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Raman spectra have been recorded from 300--10 K for lanthanide hexachloroelpasolites, Cs₂{NaLCl}₆$. Electronic Raman-scattering intensity ratios have been calculated using Judd-Ofelt-Axe theory and are in reasonable agreement with experimental results, except for those cases where electron-phonon coupling has important consequences. Bands resulting from temperature-dependent electron-phonon coupling phenomena have been observed not only in the Raman spectrum of Cs₂{NaYbCl}₆$ but also in that of ${Cs}₂NaTmCl₆, and the interaction mechanism is discussed. The coupling element between the coupled aΓ₅{~}Γ₁+ν₅ phonon-electron states of ³H₆ in Cs₂{NaTmCl}₆$ is estimated to be 20 ${cm}^{{{-}}1}$, and the corrected wave functions for these coupled states enable a consistent reinterpretation to be made of the optical spectra of ${TmCl}₆^{3{{-}}}$. Excited-state electronic Raman scattering has been observed in the 120-K Raman spectrum of ${Cs}₂NaTmCl₆. Using fixed wavelength argon-ion laser lines, there is evidence for a small resonance enhancement of electronic Raman-scattering intensity, and the unusual mechanism for this is discussed. The mixed crystal system Cs₂{NaGd}_{1{{-}}x}Ybₓ{Cl}₆$ exhibits unimodal behavior for the ${{ν}}₁$ and ${{ν}}₅$ vibrations, and the more complex behavior of features in the neighborhood of ${{ν}}₂$ is described. The vibrational energies of the gerade internal ${LCl}₆^{3{{-}}}$ modes (determined from Raman spectra) vary linearly with atomic number of L, except where electron-phonon coupling effects occur.
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Tanner et al. (1997) studied this question.
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