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25 records · Page 2

Materials Data on FeCoO2 by Materials Project

CoFeO2 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Fe2+ is bonded to six equivalent O2- atoms to form edge-sharing FeO6 octahedra. There is two shorter (1.99 Å) and four longer (2.00 Å) Fe–O bond length. Co2+ is bonded in a linear geometry to two equivalent O2- atoms. Both Co–O bond lengths are 1.84 Å. O2- is bonded to three equivalent Fe2+ and one Co2+ atom to form a mixture of distorted edge and corner-sharing OFe3Co trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Fe(CoO3)2 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 Fe2CoO6 by Materials Project

Fe2CoO6 is Hydrophilite-derived structured and crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are four inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with four equivalent CoO6 octahedra, corners with six FeO6 octahedra, and an edgeedge with one CoO6 octahedra. The corner-sharing octahedra tilt angles range from 50–53°. There are a spread of Fe–O bond distances ranging from 1.98–2.03 Å. In the second Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with two equivalent CoO6 octahedra, corners with six FeO6 octahedra, and edges with two equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 50–54°. There are a spread of Fe–O bond distances ranging from 1.94–1.98 Å. In the third Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with two equivalent CoO6 octahedra, corners with six FeO6 octahedra, and edges with two equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 51–53°. There are a spread of Fe–O bond distances ranging from 1.94–1.99 Å. In the fourth Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with four equivalent CoO6 octahedra, corners with six FeO6 octahedra, and an edgeedge with one CoO6 octahedra. The corner-sharing octahedra tilt angles range from 51–52°. There are a spread of Fe–O bond distances ranging from 1.98–2.04 Å. There are two inequivalent Co sites. In the first Co site, Co is bonded to six O atoms to form CoO6 octahedra that share corners with six FeO6 octahedra and edges with three FeO6 octahedra. The corner-sharing octahedra tilt angles range from 51–53°. There are a spread of Co–O bond distances ranging from 1.86–1.88 Å. In the second Co site, Co is bonded to six O atoms to form CoO6 octahedra that share corners with six FeO6 octahedra and edges with three FeO6 octahedra. The corner-sharing octahedra tilt angles range from 52–54°. There are a spread of Co–O bond distances ranging from 1.83–1.88 Å. There are nine inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to two Fe and one Co atom. In the second O site, O is bonded in a trigonal planar geometry to two Fe and one Co atom. In the third O site, O is bonded in a distorted trigonal planar geometry to two Fe and one Co atom. In the fourth O site, O is bonded in a distorted trigonal planar geometry to two Fe and one Co atom. In the fifth O site, O is bonded in a trigonal planar geometry to two Fe and one Co atom. In the sixth O site, O is bonded in a trigonal planar geometry to two Fe and one Co atom. In the seventh O site, O is bonded in a distorted trigonal planar geometry to two Fe and one Co atom. In the eighth O site, O is bonded in a distorted trigonal planar geometry to two Fe and one Co atom. In the ninth O site, O is bonded in a trigonal planar geometry to two Fe and one Co atom.

36 MATERIALS SCIENCE↗

Materials Data on Fe19Co5O32 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 Fe3Co5O16 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 FeCo5O12 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 Fe(CoO2)2 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↗