Page 385 - Introduction to Information Optics
P. 385

370                   7. Pattern Recognition with Optics

       comparison, the output light distribution as obtained from the conventional
       JTC (CJTC) is provided in Fig. 7.17c. We see that the correlation peaks have
       been overwhelmed by the zero-order diffraction.
          In summary, besides the removal of the zero-order diffraction, there are
       other benefits of using NOJTC; for example, high diffraction efficiency and
       better utilization of SLM pixel elements. Despite these benefits, there is a small
       price to pay; NOJTC requires additional steps to capture and store the
       zero-order power spectra.



       7.2.3. POSITION-ENCODING JOINT-TRANSFORM DETECTION

          The JTC can perform the convolution of two functions without using a
       Fourier-domain filter, and it can also be used as a general optical processor.
       Even though the JTC usually has a lower detection efficiency, the architecture
       has certain merits. For instance, it does not have the stringent filter alignment
       problem as does VLC. It is suitable for real-time implementation and more
       robust to environment perturbation. To realize a spatial-domain filter in a
       JTC, complex function implementation is often needed. It is, however, possible
       to obtain complex-valued reference functions with an amplitude-modulated
       SLM.
                                                                       f
          It is well known that a real function can be decomposed into c^, + c 2 l>i,
       and a complex function can be decomposed into tj</> 0 + t' 20 2/3 + r 3<^ 4/3, where
       t-j, c 2, and c 3 are nonnegative coefficients, and <p k = exp(m/c) are elementary
       phase vectors. The decompositions can be optically realized with position
       encoding, as illustrated in Fig. 7.18.
          A proof-of-concept experiment is shown in Fig. 7.19. Position-encoded
             U
       letters £T and "F" are shown in Fig. 7.19a and the corresponding output
       correlation distribution is shown in Fig. 7.19b. The autocorrelation peaks for
       detecting F can readily be seen; they were measured to be about twice as high



                                          CCL
                                               Cl X FOB
                                                    \
                                                     \   /T
                                             >C 2
                                                  • r '^
                                                 -,.
                                               C3 OK>
                                            -> J^
                                              3dsin0=X


       Fig. 7.18. Optical realization of (a) real value and (b) complex value representations with a
       position encoding method. CCL: coherent coliminated light; FOD: first-order diffraction.
   380   381   382   383   384   385   386   387   388   389   390