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2.4. Fourier Transform Processing

                              \m[H( P,














                         Fig. 2.11. Complex amplitude transmittance.



       and the phase delay varies with the thickness of the spatial filter. Thus, a
       complex spatial filter in principle can be constructed by combining an
       amplitude filter and a phase-delay filter. However, in most cases, this would be
       very difficult to realize in practice.
          Let us now discuss the technique developed by Vander Lugt for construct-
       ing a complex spatial filter using a holographic technique, as shown in Fig.
       2.12. The complex light field over the spatial-frequency plane is

                           E(p, q) - F(p, q) + exp(-/a 0p),


       where oc 0 = / sin 6, f, the focal length of the transform lens, and

                           F(p, q) = \F(p, q)\ exp[z0(p, <?)].


                                      /(*, y)                         F(p,
















       Fig. 2.12. Holographic construction of a Fourier domain matched filter, /(x, y), input object
       transparency; R, reference plane wave; PH, photographic recording medium.
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