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Materials Data on Sr4Fe4O11 by Materials Project

Sr4Fe4O11 crystallizes in the orthorhombic Pnnm space group. The structure is three-dimensional. Sr is bonded in a distorted q6 geometry to eleven O atoms. There are a spread of Sr–O bond distances ranging from 2.69–2.89 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with two equivalent FeO6 octahedra and corners with four equivalent FeO5 square pyramids. The corner-sharing octahedral tilt angles are 0°. There are a spread of Fe–O bond distances ranging from 1.94–2.06 Å. In the second Fe site, Fe is bonded to five O atoms to form FeO5 square pyramids that share corners with four equivalent FeO6 octahedra and a cornercorner with one FeO5 square pyramid. The corner-sharing octahedra tilt angles range from 2–14°. There are a spread of Fe–O bond distances ranging from 1.88–1.99 Å. There are six inequivalent O sites. In the first O site, O is bonded in a 6-coordinate geometry to four equivalent Sr and two Fe atoms. In the second O site, O is bonded to four equivalent Sr and two equivalent Fe atoms to form a mixture of distorted corner and edge-sharing OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 11–60°. In the third O site, O is bonded to four equivalent Sr and two equivalent Fe atoms to form a mixture of distorted corner, edge, and face-sharing OSr4Fe2 octahedra. The corner-sharing octahedral tilt angles are 4°. In the fourth O site, O is bonded to four equivalent Sr and two Fe atoms to form a mixture of distorted corner, edge, and face-sharing OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 4–60°. In the fifth O site, O is bonded in a distorted linear geometry to four equivalent Sr and two equivalent Fe atoms. In the sixth O site, O is bonded in a distorted linear geometry to four equivalent Sr and two Fe atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sr4Fe4O11 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↗