Page 135 - Introduction to Information Optics
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120                   2. Signal Processing with Optics

                                  Photorefractive
                                     midium






                                                      A3




                         Fig. 2.37. A four-wave mixing configuration.


         For example, if the index hologram is generated by the two writing beams
       A! and A 2 and this recorded hologram is illuminated by a counterpropagating
                      k2
       reading beam A 3e'  \ the diffraction can be written by

                               0(x) =                               (2.103)

       in which we see that the diffracted beam counterpropagates with respect to the
       writing beam A v If both the writing beam A 2 and reading beam A 3 are plane
       waves, the diffraction is a time-reserved replica of A l. Therefore, four-wave
       mixing provides a convenient method for the generation of phase conjugate
       waves. In general, however, all three waves can carry spatially modulated
       signals and the amplitude of the diffracted beam represents the multiplication
       of these three images. By suitably manipulating the diffracted beam, many
       image processing operations can be implemented.
         Beams A l and A 2 write a transmission-type hologram in the PR medium. If
       the beams A v and A 2 are used in the writing process, a reflection-type hologram
       is formed, which can be read with beam A 2 and generates the same diffraction
       beam as given by the preceding equation. Note that the transmission and
       reflection modes have different response times selectivities and diffraction
       efficiencies. They are suitable for different applications.
         Multiple images can be stored in a single piece of PR medium via wave
       multiplexing. Once these images are stored, they can be retrieved and can serve
       as a library of reference images for signal detection and pattern recognition.
       Due to the parallel readout and fast access capabilities of wave mixing storage,
       an input image can be compared with all the stored reference images at very
       high speed. The three most commonly used multiplexing schemes in volume
       holographic storage are angular multiplexing, wavelength multiplexing, and
       phase-code multiplexing. All three multiplexing options are based on Bragg-
       selective readout of thick holograms (discussed later).
         In an angular multiplexing scheme, the address of each image is represented
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