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Materials Data on BaYMnCoO5 by Materials Project

YBaMnCoO5 crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. Ba2+ is bonded to twelve O2- atoms to form distorted BaO12 cuboctahedra that share corners with four equivalent BaO12 cuboctahedra, faces with four equivalent BaO12 cuboctahedra, faces with four equivalent MnO5 square pyramids, and faces with four equivalent CoO5 square pyramids. There are four shorter (2.78 Å) and eight longer (3.16 Å) Ba–O bond lengths. Y3+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Y–O bond lengths are 2.43 Å. Mn2+ is bonded to five O2- atoms to form MnO5 square pyramids that share corners with five equivalent CoO5 square pyramids and faces with four equivalent BaO12 cuboctahedra. There are four shorter (1.97 Å) and one longer (2.06 Å) Mn–O bond lengths. Co3+ is bonded to five O2- atoms to form CoO5 square pyramids that share corners with five equivalent MnO5 square pyramids and faces with four equivalent BaO12 cuboctahedra. There are four shorter (2.04 Å) and one longer (2.09 Å) Co–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Ba2+, one Mn2+, and one Co3+ atom to form a mixture of edge and corner-sharing OBa4MnCo octahedra. The corner-sharing octahedral tilt angles are 1°. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+, two equivalent Y3+, one Mn2+, and one Co3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on BaYMnCoO5 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 BaYMnCoO5 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 BaYMnCoO5 by Materials Project

YBaMnCoO5 crystallizes in the tetragonal P4mm space group. The structure is three-dimensional. Ba2+ is bonded to twelve O2- atoms to form distorted BaO12 cuboctahedra that share corners with four equivalent BaO12 cuboctahedra, faces with four equivalent BaO12 cuboctahedra, faces with four equivalent CoO5 square pyramids, and faces with four equivalent MnO5 trigonal bipyramids. There are a spread of Ba–O bond distances ranging from 2.78–3.28 Å. Y3+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are four shorter (2.41 Å) and four longer (2.44 Å) Y–O bond lengths. Mn2+ is bonded to five O2- atoms to form distorted MnO5 trigonal bipyramids that share a cornercorner with one CoO5 square pyramid, corners with four equivalent MnO5 trigonal bipyramids, and faces with four equivalent BaO12 cuboctahedra. There are four shorter (2.02 Å) and one longer (2.04 Å) Mn–O bond lengths. Co3+ is bonded to five O2- atoms to form CoO5 square pyramids that share corners with four equivalent CoO5 square pyramids, a cornercorner with one MnO5 trigonal bipyramid, and faces with four equivalent BaO12 cuboctahedra. There are four shorter (2.00 Å) and one longer (2.13 Å) Co–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Ba2+, one Mn2+, and one Co3+ atom to form a mixture of distorted corner and edge-sharing OBa4MnCo octahedra. The corner-sharing octahedral tilt angles are 6°. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+, two equivalent Y3+, and two equivalent Co3+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+, two equivalent Y3+, and two equivalent Mn2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on BaYMnCoO5 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 BaYMnCoO5 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↗