Multicritical points and crossover mediating the strong violation of universality: Wang-Landau determinations in the random-bond d=2 Blume-Capel model

The effects of bond randomness on the phase diagram and critical behavior of the square lattice ferromagnetic Blume-Capel model are discussed. The system is studied in both the pure and disordered versions by the same efficient two-stage Wang-Landau method for many values of the crystal field, restr...

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Main Authors: Malakis, A. (Author), Berker, A. Nihat (Contributor), Hadjiagapiou, I. A. (Author), Fytas, N. G. (Author), Papakonstantinou, T. (Author)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2010-10-04T13:49:13Z.
Subjects:
Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Malakis, A.  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Berker, A. Nihat  |e contributor 
100 1 0 |a Berker, A. Nihat  |e contributor 
700 1 0 |a Berker, A. Nihat  |e author 
700 1 0 |a Hadjiagapiou, I. A.  |e author 
700 1 0 |a Fytas, N. G.  |e author 
700 1 0 |a Papakonstantinou, T.  |e author 
245 0 0 |a Multicritical points and crossover mediating the strong violation of universality: Wang-Landau determinations in the random-bond d=2 Blume-Capel model 
260 |b American Physical Society,   |c 2010-10-04T13:49:13Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/58843 
520 |a The effects of bond randomness on the phase diagram and critical behavior of the square lattice ferromagnetic Blume-Capel model are discussed. The system is studied in both the pure and disordered versions by the same efficient two-stage Wang-Landau method for many values of the crystal field, restricted here in the second-order phase-transition regime of the pure model. For the random-bond version several disorder strengths are considered. We present phase diagram points of both pure and random versions and for a particular disorder strength we locate the emergence of the enhancement of ferromagnetic order observed in an earlier study in the ex-first-order regime. The critical properties of the pure model are contrasted and compared to those of the random model. Accepting, for the weak random version, the assumption of the double-logarithmic scenario for the specific heat we attempt to estimate the range of universality between the pure and random-bond models. The behavior of the strong disorder regime is also discussed and a rather complex and yet not fully understood behavior is observed. It is pointed out that this complexity is related to the ground-state structure of the random-bond version. 
520 |a University of Athens (grant no. 70/4/4071) 
546 |a en_US 
655 7 |a Article 
773 |t Physical Review E