2019
DOI: 10.1088/1367-2630/ab41bb
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First passage and first hitting times of Lévy flights and Lévy walks

Abstract: For both Lévy flight and Lévy walk search processes we analyse the full distribution of first-passage and first-hitting (or first-arrival) times. These are, respectively, the times when the particle moves across a point at some given distance from its initial position for the first time, or when it lands at a given point for the first time. For Lévy motions with their propensity for long relocation events and thus the possibility to jump across a given point in space without actually hitting it ('leapovers'), … Show more

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Cited by 74 publications
(54 citation statements)
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“…In our analysis, we derive upper and lower bounds on the hitting time of a Lévy walk on Z 2 . Bounds on the hitting time and related quantities for Lévy walks on the (one-dimensional) real line are given in [29]. Bounds for general random walks on Z , for ≥ 1, in the case where the walk has bounded second (or higher) moments can be found in [37].…”
Section: Related Workmentioning
confidence: 99%
“…In our analysis, we derive upper and lower bounds on the hitting time of a Lévy walk on Z 2 . Bounds on the hitting time and related quantities for Lévy walks on the (one-dimensional) real line are given in [29]. Bounds for general random walks on Z , for ≥ 1, in the case where the walk has bounded second (or higher) moments can be found in [37].…”
Section: Related Workmentioning
confidence: 99%
“…As can be seen, only for the case of Brownian motion (α = 2) the PDF has value zero at t = 0, while for LFs with α < 2 the first-passage time PDF exhibits a non-zero value at t = 0, thus demonstrating that LFs can instantly cross the boundary with their first jump away from their initial position x 0 . The magnitude of ℘(t → 0) can be estimated from the survival probability, as shown by equations ( 3) and (A.5) in [123] for symmetric LFs and here by equation ( 71) in section 5.2.5 below for asymmetric LFs with α ∈ (0, 2] and β ∈ (−1, 1] (excluding α = 1 with β = 0). Of course, in the case of symmetric LFs (β = 0) equation ( 71) coincides with equation (3) in [123].…”
Section: Symmetric Lfs In a Semi-infinite Domainmentioning
confidence: 99%
“…Our analysis follows closely the one reported in del-Castillo-Negrete (1998) for the transport of passive scalars in vortices in the presence of a shear flow. Also, the study of exit time statistics of EP is closely related to the fundamental first-passage problem in non-equilibrium statistical mechanics, which is an open research problem in systems with nontrivial dynamics (see for example Benkadda et al (1997), Dybiec et al (2017), Palyulin et al (2019) and references therein). We follow during ∼10 7 cyclotron periods an ensemble of ∼10 5 energetic particles initialised with E ≈ 20E th in the chaotic region.…”
Section: Anomalous Exit Time and Asymmetric Diffusionmentioning
confidence: 99%