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Materials Data on Li3VOF5 by Materials Project

Li3VOF5 crystallizes in the monoclinic Pc space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to one O2- and five F1- atoms to form LiOF5 octahedra that share corners with six equivalent VOF5 octahedra. The corner-sharing octahedra tilt angles range from 39–51°. The Li–O bond length is 2.10 Å. There are a spread of Li–F bond distances ranging from 2.00–2.23 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to one O2- and three F1- atoms. The Li–O bond length is 2.12 Å. There are a spread of Li–F bond distances ranging from 1.93–2.13 Å. In the third Li1+ site, Li1+ is bonded in a 7-coordinate geometry to two equivalent O2- and five F1- atoms. There are one shorter (2.61 Å) and one longer (2.65 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.97–2.45 Å. V4+ is bonded to one O2- and five F1- atoms to form VOF5 octahedra that share corners with six equivalent LiOF5 octahedra. The corner-sharing octahedra tilt angles range from 39–51°. The V–O bond length is 1.67 Å. There are a spread of V–F bond distances ranging from 1.96–2.04 Å. O2- is bonded in a 3-coordinate geometry to four Li1+ and one V4+ atom. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded to three Li1+ and one V4+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the second F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V4+ atom. In the third F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V4+ atom. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V4+ atom. In the fifth F1- site, F1- is bonded to three Li1+ and one V4+ atom to form distorted corner-sharing FLi3V tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li3VOF5 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↗