Abstract
Raman spectra are presented for single crystal metallic potassium fulleride at low temperatures. As compared to the undoped material dramatic changes in line position (\ensuremath{\Delta}\ensuremath{\omega}\ensuremath{\ge}80 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$) and linewidth (\ensuremath{\gamma}\ensuremath{\ge}60 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$), particularly for the two highest and the two lowest ${\mathit{H}}_{\mathit{g}}$ modes, were observed. The lowest frequency ${\mathit{H}}_{\mathit{g}}$ modes were found to be asymmetric but structured and could be fitted with five components which exhibit a line shift-linewidth relation. The experimental results are discussed in a model of single-particle excitation (Landau damping). Electron-phonon coupling constants ${\ensuremath{\lambda}}_{\mathit{i}}$ were determined for all eight ${\mathit{H}}_{\mathit{g}}$ modes using Allen's formula. The total for all ${\ensuremath{\lambda}}_{\mathit{i}}$ was found to be 0.9 for a density of states at the Fermi level of 12 ${\mathrm{eV}}^{\mathrm{\ensuremath{-}}1}$. \textcopyright{} 1996 The American Physical Society.
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