Solutions of first-passage time problems: A biscaling approach

We study the first-passage time (FPT) problem for widespread recurrent processes in confined though large systems and present a comprehensive framework for characterizing the FPT distribution over many timescales. We find that the FPT statistics can be described by two scaling functions: one corresponds to the solution for an infinite system, and the other describes a scaling that depends on system size. We find a universal scaling relationship for the FPT moments 〈t^{q}〉 with respect to the domain size and the source-target distance. This scaling exhibits a transition at q_{c}=θ, where θ is the persistence exponent. For low-order moments with q<q_{c}, convergence occurs towards the moments of an infinite system. In contrast, the high-order moments, q>q_{c}, can be derived from an infinite density function. The presented uniform approximation, connecting the two scaling functions, provides a description of the first-passage time statistics across all timescales. We extend the results to include diffusion in a confining potential in the high-temperature limit, where the potential strength takes the place of the system's size as the relevant scale. This study has been applied to various mediums, including a particle in a box, two-dimensional wedge, fractal geometries, non-Markovian processes, and the nonequilibrium process of resetting.

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Publication Details

Journal
Physical review. E
Published
2025-04-01
DOI
https://doi.org/10.1103/physreve.111.044103
Citations
4
Primary Topic
Diffusion and Search Dynamics
Type
article
Field-Weighted Citation Impact
3.22

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article

Solutions of first-passage time problems: A biscaling approach

David A. Kessler, Eli Barkai, Talia Baravi
4 citations
Physical review. E
Diffusion and Search Dynamics
3.22
article

Solutions of first-passage time problems: A biscaling approach

David A. Kessler, Eli Barkai, Talia Baravi
article en
4 citations

Abstract

We study the first-passage time (FPT) problem for widespread recurrent processes in confined though large systems and present a comprehensive framework for characterizing the FPT distribution over many timescales. We find that the FPT statistics can be described by two scaling functions: one corresponds to the solution for an infinite system, and the other describes a scaling that depends on system size. We find a universal scaling relationship for the FPT moments 〈t^{q}〉 with respect to the domain size and the source-target distance. This scaling exhibits a transition at q_{c}=θ, where θ is the persistence exponent. For low-order moments with q<q_{c}, convergence occurs towards the moments of an infinite system. In contrast, the high-order moments, q>q_{c}, can be derived from an infinite density function. The presented uniform approximation, connecting the two scaling functions, provides a description of the first-passage time statistics across all timescales. We extend the results to include diffusion in a confining potential in the high-temperature limit, where the potential strength takes the place of the system's size as the relevant scale. This study has been applied to various mediums, including a particle in a box, two-dimensional wedge, fractal geometries, non-Markovian processes, and the nonequilibrium process of resetting.

Physical review. EVol. 111(4)
Bar-Ilan University (IL)
Israel Science Foundation
Climate action
Openalex Percentile: Top 9%
Diffusion and Search Dynamics
3.22
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