The kinetic theory of the stationary and nonstationary thermal filamentatio
n instability in fully ionized plasmas is presented. The collisionless tran
sport limit is modeled by new transport coefficients corresponding to the c
onvective heat flux and the temperature anisotropy. It is shown, in particu
lar, that these effects decrease the instability growth rates by about a fa
ctor of 2, in conditions typical of current experiments. These two effects,
combined with the collisional absorption of the light energy by the plasma
electrons, lead to a thermal growth rate comparable to the one due to the
ponderomotive drive. The comparison of the results obtained in this work wi
th the principal results established in the literature, is also presented.
(C) 1999 American Institute of Physics. [S1070-664X(99)00509-1].