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The Radon-Wigner Transform     145


               where x   ,y   , and z   are three spectral sensitivity functions associated
               with the measured chromaticity. These functions depend, obviously,
               on the specific color detector actually used. In the case of a conven-
               tional digital color camera, these channels can be associated with the
               R, G, and B bands of the three pixel families in the detector array.
               On the other hand, when a visual inspection of the final image is
               considered, these sensitivity functions are the well-known spectral
               tristimulus values of the human eye. 49
                 Equations (4.91) establish the formulas to describe completely the
               response of a system from a spatial-frequency point of view. To
               numerically compute the functions described there, the evaluation
               of the monochromatic OTFs for a sufficient number of wavelengths
               inside the illumination spectrum has to be performed. Since any of
               these monochromatic transfer functions can be obtained from a same
               single RWD, as stated in the previous section, these computations can
               be done in a much more efficient way by use of this two-dimensional
               display. Furthermore, the same imaging system (i.e., the same pupil
               function) but suffering from different longitudinal chromatic aberra-
               tion can be assessed as well, with no additional computation of the
               RWD. This is a critical issue in the saving of computation time which
               provides this technique with a great advantage compared to other
               classic techniques, as cited above.
                 To illustrate this technique, we present the result of the computa-
               tion of the polychromatic OTFs associated with a conventional one-
               dimensional clear-pupil optical system (slit of width h) but suffering
               from two different chromatic aberration states (systems I and II from
               now on), as shown in Fig. 4.23. We assume that no other aberrations

                               2.0
                           Longitudinal chromatic aberration   δW 20 (μm) coefficient:  –1.0
                               1.0

                               0.0



                              –2.0
                              –3.0
                              –4.0
                                                  System II
                              –5.0                System I
                                   400    500    600    700
                                          Wavelength: λ (nm)

               FIGURE 4.23 Longitudinal chromatic aberration coefficient associated with
               the two different correction states of the system under study.
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