Page 55 - Optofluidics Fundamentals, Devices, and Applications
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36     Cha pte r  T h ree


           Beam-tracing chamber filled with a fluorescent dye
                                              2
                                             L  lens formed
                                             inside a microchannel

                                              Shutters formed  Laser light coupled
                                              by filling a channel  into the PDMS
                                              with black ink  device via a fiber

          FIGURE 3-3  Bright-fi eld image of beam-tracing chamber showing the optical path
          behind the L  lens.  The laser beam from the fi ber is visible in front of the aperture
                   2
          because PDMS contains nanoparticles of silica that scatter light. The focused beam
          in the beam-tracing chamber is visualized by the fl uorescence of a rhodamine dye
          fi lling the chamber. (S. K. Y. Tang, C. A. Stan, and G. M. Whitesides, “Dynamically
          reconfigurable liquid-core liquid-cladding lens in a microfluidic channel,” Lab Chip, 8,
          (2008), 395–401. Reproduced by permission of the Royal Society of Chemistry.)

               sealed channels with a razor blade (Fig. 3-2a; x-x’). This cut opens a
               channel at the edge of the PDMS that has the dimensions of the fiber
               (width × height ~ 100 μm × 100 μm). The open channel accommodat-
               ing the optical fiber ends at a distance from the fluidic channel, and is
               isolated from the fluids. Depending on the application, this distance
                                                2
               varies from a few 10s of microns (for L  waveguides) to a few milli-
                          2
               meters (for L  lens). The optical fiber is then manually inserted into
               this open channel. Index-matching liquids can be applied to fill any
               air gap between PDMS and the optical fiber. The center of the fiber
               channel is collinear with the center of the microfluidic channel.
                  To visualize the propagation of light inside the PDMS device, one
               can introduce fluorescent dyes in a chamber fabricated in the optical
               path [2]. This “beam-tracing” chamber is used for characterization of
                                                                    2
               the focal distance and the quality of the focused beam of the L  lens,
               for example (Fig. 3-3). The solution of dye fluoresces only in regions
               where there was optical illumination. The concentration of the dye
               solution should be sufficiently low such that the incident light could
               propagate through the beam-tracing chamber without being signifi-
               cantly attenuated or absorbed. To avoid photobleaching of the dye
               during the experiment, the intensity of the incident light should also
               be sufficiently low; alternatively, new dye solution can be injected
               continuously to replace the photobleached dyes.

          3-3  Index of Refraction of Common Liquids
               Contrast of refractive index in liquids can be provided in several
               ways, including
                   1.  Different liquids: A wide range of common liquids are trans-
                      parent in the visible region of the spectrum, and have refrac-
                      tive indices ranging from 1.28 to 1.75 [3]. Table 3-1 lists the
                      refractive indices of some common solvents.
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