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to this chaotic state is characterized by a series of bifurcations which will be carefully outlined and detailed in Section 4.4, Weak Feedback Effects . The low frequency fluctuation regime will be introduced and its dynamical state discussed in Section 4.6 Moderate Optical Feedback . Still further increase in the optical feedback level results in a transition to another single mode, constant intensity, and narrow linewidth regime (Regime V) when the diode laser facet facing the mirror has been anti-reflection coated. This regime cannot be reached when diodes with uncoated facets are used. Regime V, in which the laser is operating on a steady state, will not be discussed as it is rather uninteresting from the dynamical viewpoint. In the next few sections the most important effects in each of the feedback regimes will be discussed with emphasis on the sequence of bifurcations as a function of the feedback strength. In addition, some particular experimental effects that occur in short external cavities and also in double cavity systems will be outlined (Sections 4.7 and 4.8). One section will be devoted to multimode effects (Section 4.9). In this section the external cavity feedback phenomena under single or multimode operation of the laser will be contrasted. In the Control section (Section 4.10) we discuss several experimental procedures to alleviate the chaotic behavior of the laser in the external cavity but still retain all the operational characteristics of the laser. The following section reviews the experimental literature of the semiconductor laser in an external cavity with the addition of current modulation of the laser. Indeed, one such technique is to take advantage of modulation to open loop stabilize the external cavity laser. The penultimate section of this chapter discusses the effects and phenomena observed asp.net upc-a UPC-A . NET Control - UPC-A barcode generator with free . NET ...
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