An extension of the adiabatic factorization of the time evolution operator is
studied for spin in a general time varying magnetic field B(t). When B(t)
changes adiabatically, such a factorization reduces to the product of the
geometric operator which embodies the Berry phase phenomenon and a usual
dynamical operator. For a general time variation of B(t), there should be
another operator N(t) in the factorization that is related to non-adiabatic
transitions. A simple and explicit expression for the instantaneous angular
velocity of this operator is derived. This is done in a way that is independent
of any specific representation of spin. Two classes of simple conditions are
given under which the operator N(t) can be made explicit. As a special case,
a generalization of the traditional magnetic resonance condition is pointed
out.Comment: 10 page