1. Test Particles in a Completely Ionized Plasma
2. On Bogoliubov's kinetic equation for a spatially homogeneous plasma
3. It is assumed that hn(υ⊥,υz;p) has no poles in whichphas a positive real part. The class of admissible functions f(0)(υ⊥,υz) is therefore restricted to stable distribution functions, i.e., functions for which there are no solutions of ɛ(k,p) = 0 in whichphas a positive real part. ɛ(k,p is defined in Eq. (24).