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Materials Data on Li2VOF3 by Materials Project

Li2VOF3 crystallizes in the orthorhombic Pnc2 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to two equivalent O2- and four F1- atoms to form LiO2F4 octahedra that share corners with two equivalent VO2F4 octahedra and edges with three VO2F4 octahedra. The corner-sharing octahedral tilt angles are 55°. Both Li–O bond lengths are 2.19 Å. There are two shorter (2.04 Å) and two longer (2.09 Å) Li–F bond lengths. In the second 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 1.91–2.29 Å. In the third Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two equivalent O2- and four F1- atoms. Both Li–O bond lengths are 1.93 Å. There are two shorter (2.34 Å) and two longer (2.58 Å) Li–F bond lengths. In the fourth 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 1.90–2.34 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to two equivalent O2- and four F1- atoms to form VO2F4 octahedra that share edges with two equivalent LiO2F4 octahedra and edges with two equivalent VO2F4 octahedra. Both V–O bond lengths are 1.95 Å. There are two shorter (2.04 Å) and two longer (2.08 Å) V–F bond lengths. In the second V3+ site, V3+ is bonded to two equivalent O2- and four F1- atoms to form VO2F4 octahedra that share corners with two equivalent LiO2F4 octahedra, an edgeedge with one LiO2F4 octahedra, and edges with two equivalent VO2F4 octahedra. The corner-sharing octahedral tilt angles are 55°. Both V–O bond lengths are 1.93 Å. All V–F bond lengths are 2.08 Å. O2- is bonded to two Li1+ and two V3+ atoms to form a mixture of distorted corner and edge-sharing OLi2V2 trigonal pyramids. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the second F1- site, F1- is bonded in a 5-coordinate geometry to four Li1+ and one V3+ atom. In the third F1- site, F1- is bonded in a 5-coordinate geometry to four Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li2VOF3 by Materials Project

Li2VOF3 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 to four F1- atoms to form distorted LiF4 tetrahedra that share corners with three VO2F4 octahedra, corners with two equivalent LiF4 tetrahedra, and an edgeedge with one VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 51–73°. There are a spread of Li–F bond distances ranging from 1.91–2.03 Å. In the second Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.06 Å) and one longer (2.07 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.93–2.57 Å. In the third Li1+ site, Li1+ is bonded to four F1- atoms to form distorted LiF4 tetrahedra that share corners with three VO2F4 octahedra, corners with two equivalent LiF4 tetrahedra, and an edgeedge with one VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 52–71°. There are a spread of Li–F bond distances ranging from 1.90–2.04 Å. In the fourth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.05 Å) and one longer (2.12 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.93–2.60 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four equivalent VO2F4 octahedra, corners with three LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 42–43°. There is one shorter (1.89 Å) and one longer (1.93 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.07–2.13 Å. In the second V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four equivalent VO2F4 octahedra, corners with three LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 42–43°. There is one shorter (1.89 Å) and one longer (1.93 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.08–2.12 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+ and two V3+ atoms. In the second O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+ and two V3+ atoms. 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 tetrahedral geometry to three Li1+ and one V3+ atom. In the third F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the fourth F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the fifth F1- site, F1- is bonded in a distorted see-saw-like 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 Li2VOF3 by Materials Project

