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Materials Data on FeCO3 by Materials Project

FeCO3 is Calcite structured and crystallizes in the trigonal R-3c space group. The structure is three-dimensional. Fe2+ is bonded to six equivalent O2- atoms to form corner-sharing FeO6 octahedra. The corner-sharing octahedral tilt angles are 60°. All Fe–O bond lengths are 2.17 Å. C4+ is bonded in a trigonal planar geometry to three equivalent O2- atoms. All C–O bond lengths are 1.30 Å. O2- is bonded in a distorted trigonal planar geometry to two equivalent Fe2+ and one C4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Fe2(CO)9 by Materials Project

Fe2(CO)9 crystallizes in the hexagonal P6_3/m space group. The structure is zero-dimensional and consists of six formaldehyde molecules and four Fe(CO)3 clusters. In each Fe(CO)3 cluster, Fe3+ is bonded in a 3-coordinate geometry to three equivalent C+1.33+ atoms. All Fe–C bond lengths are 1.82 Å. C+1.33+ is bonded in a distorted single-bond geometry to one Fe3+ and one O2- atom. The C–O bond length is 1.16 Å. O2- is bonded in a single-bond geometry to one C+1.33+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Fe4C14O13 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(CO)5 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 Fe2C2O7 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 Fe2CO5 by Materials Project

Fe2O2CO3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing FeO6 octahedra. The corner-sharing octahedra tilt angles range from 59–60°. There are a spread of Fe–O bond distances ranging from 1.84–2.12 Å. In the second Fe3+ site, Fe3+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing FeO6 octahedra. The corner-sharing octahedra tilt angles range from 59–60°. There are a spread of Fe–O bond distances ranging from 1.93–2.09 Å. C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.23–1.36 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to two equivalent Fe3+ and one C4+ atom. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to three Fe3+ and one C4+ atom. In the third O2- site, O2- is bonded in a 2-coordinate geometry to one Fe3+ and one C4+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to three Fe3+ atoms. In the fifth O2- site, O2- is bonded in a trigonal non-coplanar geometry to three Fe3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Fe(CO3)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 Fe3C7O19 by Materials Project

Fe3C7O19 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two Fe3C7O19 clusters. there are three inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form distorted FeO6 octahedra that share a cornercorner with one FeO5 square pyramid and a cornercorner with one FeO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 1.93–2.46 Å. In the second Fe site, Fe is bonded to four O atoms to form distorted FeO4 tetrahedra that share a cornercorner with one FeO6 octahedra and a cornercorner with one FeO5 square pyramid. The corner-sharing octahedral tilt angles are 60°. There are a spread of Fe–O bond distances ranging from 1.97–2.36 Å. In the third Fe site, Fe is bonded to five O atoms to form distorted FeO5 square pyramids that share a cornercorner with one FeO6 octahedra and a cornercorner with one FeO4 tetrahedra. The corner-sharing octahedral tilt angles are 64°. There are a spread of Fe–O bond distances ranging from 2.03–2.19 Å. There are seven inequivalent C sites. In the first C site, C is bonded in a distorted bent 150 degrees geometry to two O atoms. There is one shorter (1.24 Å) and one longer (1.25 Å) C–O bond length. In the second C site, C is bonded in a linear geometry to two O atoms. There is one shorter (1.16 Å) and one longer (1.19 Å) C–O bond length. In the third C site, C is bonded in a linear geometry to two O atoms. There is one shorter (1.17 Å) and one longer (1.19 Å) C–O bond length. In the fourth C site, C is bonded in a distorted bent 150 degrees geometry to two O atoms. There is one shorter (1.24 Å) and one longer (1.25 Å) C–O bond length. In the fifth C site, C is bonded in a linear geometry to two O atoms. There is one shorter (1.17 Å) and one longer (1.18 Å) C–O bond length. In the sixth C site, C is bonded in a linear geometry to two O atoms. There is one shorter (1.17 Å) and one longer (1.18 Å) C–O bond length. In the seventh C site, C is bonded in a linear geometry to two O atoms. There is one shorter (1.16 Å) and one longer (1.19 Å) C–O bond length. There are nineteen inequivalent O sites. In the first O site, O is bonded in a distorted bent 150 degrees geometry to one Fe and one C atom. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one Fe and one C atom. In the third O site, O is bonded in a single-bond geometry to one O atom. The O–O bond length is 1.34 Å. In the fourth O site, O is bonded in a single-bond geometry to one C atom. In the fifth O site, O is bonded in a bent 120 degrees geometry to one Fe and one C atom. In the sixth O site, O is bonded in a distorted single-bond geometry to one Fe and one C atom. In the seventh O site, O is bonded in a single-bond geometry to one C atom. In the eighth O site, O is bonded in a single-bond geometry to one C atom. In the ninth O site, O is bonded in a distorted single-bond geometry to one Fe and one O atom. In the tenth O site, O is bonded in a trigonal planar geometry to three Fe atoms. In the eleventh O site, O is bonded in a distorted bent 120 degrees geometry to one Fe and one C atom. In the twelfth O site, O is bonded in a 1-coordinate geometry to one Fe and one O atom. The O–O bond length is 1.37 Å. In the thirteenth O site, O is bonded in a distorted bent 120 degrees geometry to one Fe and one C atom. In the fourteenth O site, O is bonded in a single-bond geometry to one C atom. In the fifteenth O site, O is bonded in a distorted bent 120 degrees geometry to one Fe and one C atom. In the sixteenth O site, O is bonded in a single-bond geometry to one C atom. In the seventeenth O site, O is bonded in a 2-coordinate geometry to one Fe and one C atom. In the eighteenth O site, O is bonded in a bent 120 degrees geometry to one Fe and one C atom. In the nineteenth O site, O is bonded in a 1-coordinate geometry to one Fe and one O atom.

36 MATERIALS SCIENCE↗

Materials Data on Fe2(CO3)3 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 Fe2C2O7 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 Fe2C2O7 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(CO3)2 by Materials Project

Fe(CO3)2 crystallizes in the orthorhombic Cccm space group. The structure is zero-dimensional and consists of sixteen carbon dioxide molecules and eight iron dihydroxide molecules.

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