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7.7. Pattern Recognition with Photorefractive Optics  405













                    8o(x)          -> x
                          output plane
       Fig. 7.42. A PR-based RC. g 0(x), reference target; g t(x), input scene; /c (), reference beam.




       where v\ is the refractive index of the PR crystal, and /' is the apparent (or
       actual) focal length, which is given by


                                                                     (7.54)


       Thus, the allowable thickness of the PR crystal filter is limited by

                                t = 25'                              (7,55)


       in which we assume that the thick-crystal filter is centered at the apparent focal
       length /'. By using the coupled-wave theory, the output correlation peak
       intensity can be shown as

                                             nt S(x 0 — S)
                                      2
                                  \g 0(x)\  sine         dx          (7.56)
                              -b/2
       The width of the sine factor is given by

                                    „,  2 ^/' 2                      (7.57)
                                          st

       To maintain a high correlation peak intensity, the target width should be
       adequately small, such as
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