1992
DOI: 10.1364/josab.9.001358
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Wave breaking in nonlinear-optical fibers

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Cited by 219 publications
(123 citation statements)
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“…The nonmonotonic chirp induced by SPM gives rise to the overlapping between different frequencies in the pulse tails at the normal dispersion regime [2]. This situation leads to nonlinear frequency mixing through χ 3 susceptibility.…”
Section: Introductionmentioning
confidence: 99%
“…The nonmonotonic chirp induced by SPM gives rise to the overlapping between different frequencies in the pulse tails at the normal dispersion regime [2]. This situation leads to nonlinear frequency mixing through χ 3 susceptibility.…”
Section: Introductionmentioning
confidence: 99%
“…Finally, another aspect we stress is that the dynamics undergone in the anomalous dispersive fiber of the soliton regenerator leads to a soliton-like compression [21,26], which is fundamentally different from the continuous temporal broadening undergone in the normal regime [25].…”
Section: B Temporal Properties Of the Regenerated Signalmentioning
confidence: 98%
“…According to the initial conditions of the input pulse, the initial stage of nonlinear dynamics in the fiber, where Kerr-induced self-phase modulation (SPM) dominates over GVD, may be very different. Indeed, input pulses with a negative chirp coefficient will experience spectral compression as a result of SPM [15,28,29], whereas for initially positively chirped (or Fourier transform-limited) pulses, spectral broadening will drive the nonlinear dynamics and eventually lead to optical wave-breaking [30]. Moreover, propagation in the nonlinear fiber is impacted by both GVD and SPM effects, which are characterized by the respective coefficients 2 and .…”
Section: Principle Of Nonlinear Pulse Shaping and Available Degrees Omentioning
confidence: 99%
“…2 that there are three different regions of parameter space that support the formation of a parabolic pulse with the desired duration. The region featuring normal input chirping corresponds to a transient state of the nonlinear dynamic pulse evolution in the fiber toward wave breaking [18,30,45]. The region featuring low input powers (N below 2) and large propagated lengths corresponds to a long-term far-field evolution regime in the fiber characterized by the formation of pulses of a spectronic nature [20,21,46].…”
mentioning
confidence: 99%