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familiar with is how to apply the capacitor and inductor to the matching network. To build a narrow-band impedance matching network, one, two, or three parts are needed. However, the number of parts may be increased, depending on the relative bandwidth. Third, it is necessary to pay attention to the demarcation of narrow and wide bands. As a matter of fact, this demarcation is not derived strictly from theory, but rather from the engineering design experience. Generally speaking, an RF circuit block is categorized as a narrow-band block if its relative bandwidth of operation is less than 15%; an RF circuit block is categorized as a wide-band block if its relative bandwidth of operation is more than 15%. When the relative bandwidth of operation is around 15%, it is better to treat an RF circuit block as a wide-band block so as to have a reasonable performance for both wide-band and narrow-band cases. In the return loss RL (S11 or S22) testing, the trace of impedance Z or return loss RL (S11 or S22) displayed in the Smith chart corresponds to the response for a frequency bandwidth. An example is shown in Figure 10.1, where the displayed trace shows the frequency response of impedance Z or return loss RL (S11 or S22) from lowest frequency to highest frequency, that is, f = fmax fmin, (10.1)



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Figure Figure Figure Figure 1-1: 1-2: 1-3: 1-4: The .NET experience The .NET Framework JIT compilation process Common Type System The New Project dialog box. A sample Windows Application project. A Label control is selected in the Properties window. A sample form for the Hello World Windows The Code window displaying the Visual Basic code. A sample Web Forms page.





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A long-standing dispute has raged over the effects of file size on speed. Here are the facts: When SolidWorks creates a configuration, it stores information about the 3D geometry and a preview thumbnail of the configuration inside the part file. This makes it faster to access the configuration the next time because it has only to read the data, rather than read other data and then recalculate the new data. As a result, saving the stored data makes the file larger, but also enables you to avoid having to recalculate it. Many people assign more importance to file size than I do, and use it as a criterion on which to base decisions about which features or techniques to use or not use. If I can use a single file instead of

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Stranski Krastanov lm growth mode, 244 Stress concentration and fracture, in transfer printing, 421 423 Stretchability of exible macroelectronics, 436 441 two-dimensional, 440 441 Stretchable electronics, transfer printing techniques for, 412 426 Striations, 54 Structural defects, 323 Structural evolution, 41 Structural health monitor systems, 431 432 Structural relaxation, 56 Structured dielectrics, laminated approach to, 125 Structure shrinkage problem, 297 298 Substrates, low-temperature, 15 Substrate separation, in batch-produced CBD CdS, 202 Substrate surface, for successful lm deposition, 81 Substrate surface preparation, in chemical solution deposition, 34 36 Successive ionic layer adsorption and reaction (SILAR) technique, xiv, 210, 239 282. See also SILAR entries advantages and disadvantages of, 241 242 basic principles of, 240 244 chalcogenide lms grown by, 252 263 materials grown by, 244 264 mechanism of lm growth in, 243 244 metallic lms grown by, 263 264 oxide lms grown by, 244 252 Sulfato ligands, 114 Superconductive transition temperature, 220 221 Superconductivity (SC) behavior, 218 Superlattices, 331 332 Supply chain development, roadmapping for, 400 Surface acoustic waves (SAWS), 59, 289, 291 Surface chemistry, in transfer printing, 415 417, 418

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Figure 5.8.32 Ritsumeikan University SR center; 1 m diameter synchrotron radiation facility. Several beamlines are for XAFS spectroscopy. Taken from http://www.ritsumei.ac.jp/se/d11/index-e.html

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