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This calibration technique works quite well for circuits in which the generated current is (inversely) linearly related to the value of the resistor such as a bandgap and proportional to absolute temperature (PTAT) currents. At times, bias currents may be needed in which the generated current is not linearly related to the value of the resistor. One common example is a MOS Gm-based bias circuit, in which case the bias current is inversely related to the MOSFET Gm. In this case the generated bias current is related to 1/R2. A small variation in the value of R therefore can result in a large variation in the bias current. The application of a calibration circuit to this case is even more crucial that the previously discussed cases. However, it should be noted that a small residual calibration error can result in fairly large bias current error. One important point is that if a constant voltage swing is desired from a certain resistively loaded stage (e.g., on a high frequency divider), a calibrated current must not be used, assuming that the stage is utilizing the same type of resistor as that used for generating the bias current. In such a block the variation of the resistor is canceled in the generation of the output voltage.

(3.7)

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Other insights have been gained by comparing dropout statistics in a multimode system to a comparable single-mode system, and analyzing the results in terms of the LK model Among other findings in [84], it was observed that the dropouts in single-mode LFF tended to occur roughly three times more frequently than if an otherwise identical system were operating in a multimode condition Fast pulsing dynamics have also been measured statistically to compare single-mode and multimode behavior in the LFF and coherence collapse regimes These experiments typically demand high-bandwidth detection apparatus, such as a digital sampling oscilloscope or streak camera In one such experiment [85], a Hitachi HLP-1400 laser with a solitary threshold of 53 mA was used in a cavity of length L = 22 cm which provided feedback sufficient to produce a threshold reduction of 10%.

(5.77)

<0.1 0.8 2 5 8 14 22

A digital sampling scope was used to measure the probability distribution of the laser intensity These statistical samples of the fast dynamics showed maxima near the average laser intensity, with exponential tails extending to three times the average These data are shown in Figure 438, plotting the intensity probability versus the normalized injection current; the different symbols correspond to four different current levels ranging from 70 to 99 mA, but all distributions appear quite similar Time-resolved probability measurements following dropouts were also made, and showed an initially deterministic recovery, followed by a strongly modulated transient stage which then relaxed to a lower level of fluctuations These data were not well described by the single-mode LK model Subsequent experiments were performed in similar systems In [86], two different experimental systems were investigated, and were used to compare single-mode and multimode behavior in the LFF regime.

Asking for parameters through InputBox and MsgBox may not always be suitable. You might want to supply the information as command-line parameters, calling your script like a DOS or UNIX utility. Not interested in command-line arguments You like the drag-and-drop Windows way Read on, this part is still right for you! In order to make your scripts drag-and-drop-capable and to place scripts into one of the Windows context menus, you use exactly the same technique.

As mentioned earlier, the usefulness of spatial diversity decreases with increasing bandwidth, since signal cancelation caused by fading becomes more unlikely with larger bandwidth. Therefore, the central question is to nd the threshold bandwidth to which spatial diversity is still worth exploiting. In order to avoid any misleading array gain and to investigate the diversity gain only, Alamouti-STC with two

The following program does just that. Pointers in the chunk s header are overwritten before the malloc() call is made. Then malloc() is tricked into overwriting a function pointer (the Global Offset Table entry for printf()). Then printf() redirects into our shellcode, currently just 0xcc, which is int3, the debug interrupt. It is important to align our buffers so they are not at addresses with the lower bits set (that is, we don t want malloc() to think our buffers are mmapped() or have the previous bit set).

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