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At least 91 records · Page 5

Materials Data on NiAs2S6N4(OF2)8 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 CoBC8(OF2)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 K2NaNb(OF2)2 by Materials Project

K2NaNbO2F4 is (Cubic) Perovskite-derived structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. K1+ is bonded to four equivalent O2- and eight F1- atoms to form KO4F8 cuboctahedra that share corners with twelve equivalent KO4F8 cuboctahedra, faces with six equivalent KO4F8 cuboctahedra, faces with four equivalent NaO2F4 octahedra, and faces with four equivalent NbO2F4 octahedra. All K–O bond lengths are 3.06 Å. All K–F bond lengths are 3.05 Å. Na1+ is bonded to two equivalent O2- and four F1- atoms to form NaO2F4 octahedra that share corners with six equivalent NbO2F4 octahedra and faces with eight equivalent KO4F8 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. Both Na–O bond lengths are 2.41 Å. There are two shorter (2.27 Å) and two longer (2.29 Å) Na–F bond lengths. Nb5+ is bonded to two equivalent O2- and four F1- atoms to form NbO2F4 octahedra that share corners with six equivalent NaO2F4 octahedra and faces with eight equivalent KO4F8 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. Both Nb–O bond lengths are 1.90 Å. All Nb–F bond lengths are 2.04 Å. O2- is bonded in a distorted linear geometry to four equivalent K1+, one Na1+, and one Nb5+ atom. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted linear geometry to four equivalent K1+, one Na1+, and one Nb5+ atom. In the second F1- site, F1- is bonded in a distorted linear geometry to four equivalent K1+, one Na1+, and one Nb5+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Co3(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↗

Materials Data on Mn3(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↗

Materials Data on Co3(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↗

Materials Data on Mn3(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↗

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↗

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↗

Materials Data on Co3(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↗

Materials Data on Mn3(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↗

Materials Data on CsTaCo(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↗

Materials Data on Mn3(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↗

Materials Data on SiN4(OF2)3 by Materials Project

(N2)3(SiF6)2(NO3)2 crystallizes in the orthorhombic Cmcm space group. The structure is zero-dimensional and consists of twelve ammonia molecules, four nitric acid molecules, and four SiF6 clusters. In each SiF6 cluster, Si4+ is bonded in an octahedral geometry to six equivalent F1- atoms. All Si–F bond lengths are 1.71 Å. F1- is bonded in a single-bond geometry to one Si4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on LiFe5(OF2)4 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 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↗

Materials Data on Li6Mn(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↗

Materials Data on Mn3(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↗