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Materials Data on Li4V(TeO4)3 by Materials Project

Li4V(TeO4)3 is Ilmenite-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first 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 2.02–2.40 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 2.00–2.39 Å. In the third Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with two equivalent TeO6 octahedra and edges with three TeO6 octahedra. The corner-sharing octahedra tilt angles range from 62–63°. There are a spread of Li–O bond distances ranging from 2.08–2.28 Å. In the fourth 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 2.02–2.40 Å. V4+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.71–2.41 Å. There are three inequivalent Te+5.33+ sites. In the first Te+5.33+ site, Te+5.33+ is bonded to six O2- atoms to form TeO6 octahedra that share corners with four equivalent TeO6 octahedra and an edgeedge with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 40–45°. There are a spread of Te–O bond distances ranging from 1.90–2.11 Å. In the second Te+5.33+ site, Te+5.33+ is bonded to six O2- atoms to form distorted TeO6 octahedra that share corners with two equivalent TeO6 octahedra and edges with two equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 37–38°. There are a spread of Te–O bond distances ranging from 1.92–2.51 Å. In the third Te+5.33+ site, Te+5.33+ is bonded to six O2- atoms to form TeO6 octahedra that share corners with two equivalent LiO6 octahedra and corners with six TeO6 octahedra. The corner-sharing octahedra tilt angles range from 37–63°. There are a spread of Te–O bond distances ranging from 2.00–2.22 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two Li1+, one V4+, and one Te+5.33+ atom. In the second O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+ and two Te+5.33+ atoms. In the third O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+ and two Te+5.33+ atoms. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to two Li1+, one V4+, and one Te+5.33+ atom. In the fifth O2- site, O2- is bonded to two Li1+ and two Te+5.33+ atoms to form distorted corner-sharing OLi2Te2 trigonal pyramids. In the sixth O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+ and two Te+5.33+ atoms. In the seventh O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+, one V4+, and one Te+5.33+ atom. In the eighth O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+ and two Te+5.33+ atoms. In the ninth O2- site, O2- is bonded to two Li1+ and two Te+5.33+ atoms to form distorted OLi2Te2 trigonal pyramids that share corners with four OLi2Te2 trigonal pyramids and an edgeedge with one OLi2VTe trigonal pyramid. In the tenth O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+, one V4+, and one Te+5.33+ atom. In the eleventh O2- site, O2- is bonded to two Li1+, one V4+, and one Te+5.33+ atom to form a mixture of distorted edge and corner-sharing OLi2VTe trigonal pyramids. In the twelfth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one V4+, and one Te+5.33+ atom.

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Materials Data on LiVTeO5 by Materials Project

LiVTeO5 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form distorted edge-sharing LiO6 octahedra. There are a spread of Li–O bond distances ranging from 2.10–2.53 Å. V5+ is bonded in a 4-coordinate geometry to five O2- atoms. There are a spread of V–O bond distances ranging from 1.65–2.46 Å. Te4+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Te–O bond distances ranging from 1.89–2.77 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one V5+ and one Te4+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Li1+ and one V5+ atom. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+, one V5+, and one Te4+ atom. In the fourth O2- site, O2- is bonded to two equivalent Li1+, one V5+, and one Te4+ atom to form distorted corner-sharing OLi2VTe trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Li2V3TeO8 by Materials Project

