Diffraction-controlled backscattering threshold and application to Raman gap

In most classic analytical models of linear stimulated scatter, light diffraction is omitted, a priori. However, modern laser optic typically includes a variant of the random phase plate Y. Kato, Phys. Rev. Lett. 53, 1057 (1984), resulting in diffraction limited laser intensity fluctuations-or localized speckles-which may result in explosive reflectivity growth as the average laser intensity approaches a critical value H. A. Rose and D. F. DuBois, Phys. Rev. Lett. 72, 2883 (1994). Among the differences between stimulated Raman scatter (SRS) and stimulated Brillouin scatter is that the SRS scattered light diffracts more strongly than the laser light with increase of electron density. This weakens the tendency of the SRS light to closely follow the most amplified paths, diminishing gain. Let G₀ be the one-dimensional power gain exponent of the stimulated scatter. In this paper we show that differential diffraction gives rise to an increase of G₀ at the SRS physical threshold with increase of electron density up to a drastic disruption of SRS as electron density approaches one fourth of its critical value from below. For three wave interaction lengths not small compared to a speckle length, this is a physically robust Raman gap mechanism.