dc.creatorLongone, Pablo Jesus
dc.creatorCentres, Paulo Marcelo
dc.creatorRamirez Pastor, Antonio Jose
dc.date.accessioned2020-05-06T21:02:34Z
dc.date.accessioned2022-10-15T03:33:43Z
dc.date.available2020-05-06T21:02:34Z
dc.date.available2022-10-15T03:33:43Z
dc.date.created2020-05-06T21:02:34Z
dc.date.issued2012-01-04
dc.identifierLongone, Pablo Jesus; Centres, Paulo Marcelo; Ramirez Pastor, Antonio Jose; Percolation of aligned rigid rods on two-dimensional square lattices; American Physical Society; Physical Review E: Statistical, Nonlinear and Soft Matter Physics; 85; 11108; 4-1-2012; 1-7
dc.identifier1539-3755
dc.identifierhttp://hdl.handle.net/11336/104442
dc.identifier1550-2376
dc.identifierCONICET Digital
dc.identifierCONICET
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4340533
dc.description.abstractThe percolation behavior of aligned rigid rods of length k (kmers) on two-dimensional square lattices has been studied by numerical simulations and finite-size scaling analysis. The kmers, containing k identical units (each one occupying a lattice site), were irreversibly deposited along one of the directions of the lattice. The process was monitored by following the probability RL,k(p) that a lattice composed of L×L sites percolates at a concentration p of sites occupied by particles of size k. The results, obtained for k ranging from 1 to 14, show that (i) the percolation threshold exhibits a decreasing function when it is plotted as a function of the kmer size; (ii) for any value of k (k>1), the percolation threshold is higher for aligned rods than for rods isotropically deposited; (iii) the phase transition occurring in the system belongs to the standard random percolation universality class regardless of the value of k considered; and (iv) in the case of aligned kmers, the intersection points of the curves of RL,k(p) for different system sizes exhibit nonuniversal critical behavior, varying continuously with changes in the kmer size. This behavior is completely different to that observed for the isotropic case, where the crossing point of the curves of RL,k(p) do not modify their numerical value as k is increased.
dc.languageeng
dc.publisherAmerican Physical Society
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/pre/abstract/10.1103/PhysRevE.85.011108
dc.relationinfo:eu-repo/semantics/altIdentifier/doi/http://dx.doi.org/10.1103/PhysRevE.85.011108
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://arxiv.org/abs/1906.03966
dc.rightshttps://creativecommons.org/licenses/by/2.5/ar/
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectPERCOLATION
dc.subjectALIGNED RIGID RODS OF LENGTH K
dc.subjectPERCOLATION THRESHOLD
dc.subjectUNIVERSALITY CLASS
dc.titlePercolation of aligned rigid rods on two-dimensional square lattices
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:ar-repo/semantics/artículo
dc.typeinfo:eu-repo/semantics/publishedVersion


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