The nonlinear interaction of helicons (whistlers) is found to depend radically on whether the plasma has diffuse or sharp boundaries. The conventional picture of three-wave interaction obtained by perturbing the normal-mode amplitudes is valid for the diffuse case. However, for a plasma with sharp boundaries, e.g., a solid-state plasma including collisions, surface currents play an important role in the limit of large Ω_τ, where Ω is the electron gyrofrequency and τ is the relaxation time. It is shown that the normal-mode method breaks down even at very small amplitudes. A new strong-coupling method is developed which predicts an interaction rate in the large-Ω_τ limit that never exceeds the order of the wave linear damping, but should be experimentally observable.
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Sudan et al. (1967) studied this question.
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