This content will become publicly available on July 1, 2027

Title: Control of kinetic plasma instabilities by laser fields
We study the possibility of controlling kinetic plasma instabilities by using lasers to apply external transverse electromagnetic fields. We derive the dispersion relation for the corresponding mathematical description, a reduced Vlasov–Maxwell system, by extending the well-known Penrose condition. It is observed that, under very mild assumptions, the dispersion relation decouples into two parts. The first part is identical to the classic Penrose condition for the Vlasov–Poisson system, while the second part describes the influence of the laser on the transverse dynamics (e.g., a Weibel instability). In particular, this means that the longitudinal dynamics (e.g., a two-stream instability) cannot be stabilized in this manner as far as linear theory is concerned. We show that, however, nonlinear effects can be used to couple the two parts and achieve an effective control. This is done by determining the control parameters (i.e., the form of the external electric and magnetic fields) by solving a partial differential equation (PDE)-constrained optimization problem.  more » « less
Award ID(s):
2308440
PAR ID:
10707824
Author(s) / Creator(s):
; ; ; ;
Publisher / Repository:
American Institute of Physics
Date Published:
Journal Name:
Physics of Plasmas
Volume:
33
Issue:
7
ISSN:
1070-664X
Format(s):
Medium: X
Sponsoring Org:
National Science Foundation
More Like this
  1. We prove asymptotic stability of the Poisson homogeneous equilibrium among solu- tions of the Vlasov–Poisson system in the Euclidean space R3. More precisely, we show that small, smooth, and localized perturbations of the Poisson equilibrium lead to global solutions of the Vlasov–Poisson system, which scatter to linear solutions at a polynomial rate as t → ∞. The Euclidean problem we consider here differs signif- icantly from the classical work on Landau damping in the periodic setting, in several ways. Most importantly, the linearized problem cannot satisfy a “Penrose condition”. As a result, our system contains resonances (small divisors) and the electric field is a superposition of an electrostatic component and a larger oscillatory component, both with polynomially decaying rates. 
    more » « less
  2. Although the nuclear fusion process has received a great deal of attention in recent years, the amount of mathematical analysis that supports the stability of the system seems to be relatively insufficient. This paper deals with the mathematical analysis of the magnetic confinement of the plasma via kinetic equations. We prove the global wellposedness of the Vlasov-Maxwell system in a two-dimensional annulus when a huge (but finite-in-time) external magnetic potential is imposed near the boundary. We assume that the solution is axisymmetric. The authors hope that this work is a step towards a more generalized work on the three-dimensional Tokamak structure. The highlight of this work is the physical assumptions on the external magnetic potential well which remains finite within a finite time interval and from that, we prove that the plasma never touches the boundary. In addition, we provide a sufficient condition on the magnitude of the external magnetic potential to guarantee that the plasma is confined in an annulus of the desired thickness which is slightly larger than the initial support. Our method uses the cylindrical coordinate forms of the Vlasov-Maxwell system. 
    more » « less
  3. We present a study of the standard plasma physics test, Landau damping, using the Particle-In-Cell (PIC) algorithm. The Landau damping phenomenon consists of the damping of small oscillations in plasmas without collisions. In the PIC method, a hybrid discretization is constructed with a grid of finitely supported basis functions to represent the electric, magnetic and/or gravitational fields, and a distribution of delta functions to represent the particle field. Approximations to the dispersion relation are found to be inadequate in accurately calculating values for the electric field frequency and damping rate when parameters of the physical system, such as the plasma frequency or thermal velocity, are varied. We present a full derivation and numerical solution for the dispersion relation, and verify the PETSC-PIC numerical solutions to the Vlasov-Poisson for a large range of wave numbers and charge densities. 
    more » « less
  4. The Moore–Saffman–Tsai–Widnall (MSTW) instability is a parametric instability that arises in strained vortex columns. The strain is assumed to be weak and perpendicular to the vortex axis. In this second part of our investigation of vortex instability including density and surface tension effects, a linear stability analysis for this situation is presented. The instability is caused by resonance between two Kelvin waves with azimuthal wavenumber separated by two. The dispersion relation for Kelvin waves and resonant modes are obtained. Results show that the stationary resonant waves for $$m=\pm 1$$ are more unstable when the density ratio $$\rho_2/\rho_1$$ , the ratio of vortex to ambient fluid density, approaches zero, whereas the growth rate is maximised near $$\rho _2/\rho _1 =0.215$$ for the resonance $(m,m+2)=(0,2)$ . Surface tension suppresses the instability, but its effect is less significant than that of density. As the azimuthal wavenumber $$m$$ increases, the MSTW instability decays, in contrast to the curvature instability examined in Part 1 (Chang & Llewellyn Smith, J. Fluid Mech. vol. 913, 2021, A14). 
    more » « less
  5. The spectrum of collective excitations in Weyl materials is studied by using a consistent hydro- dynamics. The corresponding framework includes the vortical and chiral anomaly effects, as well as the dependence on the separation between the Weyl nodes in energy b0 and momentum b. The latter are introduced via the Chern–Simons contributions to the electric current and charge densities in the Maxwell’s equations. It is found that, even in the absence of a background magnetic field, certain collective excitations (e.g., the helicon-like modes and anomalous Hall waves) are strongly affected by the chiral shift b. In a background magnetic field, the existence of distinctive longi- tudinal and transverse anomalous Hall waves with a linear dispersion relation is predicted. They originate from the oscillations of the electric charge density and electromagnetic fields, in which different components of the fields are connected via the anomalous Hall effect in Weyl semimetals. 
    more » « less