The relativistic oscillation of the electron mass in very intense high frequency fields can give rise to parametric instabilities. These instabilities, whose growth rates do not depend on the electron-to-ion mass ratio, will surpass the oscillating two-stream instability and become the dominant process when the laser beam produces electron mass variations of the order of (me/Mi)1/3 or about 6.5×10−2 for deuterium. This corresponds to oscillating energies of a few ten keV. The linear and nonlinear stages of these instabilities are investigated through analytic methods and computer simulations.
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Lin et al. (1976) studied this question.
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