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In general, the modes will shift frequency toward the red as the feedback ratio is increased, the inversion will become more negative and the power will increase The birth of another mode through a saddle-node bifurcation also gives rise to a hysteresis phenomenon as a function of the feedback phase but of fixed feedback strength This hysteresis can be seen in the output power of the laser as well as the frequency as the feedback phase is scanned through 2 This bistability was studied experimentally and theoretically using Equations (43) (44) in [27] The apparent splitting is illustrated in the sequence of spectra shown in Figure 45 Indeed, this effect is clearly seen by comparing the spectra of the laser without feedback Figure 45(a), the laser with a weak feedback, 62 dB, in phase, Figure 4.

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node applies some parameters a and b, such that if a[DIST(S)] b ! DIST(i), then the neighbor node forwards the route request with DIST(i) and XD, YD information. That is, DIST(i) replaces DIST(S ). Otherwise the node discards the route request. When the neighbor node (i) forwards the route request to another node ( p), then the above calculation is repeated except that DIST(i) replaces DIST(S) that is, a[DIST(i)] b ! DIST( p)]. An example of this process is shown in Figure 15.16. Here, nodes I and N forward M s route request since a[DIST(M)] b ! DIST(i) and a[DIST(M)] b ! DIST(n). However, node Q will not forward M s route request, because DIST(q) . a[DIST(M)] b. Since GPS may include some error, the coordinates of a node may not be entirely reliable. While LAR addresses possible location error in scheme 1 by adding an error value e to the expected zone radius, scheme 2 does not account for possible location error. In either case, location error can contribute to the need by a source node to initiate multiple route discoveries. Moreover, the authors of [52] acknowledge that more work is needed to determine when the degree of location error nulli es the effectiveness of LAR schemes. Of course, UWB may alleviate these concerns. 15.5.10 LBR

5(b), and the laser at the same feedback level but with the relative feedback phase out of phase Figure 45(c) In addition, it can be shown that the splitting depends on the amount of feedback and it can be easily calculated from the solutions of Equation (410) Indeed, the agreement between experimentally determined splitting versus feedback denoted by the filled circles, and the calculated solid line in Figure 46 is impressive [19] for a 1 5 m DFB laser The mode hopping phenomenon is very interesting because it combines the external cavity dynamics and noise-induced phenomena Since the external cavity is in general long and the frequency separation between modes is small, there is always a finite probability that the laser will jump from one available mode into another To study such effects, the Lang Kobayashi.

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copper losses. For comparison, Figure 4.32 also shows the insertion loss of a highly resistive trace at low frequency; the losses do not tend toward zero at low frequency because of the high resistivity (DC loss) of the metal.

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