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30 records · Page 2

Materials Data on VCuO3 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 VCuO4 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 V12Cu2O29 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 V2(CuO3)3 by Materials Project

V2(CuO3)3 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are two inequivalent V5+ sites. In the first V5+ site, V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share a cornercorner with one CuO5 square pyramid, a cornercorner with one VO4 tetrahedra, and corners with three equivalent CuO5 trigonal bipyramids. There are a spread of V–O bond distances ranging from 1.67–1.79 Å. In the second V5+ site, V5+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with two equivalent CuO5 square pyramids, a cornercorner with one VO4 tetrahedra, and a cornercorner with one CuO5 trigonal bipyramid. There are a spread of V–O bond distances ranging from 1.70–1.79 Å. There are three inequivalent Cu+2.67+ sites. In the first Cu+2.67+ site, Cu+2.67+ is bonded in a distorted square co-planar geometry to four O2- atoms. There is two shorter (1.89 Å) and two longer (1.94 Å) Cu–O bond length. In the second Cu+2.67+ site, Cu+2.67+ is bonded to five O2- atoms to form distorted CuO5 square pyramids that share corners with three VO4 tetrahedra and an edgeedge with one CuO5 trigonal bipyramid. There are a spread of Cu–O bond distances ranging from 1.77–2.40 Å. In the third Cu+2.67+ site, Cu+2.67+ is bonded to five O2- atoms to form distorted CuO5 trigonal bipyramids that share corners with four VO4 tetrahedra and an edgeedge with one CuO5 square pyramid. There are a spread of Cu–O bond distances ranging from 1.88–2.22 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded to four Cu+2.67+ atoms to form corner-sharing OCu4 tetrahedra. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to one V5+ and two Cu+2.67+ atoms. In the third O2- site, O2- is bonded in a 1-coordinate geometry to one V5+ and two Cu+2.67+ atoms. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to one V5+ and one Cu+2.67+ atom. In the fifth O2- site, O2- is bonded in a linear geometry to one V5+ and one Cu+2.67+ atom. In the sixth O2- site, O2- is bonded in a linear geometry to two V5+ atoms. In the seventh O2- site, O2- is bonded in a single-bond geometry to one Cu+2.67+ atom.

36 MATERIALS SCIENCE↗

Materials Data on V8CuO20 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 V2CuO6 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 V18Cu20O57 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 VCuO3 by Materials Project

CuVO3 crystallizes in the cubic Im-3 space group. The structure is three-dimensional. V5+ is bonded to six equivalent O2- atoms to form VO6 octahedra that share corners with six equivalent VO6 octahedra and faces with two equivalent CuO12 cuboctahedra. The corner-sharing octahedral tilt angles are 38°. All V–O bond lengths are 1.94 Å. There are two inequivalent Cu1+ sites. In the first Cu1+ site, Cu1+ is bonded to twelve equivalent O2- atoms to form CuO12 cuboctahedra that share faces with eight equivalent VO6 octahedra. All Cu–O bond lengths are 2.59 Å. In the second Cu1+ site, Cu1+ is bonded in a square co-planar geometry to four equivalent O2- atoms. All Cu–O bond lengths are 1.96 Å. O2- is bonded in a 3-coordinate geometry to two equivalent V5+ and two Cu1+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on V6Cu2O15 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 V2CuO6 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 V6Cu11O26 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 V6CuO15 by Materials Project

V6CuO15 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are six inequivalent V+4.83+ sites. In the first V+4.83+ site, V+4.83+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of V–O bond distances ranging from 1.62–2.02 Å. In the second V+4.83+ site, V+4.83+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of V–O bond distances ranging from 1.66–2.00 Å. In the third V+4.83+ site, V+4.83+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.64–2.31 Å. In the fourth V+4.83+ site, V+4.83+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.65–2.25 Å. In the fifth V+4.83+ site, V+4.83+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.67–2.19 Å. In the sixth V+4.83+ site, V+4.83+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of V–O bond distances ranging from 1.61–2.34 Å. Cu1+ is bonded in a distorted trigonal bipyramidal geometry to five O2- atoms. There are a spread of Cu–O bond distances ranging from 1.82–2.50 Å. There are sixteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three V+4.83+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three V+4.83+ atoms. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one V+4.83+ and one Cu1+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one V+4.83+ and one Cu1+ atom. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to three V+4.83+ atoms. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to three V+4.83+ atoms. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to one V+4.83+ and one Cu1+ atom. In the eighth O2- site, O2- is bonded in a distorted single-bond geometry to one V+4.83+ and one Cu1+ atom. In the ninth O2- site, O2- is bonded in a linear geometry to two equivalent V+4.83+ atoms. In the tenth O2- site, O2- is bonded in a linear geometry to two equivalent V+4.83+ atoms. In the eleventh O2- site, O2- is bonded in a linear geometry to one V+4.83+ and one Cu1+ atom. In the twelfth O2- site, O2- is bonded in a single-bond geometry to one V+4.83+ atom. In the thirteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three V+4.83+ atoms. In the fourteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three V+4.83+ atoms. In the fifteenth O2- site, O2- is bonded in a 4-coordinate geometry to four V+4.83+ atoms. In the sixteenth O2- site, O2- is bonded in a 4-coordinate geometry to four V+4.83+ atoms.

36 MATERIALS SCIENCE↗