Raman spectra of CuCl were measured at T = 5 K under hydrostatic pressures
up to 3.3 GPa. The anomalous line shape of the transverse-optic (TO) scatte
ring, which consists of a broad structure with several maxima, undergoes a
drastic change under pressure. The anomaly disappears completely at 3 GPa.
These pressure effects are well reproduced by a model calculation of the an
harmonic coupling of the TO mode to acoustic two-phonon states (Fermi reson
ance). The results demonstrate that the ambient pressure TO anomaly does no
t arise from local vibrational modes of Cu atoms in off-center positions.