dorsal/arxiv
View SchemaDiffusive synchronization of phase waves in the FitzHugh-Nagumo system
| Authors | Montie Avery, Paul Carter, Björn de Rijk, Arnd Scheel |
|---|---|
| Categories | |
| ArXiv ID | 2601.05377vv1 |
| URL | https://arxiv.org/abs/2601.05377 |
| License | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ |
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.
{
"annotation_id": "69ea74e0-27d9-4cf4-be9c-6d5a381d5e90",
"date_created": "2026-02-17T05:53:04.881000Z",
"date_modified": "2026-02-17T05:53:04.881000Z",
"file_hash": "2ac34db1acfc27ccef8be28186f176082feabbd31071a603293f0377f2c4c8ce",
"private": false,
"record": {
"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\u0027s 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.",
"arxiv_id": "2601.05377",
"authors": [
"Montie Avery",
"Paul Carter",
"Bj\u00f6rn de Rijk",
"Arnd Scheel"
],
"categories": [
"math.AP",
"math.DS",
"nlin.PS"
],
"license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
"title": "Diffusive synchronization of phase waves in the FitzHugh-Nagumo system",
"url": "https://arxiv.org/abs/2601.05377",
"version": "v1"
},
"schema_id": "dorsal/arxiv",
"source": {
"execution_id": "b408b8d8-e5e2-4f47-83f4-6e61a03db8cd",
"id": "arXiv Dataset",
"type": "Model",
"variant": "snapshot-2026-01-17",
"version": "0.1.0"
},
"user_id": 1000002
}