Nonlinear adiabatic electron plasma waves. I. General theory and nonlinear frequency shift
arXiv:2112.15583 · doi:10.1063/5.0085177
Abstract
This paper provides a complete self-consistent nonlinear theory for electron plasma waves, within the framework of the adiabatic approximation. The theory applies whatever the variations of the wave amplitude, provided that they are slow enough, and it is also valid when the plasma is inhomogeneous and non stationary. Moreover, it accounts for: (i) the geometrical jump in action resulting from separatrix crossing; (ii) the continuous change in phase velocity making the wave frame non-inertial; (iii) the harmonic content of the scalar potential ; (iv) a non-zero vector potential ; (v) the transition probabilities from one region of phase space to the other when an orbit crosses the separatrix ; (vi) the possible change in direction of the wavenumber. The relative importance of each of the aforementioned effects is discussed in detail, based on the derivation of the nonlinear frequency shift. This allows to specify how the general formalism may be simplified, depending on the value of the wavenumber normalized to the Debye length. Specific applications of our theory are reported on the companion paper.
References in corpus (8)
- Exact relativistic kinetic theory of an electron beam-plasma system: hierarchy of the competing modes in the system parameter space
- Self-consistent Langmuir waves in resonantly driven thermal plasmas
- Directed transport in a spatially periodic potential under periodic non-biased forcing
- Envelope equation for the linear and nonlinear propagation of an electron plasma wave, including the effects of Landau damping, trapping, plasma inhomogeneity, and the change in the state of wave
- Global change in action due to trapping, how to derive it whatever the rate of variation of the dynamics
- Nonlocal adiabatic theory. I. The action distribution function
- Nonlinear adiabatic electron plasma waves. II. Applications
- Self-consistent theory for the linear and nonlinear propagation of a sinusoidal electron plasma wave. Application to stimulated Raman scattering in a non-uniform and non-stationary plasma