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Materials Data on Li3(FeO3)2 by Materials Project

Li3(FeO3)2 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are two inequivalent Li sites. In the first Li site, Li is bonded to six O atoms to form LiO6 octahedra that share corners with four FeO6 octahedra, edges with four FeO6 octahedra, and edges with six equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 12–13°. There are a spread of Li–O bond distances ranging from 1.95–2.23 Å. In the second Li site, Li is bonded to six O atoms to form distorted LiO6 octahedra that share corners with four FeO6 octahedra, edges with four FeO6 octahedra, and edges with six LiO6 octahedra. The corner-sharing octahedra tilt angles range from 12–15°. There are a spread of Li–O bond distances ranging from 2.01–2.34 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six LiO6 octahedra, edges with three equivalent FeO6 octahedra, and edges with six LiO6 octahedra. The corner-sharing octahedra tilt angles range from 12–14°. There is four shorter (1.92 Å) and two longer (1.94 Å) Fe–O bond length. In the second Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six LiO6 octahedra, edges with three equivalent FeO6 octahedra, and edges with six LiO6 octahedra. The corner-sharing octahedra tilt angles range from 12–15°. There is four shorter (1.94 Å) and two longer (1.97 Å) Fe–O bond length. There are three inequivalent O sites. In the first O site, O is bonded to three Li and two Fe atoms to form a mixture of edge and corner-sharing OLi3Fe2 square pyramids. In the second O site, O is bonded to three Li and two Fe atoms to form a mixture of edge and corner-sharing OLi3Fe2 square pyramids. In the third O site, O is bonded to three Li and two Fe atoms to form a mixture of edge and corner-sharing OLi3Fe2 square pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Li3(FeO3)2 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 Li3(FeO3)2 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 Li3(FeO3)2 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↗