Abstract
Second-order Raman measurements have been made on oriented GaSb with various combinations of incident and scattered polarizations in order to obtain the three irreducible components of the Raman tensor Γ1, Γ15, and Γ12. The dominant Γ1 Raman spectrum is compared with the recently reported one-phonon density of states calculation based upon shell-model parameters that were fitted to neutron data. Significant deviations exist and we believe these to be artifacts of the shell-model parameters used. The observed dependence of the 2LO(Γ) and 2TO(Δ) Raman peaks upon incident photon energy was attributed to resonance Raman effect with the E1+Δ1 direct gap and with the Γ15νΔ1c indirect gap, respectively.