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Materials Data on CoO2 by Materials Project

Lix0CoO2 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are twelve inequivalent Co4+ sites. In the first Co4+ site, Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with three CoO4 tetrahedra and edges with four CoO6 octahedra. There are a spread of Co–O bond distances ranging from 1.80–1.97 Å. In the second Co4+ site, Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with three equivalent CoO4 tetrahedra and edges with four CoO6 octahedra. There are a spread of Co–O bond distances ranging from 1.80–1.97 Å. In the third Co4+ site, Co4+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. The corner-sharing octahedra tilt angles range from 50–57°. There are a spread of Co–O bond distances ranging from 1.74–1.91 Å. In the fourth Co4+ site, Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with four CoO4 tetrahedra and edges with three CoO6 octahedra. There are a spread of Co–O bond distances ranging from 1.82–1.91 Å. In the fifth Co4+ site, Co4+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. The corner-sharing octahedra tilt angles range from 55–59°. There are a spread of Co–O bond distances ranging from 1.84–1.91 Å. In the sixth Co4+ site, Co4+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. The corner-sharing octahedra tilt angles range from 50–56°. There are a spread of Co–O bond distances ranging from 1.74–1.90 Å. In the seventh Co4+ site, Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with six CoO4 tetrahedra and edges with two equivalent CoO6 octahedra. There are a spread of Co–O bond distances ranging from 1.84–1.91 Å. In the eighth Co4+ site, Co4+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. The corner-sharing octahedra tilt angles range from 51–56°. There are a spread of Co–O bond distances ranging from 1.75–1.90 Å. In the ninth Co4+ site, Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with five CoO4 tetrahedra and edges with three CoO6 octahedra. There are a spread of Co–O bond distances ranging from 1.81–1.97 Å. In the tenth Co4+ site, Co4+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. The corner-sharing octahedra tilt angles range from 50–57°. There are a spread of Co–O bond distances ranging from 1.75–1.91 Å. In the eleventh Co4+ site, Co4+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with three equivalent CoO4 tetrahedra and edges with four CoO6 octahedra. There are a spread of Co–O bond distances ranging from 1.80–1.97 Å. In the twelfth Co4+ site, Co4+ is bonded to four O2- atoms to form corner-sharing CoO4 tetrahedra. The corner-sharing octahedra tilt angles range from 53–60°. There are a spread of Co–O bond distances ranging from 1.83–1.94 Å. There are twenty-four inequivalent O2- sites. In the first O2- site, O2- is bonded in a water-like geometry to two Co4+ atoms. In the second O2- site, O2- is bonded in a water-like geometry to two equivalent Co4+ atoms. In the third O2- site, O2- is bonded in a distorted T-shaped geometry to three Co4+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to four Co4+ atoms. In the fifth O2- site, O2- is bonded in a water-like geometry to two Co4+ atoms. In the sixth O2- site, O2- is bonded in a trigonal planar geometry to three Co4+ atoms. In the seventh O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the eighth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the ninth O2- site, O2- is bonded in a distorted T-shaped geometry to three Co4+ atoms. In the tenth O2- site, O2- is bonded in a bent 120 degrees geometry to two Co4+ atoms. In the eleventh O2- site, O2- is bonded in a trigonal planar geometry to three Co4+ atoms. In the twelfth O2- site, O2- is bonded in a bent 120 degrees geometry to two Co4+ atoms. In the thirteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the fourteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the fifteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the sixteenth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the seventeenth O2- site, O2- is bonded in a bent 120 degrees geometry to two Co4+ atoms. In the eighteenth O2- site, O2- is bonded in a bent 120 degrees geometry to two Co4+ atoms. In the nineteenth O2- site, O2- is bonded in a water-like geometry to two equivalent Co4+ atoms. In the twentieth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the twenty-first O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms. In the twenty-second O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to four Co4+ atoms. In the twenty-third O2- site, O2- is bonded in a trigonal planar geometry to three Co4+ atoms. In the twenty-fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Co4+ atoms.

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Materials Data on Zn(CoO2)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

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Materials Data on Zn(CoO2)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 CoO2 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 Ca(CoO2)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 Li3Nb(CoO2)4 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 CoO2 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 CoO2 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 Na2(CoO2)3 by Materials Project

(Na2Co3O5)2O2 crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional and consists of two hydrogen peroxide molecules and one Na2Co3O5 framework. In the Na2Co3O5 framework, there are three inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a 4-coordinate geometry to four equivalent O2- atoms. All Na–O bond lengths are 2.29 Å. In the second Na1+ site, Na1+ is bonded in a 4-coordinate geometry to four equivalent O2- atoms. All Na–O bond lengths are 2.52 Å. In the third Na1+ site, Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.39–2.83 Å. There are two inequivalent Co+3.33+ sites. In the first Co+3.33+ site, Co+3.33+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of Co–O bond distances ranging from 1.79–1.82 Å. In the second Co+3.33+ site, Co+3.33+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There is two shorter (1.85 Å) and two longer (1.86 Å) Co–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Na1+ and two Co+3.33+ atoms. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Na1+ and two Co+3.33+ atoms. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two equivalent Na1+ and two equivalent Co+3.33+ atoms.

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Materials Data on Al(CoO2)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 Li(CoO2)4 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(CoO2)4 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 CoO2 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 Li3Fe(CoO2)4 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 Li(CoO2)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 Mn(CoO2)2 by Materials Project

MnCo2O4 is Spinel structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Mn2+ is bonded to four equivalent O2- atoms to form MnO4 tetrahedra that share corners with twelve equivalent CoO6 octahedra. The corner-sharing octahedral tilt angles are 59°. All Mn–O bond lengths are 2.03 Å. Co3+ is bonded to six equivalent O2- atoms to form CoO6 octahedra that share corners with six equivalent MnO4 tetrahedra and edges with six equivalent CoO6 octahedra. All Co–O bond lengths are 2.04 Å. O2- is bonded to one Mn2+ and three equivalent Co3+ atoms to form a mixture of distorted edge and corner-sharing OMnCo3 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Li3Cr(CoO2)4 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

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