Abstract

A spin-1 Blume–Capel model with dilute and random crystal fields is examined for honeycomb and square lattices by introducing an effective-field approximation that takes into account the correlations between different spins that emerge when expanding the identities. For dilute crystal fields, we have given a detailed exploration of the global phase diagrams of the system in kBTc/J−D/J plane with the second and first order transitions, as well as tricritical points. We have also investigated the effect of the random crystal field distribution characterized by two crystal field parameters D/J and △/J on the phase diagrams of the system. The system exhibits clear distinctions in a qualitative manner with coordination number q for random crystal fields with △/J,D/J≠0. We have also found that, under certain conditions, the system may exhibit a number of interesting and unusual phenomena, such as reentrant behavior of first and second order, as well as a double reentrance with three successive phase transitions.

Highlights

  • Spin-1 Blume–Capel (BC) model [1,2] is one of the most extensively studied models in statistical mechanics and condensed matter physics

  • The phase diagrams have a symmetric shape with respect to △/J which comes from the fact that p = 1/2, and as seen in Fig. 4, transition temperatures are second order, and it is clear that the system exhibit different characteristic features depending on the coordination number q

  • We have introduced an effective-field approximation that takes into account the correlations between different spins in the cluster of a considered lattice and examined the phase diagrams as well as magnetization curves of the system for different types of crystal field distributions, namely, dilute crystal fields and a double peaked delta distribution, given by Eqs. (2) and (3), respectively

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Summary

Introduction

Spin-1 Blume–Capel (BC) model [1,2] is one of the most extensively studied models in statistical mechanics and condensed matter physics. From the theoretical point of view, the BC model with a random crystal field (RCF) has been studied by a variety of techniques such as the cluster variational method (CVM) [4], Bethe lattice approximation (BLA) [5], effective field theory (EFT) [6,7,8,9,10], finite cluster approximation (FCA) [11,12], mean field theory (MFT) [13,14,15,16,17,18,19], Monte Carlo (MC) simulations [20], pair approximation (PA) [21], and the renormalization group (RG) method [22].

Formulation
Results and discussion
Phase diagrams of the system with dilute crystal field
Phase diagrams of the system with random crystal field
Conclusions
Full Text
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