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Super Resolved Imaging in Wigner-Based Phase Space      205












                            (a)                           (b)

               FIGURE 6.6 (a) Low-resolution Lena image containing 3 bits of dynamic
               range; (b) super resolved reconstruction using gray-level multiplexing.


                 In Fig. 6.6 we simulated this approach by taking Lena image con-
               taining 3 bits of gray level and coded it with gray-level mask similar to
               the one presented in Fig. 6.5 (except that since the original object has 3
               bits, the values of the coding mask should be 1, 8, 64, 512). We assume
               that the dynamic range of the sensor has 12 bits (maximal value of
               4096). In Fig. 6.6a we present the low-resolution and dynamic range-
               limited image. In Fig. 6.6b we present the reconstruction. Clearly a
               resolution improvement of close to a factor of 2 in each axis is ob-
               tained. This is especially evident by observing the borders (e.g., the
               borders of the hat of Lena).


               6.3.6 Description in the Phase-Space Domain
               In this subsection we describe the previously discussed SR principles,
               using the Wigner transformation. As previously mentioned, a more
               heuristic phase-space diagram can also do the job of describing the
               SR principles. However, the advantages of using the Wigner transfor-
               mation are connected to the relation between this distribution and the
               spatial degrees of freedom.
                 In Fig. 6.7 we schematically present the various steps of the setup of
               Fig. 6.2 for the case of time and polarization (which is time-varying)
               SR approaches where the degrees of freedom are converted from the
               spatial domain to the time or polarization domains.
                 In our schematic representations to come we deal with the case in
               which the spectral bandwidth of the signal is 3 times larger than the
               bandwidth that may be transmitted through the aperture of the imag-
               ing lens. The maximal bandwidth that may fit through the aperture
               of the lens is denoted by   , where   and x designate the spectral and
               the spatial domain coordinates, respectively.
                 In Fig. 6.7a we present the phase-space diagram of a randomly var-
               ied distribution having high spatial resolution. This chart presents the
               time-varying random encoding mask that we will use. Every different
               spatial value is designated with a different color. Since we are talking
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