We present an analytic solution for Raman backscatter in a cold homogeneous plasma, valid until saturation by breaking of the longitudinal waves, or by self-consistent depletion of the pump. We give quantitative values for the pump strength necessary for the former to occur first, and the transmission at saturation. Nonlinear particle bunching causes growth of electromagnetic sidebands. In quarter-critical plasma, a sideband at ω=3/2ω₀ reaches 8% of the pump intensity at wave breaking.
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Koch et al. (1975) studied this question.
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