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Materials Data on Li2AlCoO4 by Materials Project

Li2CoAlO4 is Theoretical Carbon Structure-derived structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with two equivalent CoO4 tetrahedra, corners with four equivalent LiO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, and an edgeedge with one CoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.13 Å. Co3+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, and edges with two equivalent LiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.86–1.90 Å. Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with four equivalent CoO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. There are a spread of Al–O bond distances ranging from 1.77–1.79 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Li1+, one Co3+, and one Al3+ atom to form a mixture of distorted edge and corner-sharing OLi2AlCo tetrahedra. In the second O2- site, O2- is bonded to two equivalent Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra. In the third O2- site, O2- is bonded to two equivalent Li1+, one Co3+, and one Al3+ atom to form a mixture of edge and corner-sharing OLi2AlCo trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Li2AlCoO4 by Materials Project

Li2CoAlO4 is Stannite-like structured and crystallizes in the orthorhombic Pna2_1 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent CoO4 tetrahedra, and corners with four equivalent AlO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.02 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent CoO4 tetrahedra, and corners with four equivalent AlO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.99–2.02 Å. Co3+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four equivalent AlO4 tetrahedra and corners with eight LiO4 tetrahedra. There is three shorter (1.88 Å) and one longer (1.89 Å) Co–O bond length. Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with four equivalent CoO4 tetrahedra and corners with eight LiO4 tetrahedra. All Al–O bond lengths are 1.78 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra. In the second O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra. In the third O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra. In the fourth O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li2AlCoO4 by Materials Project

Li2CoAlO4 is beta beryllia-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent CoO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Li–O bond distances ranging from 1.96–2.05 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form distorted LiO4 trigonal pyramids that share corners with two equivalent LiO4 tetrahedra, corners with two equivalent AlO4 tetrahedra, corners with four equivalent CoO4 tetrahedra, an edgeedge with one LiO4 tetrahedra, and an edgeedge with one AlO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.22 Å. Co3+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, and corners with four equivalent LiO4 trigonal pyramids. There are a spread of Co–O bond distances ranging from 1.85–1.89 Å. Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent CoO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, and an edgeedge with one LiO4 trigonal pyramid. There is two shorter (1.78 Å) and two longer (1.79 Å) Al–O bond length. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form a mixture of corner and edge-sharing OLi2AlCo tetrahedra. In the second O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form a mixture of corner and edge-sharing OLi2AlCo tetrahedra. In the third O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form a mixture of distorted corner and edge-sharing OLi2AlCo trigonal pyramids. In the fourth O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li2AlCoO4 by Materials Project

Li2CoAlO4 is beta beryllia-derived structured and crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent CoO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Li–O bond distances ranging from 1.96–2.06 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 trigonal pyramids that share corners with two equivalent LiO4 tetrahedra, corners with two equivalent CoO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, an edgeedge with one LiO4 tetrahedra, and an edgeedge with one CoO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.97–2.13 Å. Co3+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Co–O bond distances ranging from 1.86–1.90 Å. Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent CoO4 tetrahedra, and corners with four equivalent LiO4 trigonal pyramids. There is three shorter (1.78 Å) and one longer (1.79 Å) Al–O bond length. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form a mixture of edge and corner-sharing OLi2AlCo tetrahedra. In the second O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form a mixture of edge and corner-sharing OLi2AlCo tetrahedra. In the third O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form a mixture of distorted edge and corner-sharing OLi2AlCo trigonal pyramids. In the fourth O2- site, O2- is bonded to two Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li2AlCoO4 by Materials Project

Li2CoAlO4 is alpha Po-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with three equivalent CoO6 octahedra, corners with three equivalent AlO6 octahedra, edges with three equivalent CoO6 octahedra, edges with three equivalent AlO6 octahedra, and edges with six equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 3–9°. There are a spread of Li–O bond distances ranging from 2.12–2.17 Å. Co3+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with two equivalent CoO6 octahedra, edges with four equivalent AlO6 octahedra, and edges with six equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 7–9°. There are four shorter (2.00 Å) and two longer (2.03 Å) Co–O bond lengths. Al3+ is bonded to six O2- atoms to form AlO6 octahedra that share corners with six equivalent LiO6 octahedra, edges with two equivalent AlO6 octahedra, edges with four equivalent CoO6 octahedra, and edges with six equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 3–6°. There is four shorter (1.94 Å) and two longer (1.95 Å) Al–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to three equivalent Li1+, two equivalent Co3+, and one Al3+ atom to form a mixture of edge and corner-sharing OLi3AlCo2 octahedra. The corner-sharing octahedra tilt angles range from 0–4°. In the second O2- site, O2- is bonded to three equivalent Li1+, one Co3+, and two equivalent Al3+ atoms to form a mixture of edge and corner-sharing OLi3Al2Co octahedra. The corner-sharing octahedra tilt angles range from 0–4°.

36 MATERIALS SCIENCE↗

Materials Data on Li2AlCoO4 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 Li2AlCoO4 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 Li2AlCoO4 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 Li2AlCoO4 by Materials Project

Li2CoAlO4 is Stannite-like structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with two equivalent LiO4 tetrahedra, corners with four equivalent CoO4 tetrahedra, corners with four equivalent AlO4 tetrahedra, and an edgeedge with one LiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.96–2.04 Å. Co3+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four equivalent AlO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. There is two shorter (1.87 Å) and two longer (1.90 Å) Co–O bond length. Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with four equivalent CoO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. All Al–O bond lengths are 1.79 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Li1+, one Co3+, and one Al3+ atom to form a mixture of distorted corner and edge-sharing OLi2AlCo tetrahedra. In the second O2- site, O2- is bonded to two equivalent Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra. In the third O2- site, O2- is bonded to two equivalent Li1+, one Co3+, and one Al3+ atom to form corner-sharing OLi2AlCo tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li2AlCoO4 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 Li2AlCoO4 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 Li2AlCoO4 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↗