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Materials Data on CsRb2PdF5 by Materials Project

CsRb2PdF5 crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Cs1+ is bonded in a distorted q6 geometry to ten F1- atoms. There are two shorter (3.27 Å) and eight longer (3.35 Å) Cs–F bond lengths. Rb1+ is bonded in a 8-coordinate geometry to eight F1- atoms. There are a spread of Rb–F bond distances ranging from 2.82–3.04 Å. Pd2+ is bonded in a square co-planar geometry to four equivalent F1- atoms. All Pd–F bond lengths are 1.99 Å. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a 6-coordinate geometry to two equivalent Cs1+, three equivalent Rb1+, and one Pd2+ atom. In the second F1- site, F1- is bonded to two equivalent Cs1+ and four equivalent Rb1+ atoms to form corner-sharing FCs2Rb4 octahedra. The corner-sharing octahedra tilt angles range from 0–32°.

36 MATERIALS SCIENCE↗

Materials Data on Cs2RbPdF6 by Materials Project

Cs2RbPdF6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs is bonded to twelve equivalent F atoms to form CsF12 cuboctahedra that share corners with twelve equivalent CsF12 cuboctahedra, faces with six equivalent CsF12 cuboctahedra, faces with four equivalent RbF6 octahedra, and faces with four equivalent PdF6 octahedra. All Cs–F bond lengths are 3.37 Å. Rb is bonded to six equivalent F atoms to form RbF6 octahedra that share corners with six equivalent PdF6 octahedra and faces with eight equivalent CsF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–F bond lengths are 2.68 Å. Pd is bonded to six equivalent F atoms to form PdF6 octahedra that share corners with six equivalent RbF6 octahedra and faces with eight equivalent CsF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Pd–F bond lengths are 2.07 Å. F is bonded in a distorted linear geometry to four equivalent Cs, one Rb, and one Pd atom.

36 MATERIALS SCIENCE↗

Materials Data on CsRb2PdF6 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↗