2018
DOI: 10.1364/ol.43.005367
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Temporal localized structures in mode-locked vertical external-cavity surface-emitting lasers

Abstract: Temporal Localized States (TLSs) are individually addressable structures traveling in optical resonators. They can be used as bits of information and to generate frequency combs with tunable spectral density. We show that a pair of specially designed nonlinear mirrors, a ½ Vertical-Cavity Surface-Emitting Laser and a Semiconductor Saturable Absorber, coupled in self-imaging conditions, can lead to the generation of such TLSs. Our results indicate how a conventional passive modelocking scheme can be adapted to … Show more

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Cited by 23 publications
(15 citation statements)
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“…The SESAM features a single strained InGaAs/GaAs QW located near the external surface [42] leading to recombination rate approximately two orders of magnitudes faster than the gain medium. It has been engineered for achieving a modulation depth larger than 8 % between the saturated regime and the unsaturated one (saturable losses) which appears to be critical for obtaining bistability of the VECSEL close to threshold [39]. Moreover, the amount of saturable losses experienced by the electromagnetic field inside the cavity is varied by tuning the gain mirror and the SESAM microcavities resonances (λ G and λ SA respectively), δλ = λ SA − λ G ), as detailed in Suppl.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The SESAM features a single strained InGaAs/GaAs QW located near the external surface [42] leading to recombination rate approximately two orders of magnitudes faster than the gain medium. It has been engineered for achieving a modulation depth larger than 8 % between the saturated regime and the unsaturated one (saturable losses) which appears to be critical for obtaining bistability of the VECSEL close to threshold [39]. Moreover, the amount of saturable losses experienced by the electromagnetic field inside the cavity is varied by tuning the gain mirror and the SESAM microcavities resonances (λ G and λ SA respectively), δλ = λ SA − λ G ), as detailed in Suppl.…”
Section: Resultsmentioning
confidence: 99%
“…[13,14,40] together with a broad area pumped section. These two conditions were not fulfilled in [39], leading to a VECSEL that could only be operated in the single-transverse mode emission.…”
Section: Introductionmentioning
confidence: 99%
“…This analysis was performed in the (G 0 /G th , τ 2 /T )-plane. We set (α g , α q ) = (1.5, 0.5) to better match previous works [4,53,56]. Our results are shown in Fig.…”
Section: Emergence Of Lssmentioning
confidence: 97%
“…Here, the PML can be archived by closing the external cavity with a semiconductor saturable absorber (SA) mirror 1,6 . Recently, a regime of temporal localization allowing arbitrary low repetition rates was demonstrated in such systems [10][11][12][13][14][15][16] . In this regime in which the cava) Electronic mail: gurevics@uni-muenster.de ity round trip is much larger than the gain recovery time, the PML pulses become individually addressable temporal localized states (TLSs) coexisting with the off solution 10,17,18 .…”
Section: Introductionmentioning
confidence: 99%