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fourth, and fth packages With his rst package, Stokes varied the algorithm, the convergence tolerance, starting values, and so on This is something that every user should do with every nonlinear estimation Suppose that a user has done this and identi ed a possible solution How might he verify the solution McCullough and Vinod (2004) recommend four steps: 1 Examine the gradient Is ||g|| 0|| 2 Inspect the sequence of function values Does it exhibit the expected rate of convergence 3 Analyze the Hessian Is it positive semide nite Is it ill conditioned 4 Pro le the objective function Is the function approximately quadratic Gill et al (1981, p 313) note that if the rst three conditions hold, very probably a solution has been found, regardless of whether the program has declared convergence.



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Summary

PageSettings (Public Instance Property)

or, when GS = GS ,opt , BS = BS ,opt , the noisy two-port block reaches a minimum of noise gure, NF = NFmin. (18.74) (18.72) (18.73)

If you would like to practice with this part, it is on the CD-ROM for 26; the imported Parasolid file is named 26 Pattern import.x_t.

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The fourth step justi es the use of the usual t-statistics for coef cients reported by most packages These t-statistics are Wald statistics and, as such, are predicated on the assumption that the objective function, in this case the sum-of-squares function, is approximately quadratic in the vicinity of the minimum If the function is not approximately quadratic, the Wald statistic is invalid and other methods are more appropriate (eg, likelihood ratio intervals); this topic is addressed in detail in Section 86 The easy way to determine whether the objective function is approximately quadratic is to pro le the objective function Each of these four steps is discussed in turn 851 Step 1: Examine the Gradient At the solution, each component of the gradient should be zero.

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Optimal bounded-influence tests can be obtained by extending Hampel's optimality criterion for estimators (see Section 12.2) by finding a test in a given class that maximizes the asymptotic power at the model, subject to a bound on the level and power influence functions. If the test statistic T is Fisher-consistent, that is, ('(00) = 1, then E-l = V(F0,. T ) , the asymptotic variance of the test statistic. Thus, finding the test that maximizes the asymptotic power at the model, subject to a bound on the level and power influence function, is equivalent to finding an estimator T that minimizes the asymptotic variance, subject to a bound on the absolute value of its self-standardized influence function. The class of solutions for different bounds is the same for all levels, and it does not depend on the distance of the alternative A. Therefore, the optimal bounded-influence test is Uniformly Most Powerful. A similar

FIGURE 14.12 Power spectral densities of sources of ambient light and the spectral center of the GaAs diodes used for diffused infrared communications. (From [Gfe79b] IEEE.)

[l41 N. Anderson and P. Howard, Technology and Transceiver Architecture Considerations for Adaptive Antenna Systems, in Proceedings of ACTS Summit, pp. 965-970, 1997. [l51 J. Strandell, M. Wennstrom, A. Rydberg, T. Oberg, 0. Gladh, L. Rexberg, E. Sandberg, B. V. Anderson, and M. Appelgren, Experimental Evaluation of an Adaptive Antenna for a TDMA Mobile Telephony System, inProceedings of PIMRC, pp. 7984, 1997. 1161 J. J. Monot, J. Thibault, P. Chevalier, F. Pipon, S. Mayrargue, and A. Levy, A fully programmable prototype for the experimentation of the SDMA concept and and use of smart antennas for UMTS and GSMDCS 1800 networks, in Proceedings of PIMRC, (Helsinki, Finland), pp. 534-538, September 1997.

SPLIT-FERRITE CURRENT PROBE* Split-ferrite cylinders (or clamp-on ferrite beads) can be used as a calibrated current probe when clamped over a cable of interest. Common-mode currents are useful for measuring both frequency and amplitude components that may cause radiated EMI to exist above acceptable levels. This probe produces a voltage output that is related

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