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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.

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 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↗