Large deviations of slow-fast systems driven by fractional Brownian motion
Siragan Gailus, Ioannis Gasteratos
TL;DR
The paper develops a large deviations framework for slow-fast stochastic systems driven by a fractional Brownian motion with $H>1/2$, under a homogenization regime where $\epsilon\to0$, $\eta\to0$, and $\sqrt{\eta}/\sqrt{\epsilon}\to0$. Employing a weak convergence/variational approach with controlled slow-fast dynamics and occupation measures, it proves an LDP with a rate function $S^H_{x_0}$ that, in certain regimes, takes an explicit non-variational form and exhibits a discontinuity as $H\to1/2^+$. The rate function is analyzed relative to the classical Freidlin–Wentzell theory, including a detailed limit as $H\to1/2^+$ and conditions under which the LDP rate remains continuous. The results advance the understanding of tail behavior in models with memory effects and offer a starting point for numerical rare-event methods in fractional-noise settings. The work also identifies avenues for extending the theory to general Gaussian inputs and alternative time-scale regimes.
Abstract
We consider a multiscale system of stochastic differential equations in which the slow component is perturbed by a small fractional Brownian motion with Hurst index $H>1/2$ and the fast component is driven by an independent Brownian motion. Working in the framework of Young integration, we use tools from fractional calculus and weak convergence arguments to establish a Large Deviation Principle in the homogenized limit, as the noise intensity and time-scale separation parameters vanish at an appropriate rate. Our approach is based in the study of the limiting behavior of an associated controlled system. We show that, in certain cases, the non-local rate function admits an explicit non-variational form. The latter allows us to draw comparisons to the case $H=1/2$ which corresponds to the classical Freidlin-Wentzell theory. Moreover, we study the asymptotics of the rate function as $H\rightarrow{1/2}^+$ and show that it is discontinuous at $H=1/2.$
