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40   Chapter One



          1.9 Conclusion
               WehavepresentedanoverviewoftheWignerdistributionandofsome
               of its properties and applications in an optical context. The Wigner
               distribution describes a signal in space (i.e., position) and spatial fre-
               quency (i.e., direction) simultaneously and can be considered as the
               local frequency spectrum of the signal, like the score in music and the
               phase space in mechanics. Although it is derived in terms of Fourier
               optics, the description of a signal by means of its Wigner distribution
               closelyresemblestherayconceptingeometricaloptics.Itthuspresents
               a link between Fourier optics and geometrical optics. Moreover, the
               concept of the Wigner distribution is not restricted to deterministic
               signals (i.e., completely coherent light); it can be applied to stochastic
               signals (i.e., partially coherent light) as well, thus presenting a link
               between partial coherence and radiometry.
                 Properties of the Wigner distribution and its propagation through
               linear systems have been considered; the corresponding description
               of signals and systems can be directly interpreted in geometric-optical
               terms. For first-order optical systems, the propagation of the Wigner
               distribution is completely determined by the system’s ray transfor-
               mation matrix, thus presenting a strong interconnection with matrix
               optics.
                 We have studied the second-order moments of the Wigner distribu-
               tion and some interesting combinations of these moments, together
               with the propagation of these moment combinations through first-
               order optical systems. Special attention has been paid to systems that
               perform rotations in phase space.
                 In the case of completely coherent light, the Wigner distribution is
               a member of a broad class of bilinear signal representations, known
               as the Cohen class. Each member of this class is related to the Wigner
               distribution by means of a convolution with a certain kernel. Because
               of the quadratic nature of such signal representations, they suffer from
               unwanted cross-terms, which one tries to minimize by a proper choice
               of this kernel. Some members of the Cohen class have been reviewed,
               and special attention was devoted to the smoothed interferogram
               in combination with the optimal angle in phase space in which the
               smoothing takes place.




          References
                1. E. Wigner, “On the quantum correction for thermodynamic equilibrium,” Phys.
                  Rev. 40, 749–759 (1932).
                2. L. S. Dolin, “Beam description of weakly-inhomogeneous wave fields,” Izv.
                  Vyssh. Uchebn. Zaved. Radiofiz. 7, 559–563 (1964).
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