SearcharxivSearch

arXiv · 2603.20653

Polynomial Random Dynamical Systems with Complete Connections and the Probability of Tending to Infinity

Abstract

We study polynomial random dynamical systems with complete connections on the Riemann sphere. In this framework, the choice of the next polynomial map is governed by a state-dependent rule with memory, extending both i.i.d. random dynamics and non-i.i.d. Markovian models. For each initial state, we define the probability that the random orbit tends to infinity. We prove that it is locally constant on the Fatou set, and that if all kernel Julia sets are empty, then it is continuous on the whole space. We also introduce stationary-averaged escaping probabilities with respect to stationary distributions of the induced state chain. Under the same kernel-emptiness assumption, these averaged probabilities are continuous. In addition, for each point of the Riemann sphere, the set of all possible stationary-averaged values is shown to be a compact interval determined by ergodic stationary distributions. We further give a sufficient condition for the stationary-averaged escaping probability to be everywhere positive and nontrivial. Finally, we provide examples showing RSCC-specific phenomena, including reinforcement-induced discontinuity, recovery of continuity under truncation, and genuinely mixed escaping behavior produced by stationary averaging.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Yoshiyuki Endo. 2026-03-21. Polynomial Random Dynamical Systems with Complete Connections and the Probability of Tending to Infinity. https://arxiv.org/abs/2603.20653

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

KEEP EXPLORING

Related papers

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

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

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