The amplitude at which a single unstable Langmuir or ion-acoustic wave in a collisionless plasma saturates due to electron trapping is estimated using both the adiabatic and sudden approximations, and is shown to obey the approximate relation ωb∼3γlin. This is found from momentum conservation. It is found that energy conservation implies a nonlinear dispersion relation that is linearly independent of that derived from Poisson's equation, but that a reasonable distribution of resonant particles can be found that satisfies both relations.
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R. L. Dewar (1973) studied this question.
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