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Optofluidic Optical Components      67


               slot waveguides were also used for the realization of MRRs for bio-
               sensing applications [27]. Resonance shift of 212 nm/RIU (refractive
               index unit) was reported. By using a similar platform, a label-free
               biosensing of bovine serum albumin (BSA) and anti-BSA was also
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               demonstrated, with sensitivity limit in the range of 16 to 28 pg/mm .

          4-3  Optofluidic Components for Manipulation
                of Optical Signals
               In parallel to the rapid progress in optofluidic waveguides there is a
               growing effort to develop variety of other optofluidic components,
               with a prime goal of manipulating and processing optical signals.
               The integration of photonic components with liquids on the micro-/
               nanoscale paves the way to widen and enhance their optical function-
               alities, forming eventually a new class of optofluidic components for
               manipulating optical signals. Components such as tunable filters,
               switches, splitters and combiners, and beam deflectors were recently
               demonstrated. This section describes some of the recent work in the
               field, with a specific focus on tunable optofluidic filters. Other com-
               ponents, for example, switches, splitters, and beam-steering devices
               are covered in Chap. 8.

               4-3-1 Optofluidic Filters
               Optical filters are the subject of scientific and technological effort for
               many years, with applications in microscopy, avionics, spectroscopy,
               optical communication, sensing, astronomy, machine vision, laser range
               finders, and environmental monitoring, to name a few. Optofluidics is a
               promising approach for the realization of optical filters because (a) it
               offers a wide tunability range, much larger than can be achieved by most
               other physical effects, and (b) it allows the interaction of analytes carried
               by the liquid with the optical filter, thus enabling on-chip realization of
               optofluidic-filtering devices and systems. Two of the dominant mecha-
               nisms used for the realization of optical filters are absorption and interfer-
               ence. Optofluidic-absorption filters can be easily realized by introducing
               absorptive liquid into the filtering region. The spectral absorption prop-
               erties of the liquid determine the spectral response of the filter. The func-
               tion of tunability can be acquired by replacing the liquid with another
               liquid, having different spectral absorption properties. By mixing of liq-
               uids it is possible to achieve continuous tuning of such filters. Macro-
               scopic liquid absorption filters were already demonstrated many years
               ago [28,29]. For example, Ref. 29 describes an optical cell with a variable
               path length designed for use in conjunction with liquid filters. A path
               length change from 1 mm to 14 mm changes the cutoff wavelength
               by typically 30 nm. The miniaturization and on-chip integration of
               absorption-based liquid filters holds great promise for the realization of
               flexible, high-performance, and integrated optofluidic systems.
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