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Materials Data on Li3VO4 by Materials Project

Li3VO4 is Enargite structured and crystallizes in the orthorhombic Pmn2_1 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent VO4 tetrahedra and corners with eight LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.01 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent VO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. There are one shorter (2.01 Å) and three longer (2.02 Å) Li–O bond lengths. V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with twelve LiO4 tetrahedra. There is one shorter (1.74 Å) and three longer (1.75 Å) V–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to three Li1+ and one V5+ atom to form corner-sharing OLi3V tetrahedra. In the second O2- site, O2- is bonded to three Li1+ and one V5+ atom to form corner-sharing OLi3V tetrahedra. In the third O2- site, O2- is bonded to three Li1+ and one V5+ atom to form corner-sharing OLi3V tetrahedra.

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Materials Data on LiVO2 by Materials Project

LiVO2 is Caswellsilverite structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Li1+ is bonded to six equivalent O2- atoms to form LiO6 octahedra that share corners with six equivalent VO6 octahedra, edges with six equivalent LiO6 octahedra, and edges with six equivalent VO6 octahedra. The corner-sharing octahedral tilt angles are 4°. All Li–O bond lengths are 2.18 Å. V3+ is bonded to six equivalent O2- atoms to form VO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with six equivalent LiO6 octahedra, and edges with six equivalent VO6 octahedra. The corner-sharing octahedral tilt angles are 4°. All V–O bond lengths are 2.06 Å. O2- is bonded to three equivalent Li1+ and three equivalent V3+ atoms to form a mixture of edge and corner-sharing OLi3V3 octahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on LiVO3 by Materials Project

LiVO3 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent VO4 tetrahedra and edges with two equivalent LiO6 octahedra. There are a spread of Li–O bond distances ranging from 2.05–2.33 Å. In the second Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Li–O bond distances ranging from 2.02–2.64 Å. V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with three equivalent LiO6 octahedra and corners with two equivalent VO4 tetrahedra. The corner-sharing octahedra tilt angles range from 27–64°. There are a spread of V–O bond distances ranging from 1.66–1.84 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent V5+ atoms. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V5+ atom. In the third O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Li1+ and one V5+ atom.

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Materials Data on LiV2O4 by Materials Project

LiV2O4 is Spinel structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Li1+ is bonded to four equivalent O2- atoms to form LiO4 tetrahedra that share corners with twelve equivalent VO6 octahedra. The corner-sharing octahedral tilt angles are 58°. All Li–O bond lengths are 1.97 Å. V+3.50+ is bonded to six equivalent O2- atoms to form VO6 octahedra that share corners with six equivalent LiO4 tetrahedra and edges with six equivalent VO6 octahedra. All V–O bond lengths are 2.01 Å. O2- is bonded to one Li1+ and three equivalent V+3.50+ atoms to form a mixture of distorted corner and edge-sharing OLiV3 trigonal pyramids.

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Materials Data on Li3V6O13 by Materials Project

