Constant residual electrostatic electron plasma mode in Vlasov-Ampere system
arXiv:1304.5883 · doi:10.1063/1.4831761
Abstract
In a collisionless Vlasov-Poisson (V-P) electron plasma system, two types of modes for electric field perturbation exist: the exponentially Landau damped electron plasma waves and the initial-value sensitive ballistic modes. Here, the V-P system is modified slightly to a Vlasov-Ampere (V-A) system. A new constant residual mode is revealed. Mathematically, this mode comes from the Laplace transform of an initial electric field perturbation, and physically represents that an initial perturbation (e.g., external electric field perturbation) would not be damped away. Thus, this residual mode is more difficult to be damped than the ballistic mode. [Physics of Plasmas 20, 112108 (2013); doi: 10.1063/1.4831761]
5 pages, 4 figures, (compared to v1, the title has been changed)
Cited by in corpus (4)
- PDRK: A General Kinetic Dispersion Relation Solver for Magnetized Plasma
- Generalized Plasma Dispersion Function: One-Solve-All Treatment, Visualizations, and Application to Landau Damping
- Comparisons and Applications of Four Independent Numerical Approaches for Linear Gyrokinetic Drift Modes
- Machine-learning heat flux closure for multi-moment fluid modeling of nonlinear Landau damping