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Materials Data on Co3OF5 by Materials Project

Co3OF5 is Hydrophilite-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are four inequivalent Co+2.33+ sites. In the first Co+2.33+ site, Co+2.33+ is bonded to one O2- and five F1- atoms to form a mixture of corner and edge-sharing CoOF5 octahedra. The corner-sharing octahedra tilt angles range from 47–53°. The Co–O bond length is 1.77 Å. There are four shorter (2.07 Å) and one longer (2.10 Å) Co–F bond lengths. In the second Co+2.33+ site, Co+2.33+ is bonded to one O2- and five F1- atoms to form a mixture of corner and edge-sharing CoOF5 octahedra. The corner-sharing octahedra tilt angles range from 47–53°. The Co–O bond length is 2.01 Å. There are a spread of Co–F bond distances ranging from 2.06–2.15 Å. In the third Co+2.33+ site, Co+2.33+ is bonded to six F1- atoms to form a mixture of corner and edge-sharing CoF6 octahedra. The corner-sharing octahedra tilt angles range from 48–51°. There are two shorter (1.99 Å) and four longer (2.08 Å) Co–F bond lengths. In the fourth Co+2.33+ site, Co+2.33+ is bonded to two equivalent O2- and four F1- atoms to form a mixture of corner and edge-sharing CoO2F4 octahedra. The corner-sharing octahedra tilt angles range from 49–51°. Both Co–O bond lengths are 2.04 Å. There are two shorter (2.05 Å) and two longer (2.11 Å) Co–F bond lengths. O2- is bonded in a distorted trigonal planar geometry to three Co+2.33+ atoms. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.33+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.33+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.33+ atoms. In the fourth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Co+2.33+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Co3OF5 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↗