1998
DOI: 10.1016/s0030-4018(98)00263-6
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High-order dispersion effects in solitary mode-locked lasers: side-band generation

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Cited by 22 publications
(18 citation statements)
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“…As an additional destabilizing factor, the dispersive perturbations in the laser system with self-phase modulation and negative net-GDD give rise to the spectral sidebands [1], [37], [38]. Their position in the absence of the higher order dispersion can be found from the condition , where , 2 , and are the normalized to inverse cavity length wave numbers of the dispersive wave, solitary wave, and periodic perturbation, respectively, is the sideband frequency, is the width of the soliton-like pulse with the shape , and is an integer.…”
Section: A Negative Gddmentioning
confidence: 99%
“…As an additional destabilizing factor, the dispersive perturbations in the laser system with self-phase modulation and negative net-GDD give rise to the spectral sidebands [1], [37], [38]. Their position in the absence of the higher order dispersion can be found from the condition , where , 2 , and are the normalized to inverse cavity length wave numbers of the dispersive wave, solitary wave, and periodic perturbation, respectively, is the sideband frequency, is the width of the soliton-like pulse with the shape , and is an integer.…”
Section: A Negative Gddmentioning
confidence: 99%
“…The spectral energy of the dispersive wave was estimated to be 6.9% of the total spectral energy, and its presence did not deteriorate the long-term stability of the mode-locked laser. The coexistence of dispersive waves with the main modelocked pulse has been reported and analyzed previously [27][28][29][30][31][32]. These waves co-propagate with the main pulse, and some of the pulse energy is coupled out to the dispersive waves if they are phase-matched.…”
Section: Resultsmentioning
confidence: 95%
“…The higher order dispersion coefficients have the substantial effect in this regime. A general phase-matching condition can be expressed as [31] (1) where are dispersion coefficients, 0 is the carrier frequency, ( ) is the phase delay per round-trip, is the dispersive wave frequency and where is the FWHM of the mode-locked pulse duration. Figure 2(b) (upper curve).…”
Section: Resultsmentioning
confidence: 99%
“…Moreover, if the considerable amount of a pulse energy is located in the Kelly sidebands, then the sideband itself can be considered as a sub-ns pulse with a very high soliton number [43,44]. If such a pulse is being amplified, it could lead to the modulational instability effect [16] contributing to the supercontinuum formation.…”
Section: Sc In Single-mode Step-index Chalcogenide Fibermentioning
confidence: 99%