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Instability of finite amplitude circularly polarized Alfven waves

Journal Article · · Astrophys. J.; (United States)
DOI:https://doi.org/10.1086/155829· OSTI ID:5188098
A circularly polarized, large-amplitude Alfven wave in a plasma with finite plasma ..beta.. is shown to be unstable. The wave decays by coupling to random density and magnetic fluctuations in the ambient medium. Daughter waves are produced at the sidebands which are at the first harmonic of the Alfven wave frequency and wavenumber. This is a four-wave coupling in which the initial Alfven wave excites forward-propagating density and magnetic waves as well as a backward-propagating magnetic wave. In general, the driven waves are not normal modes of the plasma, although in the limit of ..beta -->..0 the ''decay'' instability is recovered in which the density wave is ion-acoustic and one of the magnetic waves is a backward-propagating Alfven wave. For parameters more typical of the solar corona and solar wind, large decay rates are found for 0.1 < or =..beta..< or =1 and 0.1< or =eta< or =0.9, where eta is the ratio of magnetic energy density of the initial Alfven wave to that of the background magnetic field. The possible role played by this instability in several astrophysical situations is briefly considered.
Research Organization:
NASA/Goddard Space Flight Center, Laboratory for Extraterrestrial Physics, Greenbelt, Maryland
OSTI ID:
5188098
Journal Information:
Astrophys. J.; (United States), Journal Name: Astrophys. J.; (United States) Vol. 219:2; ISSN ASJOA
Country of Publication:
United States
Language:
English