Page 67 - Optofluidics Fundamentals, Devices, and Applications
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48     Cha pte r  T h ree


               by filling two separate channels with black ink. For applications that
               require higher intensity at the focus, the aperture can be removed. In
               order to visualize the optical path, a beam-tracing chamber filled flu-
               orescent dyes (2.5 μM rhodamine 640 perchlorate in ethylene glycol)
               is incorporated behind the L  lens.
                                       2
               Characterization
                                             2
               Figure 3-9 shows the shapes of the L  lens under different flow condi-
               tions. Since the height of the expansion chamber was much smaller
               than its width and length, the flow was quasi-two-dimensional, and
               the L  lens is roughly cylindrical. When the rates of flow of the left
                    2
               and the right cladding streams were the same, the core stream, or the
               L  lens, was biconvex and symmetrical inside the expansion chamber.
                2
               Varying the relative flow rates between the left and the right clad-
               dings varies the curvatures of the left and right interfaces separately.
               It is therefore possible to obtain an extensive range of lens shapes:
               meniscus, plano-convex, and biconvex.
                  The L  lens focused light; the FWHM (full width at half-maximum)
                       2
               of the beam at the focus achieved was ~ 16 μm, 20 times less than the
               initial beam width, using a 334-μm aperture. This beam size was lim-
                                                  2
               ited by aberration due to the shape of the L  lens; the diffraction-limited
               width at the focal point is ~ 7 μm using this aperture. The enhancement
               factor (defined here as the ratio of the peak intensity of a focused beam
               to the intensity of an unfocused beam at the same point) achieved was
               9 without any aperture (the enhancement factors were usually between
               3 and 4 among previous works on microfabricated lenses).



                                 Increasing core flow rate






                                        (a)
                               Increasing left cladding flow rate






                                        (b)

                                           2
          FIGURE 3-9  (a) Fluorescence images of the L  lens in the expansion chamber as the
          rate of fl ow of the core stream increases (from left to right).  The cladding liquid was
                                                                    2
          dyed to make it easily imaged; the dye was omitted in normal operation of the L  lens.
          (b) Fluorescence images of the L  lens as the rate of fl ow of the left cladding stream
                                  2
          increases (from left to right).
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