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These could appear as a result of injection of radiation from another laser, reflection from external optics, feedback from a phase conjugator, injection current modulation, in addition to optical feedback, etc The reinjection of the optical radiation can also be modulated by a phase modulator inserted in the external cavity, or frequency shifted by an acousto-optic modulator before reinjection All these effects lead to an additional coupling of the phase of the laser to the intensity and can produce a variety of dynamical outputs In addition, the delayed nature of the reinjected field enlarges an already complicated dynamical structure and leads to so many interesting phenomena, that, almost thirty years after the first observations of instabilities in these systems, they still continue to be actively investigated In this chapter we will concentrate on experimental observations of the dynamics of emitted radiation of semiconductor lasers in an external cavity.

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The dynamics of such devices will be outlined as a function of feedback levels starting progressively from weak feedback at which the basic local bifurcations take place, to moderate feedback at which global bifurcations, and what is known as the low frequency fluctuations begin to appear Finally, we will briefly examine strong feedback and the transition from coherence collapse to single mode narrow-line emission This can be very nicely summarized by the diagram [19] shown in Figure 41 At the lowest feedback levels, Regime I, the laser is operating on a single external cavity mode that emerges from the solitary laser mode, which has been narrowed or broadened depending on the phase of the feedback In Regime II and at a feedback level that depends on the distance from the external reflector, the mode appears to split into two modes, an effect arising from rapid mode hopping.

30 40 50 Laser Current (mA) (b)

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