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Leftward, rightward, and complete exit-time distributions of jump processes

J. Klinger, R. Voituriez, and O. Bénichou
Phys. Rev. E 107, 054109 – Published 8 May 2023

Abstract

First-passage properties of continuous stochastic processes confined in a one-dimensional interval are well described. However, for jump processes (discrete random walks), the characterization of the corresponding observables remains elusive, despite their relevance in various contexts. Here we derive exact asymptotic expressions for the leftward, rightward, and complete exit-time distributions from the interval [0,x] for symmetric jump processes starting from x0=0, in the large x and large time limit. We show that both the leftward probability F0̲,x(n) to exit through 0 at step n and rightward probability F0,x̲(n) to exit through x at step n exhibit a universal behavior dictated by the large-distance decay of the jump distribution parametrized by the Levy exponent μ. In particular, we exhaustively describe the n(x/aμ)μ and n(x/aμ)μ limits and obtain explicit results in both regimes. Our results finally provide exact asymptotics for exit-time distributions of jump processes in regimes where continuous limits do not apply.

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  • Received 5 December 2022
  • Accepted 3 April 2023

DOI:https://doi.org/10.1103/PhysRevE.107.054109

©2023 American Physical Society

Physics Subject Headings (PhySH)

Statistical Physics & Thermodynamics

Authors & Affiliations

J. Klinger1,2, R. Voituriez1,2, and O. Bénichou1

  • 1Laboratoire de Physique Théorique de la Matière Condensée, CNRS/Sorbonne Université, 4 Place Jussieu, 75005 Paris, France
  • 2Laboratoire Jean Perrin, CNRS/Sorbonne Université, 4 Place Jussieu, 75005 Paris, France

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Vol. 107, Iss. 5 — May 2023

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Images

  • Figure 1
    Figure 1

    Rightward and leftward FETPs. In this specific realization, after taking two steps inside the interval, the jump process escapes either through x or through 0 on its third step, with respective probabilities F0,x̲(3|x0) (red rightward dot) or F0̲,x(3|x0) (purple leftward dot).

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  • Figure 2
    Figure 2

    Rightward FETP for a jump process with p()e|l| (yielding μ=2). Upon rescaling according to Eq. (5), F0,x̲(n) converges to the scaling function h2(τ), defined by Eq. (6).

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  • Figure 3
    Figure 3

    Small τ behavior of the rightward FETP for various Levy flights with μ<2. The universal small τ behavior of F0,x̲(n) predicted by Eq. ((7a)) is displayed, with γμ=Γ(μ/2)sin(πμ/2)π32.

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  • Figure 4
    Figure 4

    Leftward FETP for n(x/aμ)μ. Defining τ̃=λ12μτ and rescaling F0̲,x(n|0) according to (11), all curves collapse onto a single exponential for various processes with 0<μ2. The Laplace jump process is defined by p()e||, corresponding to μ=2. C is given by Eq. (8), and here γμ=Γ(1+μ2)π.

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  • Figure 5
    Figure 5

    x0 dependence of exit-time probabilities. (a) Leftward FETP for a Laplace jump process. After rescaling, the rightward FETP collapses to the U(x0)=1π+V(x0) function, for various τ values. (b) Rescaled rightward FETP for an F-distributed jump process defined by p()[|l|(1+|l|)]1. The x0 dependence is in this case sublinear.

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