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Materials Data on Li8(CoO2)5 by Materials Project

Li8(CoO2)5 crystallizes in the triclinic P1 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 1.94–2.09 Å. In the second 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 1.95–2.08 Å. In the third 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 1.96–2.09 Å. In the fourth 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 1.91–2.03 Å. In the fifth Li1+ site, Li1+ is bonded to four O2- atoms to form a mixture of distorted edge and corner-sharing LiO4 tetrahedra. There is three shorter (1.95 Å) and one longer (2.03 Å) Li–O bond length. In the sixth 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 1.92–2.22 Å. In the seventh 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 1.90–2.10 Å. In the eighth 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 1.94–2.19 Å. There are five inequivalent Co+2.40+ sites. In the first Co+2.40+ site, Co+2.40+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Co–O bond distances ranging from 1.92–2.02 Å. In the second Co+2.40+ site, Co+2.40+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Co–O bond distances ranging from 1.87–2.02 Å. In the third Co+2.40+ site, Co+2.40+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Co–O bond distances ranging from 1.90–1.96 Å. In the fourth Co+2.40+ site, Co+2.40+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Co–O bond distances ranging from 1.82–1.90 Å. In the fifth Co+2.40+ site, Co+2.40+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Co–O bond distances ranging from 1.96–2.04 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 Co+2.40+ atoms. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Co+2.40+ atoms. In the third O2- site, O2- is bonded to four Li1+ and two Co+2.40+ atoms to form distorted OLi4Co2 octahedra that share corners with three OLi4Co2 octahedra, a cornercorner with one OLi3Co2 trigonal bipyramid, edges with two equivalent OLi4Co2 octahedra, and edges with four OLi3Co2 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 3–46°. In the fourth O2- site, O2- is bonded to three Li1+ and two Co+2.40+ atoms to form OLi3Co2 trigonal bipyramids that share corners with four OLi3Co2 trigonal bipyramids and edges with four OLi4Co2 octahedra. In the fifth O2- site, O2- is bonded to four Li1+ and two Co+2.40+ atoms to form distorted OLi4Co2 octahedra that share corners with two equivalent OLi4Co2 octahedra, a cornercorner with one OLi3Co2 trigonal bipyramid, edges with three equivalent OLi4Co2 octahedra, and edges with three OLi3Co2 trigonal bipyramids. The corner-sharing octahedral tilt angles are 45°. In the sixth O2- site, O2- is bonded to three Li1+ and two Co+2.40+ atoms to form OLi3Co2 trigonal bipyramids that share corners with two OLi4Co2 octahedra, corners with three OLi3Co2 trigonal bipyramids, and edges with three OLi4Co2 octahedra. The corner-sharing octahedra tilt angles range from 1–5°. In the seventh O2- site, O2- is bonded to three Li1+ and two Co+2.40+ atoms to form OLi3Co2 trigonal bipyramids that share corners with two OLi4Co2 octahedra, corners with three OLi3Co2 trigonal bipyramids, and edges with three OLi4Co2 octahedra. The corner-sharing octahedra tilt angles range from 0–4°. In the eighth O2- site, O2- is bonded to three Li1+ and two Co+2.40+ atoms to form OLi3Co2 trigonal bipyramids that share corners with four OLi3Co2 trigonal bipyramids and edges with four OLi4Co2 octahedra. In the ninth O2- site, O2- is bonded to four Li1+ and two Co+2.40+ atoms to form distorted OLi4Co2 octahedra that share corners with three OLi4Co2 octahedra, a cornercorner with one OLi3Co2 trigonal bipyramid, edges with two equivalent OLi4Co2 octahedra, and edges with four OLi3Co2 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 3–44°. In the tenth O2- site, O2- is bonded to four Li1+ and two Co+2.40+ atoms to form distorted OLi4Co2 octahedra that share corners with two equivalent OLi4Co2 octahedra, a cornercorner with one OLi3Co2 trigonal bipyramid, edges with three equivalent OLi4Co2 octahedra, and edges with three OLi3Co2 trigonal bipyramids. The corner-sharing octahedral tilt angles are 45°.

36 MATERIALS SCIENCE↗

Materials Data on Li8(CoO2)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(CoO2)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(CoO2)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(CoO2)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(CoO2)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(CoO2)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↗