“…In [3], it was shown and verified by comparison with experiment that, for a weakly nonideal gas plasma in the range of classical motion under high magnetic field conditions, i.e., when the Thomson formula for the collisional recombina tion coefficient has the form (9) Taking into account the complete analogy between the physical processes in these two physical systems, we can rewrite (8) for the case of the high magnetic field as (10)…”