Instability bands for periodic traveling waves in the modified Korteweg-de Vries equation
Shikun Cui, Dmitry E. Pelinovsky
TL;DR
This work studies spectral stability of periodic traveling waves in the focusing mKdV equation by leveraging a squared-eigenfunction relation between the Lax pair and the linearized stability problem. It confirms that the dnoidal-like wave (dn-generalization) is spectrally stable for all parameters, while the cn-like wave (cn-generalization) is spectrally unstable for all parameters; crucially, the onset of co-periodic instability for the cn-family transforms instability bands from a figure-8 pattern (crossing the imaginary axis) to a figure-infinity pattern (crossing the real axis). Analytical criteria, grounded in the Lax spectrum and the root structure of the associated quartic invariant, are complemented by robust Fourier-collocation numerics that illustrate both stable and unstable regimes and the 8→∞ transition. The results enhance understanding of modulational-type instabilities in integrable and near-integrable wave models and have potential relevance for Stokes-wave-type phenomena in fluids and optical systems, with open questions about explicit Lax-spectrum locations for cn-waves and extensions to nonintegrable settings.
Abstract
Two families of periodic traveling waves exist in the focusing mKdV (modified Korteweg-de Vries) equation. Spectral stability of these waveforms with respect to co-periodic perturbations of the same period has been previously explored by using spectral analysis and variational formulation. By using tools of integrability such as a relation between squared eigenfunctions of the Lax pair and eigenfunctions of the linearized stability problem, we revisit the spectral stability of these waveforms with respect to perturbations of arbitrary periods. In agreement with previous works, we find that one family is spectrally stable for all parameter configurations, whereas the other family is spectrally unstable for all parameter configurations. We show that the onset of the co-periodic instability for the latter family changes the instability bands from figure-$8$ (crossing at the imaginary axis) into figure-$\infty$ (crossing at the real axis).