Li2VOF3 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are sixteen 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 1.91–2.03 Å. In the second Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.02 Å) and one longer (2.03 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.91–2.59 Å. In the third Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.05 Å) and one longer (2.08 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.92–2.64 Å. In the fourth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to one O2- and five F1- atoms. The Li–O bond length is 2.53 Å. There are a spread of Li–F bond distances ranging from 1.91–2.38 Å. In the fifth Li1+ site, Li1+ is bonded to four F1- atoms to form distorted LiF4 tetrahedra that share corners with three VO2F4 octahedra and an edgeedge with one VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 51–74°. There are a spread of Li–F bond distances ranging from 1.90–2.03 Å. In the sixth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.05 Å) and one longer (2.07 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.92–2.54 Å. In the seventh Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.04 Å) and one longer (2.08 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.92–2.59 Å. In the eighth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.03 Å) and one longer (2.08 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.92–2.61 Å. In the ninth 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 1.90–2.02 Å. In the tenth Li1+ site, Li1+ is bonded to four F1- atoms to form distorted LiF4 tetrahedra that share corners with three VO2F4 octahedra and an edgeedge with one VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 51–75°. There are a spread of Li–F bond distances ranging from 1.90–2.01 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 1.90–2.05 Å. In the twelfth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.05 Å) and one longer (2.06 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.92–2.53 Å. In the thirteenth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.04 Å) and one longer (2.07 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.93–2.54 Å. In the fourteenth 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 1.91–2.02 Å. In the fifteenth 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 1.90–2.03 Å. In the sixteenth Li1+ site, Li1+ is bonded in a 6-coordinate geometry to two O2- and four F1- atoms. There are one shorter (2.02 Å) and one longer (2.12 Å) Li–O bond lengths. There are a spread of Li–F bond distances ranging from 1.93–2.49 Å. There are eight inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four VO2F4 octahedra and corners with two LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 43–45°. There is one shorter (1.89 Å) and one longer (1.94 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.05–2.13 Å. In the second V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four VO2F4 octahedra and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 44–45°. There is one shorter (1.90 Å) and one longer (1.95 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.06–2.13 Å. In the third V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four VO2F4 octahedra and a cornercorner with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 43–45°. There is one shorter (1.90 Å) and one longer (1.95 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.05–2.12 Å. In the fourth V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four VO2F4 octahedra and a cornercorner with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 44–45°. There is one shorter (1.90 Å) and one longer (1.95 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.06–2.11 Å. In the fifth V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four VO2F4 octahedra, a cornercorner with one LiF4 tetrahedra, and an edgeedge with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 44–45°. There is one shorter (1.90 Å) and one longer (1.95 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.06–2.12 Å. In the sixth V3+ site, V3+ is bonded to two O2- and four F1- atoms to form corner-sharing VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 44–45°. There is one shorter (1.91 Å) and one longer (1.93 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.06–2.14 Å. In the seventh V3+ site, V3+ is bonded to two O2- and four F1- atoms to form corner-sharing VO2F4 octahedra. The corner-sharing octahedra tilt angles range from 43–45°. There is one shorter (1.91 Å) and one longer (1.94 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.06–2.12 Å. In the eighth V3+ site, V3+ is bonded to two O2- and four F1- atoms to form VO2F4 octahedra that share corners with four VO2F4 octahedra and a cornercorner with one LiF4 tetrahedra. The corner-sharing octahedra tilt angles range from 43–45°. There is one shorter (1.90 Å) and one longer (1.94 Å) V–O bond length. There are a spread of V–F bond distances ranging from 2.06–2.11 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the third O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+ and two V3+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to three Li1+ and two V3+ atoms. In the seventh O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. There are twenty-four 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 4-coordinate geometry to three Li1+ and one V3+ atom. In the third F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the fourth F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the fifth F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the sixth F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the seventh F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the eighth F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the ninth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the tenth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the eleventh F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the twelfth F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the thirteenth F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the fourteenth F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the fifteenth F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the sixteenth F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the seventeenth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the eighteenth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the nineteenth F1- site, F1- is bonded in a 4-coordinate geometry to three Li1+ and one V3+ atom. In the twentieth F1- site, F1- is bonded in a 3-coordinate geometry to two Li1+ and two V3+ atoms. In the twenty-first F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the twenty-second F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two V3+ atoms. In the twenty-third F1- site, F1- is bonded in a distorted see-saw-like geometry to three Li1+ and one V3+ atom. In the twenty-fourth F1- site, F1- is bonded in a 5-coordinate geometry to four Li1+ and one V3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li2VOF3 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 Li2VOF3 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 Li2VOF3 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 Li2VOF3 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↗