DO LARMOR-SCALE INSTABILITIES AFFECT THE GLOBAL DYNAMICS OF WEAKLY COLLISIONAL MAGNETIZED ASTROPHYSICAL PLASMAS ?

F. Rincon, Laboratoire d'Astrophysique de Toulouse-Tarbes,

joint work with M. S. Rosin, A. A. Schekochihin, S. C. Cowley.


The large-scale features and dynamics of many objects in the Universe depend very strongly on how small-scale turbulence affects the transport properties of astrophysical plasmas. This critical transport problem has so far mostly been studied in the fluid MHD framework, whereas many turbulent magnetized astrophysical plasmas, such as the solar wind, the intracluster medium or plasma accreted onto black holes are thought to be only weakly collisional. How the couplings between turbulence and kinetic processes affect transport and magnetic field generation in this kind of environment is very poorly understood at the moment. In weakly collisional, high-beta magnetized plasmas, a suspected very important effect is that large-scale, field-stretching motions, by generating pressure anisotropies with respect to the local field, trigger extremely fast mirror and firehose instabilities at microscopic scales comparable to the ion Larmor radius.
As a first step towards understanding the dynamical macroscopic consequences of these instabilities, we present a kinetic theory of the nonlinear development of the parallel firehose instability with finite Larmor radius effects. We show that this process leads to a significant modification of the local magnetic field geometry and that any firehose-unstable pressure anisotropy evolves nonlinearly towards its critical value for instability in the course of the process. We finally discuss the possible consequences of this evolution for turbulence and magnetic field generation in weakly collisional astrophysical plasmas.