2006
DOI: 10.1364/josab.23.000663
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Q-switching instability in a mode-locked semiconductor laser

Abstract: We suggest analytic estimates for the Q-switching instability boundary of the continuous-wave mode-locking regime domain for a ring cavity semiconductor laser. We use a differential delay laser model that allows to assume large gain and loss in the cavity, which is a typical situation for this laser class. The slow saturable absorber approximation is applied to derive a map that describes the transformation of the pulse parameters after a round trip in the cavity. The Q-switching instability boundary is then o… Show more

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Cited by 30 publications
(28 citation statements)
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“…Increase of the parameter s leads usually to an increase of the ML stability domain and improvement of the pulse quality. 7,14,15 A similar decrease of the locking range is observed with the increase of the spectral filtering width ␥ which also leads to a decrease of the pulse width, see Fig. 4͑a͒.…”
supporting
confidence: 67%
“…Increase of the parameter s leads usually to an increase of the ML stability domain and improvement of the pulse quality. 7,14,15 A similar decrease of the locking range is observed with the increase of the spectral filtering width ␥ which also leads to a decrease of the pulse width, see Fig. 4͑a͒.…”
supporting
confidence: 67%
“…One of them lies around G 0 350 and involves a transition to a quasiperiodic solution with four pulses per round-trip. The other lies on the single-pulse branch, at G 0 90, and can be identified as a Q-switching instability [31], as we have found the envelope of the resulting oscillatory pulse train to be modulated at the Q-switching frequency. Q-switching is a process in which the laser response undergoes a periodic modulation on a time scale much larger than the round-trip time, typically on the order of the geometric mean of the photon and gain medium population lifetimes in the cavity.…”
Section: Bifurcation Diagramsmentioning
confidence: 72%
“…Solving the laser equations for the two stages analytically and gluing the solutions one obtains the map governing the transformation of the pulse energy, saturable gain, and saturable loss after a complete round trip in the cavity. We skip the details of these calculations, which are described in Rachinskii and Vladimirov (2004), and present only the results of the analytical study of this map (see Fig. 8).…”
Section: Delay-differential Equation Modelmentioning
confidence: 99%