2019
DOI: 10.1007/s11071-019-04991-x
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Non-autonomous solitons in inhomogeneous nonlinear media with distributed dispersion

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Cited by 37 publications
(25 citation statements)
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“…)Z, and other parameters ζ, X and Z are as given in Eq. (14). This IICS admits well-known bell-type/symmetric-single-hump profile with certain amplitude B j , width (proportional to inverse of amplitude), and velocity 2δk 1I of propagation represented by the above form.…”
Section: Inhomogeneous Incoherently Coupled Solitonsmentioning
confidence: 99%
See 1 more Smart Citation
“…)Z, and other parameters ζ, X and Z are as given in Eq. (14). This IICS admits well-known bell-type/symmetric-single-hump profile with certain amplitude B j , width (proportional to inverse of amplitude), and velocity 2δk 1I of propagation represented by the above form.…”
Section: Inhomogeneous Incoherently Coupled Solitonsmentioning
confidence: 99%
“…From the above general one-soliton solution (14), one can easily understand that the choice S 1 = 0 leads to e δ (1) 11 and e 11 vanish. This results into a simple form corresponding to that of Manakov type solitons without the contribution from coherent nonlinearity, which can be designated as inhomogeneous incoherently coupled solitons (IICSs).…”
Section: Inhomogeneous Incoherently Coupled Solitonsmentioning
confidence: 99%
“…(37)-(38d) that β is constant, while α(t) and g 0 (t) satisfy the nonlinear second-order ODE, Thus, in the special case of constant λ 0 , λ and β, the problem of finding (t), η(t), and T (t) amounts to solving Eq. (49). The simplest possibility is to solve it for α(t) if g 0 (t) is known.…”
Section: Modulational Instability In the Inhomogeneous Cubic Derivatimentioning
confidence: 99%
“…The FR can also be imposed optically, by appropriate laser illumination [39][40][41][42], as well as by microwave [43] and electrostatic [44] fields. Then, NM for BEC may be realized using time-dependent and/or nonuniform control fields [4,8,40,41,[45][46][47]49]. In particular, the FR technique makes it possible to quickly reverse (in time) the interaction sign from repulsion to attraction (positive to negative scattering length), which gives rise, via the onset of the collapse, to abrupt shrinkage of the condensate, followed by a burst of emitted atoms and the formation of a stable residual condensate [50].…”
Section: Introductionmentioning
confidence: 99%
“…In a general system, the localized waves are spatially, temporally (solitons and breathers) or spatiotemporally (RWs) localized, and will arise from vanishing or nonvanishing backgrounds, however, these solutions may also exhibit non-localized phenomena, or appear in a variable background height in some special systems, e.g. nonautonomous systems [44,45]. Considering the Gross-Pitaevskii equation (GPE) as [7] ih…”
Section: Introductionmentioning
confidence: 99%