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At large r, we recover the Fourier series of the 2 -periodic angle function:

[0, 2 )

The latter result can be equally understood in terms of the classical limit of these quantum objects Indeed, by reinjecting into our formulas physical dimensions, we know that the quantity |z|2 = r 2 acquires the dimension of an action and should appear in the formulas divided by the Planck constant Hence, the limit r in our previous expressions can also be considered as the classical limit

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0 Since we have at our disposal the number operator N = a a, which is, up to a constant shift, the quantization of the classical action, and an angle operator, we can examine their commutator and its lower symbol to measure the extent to which we get something close to the expected canonical value, namely, i IH The commutator reads as [Aarg , N ] = i

n+n +1 2 |n n | n!n !

(1215)

qc q (r) cos q = i C(r, ) ,

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(1216)

with the same c q (r) as in (1214) At small r, the function C(r, ) oscillates around 0 with amplitude equal to r: C(r, ) W r cos

At large r, the function C(r, ) tends to the Fourier series 2 q=1 cos q , whose convergence has to be understood in the sense of distributions Applying the Poisson summation formula, we get at r (or 0) the expected canonical behavior for (0, 2 ) More precisely, we obtain in this quasi-classical regime the following asymptotic behavior: (r, )|[Aarg , N ]|(r, ) W i + 2 i

( 2 n)

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(1217)

The fact that this commutator is not exactly canonical was expected since we know from Dirac [163] the impossibility of getting canonical commutation rules for the quantum versions of the classical action angle pair One can observe that the commutator symbol becomes canonical for = 2 n, n Z Dirac singularities are / located at the discontinuity points of the 2 -periodic extension of the linear function f ( ) = for [0, 2 )

It is commonly accepted that a coherent state diagonal representation of the type (123) is possible only for a restricted class of operators in H The reason is that we usually impose too strong conditions on the upper symbol f (z, z ) viewed as a classical observable on the phase space, and so subjected to belonging to the space of in nitely differentiable functions on R2 We already noticed that a reasonable phase or angle operator is easily built starting from the classical discontinuous periodic angle function The application of the same quantization method

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