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CHAPTER4





                                       The Radon-Wigner



                                Transform in Analysis,


                              Design, and Processing



                                        of Optical Signals





               Walter D. Furlan and Genaro Saavedra
               Universitat de Val` encia, Optics Department
               Burjassot, Spain




          4.1 Introduction
               One of the main features of phase space is that its conjugate coor-
               dinates are noncommutative and cannot be simultaneously specified
               with absolute accuracy. As a consequence, there is no phase-space joint
               distribution that can be formally interpreted as a joint probability den-
               sity. Indeed, most of the classic phase-space distributions, such as the
               Wigner distribution function (WDF), the ambiguity function (AF), or
               the complex spectrogram, have difficult interpretation problems due
               to the complex, or negative, values they have in general. Besides, they
               may be nonzero even in regions of the phase space where either the
               signal or its Fourier transform vanishes. This is a critical issue, espe-
               cially for the characterization of nonstationary or nonperiodic signals.
               As an alternative, the projections (marginals) of the phase-space distri-
               butions are strictly positive, and as we will see later, they give informa-
               tion about the signal on both phase-space variables. These projections
               can be formally associated with probability functions, avoiding all
               interpretation ambiguities associated with the original phase-space
               distributions. This is the case of the Radon-Wigner transform (RWT),


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