We reexamine the semiclassical approximation for quantum gravity in th
e canonical formulation, focusing an the definition of a quasiclassica
l state for the gravitational field. It is shown that a state with cla
ssical correlations must be a superposition of states of the form e(iS
) In terms of a reduced phase-space formalism, this type of state-can
be expressed as a coherent superposition of eigenstates of operators t
hat commute with the constraints and so correspond to constants of the
motion. Contact is made witt the usual semiclassical approximation by
showing that a superposition of this kind can be approximated by a WK
B state with an appropriately localized prefactor. A qualitative analy
sis is given of the effects of geometry fluctuations, and the possibil
ity of a breakdown of the semiclassical approximation due to interfere
nce between neighboring classical trajectories is discussed. It is sho
wn that a breakdown in the semiclassical approximation can be a coordi
nate-dependent phenomenon, as has been argued to be the case close to
a black hole horizon.