Nonlinear envelope equation and nonlinear Landau damping rate for a driven electron plasma wave

Abstract

In this paper, we provide a theoretical description, and calculate, the nonlinear frequency shift, group velocity and collionless damping rate, $ν$, of a driven electron plasma wave (EPW). All these quantities, whose physical content will be discussed, are identified as terms of an envelope equation allowing one to predict how efficiently an EPW may be externally driven. This envelope equation is derived directly from Gauss law and from the investigation of the nonlinear electron motion, provided that the time and space rates of variation of the EPW amplitude, $E_p$, are small compared to the plasma frequency or the inverse of the Debye length. $ν$ arises within the EPW envelope equation as more complicated an operator than a plain damping rate, and may only be viewed as such because $(νE_p)/E_p$ remains nearly constant before abruptly dropping to zero. We provide a practical analytic formula for $ν$ and show, without resorting to complex contour deformation, that in the limit $E_p \to 0$, $ν$ is nothing but the Landau damping rate. We then term $ν$ the "nonlinear Landau damping rate" of the driven plasma wave. As for the nonlinear frequency shift of the EPW, it is also derived theoretically and found to assume values significantly different from previously published ones, assuming that the wave is freely propagating. Moreover, we find no limitation in $k λ_D$, $k$ being the plasma wavenumber and $λ_D$ the Debye length, for a solution to the dispertion relation to exist, and want to stress here the importance of specifying how an EPW is generated to discuss its properties. Our theoretical predictions are in excellent agreement with results inferred from Vlasov simulations of stimulated Raman scattering (SRS), and an application of our theory to the study of SRS is presented.