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Materials Data on LiVCuO4 by Materials Project

LiCuVO4 is Spinel-derived structured and crystallizes in the tetragonal P4_322 space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six equivalent CuO4 tetrahedra, edges with two equivalent LiO6 octahedra, and edges with four equivalent VO6 octahedra. There are a spread of Li–O bond distances ranging from 2.09–2.19 Å. V5+ is bonded to six O2- atoms to form distorted VO6 octahedra that share corners with six equivalent CuO4 tetrahedra, edges with two equivalent VO6 octahedra, and edges with four equivalent LiO6 octahedra. There are a spread of V–O bond distances ranging from 1.77–2.10 Å. Cu2+ is bonded to four O2- atoms to form CuO4 tetrahedra that share corners with six equivalent LiO6 octahedra and corners with six equivalent VO6 octahedra. The corner-sharing octahedra tilt angles range from 50–71°. There is two shorter (1.95 Å) and two longer (1.97 Å) Cu–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Li1+, one V5+, and one Cu2+ atom to form a mixture of distorted edge and corner-sharing OLi2VCu trigonal pyramids. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Li1+, two equivalent V5+, and one Cu2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on LiVCuO4 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 LiVCuO4 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↗