Page 655 - Introduction to Information Optics
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11.3. 3-D Holographic Display            639
       where A and B are constants, representing the amplitude of the plane wave and
       the diverging spherical wave, respectively. The frequencies co 0 + Q and co 0 are
       the temporal frequencies of the plane wave and the spherical wave, respectively.
       The parameter z is a depth parameter measured away from the focal plane of
       lens L (which is on the surface of the 2-D scanning mirrors) toward the 3-D
       object. Equation (11.25) can be expanded and written as


                                   2
                              2
                                                        2
                  I(x, y; Q) = A  + C  + 2AC sin    + v )+n r       (11.26)
       where C = Bk 0/2izz. This is a familiar Fresnel zone plate (FZP) expression
       (see Eq. [11.21]) but has a time-dependent variable. We shall call it a time-
       dependent Fresnel zone plate (TDFZP). This TDFZP is now used to scan the
       3-D object in two dimensions and the photodetector collects all the transmitted
       light. For the sake of explaining the concept, let us assume that a single off-axis
       point object 8(x — x 0, y — y 0) is located Z Q away from the focal plane of lens
       L. The scanning of the TDFZP on the point object will cause the photodetec-
       tor to deliver a heterodyne-scanned current z(x, y; z, t) given by



                                                        2
                                                                      1 27
                                                   - Vo) ] + «4-    d -  )
       After electronic multiplying with sin(iQf) and low-pass filtering, the scanned
       demodulated electrical signal i d, as indicated in Fig. 11.17, is given by


                                              2
                                                         2
                      i d(x, y) ~ cos \^- [(x - x 0)  + (y - >' 0) ] j ,  ( H -28)
                                   z
                                 C^ o                    J
       where x and y in the above equation are determined by the motion of the
       scanning mechanism. Note that the electrical signal i d contains the location
       (x 0, y 0) as well as the depth (z 0) information of the off-axis point object. If this
       scanned demodulated signal is stored in synchronization with the x — y scan
       signals of the scanning mechanism, then what is stored is the 3-D information
       of the object or a hologram and the transmission function of the hologram is
       t s(x, y) oc i d(x, y). Hence t d(x, y) is the hologram of 6(x — x 0, y — y 0) when it is
       located z 0 from the focus of the spherical wave which is used to generate the
       scanning time-dependent Fresnel zone plate. This way of generating holo-
       graphic information is nowadays commonly known as electronic holography
       [25].
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