In connection with fundamental issues relevant to magnetized target fusion,
the distribution function of thermonuclear alpha particles produced in sit
u in a dense, hot, and strongly magnetized hydrogenic plasma considered ful
ly ionized in a cylindrical geometry is investigated. The latter is assumed
in local thermodynamic equilibrium with Maxwellian charged particles. The
approach is based on the Fokker-Planck equation with isotropic source S and
loss s terms, which may be taken arbitrarily under the proviso that they r
emain compatible with a steady state. A novel and general expression is the
n proposed for the isotropic and stationary distribution f(v). Its time-dep
endent extension is worked out numerically. The solutions are valid for any
particle velocity v and plasma temperature T. Higher order magnetic and co
llisional corrections are also obtained for electron gyroradius larger than
Debye length. f(v) moments provide particle diffusion coefficient and heat
thermal conductivity. Their scaling on collision time departs from Bragins
ki's. (C) 2000 American Institute of Physics. [S1070-664X(00)00211-1].