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Materials Data on Li3V(BO3)2 by Materials Project

Li3V(BO3)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Li–O bond distances ranging from 1.97–2.31 Å. In the second Li1+ site, Li1+ is bonded in a distorted octahedral geometry to six O2- atoms. There are a spread of Li–O bond distances ranging from 2.01–2.48 Å. In the third Li1+ site, Li1+ is bonded in a 2-coordinate geometry to five O2- atoms. There are a spread of Li–O bond distances ranging from 1.94–2.68 Å. V3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of V–O bond distances ranging from 2.03–2.38 Å. There are two inequivalent B3+ sites. In the first B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.36–1.40 Å. In the second B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.37–1.40 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+, one V3+, and one B3+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to three Li1+, two equivalent V3+, and one B3+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one V3+, and one B3+ atom. In the fourth O2- site, O2- is bonded to three Li1+, one V3+, and one B3+ atom to form distorted edge-sharing OLi3VB trigonal bipyramids. In the fifth O2- site, O2- is bonded in a 1-coordinate geometry to four Li1+, one V3+, and one B3+ atom. In the sixth O2- site, O2- is bonded to two Li1+, one V3+, and one B3+ atom to form distorted edge-sharing OLi2VB tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li3V(BO3)2 by Materials Project

Li3V(BO3)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.89–2.07 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form distorted LiO4 tetrahedra that share corners with four equivalent VO7 pentagonal bipyramids. There are a spread of Li–O bond distances ranging from 1.94–2.04 Å. In the third Li1+ site, Li1+ is bonded in a distorted rectangular see-saw-like geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.87–2.07 Å. V3+ is bonded to seven O2- atoms to form VO7 pentagonal bipyramids that share corners with four equivalent LiO4 tetrahedra and an edgeedge with one VO7 pentagonal bipyramid. There are a spread of V–O bond distances ranging from 2.10–2.28 Å. There are two inequivalent B3+ sites. In the first B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.37–1.41 Å. In the second B3+ site, B3+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of B–O bond distances ranging from 1.37–1.39 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one V3+, and one B3+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one V3+, and one B3+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one V3+, and one B3+ atom. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to three Li1+, one V3+, and one B3+ atom. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to one Li1+, two equivalent V3+, and one B3+ atom. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one V3+, and one B3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3V(BO3)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 Li3V(BO3)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↗