Regularized Boltzmann-Gibbs statistics for a Brownian particle in a non-confining field

Abstract

We consider an overdamped Brownian particle subject to an asymptotically flat potential with a trap of depth $U_0$ around the origin. When the temperature is small compared to the trap depth ($\xi =k_{B}T/U_0\ll 1$), there exists a range of timescales over which physical observables remain practically constant. This range can be very long, of the order of the Arrhenius factor ${\mathrm{e}}^{1/\xi }$. For these quasi-equilibrium states, the usual Boltzmann-Gibbs recipe does not work, since the partition function is divergent due to the flatness of the potential at long distances. However, we show that the standard Boltzmann-Gibbs (BG) statistical framework and thermodynamic relations can still be applied through proper regularization. This can be a valuable tool for the analysis of metastability in the non-confining potential fields that characterize a vast number of systems.

arXiv comment9 pages, 6 figures

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• Local equilibrium properties of ultraslow diffusion in the Sinai model
• A work fluctuation theorem for a Brownian particle in a non confining potentia
• Non-normalizable quasi-equilibrium states under fractional dynamics
• Brownian Fluctuations of a non-confining potential