1996
DOI: 10.1070/qe1996v026n03abeh000635
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New principle of formation of ultrashort pulses in solid-state lasers with self-phase-modulation and gain saturation

Abstract: It is shown for the first time that the balance between self-phase-modulation (SPM) and gain saturation in an active medium of a solid-state laser with a limited gain bandwidth can generate a chirped frequency-shifted quasisoliton. Introduction of additional amplitude or phase modulation stabilises this quasisoliton.

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Cited by 5 publications
(3 citation statements)
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“…The complex confinement potential in [15] corresponds to a cigar-like confining potential in a weakly-dissipative BEC (figure 1(a)) [16]. As it was previously found, an external periodical phase modulation can substantially enhance 1D-soliton stability in a dissipative laser system in the presence of Kerrnonlinearity [50][51][52][53][54]. As a rule, a periodic phase modulation (∝t 2 + H.O.T.)…”
Section: Introductionsupporting
confidence: 52%
“…The complex confinement potential in [15] corresponds to a cigar-like confining potential in a weakly-dissipative BEC (figure 1(a)) [16]. As it was previously found, an external periodical phase modulation can substantially enhance 1D-soliton stability in a dissipative laser system in the presence of Kerrnonlinearity [50][51][52][53][54]. As a rule, a periodic phase modulation (∝t 2 + H.O.T.)…”
Section: Introductionsupporting
confidence: 52%
“…That is obviously connected to co-existence of nonlinearities with different time scales: instantaneous non-dissipative SPM, and non-instantaneous dissipative nonlinearities like stimulated Raman scattering (SRS), saturable absorber losses, and gain saturation. This issue is especially intriguing, as the dynamic gain saturation can provide a supplementary mechanism of DS formation [71].…”
Section: Main Obstacles To the Ds Energy Harvestingmentioning
confidence: 99%
“…[10], it reduces the total anomalous group-velocity dispersion and, consequently, increases the contribution of the higher-order dispersion (particularly the third-order contribution). For this reason we shall subtract the third-order dispersion, which can be done by introducing into Eqn (1) a perturbation term d 3 q 3 aaqt 3 (d 3 is the dimensionless coefficient of the third-order group-velocity dispersion) while retaining the shape of an ultrashort pulse ak, t a 0 sech t À Wk t p 1ic expfijk ot À Wkg , where 5 is the time delay of a pulse in a round trip through the cavity; o is the frequency detuning of a pulse from the centre of the pass band of a frequency-selective component [14]. The right-hand sides of the iteration relationships (4) must then be supplemented by the following terms:…”
mentioning
confidence: 99%