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dc.creatorRojas, O.-
dc.creatorSouza, S. M. de-
dc.date.accessioned2020-11-13T23:02:15Z-
dc.date.available2020-11-13T23:02:15Z-
dc.date.issued2012-05-25-
dc.identifier.citationROJAS, O.; SOUZA, S. M. de. Equivalence between non-bilinear spin-S Ising model and Wajnflasz model. The European Physical Journal B, [S.l.], v. 85, May 2012. DOI: 10.1140/epjb/e2012-20998-0.pt_BR
dc.identifier.urihttps://link.springer.com/article/10.1140/epjb/e2012-20998-0pt_BR
dc.identifier.urihttp://repositorio.ufla.br/jspui/handle/1/45508-
dc.description.abstractWe propose the mapping of polynomial of degree 2S constructed as a linear combination of powers of spin-S (for simplicity, we called as spin-S polynomial) onto spin-crossover state. The spin-S polynomial in general can be projected onto non-symmetric degenerated spin up (high-spin) and spin down (low-spin) momenta. The total number of mapping for each general spin-S is given by 2(22S − 1). As an application of this mapping, we consider a general non-bilinear spin-S Ising model which can be transformed onto spin-crossover described by Wajnflasz model. Using a further transformation we obtain the partition function of the effective spin-1/2 Ising model, making a suitable mapping the non-symmetric contribution leads us to a spin-1/2 Ising model with a fixed external magnetic field, which in general cannot be solved exactly. However, for a particular case of non-bilinear spin-S Ising model could become equivalent to an exactly solvable Ising model. The transformed Ising model exhibits a residual entropy, then it should be understood also as a frustrated spin model, due to competing parameters coupling of the non-bilinear spin-S Ising model.pt_BR
dc.languageen_USpt_BR
dc.publisherElsevierpt_BR
dc.rightsrestrictAccesspt_BR
dc.sourceThe European Physical Journal B: Condensed Matter and Complex Systemspt_BR
dc.subjectStatistical physicspt_BR
dc.subjectNonlinear physicspt_BR
dc.titleEquivalence between non-bilinear spin-S Ising model and Wajnflasz modelpt_BR
dc.typeArtigopt_BR
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