Abstract:We address the stability of multi-solitons for the cubic nonlinear Schrödinger (NLS) equation on the line. By using the dressing transformation and the inverse scattering transform methods, we establish the orbital stability of multi-solitons in the L 2 (R) space when the initial data is in a weighted L 2 (R) space.
“…Our approach follows the strategy used by Mizumachi and Pelinovsky in [25] for proving L 2 -orbital stability of the NLS solitons. Their result was extended by Contreras and Pelinovsky in [11] to multi-solitons of the NLS equation by using a more general dressing transformation. Furthermore, the recent work [12] of Cuccagna and Pelinovsky shows how an asymptotic stability of the NLS solitons can be deduced by combining the auto-Bäcklund transformation and the nonlinear steepest descent method.…”
We prove L 2 orbital stability of Dirac solitons in the massive Thirring model. Our analysis uses local well posedness of the massive Thirring model in L 2 , conservation of the charge functional, and the auto-Bäcklund transformation. The latter transformation exists because the massive Thirring model is integrable via the inverse scattering transform method.
“…Our approach follows the strategy used by Mizumachi and Pelinovsky in [25] for proving L 2 -orbital stability of the NLS solitons. Their result was extended by Contreras and Pelinovsky in [11] to multi-solitons of the NLS equation by using a more general dressing transformation. Furthermore, the recent work [12] of Cuccagna and Pelinovsky shows how an asymptotic stability of the NLS solitons can be deduced by combining the auto-Bäcklund transformation and the nonlinear steepest descent method.…”
We prove L 2 orbital stability of Dirac solitons in the massive Thirring model. Our analysis uses local well posedness of the massive Thirring model in L 2 , conservation of the charge functional, and the auto-Bäcklund transformation. The latter transformation exists because the massive Thirring model is integrable via the inverse scattering transform method.
“…The N-fold transformation for the NLS equation was derived and justified in [29] by using the dressing method. Adopting the present notations with N = 1, [29] and σ 1 and σ 3 are standard Pauli matrices, we obtain the onefold transformation in the explicit formũ…”
Section: (B) Darboux Transformationmentioning
confidence: 99%
“…By solving the linear system of the dressing method obtained in [29], we obtain solutions r 1,2 of the linear system (1.2)-(1.3) with λ 1,2 and the new potentialũ, where r 1 , r 2 andũ are defined in the form…”
Section: (B) Darboux Transformationmentioning
confidence: 99%
“…This solution was used in [29] to inspect two-soliton solutions of the NLS equation (1.1). By using the non-periodic solutions of the linear system (1.2)-(1.3) and the Darboux transformations (3.13) and (3.14), we can finally obtain the exact solutions for the rogue periodic waves of the NLS equation (1.1) in the sense of definition (1.11).…”
Section: (B) Darboux Transformationmentioning
confidence: 99%
“…To obtain the twofold Darboux transformation by using the formalism of [29], we set N = 2, λ 1,2 = −iz 1,2 , (p 1,2 , q 1,2 ) = σ 3 σ 1s1,2 and the transformation matrix…”
stand for rogue waves on a periodic background. The nonlinear Schrödinger equation in the focusing case admits two families of periodic wave solutions expressed by the Jacobian elliptic functions and. Both periodic waves are modulationally unstable with respect to long-wave perturbations. Exact solutions for the rogue periodic waves are constructed by using the explicit expressions for the periodic eigenfunctions of the Zakharov-Shabat spectral problem and the Darboux transformations. These exact solutions generalize the classical rogue wave (the so-called Peregrine's breather). The magnification factor of the rogue periodic waves is computed as a function of the elliptic modulus. Rogue periodic waves constructed here are compared with the rogue wave patterns obtained numerically in recent publications.
We consider the massive Thirring model in the laboratory coordinates and explain how the inverse scattering transform can be developed with the Riemann-Hilbert approach. The key ingredient of our technique is to transform the corresponding spectral problem to two equivalent forms: one is suitable for the spectral parameter at the origin and the other one is suitable for the spectral parameter at infinity. Global solutions to the massive Thirring model are recovered from the reconstruction formulae at the origin and at infinity.A.S. gratefully acknowledges financial support from the project SFB-TRR 191 "Symplectic Structures in Geometry, Algebra and Dynamics" (Cologne University, Germany).
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