“…However, the Raman spectrum of the DZ phase would rather resemble that of the first-order one-phonon density of states of the zinc blende phase because disorder of cations and vacancies at cation sites will promote defect-induced or defect-assisted Raman scattering (DARS) due to the loss of the translational symmetry of the crystal. This Raman activity has been observed in many disordered, nanocrystalline, and pressure-treated compounds; [33][34][35][36] however, as already commented, no Raman scattering similar to a one-phonon density of states of the zinc blende phase has been ever reported to occur at high pressures neither above the pressure range 11-14 GPa in DCCdGa 2 Se 4 nor in other adamantine ternary OVCs at high pressures. 11,12,19,20 In fact, Ursaki et al concluded, from the analysis of their Raman results, 11 that the decrease of the intensity of the A 1 mode above 11 GPa was due to the onset of a second stage of disorder where all cations and vacancies mixed together, thus leading to the DZ phase in good agreement with the theoretically predicted stages of disorder proposed by Bernard and Zunger for OVCs at high temperatures but not for high pressures.…”