2014
DOI: 10.1088/0951-7715/27/4/r1
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Superregular solitonic solutions: a novel scenario for the nonlinear stage of modulation instability

Abstract: We describe a general N -solitonic solution of the focusing nonlinear Schrödinger equation in the presence of a condensate by using the dressing method. We give the explicit form of one-and two-solitonic solutions and study them in detail as well as solitonic atoms and degenerate solutions. We distinguish a special class of solutions that we call regular solitonic solutions. Regular solitonic solutions do not disturb phases of the condensate at infinity by coordinate. All of them can be treated as localized pe… Show more

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Cited by 122 publications
(180 citation statements)
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“…[33,34] obtained within the framework of the self-focusing NLSE in dimensionless form, iψ ξ þ 1=2ψ ττ þ │ψ│ 2 ψ ¼ 0, where subscripted variables stand for partial differentiations. Here, ψ is a wave group or wave envelope which is a function of ξ (a scaled propagation distance or longitudinal variable) and τ (a comoving time, or transverse variable, moving with the wave-group velocity).…”
Section: Breather Formalismmentioning
confidence: 99%
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“…[33,34] obtained within the framework of the self-focusing NLSE in dimensionless form, iψ ξ þ 1=2ψ ττ þ │ψ│ 2 ψ ¼ 0, where subscripted variables stand for partial differentiations. Here, ψ is a wave group or wave envelope which is a function of ξ (a scaled propagation distance or longitudinal variable) and τ (a comoving time, or transverse variable, moving with the wave-group velocity).…”
Section: Breather Formalismmentioning
confidence: 99%
“…In general, the one-breather solution is a localized object with characteristic size δτ ∼ 1=2η ¼ ½ðR − 1=RÞ cos α −1 , moving on top of the continuous wave with breather group velocity V g ¼ γ=η ¼ 2sinαðR 4 þ 1Þ=½RðR 2 − 1Þ , and oscillating with period T ¼2π=2ω¼2πR 2 = ½ðR 4 −1Þcos2α [34]. Thus, R, α control the main breather properties.…”
Section: Breather Formalismmentioning
confidence: 99%
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