Physics – Plasma Physics
Scientific paper
Dec 2011
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2011agufmsh43c1967r&link_type=abstract
American Geophysical Union, Fall Meeting 2011, abstract #SH43C-1967
Physics
Plasma Physics
[2164] Interplanetary Physics / Solar Wind Plasma, [7863] Space Plasma Physics / Turbulence
Scientific paper
The measured spectrum of kinetic Alfven wave (KAW) fluctuations in the turbulent solar wind plasma is used to calculate the electron and ion distribution functions resulting from quasi-linear diffusion. Quasi-linear diffusion establishes a step-like profile on the distribution function over parallel velocity [1]. The size of "plateau" vme/vte~0.5 , which can be created within the time of travel of solar wind plasma to the Earth ~ 10^5 s, is estimated for electrons as , while for ions vmi/vti~3. In this case the evolution of the ion tail distribution function can be approximated as ftail~exp(-vz^7/vmi^7). As a result, the Landau damping of KAW and whistlers in the high beta solar wind plasma is strongly diminished. Also the ion tail distribution function is found to be unstable to electromagnetic ion cyclotron (EMIC) waves [2]. These waves pitch angle scatter the parallel component of the ion velocity into the perpendicular velocity. With less than 1% of turbulent magnetic field energy in EMIC waves the perpendicular ion heating can be possible. [1] L. Rudakov et. al., Phys. Plasma, 18, 012307 (2011). [2] L. Rudakov et. al., arxiv.org:physics.plasm-ph:1012.2398v2, (2011b). * Supported by ONR.
Crabtree C. E.
Ganguli Gurudas
Mithaiwala Manish
Rudakov Leonid
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