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Materials Data on LiCo3(SiO4)2 by Materials Project

LiCo3(SiO4)2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.97–2.42 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form distorted LiO4 trigonal pyramids that share corners with four CoO4 tetrahedra and corners with four SiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 2.00–2.39 Å. In the third Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four CoO4 tetrahedra and corners with four SiO4 tetrahedra. There are a spread of Li–O bond distances ranging from 2.04–2.21 Å. There are nine inequivalent Co+2.33+ sites. In the first Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with two equivalent LiO4 tetrahedra, corners with two CoO4 tetrahedra, and corners with four SiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.93–2.02 Å. In the second Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four CoO4 tetrahedra and corners with four SiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.96–1.99 Å. In the third Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share a cornercorner with one LiO4 tetrahedra, corners with three CoO4 tetrahedra, and corners with four SiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.89–1.99 Å. In the fourth Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with two CoO4 tetrahedra and corners with four SiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.87–2.00 Å. In the fifth Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with two CoO4 tetrahedra, corners with four SiO4 tetrahedra, and corners with two equivalent LiO4 trigonal pyramids. There are a spread of Co–O bond distances ranging from 1.90–2.02 Å. In the sixth Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four CoO4 tetrahedra and corners with four SiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.94–2.03 Å. In the seventh Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with four CoO4 tetrahedra and corners with four SiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.96–2.03 Å. In the eighth Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share a cornercorner with one LiO4 tetrahedra, a cornercorner with one CoO4 tetrahedra, and corners with four SiO4 tetrahedra. There are a spread of Co–O bond distances ranging from 1.86–1.95 Å. In the ninth Co+2.33+ site, Co+2.33+ is bonded to four O2- atoms to form CoO4 tetrahedra that share corners with two CoO4 tetrahedra, corners with four SiO4 tetrahedra, and corners with two equivalent LiO4 trigonal pyramids. There are a spread of Co–O bond distances ranging from 1.91–2.05 Å. There are six inequivalent Si4+ sites. In the first Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share corners with six CoO4 tetrahedra and corners with two equivalent LiO4 trigonal pyramids. There are a spread of Si–O bond distances ranging from 1.62–1.67 Å. In the second Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share corners with six CoO4 tetrahedra and a cornercorner with one LiO4 trigonal pyramid. There are a spread of Si–O bond distances ranging from 1.64–1.66 Å. In the third Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share corners with two equivalent LiO4 tetrahedra and corners with six CoO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.63–1.67 Å. In the fourth Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share corners with six CoO4 tetrahedra and a cornercorner with one LiO4 trigonal pyramid. There are a spread of Si–O bond distances ranging from 1.63–1.67 Å. In the fifth Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one LiO4 tetrahedra and corners with five CoO4 tetrahedra. There are a spread of Si–O bond distances ranging from 1.63–1.66 Å. In the sixth Si4+ site, Si4+ is bonded to four O2- atoms to form SiO4 tetrahedra that share a cornercorner with one LiO4 tetrahedra and corners with seven CoO4 tetrahedra. There is two shorter (1.64 Å) and two longer (1.65 Å) Si–O bond length. There are twenty-four inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the second O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the third O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the fourth O2- site, O2- is bonded in a trigonal non-coplanar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the fifth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the seventh O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the eighth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the ninth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the tenth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the eleventh O2- site, O2- is bonded in a distorted trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the twelfth O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the thirteenth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the fourteenth O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the fifteenth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the sixteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to two Co+2.33+ and one Si4+ atom. In the seventeenth O2- site, O2- is bonded in a trigonal non-coplanar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the eighteenth O2- site, O2- is bonded in a trigonal non-coplanar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the nineteenth O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the twentieth O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the twenty-first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Li1+, one Co+2.33+, and one Si4+ atom. In the twenty-second O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the twenty-third O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom. In the twenty-fourth O2- site, O2- is bonded in a trigonal planar geometry to two Co+2.33+ and one Si4+ atom.

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Materials Data on Li2CoSiO4 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 LiCoSiO4 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 Li2Co(Si2O5)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 Li2CoSiO4 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 Li3Co2(SiO4)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↗