Nonlinear wave damping due to multi-plasmon resonances
arXiv:1604.05983 · doi:10.1088/1361-6587/aa979d
Abstract
For short wavelengths, it is well known that the linearized Wigner-Moyal equation predicts wave damping due to wave-particle interaction, where the resonant velocity shifted from the phase velocity by a velocity . Here is the reduced Planck constant, is the wavenumber and is the electron mass. Going beyond linear theory, we find additional resonances with velocity shifts , , giving rise to a new wave-damping mechanism that we term \emph{multi-plasmon damping}, as it can be seen as the simultaneous absorption (or emission) of multiple plasmon quanta. Naturally this wave damping is not present in classical plasmas. For a temperature well below the Fermi temperature, if the linear () resonant velocity is outside the Fermi sphere, the number of linearly resonant particles is exponentially small, while the multi-plasmon resonances can be located in the bulk of the distribution. We derive sets of evolution equations for the case of two-plasmon and three-plasmon resonances for Langmuir waves in the simplest case of a fully degenerate plasma. By solving these equations numerically for a range of wave-numbers we find the corresponding damping rates, and we compare them to results from linear theory to estimate the applicability. Finally, we discuss the effects due to a finite temperature.
Accepted for publication in Plasma Physics and Controlled Fusion
References in corpus (2)
Cited by in corpus (5)
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