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2   Chapter One


               in Fourier-optical terms, the Wigner distribution will form a link to
               such diverse fields as geometrical optics, ray optics, matrix optics, and
               radiometry.
                 Sections 1.2 through 1.7 mainly deal with optical signals and sys-
               tems. We treat the description of completely coherent and partially
               coherent light fields in Sec. 1.2. The Wigner distribution is introduced
               in Sec. 1.3 and elucidated with some optical examples. Properties of
               the Wigner distribution are considered in Sec. 1.4. In Sec. 1.5 we restrict
               ourselves to the one-dimensional case and observe the strong connec-
               tion of the Wigner distribution to the fractional Fourier transformation
               and rotations in phase space. The propagation of the Wigner distri-
               bution through Luneburg’s first-order optical systems is the topic of
               Sec. 1.6, while the propagation of its moments is discussed in Sec. 1.7.
               The final Sec. 1.8 is devoted to the broad class of bilinear signal repre-
               sentations known as the Cohen class, of which the Wigner distribution
               is an important representative.









          1.2 Elementary Description of Optical
                Signals and Systems
               We consider scalar optical signals, which can be described by, say,
                ˜
                f (x, y, z, t), where x, y, z denote space variables and t represents the
               time variable. Very often we consider signals in a plane z = constant,
               in which case we can omit the longitudinal space variable z from the
               formulas. Furthermore, the transverse space variables x and y are
               combined into a two-dimensional column vector r. The signals with
                                                              ˜
               which we are dealing are thus described by a function f (r,t).
                 Although real-world signals are real, we will not consider these
                                       ˜
               signals as such. The signals f (r,t) that we consider in this chapter are
               analytic signals, and our real-world signals follow as the real part of
               these analytic signals.
                 Throughout we denote column vectors by boldface lowercase sym-
               bols, while matrices are denoted by boldface uppercase symbols;
               transposition of vectors and matrices is denoted by the superscript t.
               Hence, for instance, the two-dimensional column vectors r and q rep-
                                                                        t
                                                              t
               resent the space and spatial-frequency variables [x, y] and [u, v] ,
                               t
               respectively, and q r represents the inner product ux + vy. Moreover,
               in integral expressions, dr and dq are shorthand notations for dx dy
               and du dv, respectively.
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