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Materials Data on LiV3O5F3 by Materials Project

LiV3O5F3 is zeta iron carbide-derived structured and crystallizes in the monoclinic Cc space group. The structure is three-dimensional. Li1+ is bonded to three O2- and three F1- atoms to form distorted LiO3F3 octahedra that share corners with eight VO4F2 octahedra and edges with two equivalent VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 46–62°. There are one shorter (2.10 Å) and two longer (2.21 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 2.00–2.15 Å. There are three inequivalent V4+ sites. In the first V4+ site, V4+ is bonded to four O2- and two F1- atoms to form VO4F2 octahedra that share corners with four equivalent LiO3F3 octahedra, corners with four equivalent VO4F2 octahedra, and edges with two equivalent VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 46–60°. There are a spread of V–O bond distances ranging from 1.77–2.00 Å. There are one shorter (2.05 Å) and one longer (2.06 Å) V–F bond lengths. In the second V4+ site, V4+ is bonded to four O2- and two F1- atoms to form VO4F2 octahedra that share corners with eight VO4F2 octahedra and edges with two equivalent LiO3F3 octahedra. The corner-sharing octahedra tilt angles range from 29–56°. There are a spread of V–O bond distances ranging from 1.74–2.00 Å. There are one shorter (2.03 Å) and one longer (2.14 Å) V–F bond lengths. In the third V4+ site, V4+ is bonded to four O2- and two equivalent F1- atoms to form distorted VO4F2 octahedra that share corners with four equivalent LiO3F3 octahedra, corners with four equivalent VO4F2 octahedra, and edges with two equivalent VO4F2 octahedra. The corner-sharing octahedra tilt angles range from 29–62°. There are a spread of V–O bond distances ranging from 1.75–2.07 Å. There are one shorter (2.01 Å) and one longer (2.09 Å) V–F bond lengths. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent V4+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to three V4+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+ and two V4+ atoms. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+ and two V4+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to three V4+ atoms. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two V4+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two V4+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent V4+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiV3O5F3 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 LiV3O5F3 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 LiV3O5F3 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↗