Page 159 - Optofluidics Fundamentals, Devices, and Applications
P. 159

134     Cha pte r  Se v e n


               crystal fiber (PCF) tuned using microfluidics. We review optofluidics
               in a variety of MOFs, including grapefruit fibers, transverse PCFs,
               fluid-filled PCFs transformed into bandgap-guiding fibers, and fiber-
               based ultracompact optofluidic interferometers.


          7-1 Introduction


               7-1-1 Optical Fibers
               Since optical fibers are the defining characteristic of the optoflu-
               idic devices discussed here, a variety of relevant optical fiber
               designs warrant discussion. The ubiquitous silica telecommunica-
               tions single-mode fiber (SMF) [6] is used for optical transport,
               while microstructured optical fibers (MOFs) [9–14], including
               photonic crystal fibers (PCFs) [15–19] are used for both optical and
               microfluidic transport and manipulation. In this section, both vari-
               eties will be discussed, with emphasis on the MOFs that form the
               optofluidic devices.
                  The most prevalent optical fiber design is the silica telecommuni-
               cations SMF [6]. After many years of research and development, the
               SMF is deployed across the world, providing the physical backbone
               of modern communications. A consequence of this widespread use is
               that SMF and its associated light source and detection technologies
               provide high-quality, low-loss, modular means of generating, trans-
               porting, and analyzing light. This platform forms the basis for inves-
               tigation into fiber-based optofluidic devices. SMFs are composed of
               highly pure fused silica whose circular core is a region, 8 μm in diam-
               eter silica doped using heavy ions during the fabrication process [20].
               This doping provides a refractive index contrast against the sur-
               rounding silica cladding that is 125 μm in diameter and itself is
               protected by a variety of polymer coatings. Typically, these fibers
               support a single propagating mode at 1550 nm with a multimode
               cutoff wavelength of around 1100 nm. The single mode propagates
               with very low loss, approximately 0.2 dB/km [21].
                  Figure 7-1 shows several more recent developments in fiber
               waveguides: the MOF. MOFs are characterized by hollow inclusions
               that run the length of the fiber. These come in many forms, from fibers
               with a single hole forming a hollow core [22] to fibers with inclusions
               that surround an SMF-like core, known as a grapefruit fiber [23]. A
               special class of MOF is the PCF. These fibers consist of a periodic
               array of inclusions surrounding a core that may be either solid [16] or
               hollow [18,24]. These fibers display a wealth of optical phenomena
               [25–30]; however, it is the cladding/core inclusions comprising the
               fiber microstructure that are of interest in fiber-based optofluidics.
               These inclusions form a natural home for microfluids, and their over-
               lap with the guided mode of the fiber allows them to influence the
   154   155   156   157   158   159   160   161   162   163   164