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Brazilian Journal of Physics

Local persistence and blocking in the two-dimensional blume-capel model

Roberto da Silva, Sílvio R. Dahmen

Published Dec 1, 2004• 7 citations
Publisher

Abstract

In this paper we study the local persistence of the two-dimensional Blume-Capel Model by extending the concept of Glauber dynamics. We verify that for any value of the ratio alpha = D/J between anisotropy D and exchange J the persistence shows a power law behavior. In particular for alpha < 0 we find a persistence exponent thetal = 0:2096(13), i.e. in the Ising universality class. For alpha > 0 ( a ¹ 1) we observe the occurrence of blocking.

DOI
10.1590/s0103-97332004000700027

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Local persistense and blocking in the two dimensional Blume-Capel Model

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arXiv:1501.05178•Jan 21, 2015•0 citations
In this paper we study the local persistence of the two-dimensional Blume-Capel Model by extending the concept of Glauber dynamics. We verify that for any value of the ratio alpha = D/J between anisotropy D and exchange J the persistence shows a power law behavior. In particular for alpha < 0 we find a persistence exponent thetal = 0:2096(13), i.e. in the Ising universality class. For alpha > 0 ( a ¹ 1) we observe the occurrence of blocking.
In this letter we study the local persistence of the two--dimensional Blume-- Capel Model by extension of the concept of Glauber dynamics. We verify that for any value of the ratio α=D/Jα=D/Jα=D/J between anisotropy DDD and exchange JJJ the persistence shows a power law behavior. In particular for α<0α<0α<0 we find a persistence exponent θl=0.2096(13)θ_{l}=0.2096(13)θl​=0.2096(13), \textit{i.e.} in the Ising universality class. For α>0α>0α>0 (α≠1α\neq 1α=1) we observe the occurrence of blocking.
We employed Monte Carlo simulations and short-time dynamic scaling to determine the static and dynamic critical exponents for the generalized two-dimensional Blume-Capel model of spin-3/2. We showed that the critical behavior at the second-order phase-transition line between the paramagnetic and ferromagnetic phases is in the same universality class of the two-dimensional Ising model. However, at the double critical end point, which is present in the phase diagram of the model, the critical exponent beta , associated to the order parameter, is different from that of the Ising model.
We study purely dissipative relaxational dynamics in the three-dimensional Ising universality class. To this end, we simulate the improved Blume-Capel model on the simple cubic lattice by using local algorithms. We perform a finite size scaling analysis of the integrated autocorrelation time of the magnetic susceptibility in equilibrium at the critical point. We obtain z=2.0245(15) for the dynamic critical exponent. As a complement, fully magnetized configurations are suddenly quenched to the critical temperature, giving consistent results for the dynamic critical exponent. Furthermore, our estimate of z is fully consistent with recent field theoretic results.
We study the dynamics of ordering in ferromagnets via Monte Carlo simulations of the Ising model, employing the Glauber spin-flip mechanism, in space dimensions d=2d=2d=2 and 333. Results for the persistence probability and the domain growth are discussed for quenches to various temperatures (TfT_fTf​) below the critical one (TcT_{c}Tc​), from different initial temperatures Ti≥TcT_{i} \geq T_{c}Ti​≥Tc​. In long time limit, for Ti>TcT_{i} > T_{c}Ti​>Tc​, the persistence probability exhibits power-law decay with exponents θ≃0.22θ\simeq 0.22θ≃0.22 and ≃0.18\simeq 0.18≃0.18 in d=2d=2d=2 and 333, respectively. For finite TiT_iTi​, the early time behavior is a different power-law whose life-time diverges and exponent decreases as Ti→TcT_{i} \rightarrow T_{c}Ti​→Tc​. The crossover length between the two steps diverges as the equilibrium correlation length. Ti=TcT_i=T_cTi​=Tc​ is expected to provide a {\it{new universality class}} for which we obtain θ≃0.035θ\simeq 0.035θ≃0.035 in d=2d=2d=2 and ≃0.10\simeq 0.10≃0.10 in d=3d=3d=3. The time dependence of the average domain size ℓ\ellℓ, however, is observed to be rather insensitive to the choice of TiT_iTi​.