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1 and then including the number operator as Ae i N 2 = a in a similar way to that 1 i P B 2 N The commutation relation bein [193], where the authors used instead e tween both operators is [ , a ] = 1 N |N 1 N 1| , a (1495)

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which converges to the common result only when the expectation value is taken on states where extremal state components vanish as N tends to in nity As the phase operator is not built from a spectral decomposition, it is clear that A 2 = A2 and the link with an uncertainty relation is not straightforward as in [193] / Instead, as suggested in [195], a different de nition for the variance should be used The phase operator constructed here has most of the advantages of the Pegg Barnett operator but allows more freedom within the Hilbertian framework It is clear that a well-de ned phase operator must be parameterized by all points in the circle to have convergence to the commutation relation consistent with the classical limit It is also clear that the inconveniences due to the nonperiodicity of the phase pointed out in [190] are avoided from the very beginning by the choice of X = S 1





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In most of the introductory textbooks devoted to quantum mechanics the quantum versions of two simple models are presented, namely, the motion of a particle on the circle and in an interval (the in nite square well potential) In this chapter, we revisit these examples in the light of coherent state quantization of the corresponding phase spaces, namely, the cylinder [198] and an in nite strip in the plane [199, 200] We also apply our method to motion on the 1 + 1 de Sitter spacetime, since the corresponding phase space is topologically a cylinder We nally consider under the same angle a more exotic example, the motion on a discrete set of points as was presented in [201] under the name of shadow Schr dinger quantum mechanics

R j ( j + 1)

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For this exercise, highlight the macro, Snapshot OutPut to -, in the macro section of the database container and either click the Run button in the container or doubleclick the name. When the macro runs, it will display the report in Print Preview mode in one window and activate the Output to dialog box and prompt you for a name to save the snapshot file to. You can give it any name you want and click the OK button. After you have given it a name, Access will take the report and save it in snapshot view. Figure 29-21 shows the snapshot file in the Snapshot viewer of Microsoft Office.

(1724)

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in the above expansion (1722) of f (in the usual construction, this would j be J a instead of a ) We immediately note that the three operators (1724) obey the constraint ( a )2 + ( a )2 + ( a )2 = R 2 x x x and the commutation rules x a , x b = i ab c x c (1726) (1725)

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