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Materials Data on Li4FeTe2WO12 by Materials Project

Li4WFeTe2O12 is Ilmenite-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Li–O bond distances ranging from 1.97–2.52 Å. In the second Li1+ site, Li1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Li–O bond distances ranging from 1.95–2.52 Å. In the third Li1+ site, Li1+ is bonded in a distorted trigonal planar geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.94–2.62 Å. In the fourth Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share a cornercorner with one FeO6 octahedra, corners with two equivalent WO6 octahedra, edges with three TeO6 octahedra, and a faceface with one FeO6 octahedra. The corner-sharing octahedra tilt angles range from 55–65°. There are a spread of Li–O bond distances ranging from 2.04–2.23 Å. W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with two equivalent LiO6 octahedra and corners with six TeO6 octahedra. The corner-sharing octahedra tilt angles range from 39–58°. There are a spread of W–O bond distances ranging from 1.90–2.02 Å. Fe2+ is bonded to six O2- atoms to form FeO6 octahedra that share a cornercorner with one LiO6 octahedra, corners with six TeO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 36–65°. There are a spread of Fe–O bond distances ranging from 1.99–2.12 Å. There are two inequivalent Te6+ sites. In the first Te6+ site, Te6+ is bonded to six O2- atoms to form TeO6 octahedra that share corners with two equivalent WO6 octahedra, corners with four equivalent FeO6 octahedra, and edges with two equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 36–40°. There are a spread of Te–O bond distances ranging from 1.91–2.08 Å. In the second Te6+ site, Te6+ is bonded to six O2- atoms to form TeO6 octahedra that share corners with two equivalent FeO6 octahedra, corners with four equivalent WO6 octahedra, and an edgeedge with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 38–44°. There are a spread of Te–O bond distances ranging from 1.96–2.18 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+, one Fe2+, and one Te6+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one W6+, and one Te6+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one W6+, and one Te6+ atom. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one Fe2+, and one Te6+ atom. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one W6+, and one Te6+ atom. In the sixth O2- site, O2- is bonded to two Li1+, one Fe2+, and one Te6+ atom to form distorted corner-sharing OLi2FeTe tetrahedra. In the seventh O2- site, O2- is bonded in a distorted see-saw-like geometry to two Li1+, one Fe2+, and one Te6+ atom. In the eighth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one W6+, and one Te6+ atom. In the ninth O2- site, O2- is bonded to two Li1+, one Fe2+, and one Te6+ atom to form distorted corner-sharing OLi2FeTe tetrahedra. In the tenth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one W6+, and one Te6+ atom. In the eleventh O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one W6+, and one Te6+ atom. In the twelfth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one Fe2+, and one Te6+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li4FeTe(WO6)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 Li4FeTe(WO6)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 Li4FeTe(WO6)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 Li4Fe2TeWO12 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 Li4FeTe(WO6)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 Li4FeTe(WO6)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↗