Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperature

Propagation of large-amplitude waves in plasmas is subject to several sources of nonlinearity due to relativistic effects, either when particle quiver velocities in the wave field are large, or when thermal velocities are large due to relativistic temperatures. Wave propagation in these conditions h...

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Main Authors: V. Muñoz, F. A. Asenjo, M. Domínguez, R. A. López, J. A. Valdivia, A. Viñas, T. Hada
Format: Article
Language:English
Published: Copernicus Publications 2014-02-01
Series:Nonlinear Processes in Geophysics
Online Access:http://www.nonlin-processes-geophys.net/21/217/2014/npg-21-217-2014.pdf
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author V. Muñoz
F. A. Asenjo
M. Domínguez
R. A. López
J. A. Valdivia
A. Viñas
T. Hada
author_facet V. Muñoz
F. A. Asenjo
M. Domínguez
R. A. López
J. A. Valdivia
A. Viñas
T. Hada
author_sort V. Muñoz
collection DOAJ
description Propagation of large-amplitude waves in plasmas is subject to several sources of nonlinearity due to relativistic effects, either when particle quiver velocities in the wave field are large, or when thermal velocities are large due to relativistic temperatures. Wave propagation in these conditions has been studied for decades, due to its interest in several contexts such as pulsar emission models, laser-plasma interaction, and extragalactic jets. <br><br> For large-amplitude circularly polarized waves propagating along a constant magnetic field, an exact solution of the fluid equations can be found for relativistic temperatures. Relativistic thermal effects produce: (a) a decrease in the effective plasma frequency (thus, waves in the electromagnetic branch can propagate for lower frequencies than in the cold case); and (b) a decrease in the upper frequency cutoff for the Alfvén branch (thus, Alfvén waves are confined to a frequency range that is narrower than in the cold case). It is also found that the Alfvén speed decreases with temperature, being zero for infinite temperature. <br><br> We have also studied the same system, but based on the relativistic Vlasov equation, to include thermal effects along the direction of propagation. It turns out that kinetic and fluid results are qualitatively consistent, with several quantitative differences. Regarding the electromagnetic branch, the effective plasma frequency is always larger in the kinetic model. Thus, kinetic effects reduce the transparency of the plasma. As to the Alfvén branch, there is a critical, nonzero value of the temperature at which the Alfvén speed is zero. For temperatures above this critical value, the Alfvén branch is suppressed; however, if the background magnetic field increases, then Alfvén waves can propagate for larger temperatures. <br><br> There are at least two ways in which the above results can be improved. First, nonlinear decays of the electromagnetic wave have been neglected; second, the kinetic treatment considers thermal effects only along the direction of propagation. We have approached the first subject by studying the parametric decays of the exact wave solution found in the context of fluid theory. The dispersion relation of the decays has been solved, showing several resonant and nonresonant instabilities whose dependence on the wave amplitude and plasma temperature has been studied systematically. Regarding the second subject, we are currently performing numerical 1-D particle in cell simulations, a work that is still in progress, although preliminary results are consistent with the analytical ones.
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spelling doaj.art-69e6a197a60144ff9ccd3b3ab8f76d102022-12-22T00:58:03ZengCopernicus PublicationsNonlinear Processes in Geophysics1023-58091607-79462014-02-0121121723610.5194/npg-21-217-2014Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperatureV. Muñoz0F. A. Asenjo1M. Domínguez2R. A. López3J. A. Valdivia4A. Viñas5T. Hada6Departamento de Física, Facultad de Ciencias, Universidad de Chile, Casilla 653, Santiago, ChileDepartamento de Ciencias, Facultad de Artes Liberales, Facultad de Ingeniería y Ciencias, Universidad Adolfo Ibáñez, Santiago, ChileDepartamento de Física, Facultad de Ciencias, Universidad de Chile, Casilla 653, Santiago, ChileDepartamento de Física, Facultad de Ciencias, Universidad de Chile, Casilla 653, Santiago, ChileDepartamento de Física, Facultad de Ciencias, Universidad de Chile, Casilla 653, Santiago, ChileNASA Goddard Space Flight Center, Heliophysics Science Division, Geospace Physics Laboratory, Greenbelt, MD, USADepartment of Earth System Science and Technology, Kyushu University, Fukuoka, Fukuoka Prefecture 812-8581, JapanPropagation of large-amplitude waves in plasmas is subject to several sources of nonlinearity due to relativistic effects, either when particle quiver velocities in the wave field are large, or when thermal velocities are large due to relativistic temperatures. Wave propagation in these conditions has been studied for decades, due to its interest in several contexts such as pulsar emission models, laser-plasma interaction, and extragalactic jets. <br><br> For large-amplitude circularly polarized waves propagating along a constant magnetic field, an exact solution of the fluid equations can be found for relativistic temperatures. Relativistic thermal effects produce: (a) a decrease in the effective plasma frequency (thus, waves in the electromagnetic branch can propagate for lower frequencies than in the cold case); and (b) a decrease in the upper frequency cutoff for the Alfvén branch (thus, Alfvén waves are confined to a frequency range that is narrower than in the cold case). It is also found that the Alfvén speed decreases with temperature, being zero for infinite temperature. <br><br> We have also studied the same system, but based on the relativistic Vlasov equation, to include thermal effects along the direction of propagation. It turns out that kinetic and fluid results are qualitatively consistent, with several quantitative differences. Regarding the electromagnetic branch, the effective plasma frequency is always larger in the kinetic model. Thus, kinetic effects reduce the transparency of the plasma. As to the Alfvén branch, there is a critical, nonzero value of the temperature at which the Alfvén speed is zero. For temperatures above this critical value, the Alfvén branch is suppressed; however, if the background magnetic field increases, then Alfvén waves can propagate for larger temperatures. <br><br> There are at least two ways in which the above results can be improved. First, nonlinear decays of the electromagnetic wave have been neglected; second, the kinetic treatment considers thermal effects only along the direction of propagation. We have approached the first subject by studying the parametric decays of the exact wave solution found in the context of fluid theory. The dispersion relation of the decays has been solved, showing several resonant and nonresonant instabilities whose dependence on the wave amplitude and plasma temperature has been studied systematically. Regarding the second subject, we are currently performing numerical 1-D particle in cell simulations, a work that is still in progress, although preliminary results are consistent with the analytical ones.http://www.nonlin-processes-geophys.net/21/217/2014/npg-21-217-2014.pdf
spellingShingle V. Muñoz
F. A. Asenjo
M. Domínguez
R. A. López
J. A. Valdivia
A. Viñas
T. Hada
Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperature
Nonlinear Processes in Geophysics
title Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperature
title_full Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperature
title_fullStr Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperature
title_full_unstemmed Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperature
title_short Large-amplitude electromagnetic waves in magnetized relativistic plasmas with temperature
title_sort large amplitude electromagnetic waves in magnetized relativistic plasmas with temperature
url http://www.nonlin-processes-geophys.net/21/217/2014/npg-21-217-2014.pdf
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