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Materials Data on Te3WO12 by Materials Project

WTe3O12 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with six TeO6 octahedra. The corner-sharing octahedra tilt angles range from 35–36°. There is four shorter (1.93 Å) and two longer (1.94 Å) W–O bond length. There are three 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 and corners with four equivalent TeO6 octahedra. The corner-sharing octahedra tilt angles range from 36–40°. There are a spread of Te–O bond distances ranging from 1.93–1.96 Å. In the second Te6+ site, Te6+ is bonded to six O2- atoms to form TeO6 octahedra that share corners with two equivalent TeO6 octahedra and corners with four equivalent WO6 octahedra. The corner-sharing octahedra tilt angles range from 35–40°. There are a spread of Te–O bond distances ranging from 1.92–1.96 Å. In the third Te6+ site, Te6+ is bonded to six O2- atoms to form corner-sharing TeO6 octahedra. The corner-sharing octahedral tilt angles are 40°. There is two shorter (1.95 Å) and four longer (1.96 Å) Te–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to two Te6+ atoms. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one Te6+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one Te6+ atom. In the fourth O2- site, O2- is bonded in a bent 150 degrees geometry to two Te6+ atoms. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one Te6+ atom. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to two Te6+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on TeWO6 by Materials Project

WTeO6 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with six equivalent TeO6 octahedra. The corner-sharing octahedral tilt angles are 31°. There is two shorter (1.93 Å) and four longer (1.94 Å) W–O bond length. Te6+ is bonded to six O2- atoms to form TeO6 octahedra that share corners with six equivalent WO6 octahedra. The corner-sharing octahedral tilt angles are 31°. There is two shorter (1.92 Å) and four longer (1.93 Å) Te–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one Te6+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one Te6+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one Te6+ atom.

36 MATERIALS SCIENCE↗

Materials Data on TeWO6 by Materials Project

WTeO6 is High-temperature superconductor-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with six equivalent TeO6 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. All W–O bond lengths are 1.92 Å. Te6+ is bonded to six O2- atoms to form TeO6 octahedra that share corners with six equivalent WO6 octahedra. The corner-sharing octahedra tilt angles range from 0–1°. All Te–O bond lengths are 1.91 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to one W6+ and one Te6+ atom. In the second O2- site, O2- is bonded in a linear geometry to one W6+ and one Te6+ atom. In the third O2- site, O2- is bonded in a linear geometry to one W6+ and one Te6+ atom. In the fourth O2- site, O2- is bonded in a linear geometry to one W6+ and one Te6+ atom. In the fifth O2- site, O2- is bonded in a linear geometry to one W6+ and one Te6+ atom. In the sixth O2- site, O2- is bonded in a linear geometry to one W6+ and one Te6+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Te(WO4)3 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↗