Diffusive synchronization of phase waves in the FitzHugh-Nagumo system

TL;DR

This paper investigates the synchronization of phase waves in the FitzHugh-Nagumo reaction-diffusion system, revealing weak interactions and potential instabilities through advanced spectral and geometric analysis methods.

Contribution

It provides the first detailed analysis of phase wave synchronization in the FitzHugh-Nagumo system, introducing novel geometric and spectral techniques to handle complex eigenfunction scattering.

Findings

Weak interaction strength of order ε^{8/3}

Spectral stability ensures diffusive synchronization

Identification of potential finite-wavelength instabilities

Abstract

We analyze synchronization of relaxation oscillations in multiple-timescale reaction-diffusion systems. Interpreting synchronization as convergence to frequency-synchronized wave-train solutions, we resolve for the first time the case of phase waves. These waves are nearly phase-synchronized relaxation oscillations, featuring quasistationary plateaus of length $\varepsilon^{-1}$ separated by fast transition layers, where $\varepsilon\ll1$ is the timescale separation parameter. Tracking the decay of modulations via a Bloch-wave eigenfunction analysis, we find a remarkably weak interaction strength of order $\varepsilon^{8/3}$. This weak layer interaction and many of the technical difficulties arise from repeated scattering of eigenfunctions through fold points at the ends of the quasistationary plateaus. We capture this by combining a novel geometric desingularization approach with Lin's method, exponential trichotomies, and the Riccati transform. While our spectral stability analysis yields diffusive synchronization of all phase waves in the FitzHugh-Nagumo system, it also identifies potential finite-wavelength instabilities, which we realize in a system variant.