Li2V3TeO8 is Hausmannite-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are eight 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 TeO4 tetrahedra, corners with three LiO4 tetrahedra, and edges with six VO6 octahedra. There are a spread of Li–O bond distances ranging from 2.10–2.35 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with three LiO6 octahedra and corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 44–69°. There are a spread of Li–O bond distances ranging from 2.01–2.12 Å. In the third Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with three LiO6 octahedra and corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 44–71°. There are a spread of Li–O bond distances ranging from 2.00–2.13 Å. In the fourth Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, and edges with six VO6 octahedra. There are a spread of Li–O bond distances ranging from 2.08–2.34 Å. In the fifth Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with three LiO4 tetrahedra and edges with six VO6 octahedra. There are a spread of Li–O bond distances ranging from 2.09–2.33 Å. In the sixth Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with three LiO6 octahedra and corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 48–70°. There are a spread of Li–O bond distances ranging from 2.04–2.10 Å. In the seventh Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with three LiO6 octahedra and corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 45–69°. There are a spread of Li–O bond distances ranging from 2.01–2.12 Å. In the eighth Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, and edges with six VO6 octahedra. There are a spread of Li–O bond distances ranging from 2.07–2.35 Å. There are twelve inequivalent V5+ sites. In the first V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.93–2.29 Å. In the second V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.86–2.35 Å. In the third V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.81–2.46 Å. In the fourth V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.84–2.46 Å. In the fifth V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.95–2.28 Å. In the sixth V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.93–2.30 Å. In the seventh V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.93–2.33 Å. In the eighth V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.95–2.27 Å. In the ninth V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.84–2.47 Å. In the tenth V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.94–2.40 Å. In the eleventh V5+ site, V5+ is bonded to six O2- atoms to form VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.97–2.26 Å. In the twelfth V5+ site, V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one TeO4 tetrahedra, corners with three LiO4 tetrahedra, edges with two LiO6 octahedra, and edges with four VO6 octahedra. There are a spread of V–O bond distances ranging from 1.92–2.34 Å. There are four inequivalent Te1- sites. In the first Te1- site, Te1- is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Te–O bond distances ranging from 1.92–2.63 Å. In the second Te1- site, Te1- is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Te–O bond distances ranging from 1.92–2.61 Å. In the third Te1- site, Te1- is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Te–O bond distances ranging from 1.91–2.61 Å. In the fourth Te1- site, Te1- is bonded to four O2- atoms to form distorted TeO4 tetrahedra that share corners with three LiO6 octahedra and corners with nine VO6 octahedra. The corner-sharing octahedra tilt angles range from 52–74°. There are a spread of Te–O bond distances ranging from 1.93–2.56 Å. There are thirty-two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the third O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three V5+ atoms. In the fourth O2- site, O2- is bonded to two Li1+ and two V5+ atoms to form distorted corner-sharing OLi2V2 trigonal pyramids. In the fifth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the sixth O2- site, O2- is bonded to three V5+ and one Te1- atom to form distorted corner-sharing OV3Te tetrahedra. In the seventh O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the eighth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the ninth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the tenth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the eleventh O2- site, O2- is bonded to three V5+ and one Te1- atom to form distorted corner-sharing OV3Te tetrahedra. In the twelfth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the thirteenth O2- site, O2- is bonded to two Li1+ and two V5+ atoms to form distorted corner-sharing OLi2V2 trigonal pyramids. In the fourteenth O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three V5+ atoms. In the fifteenth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the sixteenth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the seventeenth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the eighteenth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the nineteenth O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three V5+ atoms. In the twentieth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the twenty-first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the twenty-second O2- site, O2- is bonded in a distorted tetrahedral geometry to three V5+ and one Te1- atom. In the twenty-third O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the twenty-fourth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the twenty-fifth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the twenty-sixth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the twenty-seventh O2- site, O2- is bonded in a distorted tetrahedral geometry to three V5+ and one Te1- atom. In the twenty-eighth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+, two V5+, and one Te1- atom. In the twenty-ninth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the thirtieth O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+ and three V5+ atoms. In the thirty-first O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two V5+ atoms. In the thirty-second O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two V5+ atoms.

