{ "id": "2109.11101", "version": "v1", "published": "2021-09-23T01:51:28.000Z", "updated": "2021-09-23T01:51:28.000Z", "title": "First passage of a diffusing particle under stochastic resetting in bounded domains with spherical symmetry", "authors": [ "Hanshuang Chen", "Feng Huang" ], "comment": "6 pages, 7 figures", "categories": [ "cond-mat.stat-mech" ], "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 $\\gamma$ 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 $\\gamma_{{\\rm opt}}$ at which the MTA is a minimum, where $r_c=\\sqrt {d/\\left( {d + 4} \\right)} R$ and $R$ is the radius of sphere. As $r$ increases, $\\gamma_{{\\rm opt}}$ exhibits a continuous transition from zero to nonzero at $r=r_c$. Furthermore, we consider that the particle lies in between two two-dimensional or three-dimensional concentric spheres, and obtain the domain in which resetting expedites the MTA, which is $(R_1, r_{c_1}) \\cup (r_{c_2},R_2)$, with $R_1$ and $R_2$ being the radius of inner and outer spheres, respectively. Interestingly, when $R_1/R_2$ is less than a critical value, $\\gamma_{{\\rm opt}}$ exhibits a discontinuous transition at $r=r_{c_1}$; otherwise, such a transition is continuous. Whereas at $r=r_{c_2}$, $\\gamma_{{\\rm opt}}$ always shows a continuous transition.", "revisions": [ { "version": "v1", "updated": "2021-09-23T01:51:28.000Z" } ], "analyses": { "keywords": [ "stochastic resetting", "diffusing particle", "bounded domains", "spherical symmetry", "particle diffusing freely inside" ], "note": { "typesetting": "TeX", "pages": 6, "language": "en", "license": "arXiv", "status": "editable" } } }