The Hopf term in the (2 + 1)-dimensional O(3) nonlinear sigma model, w
hich is known to be responsible for fractional spin and statistics, is
re-examined from the viewpoint of quantization ambiguity. It is confi
rmed that the Hopf term can be understood as a term induced quantum me
chanically, in precisely the same manner as the theta-term in QCD, We
present a detailed analysis of the topological aspect of the model bas
ed on the adjoint orbit parametrization of the spin vectors, which is
not only very useful in handling topological (soliton and/or Hopf) num
bers, but also plays a crucial role in defining the Hopf term for conf
igurations of nonvanishing soliton numbers. The Hopf term is seen to a
rise explicitly as a quantum effect which emerges when quantizing an S
-1 degree of freedom hidden in the configuration space. (C) 1998 Elsev
ier Science B.V.