We derive (quasi-)quantum groups in 2 + 1 dimensional topological fiel
d theory directly from the classical action and the path integral. Det
ailed computations are carried out for the Chem-Simons theory with fin
ite gauge group. The principles behind our computations are presumably
more general. We extend the classical action in a d + 1 dimensional t
opological theory to manifolds of dimension less than d + 1. We then '
'construct'' a generalized path integral which in d + 1 dimensions red
uces to the standard one and in d dimensions reproduces the quantum Hi
lbert space. In a 2 + 1 dimensional topological theory the path integr
al over the circle is the category of representations of a quasi-quant
um group. In this paper we only consider finite theories, in,which the
generalized path integral reduces to a finite sum. New ideas are need
ed to extend beyond the finite theories treated here.