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Asymptotic kinetic theory of magnetized plasmas : quasi-particle concept
Petro P. Sosenko 1, 2, Anatoly H. Zagorodny 1, 2
(2004-06-14)

The asymptotic kinetic theory of magnetized plasmas is elaborated within the context of general statistical approach and asymptotic methods, developed by M. Krylov and M. Bohol'ubov, for linear and non-linear dynamic systems with a rapidly rotating phase. The quasi-particles are introduced already on the microscopic level. Asymptotic expansions enable to close the description for slow processes, and to relate consistently particles and guiding centres to quasi-particles. The kinetic equation for quasi-particles is derived. It makes a basis for the reduced description of slow collective phenomena in the medium. The kinetic equation for quasi-particles takes into account self-consistent interaction fields, quasi-particle collisions and collective-fluctuation-induced relaxation of quasi-particle distribution function. The relationships between the distribution functions for particles, guiding centres and quasi-particles are derived taking into account fluctuations, which can be especially important in turbulent states. In this way macroscopic (statistical) particle properties can be obtained from those of quasi-particles in the general case of non-equilibrium media.
1:  Physique des milieux ionisés et applications (LPMIA)
CNRS : UMR7040 – Université Henri Poincaré - Nancy I
2:  International Centre of Physics
International Centre of Physics
Physics/Physics/Plasma Physics
magnetized plasma – asymptotic methods – quasi-particles – kinetic equations – fluctuations and turbulence
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