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Materials Data on V6O11F by Materials Project

V6O11F is zeta iron carbide-derived structured and crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are four inequivalent V+3.83+ sites. In the first V+3.83+ site, V+3.83+ is bonded to five O2- and one F1- atom to form VO5F octahedra that share corners with eight VO6 octahedra and edges with two VO5F octahedra. The corner-sharing octahedra tilt angles range from 41–55°. There are a spread of V–O bond distances ranging from 1.77–2.00 Å. The V–F bond length is 2.15 Å. In the second V+3.83+ site, V+3.83+ is bonded to six O2- atoms to form VO6 octahedra that share corners with eight equivalent VO6 octahedra and edges with two equivalent VO5F octahedra. The corner-sharing octahedra tilt angles range from 51–52°. There are a spread of V–O bond distances ranging from 1.97–2.10 Å. In the third V+3.83+ site, V+3.83+ is bonded to six O2- atoms to form VO6 octahedra that share corners with eight VO5F octahedra and edges with two VO6 octahedra. The corner-sharing octahedra tilt angles range from 41–55°. There are a spread of V–O bond distances ranging from 1.84–2.14 Å. In the fourth V+3.83+ site, V+3.83+ is bonded to five O2- and one F1- atom to form VO5F octahedra that share corners with eight equivalent VO5F octahedra and edges with two equivalent VO6 octahedra. The corner-sharing octahedra tilt angles range from 45–54°. There is one shorter (1.81 Å) and four longer (1.95 Å) V–O bond length. The V–F bond length is 2.25 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to three V+3.83+ atoms. In the second O2- site, O2- is bonded in a trigonal planar geometry to three V+3.83+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to three V+3.83+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three V+3.83+ atoms. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to three V+3.83+ atoms. F1- is bonded in a 3-coordinate geometry to three V+3.83+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on V6O11F 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 V6O11F 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 V6O11F 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 V6O11F 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↗