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October 17, 2025Electronic Journal of Differential Equations0 citationsOpen Access

Inverse scattering method for an integrable system of derivative nonlinear Schrodinger equations

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MÜMehmet Ünlü

Key Points

  • The proposed method retrieves potentials from the Marchenko system using input data including reflection coefficients.
  • A set of linear integral equations is established, specifically the Marchenko system, to solve the inverse scattering problem.
  • Energy-dependent potentials are derived from the solution to the Marchenko system, providing insights into the integrable DNLS II system.
  • Time-evolved potentials are recovered from initial input data, showcasing the dynamic solution behavior of the system.

Abstract

We present a method for solving integrable systems of nonlinear partial differential equations, known as the derivative nonlinear Schrodinger II system (DNSL II system), also called the Chen-Lee-Liu system. This is done by presenting a solution technique for the inverse scattering problem for the corresponding linear system of ordinary differential equations with energy-dependent potentials. The relevant inverse scattering problem is solved by establishing a system of linear integral equations, which we refer to as the Marchenko system of linear integral equations. In solving the inverse scattering problem we use the input data set consisting of a transmission coefficient, a reflection coefficient, and the bound-state information presented in the form of a pair of matrix triplets. Using our data set as input to the Marchenko system, we recover the potentials from the solution to the Marchenko system. By using the time-evolved input data set, we recover the time-evolved potentials, where those potentials form a solution to the integrable DNLS II system. For more information and the latex file, see https://ejde.math.txstate.edu/Volumes/2025/97/abstr.html

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Cite This Study

Mehmet Ünlü (2025) studied this question.

synapsesocial.com/papers/68f199c5de32064e504dd023https://doi.org/10.58997/ejde.2025.97
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