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Nearest-neighbor distances in diffusion-controlled reactions modelled by a single mobile trap

dc.contributor.authorSchoonover, Rodneyen_US
dc.contributor.authorBen-Avraham, Danielen_US
dc.contributor.authorHavlin, Shlomoen_US
dc.contributor.authorKopelman, Raoulen_US
dc.contributor.authorWeiss, George H.en_US
dc.date.accessioned2006-04-10T14:48:18Z
dc.date.available2006-04-10T14:48:18Z
dc.date.issued1991-02-15en_US
dc.identifier.citationSchoonover, Rodney, Ben-Avraham, Daniel, Havlin, Shlomo, Kopelman, Raoul, Weiss, George H. (1991/02/15)."Nearest-neighbor distances in diffusion-controlled reactions modelled by a single mobile trap." Physica A: Statistical and Theoretical Physics 171(2): 232-238. <http://hdl.handle.net/2027.42/29454>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TVG-46TY53C-8H/2/5b04b82df229ffb5d1ba0df0d734cd81en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/29454
dc.description.abstractWe consider a system consisting of an infinite number of identical particles on a lattice initially uniformly distributed, which diffuese in the presence of a singke mobile trap and ask for the time-dependent behavior of the distance of the trap from the nearest particle. This quantity is a measure of the tendency of the system to self-segregate. We show, by a simulation incorporating the exact enumeration method, that in one dimension the expected distance L(t)&gt; scales as L(t)&gt;[approximate]t[alpha] as t--&gt;[infinity], where the exponent [alpha] depends only on the ratio of the diffusion constant. A heuristic expression for [alpha] is suggested, analogous to a rigorous exponent found by ben-Avraham for a similar but not identical problem. The flux into the trap is found to vary as t-1/2 independent of the diffusion constants.en_US
dc.format.extent395722 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleNearest-neighbor distances in diffusion-controlled reactions modelled by a single mobile trapen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelMathematicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationotherDepartment of Physics, Clarkson University, Postdam, NY 13676, USAen_US
dc.contributor.affiliationotherNational Institutes of Health, Bethesda, MD 20892, USA;en_US
dc.contributor.affiliationotherNational Institutes of Health, Bethesda, MD 20892, USAen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/29454/1/0000536.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0378-4371(91)90275-Hen_US
dc.identifier.sourcePhysica A: Statistical and Theoretical Physicsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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