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Materials Data on Li8(FeO2)5 by Materials Project

Li8(FeO2)5 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are eight inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of distorted edge and corner-sharing LiO4 trigonal pyramids. There are a spread of Li–O bond distances ranging from 1.93–2.23 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of distorted edge and corner-sharing LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.07 Å. In the third Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of distorted edge and corner-sharing LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.91–2.03 Å. In the fourth Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of distorted edge and corner-sharing LiO4 trigonal pyramids. There are a spread of Li–O bond distances ranging from 1.95–2.19 Å. In the fifth Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of distorted edge and corner-sharing LiO4 trigonal pyramids. There are a spread of Li–O bond distances ranging from 1.96–2.15 Å. In the sixth Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of edge and corner-sharing LiO4 trigonal pyramids. There are a spread of Li–O bond distances ranging from 1.92–2.06 Å. In the seventh Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of distorted edge and corner-sharing LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.93–2.06 Å. In the eighth Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of edge and corner-sharing LiO4 trigonal pyramids. There are a spread of Li–O bond distances ranging from 1.99–2.05 Å. There are five inequivalent Fe+2.40+ sites. In the first Fe+2.40+ site, Fe+2.40+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Fe–O bond distances ranging from 1.84–1.96 Å. In the second Fe+2.40+ site, Fe+2.40+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Fe–O bond distances ranging from 1.97–2.09 Å. In the third Fe+2.40+ site, Fe+2.40+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Fe–O bond distances ranging from 1.98–2.07 Å. In the fourth Fe+2.40+ site, Fe+2.40+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Fe–O bond distances ranging from 1.96–2.05 Å. In the fifth Fe+2.40+ site, Fe+2.40+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Fe–O bond distances ranging from 1.86–1.93 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Fe+2.40+ atoms. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Fe+2.40+ atoms. In the third O2- site, O2- is bonded to three Li1+ and two Fe+2.40+ atoms to form distorted OLi3Fe2 trigonal bipyramids that share corners with four OLi3Fe2 trigonal bipyramids and edges with four OLi4Fe2 octahedra. In the fourth O2- site, O2- is bonded to four Li1+ and two Fe+2.40+ atoms to form distorted OLi4Fe2 octahedra that share corners with three OLi4Fe2 octahedra, a cornercorner with one OLi3Fe2 trigonal bipyramid, edges with two equivalent OLi4Fe2 octahedra, and edges with four OLi3Fe2 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 5–41°. In the fifth O2- site, O2- is bonded to three Li1+ and two Fe+2.40+ atoms to form OLi3Fe2 trigonal bipyramids that share corners with two OLi4Fe2 octahedra, corners with three OLi3Fe2 trigonal bipyramids, and edges with three OLi4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–2°. In the sixth O2- site, O2- is bonded to four Li1+ and two Fe+2.40+ atoms to form distorted OLi4Fe2 octahedra that share corners with two equivalent OLi4Fe2 octahedra, a cornercorner with one OLi3Fe2 trigonal bipyramid, edges with three equivalent OLi4Fe2 octahedra, and edges with three OLi3Fe2 trigonal bipyramids. The corner-sharing octahedral tilt angles are 45°. In the seventh O2- site, O2- is bonded to three Li1+ and two Fe+2.40+ atoms to form OLi3Fe2 trigonal bipyramids that share corners with four OLi3Fe2 trigonal bipyramids and edges with four OLi4Fe2 octahedra. In the eighth O2- site, O2- is bonded to three Li1+ and two Fe+2.40+ atoms to form OLi3Fe2 trigonal bipyramids that share corners with two OLi4Fe2 octahedra, corners with three OLi3Fe2 trigonal bipyramids, and edges with three OLi4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 1–7°. In the ninth O2- site, O2- is bonded to four Li1+ and two Fe+2.40+ atoms to form distorted OLi4Fe2 octahedra that share corners with three OLi4Fe2 octahedra, a cornercorner with one OLi3Fe2 trigonal bipyramid, edges with two equivalent OLi4Fe2 octahedra, and edges with four OLi3Fe2 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 5–47°. In the tenth O2- site, O2- is bonded to four Li1+ and two Fe+2.40+ atoms to form distorted OLi4Fe2 octahedra that share corners with two equivalent OLi4Fe2 octahedra, a cornercorner with one OLi3Fe2 trigonal bipyramid, edges with three equivalent OLi4Fe2 octahedra, and edges with three OLi3Fe2 trigonal bipyramids. The corner-sharing octahedral tilt angles are 46°.

36 MATERIALS SCIENCE↗

Materials Data on Li8(FeO2)5 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 Li8(FeO2)5 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 Li8(FeO2)5 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↗