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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 )



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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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to the free particle time q/ p, which is obviously singular at p = 0, was carried out in [160] and yields a fairly reasonable time operator for the free motion on the line Owing to the general expression (128) for matrix elements of the quantized version of an observable f, one can immediately think of extending the method to tempered distributions In particular, we will show that any simple operator nn = |n n | also has a coherent state diagonal representation by including distributions on R2 in the class of classical observables In (128), the functions (z, z ) e |z| z n z n

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are rapidly decreasing C functions on the plane with respect to the canonical coordinates (q, p), or equivalently with respect to the coordinates (z, z ): they belong to the Schwartz space S(R2 ) The use of complex coordinates is clearly more adapted to the present context, and we adopt the following de nitions and notations for tempered distributions Firstly, any function f (z, z ) that is slowly increasing and locally integrable with respect to the Lebesgue measure d 2 z on the plane de nes a regular tempered distribution T f , that is, a continuous linear form on the vector space S(R2 ) equipped with the usual topology of uniform convergence at each order of partial derivatives multiplied by polynomial of arbitrary degree [164] This de nition rests on the map S(R2 ) T f, =

d 2 z f (z, z ) (z, z ) ,

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