2018
DOI: 10.1103/physreve.97.022208
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Formation of rogue waves from a locally perturbed condensate

Abstract: The one-dimensional focusing nonlinear Schrödinger equation (NLSE) on an unstable condensate background is the fundamental physical model, that can be applied to study the development of modulation instability (MI) and formation of rogue waves. The complete integrability of the NLSE via inverse scattering transform enables the decomposition of the initial conditions into elementary nonlinear modes: breathers and continuous spectrum waves. The small localized condensate perturbations (SLCP) that grow as a resul… Show more

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Cited by 60 publications
(67 citation statements)
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“…The spectral curve Γ 0 corresponding to the background (2) is rational, and a point γ ∈ Γ 0 is a pair of complex numbers γ = (λ, µ) satisfying the quadratic equation µ 2 = λ 2 + |a| 2 . The corresponding monodromy matrix: tr T 0 (λ) = 2 cos(µL) (37) defines the branch points (λ ± 0 , µ 0 ) = (±i|a|, 0) and the resonant (double) points (λ ± n , µ n ) = (± (nπ/L) 2 − |a| 2 , nπ/L), n ∈ Z, n = 0. Near the resonant points:…”
Section: Finite-gap Approximation Of the Aw Cauchy Problemmentioning
confidence: 99%
See 1 more Smart Citation
“…The spectral curve Γ 0 corresponding to the background (2) is rational, and a point γ ∈ Γ 0 is a pair of complex numbers γ = (λ, µ) satisfying the quadratic equation µ 2 = λ 2 + |a| 2 . The corresponding monodromy matrix: tr T 0 (λ) = 2 cos(µL) (37) defines the branch points (λ ± 0 , µ 0 ) = (±i|a|, 0) and the resonant (double) points (λ ± n , µ n ) = (± (nπ/L) 2 − |a| 2 , nπ/L), n ∈ Z, n = 0. Near the resonant points:…”
Section: Finite-gap Approximation Of the Aw Cauchy Problemmentioning
confidence: 99%
“…Concerning the NLS Cauchy problems in which the initial condition consists of a perturbation of the exact background (2), what we call the Cauchy problem of the AWs, if such a perturbation is localized, then slowly modulated periodic oscillations described by the elliptic solution of (1) play a relevant role in the longtime regime [16,17]. The relevance of the Kuznetsov -Kawata -Inoue -Ma solitons and of the superregular solitons (constructed by Zakharov and Gelash [93], see also [94], [95]) in this problem was investigated in [37].…”
Section: Introductionmentioning
confidence: 99%
“…These explicit expressions come from the exact SR breather solution (see Appendix A), where V grj is extracted from the hyperbolic function cosh Θ j , while V phj is extracted from the trigonometric function cos Φ j . If the higher-order terms are absent, α n>2 = 0, V grj , V phj reduce to their values for the simplest NLSE [18][19][20][21]. Figure 1 shows the evolution of V grj , V phj with q.…”
Section: Sr Breather Propertymentioning
confidence: 99%
“…Just as solitons, breathers may collide with each other creating complex interference patterns. They reveal high amplitude peaks when the breathers are synchronised [26,35,36], similar to the case of the soliton synchronisation [37,38].…”
mentioning
confidence: 66%