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The transition time increases considerably as a function of feedback, as can be seen from the three traces: upper 45 dB, middle 45 7 dB, lower 46 4 dB. This is in complete agreement with the model, since the barrier increases with . From such measurements the first passage time can be computed as the average time spent by the laser in one of the longitudinal modes before it hops to the adjacent mode as a function of feedback. The relative transition time is shown in Figure 4.9 along with the prediction of Equation (4.14) as a function of feedback and for three different pumping levels. The solid lines are the theoretical calculations and the solid squares are the experimental data for injection current I = 24 mA, open triangles for I = 28 mA, and filled circles for I = 32 mA. The agreement with the

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Based on the relative amount of pumping and including noise, it was shown that the laser would show random dropout events in the intensity followed by a stepwise climb back to high intensity levels [61] [62] It was also noticed, that omitting noise in the full equations, the LFF persisted confirming the notion that they are taking place on a chaotic attractor Another rather successful model attributed the drop-off events to a peculiar instability of the steady state [63] In particular, it was argued that even though the maximum gain mode and the external cavity modes close to the maximum gain mode (MGM) or equivalently maximum intensity mode, appeared to be stable in the usual linear stability approximation, higher-order contributions from quadratic terms can modify the stability arguments in the presence of spontaneous emission noise.

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Recommendations Conclusion Appendix A Glossary Appendix B A WLAN Exploitation Guide WLAN Configurations The IEEE 802.11 Physical (PHY) Layer

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The authors were successful in deriving an equation that described the fluctuations of the laser about the steady state in terms of a particle in a quadratic-cubic potential well Such potentials display a minimum at the MGM and a barrier assures its stability in the absence of noise However, in the presence of noise and under favorable conditions of feedback and pumping current, spontaneous emission noise can produce finite probabilities for the system to overcome the barrier and drop down the hill to the zero intensity level Naturally, after the drop-off event, due to high inversion the laser must return to the high intensity equilibrium The theory nicely determines the transition probability and the average transition time between dropout events as a function of feedback and pumping current [63] An alternate explanation was suggested by Sano [64] and elaborated by van Tartwijk [65].

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The creation of the new node in another, possibly remote, doer will be accompanied by transference of the rest of the program together with frontal variables to this new doer, also leaving track control with the previous doer (the latter is implied but not shown in Fig. 4.12, it will also be implied in the following operations). This transference (which also involves new node and link names) may be done electronically through a direct communication channel (or communication network, possibly, via other doers), if the frontal variables associated with the wave program keep information only.

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