2007
DOI: 10.1364/josab.24.001254
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Conversion of a chirped Gaussian pulse to a soliton or a bound multisoliton state in quasi-lossless and lossy optical fiber spans

Abstract: The formation of single-soliton or bound-multisoliton states from a single linearly chirped Gaussian pulse in quasi-lossless and lossy fiber spans is examined. The conversion of an input-chirped pulse into soliton states is carried out by virtue of the so-called direct Zakharov-Shabat spectral problem, the solution of which allows one to single out the radiative (dispersive) and soliton constituents of the beam and determine the parameters of the emerging bound state(s). We describe here how the emerging pulse… Show more

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Cited by 15 publications
(8 citation statements)
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“…This has mostly been considered for distributed (continuous) loss, see Refs. [15,[40][41][42], but in Ref. [30] an asymmetrically tuned spectral filter was considered.…”
Section: B Imaginary Eigenvalues Can Move Up and Downmentioning
confidence: 99%
“…This has mostly been considered for distributed (continuous) loss, see Refs. [15,[40][41][42], but in Ref. [30] an asymmetrically tuned spectral filter was considered.…”
Section: B Imaginary Eigenvalues Can Move Up and Downmentioning
confidence: 99%
“…The threshold value |c k | th coincides with the well-known area criterion (see [29]) for a soliton nucleation, although the latter is strictly valid only for single-hump pulses with a constant phase [46] and is usually violated in the case of chirped inputs [45,47], where the creation of solitons is significantly suppressed (the latter fact was utilized in the concept of a solitonbased discriminator [48]). In the context of coherent optical communication, due to highly mixed phases of the optical signal resulting from signal overlap from different time slots or from the use of many sub-carriers in OFDM, the phase of an optical signal becomes effectively random [49] and the soliton formation is dramatically suppressed [48].…”
Section: Correspondence Between the Ns And Linear Spectrum Soliton Cmentioning
confidence: 78%
“…Note that for the chirped and random profiles, the soliton nucleation is strongly suppressed by both the chirp intensity (rapid phase variations) [47] and the incoherence in the input signal [44,45,[48][49][50], and one can expect the mitigation of the threshold values (34) produced by a single tone in the case of a multitone randomly coded signal.…”
Section: Correspondence Between the Ns And Linear Spectrum Soliton Cmentioning
confidence: 99%
“…The BO method was used in the works [49,[51][52][53] for the calculation of continuous nonlinear spectrum for the nonlinear inverse synthesis scheme (see subsection 5B below). It also demonstrated good results in the calculation of the perturbed dynamics of solitonic eigenvalues [102][103][104]. The calculation of norming constants, requiring a (ζ n ), is described in [101,102].…”
Section: Boffetta-osborne (Bo) Transfer Methodmentioning
confidence: 93%