The propagator of a spinning particle in an external Abelian field and
in arbitrary dimensions is presented by means of a path integral. The
problem has distinct solutions in even and odd dimensions. In even di
mensions the representation is just a generalization of the one in fou
r dimensions (which is already known), In this case the gauge invarian
t part of the effective action in the path integral has the form of th
e standard (Berezin-Marinov) pseudoclassical action, In odd dimensions
the solution is presented for the first time and, in particular, it t
urns out that the gauge invariant part of the effective action differs
from the standard one, We propose this new action as a candidate to d
escribe spinning particles in odd dimensions, Studying the Hamiltoniza
tion of the pseudoclassical theory with the new action we show that th
e operator quantization leads to an adequate minimal quantum theory of
spinning particles in odd dimensions, Finally the consideration is ge
neralized for the case of a particle with an anomalous magnetic moment
.