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Materials Data on In2(WO4)3 by Materials Project

In2(WO4)3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are six inequivalent W6+ sites. In the first W6+ site, W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with four InO6 octahedra. The corner-sharing octahedra tilt angles range from 19–40°. There are a spread of W–O bond distances ranging from 1.80–1.82 Å. In the second W6+ site, W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with four InO6 octahedra. The corner-sharing octahedra tilt angles range from 22–46°. There are a spread of W–O bond distances ranging from 1.81–1.83 Å. In the third W6+ site, W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with four InO6 octahedra. The corner-sharing octahedra tilt angles range from 12–39°. There are a spread of W–O bond distances ranging from 1.80–1.82 Å. In the fourth W6+ site, W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with four InO6 octahedra. The corner-sharing octahedra tilt angles range from 18–44°. There is two shorter (1.81 Å) and two longer (1.82 Å) W–O bond length. In the fifth W6+ site, W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with four InO6 octahedra. The corner-sharing octahedra tilt angles range from 13–43°. There is one shorter (1.80 Å) and three longer (1.82 Å) W–O bond length. In the sixth W6+ site, W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with four InO6 octahedra. The corner-sharing octahedra tilt angles range from 14–34°. There is three shorter (1.81 Å) and one longer (1.82 Å) W–O bond length. There are four inequivalent In3+ sites. In the first In3+ site, In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with six WO4 tetrahedra. There are a spread of In–O bond distances ranging from 2.15–2.19 Å. In the second In3+ site, In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with six WO4 tetrahedra. There are a spread of In–O bond distances ranging from 2.15–2.20 Å. In the third In3+ site, In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with six WO4 tetrahedra. There are a spread of In–O bond distances ranging from 2.13–2.18 Å. In the fourth In3+ site, In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with six WO4 tetrahedra. There are a spread of In–O bond distances ranging from 2.13–2.18 Å. There are twenty-four inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to one W6+ and one In3+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the fourth O2- site, O2- is bonded in a linear geometry to one W6+ and one In3+ atom. In the fifth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the seventh O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the ninth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one W6+ and one In3+ atom. In the tenth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one W6+ and one In3+ atom. In the eleventh O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the twelfth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the thirteenth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one W6+ and one In3+ atom. In the fourteenth O2- site, O2- is bonded in a linear geometry to one W6+ and one In3+ atom. In the fifteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the sixteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the seventeenth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the eighteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the nineteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the twentieth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one W6+ and one In3+ atom. In the twenty-first O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the twenty-second O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom. In the twenty-third O2- site, O2- is bonded in a linear geometry to one W6+ and one In3+ atom. In the twenty-fourth O2- site, O2- is bonded in a bent 150 degrees geometry to one W6+ and one In3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on In2WO6 by Materials Project

WIn2O6 crystallizes in the orthorhombic Pbca space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form WO6 octahedra that share corners with two equivalent WO6 octahedra, corners with three equivalent InO7 pentagonal bipyramids, and an edgeedge with one InO7 pentagonal bipyramid. The corner-sharing octahedral tilt angles are 51°. There are a spread of W–O bond distances ranging from 1.82–2.17 Å. There are two inequivalent In3+ sites. In the first In3+ site, In3+ is bonded to seven O2- atoms to form distorted InO7 pentagonal bipyramids that share corners with three equivalent WO6 octahedra, an edgeedge with one WO6 octahedra, and edges with three equivalent InO7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 13–36°. There are a spread of In–O bond distances ranging from 2.19–2.37 Å. In the second In3+ site, In3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of In–O bond distances ranging from 2.17–2.58 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent W6+ and two equivalent In3+ atoms to form distorted OIn2W2 trigonal pyramids that share corners with two equivalent OIn4 tetrahedra, an edgeedge with one OIn4 tetrahedra, and edges with two equivalent OIn2W2 trigonal pyramids. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one W6+ and two equivalent In3+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one W6+ and two equivalent In3+ atoms. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one W6+ and two equivalent In3+ atoms. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to one W6+ and two In3+ atoms. In the sixth O2- site, O2- is bonded to four In3+ atoms to form OIn4 tetrahedra that share corners with two equivalent OIn2W2 trigonal pyramids, edges with two equivalent OIn4 tetrahedra, and an edgeedge with one OIn2W2 trigonal pyramid.

36 MATERIALS SCIENCE↗

Materials Data on In2(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↗

Materials Data on In2WO6 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 In2WO6 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 In6WO12 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 In2WO6 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↗