The nature of the classical canonical phase-space variables for gravity sug
gests that the associated quantum field operators should obey affine commut
ation relations rather than canonical commutation relations. Prior to the i
ntroduction of constraints, a primary kinematical representation is derived
in the form of a reproducing kernel and its associated reproducing kernel
Hilbert space. Constraints are introduced following the projection operator
method, which involves no gauge fixing, no complicated moduli space, nor a
ny auxiliary fields. The result, which is only qualitatively sketched in th
e present paper, involves another reproducing kernel with which inner produ
cts are defined for the physical Hilbert space and which is obtained throug
h a reduction of the original reproducing kernel. Several of the steps invo
lved in this general analysis are illustrated by means of analogous steps a
pplied to one-dimensional quantum mechanical models. These toy models help
in motivating and understanding the analysis in the case of gravity. (C) 19
99 American Institute of Physics. [S0022-2488(99)02011-3].