Page 80 - Optofluidics Fundamentals, Devices, and Applications
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Optofluidic Optical Components      61


               In this section we describe in detail some of the major configurations
               used for the realization of optofluidic waveguides.

               4-2-1 Solid-Core/Liquid Clad Waveguide
               The most straightforward and simple optofluidic waveguide config-
               uration is a structure made of solid core surrounded by a liquid clad
               (SCLC). A schematic sketch of such structure is shown in Fig. 4-1.
                  A solid core (typically made of glass, polymer, or semiconductor)
               is positioned on top of a lower solid clad and covered by a liquid
               forming the upper and side clad. Typical liquids being used for clad-
               ding material are distilled [DI] water (n~1.33 at visible wavelength),
               water-based solutions (n~1.33–1.45) and organic-based liquids
               (n~1.45–1.55). Liquids with higher refractive indices, up to ~2.3, are
               also available, although some of them are toxic. More details about
               commercially available liquid solutions and their properties can be
               found in Ref. 4. The solid lower clad is frequently made of silicon
               dioxide (SiO , n~1.45). In some specific cases the SiO  clad can be
                          2                                  2
               etched (e.g., by buffered HF), forming a bridged waveguide. Such a
               waveguide can be surrounded by liquid from all directions.
                  A silicon wafer is covered by a few microns–thick oxide layer. The
               solid core (SC) is positioned on top of the oxide. A microfluidic chan-
               nel is defined in PDMS and filled with a liquid clad (LC), surrounding
               the SC. Liquids can be stationary or in constant flow. The guiding
               mechanism of most SCLC waveguides is based on total internal
               reflection (TIR). The optical mode in such waveguides extends
               beyond the core, and decays exponentially in the clad. This portion of
               the optical mode is known as the evanescent field. The interaction of
               light propagating through the SCLC waveguide with the liquid takes
               place via the spatial overlap between the liquid and the evanes-
               cent field in the clad. An important parameter for classifying and
               characterizing an optical waveguide is the confinement factor,
               defined as the portion of the optical mode that is confined to the core.





                                          PDMS



                                           SC    LC
                                         SiO 2

                                        Silicon wafer

               FIGURE 4-1  Schematic drawing showing a cross section of a typical SCLC
               waveguide.
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