Abstract

The authors show the disintegration of a higher-order rogue wave solution of the nonlinear Schr\odinger equation into its constituent parts in the presence of system perturbation.

Highlights

  • The discovery of the soliton solutions for certain types of nonlinear evolution equations marks an important milestone in mathematical physics

  • nonlinear Schrödinger equation (NLSE) and its solutions have been applied in optics, plasma physics, hydrodynamics, condensed matter physics, and Bose-Einstein condensates [1,2,3,4], while in mathematics they are studied in integrability, Riemann-Hilbert problems, as well as in the theory of solitons and rogue waves [5,6]

  • The successful implementation of the inverse scattering transformation on NLSE by Zakharov and Shabat led to the soliton solutions in their exact mathematical forms [7]

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Summary

INTRODUCTION

The discovery of the soliton solutions for certain types of nonlinear evolution equations marks an important milestone in mathematical physics. In the Fourier domain, this translates to generating a cascade of spectral sidebands These sidebands and the original continuous-wave exchange energy, eventually forming a series of pulses which gives rise to the Akhmediev breather solution [14]. This breather solution appears in the form of well-known rogue wave solution as its limiting case when the period in the transverse dimension becomes infinite. We demonstrate that under weak symmetry-breaking perturbation, a higher-order rogue wave solution breaks apart and reduces to its constituent fundamental rogue waves. This fascinating observation bears a striking similarity to soliton fission phenomena. Its amplitude and phase profiles at the maximum compression point are shown in Figs. 1(c) and 1(d)

SECOND-ORDER ROGUE WAVE SOLUTION AND ITS FISSION
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THIRD- AND HIGHER-ORDER ROGUE WAVE FISSION
EVOLUTION DYNAMICS BEYOND ROGUE WAVE FISSION
CONCLUSION
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