Materials Data on Co3(SO6)2 by Materials Project

Co3(SO6)2 crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. there are two inequivalent Co4+ sites. In the first Co4+ site, Co4+ is bonded to six O2- atoms to form distorted CoO6 octahedra that share corners with two equivalent CoO6 octahedra, corners with three SO4 tetrahedra, and edges with two equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 50–56°. There are a spread of Co–O bond distances ranging from 1.62–2.24 Å. In the second Co4+ site, Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with four equivalent CoO6 octahedra and corners with four SO4 tetrahedra. The corner-sharing octahedra tilt angles range from 50–56°. There are a spread of Co–O bond distances ranging from 1.84–2.11 Å. There are two inequivalent S6+ sites. In the first S6+ site, S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with six CoO6 octahedra. The corner-sharing octahedra tilt angles range from 45–55°. There is two shorter (1.47 Å) and two longer (1.51 Å) S–O bond length. In the second S6+ site, S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with four CoO6 octahedra. The corner-sharing octahedra tilt angles range from 33–57°. There are a spread of S–O bond distances ranging from 1.45–1.51 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three Co4+ atoms. In the second O2- site, O2- is bonded in a bent 120 degrees geometry to one Co4+ and one S6+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Co4+ and one S6+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to one Co4+ and one S6+ atom. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Co4+ and one S6+ atom. In the seventh O2- site, O2- is bonded in a single-bond geometry to one Co4+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Co4+ and one S6+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Co3(PO4)2 by Materials Project

Co3(PO4)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Co2+ sites. In the first Co2+ site, Co2+ is bonded to five O2- atoms to form distorted CoO5 trigonal bipyramids that share a cornercorner with one CoO6 octahedra, corners with three equivalent PO4 tetrahedra, an edgeedge with one CoO6 octahedra, an edgeedge with one PO4 tetrahedra, and an edgeedge with one CoO5 trigonal bipyramid. The corner-sharing octahedral tilt angles are 59°. There are a spread of Co–O bond distances ranging from 2.00–2.26 Å. In the second Co2+ site, Co2+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with six equivalent PO4 tetrahedra, corners with two equivalent CoO5 trigonal bipyramids, and edges with two equivalent CoO5 trigonal bipyramids. There are a spread of Co–O bond distances ranging from 2.05–2.23 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with three equivalent CoO6 octahedra, corners with three equivalent CoO5 trigonal bipyramids, and an edgeedge with one CoO5 trigonal bipyramid. The corner-sharing octahedra tilt angles range from 35–53°. There are a spread of P–O bond distances ranging from 1.55–1.57 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to two Co2+ and one P5+ atom. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to two equivalent Co2+ and one P5+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to two Co2+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted T-shaped geometry to two Co2+ and one P5+ atom.

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Materials Data on Sr6Co4Bi2O15 by Materials Project

Sr6Co4Bi2O15 crystallizes in the orthorhombic C222 space group. The structure is three-dimensional. there are six inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.60–2.99 Å. In the second Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.57–2.96 Å. In the third Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.59–3.00 Å. In the fourth Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.61–2.98 Å. In the fifth Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.58–2.90 Å. In the sixth Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.62–2.81 Å. There are four inequivalent Co3+ sites. In the first Co3+ site, Co3+ is bonded to five O2- atoms to form CoO5 trigonal bipyramids that share corners with two equivalent CoO6 octahedra, a cornercorner with one CoO5 trigonal bipyramid, and edges with two equivalent CoO5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 7–10°. There are a spread of Co–O bond distances ranging from 1.87–1.99 Å. In the second Co3+ site, Co3+ is bonded to six O2- atoms to form distorted CoO6 octahedra that share corners with two equivalent CoO6 octahedra and corners with two equivalent CoO5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 2–10°. There are a spread of Co–O bond distances ranging from 1.92–2.53 Å. In the third Co3+ site, Co3+ is bonded to five O2- atoms to form CoO5 trigonal bipyramids that share corners with two equivalent CoO6 octahedra, a cornercorner with one CoO5 trigonal bipyramid, and edges with two equivalent CoO5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 11–12°. There are a spread of Co–O bond distances ranging from 1.79–2.08 Å. In the fourth Co3+ site, Co3+ is bonded to six O2- atoms to form distorted CoO6 octahedra that share corners with two equivalent CoO6 octahedra and corners with two equivalent CoO5 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 2–9°. There are a spread of Co–O bond distances ranging from 1.93–2.54 Å. There are two inequivalent Bi3+ sites. In the first Bi3+ site, Bi3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Bi–O bond distances ranging from 2.13–3.08 Å. In the second Bi3+ site, Bi3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Bi–O bond distances ranging from 2.14–3.10 Å. There are eighteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+, one Co3+, and one Bi3+ atom. In the second O2- site, O2- is bonded in a square co-planar geometry to four Sr2+ atoms. In the third O2- site, O2- is bonded to four Sr2+ and two equivalent Co3+ atoms to form a mixture of distorted corner and face-sharing OSr4Co2 octahedra. The corner-sharing octahedral tilt angles are 60°. In the fourth O2- site, O2- is bonded in a 5-coordinate geometry to two Sr2+ and three equivalent Bi3+ atoms. In the fifth O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+, one Co3+, and one Bi3+ atom. In the sixth O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+ and two Co3+ atoms. In the seventh O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+ and two Co3+ atoms. In the eighth O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+ and two Co3+ atoms. In the ninth O2- site, O2- is bonded to four Sr2+ and two equivalent Co3+ atoms to form a mixture of distorted corner and face-sharing OSr4Co2 octahedra. The corner-sharing octahedral tilt angles are 59°. In the tenth O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+ and two Co3+ atoms. In the eleventh O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+, one Co3+, and one Bi3+ atom. In the twelfth O2- site, O2- is bonded in a 6-coordinate geometry to four Sr2+, one Co3+, and one Bi3+ atom. In the thirteenth O2- site, O2- is bonded to four Sr2+ and two Co3+ atoms to form distorted corner-sharing OSr4Co2 octahedra. The corner-sharing octahedra tilt angles range from 2–60°. In the fourteenth O2- site, O2- is bonded to four Sr2+ and two equivalent Co3+ atoms to form a mixture of distorted corner and face-sharing OSr4Co2 octahedra. The corner-sharing octahedral tilt angles are 60°. In the fifteenth O2- site, O2- is bonded to four Sr2+ and two equivalent Co3+ atoms to form a mixture of distorted corner and face-sharing OSr4Co2 octahedra. The corner-sharing octahedral tilt angles are 59°. In the sixteenth O2- site, O2- is bonded in a 2-coordinate geometry to four Sr2+ and two Co3+ atoms. In the seventeenth O2- site, O2- is bonded in a 5-coordinate geometry to two Sr2+ and three equivalent Bi3+ atoms. In the eighteenth O2- site, O2- is bonded in a rectangular see-saw-like geometry to four Co3+ atoms.

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Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2Co(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2Co(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2Co(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on Li2Co(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗

Materials Data on LiCo(CO3)2 by Materials Project

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

36 MATERIALS SCIENCE↗