Li3V6O13 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to five O2- atoms to form LiO5 square pyramids that share a cornercorner with one VO6 octahedra, corners with two equivalent LiO5 square pyramids, edges with four VO6 octahedra, and an edgeedge with one LiO5 square pyramid. The corner-sharing octahedral tilt angles are 8°. There are a spread of Li–O bond distances ranging from 1.99–2.14 Å. In the second Li1+ site, Li1+ is bonded to five O2- atoms to form LiO5 square pyramids that share a cornercorner with one VO6 octahedra, corners with two equivalent LiO5 square pyramids, edges with four VO6 octahedra, and an edgeedge with one LiO5 square pyramid. The corner-sharing octahedral tilt angles are 8°. There are a spread of Li–O bond distances ranging from 1.99–2.15 Å. In the third Li1+ site, Li1+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 2.01–2.21 Å. There are six inequivalent V+3.83+ sites. In the first V+3.83+ site, V+3.83+ is bonded to six O2- atoms to form a mixture of corner and edge-sharing VO6 octahedra. The corner-sharing octahedra tilt angles range from 0–15°. There are a spread of V–O bond distances ranging from 1.97–2.03 Å. In the second V+3.83+ site, V+3.83+ is bonded to six O2- atoms to form a mixture of corner and edge-sharing VO6 octahedra. The corner-sharing octahedra tilt angles range from 0–11°. There are a spread of V–O bond distances ranging from 1.84–2.04 Å. In the third V+3.83+ site, V+3.83+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with three VO6 octahedra, a cornercorner with one LiO5 square pyramid, an edgeedge with one VO6 octahedra, and edges with four LiO5 square pyramids. The corner-sharing octahedra tilt angles range from 8–18°. There are a spread of V–O bond distances ranging from 1.71–2.18 Å. In the fourth V+3.83+ site, V+3.83+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with three VO6 octahedra, a cornercorner with one LiO5 square pyramid, an edgeedge with one VO6 octahedra, and edges with four LiO5 square pyramids. The corner-sharing octahedra tilt angles range from 4–18°. There are a spread of V–O bond distances ranging from 1.70–2.17 Å. In the fifth V+3.83+ site, V+3.83+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.68–2.35 Å. In the sixth V+3.83+ site, V+3.83+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.69–2.36 Å. There are thirteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a square co-planar geometry to one Li1+ and three V+3.83+ atoms. In the second O2- site, O2- is bonded in a square co-planar geometry to one Li1+ and three V+3.83+ atoms. In the third O2- site, O2- is bonded to two Li1+ and three V+3.83+ atoms to form OLi2V3 square pyramids that share corners with two equivalent OLi2V3 square pyramids, corners with two OLiV4 trigonal bipyramids, an edgeedge with one OLi2V3 square pyramid, and edges with seven OLiV4 trigonal bipyramids. In the fourth O2- site, O2- is bonded to two Li1+ and three V+3.83+ atoms to form OLi2V3 square pyramids that share corners with two equivalent OLi2V3 square pyramids, corners with two OLiV4 trigonal bipyramids, an edgeedge with one OLi2V3 square pyramid, and edges with seven OLiV4 trigonal bipyramids. In the fifth O2- site, O2- is bonded to one Li1+ and four V+3.83+ atoms to form distorted OLiV4 trigonal bipyramids that share a cornercorner with one OLi2V3 square pyramid, corners with three OLiV4 trigonal bipyramids, edges with three OLi2V3 square pyramids, and edges with five OLiV4 trigonal bipyramids. In the sixth O2- site, O2- is bonded to one Li1+ and four V+3.83+ atoms to form distorted OLiV4 trigonal bipyramids that share a cornercorner with one OLi2V3 square pyramid, corners with three OLiV4 trigonal bipyramids, edges with three OLi2V3 square pyramids, and edges with five OLiV4 trigonal bipyramids. In the seventh O2- site, O2- is bonded in a square co-planar geometry to two equivalent Li1+ and two V+3.83+ atoms. In the eighth O2- site, O2- is bonded in a linear geometry to two V+3.83+ atoms. In the ninth O2- site, O2- is bonded in a linear geometry to two V+3.83+ atoms. In the tenth O2- site, O2- is bonded in a linear geometry to two V+3.83+ atoms. In the eleventh O2- site, O2- is bonded in a linear geometry to two V+3.83+ atoms. In the twelfth O2- site, O2- is bonded to two equivalent Li1+ and three V+3.83+ atoms to form OLi2V3 trigonal bipyramids that share a cornercorner with one OLi2V3 square pyramid, corners with three OLiV4 trigonal bipyramids, edges with four OLi2V3 square pyramids, and edges with four OLiV4 trigonal bipyramids. In the thirteenth O2- site, O2- is bonded to two equivalent Li1+ and three V+3.83+ atoms to form OLi2V3 trigonal bipyramids that share a cornercorner with one OLi2V3 square pyramid, corners with three OLiV4 trigonal bipyramids, edges with four OLi2V3 square pyramids, and edges with four OLiV4 trigonal bipyramids.

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Materials Data on Li3V5O10 by Materials Project

