Abstract

Lévy flights are paradigmatic generalised random walk processes, in which the independent stationary increments—the ‘jump lengths’—are drawn from an -stable jump length distribution with long-tailed, power-law asymptote. As a result, the variance of Lévy flights diverges and the trajectory is characterised by occasional extremely long jumps. Such long jumps significantly decrease the probability to revisit previous points of visitation, rendering Lévy flights efficient search processes in one and two dimensions. To further quantify their precise property as random search strategies we here study the first-passage time properties of Lévy flights in one-dimensional semi-infinite and bounded domains for symmetric and asymmetric jump length distributions. To obtain the full probability density function of first-passage times for these cases we employ two complementary methods. One approach is based on the space-fractional diffusion equation for the probability density function, from which the survival probability is obtained for different values of the stable index and the skewness (asymmetry) parameter . The other approach is based on the stochastic Langevin equation with -stable driving noise. Both methods have their advantages and disadvantages for explicit calculations and numerical evaluation, and the complementary approach involving both methods will be profitable for concrete applications. We also make use of the Skorokhod theorem for processes with independent increments and demonstrate that the numerical results are in good agreement with the analytical expressions for the probability density function of the first-passage times.

Highlights

  • Normal Brownian motion described by Fick’s second law, the diffusion equation, is characterised by the linear time dependence x2(t) t of the mean squared displacement (MSD) [1]

  • In the following we study the first-passage properties of random walk processes with α-stable jump length distribution obtained from two numerical methods: the space-fractional diffusion equation and the Langevin approach

  • In the following we investigate the properties of the survival probability and the first-passage time density in a finite interval for symmetric and asymmetric α-stable laws underlying the space-fractional diffusion equation

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Summary

Introduction

Normal Brownian motion described by Fick’s second law, the diffusion equation, is characterised by the linear time dependence x2(t) t of the mean squared displacement (MSD) [1]. When the continuous time random walk has a finite characteristic waiting time but is equipped with a scale-free distribution of jump lengths with power-law asymptote λ(x) ∼ |x|−1−α (0 < α < 2) the resulting process is a ‘Lévy flight’ (LF). Our approach is based on the convenient formulation of LFs in terms of the space-fractional diffusion equation We derive these integro-differential equations for LFs based on general asymmetric α-stable distributions of relocation lengths in finite domains, and go beyond studies of the exit time and escape probability in bounded domain for symmetric LFs [129,130,131]. For all other choices of the parameters by substitution of relations (8a), (8b), and (11) into equation (4) we recover the characteristic function (1) of the α-stable process after Fourier transform

Diffusion description
Langevin dynamics
Comparison with α-stable distributions
Survival probability and first-passage properties
First-passage processes for symmetric α-stable laws
First-passage processes for asymmetric α-stable laws
Discussion and unsolved problems
First-passage time PDF for Brownian motion
First-passage time PDF for symmetric α-stable processes

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