Conundrum of weak-noise limit for diffusion in a tilted periodic potential

The weak-noise limit of dissipative dynamical systems is often the most fascinating one. In such a case fluctuations can interact with a rich complexity, frequently hidden in deterministic systems, to give rise to phenomena that are absent for both noiseless and strong fluctuations regimes. Unfortunately, this limit is also notoriously hard to approach analytically or numerically. We reinvestigate in this context the paradigmatic model of nonequilibrium statistical physics consisting of inertial Brownian particles diffusing in a tilted periodic potential by exploiting state-of-the-art computer simulations of an extremely long timescale. In contrast to previous results on this longstanding problem, we draw an inference that in the parameter regime for which the particle velocity is bistable the lifetime of ballistic diffusion diverges to infinity when the thermal noise intensity tends to zero, i.e., an everlasting ballistic diffusion emerges. As a consequence, the diffusion coefficient does not reach its stationary constant value.

Automated summary

This study revisited the paradigmatic model of inertial Brownian particles diffusing in a tilted periodic potential using state-of-the-art computer simulations. The results indicate that in the parameter regime where the particle velocity is bistable, an everlasting ballistic diffusion emerges when the thermal noise intensity tends to zero, resulting in the diffusion coefficient not reaching its stationary constant value.