We re-examine three issues, the Hopf term, fractional spin and the sol
iton operators, in the 2 + 1 dimensional O(3) non-linear sigma model b
ased on the adjoint orbit parametrization (AOP) introduced earlier. It
is shown that the Hopf term is well defined for configurations of any
soliton charge Q if we adopt a time-independent boundary condition at
spatial infinity. We then develop the Hamiltonian formulation of the
model in the AOP and thereby argue that the well-known Q(2) formula fo
r fractional spin holds only for a restricted class of configurations.
Operators that create states of given classical configurations of any
soliton number in the (physical) Hilbert space are constructed. Our r
esults clarify some of the points that are crucial for the above three
topological issues and yet have remained obscure in the literature. (
C) 1998 Elsevier Science B.V.