Analysis on an extended Majda--Biello system

In this paper, we begin with extended Majda--Biello system (BSAB equations): $$ \left\{\begin{array}{l} 0=A_t-DA_3+\mu A_1+\Gamma_S B^S_1+\Gamma_A B_1^A+\left(AB^S\right)_x \\ 0=B^S_t-B_3^S+\Gamma_SA_1+\lambda B_1^S+\sigma B^A_1+AA_1 \\ 0=B^A_t-B_3^A+\Gamma_A A_1+\sigma B_1^S-\lambda B_1^A \end{arra...

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Bibliographic Details
Published in:arXiv.org 2015-01
Main Author: Li, Yezheng
Format: Article
Language:English
Subjects:
Polynomials
Solitary waves
Well posed problems
Online Access:Get full text
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Summary:In this paper, we begin with extended Majda--Biello system (BSAB equations): $$ \left\{\begin{array}{l} 0=A_t-DA_3+\mu A_1+\Gamma_S B^S_1+\Gamma_A B_1^A+\left(AB^S\right)_x \\ 0=B^S_t-B_3^S+\Gamma_SA_1+\lambda B_1^S+\sigma B^A_1+AA_1 \\ 0=B^A_t-B_3^A+\Gamma_A A_1+\sigma B_1^S-\lambda B_1^A \end{array}\right. $$ We conclude global well-posedness in \(L^2(\mathbb{R})\times L^2(\mathbb{R})\times L^2(\mathbb{R})\) by Brougain's method and the stability of solitary wave solutions by putting it in a framework of generalised KdV type system with three components, where Hamiltonian structure plays an important role. Both of them are bases for numerical tests.\par Last but not least, we explore the effect of interaction of two solitary waves in Majda--Biello system in a novel way : \par \textit{While fixing initial data for one soliton \(U\), we point out the effect on \(U\) decays, to some extent and in certain range, in a polynomial way.} \par Since effect of interaction of two solitary waves are practically interesting, such kind of analysis, as we have explained, is likely be fundamental for generalised KdV type systems.
ISSN:2331-8422