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Materials Data on LiFeF3 by Materials Project

LiFeF3 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.93–2.52 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to six F1- atoms. There are a spread of Li–F bond distances ranging from 1.93–2.52 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing FeF6 octahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of Fe–F bond distances ranging from 2.03–2.15 Å. In the second Fe2+ site, Fe2+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing FeF6 octahedra. The corner-sharing octahedral tilt angles are 48°. There are a spread of Fe–F bond distances ranging from 2.02–2.15 Å. There are six inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe2+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe2+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to four Li1+ and one Fe2+ atom. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to four Li1+ and one Fe2+ atom. In the fifth F1- site, F1- is bonded to two Li1+ and two equivalent Fe2+ atoms to form distorted corner-sharing FLi2Fe2 trigonal pyramids. In the sixth F1- site, F1- is bonded to two Li1+ and two equivalent Fe2+ atoms to form distorted corner-sharing FLi2Fe2 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

LiFeF3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Li1+ is bonded to four F1- atoms to form distorted LiF4 trigonal pyramids that share corners with four equivalent FeF6 octahedra, corners with two equivalent LiF4 trigonal pyramids, and edges with two equivalent FeF6 octahedra. The corner-sharing octahedra tilt angles range from 35–73°. There are a spread of Li–F bond distances ranging from 1.85–2.11 Å. Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent FeF6 octahedra, corners with four equivalent LiF4 trigonal pyramids, edges with two equivalent FeF6 octahedra, and edges with two equivalent LiF4 trigonal pyramids. The corner-sharing octahedral tilt angles are 18°. There are a spread of Fe–F bond distances ranging from 2.02–2.22 Å. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded to two equivalent Li1+ and two equivalent Fe2+ atoms to form corner-sharing FLi2Fe2 trigonal pyramids. In the second F1- site, F1- is bonded in a 3-coordinate geometry to one Li1+ and two equivalent Fe2+ atoms. In the third F1- site, F1- is bonded in a T-shaped geometry to one Li1+ and two equivalent Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 by Materials Project

LiFeF3 is pyrite-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Li1+ is bonded to five F1- atoms to form distorted LiF5 tetrahedra that share corners with six FeF6 octahedra, corners with four equivalent LiF5 tetrahedra, and edges with two FeF6 octahedra. The corner-sharing octahedra tilt angles range from 53–71°. There are a spread of Li–F bond distances ranging from 1.93–2.53 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent FeF6 octahedra, corners with six equivalent LiF5 tetrahedra, edges with two equivalent FeF6 octahedra, and edges with two equivalent LiF5 tetrahedra. The corner-sharing octahedral tilt angles are 64°. There are a spread of Fe–F bond distances ranging from 2.08–2.17 Å. In the second Fe2+ site, Fe2+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with two equivalent FeF6 octahedra, corners with six equivalent LiF5 tetrahedra, edges with two equivalent FeF6 octahedra, and edges with two equivalent LiF5 tetrahedra. The corner-sharing octahedral tilt angles are 64°. There are a spread of Fe–F bond distances ranging from 2.05–2.17 Å. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a 3-coordinate geometry to one Li1+ and two Fe2+ atoms. In the second F1- site, F1- is bonded to two equivalent Li1+ and two Fe2+ atoms to form corner-sharing FLi2Fe2 tetrahedra. In the third F1- site, F1- is bonded in a 4-coordinate geometry to two equivalent Li1+ and two Fe2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFeF3 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 LiFeF3 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 LiFeF3 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↗