Page 192 - Optofluidics Fundamentals, Devices, and Applications
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Optofluidic Photonic Crystal Fibers: Pr operties and Applications   167


               optical activity [58], or refractive index measurements using the shift
               of bandgaps [99] and/or of LPG resonances [61,162,163]. Such dip-
               sensors could in principle be manufactured by the millions in one
               single drawing process, and thus would be cheap, disposable
               (avoiding the issues of sample cross contamination in the microflu-
               idic channels), safe, and biocompatible. Polymer MOFs, which are
               more readily coated with biosensitive organic molecules and avoid
               the risk of leaving glass shards in the sample (possibly a living organ-
               ism) [58], are especially well suited for this application.
                  The shift of LPG resonances in fluidic photonic bandgap fibers is
               one of the most sensitive in-fiber refractive-index-sensing schemes
               [61]. However, this mechanism cannot be used for fluids with refrac-
               tive indices below that of the fiber material (as the fibers then become
               index guiding), de facto excluding most biomedically relevant water-
               based analytes. One solution to circumvent this problem is to add a
               high-refractive-index coating to the holes of the PCFs, which can
               restore bandgap guidance [164].
                  Some of the more noticeable recent efforts to increase the sensitiv-
               ity of PCF sensors include the combination of PCFs with existing
               highly sensitive techniques, such as SPR and SERS. Indeed, compel-
               ling arguments can be made in favor of including SPR techniques
               into PCFs—for the small sample volumes, propagation constant engi-
               neering, and ready access to waveguide fields [164–167]—however,
               achieving metallic coatings of sufficient quality (~50-nm thickness
               and negligible surface roughness) to allow unhindered propagation
               of surface plasmons at the metal/analyte interface remains a chal-
               lenge. So far the only surface plasmon resonances that have been
               clearly demonstrated in PCFs have used bulk metallic inclusions
               (fully filled holes), which can be very smooth at the metal/silica inter-
               face, but can hardly be used for sensing [168, 169]. A number of metallic
               coating techniques have been applied to PCFs, mostly in a non-SPR
               context: liquid phase deposition is reasonably easy to implement and
               can coat several meters of PCF holes at a time, but leads to surfaces
               too rough for SPR [170, 171]. Sazio et al. demonstrated high-pressure
               chemical vapor deposition of thin gold coatings in PCF holes with
               what appear to be extremely smooth interfaces [170]. This seems to be
               the most promising technique to achieve SPR capable PCFs, but is not
               easily implemented, and to the best of our knowledge no one has yet
               tried to use such fibers in the context of SPR sensing.
                  While the silver surfaces obtained with liquid phase depositions
               are not suitable for SPR, their roughness makes them a very good
               candidate for SERS. “Conventional” SERS techniques exploit hot
               spots (spots of extreme plasmonic field enhancement) to locally
               increase Raman scattering cross sections by up to 14 orders of magni-
               tude. These hot spots are obtained using either a suspension of metal
               nanoparticles or a rough gold or silver surface. The difficulty is that
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