In (2+1)-dimensional general relativity the path integral for a manifo
ld M can be expressed in terms of a topological invariant, the Ray-Sin
ger torsion of a flat bundle over M. For some manifolds, this makes an
explicit computation of transition amplitudes possible. In this paper
, the amplitude for a simple topology-changing process is evaluated. I
t is shown that certain amplitudes for spatial topology change are non
vanishing-in fact, they can be infrared divergent-but that they are in
finitely suppressed relative to similar topology-preserving amplitudes
.