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Journal of Statistical Physics

Effect of the block-spin configuration on the location of βc in two-dimensional Ising modelsin two-dimensional Ising models

Mohamed Ould-Lemrabott

Published Mar 1, 1997• 3 citations
Publisher
DOI
10.1007/bf02183616

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Low temperature series expansions for the spin S = 1 Ising model on various two and three dimensional lattices have been generated. By extrapolation of these series, it is found that the critical exponents β, γ' and δ appear to be the same as for the spin S = 1/2 Ising model. For the spin S = 1/2 Ising model, we have found that the class of configurations represented by Cayley trees make a significant contribution to the low temperature series coefficients. In particular, we find that the distribution of singularities within the disk | u | ≤ |uc |(uc = exp[- 4 J/kTc], Tc is the critical temperature) is well represented by including only the Cayley trees in the partition function.

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Spin Correlations and Magnetic Susceptivility of the Two-Dimensional Ising Model

Yoshiaki Tanaka

Journal of the Physical Society of Japan•May 15, 1995•0 citations
A family of nonequilibrium kinetic Ising models, introduced earlier, evolving under the competing effect of spin flips at zero temperature and nearest-neighbour random spin exchanges, is further investigated. By increasing the range of spin exchanges and/or their strength the nature of the phase transition 'Ising-to-active' becomes of (dynamic) mean-field type and a first-order tricritical point is located at the Glauber ( delta =0) limit. Corrections to the mean-field theory are evaluated up to sixth order in a cluster approximation and found to give good results concerning the phase boundary and the critical exponent beta of the order parameter which is obtained as beta approximately=1.0.
The critical behavior of the two-dimensional Ising model (square lattice, exchange constant J) in an uniform field, and in an annealed random field is considered. The random field is generated by decorating the horizontal and vertical bonds of the lattice, and it satisfies an arbitrary distribution which is imposed by introducing a pseudo-chemical potential. By decimating the decorating variables the model can be mapped onto a homogeneous Ising model with effective exchange constant J′ and effective external field h′, dependent on the temperature. These parameters, which satisfy a set of coupled equations, depend on the spin average and nearest-neighbor two-spin correlation, and are obtained numerically. For the symmetric field distribution [Formula: see text] the mapping of the critical frontier on the (K′=βJ′,H′=βh′) plane onto the (K=β J,H=βh) plane is determined and, as in the model introduced by Essam and Place, there is a region on the (K, H) plane which cannot be reached from any real values of (K′, H′). The critical exponents are determined numerically, and it is shown that they do not satisfy renormalization relations obtained for their model.
Low temperature series expansions for the spin S = 1 Ising model on various two and three dimensional lattices have been generated. By extrapolation of these series, it is found that the critical exponents β, γ' and δ appear to be the same as for the spin S = 1/2 Ising model. For the spin S = 1/2 Ising model, we have found that the class of configurations represented by Cayley trees make a significant contribution to the low temperature series coefficients. In particular, we find that the distribution of singularities within the disk | u | ≤ |uc |(uc = exp[- 4 J/kTc], Tc is the critical temperature) is well represented by including only the Cayley trees in the partition function.