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Materials Data on LiFe2OF3 by Materials Project

LiFe2OF3 is Spinel-derived structured and crystallizes in the tetragonal P4_3 space group. The structure is three-dimensional. Li1+ is bonded to one O2- and five F1- atoms to form LiOF5 octahedra that share corners with six equivalent FeOF3 tetrahedra, edges with two equivalent LiOF5 octahedra, and edges with four equivalent FeO2F4 octahedra. The Li–O bond length is 2.01 Å. There are a spread of Li–F bond distances ranging from 2.06–2.21 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to two equivalent O2- and four F1- atoms to form FeO2F4 octahedra that share corners with six equivalent FeOF3 tetrahedra, edges with two equivalent FeO2F4 octahedra, and edges with four equivalent LiOF5 octahedra. There are one shorter (1.99 Å) and one longer (2.07 Å) Fe–O bond lengths. There are a spread of Fe–F bond distances ranging from 2.15–2.27 Å. In the second Fe2+ site, Fe2+ is bonded to one O2- and three F1- atoms to form FeOF3 tetrahedra that share corners with six equivalent LiOF5 octahedra and corners with six equivalent FeO2F4 octahedra. The corner-sharing octahedra tilt angles range from 51–68°. The Fe–O bond length is 1.89 Å. There are a spread of Fe–F bond distances ranging from 2.01–2.13 Å. O2- is bonded to one Li1+ and three Fe2+ atoms to form distorted corner-sharing OLiFe3 tetrahedra. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms. In the second F1- site, F1- is bonded in a rectangular see-saw-like geometry to two equivalent Li1+ and two Fe2+ atoms. In the third F1- site, F1- is bonded in a rectangular see-saw-like geometry to two equivalent Li1+ and two Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFe2OF3 by Materials Project

LiFe2OF3 is Ilmenite-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Li1+ is bonded to one O2- and three F1- atoms to form distorted LiOF3 tetrahedra that share corners with six FeO2F4 octahedra and edges with three FeO2F4 octahedra. The corner-sharing octahedra tilt angles range from 60–65°. The Li–O bond length is 1.86 Å. There is one shorter (1.97 Å) and two longer (2.00 Å) Li–F bond length. There are three inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to two equivalent O2- and four F1- atoms to form FeO2F4 octahedra that share corners with four equivalent FeF6 octahedra, corners with two equivalent LiOF3 tetrahedra, edges with four FeO2F4 octahedra, and edges with two equivalent LiOF3 tetrahedra. The corner-sharing octahedra tilt angles range from 50–52°. Both Fe–O bond lengths are 1.96 Å. There are two shorter (2.30 Å) and two longer (2.36 Å) Fe–F bond lengths. In the second Fe2+ site, Fe2+ is bonded to two equivalent O2- and four equivalent F1- atoms to form FeO2F4 octahedra that share corners with four equivalent FeF6 octahedra, corners with two equivalent LiOF3 tetrahedra, edges with four equivalent FeO2F4 octahedra, and edges with two equivalent LiOF3 tetrahedra. The corner-sharing octahedral tilt angles are 48°. Both Fe–O bond lengths are 2.04 Å. All Fe–F bond lengths are 2.23 Å. In the third Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with twelve FeO2F4 octahedra and corners with six equivalent LiOF3 tetrahedra. The corner-sharing octahedra tilt angles range from 48–52°. There are four shorter (2.15 Å) and two longer (2.16 Å) Fe–F bond lengths. O2- is bonded to one Li1+ and three Fe2+ atoms to form corner-sharing OLiFe3 tetrahedra. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms. In the second F1- site, F1- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFe2OF3 by Materials Project

LiFe2OF3 is Spinel-derived structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Li1+ is bonded to one O2- and three equivalent F1- atoms to form LiOF3 tetrahedra that share corners with twelve FeF6 octahedra. The corner-sharing octahedra tilt angles range from 53–63°. The Li–O bond length is 1.99 Å. All Li–F bond lengths are 1.98 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to two equivalent O2- and four equivalent F1- atoms to form FeO2F4 octahedra that share corners with six equivalent LiOF3 tetrahedra and edges with six FeF6 octahedra. Both Fe–O bond lengths are 2.00 Å. All Fe–F bond lengths are 2.27 Å. In the second Fe2+ site, Fe2+ is bonded to six equivalent F1- atoms to form FeF6 octahedra that share corners with six equivalent LiOF3 tetrahedra and edges with six equivalent FeO2F4 octahedra. All Fe–F bond lengths are 2.12 Å. O2- is bonded to one Li1+ and three equivalent Fe2+ atoms to form corner-sharing OLiFe3 tetrahedra. F1- is bonded in a rectangular see-saw-like geometry to one Li1+ and three Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFe2OF3 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 LiFe2OF3 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 LiFe2OF3 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 LiFe2OF3 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 LiFe2OF3 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↗