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Materials Data on Li47(NiO4)8 by Materials Project

Li47(NiO4)8 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are forty-seven inequivalent Li sites. In the first Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.95–2.10 Å. In the second Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.10 Å. In the third Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with five LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.08 Å. In the fourth Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with five LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.94–2.03 Å. In the fifth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.99–2.07 Å. In the sixth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.11 Å. In the seventh Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with four NiO4 tetrahedra, corners with nine LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, and edges with five LiO4 tetrahedra. There are one shorter (2.02 Å) and three longer (2.03 Å) Li–O bond lengths. In the eighth Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with four NiO4 tetrahedra, corners with eight LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.93–2.13 Å. In the ninth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, edges with three LiO4 tetrahedra, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Li–O bond distances ranging from 1.97–2.03 Å. In the tenth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.93–2.05 Å. In the eleventh Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 2.01–2.06 Å. In the twelfth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.07 Å. In the thirteenth Li site, Li is bonded in a 4-coordinate geometry to four O atoms. There are a spread of Li–O bond distances ranging from 1.99–2.12 Å. In the fourteenth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.06 Å. In the fifteenth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.09 Å. In the sixteenth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.06 Å. In the seventeenth Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with four NiO4 tetrahedra, corners with ten LiO4 tetrahedra, and edges with five LiO4 tetrahedra. There are three shorter (2.01 Å) and one longer (2.03 Å) Li–O bond lengths. In the eighteenth Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with four NiO4 tetrahedra, corners with ten LiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are one shorter (2.01 Å) and three longer (2.02 Å) Li–O bond lengths. In the nineteenth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.05 Å. In the twentieth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with three LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.99–2.07 Å. In the twenty-first Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with nine LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with five LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.95–2.01 Å. In the twenty-second Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.95–2.01 Å. In the twenty-third Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.08 Å. In the twenty-fourth Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.06 Å. In the twenty-fifth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one NiO4 tetrahedra, and edges with three LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.92–2.14 Å. In the twenty-sixth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 2.00–2.10 Å. In the twenty-seventh Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with nine LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with five LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.02 Å. In the twenty-eighth Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with nine LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one NiO4 tetrahedra, and edges with five LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.02 Å. In the twenty-ninth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.93–2.07 Å. In the thirtieth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.05 Å. In the thirty-first Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with four NiO4 tetrahedra, corners with nine LiO4 tetrahedra, and edges with five LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.99–2.07 Å. In the thirty-second Li site, Li is bonded to four O atoms to form LiO4 tetrahedra that share corners with four NiO4 tetrahedra, corners with nine LiO4 tetrahedra, edges with four LiO4 tetrahedra, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Li–O bond distances ranging from 1.99–2.07 Å. In the thirty-third Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.07 Å. In the thirty-fourth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with ten LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one NiO4 tetrahedra, and edges with three LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.92–2.14 Å. In the thirty-fifth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.98–2.08 Å. In the thirty-sixth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, and edges with four LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 2.00–2.07 Å. In the thirty-seventh Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with eleven LiO4 tetrahedra, an edgeedge with one NiO4 tetrahedra, edges with three LiO4 tetrahedra, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Li–O bond distances ranging from 1.93–2.07 Å. In the thirty-eighth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with two NiO4 tetrahedra, corners with twelve LiO4 tetrahedra

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Materials Data on Li7Ni5O12 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 Li17Ni11O28 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 LiNiO3 by Materials Project

LiNiO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Li is bonded to twelve equivalent O atoms to form LiO12 cuboctahedra that share corners with twelve equivalent LiO12 cuboctahedra, faces with six equivalent LiO12 cuboctahedra, and faces with eight equivalent NiO6 octahedra. All Li–O bond lengths are 2.67 Å. Ni is bonded to six equivalent O atoms to form NiO6 octahedra that share corners with six equivalent NiO6 octahedra and faces with eight equivalent LiO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ni–O bond lengths are 1.89 Å. O is bonded in a linear geometry to four equivalent Li and two equivalent Ni atoms.

36 MATERIALS SCIENCE↗

Materials Data on Li5(NiO2)8 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(NiO2)11 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 LiNi3O4 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 Li5NiO4 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 Li5Ni7O12 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 LiNi2O3 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 Li7(NiO2)9 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(NiO2)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 LiNiO2 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 LiNiO2 by Materials Project

LiNiO2 is Caswellsilverite-like structured and crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with nine equivalent NiO6 octahedra, edges with three equivalent NiO6 octahedra, edges with six equivalent LiO6 octahedra, and a faceface with one NiO6 octahedra. The corner-sharing octahedra tilt angles range from 6–50°. There are a spread of Li–O bond distances ranging from 2.06–2.32 Å. Ni3+ is bonded to six O2- atoms to form NiO6 octahedra that share corners with nine equivalent LiO6 octahedra, edges with three equivalent LiO6 octahedra, edges with six equivalent NiO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 6–50°. There are a spread of Ni–O bond distances ranging from 1.91–2.15 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to three equivalent Li1+ and three equivalent Ni3+ atoms to form edge-sharing OLi3Ni3 octahedra. In the second O2- site, O2- is bonded in a 6-coordinate geometry to three equivalent Li1+ and three equivalent Ni3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on LiNi3O4 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 LiNiO2 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 LiNiO2 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 Li12Ni11O28 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↗