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At least 37 records · Page 2

Materials Data on Ca5V3O13 by Materials Project

Ca5V3O13 crystallizes in the hexagonal P6_3 space group. The structure is three-dimensional. there are three inequivalent Ca sites. In the first Ca site, Ca is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Ca–O bond distances ranging from 2.41–2.94 Å. In the second Ca site, Ca is bonded in a 6-coordinate geometry to six O atoms. There are three shorter (2.38 Å) and three longer (2.46 Å) Ca–O bond lengths. In the third Ca site, Ca is bonded to six O atoms to form distorted CaO6 pentagonal pyramids that share corners with six equivalent CaO6 pentagonal pyramids, corners with three equivalent VO4 tetrahedra, and an edgeedge with one VO4 tetrahedra. There are a spread of Ca–O bond distances ranging from 2.34–2.50 Å. V is bonded to four O atoms to form VO4 tetrahedra that share corners with three equivalent CaO6 pentagonal pyramids and an edgeedge with one CaO6 pentagonal pyramid. There are a spread of V–O bond distances ranging from 1.73–1.76 Å. There are five inequivalent O sites. In the first O site, O is bonded to three Ca and one V atom to form distorted edge-sharing OCa3V tetrahedra. In the second O site, O is bonded in a trigonal planar geometry to three equivalent Ca atoms. In the third O site, O is bonded in a 4-coordinate geometry to three Ca and one V atom. In the fourth O site, O is bonded in a 3-coordinate geometry to two equivalent Ca and one V atom. In the fifth O site, O is bonded in a 1-coordinate geometry to two Ca and one V atom.

36 MATERIALS SCIENCE↗

Materials Data on CaV2O4 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 CaV4O6 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 CaVO3 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 CaV5O7 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 CaV5O7 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 Ca2V2O9 by Materials Project

Ca2V2O9 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent Ca sites. In the first Ca site, Ca is bonded in a 6-coordinate geometry to eight O atoms. There are a spread of Ca–O bond distances ranging from 2.33–3.04 Å. In the second Ca site, Ca is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Ca–O bond distances ranging from 2.33–3.00 Å. There are two inequivalent V sites. In the first V site, V is bonded to four O atoms to form corner-sharing VO4 tetrahedra. There are a spread of V–O bond distances ranging from 1.68–1.82 Å. In the second V site, V is bonded to four O atoms to form corner-sharing VO4 tetrahedra. There are a spread of V–O bond distances ranging from 1.71–1.80 Å. There are nine inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to two V atoms. In the second O site, O is bonded in a distorted trigonal non-coplanar geometry to two Ca and one V atom. In the third O site, O is bonded in a bent 150 degrees geometry to one Ca and one V atom. In the fourth O site, O is bonded in a 1-coordinate geometry to three Ca and one V atom. In the fifth O site, O is bonded in a distorted T-shaped geometry to two Ca and one V atom. In the sixth O site, O is bonded in a distorted T-shaped geometry to two Ca and one V atom. In the seventh O site, O is bonded in a 4-coordinate geometry to three Ca and one V atom. In the eighth O site, O is bonded in a bent 120 degrees geometry to one Ca and one O atom. The O–O bond length is 1.23 Å. In the ninth O site, O is bonded in a distorted bent 120 degrees geometry to one Ca and one O atom.

36 MATERIALS SCIENCE↗

Materials Data on Ca3V2O8 by Materials Project

Ca3(VO4)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ca–O bond distances ranging from 2.25–2.93 Å. In the second Ca2+ site, Ca2+ is bonded in a distorted hexagonal planar geometry to six O2- atoms. There are two shorter (2.49 Å) and four longer (2.50 Å) Ca–O bond lengths. V5+ is bonded in a tetrahedral geometry to four O2- atoms. There are a spread of V–O bond distances ranging from 1.71–1.75 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to four Ca2+ and one V5+ atom. In the second O2- site, O2- is bonded in a linear geometry to one Ca2+ and one V5+ atom. In the third O2- site, O2- is bonded in a 1-coordinate geometry to four Ca2+ and one V5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on CaV4O6 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 CaV5O7 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 CaV8O24 by Materials Project

