Diffusive escape through a narrow opening: new insights into a classic problem
Denis S Grebenkov, Gleb Oshanin

TL;DR
This paper develops a self-consistent approximation to analyze the mean first exit time for diffusing particles in micro-domains with small escape windows, highlighting the dominant role of energy barriers over diffusion in narrow escape problems.
Contribution
It introduces a general expression for escape time considering energy barriers and long-range interactions, revealing the barrier-limited nature of the problem and providing analytical formulas validated by simulations.
Findings
Barrier effects dominate as escape window size decreases.
Escape time is minimized at intermediate interaction ranges.
Analytical results agree well with numerical simulations.
Abstract
We study the mean first exit time of a particle diffusing in a circular or a spherical micro-domain with an impenetrable confining boundary containing a small escape window (EW) of an angular size . Focusing on the effects of an energy/entropy barrier at the EW, and of the long-range interactions (LRI) with the boundary on the diffusive search for the EW, we develop a self-consistent approximation to derive for a general expression, akin to the celebrated Collins-Kimball relation in chemical kinetics and accounting for both rate-controlling factors in an explicit way. Our analysis reveals that the barrier-induced contribution to is the dominant one in the limit , implying that the narrow escape problem is not "diffusion-limited" but rather "barrier-limited". We present the small- expansion for , in which the coefficients in…
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