Li3V5O10 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share a cornercorner with one LiO6 octahedra, corners with five VO6 octahedra, edges with four LiO6 octahedra, and edges with five VO6 octahedra. The corner-sharing octahedra tilt angles range from 7–20°. There are a spread of Li–O bond distances ranging from 2.09–2.36 Å. In the second Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with two equivalent LiO6 octahedra, corners with two equivalent VO6 octahedra, edges with four equivalent LiO6 octahedra, and edges with six VO6 octahedra. The corner-sharing octahedra tilt angles range from 11–14°. There are a spread of Li–O bond distances ranging from 1.98–2.43 Å. There are three inequivalent V+3.40+ sites. In the first V+3.40+ site, V+3.40+ is bonded to six O2- atoms to form VO6 octahedra that share a cornercorner with one VO6 octahedra, corners with two equivalent LiO6 octahedra, edges with five LiO6 octahedra, and edges with five VO6 octahedra. The corner-sharing octahedra tilt angles range from 11–15°. There are a spread of V–O bond distances ranging from 1.81–2.10 Å. In the second V+3.40+ site, V+3.40+ is bonded to six O2- atoms to form VO6 octahedra that share corners with two equivalent LiO6 octahedra, corners with four VO6 octahedra, edges with two equivalent LiO6 octahedra, and edges with six VO6 octahedra. The corner-sharing octahedra tilt angles range from 11–16°. There are four shorter (2.04 Å) and two longer (2.10 Å) V–O bond lengths. In the third V+3.40+ site, V+3.40+ is bonded to six O2- atoms to form VO6 octahedra that share a cornercorner with one VO6 octahedra, corners with three equivalent LiO6 octahedra, edges with two LiO6 octahedra, and edges with seven VO6 octahedra. The corner-sharing octahedra tilt angles range from 7–20°. There are a spread of V–O bond distances ranging from 1.98–2.16 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded to one Li1+ and four V+3.40+ atoms to form a mixture of edge and corner-sharing OLiV4 square pyramids. In the second O2- site, O2- is bonded to three Li1+ and two equivalent V+3.40+ atoms to form a mixture of edge and corner-sharing OLi3V2 square pyramids. In the third O2- site, O2- is bonded in a rectangular see-saw-like geometry to four V+3.40+ atoms. In the fourth O2- site, O2- is bonded to two Li1+ and three V+3.40+ atoms to form distorted OLi2V3 square pyramids that share corners with six OLi3V2 square pyramids and edges with seven OLiV4 square pyramids. In the fifth O2- site, O2- is bonded to three Li1+ and two V+3.40+ atoms to form a mixture of distorted edge and corner-sharing OLi3V2 square pyramids.

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Materials Data on Li2V3O8 by Materials Project

Li2V3O8 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 51–60°. There are a spread of Li–O bond distances ranging from 1.96–2.00 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 51–60°. There are a spread of Li–O bond distances ranging from 1.96–2.00 Å. In the third Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 52–61°. There are a spread of Li–O bond distances ranging from 1.97–2.00 Å. In the fourth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 52–61°. There are a spread of Li–O bond distances ranging from 1.97–2.00 Å. There are six inequivalent V+4.67+ sites. In the first V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six LiO4 tetrahedra and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.83–2.05 Å. In the second V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with six LiO4 tetrahedra and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.74–2.12 Å. In the third V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with six LiO4 tetrahedra and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.77–2.14 Å. In the fourth V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with six LiO4 tetrahedra and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.74–2.12 Å. In the fifth V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with six LiO4 tetrahedra and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.77–2.13 Å. In the sixth V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six LiO4 tetrahedra and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.83–2.04 Å. There are sixteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the third O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+ and three V+4.67+ atoms. In the fourth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the seventh O2- site, O2- is bonded in a trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the eighth O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to one Li1+ and three V+4.67+ atoms. In the ninth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the tenth O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to one Li1+ and three V+4.67+ atoms. In the eleventh O2- site, O2- is bonded in a trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the twelfth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the thirteenth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+ and three V+4.67+ atoms. In the fourteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the fifteenth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+ and two V+4.67+ atoms. In the sixteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two V+4.67+ atoms.

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Materials Data on LiVO2 by Materials Project

LiVO2 crystallizes in the triclinic P1 space group. The structure is two-dimensional and consists of one LiVO2 sheet oriented in the (0, 0, 1) direction. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 5-coordinate geometry to one V3+ and four O2- atoms. The Li–V bond length is 2.20 Å. There are a spread of Li–O bond distances ranging from 1.97–2.24 Å. In the second Li1+ site, Li1+ is bonded in a 5-coordinate geometry to one V3+ and four O2- atoms. The Li–V bond length is 2.21 Å. There are a spread of Li–O bond distances ranging from 1.96–2.25 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded in a 5-coordinate geometry to one Li1+ and four O2- atoms. There are a spread of V–O bond distances ranging from 1.96–2.25 Å. In the second V3+ site, V3+ is bonded in a 5-coordinate geometry to one Li1+ and four O2- atoms. There are a spread of V–O bond distances ranging from 1.96–2.25 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Li1+ and two equivalent V3+ atoms. In the second O2- site, O2- is bonded in a distorted square co-planar geometry to two equivalent Li1+ and two equivalent V3+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Li1+ and two equivalent V3+ atoms. In the fourth O2- site, O2- is bonded in a distorted square co-planar geometry to two equivalent Li1+ and two equivalent V3+ atoms.

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Materials Data on LiV3O8 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 Li2V5O10 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 Li9V14O35 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 LiV3O4 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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