A solvable normal form for coupled swarmalators
Abstract
Swarmalators are mobile generalizations of phase oscillators. Introduced to model systems in which sync and self-assembly interact, they remain poorly understood theoretically. Unlike the Kuramoto model for coupled oscillators, existing swarmalator models lack a normal-form foundation, and their basic stabilities and bifurcations remain largely unsolved. Here we address both problems. Building on Tanaka's reduction of chemotactic oscillators, we show that the canonical one-dimensional swarmalator model -- previously introduced as an ad hoc toy model -- is recovered in the first-harmonic, zero-lag limit, implying its behavior is generic. We then derive the stability boundaries organizing its four collective states, show they meet at a single cusp, correct a previously published order-parameter formula, and uncover a non-monotonic sync response absent in the Kuramoto model.
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BibTeX
@misc{okeeffe2026solvable,
title = {{A solvable normal form for coupled swarmalators}},
author = {Kevin P. O'Keeffe},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2607.09810},
eprint = {2607.09810},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2607.09810},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - A solvable normal form for coupled swarmalators
AU - Kevin P. O'Keeffe
PY - 2026
DA - 2026/09/30
PB - arXiv
DO - 10.48550/arxiv.2607.09810
UR - https://arxiv.org/abs/2607.09810
AB - Swarmalators are mobile generalizations of phase oscillators. Introduced to model systems in which sync and self-assembly interact, they remain poorly understood theoretically. Unlike the Kuramoto model for coupled oscillators, existing swarmalator models lack a normal-form foundation, and their basic stabilities and bifurcations remain largely unsolved. Here we address both problems. Building on Tanaka's reduction of chemotactic oscillators, we show that the canonical one-dimensional swarmalator model -- previously introduced as an ad hoc toy model -- is recovered in the first-harmonic, zero-lag limit, implying its behavior is generic. We then derive the stability boundaries organizing its four collective states, show they meet at a single cusp, correct a previously published order-parameter formula, and uncover a non-monotonic sync response absent in the Kuramoto model.
ER -