scholarly journals Steady state, relaxation and first-passage properties of a run-and-tumble particle in one-dimension

2018 ◽  
Vol 2018 (4) ◽  
pp. 043215 ◽  
Author(s):  
Kanaya Malakar ◽  
V Jemseena ◽  
Anupam Kundu ◽  
K Vijay Kumar ◽  
Sanjib Sabhapandit ◽  
...  
2019 ◽  
Vol 99 (3) ◽  
Author(s):  
Abhishek Dhar ◽  
Anupam Kundu ◽  
Satya N. Majumdar ◽  
Sanjib Sabhapandit ◽  
Grégory Schehr

Author(s):  
Tian Zhou ◽  
Pengbo Xu ◽  
Weihua Deng

Abstract Almost all the media the particles move in are non-static, one of which is the most common expanding or contracting (by a scale factor) non-static medium discussed in this paper. Depending on the expected resolution of the studied dynamics and the amplitude of the displacement caused by the non-static media, sometimes the non-static behaviors of the media can not be ignored. In this paper, we build the model describing L\'evy walks in one-dimension uniformly non-static media, where the physical and comoving coordinates are connected by scale factor. We derive the equation governing the probability density function of the position of the particles in comoving coordinate. Using the Hermite orthogonal polynomial expansions, some statistical properties are obtained, such as mean squared displacements (MSDs) in both coordinates and kurtosis. For some representative non-static media and L\'{e}vy walks, the asymptotic behaviors of MSDs in both coordinates are analyzed in detail. The stationary distributions and mean first passage time for some cases are also discussed through numerical simulations.


2020 ◽  
Vol 101 (5) ◽  
Author(s):  
Tirthankar Banerjee ◽  
Satya N. Majumdar ◽  
Alberto Rosso ◽  
Grégory Schehr

1985 ◽  
Vol 22 (3) ◽  
pp. 611-618 ◽  
Author(s):  
A. G. Nobile ◽  
L. M. Ricciardi ◽  
L. Sacerdote

The asymptotic behavior of the first-passage-time p.d.f. through a constant boundary is studied when the boundary approaches the endpoints of the diffusion interval. We show that for a class of diffusion processes possessing a steady-state distribution this p.d.f. is approximately exponential, the mean being the average first-passage time to the boundary. The proof is based on suitable recursive expressions for the moments of the first-passage time.


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