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Materials Data on Li2V3TeO8 by Materials Project

Li2V3TeO8 is Spinel-derived structured and crystallizes in the trigonal P31c 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 three equivalent TeO6 octahedra and corners with nine equivalent VO6 octahedra. The corner-sharing octahedra tilt angles range from 56–63°. There are three shorter (2.01 Å) and one longer (2.06 Å) Li–O bond lengths. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form distorted LiO4 trigonal pyramids that share corners with three equivalent VO6 octahedra, corners with three equivalent TeO6 octahedra, and edges with three equivalent VO6 octahedra. The corner-sharing octahedra tilt angles range from 62–63°. There is one shorter (1.83 Å) and three longer (1.96 Å) Li–O bond length. V5+ is bonded to six O2- atoms to form VO6 octahedra that share corners with two equivalent TeO6 octahedra, corners with three equivalent LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one TeO6 octahedra, edges with four equivalent VO6 octahedra, and an edgeedge with one LiO4 trigonal pyramid. The corner-sharing octahedra tilt angles range from 51–55°. There are a spread of V–O bond distances ranging from 1.99–2.13 Å. Te1- is bonded to six O2- atoms to form TeO6 octahedra that share corners with six equivalent VO6 octahedra, corners with three equivalent LiO4 tetrahedra, corners with three equivalent LiO4 trigonal pyramids, and edges with three equivalent VO6 octahedra. The corner-sharing octahedra tilt angles range from 51–55°. There are three shorter (2.09 Å) and three longer (2.21 Å) Te–O bond lengths. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+, two equivalent V5+, and one Te1- atom. In the second O2- site, O2- is bonded to one Li1+, two equivalent V5+, and one Te1- atom to form distorted OLiV2Te tetrahedra that share corners with four OLiV2Te tetrahedra, a cornercorner with one OLiV3 trigonal pyramid, edges with two equivalent OLiV2Te tetrahedra, and an edgeedge with one OLiV3 trigonal pyramid. In the third O2- site, O2- is bonded to one Li1+ and three equivalent V5+ atoms to form a mixture of distorted edge and corner-sharing OLiV3 trigonal pyramids. In the fourth O2- site, O2- is bonded to one Li1+ and three equivalent V5+ atoms to form OLiV3 tetrahedra that share corners with six equivalent OLiV2Te tetrahedra and corners with three equivalent OLiV3 trigonal pyramids.

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Materials Data on Li2V3TeO8 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 Li2V3TeO8 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 Li2V3TeO8 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 Li2V3TeO8 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 Li4V(TeO4)3 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 LiV(TeO4)3 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 Li3V(TeO3)4 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 Li4V(TeO4)3 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 LiV3(TeO6)2 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 LiVTeO5 by Materials Project

LiVTeO5 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Li1+ is bonded in a distorted T-shaped geometry to three O2- atoms. There are a spread of Li–O bond distances ranging from 1.96–2.18 Å. V5+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of V–O bond distances ranging from 1.68–1.87 Å. Te4+ is bonded in an L-shaped geometry to two O2- atoms. There is one shorter (1.97 Å) and one longer (2.00 Å) Te–O bond length. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Te4+ and one O2- atom. The O–O bond length is 1.50 Å. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Li1+ and one V5+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one V5+ and one O2- atom. In the fourth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Li1+, one V5+, and one Te4+ atom. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to one Li1+ and one V5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li2V3TeO8 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 LiVTeO5 by Materials Project

LiVTeO5 is Antimony trioxide-derived structured and crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. Li1+ is bonded in a 4-coordinate geometry to five O2- atoms. There are a spread of Li–O bond distances ranging from 1.97–2.57 Å. V5+ is bonded in a distorted trigonal bipyramidal geometry to five O2- atoms. There are a spread of V–O bond distances ranging from 1.68–2.06 Å. Te4+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Te–O bond distances ranging from 1.90–2.36 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to one Li1+, one V5+, and one Te4+ atom. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+, one V5+, and one Te4+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one V5+ and two equivalent Te4+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+, one V5+, and one Te4+ atom. In the fifth O2- site, O2- is bonded in a trigonal non-coplanar geometry to two equivalent Li1+ and one V5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on LiV(TeO4)3 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 LiV(TeO4)3 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↗