Other
Scientific paper
May 2007
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2007agusmsm43a..06a&link_type=abstract
American Geophysical Union, Spring Meeting 2007, abstract #SM43A-06
Other
2159 Plasma Waves And Turbulence, 2728 Magnetosheath
Scientific paper
The Earth's magnetosheath represents one of the natural laboratories of the collisionless plasma turbulence. The presence of the boundaries, the bow shock and the magnetopause, can play a crucial role in the turbulence nature. Here, as in the solar wind, the spectrum of magnetic fluctuations can be described by two well defined power laws separated by a spectral break, which is observed in the vicinity of the proton cyclotron frequency fcp. In the low frequency part, the magnetosheath turbulent spectrum follows a ~ f-1 law and it is ~ f-3 in the high frequency part. The low frequency part of the spectrum thus does not follow the Kolmogorov's f-5/3 law, as it is the case in the solar wind. But another important difference is that in the magnetosheath the spectral break is frequently accompanied by a large maximum. This maximum is usually interpreted by Alfvén Ion Cyclotron waves generated by the anisotropic ion distribution downstream of quasi- perpendicular bow shocks. We have established that this maximum corresponds to space-localized coherent magnetic structures in the form of Alfvén vortices [Alexandrova et al., JGR, 2006]. The Alfvén vortex is a non-linear cylindrical Alfvén wave, with an axis quasi- parallel to the mean magnetic field B0 and which is propagating in a plane perpendicular to B0. The frequent observation of such structures is an indication of their stability in the magnetosheath plasma. We discuss the role of the bow shock in the generation of the Alfvén vortex structures in the magnetosheath turbulence.
Alexandrova Olga
Mangeney Andre
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