1997
DOI: 10.5488/cmp.11.17
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CALCULATION METHOD FOR THE THREE-DIMENSIONAL ISING FERROMAGNET THERMODYNAMICS WITHIN THE FRAMES OF rho^{6} MODEL

Abstract: Calculation of thermodynamic functions of the three-dimensional Ising ferromagnet above and below critical temperature is performed in the approximation of sixfold basis distribution (ρ 6 model). Comparison with the results for the ρ 4 model indicates that dependence of the thermodynamic functions on the renormalization group parameter s becomes weaker. The optimal interval of the renormalization group parameter values is determined.

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Cited by 15 publications
(39 citation statements)
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“…The present paper supplements the earlier works [8][9][10][11], in which the ρ 6 model was used for calculating the free energy and other thermodynamic functions of the system in the absence of an external field. The ρ 6 model provides a better quantitative description of the critical behaviour of a 3D Ising-like magnet than the ρ 4 model [10].…”
Section: Introductionsupporting
confidence: 63%
See 1 more Smart Citation
“…The present paper supplements the earlier works [8][9][10][11], in which the ρ 6 model was used for calculating the free energy and other thermodynamic functions of the system in the absence of an external field. The ρ 6 model provides a better quantitative description of the critical behaviour of a 3D Ising-like magnet than the ρ 4 model [10].…”
Section: Introductionsupporting
confidence: 63%
“…The expressions for the remaining coefficients are given in [8][9][10][11]. These coefficients are functions of s 0 , that is, of the ratio of microscopic parameters b and c. We shall use the method of "layerby-layer" integration of (6) with respect to variables ρ k described in [2][3][4].…”
Section: General Relationsmentioning
confidence: 99%
“…The methods existing at present make it possible to calculate critical characteristics to a quite high degree of accuracy (see, for example [17,18]). The advantage of the method under investigation lies in the possibility to obtain and analyze expressions for thermodynamic characteristics and their amplitudes as functions of microscopic parameters of the system [2][3][4][5]19]. It is shown (see, for example, [2,4,20,21]) that the leading critical amplitudes and the correction-to-scaling amplitudes for the specific heat, average spin moment, susceptibility of the system can be presented in the form of the product of the universal part, independent of microscopic parameters, and the nonuniversal factor, which depends on these parameters.…”
mentioning
confidence: 99%
“…The confinement to the 6th power of the CV in the expression for a measure density corresponds to the ρ 6 model. This model provides a more adequate quantitative description of the 3D Ising system behaviour in comparison with the ρ 4 model (see [7][8][9]). …”
Section: Introductionmentioning
confidence: 99%
“…In our earlier works (see, for example, [7][8][9]), an infinitely weak external field was introduced in the course of calculation of the contribution from the long-wave modes of the spin moment density oscillations to the 3D Ising system thermodynamic characteristics. In this paper, we introduce an external field in the Hamiltonian from the outset.…”
Section: Introductionmentioning
confidence: 99%