2000
DOI: 10.1007/s003400000331
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Suppression of Q-switched mode locking and break-up into multiple pulses by inverse saturable absorption

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Cited by 109 publications
(52 citation statements)
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“…Although this stability criterion is strictly speaking not valid for high repetition rate lasers, as some of the assumptions made to derive (1) are not fulfilled for multi-GHz lasers, it still can be used to obtain some useful design guidelines. For a more detailed discussion on the influence of additional effects on the QML-threshold such as two-photon absorption or incomplete recovery of the absorber, refer to [22,25,26]. Nevertheless (1) reveals the engineering parameters which can be used to obtain stable mode-locking: the effective mode areas A eff,L in the gain medium and A eff,L on the absorber, which can be influenced by the cavity design of the laser, and the parameters of the saturable absorber, namely the modulation depth R and the saturation fluence F sat,A .…”
Section: Experimental Setups and Resultsmentioning
confidence: 99%
“…Although this stability criterion is strictly speaking not valid for high repetition rate lasers, as some of the assumptions made to derive (1) are not fulfilled for multi-GHz lasers, it still can be used to obtain some useful design guidelines. For a more detailed discussion on the influence of additional effects on the QML-threshold such as two-photon absorption or incomplete recovery of the absorber, refer to [22,25,26]. Nevertheless (1) reveals the engineering parameters which can be used to obtain stable mode-locking: the effective mode areas A eff,L in the gain medium and A eff,L on the absorber, which can be influenced by the cavity design of the laser, and the parameters of the saturable absorber, namely the modulation depth R and the saturation fluence F sat,A .…”
Section: Experimental Setups and Resultsmentioning
confidence: 99%
“…It is possible to extend the 'relaxed' regime to rather high frequencies (up to 20 kHz) by operating the system in terms of power and dispersion very close to the multiple pulse break-up. The overshoot after the dumping is limited considerably due to the optimized ratio between spectral filtering and absorber action, as was analyzed in detail in [10]. In this regime the observed pulse to pulse reproducibility is very high.…”
Section: Stability Considerationsmentioning
confidence: 93%
“…The dynamics of a SESAM mode-locked laser can be described in very good approximation by three differential equations [10][11][12], for the temporal dynamics of the pulse envelope, the laser gain and the absorber loss. The master equation of mode-locking, describing the evolution of the pulse's envelope reads …”
Section: Numerical Simulationsmentioning
confidence: 99%
“…In particular, the additional absorption observed at high fluences caused by induced absorption (IA) causes a "rollover" in reflectivity. Operating the SESAM close to this rollover can lead to multi-pulsing instabilities [43][44][45] because in this case multiple pulses with lower pulse energy can have a gain advantage compared to single pulses. Therefore, the most crucial parameters of SESAMs for high-power oscillators are: -large saturation fluences to operate at moderate saturation parameters and with small spot sizes, which relaxes cavity sensitivity to alignment and possible thermal lensing, -high damage thresholds, -low nonsaturable losses to avoid thermal effects, -reduced induced absorption (IA), which is responsible for the reflectivity rollover at high fluences and can lead to multi-pulsing instabilities [43][44][45].…”
Section: Sesams In High-power Ultrafast Oscillatorsmentioning
confidence: 99%