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Optofluidic Colloidal Photonic Crystals    129


               derivatives (such as inverse opal) lead to interesting applications in
               microfluidic continuous reactors by incorporating catalysts at the
               surfaces of the colloidal crystals [42]. Both mixers and reactors are
               important units in optofluidic systems to extend their applications to
               lab-on-a-chip or micro-TAS based on optics. Therefore, in the near
               future, we expect colloidal crystals to act as multifunctional units in
               integrated optofluidic systems.



          6-5 Summary
               Colloidal crystals have a photonic stop band that results from the
               periodic modulation of the refractive index at the half-wavelength
               scale of interacting light. This stop band can be controlled by
               infiltration of fluids into the crystal interstices. Therefore, the
               integration of colloidal crystals into microfluidic systems is important
               in order to exploit this property. Integration can be simply achieved
               by evaporating a colloidal suspension in microchannels or capillaries
               with one open end. Here, crystallization leads to a close-packed fcc
               structure, which has a volume fraction of colloids of 0.7404. However,
               evaporation-induced crystallization has many disadvantages. First of
               all, the crystallization process is too slow because evaporation occurs
               only at the small opening. In addition, soft spheres can induce cracks
               or gaps between the walls and the crystals because they can form
               non-close-packed crystals before the complete evaporation of the sol-
               vent. Moreover, the generation of open gaps between the colloidal
               crystals and the channel walls represents a severe problem in
               optofluidic applications. Because of the low hydrodynamic resistance
               at the gap, the majority of the fluid flows through the gap instead of
               through the crystal interstices. To solve these problems, centrifugal-
               force-induced crystallization was developed. Colloidal particles
               located in the rotating centrifugal chip move radially outwards. These
               particles are arranged into close-packed crystals much faster than
               with the evaporation-based method. Here, the crystallization time is
               determined by the particle size, the rotation speed, and the density
               contrast between the particles and the solvent. The colloidal crystals
               prepared in the centrifugal chips can be directly used as optofluidic
               devices, and hybrid colloidal crystals of different sizes and materials
               can also be prepared. However, in order to increase the flexibility of
               optofluidic systems containing colloidal crystals, crystallization
               should be located at a desired area. To achieve this, electrowetting is
               applied, whereby the microfluidic channel is combined with the
               electrode pattern. Electrowetting enables us to move the colloidal
               suspension into the desired position, and thus pixellate the colloidal
               crystals in electrically addressable microfluidic chips.
                  Colloidal crystals integrated in microfluidic devices can also be
               used as refractive index sensors because the reflection spectra of the
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