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dc.creatorRojas, M.-
dc.creatorRojas, Onofre-
dc.creatorSouza, S. M. de-
dc.date.accessioned2020-11-13T12:55:07Z-
dc.date.available2020-11-13T12:55:07Z-
dc.date.issued2012-11-16-
dc.identifier.citationROJAS, M.; ROJAS, O.; SOUZA, S. M. de. Frustrated Ising model on the Cairo pentagonal lattice. Physical Review E, [S.l.], v. 86, n. 5, Nov. 2012. DOI: 10.1103/PhysRevE.86.051116.pt_BR
dc.identifier.urihttps://journals.aps.org/pre/abstract/10.1103/PhysRevE.86.051116pt_BR
dc.identifier.urihttp://repositorio.ufla.br/jspui/handle/1/45464-
dc.description.abstractThrough the direct decoration transformation approach, we obtain a general solution for the pentagonal Ising model, showing its equivalence to the isotropic free-fermion eight-vertex model. We study the ground-state phase diagram, in which one ferromagnetic (FM) state, one ferrimagnetic (FIM) state, and one frustrated state are found. Using the exact solution of the pentagonal Ising model, we discuss the finite-temperature phase diagrams and find a phase transition between the FIM state and the disordered state as well as a phase transition between the disordered state and the FM state. We also discuss some additional remarkable properties of the model, such as the magnetization, entropy, and specific heat, at finite temperature and at its low-temperature asymptotic limit. Because of the influence of the second-order phase transition between the frustrated and ferromagnetic phases, we obtain surprisingly low values of the entropy and the specific heat until the critical temperature is reached.pt_BR
dc.languageen_USpt_BR
dc.publisherAmerican Physical Society (APS)pt_BR
dc.rightsrestrictAccesspt_BR
dc.sourcePhysical Review E (PRE): covering statistical, nonlinear, biological, and soft matter physicspt_BR
dc.subjectPentagonal Ising modelpt_BR
dc.subjectEntropypt_BR
dc.subjectFerromagnetic (FM)pt_BR
dc.subjectFerrimagnetic (FIM)pt_BR
dc.subjectCairo pentagonal modelpt_BR
dc.titleFrustrated Ising model on the Cairo pentagonal latticept_BR
dc.typeArtigopt_BR
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