Periodic orbits in general Glass networks

Huy K. Vo

Home/Archive/arXiv

arXiv · 2311.11879

Periodic orbits in general Glass networks

Huy K. Vo

View original source ↗Read source document ↗Export metadata ↓

Abstract

Glass networks are piecewise linear ODE systems that models an interactive system where there are 'switching points': the underlying dynamic changes qualitatively when a certain variable pass over a threshold. One of the most well-studied class of models of the original Glass network are the cyclic attractor in the orthants (a sequence of orthants where the flow from one orthant to another is unanimous), which was first defined and analysed by Glass and Pasternack in 1978. In that paper, the authors gave a complete classification of the topological features of the flow in a full-rank cyclic attractor, which is a cyclic attractor that cannot be contained in any sub-cube in the graph of orthants. In this paper, we will extend the definition of cyclic attractor to one generalisation of the Glass network, one that allows for multiple switching points in each variables, and give a complete classification of the topological features of the flow for any cyclic attractor, both in the extended network and the original network, including non full-rank ones. We will show that in any cyclic attractor, there is either a unique and asymptotically stable periodic orbit, or that all periodic orbits are degenerated.

Explore related subjects

math.DS math.CA

Keep this discovery

BibTeX RIS

Huy K. Vo. 2023-11-20. Periodic orbits in general Glass networks. https://arxiv.org/abs/2311.11879

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

arXiv2026

Admissible Fourier Lengths, KAM Reducibility, and Spectral Applications

We develop a perturbative KAM reducibility theory for one-frequency $\mathrm{SL}(2,\mathbb{R})$ cocycles based on an admissible Fourier length $\ell$. The regularity relevant to the iteration is measured by positive adapted Fourier width rather than ordinary smoothness in the Euclidean length $|n|$. The same length governs Fourier decay, truncation and resonance scales, and the arithmetic condition controlling the small divisors. This framework contains the classical analytic and Gevrey settings, while non-monotone choices of $\ell$ allow classical nowhere differentiable Weierstrass-type perturbations and continuous perturbations outside every positive H\"older class. As spectral applications, we obtain purely absolutely continuous spectrum for every phase and $1/2$-H\"older continuity of the integrated density of states for the associated quasiperiodic Schr\"odinger operators. The Aubry dual has pure point spectrum for Lebesgue almost every dual phase, with eigenfunctions exponentially localized in the metric induced by $\ell$. We also construct nowhere differentiable quasiperiodic potentials with purely absolutely continuous Cantor spectrum.

math.DS↗

arXiv2026

Dynamics inside the attracting basins of some skew products

Polynomial skew products in $\mathbb{C}^2$ are maps of the form $F(z,w)=(P(z),Q(z,w))$, where $P$ and $Q$ are polynomials. Their local dynamics have been widely investigated. In this paper, we study the global dynamics inside Fatou components of some skew products. We consider all the inverse images in a Fatou component of a given point and use the Kobayashi metric to measure the distance between points. In the cases we consider, there are always arbitrarily large Kobayashi balls in the complement of these inverse sets.

math.DS↗

arXiv2026

Ergodicity of dynamical systems without uniqueness of orbits

Recently, there has been considerable interest in the study of non-deterministic dynamical systems. To analyze the chaotic behavior of such systems from a measure-theoretic viewpoint, it is desirable to consider ergodicity. However, the classical definition of ergodicity involves invariant sets, whose definition is not unique for non-deterministic dynamical systems. Thus, we are led to the question of which invariance yields an interesting definition of ergodicity. Here, we propose a definition based on the strong backward invariance and show that analogs of classical results hold. We also consider implications of the Birkhoff ergodic theorem for systems without uniqueness of orbits.

math.DS↗