Discrete Derivative Nonlinear Schrödinger Equations

We consider novel discrete derivative nonlinear Schrödinger equations (ddNLSs). Taking the continuum derivative nonlinear Schrödinger equation (dNLS), we use for the discretisation of the derivative the forward, backward, and central difference schemes, respectively, and term the corresponding equations forward, backward, and central ddNLSs. We show that in contrast to the dNLS, which is completely integrable and supports soliton solutions, the forward and backward ddNLSs can be either dissipative or expansive. As a consequence, solutions of the forward and backward ddNLSs behave drastically differently compared to those of the (integrable) dNLS. For the dissipative forward ddNLS, all solutions decay asymptotically to zero, whereas for the expansive forward ddNLS all solutions grow exponentially in time, features that are not present in the dynamics of the (integrable) dNLS. In comparison, the central ddNLS is characterized by conservative dynamics. Remarkably, for the central ddNLS the total momentum is conserved, allowing the existence of solitary travelling wave (TW) solutions. In fact, we prove the existence of solitary TWs, facilitating Schauder’s fixed-point theorem. For the damped forward expansive ddNLS we demonstrate that there exists such a balance of dissipation so that solitary stationary modes exist.

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Journal
Mathematics
Published
2024-12-30
DOI
https://doi.org/10.3390/math13010105
Primary Topic
Nonlinear Photonic Systems
Type
article
Field-Weighted Citation Impact
0.00

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article

Discrete Derivative Nonlinear Schrödinger Equations

Jesús Cuevas–Maraver, D. Hennig
Mathematics
Nonlinear Photonic Systems
article

Discrete Derivative Nonlinear Schrödinger Equations

Jesús Cuevas–Maraver, D. Hennig
article en

Abstract

We consider novel discrete derivative nonlinear Schrödinger equations (ddNLSs). Taking the continuum derivative nonlinear Schrödinger equation (dNLS), we use for the discretisation of the derivative the forward, backward, and central difference schemes, respectively, and term the corresponding equations forward, backward, and central ddNLSs. We show that in contrast to the dNLS, which is completely integrable and supports soliton solutions, the forward and backward ddNLSs can be either dissipative or expansive. As a consequence, solutions of the forward and backward ddNLSs behave drastically differently compared to those of the (integrable) dNLS. For the dissipative forward ddNLS, all solutions decay asymptotically to zero, whereas for the expansive forward ddNLS all solutions grow exponentially in time, features that are not present in the dynamics of the (integrable) dNLS. In comparison, the central ddNLS is characterized by conservative dynamics. Remarkably, for the central ddNLS the total momentum is conserved, allowing the existence of solitary travelling wave (TW) solutions. In fact, we prove the existence of solitary TWs, facilitating Schauder’s fixed-point theorem. For the damped forward expansive ddNLS we demonstrate that there exists such a balance of dissipation so that solitary stationary modes exist.

MathematicsVol. 13(1)
University of Thessaly (GR), Universidad de Sevilla (ES)
Agencia Estatal de Investigación
Openalex Percentile: Top 77%
Nonlinear Photonic Systems
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Discrete Derivative Nonlinear Schrödinger Equations — Jesús Cuevas–Maraver, D. Hennig · Mathematics (2024) | TGRS Research Map | TGRS