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Materials Data on Li3Co3OF7 by Materials Project

Li3Co3OF7 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 2-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.68–2.40 Å. In the second Li1+ site, Li1+ is bonded in a 2-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.62–2.61 Å. In the third Li1+ site, Li1+ is bonded in a 2-coordinate geometry to three F1- atoms. There are a spread of Li–F bond distances ranging from 1.63–2.17 Å. In the fourth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to one O2- and three F1- atoms. The Li–O bond length is 1.63 Å. There are a spread of Li–F bond distances ranging from 2.02–2.30 Å. In the fifth Li1+ site, Li1+ is bonded in a 2-coordinate geometry to one O2- and four F1- atoms. The Li–O bond length is 2.26 Å. There are a spread of Li–F bond distances ranging from 1.65–2.61 Å. In the sixth Li1+ site, Li1+ is bonded in a 2-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.68–2.59 Å. There are six inequivalent Co2+ sites. In the first Co2+ site, Co2+ is bonded in a 2-coordinate geometry to one O2- and two F1- atoms. The Co–O bond length is 1.58 Å. There is one shorter (1.71 Å) and one longer (2.22 Å) Co–F bond length. In the second Co2+ site, Co2+ is bonded in a 2-coordinate geometry to two F1- atoms. There is one shorter (1.64 Å) and one longer (1.74 Å) Co–F bond length. In the third Co2+ site, Co2+ is bonded in a 2-coordinate geometry to two F1- atoms. There is one shorter (1.65 Å) and one longer (1.68 Å) Co–F bond length. In the fourth Co2+ site, Co2+ is bonded in a 2-coordinate geometry to two F1- atoms. There is one shorter (1.67 Å) and one longer (1.72 Å) Co–F bond length. In the fifth Co2+ site, Co2+ is bonded in a 2-coordinate geometry to one O2- and one F1- atom. The Co–O bond length is 1.55 Å. The Co–F bond length is 1.65 Å. In the sixth Co2+ site, Co2+ is bonded in a 2-coordinate geometry to three F1- atoms. There are a spread of Co–F bond distances ranging from 1.63–2.22 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one Li1+ and one Co2+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to one Li1+ and one Co2+ atom. There are fourteen inequivalent F1- sites. In the first F1- site, F1- is bonded in a 1-coordinate geometry to two Li1+ and one Co2+ atom. In the second F1- site, F1- is bonded in a 1-coordinate geometry to one Li1+ and one Co2+ atom. In the third F1- site, F1- is bonded in a 2-coordinate geometry to two Li1+ atoms. In the fourth F1- site, F1- is bonded in a 2-coordinate geometry to one Li1+ and one Co2+ atom. In the fifth F1- site, F1- is bonded in a 1-coordinate geometry to two Li1+ and two Co2+ atoms. In the sixth F1- site, F1- is bonded in a 2-coordinate geometry to three Li1+ atoms. In the seventh F1- site, F1- is bonded in a 1-coordinate geometry to two Li1+ atoms. In the eighth F1- site, F1- is bonded in a distorted water-like geometry to one Li1+ and one Co2+ atom. In the ninth F1- site, F1- is bonded in a 1-coordinate geometry to one Li1+ and two Co2+ atoms. In the tenth F1- site, F1- is bonded in a 2-coordinate geometry to one Li1+ and one Co2+ atom. In the eleventh F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to two Li1+ and one Co2+ atom. In the twelfth F1- site, F1- is bonded in a 1-coordinate geometry to two Li1+ and one Co2+ atom. In the thirteenth F1- site, F1- is bonded in a 1-coordinate geometry to two Li1+ atoms. In the fourteenth F1- site, F1- is bonded in a 2-coordinate geometry to two Li1+ and one Co2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3Co3OF7 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 Li3Co3OF7 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↗