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development of advanced photonic devices. The dynamic control (switching) of local optical properties by light instead of an electric eld offers the advantage of having no need for patterning transparent electrodes, which can be useful for certain applications. The discussed switching mechanism based on the photochemical phase transition (Section 11.5) induced by azobenzene s photoisomerization is particularly appealing. However, a common problem with both PSLCs (Tong et al., 2005a,b; Urbas et al., 2004a) and PDLCs (Urbas et al., 2004b) is that a thorough segregation of azobenzene molecules from the polymer areas is dif cult to achieve, so that the photoisomerization not only affects the LC host as desired but also affects the polymer. This may limit the index modulation depth and thus the switching performance. For future studies, the grating fabrication method should not be limited to the photopolymerization-induced phase separation (holographically or not). For instance, if a method allows for ef cient alternative deposition of two SLCPs with controlled layer thickness in the order of 200 nm, an effective re ection grating (Bragg re ector) can be designed to have one SCLCP having a low Tg (below or close to room temperature) and bearing azobenzene mesogens, whereas the other SCLCP can be chosen to have a high Tg and contain nonazobenzene mesogens. In this case, after aligning both polymers (e.g., by rubbed surfaces at temperatures above both Tgs), upon UV light irradiation at room temperature, the photochemical LC-to-isotropic phase transition can occur only in layers of the azobenzene SCLCP, which should have no effect on the other SCLCP remaining aligned. This would resolve the phase separation problem as mentioned earlier.



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While the multicast routing algorithms we have studied above construct a single, shared routing tree that is used to route packets from all senders, the second broad class of multicast routing algorithms construct a multicast routing tree for each source in the multicast group We have already studied an algorithm (Dijkstra's link-state routing algorithm, in section 421) that computes the unicast paths that are individually the least cost paths from the source to all destinations The union of these paths might be thought of as forming a least unicast-cost path tree (or a shortest unicast path tree, if all link costs are identical) Figure 48-10 shows the construction of the least cost path tree rooted at A By comparing the tree in Figure 48-10 with that of Figure 48-8, it is evident that

Figure 7.26 On-board oxygen generation system (Courtesy of Honeywell Aerospace Yeovil)

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The author is grateful to all the students and collaborators who worked on and made contributions to the projects on tunable diffraction gratings, particularly, Dr. Shuying Bai, Xia Tong, Dr. Li Cui, Dr. Guan Wang, and Professor Tigran Galstian (Laval University, Quebec City, Canada). The author thanks Jie He for his assistance in the preparation of the manuscript. The author is also grateful for the nancial support from the Natural Sciences and Engineering Research Council of Canada (NSERC), the Fonds pour la Formation de Chercheurs et ` l Aide a la Recherche of Quebec (FQRNT), and University of Sherbrooke and St-Jean Photochemicals Inc. (St-Jean-sur-Richelieu, Quebec, Canada).

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the least cost path tree is not the same as the minimum overall cost tree computed as the solution to the Steiner tree problem The reason for this difference is that the goals of these two algortihms are different: least unicast-cost path tree minimizes the cost from the source to each of the destinations (that is, there is no other tree that has a shorter distance path from the source to any of the destinations), while the Steiner tree minimizes the sum of the link costs in the tree You might also want to convince yourself that the least unicast-cost path tree often differs from one source to another (eg, the source tree rooted at A is different from the source tree rooted at E in Figure 48-10)

Bai S, Zhao Y. 2001. Azobenzene containing thermoplastic elastomers: coupling mechan ical and optical effects. Macromolecules 34:9032 9038. Bai S, Zhao Y. 2002. Azobenzene elastomers for mechanically tunable diffraction gratings. Macromolecules 35:9657 9664.

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Engine bleed air enters the pre-conditioning system element where the temperature is reduced, ideally to less than 70 C and water is removed as far as possible. In addition it is normal at this stage to use a combined particulate and coalescing lter to remove potential contaminants including free-water that may still be contained in the inlet air. The OBOGS contains a pressure reducing valve to reduce the inlet air pressure of the air supply to that required by the OBOG generator, typically 35 psig. The next system element is the oxygen generator, or more correctly, the OBOGS concentrator that uses multiple zeolite beds to produce the oxygen-rich product gas. The switching between the zeolite beds is achieved using solenoid actuated pneumatic diaphragm valves controlled by the system monitor/controller.

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