Lyapunov Exponents versus Integrability in Random Conservative Dynamics
Gianluigi Del Magno, João Lopes Dias, José Pedro Gaivão
TL;DR
This work establishes an invariance principle for random, volume-preserving maps on $\mathbb{T}^2$ showing that vanishing Lyapunov exponents force the existence of a measurable invariant structure on the projective bundle $P M$. The authors apply this principle to two fundamental systems: random additive perturbations of convex billiards on constant-curvature surfaces and random perturbations of the standard map. They prove a sharp rigidity result: for random billiards, $\lambda^+ = 0$ almost everywhere if and only if the table is a geodesic disk; for random standard maps, $\lambda^+ = 0$ almost everywhere if and only if the map is integrable ($K=0$). These findings link stochastic perturbations to deterministic integrability, illustrating that randomness preserves integrable structure and that non-integrability manifests as positive Lyapunov exponents under random perturbations.
Abstract
We consider random dynamical systems generated by volume-preserving piecewise $C^{1}$ maps. For this class of random systems, we establish an invariance principle asserting that if the Lyapunov exponents vanish, then there exists a measurable family of probability measures on the projective bundle that is invariant under the projective cocycle induced by the derivative. We apply this principle to two classes of random systems. First, we study random additive perturbations of a single billiard map associated with a strictly convex planar table on a surface of constant curvature. In this setting, we prove that the Lyapunov exponents vanish almost everywhere if and only if the billiard table is a geodesic disk. Second, we consider random additive perturbations of a single standard map and show that the Lyapunov exponents vanish almost everywhere if and only if the standard map is integrable.
