I. Introduction
Stationary statistics of the dynamical systems can be found as the steady-state solution of a relevant PDE with the Fokker–Plank operator [1]. However, it is difficult to solve for the Fokker–Plank equation over a finite time interval. The appropriate mathematical basis to examine the escape processes in the weakly perturbed systems is large deviations theory, which provides an alternative approach to the analysis of the weakly perturbed dynamics, opposed to the PDE solution. In this paper, we use the essentials of large deviations theory in the form developed in [2]–[5].