Universality aspects of the d = 3 random-bond Blume-Capel model

The effects of bond randomness on the universality aspects of the simple cubic lattice ferromagnetic Blume-Capel model are discussed. The system is studied numerically in both its first- and second-order phase transition regimes by a comprehensive finite-size scaling analysis. We find that our data...

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Bibliographic Details
Main Authors: Malakis, A. (Author), Berker, A. Nihat (Contributor), 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, 2012-08-27T19:53:08Z.
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Online Access:Get fulltext
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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 Fytas, N. G.  |e author 
700 1 0 |a Papakonstantinou, T.  |e author 
245 0 0 |a Universality aspects of the d = 3 random-bond Blume-Capel model 
260 |b American Physical Society,   |c 2012-08-27T19:53:08Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/72355 
520 |a The effects of bond randomness on the universality aspects of the simple cubic lattice ferromagnetic Blume-Capel model are discussed. The system is studied numerically in both its first- and second-order phase transition regimes by a comprehensive finite-size scaling analysis. We find that our data for the second-order phase transition, emerging under random bonds from the second-order regime of the pure model, are compatible with the universality class of the 3d random Ising model. Furthermore, we find evidence that the second-order transition emerging under bond randomness from the first-order regime of the pure model belongs to a new and distinctive universality class. The first finding reinforces the scenario of a single universality class for the 3d Ising model with the three well-known types of quenched uncorrelated disorder (bond randomness, site and bond dilution). The second amounts to a strong violation of the universality principle of critical phenomena. For this case of the ex-first-order 3d Blume-Capel model, we find sharp differences from the critical behaviors, emerging under randomness, in the cases of the ex-first-order transitions of the corresponding weak and strong first-order transitions in the 3d three-state and four-state Potts models. 
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655 7 |a Article 
773 |t Physical Review E