Excitation of Electrostatic Standing Wave in the Superposition of Two Counter Propagating Relativistic Whistler Waves
arXiv:2104.00440 · doi:10.1088/1402-4896/ac2b43
Abstract
The problem of standing wave formation by superposing two counter-propagating whistler waves in an overdense plasma, studied recently by Sano et al. (Phys. Rev. E 100, 053205 (2019) and Phys. Rev. E 101, 013206 (2020)), has been revisited in the relativistic limit. A detailed theory along with simulation has been performed to study the standing wave formation in the interaction of two counter propagating relativistically intense whistler waves. The relativistic theory explains such interaction process more precisely and predicts correct field amplitudes of the standing wave for a much wider range of physical parameters of the problem as compared to its non-relativistic counterpart. The analytical results are compared with 1-D Particle-in-Cell (PIC) simulation results, performed using OSIRIS 4.0. The results are of relevance to ion heating and fast ignition scheme of inertial confinement fusion.
8 pages, 12 figures
References in corpus (6)
- Hole boring in a DT pellet and fast ion ignition with ultra-intense laser pulses
- One-to-one direct modeling of experiments and astrophysical scenarios: pushing the envelope on kinetic plasma simulations
- Extreme case of Faraday effect: magnetic splitting of ultrashort laser pulses in plasmas
- Particle-In-Cell Modeling of Plasma-Based Accelerators in Two and Three Dimensions
- Thermonuclear Fusion Triggered by Collapsing Standing Whistler Waves in Magnetized Overdense Plasmas
- Ultrafast Wave-Particle Energy Transfer in the Collapse of Standing Whistler Waves