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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 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 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 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 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

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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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