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Materials Data on LiVF4 by Materials Project

LiVF4 crystallizes in the orthorhombic Pmmn space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a square co-planar geometry to four F1- atoms. There are two shorter (1.91 Å) and two longer (2.15 Å) Li–F bond lengths. In the second Li1+ site, Li1+ is bonded in a linear geometry to two equivalent F1- atoms. Both Li–F bond lengths are 1.86 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 2–4°. There are a spread of V–F bond distances ranging from 1.91–2.01 Å. In the second V3+ site, V3+ is bonded to six F1- atoms to form corner-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 3–4°. There are a spread of V–F bond distances ranging from 1.96–1.99 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a linear geometry to two equivalent V3+ atoms. In the second F1- site, F1- is bonded in a linear geometry to two V3+ atoms. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one V3+ atom. In the fourth F1- site, F1- is bonded in a linear geometry to two equivalent V3+ atoms. In the fifth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on LiVF4 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↗