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在具有球对称性的有界域中,扩散粒子在随机重置下的首次通过。

First passage of a diffusing particle under stochastic resetting in bounded domains with spherical symmetry.

作者信息

Chen Hanshuang, Huang Feng

机构信息

School of Physics and Optoelectronics Engineering, Anhui University, Hefei 230601, China.

Key Laboratory of Advanced Electronic Materials and Devices & School of Mathematics and Physics, Anhui Jianzhu University, Hefei 230601, China.

出版信息

Phys Rev E. 2022 Mar;105(3-1):034109. doi: 10.1103/PhysRevE.105.034109.

Abstract

We investigate the first passage properties of a Brownian particle diffusing freely inside a d-dimensional sphere with absorbing spherical surface subject to stochastic resetting. We derive the mean time to absorption (MTA) as functions of resetting rate γ and initial distance r of the particle to the center of the sphere. We find that when r>r_{c} there exists a nonzero optimal resetting rate γ_{opt} at which the MTA is a minimum, where r_{c}=sqrt[d/(d+4)]R and R is the radius of the sphere. As r increases, γ_{opt} exhibits a continuous transition from zero to nonzero at r=r_{c}. Furthermore, we consider that the particle lies between two two-dimensional or three-dimensional concentric spheres with absorbing boundaries, and obtain the domain in which resetting expedites the MTA, which is (R_{1},r_{c_{1}})∪(r_{c_{2}},R_{2}), with R_{1} and R_{2} being the radii of inner and outer spheres, respectively. Interestingly, when R_{1}/R_{2} is less than a critical value, γ_{opt} exhibits a discontinuous transition at r=r_{c_{1}}; otherwise, such a transition is continuous. However, at r=r_{c_{2}} the transition is always continuous.

摘要

我们研究了一个在(d)维球体内部自由扩散且其球面为吸收边界并受随机重置影响的布朗粒子的首次通过性质。我们推导出了吸收平均时间(MTA)作为重置率(\gamma)以及粒子到球心初始距离(r)的函数。我们发现,当(r > r_{c})时,存在一个非零的最优重置率(\gamma_{opt}),此时MTA最小,其中(r_{c}=\sqrt{d/(d + 4)}R),(R)为球体半径。随着(r)增大,(\gamma_{opt})在(r = r_{c})处呈现从零到非零的连续转变。此外,我们考虑粒子位于两个具有吸收边界的二维或三维同心球体之间,并得到了重置会加快MTA的区域,即((R_{1},r_{c_{1}})∪(r_{c_{2}},R_{2})),其中(R_{1})和(R_{2})分别为内球和外球的半径。有趣的是,当(R_{1}/R_{2})小于一个临界值时,(\gamma_{opt})在(r = r_{c_{1}})处呈现不连续转变;否则,这种转变是连续的。然而,在(r = r_{c_{2}})处的转变总是连续的。

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