Stability analysis for localized solutions in PDEs and nonlocal equations on $\mathbb{R}^m$
Matthieu Cadiot
TL;DR
This work develops a computer-assisted framework for linear stability analysis of localized solutions to PDEs and nonlocal equations on $\mathbb{R}^m$, explicitly separating the essential spectrum, given by the symbol range $\{l(\xi): \xi\in\mathbb{R}^m\}$, from discrete eigenvalues. By translating the problem to Fourier coefficients on bounded cubes and employing a pseudo-diagonalization with a generalized Gershgorin theorem, the authors obtain explicit, computable disks that enclose eigenvalues of the Jacobian at the true localized solution $\tilde{u}$, with controlled radii and multiplicities. A two-tier homotopy argument transfers spectral enclosures from a finite-dimensional, periodic surrogate $DF(U_0)$ to the full operator $D\mathbb{F}(\tilde{u})$, providing rigorous localization away from the essential spectrum. The methodology is demonstrated on planar Swift-Hohenberg, capillary-gravity Whitham, and Gray-Scott models, yielding precise stability conclusions, kernel dimensions, and symmetry-induced structure (e.g., radial symmetry) of localized solutions. This framework advances rigorous stability analysis on unbounded domains by combining Fourier-space discretizations, operator-theoretic localization, and interval arithmetic to deliver fully explicit, verifiable results.
Abstract
In this paper, we present a general methodology for investigating the linear stability of localized solutions in PDEs and nonlocal equations on $\mathbb{R}^m$. More specifically, we control the spectrum of the Jacobian $D\mathbb{F}(\tilde{u})$ at a localized solution $\tilde{u}$, enclosing both the eigenvalues and the essential spectrum. Our approach is computer-assisted and is based on a controlled approximation of $D\mathbb{F}(\tilde{u})$ by its Fourier coefficients counterpart on a bounded domain $Ω_d = (-d,d)^m$. We first control the spectrum of the Fourier coefficients operator combining a pseudo-diagonalization and a generalized Gershgorin disk theorem. Then, deriving explicit estimates between the problem on $Ω_d$ and the one on $\mathbb{R}^m$, we construct disks in the complex plane enclosing the eigenvalues of $D\mathbb{F}(\tilde{u})$. Using computer-assisted analysis, the localization of the spectrum is made rigorous and fully explicit. We present applications to the establishment of stability for localized solutions in the planar Swift-Hohenberg PDE, in the planar Gray-Scott model and in the capillary-gravity Whitham equation.
