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same numbering scheme. Some commands report priority in the old way ; the lower the number, the higher the priority of the process. Other commands do the opposite; the higher the number, the higher the priority of the process. To avoid being confused, make sure that you know which reporting convention is being used before you interpret your process data.
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Although measuring continuous wave [CW (unchanging)] signals is a valuable part of performing RF measurements, in practical applications RF signals need to carry information from one point to another in order to be useful. Figure 9.7 shows two
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At the heart of the debates for selection of CDMA for third-generation systems, the main concerns about the CDMA technique were: 1. Implementation complexity. Spread spectrum is a two-layer modulation technique requiring greater circuit complexity than that of conventional modulation schemes. This, in turn, could lead to higher electronic power consumption and higher weight and cost for the mobile terminals. Gradual improvements in lowpower digital electronic technology resolved this concern over time. Indeed, since CDMA provides better coverage, its overall power consumption became one of its advantages.
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The fundamental principle of all physisorption techniques is the dependence on the pore size of gas condensation into the corresponding uid, as expressed, for example, by the Kelvin equation. The gases have to be chosen according to the requirement that sorption/condensation in mesopores can be detected at reasonable pressures and temperatures, and that the interaction with the solid can be described entirely on the basis of physical, but not chemical, sorption mechanisms.26 Therefore, for this reason, nitrogen and argon are usually used for the characterization of porous solids. Another reason to employ these gases is the advance in the theoretical understanding of sorption phenomena for such gases.26 Simplistically, in a typical physisorption experiment, the volume of adsorbed gas is measured as a function of the pressure of the gas in relation to its saturation pressure. Physisorption represents a powerful methodology, as various structural parameters can be obtained, such as the pore size distribution, surface area (e.g., by the BET formalism), and the overall meso- and micropore volume. However, although there is no difference in the theory between physisorption in porous bulk materials and thin lms, the standard setups and experimental procedures introduced for the bulk are not applicable to lms. As a main problem, physisorption analysis on thin lms has to face the low quantities of material and the fact that the lms are prepared on a substrate, which impedes the analysis for several reasons. Standard setups for the characterization of powders, using nitrogen or argon, require at least a surface area of several meters squared, which demands at least ca. 10 mg for any valid analysis. Evidently, the amount of material in thin lms can be orders of magnitude less. Scratching off material from a large number of samples is not desirable because of potential damage to the mesostructure. Therefore, signi cant effort has been dedicated in the past years to develop strategies to allow for physisorption experiments on a single specimen of thin lm, i.e., typically with a specimen area of the order of 1 cm2 only. Three main approaches have emerged to ll the gap of routine physisorption measurements on thin lms. 9.3.2.1 Krypton Sorption. Volumetric adsorption using gases with low saturated vapor pressure has been found to be an effective technique to gain detailed structural information for small quantities of porous materials, especially using krypton (Kr).27 The substitution of nitrogen by Kr reduces signi cantly the amount of unadsorbed molecules in the dead volume, allows for the characterization of small surface areas, and is thus ideal for mesoporous
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(7.21) be the least squares estimate of an arbitrary linear combination If F is normal, then d is automatically normal.
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Table 1.8: Parameters for the example of Section 1.3.2.4.14.
Concentration in the solution (ppb)
And at low frequencies, Zin 0 r + ( o + 1) Re . (12.103)
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