CaV8O22O2 crystallizes in the monoclinic Pm space group. The structure is two-dimensional and consists of two water molecules and one CaV8O22 sheet oriented in the (1, 0, 0) direction. In the CaV8O22 sheet, Ca is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Ca–O bond distances ranging from 2.23–2.37 Å. There are eight inequivalent V sites. In the first V site, V is bonded in a 5-coordinate geometry to five O atoms. There are a spread of V–O bond distances ranging from 1.61–2.03 Å. In the second V site, V is bonded in a 5-coordinate geometry to five O atoms. There are a spread of V–O bond distances ranging from 1.60–2.04 Å. In the third V site, V is bonded in a 5-coordinate geometry to five O atoms. There are a spread of V–O bond distances ranging from 1.60–2.04 Å. In the fourth V site, V is bonded in a 5-coordinate geometry to five O atoms. There are a spread of V–O bond distances ranging from 1.67–2.03 Å. In the fifth V site, V is bonded in a 6-coordinate geometry to six O atoms. There are a spread of V–O bond distances ranging from 1.61–2.57 Å. In the sixth V site, V is bonded in a 6-coordinate geometry to six O atoms. There are a spread of V–O bond distances ranging from 1.61–2.52 Å. In the seventh V site, V is bonded in a 6-coordinate geometry to six O atoms. There are a spread of V–O bond distances ranging from 1.66–2.58 Å. In the eighth V site, V is bonded in a 5-coordinate geometry to five O atoms. There are a spread of V–O bond distances ranging from 1.61–2.06 Å. There are twenty-two inequivalent O sites. In the first O site, O is bonded in a distorted trigonal non-coplanar geometry to three V atoms. In the second O site, O is bonded in a distorted T-shaped geometry to three V atoms. In the third O site, O is bonded in a distorted trigonal non-coplanar geometry to three V atoms. In the fourth O site, O is bonded in a distorted T-shaped geometry to three V atoms. In the fifth O site, O is bonded in a distorted bent 150 degrees geometry to three V atoms. In the sixth O site, O is bonded in a distorted bent 150 degrees geometry to two V atoms. In the seventh O site, O is bonded in a 2-coordinate geometry to three V atoms. In the eighth O site, O is bonded in a 2-coordinate geometry to three V atoms. In the ninth O site, O is bonded in a single-bond geometry to one V atom. In the tenth O site, O is bonded in a single-bond geometry to one V atom. In the eleventh O site, O is bonded in a bent 150 degrees geometry to one Ca and one V atom. In the twelfth O site, O is bonded in a single-bond geometry to one V atom. In the thirteenth O site, O is bonded in a single-bond geometry to one V atom. In the fourteenth O site, O is bonded in a single-bond geometry to one V atom. In the fifteenth O site, O is bonded in a single-bond geometry to one V atom. In the sixteenth O site, O is bonded in a bent 150 degrees geometry to one Ca and one V atom. In the seventeenth O site, O is bonded in a distorted T-shaped geometry to three V atoms. In the eighteenth O site, O is bonded in a 3-coordinate geometry to three V atoms. In the nineteenth O site, O is bonded in a 3-coordinate geometry to three V atoms. In the twentieth O site, O is bonded in a 3-coordinate geometry to three V atoms. In the twenty-first O site, O is bonded in a distorted trigonal non-coplanar geometry to two equivalent Ca and one O atom. The O–O bond length is 1.37 Å. In the twenty-second O site, O is bonded in a distorted trigonal non-coplanar geometry to two equivalent Ca and one O atom.

36 MATERIALS SCIENCE↗

Materials Data on Ca2V3O8 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 Ca5V3O12 by Materials Project

Ca5V3O12 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are three inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.44–2.83 Å. In the second Ca2+ site, Ca2+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Ca–O bond distances ranging from 2.32–2.70 Å. In the third Ca2+ site, Ca2+ is bonded to seven O2- atoms to form distorted CaO7 pentagonal bipyramids that share a cornercorner with one CaO7 pentagonal bipyramid, corners with three VO4 tetrahedra, edges with two equivalent CaO7 pentagonal bipyramids, and edges with two VO4 tetrahedra. There are a spread of Ca–O bond distances ranging from 2.31–2.68 Å. There are two inequivalent V+4.67+ sites. In the first V+4.67+ site, V+4.67+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with two equivalent CaO7 pentagonal bipyramids and an edgeedge with one CaO7 pentagonal bipyramid. There are a spread of V–O bond distances ranging from 1.77–1.79 Å. In the second V+4.67+ site, V+4.67+ is bonded to four O2- atoms to form VO4 tetrahedra that share corners with two equivalent CaO7 pentagonal bipyramids and edges with two equivalent CaO7 pentagonal bipyramids. There is one shorter (1.72 Å) and three longer (1.75 Å) V–O bond length. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to two equivalent Ca2+ and one V+4.67+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to three Ca2+ and one V+4.67+ atom. In the third O2- site, O2- is bonded in a 1-coordinate geometry to three Ca2+ and one V+4.67+ atom. In the fourth O2- site, O2- is bonded to three Ca2+ and one V+4.67+ atom to form edge-sharing OCa3V tetrahedra. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to three Ca2+ and one V+4.67+ atom. In the sixth O2- site, O2- is bonded in a distorted single-bond geometry to four Ca2+ and one V+4.67+ atom. In the seventh O2- site, O2- is bonded in a 4-coordinate geometry to three Ca2+ and one V+4.67+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Ca3V2O8 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 Ca2V2O7 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 Ca2V3O8 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 CaV4O10 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 CaV4O6 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↗