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of feedback are applied without any ltering in the external feedback path; Figure 9.15a shows the multimode of the freely running laser; Figure 9.15b shows the single-mode operation of the laser when feedback is applied; Figures 9.15c g reveal the deterioration of the spatial pro le, the spectral broadening, and the mode hopping of the laser output as the amount of external feedback is increased. The spatial pro le is changed from an almost diffraction-limited spot in Fig. 9.15a to a radiation pattern in Fig. 9.15g that is far from the diffraction limit, which corresponds to several spatial modes emitted from the laser diode array. The increase of the external feedback also leads to slow temporal alternations (on the order of minutes) of the output. At a given level of external feedback the laser diode array is forced out of single-mode operation. This occurs slowly over 10 15 minutes or immediately after the external feedback is applied, depending on the intensity and the feedback angle. In all the experiments the feedback has been optimized by adjusting the external mirror (M2). However, due to diffraction loss, and so on, it is dif cult to determine the absolute amount of re ected light that enters the laser diode array. The response to a certain amount of external feedback radiation is seen to vary from measurement to measurement. We believe that this is due to the fact that the feedback is coupled into different array modes. It is possible to alter the spatial



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Figure 9-11: Using the CHANGE command on one line. If you select more than one line, CHANGE works differently: it moves the nearest endpoints of all of the lines to the change point so that all of the lines meet at one point, as shown in Figure 9-12. Figure 9-12: Using the CHANGE command on several lines. The original lines are shown as continuous. The new lines, after using the CHANGE command, are dashed.





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experiments. In order to achieve good impedance matching and similar broadside radiation patterns for the two operating frequencies, there exists a limited range of subtending angles for the present design. In this study, the subtending angles can be varied from 87 to 100 . When the angle is greater than about 100 , it is dif cult to obtain good impedance matching for the two operating frequencies. On the other hand, when the angle is smaller than about 87 , the radiation pattern of the second resonant frequency will become asymmetric with respect to the broadside direction. It is also noted that the rst resonant frequency f 1 , about 1.6 GHz, is very slightly affected by the variation in the subtending angle of the arc-shaped slot and is also about the same as the resonant frequency (about 1.65 GHz) of the TM11 mode of the simple unslotted circular patch. On the other hand, the second resonant frequency f 2 decreases rapidly with increasing . The different effects of the arc-shaped slot on the rst two resonant frequencies result in a tunable frequency ratio f 2 / f 1 between the two operating frequencies in the range of about 1.29 1.43 (see Table 4.5). By using the simulation software IE3DTM , the excited patch surface currents for the two operating frequencies of the antennna have been simulated and analyzed. The simulated current distributions of the two operating frequencies f 1 and f 2 for = 100 are plotted in Figure 4.15. For the case of f 1 shown in Figure 4.15(a), the resonant mode is the perturbed TM11 mode. It is seen that the excited current distribution is

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2. Open AutoCAD and make the pointer change that you want on the System tab of the Options dialog box. (If you re installing a new digitizer, follow the manufacturer s instructions to install the digitizer.) Click OK. 3. Close AutoCAD. 4. In Explorer, find the new acad2006.cfg file that AutoCAD created. Change its name, using something meaningful, such as LargeDigitizer.cfg. 5. If you want to keep the original acad2006.cfg file, change its name back to acad2006.cfg. You now have two configuration files. (You can create more if you want.) To use them, you can change the command-line switch as needed, but there s an easier way, as explained in the next section.

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In cases where wireless networking devices support both encryption methods, WPA should always be used as the secure alternative. Windows XP and most WEP-only devices can be upgraded to support WPA. In cases where WEP is your only encryption option, however, it should still be used the protection offered by a vulnerable WEP network is better than using no encryption at all.

with a two-particle model. One could increase the number of macroparticles, but the analysis quickly becomes complicated. Though computer tracking codes may help, it is possible to do the bookkeeping on more than a few thousand particles, whereas real beams will contain 10'' particles per bunch or more. To proceed, one turns to a description of the beam in terms of a continuous particle density function. The basic relationship that this function must satisfy is known as the Vlasov equation.

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