Page 113 - The Indian Optician Digital Edition July-August 2021
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of a blazed, full period phase zone plate or           Since the diffractive element focuses
          kinoform (Figure 4).                                incoming light at the point P, this point
                                                              must be the second principal focus of the
             A full-period, phase zone plate is simply a      full-period, phase zone plate, F'.  Using the
          series of annular apertures the distances of        same principle as shown in Figure 5, but
          which lie successively one more wavelength          applying it to the diffractive element shown
          from some point P which lies at a distance d        in Figure 6,
          from the zone plate on its axis of symmetry
          (Figure 5).                                            y   = (f ' + m λ)  - f '    = m x 2 f ' λ
                                                                               2
                                                                                    2
                                                                   2
                                                                  m
             It can be seen from Figure 5 that the radius        and the design equation for such a plate
          of the central circular zone, y , is given by       becomes
                                       0
               2
                       2
                           2
             y  = (d + λ)  - d  = 2d λ                           y    =  2 m f ' λ.
                                                                   2
              0
                                                                  m
             ignoring the term, λ2, which is very small.         When written in the form m = y  / 2 f ' λ
                                                                                                  2
                                                                                                m
          Thus, the area of the central zone which
          contributes towards the light arriving at P is         the expression provides the number of
                                                              zones, m, for a given diameter, 2y  (Figure 7).
                                                                                               m
             2 π d λ.
             The radius of the next zone, y , is given by
                                          1
              2
                            2
                        2
             y  = (d + 2λ)  - d  = 2 x 2d λ
              1
             and the area of this whole zone is
             2 x 2 π d λ.
             The area of the first annular zone around the
          central zone is thus
             2 π d λ,                                              FIGURE 5  FULL-PERIOD PHASE ZONE PLATE
             so this annular zone contributes the same
          amount of light at P as the central zone.
             If the full-period, phase zone plate has a
          series of m annular apertures, the area of the
          mth ring will be
             m x 2 π d λ

             and the area between this ring and the
          preceding one will, again, be

             2 π d λ
             Thus, each zone adds the same amount of
          light at P, which, therefore, all arrive in phase
          and sum constructively. This diffractive element,
          or kinoform, behaves just like a plus lens
          focusing light at P (Figure 6). It can be seen in
          Figure 6 that there is a difference in the optical
          path length of the light as it passes through
          each successive zone of the kinoform which
                                                                    FIGURE 6 - DIFFRACTIVE LENS IN THE FORM
          is similar to the difference when light passes        OF A FULL-PERIOD, PHASE ZONE PLATE (KINOFORM)
          through a converging lens.


                                                                                              109 | LENS TALK
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