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The Darboux transformation of the Kundu-Eckhaus equation. (English) Zbl 1371.35277

Summary: We construct an analytical and explicit representation of the Darboux transformation (DT) for the Kundu-Eckhaus (KE) equation. Such solution and \(n\)-fold DT \(T_n\) are given in terms of determinants whose entries are expressed by the initial eigenfunctions and ‘seed’ solutions. Furthermore, the formulae for the higher order rogue wave (RW) solutions of the KE equation are also obtained by using the Taylor expansion with the use of degenerate eigenvalues \(\lambda_{2k-1}\to\lambda_1=-\frac 12a+\beta c^2+ic\), \(k=1,2,3,\dots\), all these parameters will be defined latter. These solutions have a parameter \(\beta\), which denotes the strength of the non-Kerr (quintic) nonlinear and the self-frequency shift effects. We apply the contour line method to obtain analytical formulae of the length and width for the first-order RW solution of the KE equation, and then use it to study the impact of the \(\beta\) on the RW solution. We observe two interesting results on localization characters of \(\beta\), such that if \(\beta\) is increasing from \(a/2\): (i) the length of the RW solution is increasing as well, but the width is decreasing; (ii) there exist a significant rotation of the RW along the clockwise direction. We also observe the oppositely varying trend if \(\beta\) is increasing to \(a/2\). We define an area of the RW solution and find that this area associated with \(c=1\) is invariant when \(a\) and \(\beta\) are changing.

MSC:

35Q55 NLS equations (nonlinear Schrödinger equations)
35A30 Geometric theory, characteristics, transformations in context of PDEs
37K35 Lie-Bäcklund and other transformations for infinite-dimensional Hamiltonian and Lagrangian systems
78A35 Motion of charged particles
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