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2.2. Processing under Coherent and Incoherent Illumination  75

       which describes a completely coherent illumination, where K 2 is a propor-
       tionality constant. In other words, a monochromatic point source describes a
       strictly coherent processing regime, while an extended source describes a
       strictly incoherent system. Furthermore, an extended monochromatic source is
       also known as a spatially incoherent source.
          By referring to the completely incoherent illumination, we have

                          r(.v, .y; x'y') = Kj(S(.x'


       and the intensity distribution at the output plane can be shown as


                                              2
                                                      2
                      /(a, ft = IT |/!(a - x, /? - y)!  /(.x, >')|  dxdy,  (2,14)

       in which we see that the output intensity distribution is the convolution of the
       input signal intensity with respect to the intensity impulse response. In other
       words, for the completely incoherent illumination, the optical signal processing
       system is linear in intensity, that is,


                                                                     (2.15)

       where the asterisk denotes the convolution operation. On the other hand, for
       the completely coherent illumination; i.e., F(x. y;x'y') = K 2, the output inten-
       sity distribution can be shown as


                 /(a, 0) = 0(a, /%*(a, P) = \\ h(a - x, fi - y)/(x, y) dxdy
                                       JJ                            (2.1.6)

                             h*(a - x', fi - y')f*(x', y') dxdy'


       when



                       0(a, P)=\\ h(a - x, p - >-)/(x, y) dxdy,       (2.17)


       for which we can see that the optical signal processing system is linear in
       complex amplitude. In other words, a coherent optical processor is capable of
       processing the information in complex amplitudes.
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