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It can also be shown that at larger bandwidths the sharper peak is more resistant to disturbance by receiver thermal noise, even though the precorrelation signal-to-noise ratio is increased Another advantage of a larger precorrelation bandwidth is that the spacing between the early and late reference codes in a code tracking loop can be made smaller without signi cantly reducing the gain of the loop, hence the name narrow correlator It can be shown that this causes the noises on the early and late correlator outputs to become more highly correlated, resulting in less noise on the loop error signal An additional bene t is that the code tracking loop will be affected only by the multipath-induced distortions near the peak of the correlation function.

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Leading-Edge Techniques Because the direct-path signal always precedes secondary-path signals, the leading (left-hand) portion of the correlation function is uncontaminated by multipath, as is illustrated in Fig 54 Therefore, if one could measure the location of just the leading part, it appears that the direct-path delay could be determined with no error due to multipath Unfortunately, this seemingly happy state of affairs is illusory With a small direct- to secondary-path separation, the uncontaminated portion of the correlation function is a miniscule piece at the extreme left, where the curve just begins to rise In this region, not only is the signal-.

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0.01 dB/ns and 0.001 dB/ at 10 GHz. Huang et al. (1993) developed a 3-ns YBCO delay line; loss at 8 GHz was 0.73 dB/ns or 0.092 dB/ . Talisa et al. (1995) used a closely wrapped spiral of YBCO on LaAlO, in stripline. The line is 1.5 m long! See Figure 3.20. Surface resistance at 10 GHz and 77 K is 0.5 mohm. Delay is 45 ns. Loss is 2 dB at 10 GHz and 6 dB at 20 GHz. At 10 GHz, this loss is 0.0044 dB/ , and at 20 GHz it is 0.0067 dB/ . Loss per nanosecond is 0.044 dB/ns at 10 GHz and 0.133 dB/ns at 20 GHz. Fenzi et al. (1994) developed a 100-ns delay line using TBCCO on an LaAlO substrate with meandered coplanar waveguide; see Figure 3.21. Loss at 6 GHz was below 0.08 dB/ns, which is 0.013 dB/ . This is the type of delay that might be suitable for wideband phased array steering. Fabrication details of a YBCO meanderline delayer using epitaxial liftoff were given by Koh and

An 8-bit cyclic redundancy check of the LLID elds Six-byte source and destination addresses (Fig. 2.14d). Single-station destination addresses have 0 for the highest order bit, while group addresses (multicast) use a 1, including full broadcast to all ONUs, in which case the eld is all 1 s. This leaves 47 bits. One of the consequences of the very large Ethernet address space (some 7 1013 2 1 resolvable addresses) is that every Ethernet card or unit shipped can be manufactured with a unique identi er each separate manufacturer is given a block of the 23 higher order bits by a central authority, and he then uses the remaining 24 bits to burn into the electronics of each instance of his product line output the address that that product

Working with portfolios of credit assets also leads to sources of uncertainty that don t occur in portfolios of equities. We noted previously that, for credit portfolios, we work with the distribution of losses rather than returns. As is illustrated in Exhibit 2.6, EXHIBIT 2.6 Additional Sources of Uncertainty

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As it is always the case, an established intractability invites an understanding of the limits of approximation Since it was established that computing a Nash equilibrium is PPAD-complete [20], even for two-player strategic games [12], the question of computing approximate Nash equilibria has emerged as the central remaining open problem in the area of computing Nash equilibria Assume from this point on that all utilities have been normalized to be between 0 and 1 (Clearly, this assumption is without any loss of generality) Say that a set of mixed strategies is an -approximate Nash equilibrium, where > 0, if for each player all strategies have expected payoff that is at most more that the expected payoff for its strategy in the given set (So, is an additive approximation term) Lipton et al.

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