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read out only every second or every third strip. In such a con guration the signals collected by the intermediate are coupled to the readout strips through the interstrip capacitance.

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to a stop frequency. The double side band integrated value from 100 Hz to 1 MHz is tabulated at the top right of the display and is 1.88 for this particular PLO. The minimum phase noise that can be measured is limited by the phase noise in the PLO of the spectrum analyzer making the measurement. Figure 17.10 shows the nominal phase noise oor of the spectrum analyzer described in 9. A comparison of Figures 17.9 and 17.10 shows that the spectrum analyzer is entirely adequate for measuring the phase noise of the device measured in Figure 17.9 because the spectrum analyzer phase noise oor is 25 dB below the oscillator being measured.

11

Using GetDate()

To see the sketch relations is one of the most obvious tools necessary for visualizing existing Design Intent. You can show or hide icons that represent the relations using the menu selection View, Sketch Relations. When shown, these relations appear as a small icon in a small colored box in the graphics area next to the sketch entity. Clicking on the icon highlights the sketch elements involved in that relation. Refer to Figures 1.19 through 1.25 for examples of these relations.

button on the right to download a list of relevant newsgroups available on your server. If there are no matches for the topic you ve entered, you are notified by a message in the Newsgroup description box. Try again using a different word or topic.

effective handling of large-area substrates. Vacuum-based techniques also suffer from relatively slow throughput, poor materials utilization (much of the deposited material ends up on the chamber walls), and considerable energy expenditure to heat or sputter from the target sources. Chemical vapor deposition (CVD) is an alternative vapor-based approach, which offers substantial exibility, assuming the identi cation of suitable volatile source materials.13 15 Practical constraints on reactor size, however, limit large-area deposition using this approach, and material utilization also presents a problem (much of the material owing through the system does not end up on the substrate). High substrate temperatures (>350 C) are also often required to achieve good crystallinity in lms produced using the CVD approach.13,14 Clearly, alternative cost-effective, high-throughput, low-temperature lm deposition processes are desired to enable more pervasive application of metal chalcogenide lms (especially for macroelectronics applications that rely on a large area or exible form factor). Particularly desirable among lm deposition processes are solution-based techniques, because of the relative simplicity and potential economy of these approaches. However, the covalent character of the metal chalcogenides, which provides the bene t of the desired electronic properties (e.g., high electrical mobility), represents an important barrier for solution processing. Several methods have been developed to overcome the solubility problem, including spray deposition, bath-based techniques, and electrochemical routes, each of which will be discussed in later chapters. In this chapter, a very simple dimensional reduction approach will be considered as a means of achieving a convenient solution-based route to lm deposition.

dxJn(x,y)

As will be shown, the inner product of two signals ~ ( t ) y(t) is related to and the inner product of their wavelet transforms as

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