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[l01L. Bluestein. A linear filtering approach to the computation of the discrete Fourier transform. IEEE Trans. Audio and Electroacoustics, 18:451-455, 1970. [l11 B. Boashash and A. Riley. Algorithms for time-frequency signal analysis. In Time-Frequency Signal Analysis, B. Boashash (ed.). Longman, Cheshire, 1992. [l21 S. Boll. Suppression of acoustic noise in speech using spectral subtraction. IEEE Trans. Acoust., Speech, Signal Processing,27(2):113-120, April 1979. [l31 R.N. Bracewell. The discrete Hartley transform. J. Opt. Soc. America, 73:1832-1835, December 1983. [l41 R.N. Bracewell. The fast Hartley transform. Proc. IEEE,72:lOlO-1018, 1984.

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And so on. To answer these questions, we need to revisit the goals of impedance matching: (1) to reach maximum power transportation and (2) to eliminate phase shift in power transportation. Impedance matching is therefore required between power transportation units, but is not necessary between individual parts. If an impedance matching network consists of more than one part, it implies that all the parts in the impedance matching network must be co-operated together so as to maximize the power transportation and to eliminate phase shift. In other words, the matching network, but not its individual parts, is an indivisible basic entity or a minimum cell. Their parts are indivisible in the power transportation. Impedance matching between the individual parts is meaningless. In general, impedance must be matched between two basic power transportation units. The unique exceptional case in which we do not do so is when these two basic power transportation units are combined for special performance. Let s illustrate this answer by examples. Example 1: Figure 9.12(a) shows a raw source follower without impedance matching at its output; DC bias is neglected. It consists of a MOSFET transistor and an output resistor, Ro. Looking at the emitter of the transistor in Figure 9.12 (a), it can be seen that its impedance, Zx, is usually not conjugate-matched to the impedance of the emitter resistor, Ro. Is it bene cial to the power transportation if an impedance matching network is inserted





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1. Besser, L. and Gilmore, R., The radio as typical RF system, In Practical RF Circuit Design for Modern Wireless Systems Vol. I: Passive Circuits and Systems, Artech House, Norwood, MA, 2003. 2. Pozar, D., Noise and distortion in microwave systems, In Microwave and RF Design of Wireless Systems, John Wiley & Sons, New York, 2001. References 1 and 2 provide additional background and derivation of the intermodulation product terms.

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First, if we want to prevent the prior from overpowering the evidence of the observational data, we should choose it such that ~ ( 0 ) / a (is bounded Note that 0) flatness of the prior is not involved, only boundedness of d / Q Proceeding in a more systematic fashion, we might choose a within the uncertainty range of the prior in such a way that it minimizes the bound Typically, in particular for the contamination model, this can be achieved by choosing Q to be least informative in terms of Fisher information-although, such heuristic recommendations ought to be used with circumspection Unless the parameter space has some natural symmetry (such as translation invariance), its parameterization is essentially arbitrary, and this affects the behavior of cY (Q)/cr(e) of f (x; and Q)/f(z; A possible way around 0) this problem is furnished by self-scaling, as used in (127)..

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