First-Order Transition to Chaos with Critical Slowing Down
Abstract
Can the transition from integrability to chaos be discontinuous? We show that it can, and that the resulting first-order dynamical transition coexists with critical slowing down. Using an analytically tractable confined random walk and a deterministic stadium-like billiard, we find a finite jump of the stationary diffusive observable at the transition while the relaxation time diverges. Both systems display normal diffusion and the same exponent set (α,β,z)=(0,1/2,−2). We trace this agreement to a common coarse-grained mechanism: diffusion in a finite accessible domain with a diffusion coefficient that vanishes quadratically with the perturbation. The results identify a discontinuous route from integrability to chaos and provide evidence for a broader universality class of first-order dynamical transitions.
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BibTeX
@misc{fonseca2026firstorder,
title = {{First-Order Transition to Chaos with Critical Slowing Down}},
author = {Anne Ketri P. da Fonseca and Marcelo de Almeida Presotto and Diego F. M. Oliveira and Edson D. Leonel},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.13614},
eprint = {2609.13614},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.13614},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - First-Order Transition to Chaos with Critical Slowing Down
AU - Anne Ketri P. da Fonseca
AU - Marcelo de Almeida Presotto
AU - Diego F. M. Oliveira
AU - Edson D. Leonel
PY - 2026
DA - 2026/09/12
PB - arXiv
DO - 10.48550/arxiv.2609.13614
UR - https://arxiv.org/abs/2609.13614
AB - Can the transition from integrability to chaos be discontinuous? We show that it can, and that the resulting first-order dynamical transition coexists with critical slowing down. Using an analytically tractable confined random walk and a deterministic stadium-like billiard, we find a finite jump of the stationary diffusive observable at the transition while the relaxation time diverges. Both systems display normal diffusion and the same exponent set (α,β,z)=(0,1/2,−2). We trace this agreement to a common coarse-grained mechanism: diffusion in a finite accessible domain with a diffusion coefficient that vanishes quadratically with the perturbation. The results identify a discontinuous route from integrability to chaos and provide evidence for a broader universality class of first-order dynamical transitions.
ER -