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Materials Data on LiV2F6 by Materials Project

LiV2F6 is Hydrophilite-derived structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Li1+ is bonded to six F1- atoms to form LiF6 octahedra that share corners with eight equivalent VF6 octahedra and edges with two equivalent VF6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are two shorter (2.06 Å) and four longer (2.09 Å) Li–F bond lengths. V+2.50+ is bonded to six F1- atoms to form VF6 octahedra that share corners with four equivalent LiF6 octahedra, corners with four equivalent VF6 octahedra, an edgeedge with one LiF6 octahedra, and an edgeedge with one VF6 octahedra. The corner-sharing octahedra tilt angles range from 49–50°. There are two shorter (2.03 Å) and four longer (2.05 Å) V–F bond lengths. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent V+2.50+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent V+2.50+ atoms.

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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 Li2VF4 by Materials Project

Li2VF4 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.82–2.34 Å. In the second Li1+ site, Li1+ is bonded to four F1- atoms to form distorted LiF4 trigonal pyramids that share corners with five equivalent VF6 octahedra, corners with two equivalent LiF4 trigonal pyramids, and an edgeedge with one VF6 octahedra. The corner-sharing octahedra tilt angles range from 38–74°. There are a spread of Li–F bond distances ranging from 1.82–2.13 Å. V2+ is bonded to six F1- atoms to form VF6 octahedra that share corners with two equivalent VF6 octahedra, corners with five equivalent LiF4 trigonal pyramids, an edgeedge with one VF6 octahedra, and an edgeedge with one LiF4 trigonal pyramid. The corner-sharing octahedral tilt angles are 47°. There are a spread of V–F bond distances ranging from 2.05–2.20 Å. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to two equivalent Li1+ and one V2+ atom. In the second F1- site, F1- is bonded to two Li1+ and two equivalent V2+ atoms to form a mixture of distorted edge and corner-sharing FLi2V2 trigonal pyramids. In the third F1- site, F1- is bonded to two equivalent Li1+ and two equivalent V2+ atoms to form a mixture of distorted edge and corner-sharing FLi2V2 tetrahedra. In the fourth F1- site, F1- is bonded in a trigonal planar geometry to two Li1+ and one V2+ atom.

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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 Li2VF5 by Materials Project

Li2VF5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four F1- atoms to form distorted LiF4 tetrahedra that share corners with three equivalent VF6 octahedra, a cornercorner with one LiF4 tetrahedra, an edgeedge with one VF6 octahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 34–62°. There are a spread of Li–F bond distances ranging from 1.90–2.06 Å. In the second Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with four equivalent VF6 octahedra, a cornercorner with one LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 29–52°. There are a spread of Li–F bond distances ranging from 1.86–2.01 Å. V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with seven LiF4 tetrahedra, an edgeedge with one VF6 octahedra, and an edgeedge with one LiF4 tetrahedra. There are a spread of V–F bond distances ranging from 1.90–2.11 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a T-shaped geometry to two Li1+ and one V3+ atom. In the second F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent V3+ atoms. In the fourth F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one V3+ atom. In the fifth F1- site, F1- is bonded in a bent 120 degrees geometry to one Li1+ and one V3+ atom.

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Materials Data on LiVF3 by Materials Project

LiVF3 is Ilmenite-like structured and crystallizes in the orthorhombic Pccn space group. The structure is three-dimensional. Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.91–2.48 Å. V2+ is bonded to six F1- atoms to form a mixture of corner and edge-sharing VF6 octahedra. The corner-sharing octahedra tilt angles range from 53–55°. There are a spread of V–F bond distances ranging from 2.12–2.17 Å. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a 4-coordinate geometry to two equivalent Li1+ and two equivalent V2+ atoms. In the second 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 trigonal pyramids. In the third F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to two equivalent Li1+ and two equivalent V2+ atoms. 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 trigonal pyramids.

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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.

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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

36 MATERIALS SCIENCE↗

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

36 MATERIALS SCIENCE↗

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

36 MATERIALS SCIENCE↗

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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