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Materials Data on LiFe2O2F3 by Materials Project

LiFe2O2F3 crystallizes in the monoclinic C2/m 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 1.94–2.40 Å. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to five O2- and one F1- atom to form a mixture of distorted corner and edge-sharing FeO5F octahedra. The corner-sharing octahedra tilt angles range from 21–39°. There are a spread of Fe–O bond distances ranging from 1.95–2.12 Å. The Fe–F bond length is 2.38 Å. In the second Fe3+ site, Fe3+ is bonded to two O2- and four F1- atoms to form a mixture of distorted corner and edge-sharing FeO2F4 octahedra. The corner-sharing octahedra tilt angles range from 21–33°. There are one shorter (1.93 Å) and one longer (2.11 Å) Fe–O bond lengths. There are a spread of Fe–F bond distances ranging from 1.93–2.01 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted T-shaped geometry to three Fe3+ atoms. In the second O2- site, O2- is bonded to four Fe3+ atoms to form distorted OFe4 trigonal pyramids that share a cornercorner with one FLi3Fe trigonal pyramid, corners with two equivalent OFe4 trigonal pyramids, and edges with two equivalent OFe4 trigonal pyramids. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted T-shaped geometry to two equivalent Li1+ and one Fe3+ atom. In the second F1- site, F1- is bonded to three equivalent Li1+ and one Fe3+ atom to form distorted FLi3Fe trigonal pyramids that share a cornercorner with one OFe4 trigonal pyramid, corners with two equivalent FLi3Fe trigonal pyramids, and edges with two equivalent FLi3Fe trigonal pyramids. In the third F1- site, F1- is bonded in a 4-coordinate geometry to one Li1+ and three Fe3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiFe2O2F3 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 LiFe2O2F3 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 LiFe2O2F3 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↗