Kuznetsov-Ma rogue wave clusters of the nonlinear Schrodinger equation

被引:1
|
作者
Alwashahi, Sarah [1 ,2 ]
Aleksic, Najdan B. [3 ]
Belic, Milivoj R. [3 ]
Nikolic, Stanko N. [3 ,4 ]
机构
[1] Univ Belgrade, Fac Phys, Studentski trg 12, Belgrade 11001, Serbia
[2] Univ Libya, Fac Sci Al Zawiya, Al Ajaylat, Libya
[3] Texas A&M Univ Qatar, Div Arts & Sci, POB 23874, Doha, Qatar
[4] Univ Belgrade, Inst Phys Belgrade, Pregrev 118, Belgrade 11080, Serbia
关键词
Nonlinear Schrodinger equation; Rogue waves; Kuznetsov-Ma rogue wave clusters; Darboux transformation; VARIATIONAL-PRINCIPLES; PEREGRINE SOLITON; HIROTA EQUATION; MODULATION; BREATHERS; OPTICS;
D O I
10.1007/s11071-023-08480-0
中图分类号
TH [机械、仪表工业];
学科分类号
0802 ;
摘要
In this work, we investigate rogue wave (RW) clusters of different shapes, composed of Kuznetsov-Ma solitons (KMSs) from the nonlinear Schrodinger equation (NLSE) with Kerr nonlinearity. We present three classes of exact higher-order solutions on uniform background that are calculated using the Darboux transformation (DT) scheme with precisely chosen parameters. The first solution class is characterized by strong intensity narrow peaks that are periodic along the evolution x-axis, when the eigenvalues in DT scheme generate KMSs with commensurate frequencies. The second solution class exhibits a form of elliptical rogue wave clusters; it is derived from the first solution class when the first m evolution shifts in the nth-order DT scheme are nonzero and equal. We show that the high-intensity peaks built on KMSs of order n - 2m periodically appear along the x-axis. This structure, considered as the central rogue wave, is enclosed by m ellipses consisting of a certain num- ber of the first-order KMSs determined by the ellipse index and the solution order. The third class of KMS clusters is obtained when purely imaginary DT eigenvalues tend to some preset offset value higher than one, while keeping the x-shifts unchanged. We showthat the central rogue wave at (0, 0) always retains its n - 2m order. The n tails composed of the first-order KMSs are formed above and belowthe centralmaximum. When n is even, more complicated patterns are generated, with m and m - 1 loops above and below the central RW, respectively. Finally, we compute an additional solution class on a wavy background, defined by the Jacobi elliptic dnoidal function, which displays specific intensity patterns that are consistent with the background wavy perturbation. This work demonstrates an incredible power of the DT scheme in creating new solutions of the NLSE and a tremendous richness in form and function of those solutions.
引用
收藏
页码:12495 / 12509
页数:15
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