We discuss a class of representations of quantum mechanics which uses funct
ions defined on a parameter space to represent observable quantities. We sh
ow that infinitesimal canonical transformations could be used to introduce
a phase-space-like structure consistent with the requirements of quantum me
chanics. The resulting family of phase-space representations of quantum mec
hanics contains many well-known representations as special cases, e.g., the
Weyl-Wigner-Moyal, normal and antinormal one. It is also flexible enough t
o represent, e.g., PT-symmetric theories, introduced recently within the co
ntext of non-Hermitian quantum mechanics. (C) 2001 Elsevier Science B.V. Al
l rights reserved.