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Materials Data on LiV2F7 by Materials Project

LiV2F7 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. Li1+ is bonded in a 5-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.97–2.10 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to seven F1- atoms to form a mixture of distorted edge and corner-sharing VF7 hexagonal pyramids. There are a spread of V–F bond distances ranging from 2.01–2.11 Å. In the second V3+ site, V3+ is bonded to seven F1- atoms to form a mixture of distorted edge and corner-sharing VF7 hexagonal pyramids. There are a spread of V–F bond distances ranging from 2.03–2.07 Å. There are seven inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two V3+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two V3+ atoms. In the third F1- site, F1- is bonded in a linear geometry to two V3+ atoms. In the fourth F1- site, F1- is bonded in a water-like geometry to two V3+ atoms. In the fifth F1- site, F1- is bonded in a trigonal non-coplanar geometry to one Li1+ and two V3+ atoms. In the sixth F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two V3+ atoms. In the seventh F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two V3+ atoms.

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Materials Data on LiVF3 by Materials Project

LiVF3 is Ilmenite-like structured and crystallizes in the cubic P2_13 space group. The structure is three-dimensional. Li1+ is bonded in a 6-coordinate geometry to six equivalent F1- atoms. There are three shorter (1.97 Å) and three longer (2.28 Å) Li–F bond lengths. V2+ is bonded to six equivalent F1- atoms to form distorted corner-sharing VF6 octahedra. The corner-sharing octahedral tilt angles are 52°. There are three shorter (2.13 Å) and three longer (2.14 Å) V–F bond lengths. F1- is bonded to two equivalent Li1+ and two equivalent V2+ atoms to form a mixture of distorted edge and corner-sharing FLi2V2 trigonal pyramids.

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Materials Data on LiV2F5 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

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Materials Data on Li2VF4 by Materials Project

Li2VF4 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with six VF6 octahedra, corners with two equivalent LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 52–72°. There are a spread of Li–F bond distances ranging from 1.86–2.01 Å. In the second Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with six VF6 octahedra, corners with two equivalent LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 53–71°. There are a spread of Li–F bond distances ranging from 1.86–2.01 Å. In the third Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with six VF6 octahedra, corners with two equivalent LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 52–70°. There are a spread of Li–F bond distances ranging from 1.86–2.01 Å. In the fourth Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with six VF6 octahedra, corners with two equivalent LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 53–74°. There are a spread of Li–F bond distances ranging from 1.86–2.01 Å. There are two inequivalent V2+ sites. In the first V2+ site, V2+ is bonded to six F1- atoms to form VF6 octahedra that share corners with twelve LiF4 tetrahedra and edges with two equivalent VF6 octahedra. There are a spread of V–F bond distances ranging from 2.09–2.17 Å. In the second V2+ site, V2+ is bonded to six F1- atoms to form VF6 octahedra that share corners with twelve LiF4 tetrahedra and edges with two equivalent VF6 octahedra. There are a spread of V–F bond distances ranging from 2.09–2.17 Å. There are eight inequivalent F1- sites. In the first F1- site, F1- is bonded to two equivalent Li1+ and two equivalent V2+ atoms to form a mixture of distorted corner and edge-sharing FLi2V2 tetrahedra. In the second F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one V2+ atom. In the third F1- site, F1- is bonded to two equivalent Li1+ and two equivalent V2+ atoms to form a mixture of distorted corner and edge-sharing FLi2V2 tetrahedra. In the fourth F1- site, F1- is bonded to two equivalent Li1+ and two equivalent V2+ atoms to form a mixture of distorted corner and edge-sharing FLi2V2 tetrahedra. In the fifth F1- site, F1- is bonded to two equivalent Li1+ and two equivalent V2+ atoms to form a mixture of distorted corner and edge-sharing FLi2V2 tetrahedra. In the sixth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one V2+ atom. In the seventh F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one V2+ atom. In the eighth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one V2+ atom.

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Materials Data on LiV2F7 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

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Materials Data on LiV3F10 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

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Materials Data on Li2VF6 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

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Materials Data on LiV2F7 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

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Materials Data on Li11V4F24 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

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