  We report the results of our numerical simulation of classical-dissipative
dynamics of a charged particle subjected to a non-markovian stochastic forcing.
We find that the system develops a steady-state orbital magnetic moment in the
presence of a static magnetic field. Very significantly, the sign of the
orbital magnetic moment turns out to be {\it paramagnetic} for our choice of
parameters, varied over a wide range. This is shown specifically for the case
of classical dynamics driven by a Kubo-Anderson type non-markovian noise.
Natural spatial boundary condition was imposed through (1) a soft (harmonic)
confining potential, and (2) a hard potential, approximating a reflecting wall.
There was no noticeable qualitative difference. What appears to be crucial to
the orbital magnetic effect noticed here is the non-markovian property of the
driving noise chosen. Experimental realization of this effect on the laboratory
scale, and its possible implications are briefly discussed. We would like to
emphasize that the above steady-state classical orbital paramagnetic moment
complements, rather than contradicts the Bohr-van Leeuwen (BvL) theorem on the
absence of classical orbital diamagnetism in thermodynamic equilibrium.
