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Materials Data on Mn3Cu3O8 by Materials Project

Mn3Cu3O8 is Spinel-like structured and crystallizes in the trigonal R-3m space group. The structure is three-dimensional. Mn+3.67+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six equivalent CuO4 tetrahedra, edges with two equivalent CuO6 octahedra, and edges with four equivalent MnO6 octahedra. There are four shorter (1.99 Å) and two longer (2.04 Å) Mn–O bond lengths. There are two inequivalent Cu+1.67+ sites. In the first Cu+1.67+ site, Cu+1.67+ is bonded to four O2- atoms to form CuO4 tetrahedra that share corners with three equivalent CuO6 octahedra and corners with nine equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 58–60°. There is one shorter (1.98 Å) and three longer (2.00 Å) Cu–O bond length. In the second Cu+1.67+ site, Cu+1.67+ is bonded to six equivalent O2- atoms to form CuO6 octahedra that share corners with six equivalent CuO4 tetrahedra and edges with six equivalent MnO6 octahedra. All Cu–O bond lengths are 2.06 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to three equivalent Mn+3.67+ and one Cu+1.67+ atom to form distorted corner-sharing OMn3Cu trigonal pyramids. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two equivalent Mn+3.67+ and two Cu+1.67+ atoms.

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Materials Data on Mn2CuO4 by Materials Project

CuMn2O4 is Spinel-like structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. there are two inequivalent Mn3+ sites. In the first Mn3+ site, Mn3+ is bonded to four O2- atoms to form MnO4 tetrahedra that share corners with three equivalent CuO6 octahedra and corners with nine equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 58–60°. There are one shorter (2.02 Å) and three longer (2.04 Å) Mn–O bond lengths. In the second Mn3+ site, Mn3+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with three equivalent MnO4 tetrahedra, corners with three equivalent CuO4 tetrahedra, edges with two equivalent CuO6 octahedra, and edges with four equivalent MnO6 octahedra. There are four shorter (2.00 Å) and two longer (2.08 Å) Mn–O bond lengths. There are two inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded to four O2- atoms to form CuO4 tetrahedra that share corners with three equivalent CuO6 octahedra and corners with nine equivalent MnO6 octahedra. The corner-sharing octahedra tilt angles range from 57–61°. There is one shorter (1.96 Å) and three longer (2.03 Å) Cu–O bond length. In the second Cu2+ site, Cu2+ is bonded to six O2- atoms to form CuO6 octahedra that share corners with three equivalent MnO4 tetrahedra, corners with three equivalent CuO4 tetrahedra, and edges with six equivalent MnO6 octahedra. All Cu–O bond lengths are 2.09 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to three equivalent Mn3+ and one Cu2+ atom. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two equivalent Mn3+ and two Cu2+ atoms. In the third O2- site, O2- is bonded to three Mn3+ and one Cu2+ atom to form a mixture of distorted edge and corner-sharing OMn3Cu trigonal pyramids. In the fourth O2- site, O2- is bonded to four Mn3+ atoms to form a mixture of distorted edge and corner-sharing OMn4 trigonal pyramids.

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Materials Data on Mn2CuO4 by Materials Project

CuMn2O4 is Spinel-like structured and crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. there are two inequivalent Mn3+ sites. In the first Mn3+ site, Mn3+ is bonded to four O2- atoms to form MnO4 tetrahedra that share corners with six equivalent MnO6 octahedra and corners with six equivalent CuO6 octahedra. The corner-sharing octahedra tilt angles range from 58–60°. There are two shorter (2.02 Å) and two longer (2.03 Å) Mn–O bond lengths. In the second Mn3+ site, Mn3+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with six equivalent MnO4 tetrahedra, edges with two equivalent MnO6 octahedra, and edges with four equivalent CuO6 octahedra. There are two shorter (1.96 Å) and four longer (2.05 Å) Mn–O bond lengths. Cu2+ is bonded to six O2- atoms to form CuO6 octahedra that share corners with six equivalent MnO4 tetrahedra, edges with two equivalent CuO6 octahedra, and edges with four equivalent MnO6 octahedra. There are two shorter (2.06 Å) and four longer (2.08 Å) Cu–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to three Mn3+ and one Cu2+ atom. In the second O2- site, O2- is bonded to two Mn3+ and two equivalent Cu2+ atoms to form a mixture of distorted edge and corner-sharing OMn2Cu2 trigonal pyramids.

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Materials Data on Mn2CuO4 by Materials Project

CuMn2O4 is Spinel structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Mn3+ is bonded to six equivalent O2- atoms to form MnO6 octahedra that share corners with six equivalent CuO4 tetrahedra and edges with six equivalent MnO6 octahedra. All Mn–O bond lengths are 2.04 Å. Cu2+ is bonded to four equivalent O2- atoms to form CuO4 tetrahedra that share corners with twelve equivalent MnO6 octahedra. The corner-sharing octahedral tilt angles are 58°. All Cu–O bond lengths are 2.01 Å. O2- is bonded to three equivalent Mn3+ and one Cu2+ atom to form a mixture of distorted edge and corner-sharing OMn3Cu trigonal pyramids.

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Materials Data on MnCuO2 by Materials Project

CuMnO2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Mn2+ is bonded to six equivalent O2- atoms to form edge-sharing MnO6 octahedra. There are four shorter (1.99 Å) and two longer (2.28 Å) Mn–O bond lengths. Cu2+ is bonded in a linear geometry to two equivalent O2- atoms. Both Cu–O bond lengths are 1.84 Å. O2- is bonded to three equivalent Mn2+ and one Cu2+ atom to form a mixture of distorted corner and edge-sharing OMn3Cu tetrahedra.

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Materials Data on Mn3Cu3O8 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

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