Andrew wanted me to post something I wrote on my essay blog area. This concerns a difficulty I see with Klauder's quantization. I do this with some trepidation I must confess, for I have noticed that when I point to a problem with some claimed physics this results in down votes.
Here is the problem with Klauder's idea. I have to use parentheses for langle and rangle or bra-ket stuff because this system snags up on those. If we have quantum states П€(p,r,t) = (П€(t)|p,r) then the operators bf p and bf r (bf before letter stands for operators) act on the wave function
bf pbf rП€(p,r,t) = (П€(t) bf |pbf r|p,r) = (П€(t)| bf pr|p,r) = pr(П€(t)|p,r)
and similarly I can write
bf rbf pП€(p,r,t) = (П€(t)| bf rbf p|p,r) = (П€(t)| bf rp|p,r) =rp(П€(t)|p,r)
where r and p are just eigenvalues or numbers and so rp = pr. We can then conclude [bf p, bf r] = 0, which is a big oopsie. I hinted at this problem and he responded in a way that was a bit testy. There is a problem with pointing out a possible error in somebody's paper in that they can one-bomb you.
Klauder maintains we can have a position and momentum representation of QM simultaneously. This is generally not admitted. In your paper you use the Schrödinger equation i∂ψ/∂t =Hψ to get under "langle rangle" pdq - Hdt in the classical setting. This turns out to be alright in general.
Quantum mechanics has only one representation at once. Either one has the position or momentum configurations. This hearkens back to the Heisenberg uncertainty principle. The operators used in a representation act on the variables of that representation. Unfortunately Klauder is trying to do QM in incommensurate variables or operators.
Cheers LC