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De Gruyter eBooks

Critical Temperature of a Quasi-One-Dimensional Ising Model. The Bethe- Peierls Approximation

M. A. Yurishchev

Published Dec 31, 1985• 0 citations
Publisher
DOI
10.1515/9783112494561-019

Related papers

On the critical temperature of the quasi-one-dimensional Ising model

M. A. Yurishchev

Soviet Journal of Low Temperature Physics•Sep 1, 1988•0 citations

Critical Temperature of a Quasi‐One‐Dimensional Ising Model. The Bethe‐Peierls Approximation

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Abstract The critical temperature of a three‐dimensional spatially anisotropic Ising model is computed by the Bethe‐Peierls method applied to the five‐chain cluster. A comparison is made between the results obtained and calculations based on other approaches.

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Critical temperature of the one-dimensional Ising model with inverse-square interactions

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Extended chain approximation in quasi‐one‐dimensional ising model

Y. Muraoka, Toshihiro Idogaki

Abstract The extended chain approximation (ECA) in the quasi‐one‐dimensional Ising model is proposed and is found to give the same results as the Bethe‐Peierls approximation for the ferromagnetic Ising model. It is discussed that the ECA can be applied to complicated systems such as the axial next‐nearest‐neighbour Ising (ANNNI) model, etc.

physica status solidi (b)•Jun 1, 1996•4 citations

Bethe-Peierls approximation for the 2D random Ising model

Copenhagen O Dk

The partition function of the 2D Ising model with random nearest-neighbour coupling is expressed in the dual lattice made of square plaquettes. The dual model is solved in the mean field and in different types of Bethe-Peierls approximations, using the replica method. The application of methods of mean-field type to Ising models allows one to obtain very accurate approximations of the thermodynamic quantities. However, in the presence of quenched disorder this approach is difficult to implement. In this paper, we show that rather good results can be obtained after performing a duality transformation of the Ising model with random nearest-neighbour coupling that assumes the values Jij D1 with equal probability. The model is thus defined on a dual lattice where the spin variables are attached to the square plaquettes. The advantage is that the quadratic term of the dual Hamiltonian has constant coefficients instead of random ones. It is therefore possible to use the standard methods of the mean field to estimate the quenched free energy. Our results can be generalized to higher dimensions, although the approximations become rougher, because the number of plaquette spins over the number of interaction links increases with the dimensionality (1). In particular, we obtain an extremely good estimate of the ground- state energy of the random Ising model, by applying the Bethe-Peierls approximation where part of the short-range order is taken into account. In section 1, we introduce the dual lattice made of elementary square plaquettes. On this lattice the partition function can be expressed as a function of the inverse temperature e D 1 ln tanh.1=T/ whereT D 1 is the temperature of the original lattice. In section 2, we apply the mean-field approximation to the dual model, using the replica method. In section 3, we introduce the Bethe-Peierls approximation. This allows us to obtain a very precise estimate of the ground-state energy of the two-dimensional Ising model with random coupling. In section 4, we show that it is possible to improve the Bethe-Peierls approximation by introducing an interaction between different replicas. In section 5, the reader will find some remarks and conclusions.

•Jan 1, 1996•0 citations

Critical temperature in the two-layered Ising model

Adam Lipowski

Physica A Statistical Mechanics and its Applications•Feb 1, 1998•36 citations
The partition function of the 2D Ising model with random nearest-neighbour coupling is expressed in the dual lattice made of square plaquettes. The dual model is solved in the mean field and in different types of Bethe-Peierls approximations, using the replica method. The application of methods of mean-field type to Ising models allows one to obtain very accurate approximations of the thermodynamic quantities. However, in the presence of quenched disorder this approach is difficult to implement. In this paper, we show that rather good results can be obtained after performing a duality transformation of the Ising model with random nearest-neighbour coupling that assumes the values Jij D1 with equal probability. The model is thus defined on a dual lattice where the spin variables are attached to the square plaquettes. The advantage is that the quadratic term of the dual Hamiltonian has constant coefficients instead of random ones. It is therefore possible to use the standard methods of the mean field to estimate the quenched free energy. Our results can be generalized to higher dimensions, although the approximations become rougher, because the number of plaquette spins over the number of interaction links increases with the dimensionality (1). In particular, we obtain an extremely good estimate of the ground- state energy of the random Ising model, by applying the Bethe-Peierls approximation where part of the short-range order is taken into account. In section 1, we introduce the dual lattice made of elementary square plaquettes. On this lattice the partition function can be expressed as a function of the inverse temperature e D 1 ln tanh.1=T/ whereT D 1 is the temperature of the original lattice. In section 2, we apply the mean-field approximation to the dual model, using the replica method. In section 3, we introduce the Bethe-Peierls approximation. This allows us to obtain a very precise estimate of the ground-state energy of the two-dimensional Ising model with random coupling. In section 4, we show that it is possible to improve the Bethe-Peierls approximation by introducing an interaction between different replicas. In section 5, the reader will find some remarks and conclusions.