We present a detailed investigation of the Raman spectra of isotopically ta
ilored CuBr at low temperature. The transverse optic (TO) phonon of CuBr ex
hibits an almost perfect Lorentzian line shape, whereas the longitudinal op
tic (LO) phonon displays a complex broad structure. The change of the TO fr
equency with the variation of the isotope composition can be well described
within the virtual crystal approximation (VCA), which corresponds to a ome
ga proportional to mu (-1/2) dependence on the reduced mass mu. Slight devi
ations from this general trend are attributed to anharmonic renormalization
and agree semiquantitatively with results extracted from previous measurem
ents of the temperature dependence of the Raman spectra. In the LO case, th
e broad structure is resolved into three separate features, A, B, and C. Wh
ile A and B are rather broad, C is a narrow peak located at the high-energy
side of the LO structure. Two different trends are observed when analyzing
the evolution of the LO structure with isotope substitution: peak B shows
proportional to mu (-1/2) behavior, analogous to that of the TO phonon, whe
reas peaks A and C shift almost only with the copper mass. The LO line shap
e is explained in terms of the Fermi resonance (FR) model, i.e., an interac
tion between the LO mode and a combination band of two acoustic phonons. We
have performed a shell model calculation, with parameters taken from inela
stic neutron scattering measurements, in order to obtain the one- and two-p
honon densities of states (DOS). This calculation yields Raman line shapes
in remarkable agreement with the experimental observations.