Dynamics of the Drinfeld-Sokolov-Wilson system: well-posedness and (in)stability of the traveling waves
Ognyan Christov, Sevdzhan Hakkaev, Seungly Oh, Atanas G. Stefanov
TL;DR
This work analyzes the periodic Drinfeld-Sokolov-Wilson system, proving local well-posedness at low regularity and global existence via $L^2$ conservation, plus persistence in $H^1\times L^2$ through a normal-form transformation. It constructs an explicit one-parameter family of $L$-periodic traveling waves using Jacobi elliptic functions and derives their spectral instability, showing exactly one unstable real mode and a Hamiltonian index of 1. The methodology blends Bourgain-space techniques for dispersive PDE with a normal-form approach to gain regularity, and couples analytical construction with a detailed spectral index computation (via operators $\mathcal{L}_+$, $\mathcal{H}$ and the matrix $\mathcal{D}$). The findings illuminate the delicate balance between dispersion and a dispersionless constraint in multi-component wave systems, with implications for the long-time dynamics and stability of coupled KdV-type models on periodic domains.
Abstract
We analyze the Drinfeld-Sokolob-Wilson system, which features a dispersive, KdV type evolution with a dispersionless conservation law. We establish well-posedness with low regularity initial data $L^2({\mathbb T})\times L^2({\mathbb T})$ for the Cauchy problem on periodic background, which is then extrapolated to global solutions, due to $L^2$ conservation law. We also establish a dynamically more relevant result, namely a global persistence of solutions with (large) initial data in $H^1({\mathbb T})\times L^2({\mathbb T})$. This is obtained by following a more sophisticated approach, specifically the method of normal forms. Finally, for a fixed period $L$, we construct an explicit one parameter family of periodic waves, see \eqref{2.16} below. We show that they are all spectrally unstable with respect to co-periodic perturbations. Specifically, we show that the Hamiltonian instability index is equal to one, which identifies the instability as a single positive growing mode.
