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Materials Data on Li3VF6 by Materials Project

Li3VF6 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six F1- atoms to form LiF6 octahedra that share corners with six equivalent VF6 octahedra and edges with six LiF6 octahedra. The corner-sharing octahedra tilt angles range from 44–45°. There are a spread of Li–F bond distances ranging from 2.08–2.13 Å. In the second Li1+ site, Li1+ is bonded to six F1- atoms to form LiF6 octahedra that share edges with six equivalent LiF6 octahedra and faces with two equivalent VF6 octahedra. There is four shorter (1.94 Å) and two longer (1.95 Å) Li–F bond length. V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with twelve equivalent LiF6 octahedra and faces with two equivalent LiF6 octahedra. The corner-sharing octahedra tilt angles range from 44–45°. There are two shorter (1.98 Å) and four longer (2.02 Å) V–F bond lengths. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the second F1- site, F1- is bonded in a rectangular see-saw-like geometry to three Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3VF6 by Materials Project

Li3VF6 is Ilmenite-like structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six F1- atoms to form distorted LiF6 pentagonal pyramids that share a cornercorner with one LiF6 octahedra, corners with four equivalent VF6 octahedra, an edgeedge with one LiF6 octahedra, an edgeedge with one VF6 octahedra, and a faceface with one LiF6 octahedra. The corner-sharing octahedra tilt angles range from 17–46°. There are a spread of Li–F bond distances ranging from 1.97–2.29 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.92–2.03 Å. In the third Li1+ site, Li1+ is bonded to six F1- atoms to form LiF6 octahedra that share a cornercorner with one LiF6 pentagonal pyramid, edges with three equivalent VF6 octahedra, an edgeedge with one LiF6 pentagonal pyramid, and a faceface with one LiF6 pentagonal pyramid. There are a spread of Li–F bond distances ranging from 1.96–2.22 Å. V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with four equivalent LiF6 pentagonal pyramids, edges with three equivalent LiF6 octahedra, and an edgeedge with one LiF6 pentagonal pyramid. There are a spread of V–F bond distances ranging from 1.96–2.01 Å. There are six inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the second F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the third F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the fourth F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom. In the fifth F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom. In the sixth F1- site, F1- is bonded in a rectangular see-saw-like geometry to three Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3VF6 by Materials Project

Li3VF6 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.90–2.17 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.90–2.17 Å. In the third Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.92–2.00 Å. In the fourth Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with four VF6 octahedra. The corner-sharing octahedra tilt angles range from 32–51°. There are a spread of Li–F bond distances ranging from 1.86–1.91 Å. In the fifth Li1+ site, Li1+ is bonded to four F1- atoms to form LiF4 tetrahedra that share corners with four VF6 octahedra. The corner-sharing octahedra tilt angles range from 31–51°. There are a spread of Li–F bond distances ranging from 1.86–1.91 Å. In the sixth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.92–2.00 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with four LiF4 tetrahedra. There are a spread of V–F bond distances ranging from 1.96–2.03 Å. In the second V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with four LiF4 tetrahedra. There are a spread of V–F bond distances ranging from 1.95–2.03 Å. There are twelve inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom. In the second F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the third F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to two Li1+ and one V3+ atom. In the fourth F1- site, F1- is bonded in a distorted trigonal non-coplanar geometry to two Li1+ and one V3+ atom. In the fifth F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one V3+ atom. In the sixth F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom. In the seventh F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom. In the eighth F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one V3+ atom. In the ninth F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom. In the tenth F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom. In the eleventh F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the twelfth F1- site, F1- is bonded in a distorted T-shaped geometry to two Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3VF6 by Materials Project

Li3VF6 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are twelve inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.95–2.05 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.94–2.04 Å. In the third Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.93–2.40 Å. In the fourth Li1+ site, Li1+ is bonded to five F1- atoms to form LiF5 trigonal bipyramids that share corners with five VF6 octahedra. The corner-sharing octahedra tilt angles range from 24–54°. There are a spread of Li–F bond distances ranging from 1.96–2.07 Å. In the fifth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.93–2.42 Å. In the sixth Li1+ site, Li1+ is bonded to five F1- atoms to form LiF5 trigonal bipyramids that share corners with five VF6 octahedra. The corner-sharing octahedra tilt angles range from 23–53°. There are a spread of Li–F bond distances ranging from 1.97–2.07 Å. In the seventh Li1+ site, Li1+ is bonded to five F1- atoms to form LiF5 trigonal bipyramids that share corners with five VF6 octahedra. The corner-sharing octahedra tilt angles range from 22–54°. There are a spread of Li–F bond distances ranging from 1.96–2.09 Å. In the eighth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.94–2.37 Å. In the ninth Li1+ site, Li1+ is bonded to five F1- atoms to form LiF5 trigonal bipyramids that share corners with five VF6 octahedra. The corner-sharing octahedra tilt angles range from 23–54°. There are a spread of Li–F bond distances ranging from 1.97–2.07 Å. In the tenth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.93–2.40 Å. In the eleventh Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.95–2.05 Å. In the twelfth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Li–F bond distances ranging from 1.94–2.03 Å. There are four inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with four LiF5 trigonal bipyramids. There are a spread of V–F bond distances ranging from 1.94–2.03 Å. In the second V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with four LiF5 trigonal bipyramids. There are a spread of V–F bond distances ranging from 1.94–2.03 Å. In the third V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with six LiF5 trigonal bipyramids. There are a spread of V–F bond distances ranging from 1.93–2.03 Å. In the fourth V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with six LiF5 trigonal bipyramids. There are a spread of V–F bond distances ranging from 1.93–2.02 Å. There are twenty-four inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the second F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the third F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the fifth F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the sixth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the seventh F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the eighth F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the ninth F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the tenth F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the eleventh F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the twelfth F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one V3+ atom. In the thirteenth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the fourteenth F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one V3+ atom. In the fifteenth F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the sixteenth F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the seventeenth F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the eighteenth F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the nineteenth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the twentieth F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the twenty-first F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one V3+ atom. In the twenty-second F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom. In the twenty-third F1- site, F1- is bonded to three Li1+ and one V3+ atom to form distorted corner-sharing FLi3V trigonal pyramids. In the twenty-fourth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3VF6 by Materials Project

Li3VF6 is Ilmenite-like structured and crystallizes in the trigonal R-3 space group. The structure is three-dimensional. Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.95–2.28 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded in an octahedral geometry to six equivalent F1- atoms. All V–F bond lengths are 1.97 Å. In the second V3+ site, V3+ is bonded in an octahedral geometry to six equivalent F1- atoms. All V–F bond lengths are 1.97 Å. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded to three equivalent Li1+ and one V3+ atom to form a mixture of distorted edge and corner-sharing FLi3V trigonal pyramids. In the second F1- site, F1- is bonded in a distorted see-saw-like geometry to three equivalent Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3VF6 by Materials Project

Li3VF6 is Ilmenite-like structured and crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.96–2.41 Å. In the second Li1+ site, Li1+ is bonded to six F1- atoms to form LiF6 octahedra that share edges with three equivalent VF6 octahedra. There are two shorter (2.10 Å) and four longer (2.11 Å) Li–F bond lengths. In the third Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.95–2.41 Å. V3+ is bonded to six F1- atoms to form VF6 octahedra that share edges with three equivalent LiF6 octahedra. There are a spread of V–F bond distances ranging from 1.96–1.98 Å. There are six inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the second F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the third F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the fourth F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to three Li1+ and one V3+ atom. In the fifth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the sixth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3VF6 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 Li3VF6 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 Li3VF6 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↗