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At least 469 records · Page 26
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DOE OSTI2020

Materials Data on Fe10OF19 by Materials Project

Fe10OF19 is Hydrophilite-derived structured and crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are six inequivalent Fe+2.10+ sites. In the first Fe+2.10+ site, Fe+2.10+ is bonded to one O2- and five F1- atoms to form a mixture of edge and corner-sharing FeOF5 octahedra. The corner-sharing octahedra tilt angles range from 46–53°. The Fe–O bond length is 2.06 Å. There are a spread of Fe–F bond distances ranging from 2.09–2.20 Å. In the second Fe+2.10+ site, Fe+2.10+ is bonded to six F1- atoms to form FeF6 octahedra that share corners with eight FeF6 octahedra and edges with two FeOF5 octahedra. The corner-sharing octahedra tilt angles range from 50–53°. There are a spread of Fe–F bond distances ranging from 2.05–2.14 Å. In the third Fe+2.10+ site, Fe+2.10+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 50–51°. There are two shorter (2.04 Å) and four longer (2.13 Å) Fe–F bond lengths. In the fourth Fe+2.10+ site, Fe+2.10+ is bonded to one O2- and five F1- atoms to form FeOF5 octahedra that share corners with eight equivalent FeOF5 octahedra and edges with two equivalent FeF6 octahedra. The corner-sharing octahedra tilt angles range from 46–51°. The Fe–O bond length is 1.82 Å. There are one shorter (2.07 Å) and four longer (2.08 Å) Fe–F bond lengths. In the fifth Fe+2.10+ site, Fe+2.10+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 50–51°. There are a spread of Fe–F bond distances ranging from 2.03–2.15 Å. In the sixth Fe+2.10+ site, Fe+2.10+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 50–53°. There are a spread of Fe–F bond distances ranging from 2.03–2.16 Å. O2- is bonded in a distorted trigonal planar geometry to three Fe+2.10+ atoms. There are eight inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted T-shaped geometry to three Fe+2.10+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.10+ atoms. In the third F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.10+ atoms. In the fourth F1- site, F1- is bonded in a trigonal planar geometry to three Fe+2.10+ atoms. In the fifth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.10+ atoms. In the sixth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.10+ atoms. In the seventh F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.10+ atoms. In the eighth F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.10+ atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on FeOF 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↗
DOE OSTI2020

Materials Data on Fe3(OF2)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↗
DOE OSTI2020

Materials Data on Fe3OF7 by Materials Project

Fe3OF7 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are three inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form edge-sharing FeOF5 octahedra. The Fe–O bond length is 1.94 Å. There are a spread of Fe–F bond distances ranging from 1.98–2.10 Å. In the second Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form edge-sharing FeOF5 octahedra. The Fe–O bond length is 1.99 Å. There are a spread of Fe–F bond distances ranging from 1.94–2.20 Å. In the third Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form edge-sharing FeOF5 octahedra. The Fe–O bond length is 1.95 Å. There are a spread of Fe–F bond distances ranging from 1.97–2.11 Å. O2- is bonded in a 3-coordinate geometry to three Fe3+ atoms. There are seven inequivalent F1- sites. In the first F1- site, F1- is bonded in an L-shaped geometry to two Fe3+ atoms. In the second F1- site, F1- is bonded in an L-shaped geometry to two Fe3+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three Fe3+ atoms. In the fourth F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms. In the fifth F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms. In the sixth F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms. In the seventh F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Fe5O3F7 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↗
DOE OSTI2020

Materials Data on FeOF 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↗
DOE OSTI2020

Materials Data on Fe3(OF4)2 by Materials Project

Fe3(OF4)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Fe sites. In the first Fe site, Fe is bonded to two equivalent O and four equivalent F atoms to form corner-sharing FeO2F4 octahedra. The corner-sharing octahedral tilt angles are 34°. Both Fe–O bond lengths are 1.97 Å. All Fe–F bond lengths are 1.98 Å. In the second Fe site, Fe is bonded to six F atoms to form corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 22–34°. All Fe–F bond lengths are 1.96 Å. O is bonded in a single-bond geometry to one Fe atom. There are three inequivalent F sites. In the first F site, F is bonded in a bent 150 degrees geometry to two equivalent Fe atoms. In the second F site, F is bonded in a bent 150 degrees geometry to two equivalent Fe atoms. In the third F site, F is bonded in a bent 150 degrees geometry to two Fe atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on FeOF 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↗
DOE OSTI2020

Materials Data on Fe5O7F3 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↗
DOE OSTI2020

Materials Data on Fe6O7F5 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↗
DOE OSTI2020

Materials Data on Fe10O11F9 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↗
DOE OSTI2020

Materials Data on Fe3OF5 by Materials Project

Fe3OF5 is Hydrophilite-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are four inequivalent Fe+2.33+ sites. In the first Fe+2.33+ site, Fe+2.33+ is bonded to one O2- and five F1- atoms to form FeOF5 octahedra that share corners with eight FeO2F4 octahedra and edges with two FeOF5 octahedra. The corner-sharing octahedra tilt angles range from 44–58°. The Fe–O bond length is 1.91 Å. There are a spread of Fe–F bond distances ranging from 2.08–2.10 Å. In the second Fe+2.33+ site, Fe+2.33+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing FeF6 octahedra. The corner-sharing octahedra tilt angles range from 50–54°. There are two shorter (2.06 Å) and four longer (2.14 Å) Fe–F bond lengths. In the third Fe+2.33+ site, Fe+2.33+ is bonded to two equivalent O2- and four F1- atoms to form a mixture of edge and corner-sharing FeO2F4 octahedra. The corner-sharing octahedra tilt angles range from 44–48°. Both Fe–O bond lengths are 1.90 Å. There are two shorter (2.08 Å) and two longer (2.09 Å) Fe–F bond lengths. In the fourth Fe+2.33+ site, Fe+2.33+ is bonded to one O2- and five F1- atoms to form FeOF5 octahedra that share corners with eight FeOF5 octahedra and edges with two FeO2F4 octahedra. The corner-sharing octahedra tilt angles range from 49–58°. The Fe–O bond length is 2.05 Å. There are a spread of Fe–F bond distances ranging from 2.12–2.22 Å. O2- is bonded in a distorted trigonal planar geometry to three Fe+2.33+ atoms. There are four inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.33+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to three Fe+2.33+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three Fe+2.33+ atoms. In the fourth F1- site, F1- is bonded in a trigonal planar geometry to three Fe+2.33+ atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Fe5O3F7 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↗
DOE OSTI2020

Materials Data on Fe2OF3 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↗
DOE OSTI2020

Materials Data on Fe7(OF7)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↗
DOE OSTI2020

Materials Data on Fe3O5F 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↗
DOE OSTI2020

Materials Data on FeOF 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↗
DOE OSTI2020

Materials Data on FeOF 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↗