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Convective instabilities in the strongly damped regime are shown to exhibit essential nonlinear behavior due to laser hot spots when the average laser intensity 〈I〉 approaches a critical threshold value Ic. The onset of this nonlinear regime is formally signaled by the divergence of the average convective amplification 〈A〉as 〈I〉{→}Ic. An independent hot spot model of random phase plate optics predicts that 〈A〉{~}1/(Ic-〈I〉)². A saturated hot spot model of nonlinear stimulated Brillouin scattering (SBS) predicts a rapid turn on and saturation of SBS reflectivity with laser intensity and optic f number.
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Rose et al. (1994) studied this question.
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