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Materials Data on V4O7F5 by Materials Project

V4O7F5 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent V+4.75+ sites. In the first V+4.75+ site, V+4.75+ is bonded to three O2- and three F1- atoms to form distorted corner-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 17–31°. There are a spread of V–O bond distances ranging from 1.67–2.11 Å. There are a spread of V–F bond distances ranging from 1.92–2.05 Å. In the second V+4.75+ site, V+4.75+ is bonded to four O2- and two F1- atoms to form distorted corner-sharing VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 17–39°. There are a spread of V–O bond distances ranging from 1.67–2.19 Å. There is one shorter (1.95 Å) and one longer (1.96 Å) V–F bond length. In the third V+4.75+ site, V+4.75+ is bonded to three O2- and three F1- atoms to form corner-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 19–31°. There are a spread of V–O bond distances ranging from 1.68–2.09 Å. There are a spread of V–F bond distances ranging from 1.97–2.01 Å. In the fourth V+4.75+ site, V+4.75+ is bonded to four O2- and two F1- atoms to form distorted corner-sharing VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 19–39°. There are a spread of V–O bond distances ranging from 1.67–2.20 Å. Both V–F bond lengths are 1.95 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the second O2- site, O2- is bonded in a 1-coordinate geometry to two V+4.75+ atoms. In the third O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to two V+4.75+ atoms. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the sixth O2- site, O2- is bonded in a 2-coordinate geometry to two V+4.75+ atoms. In the seventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms. In the second F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms. In the fourth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the fifth F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on V4O7F5 by Materials Project

V4O7F5 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent V+4.75+ sites. In the first V+4.75+ site, V+4.75+ is bonded to three O2- and three F1- atoms to form distorted corner-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 23–32°. There are a spread of V–O bond distances ranging from 1.65–2.24 Å. There are a spread of V–F bond distances ranging from 1.93–2.01 Å. In the second V+4.75+ site, V+4.75+ is bonded in a 6-coordinate geometry to four O2- and two F1- atoms. There are a spread of V–O bond distances ranging from 1.65–2.26 Å. There is one shorter (1.95 Å) and one longer (1.97 Å) V–F bond length. In the third V+4.75+ site, V+4.75+ is bonded to three O2- and three F1- atoms to form distorted corner-sharing VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 20–32°. There are a spread of V–O bond distances ranging from 1.66–2.24 Å. There is two shorter (1.97 Å) and one longer (2.01 Å) V–F bond length. In the fourth V+4.75+ site, V+4.75+ is bonded to four O2- and two F1- atoms to form distorted corner-sharing VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 20–28°. There are a spread of V–O bond distances ranging from 1.66–2.21 Å. There is one shorter (1.96 Å) and one longer (1.97 Å) V–F bond length. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two V+4.75+ atoms. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to two V+4.75+ atoms. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to two V+4.75+ atoms. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms. In the second F1- site, F1- is bonded in a distorted bent 150 degrees geometry to two V+4.75+ atoms. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms. In the fourth F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms. In the fifth F1- site, F1- is bonded in a bent 150 degrees geometry to two V+4.75+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on V4O7F5 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 V4O7F5 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 V4O7F5 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 V4O7F5 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 V4O7F5 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↗