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Physica A Statistical Mechanics and its Applications

Fluctuations of the specific heat in one-dimensional dilute Ising models

Toshijiro Tanaka, Hirokazu Fujisaka, Masayoshi Inoue

Published May 1, 1994• 0 citations
Publisher
DOI
10.1016/0378-4371(94)90116-3

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In chapter one, we explain briefly the continuum limit, scaling, and high temperature expansion of critical phenomena, Monte Carlo algorithms and fitting. In chapter two, different continuum limits of the Ising model in dimensions (D) 2, 3 and 4 are investigated numerically. The data indicate that triviality occurs for D = 4 and fails for D < 4 in each limit. In chapter three, a relation between the critical exponents of the leading and confluent scaling terms is derived using the finite size scaling argument. We also determine the new scaling variable of the 4D Ising model based on a new Monte Carlo simulation data. In chapter four, a Monte Carlo study of two dimensional diluted Ising systems is reported. It is shown that regular dilution does not affect critical exponents, while a random one does, with critical exponents varying continuously with impurity concentration. The importance of fluctuations in producing such effects is emphasized. In chapter five, a different point of view regarding the critical exponent of the specific heat of the 3D Ising model is presented. Based on the analysis of high temperature expansion, finite size scaling and Monte Carlo data in the symmetric phase of the 3D Ising model, it is shown that logarithmic scaling behavior of specific heat is more consistent than power scaling behavior.

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Critical behaviour of the three-dimensional Ising model specific heat below Tc

Hemda Garelick, J W Essam

The magnetization exponent β D of the Syozi model of dilute ferro-magnetism is estimated for the four most common three-dimensional lattices using the Padé approximant method. It is found in all cases that 0·354 <or= β D <or= 0·380. Using the previously established relation αprime = 1 - β/β D between the specific heat exponent αprime and the magnetization exponent β for the Ising model below T c and assuming β = fraction five-sixteens, the above result implies 0·117 <or= αprime <or= 0·178. On the grounds that previous estimates of αprime have been much lower, it is concluded that most probably αprime = fraction one-eighth = 0·125 with the consequence β D = fraction five-fourteens = 0·357.... The possibility αprime = fraction one-sixteens is well excluded by this method. The specific heat amplitude of the Ising model below T c is deduced by computation of the magnetization amplitude of the Syozi model.

Journal of Physics C Solid State Physics•Dec 1, 1968•11 citations
In chapter one, we explain briefly the continuum limit, scaling, and high temperature expansion of critical phenomena, Monte Carlo algorithms and fitting. In chapter two, different continuum limits of the Ising model in dimensions (D) 2, 3 and 4 are investigated numerically. The data indicate that triviality occurs for D = 4 and fails for D < 4 in each limit. In chapter three, a relation between the critical exponents of the leading and confluent scaling terms is derived using the finite size scaling argument. We also determine the new scaling variable of the 4D Ising model based on a new Monte Carlo simulation data. In chapter four, a Monte Carlo study of two dimensional diluted Ising systems is reported. It is shown that regular dilution does not affect critical exponents, while a random one does, with critical exponents varying continuously with impurity concentration. The importance of fluctuations in producing such effects is emphasized. In chapter five, a different point of view regarding the critical exponent of the specific heat of the 3D Ising model is presented. Based on the analysis of high temperature expansion, finite size scaling and Monte Carlo data in the symmetric phase of the 3D Ising model, it is shown that logarithmic scaling behavior of specific heat is more consistent than power scaling behavior.
The magnetization exponent β D of the Syozi model of dilute ferro-magnetism is estimated for the four most common three-dimensional lattices using the Padé approximant method. It is found in all cases that 0·354 <or= β D <or= 0·380. Using the previously established relation αprime = 1 - β/β D between the specific heat exponent αprime and the magnetization exponent β for the Ising model below T c and assuming β = fraction five-sixteens, the above result implies 0·117 <or= αprime <or= 0·178. On the grounds that previous estimates of αprime have been much lower, it is concluded that most probably αprime = fraction one-eighth = 0·125 with the consequence β D = fraction five-fourteens = 0·357.... The possibility αprime = fraction one-sixteens is well excluded by this method. The specific heat amplitude of the Ising model below T c is deduced by computation of the magnetization amplitude of the Syozi model.