Page 180 - Phase Space Optics Fundamentals and Applications
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The Radon-Wigner Transform     161


                 1.00
                                        Fractional correlation intensity 1.0
               p
                 0.75

                                         0.5
                 0.50

                                                                     1.0
                 0.25                    0.0                      0.6 0.8
                                                                 Fractional order p
                                                  0            0.2 0.4
                 0.00                       Space coordinate (x)  0.0
                           0
                           x
                                           (a)
                 1.00
                p                       1.0
                                        Fractional correlation intensity  0.5
                 0.75


                 0.50


                 0.25                                              0.8
                                                                    1.0
                                                                Fractional order p
                 0.00                    0.0      0           0.2 0.4 0.6
                           0                Space coordinate (x)  0.0
                           x
                                           (b)

               FIGURE 4.36 Multichannel fractional autocorrelation of the function
               represented in Fig. 4.35 with (a) a shift in the input plane of one-half of the
               object size and (b) a shift of the whole size of the object.



               shift-variant property becomes evident for values close to p = 0.25.
               It can be seen that as the fractional order becomes lower, the peak
               degenerates and shifts disproportionately toward the object position.
               Thus, the output of the system shows a variable degree of space vari-
               ance ranging from the pure shift variance case p = 0 to the pure shift
               invariance case p = 1, that is, the classic correlation. This kind of
               representation provides information about the object, such as classic
               correlation, but also quantifies its departure from a given reference
               position.
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