Page 680 - Introduction to Information Optics
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664                   11. Information Display with Optics

        11.42 N. Mukohzaka, N. Yoshida, H. Toyoda, Y. Kobayashi, and T. Hara, 1994, "Diffraction
            Efficiency Analysis of a Parallel-Aligned Nematic Liquid Crystal Spatial Light Modulator."
            App. Opt., 33, 2804-2811.
       11.43 P.-G. de Gennes, The Physical of Liquid Crystals, Clarendon Press, Oxford, 1974.
        11,44 T.-C. Poon, experiments conducted at Research Institute of Electronics, Shizuoka Univer-
            sity, Hamamatsu, Japan, 1997.
        J 1.45 F. T. S. Yu and S. Jutamulia, eds., Optical Pattern Recognition, Cambridge University Press,
            1998.





       EXERCISES


        11.1 For the system of equations given in Eq. (11.9)
                                                 2     2       2
             (a) Show the energy of conservation: \E 0\  + JEJ  = l£ inc| .
             (b) Solve for E 0 and E v for a* = a = a.
        11.2 Verify that Eq. (11.lie) is the solution for Eq. (11.9) when (5 = 0.
        11.3 Starting from Eq. (11.8) with a* = a = a, and assuming that Q = 0 for
             normal incidence (i.e., 0 inc = 0), find the solutions under this situation.
             This situation is known as the ideal Raman-Nath regime for the
             acousto-optic modulator.
        11.4 Design an acousto-optic intensity modulation system based on Raman-
             Nath diffraction. We want to use the zeroth-order light for transmission
             of information. Sketch an optical system that would do the job.
        11.5 Consider an acousto-optic deflector. If the interaction length is 10mm
             and its center frequency is ISOMhz, estimate the number of resolvable
             spots and the transit time of the deflector if the laser beam width is 2 mm
             and its wavelength is 0.6 /an. We assume that the sound velocity in the
             acoustic medium is 4000 m/s.
       11.6 Verify the three equations given by Eq. (11.23).
                                                                     2
        11.7 A point-object hologram is given of the form as bias + cos(k 0x /2z 0),
             where the wavenumber of the recording light is k 0 and z 0 is the location
             of the point away from the holographic film. Find the real image
             location of the point upon illumination by plane wave of light with
             wavenumber k l.
        11.8 For the hologram given by Exercise xll.7, we now assume that the
             recording film has a finite resolution limit in such a way that NA is
             given. Estimate the spot size of the reconstructed real image in terms of
             NA.
       11.9 A three-point object given by S(x, y; z — z 0) + <5(x — x 0, y; z — z 0) +
             S(x,y;z — (z 0 + Az 0)) is scanned by the time-dependent Fresnel zone
             plate expressed by Eq. (11.26). Find an expression for its hologram,
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