dc.creatorBuchini Labayen, Ana Carla
dc.creatorCentres, Paulo Marcelo
dc.creatorPasinetti, Pedro Marcelo
dc.creatorRamirez Pastor, Antonio Jose
dc.date.accessioned2020-10-28T14:06:45Z
dc.date.accessioned2022-10-15T10:30:24Z
dc.date.available2020-10-28T14:06:45Z
dc.date.available2022-10-15T10:30:24Z
dc.date.created2020-10-28T14:06:45Z
dc.date.issued2019-08
dc.identifierBuchini Labayen, Ana Carla; Centres, Paulo Marcelo; Pasinetti, Pedro Marcelo; Ramirez Pastor, Antonio Jose; Jamming and percolation of k3 -mers on simple cubic lattices; American Physical Society; Physical Review E: Statistical, Nonlinear and Soft Matter Physics; 100; 2; 8-2019; 1-9
dc.identifier1539-3755
dc.identifierhttp://hdl.handle.net/11336/117041
dc.identifier2470-0053
dc.identifierCONICET Digital
dc.identifierCONICET
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4375819
dc.description.abstractJamming and percolation of three-dimensional (3D) k×k×k cubic objects (k3-mers) deposited on simple cubic lattices have been studied by numerical simulations complemented with finite-size scaling theory. The k3-mers were irreversibly deposited into the lattice. Jamming coverage θj,k was determined for a wide range of k (2≤k≤40). θj,k exhibits a decreasing behavior with increasing k, being θj,k=∞=0.4204(9) the limit value for large k3-mer sizes. In addition, a finite-size scaling analysis of the jamming transition was carried out, and the corresponding spatial correlation length critical exponent νj was measured, being νj≈3/2. However, the obtained results for the percolation threshold θp,k showed that θp,k is an increasing function of k in the range 2≤k≤16. For k≥17, all jammed configurations are nonpercolating states, and consequently, the percolation phase transition disappears. The interplay between the percolation and the jamming effects is responsible for the existence of a maximum value of k (in this case, k=16) from which the percolation phase transition no longer occurs. Finally, a complete analysis of critical exponents and universality has been done, showing that the percolation phase transition involved in the system has the same universality class as the 3D random percolation, regardless of the size k considered.
dc.languageeng
dc.publisherAmerican Physical Society
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/pre/abstract/10.1103/PhysRevE.100.022136
dc.relationinfo:eu-repo/semantics/altIdentifier/doi/http://dx.doi.org/10.1103/PhysRevE.100.022136
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://arxiv.org/abs/1905.11440
dc.rightshttps://creativecommons.org/licenses/by/2.5/ar/
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectJamming and percolation
dc.subjectk 3 -mers
dc.subjectcubic lattices
dc.titleJamming and percolation of k3 -mers on simple cubic lattices
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:ar-repo/semantics/artículo
dc.typeinfo:eu-repo/semantics/publishedVersion


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