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Materials Data on Co6O5F7 by Materials Project

Co6O5F7 is zeta iron carbide-derived structured and crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are four inequivalent Co+2.83+ sites. In the first Co+2.83+ site, Co+2.83+ is bonded to two O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoO4F2 octahedra and edges with two CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 48–51°. There is one shorter (1.89 Å) and one longer (1.91 Å) Co–O bond length. All Co–F bond lengths are 2.02 Å. In the second Co+2.83+ site, Co+2.83+ is bonded to one O2- and five F1- atoms to form CoOF5 octahedra that share corners with eight equivalent CoO3F3 octahedra and edges with two equivalent CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 47–54°. The Co–O bond length is 1.86 Å. There are one shorter (2.01 Å) and four longer (2.05 Å) Co–F bond lengths. In the third Co+2.83+ site, Co+2.83+ is bonded to four O2- and two equivalent F1- atoms to form CoO4F2 octahedra that share corners with eight equivalent CoO2F4 octahedra and edges with two equivalent CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 48–50°. All Co–O bond lengths are 1.91 Å. Both Co–F bond lengths are 2.16 Å. In the fourth Co+2.83+ site, Co+2.83+ is bonded to three O2- and three F1- atoms to form CoO3F3 octahedra that share corners with eight CoO2F4 octahedra and edges with two CoO4F2 octahedra. The corner-sharing octahedra tilt angles range from 47–54°. There are a spread of Co–O bond distances ranging from 1.89–1.92 Å. There are one shorter (2.00 Å) and two longer (2.13 Å) Co–F bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the second O2- site, O2- is bonded in a trigonal planar geometry to three Co+2.83+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms. In the second F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Co6O5F7 by Materials Project

Co6O5F7 is zeta iron carbide-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Co+2.83+ sites. In the first Co+2.83+ site, Co+2.83+ is bonded to three O2- and three F1- atoms to form CoO3F3 octahedra that share corners with eight CoO2F4 octahedra and edges with two CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 46–53°. There is one shorter (1.88 Å) and two longer (1.90 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 1.97–2.11 Å. In the second Co+2.83+ site, Co+2.83+ is bonded to three O2- and three F1- atoms to form CoO3F3 octahedra that share corners with eight CoO2F4 octahedra and edges with two CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 45–51°. There are a spread of Co–O bond distances ranging from 1.88–1.93 Å. There are a spread of Co–F bond distances ranging from 1.98–2.13 Å. In the third Co+2.83+ site, Co+2.83+ is bonded to three O2- and three F1- atoms to form CoO3F3 octahedra that share corners with eight CoO2F4 octahedra and edges with two CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 47–61°. There are a spread of Co–O bond distances ranging from 1.96–1.99 Å. There are a spread of Co–F bond distances ranging from 2.15–2.28 Å. In the fourth Co+2.83+ site, Co+2.83+ is bonded to two O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoO3F3 octahedra and edges with two CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 45–61°. There is one shorter (1.80 Å) and one longer (1.93 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 2.03–2.10 Å. In the fifth Co+2.83+ site, Co+2.83+ is bonded to two O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoO3F3 octahedra and edges with two CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 46–59°. There is one shorter (1.86 Å) and one longer (1.93 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 2.03–2.06 Å. In the sixth Co+2.83+ site, Co+2.83+ is bonded to two O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoO3F3 octahedra and edges with two CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 46–53°. There is one shorter (1.84 Å) and one longer (1.86 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 2.01–2.09 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. There are seven inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms. In the fifth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the sixth F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms. In the seventh F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Co6O5F7 by Materials Project

Co6O5F7 is zeta iron carbide-derived structured and crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are four inequivalent Co+2.83+ sites. In the first Co+2.83+ site, Co+2.83+ is bonded to four O2- and two equivalent F1- atoms to form CoO4F2 octahedra that share corners with eight CoOF5 octahedra and edges with two equivalent CoO3F3 octahedra. The corner-sharing octahedra tilt angles range from 48–50°. All Co–O bond lengths are 1.88 Å. Both Co–F bond lengths are 2.21 Å. In the second Co+2.83+ site, Co+2.83+ is bonded to one O2- and five F1- atoms to form CoOF5 octahedra that share corners with eight CoO4F2 octahedra and edges with two equivalent CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 48–55°. The Co–O bond length is 1.78 Å. There are two shorter (2.00 Å) and three longer (2.02 Å) Co–F bond lengths. In the third Co+2.83+ site, Co+2.83+ is bonded to two O2- and four F1- atoms to form CoO2F4 octahedra that share corners with eight CoO4F2 octahedra and edges with two CoOF5 octahedra. The corner-sharing octahedra tilt angles range from 43–52°. There is one shorter (1.91 Å) and one longer (1.92 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 2.02–2.06 Å. In the fourth Co+2.83+ site, Co+2.83+ is bonded to three O2- and three F1- atoms to form CoO3F3 octahedra that share corners with eight CoOF5 octahedra and edges with two CoO4F2 octahedra. The corner-sharing octahedra tilt angles range from 43–55°. There is two shorter (1.90 Å) and one longer (1.96 Å) Co–O bond length. There are a spread of Co–F bond distances ranging from 2.07–2.17 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.83+ atoms. In the second F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to three Co+2.83+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Co6O5F7 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 Co6O5F7 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 Co6O5F7 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 Co6O5F7 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 Co6O5F7 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 Co6O5F7 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 Co6O5F7 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 Co6O5F7 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 Co6O5F7 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 Co6O5F7 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↗