Analysis on an extended Majda--Biello system

preprint2015arXivOpen access

Abstract

In this paper, we begin with extended Majda--Biello system (BSAB equations): {0=At−DA3+μA1+ΓSB1S+ΓAB1A+(ABS)x0=BtS−B3S+ΓSA1+λB1S+σB1A+AA10=BtA−B3A+ΓAA1+σB1S−λB1A \left\{\begin{array}{l} 0=A_t-DA_3+μA_1+Γ_S B^S_1+Γ_A B_1^A+\left(AB^S\right)_x \\ 0=B^S_t-B_3^S+Γ_SA_1+λB_1^S+σB^A_1+AA_1 \\ 0=B^A_t-B_3^A+Γ_A A_1+σB_1^S-λB_1^A \end{array}\right. We conclude global well-posedness in L2(R)×L2(R)×L2(R)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 UU, we point out the effect on UU 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.

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