By resorting to the Fock-Bargmann representation, we incorporate the q
uantum Weyl-Heisenberg algebra, q-WH, into the theory of entire analyt
ic functions. The q-WH algebra operators are realized in terms of fini
te difference operators in the z plane. In order to exhibit the releva
nce of our study, several applications to different cases of physical
interest are discussed; squeezed states and the relation between coher
ent states and theta functions on one side, and lattice quantum mechan
ics and Bloch functions on the other, are shown to find a deeper mathe
matical understanding in terms of q-WH. The role played by the finite
difference operators and the relevance of the lattice structure in the
completeness of the coherent states system suggest that the quantizat
ion of the WH algebra is an essential tool in the physics of discretiz
ed (periodic) systems. (C) 1995 Academic Press, Inc.