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Materials Data on Li3RhF6 by Materials Project

Li3RhF6 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a linear geometry to two equivalent F1- atoms. Both Li–F bond lengths are 1.72 Å. In the second Li1+ site, Li1+ is bonded in a square co-planar geometry to four F1- atoms. There is two shorter (1.89 Å) and two longer (1.94 Å) Li–F bond length. In the third Li1+ site, Li1+ is bonded in a linear geometry to two equivalent F1- atoms. Both Li–F bond lengths are 1.78 Å. Rh3+ is bonded in an octahedral geometry to six F1- atoms. There are four shorter (2.01 Å) and two longer (2.03 Å) Rh–F bond lengths. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to two Li1+ and one Rh3+ atom. In the second F1- site, F1- is bonded in a bent 150 degrees geometry to one Li1+ and one Rh3+ atom. In the third F1- site, F1- is bonded in an L-shaped geometry to one Li1+ and one Rh3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3RhF6 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↗