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Materials Data on V2SnO7 by Materials Project

V2SnO7 crystallizes in the cubic Pa-3 space group. The structure is three-dimensional. V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with three equivalent SnO6 octahedra and a cornercorner with one VO4 tetrahedra. The corner-sharing octahedral tilt angles are 16°. There is three shorter (1.72 Å) and one longer (1.79 Å) V–O bond length. Sn4+ is bonded to six equivalent O2- atoms to form SnO6 octahedra that share corners with six equivalent VO4 tetrahedra. All Sn–O bond lengths are 2.06 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent V5+ atoms. In the second O2- site, O2- is bonded in a distorted linear geometry to one V5+ and one Sn4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on V3SnO8 by Materials Project

V3SnO8 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are three inequivalent V+4.67+ sites. In the first V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form VO6 octahedra that share a cornercorner with one SnO6 octahedra, corners with two equivalent VO6 octahedra, an edgeedge with one VO6 octahedra, and edges with two equivalent SnO6 octahedra. The corner-sharing octahedra tilt angles range from 26–27°. There are a spread of V–O bond distances ranging from 1.85–2.10 Å. In the second V+4.67+ site, V+4.67+ is bonded to six O2- atoms to form distorted VO6 octahedra that share a cornercorner with one SnO6 octahedra, corners with two equivalent VO6 octahedra, an edgeedge with one VO6 octahedra, and an edgeedge with one SnO6 octahedra. The corner-sharing octahedra tilt angles range from 18–27°. There are a spread of V–O bond distances ranging from 1.74–2.12 Å. In the third V+4.67+ site, V+4.67+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.68–2.38 Å. Sn2+ is bonded to six O2- atoms to form distorted SnO6 octahedra that share corners with two VO6 octahedra, corners with two equivalent SnO6 octahedra, and edges with three VO6 octahedra. The corner-sharing octahedra tilt angles range from 18–34°. There are a spread of Sn–O bond distances ranging from 1.99–2.26 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted T-shaped geometry to three V+4.67+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two V+4.67+ and two equivalent Sn2+ atoms. In the third O2- site, O2- is bonded in a distorted linear geometry to two V+4.67+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three V+4.67+ atoms. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to two V+4.67+ and one Sn2+ atom. In the sixth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one V+4.67+ and one Sn2+ atom. In the seventh O2- site, O2- is bonded to three V+4.67+ and one Sn2+ atom to form distorted corner-sharing OV3Sn trigonal pyramids. In the eighth O2- site, O2- is bonded in a distorted T-shaped geometry to two equivalent V+4.67+ and one Sn2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on VSnO3 by Materials Project

VSnO3 is Orthorhombic Perovskite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. V4+ is bonded in a distorted rectangular see-saw-like geometry to four O2- atoms. There are a spread of V–O bond distances ranging from 2.13–2.28 Å. Sn2+ is bonded to six O2- atoms to form corner-sharing SnO6 octahedra. The corner-sharing octahedra tilt angles range from 43–47°. There are a spread of Sn–O bond distances ranging from 2.09–2.14 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one V4+ and two equivalent Sn2+ atoms. In the second O2- site, O2- is bonded to two equivalent V4+ and two equivalent Sn2+ atoms to form distorted corner-sharing OV2Sn2 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on V4SnO12 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↗