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Figure 53-1: Various multiple access channels We are all familiar with the notion of broadcasting, as television has been using it since its invention But traditional television is a one-way broadcast (ie, one fixed node transmitting to many receiving nodes), while nodes on a computer network broadcast channel can both send and receive Perhaps a more apt human analogy for a broadcast channel is a cocktail party, where many people gather together in a large room (the air providing the broadcast medium) to talk and listen A second good analogy is something many readers will be familiar with - a classroom where teacher(s) and student(s) similarly share the same, single, broadcast medium A central problem in both scenarios is that of determining who gets to talk (ie, transmit into the channel), and when As humans, we've evolved an elaborate set of protocols for sharing the broadcast channel ("Give everyone a chance to speak" "Don't speak until you are spoken to" "Don't monopolize the conversation" "Raise your hand if you have question" "Don't interrupt when someone is speaking" "Don't fall asleep when someone else is talking") Computer networks similarly have protocols - so-called multiple access protocols - by which nodes regulate their transmission onto the shared broadcast channel As shown in Figure 53-1, multiple access protocols are needed in a wide variety of network settings, including both wired and wireless local area networks, and satellite networks Figure 53-2 takes a more abstract view of the broadcast channel and of the nodes sharing that channel Although technically



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in pressure (DP) between bright stripes and dark stripes (POM pictures of gratings in Fig. 12.19) produced by the microphase separation, which is different from other enhancement mechanisms. The PEO blocks have a better compatibility with the isotropic polymer blocks in the dark area than the LC polymer blocks in the bright area after grating recording. Thus, better microphase separation can be obtained in the bright stripes upon annealing, inducing a higher pressure in the bright stripes compared with the dark areas, leading to the uplift of the dark

file:///D|/Downloads/Livros/computa o/Computer%20NeDown%20Approach%20Featuring%20the%20Internet/LANhtm (1 of 16)20/11/2004 15:52:35





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stripes (the peaks of the SRG). Furthermore, the molecular mobility of the azo LCBC can be improved in an isotropic phase, which enables the process of mass transport to form the surface relief enhancement. Obviously, the higher the DP induced by the microphase separation, the stronger the enhancement effect caused. As a result of the higher surface relief, a larger DE of the grating was obtained. The enhancement coef cient with recording time was estimated. The best enhancement effect was obtained at 10-s recording upon microphase separation. By precisely adjusting the recording time, the DE can be nely controlled from 0.13% to 10% (Yu et al., 2005b). All the movements in the grating formation and enhancement are summarized in Table 12.2.

each node accesses the broadcast channel through its adapter, in this section we will refer to the node as the sending and receiving device In practice, hundreds or even thousands of nodes can directly communicate over a broadcast channel

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By the cooperative effect between photoactive azo moieties and photoinert groups, a small external stimulus can induce a large change in the refractive index of the materials, a phenomenon that has been widely used in holographic recording. This is especially useful in bulk lms of azo BCs with azo mesogens in the minority phase within glassy PMMA substrates; for instance, photoinduced mass transfer is greatly prohibited because of the microphase separation in the process of holographic recording, which led to lack of surface relief structures (Frenz et al., 2004). Thus, refractive index modulation plays an important role in the grating formation in this case. As shown in Fig. 12.20, two holographic gratings were recorded in lms of two PMMA-based azo BCs, one of which is a well-de ned azo diblock copolymer; the other sample is a diblock random copolymer. Here the diblock random copolymer is formed by two blocks. One segment is well de ned, and the other mesogenic block is statistically random. After grating formation, neither lm showed a surface relief structure, and only RIGs were obtained. Upon irradiation of two coherent laser beams, RIG in the azo diblock copolymer was recorded by alignment of the azo moieties in microphase-separated domains. In contrast, the photoinduced alignment of the azo was ampli ed by the photoinert cyanobiphenyl moieties as a result of the cooperative effect in the diblock random copolymer (Yu, et al., 2008a). This resulted in a similar refractive index modulation as in the case of the left one in Fig. 12.20, although the azo content was lower in the azo BC. The cooperative motion was con ned within the nanoscale phase domains, unlike the case of random copolymers (Wu et al., 1998).

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