A theory of general stimulated backscattering by a hot, relativistic electron beam propagating through a spatially periodic, transverse magnetostatic field is presented. The electrons are chosen to have a Lorentzian distribution in velocity space. Though energy spread acts to diminish gain, its effect is negligible if Δγ/γ < < N-1, where N is the number of undulator periods. The analysis is linear and applicable to both the single-particle and collective regimes.
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