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Maas, Two-tone intermodulation in diode mixers , IEEE Trans Microwave Theory Tech, MTT-35(3), 307 314, 1987 [31] JMT Thomson, HB Stewart, Nonlinear Dynamics and Chaos, John Wiley & Sons, New York (NY), 1997 [32] MS Nakhla, J Vlach, A piecewise harmonic balance technique for the determination of the periodic response of nonlinear systems , IEEE Trans Circuits Syst, CAS-26, 85 91, 1976 [33] F Filicori, VA Monaco, C Naldi, Simulation and design of microwave Class-C ampli ers through harmonic analysis , IEEE Trans Microwave Theory Tech, MTT-27, 1043 1051, 1979 [34] V Rizzoli, A Lipparini, E Marazzi, A general-purpose program for nonlinear microwave circuit design , IEEE Trans Microwave Theory Tech, MTT-31, 762 769, 1983 [35] KS Kundert, A Sangiovanni-Vincentelli, Simulation of nonlinear circuits in the frequency domain , IEEE Trans Comput-Aided Des, CAD-5(4), 521 535, 1986.

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[36] RJ Gilmore, MB Steer, Nonlinear circuit analysis using the method of harmonic balance a review of the art: part I and part II , Int J Microwave Millimetre-Wave ComputAided Eng, 1(2), 159 180, 1991 [37] K Kundert, J White, A Sangiovanni-Vincentelli, Steady-state Methods for Simulating Analog and Microwave Circuits, Kluwer, Norwell (MA), 1990 [38] S El-Rabaie, VF Fusco, C Stewart, Harmonic balance evaluation of nonlinear microwave circuits a tutorial approach , IEEE Trans Educ, 31(3), 181 192, 1988 [39] F Filicori, VA Monaco, Computer-aided design of nonlinear microwave circuits , Alta Frequenza, 57(7), 355 378, 1988 [40] V Rizzoli, A Lipparini, A Costanzo, F Mastri, C Cecchetti, A Neri, D Masotti, State-ofthe-art harmonic-balance simulation of forced nonlinear microwave circuits by the piecewise technique , IEEE Trans Microwave Theory Tech, MTT-40(1), 12 28, 1992..

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relatively increased in obese individuals whose weight is stable, and this mechanism may help to limit further weight gain (Raben et al, 1994; Schutz, 1995; Golay et al, 1997; Ravussin and Smith, 2002) Current guidelines are to limit the energy intake from fats to less than 30% of total energy intake (NHLBI, 2000) (see Table 164) Ingestion of dietary fats may also affect cardiovascular and metabolic risk factors, in part independently of body weight Importantly, the fatty-acid composition of the diet may markedly in uence insulin sensitivity and blood lipid levels In healthy subjects, ingesting variable amounts of fat (between 20 and 40% of total energy intake) does not signi cantly affect insulin sensitivity (Swinburn et al, 1991; Borkman et al, 1991; Bisschop et al, 2001; Garg, Grundy and Unger, 1992; Hughes et al, 1995; Sarkkinen et al.

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Within the class of nanoscale materials (e.g., see Table 4.7 inspired by [206]), nanocomposites are of major interest. In nanocomposites the components are mixed at the nanoscale, resulting in materials that often have properties that are superior to conventional microscale composites and, at the same time, can be synthesized using simple and inexpensive techniques (see Table 4.8 [206]). A nanoscale dispersion of sheetlike inorganic silicate particles in a polymer matrix, for example, is superior to either constituent in such properties as optical clarity, strength, sti ness, thermal stability, reduced permeability, and ame retardancy (see Table 4.9 for a list of properties of interest [17, 206]). Recent examples of composite materials with unique characteristics include magnetic and semiconductor multilayers made from magnetite nanoparticles, which can also be combined with carbon nanotubes and clay platelets [207]. Nanostructured materials include metals, composites, polymers, liquid crystals, clusters, quantum dots, colloids, and nanotubes; nanostructures include fullerenes, nanotubes, clusters, layers, quantum dots, thin lms, surfaces, and interfaces [208].

Thus, the interferometer is compensated for the bandwidth l when the group optical path for both arms is the same. Steel (1962) pointed out that the compensation for the bandwidth of the light source can be examined by looking at the fringes formed by a white light source through a spectroscope with its slit perpendicular to the fringes. The spectrum is crossed by the fringes and their inclination shows the change of fringe position with wavelength. The fringes will be straight along the direction of dispersion if the bandwidth compensation is perfect. Otherwise, the glass optical paths can be adjusted until the fringes show a maximum (zero slope) at the

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