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Materials Data on V4O3F5 by Materials Project

V4O3F5 is zeta iron carbide-derived structured and crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. there are three inequivalent V+2.75+ sites. In the first V+2.75+ site, V+2.75+ is bonded to three O2- and three F1- atoms to form VO3F3 octahedra that share corners with eight VOF5 octahedra and edges with two equivalent VO3F3 octahedra. The corner-sharing octahedra tilt angles range from 46–55°. There are a spread of V–O bond distances ranging from 1.98–2.04 Å. There are two shorter (2.15 Å) and one longer (2.21 Å) V–F bond lengths. In the second V+2.75+ site, V+2.75+ is bonded to one O2- and five F1- atoms to form VOF5 octahedra that share corners with eight equivalent VO3F3 octahedra and edges with two equivalent VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 49–55°. The V–O bond length is 1.88 Å. There are four shorter (2.05 Å) and one longer (2.11 Å) V–F bond lengths. In the third V+2.75+ site, V+2.75+ is bonded to two O2- and four equivalent F1- atoms to form VO2F4 octahedra that share corners with eight equivalent VO3F3 octahedra and edges with two equivalent VOF5 octahedra. The corner-sharing octahedra tilt angles range from 46–47°. There is one shorter (1.90 Å) and one longer (1.91 Å) V–O bond length. All V–F bond lengths are 2.09 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three V+2.75+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to three V+2.75+ atoms. In the third O2- site, O2- is bonded in a distorted T-shaped geometry to three V+2.75+ atoms. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three V+2.75+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three V+2.75+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on V4O3F5 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↗