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Etude des films minces par la méthode de Monte Carlo dans le cadre du modèle de spin d’Ising.

Amel Benmansour

Published May 22, 2021• 0 citations
OpenAlex

Abstract

Using Monte Carlo simulations, we have studied the critical behaviours and phase diagrams of the spin-1/2 and spin-1 Ashkin Teller model ferromagnetic thin films. In the first part: The effect of the interaction with the exchange coupling 𝐽4 is studied. The phase diagrams present different ratios of the surface exchange interaction at the special point, in which all the films thickness have the same critical temperature. First and second order transitions appears in the system. Moreover, at the special point descriptions, we found another partially ordered phase for certain values of the parameter’s interaction. Finally, the critical exponents of the surface magnetization 𝛽1𝑚 are estimated. In the second part, the effects of the crystal field 𝐷 𝐽 ⁄ 2𝑏 and four-spins coupling (𝐽4𝑠 𝐽 ⁄ 2𝑏, 𝐽4𝑏 𝐽 ⁄ 2𝑏) has been studied in details. The phase diagrams in the (𝑘𝐵𝑇𝑐 𝐽 ⁄ 2𝑏 ,𝐽2𝑠 𝐽 ⁄ 2𝑏) plane exhibits the special point, for different values of 𝐷 𝐽 ⁄ 2𝑏 and (𝐽4𝑠 𝐽 ⁄ 2𝑏, 𝐽4𝑏 𝐽 ⁄ 2𝑏). Then, we found rich phase diagrams with firstand second-order phase transitions that meet at tricritical points, that are depended on the film thickness N. Finally, this model presents a new partially ordered phase < 𝜎𝑆 >, between the paramagnetic phase and the Baxter phase, which are separated by a second-order phase transition, for positive values of 𝐷 𝐽 ⁄ 2𝑏 and for each film thickness N.

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Physical review. B, Condensed matter•Mar 1, 1999•15 citations
Using Monte Carlo simulations, we have studied the critical behaviours and phase diagrams of the spin-1/2 and spin-1 Ashkin Teller model ferromagnetic thin films. In the first part: The effect of the interaction with the exchange coupling 𝐽4 is studied. The phase diagrams present different ratios of the surface exchange interaction at the special point, in which all the films thickness have the same critical temperature. First and second order transitions appears in the system. Moreover, at the special point descriptions, we found another partially ordered phase for certain values of the parameter’s interaction. Finally, the critical exponents of the surface magnetization 𝛽1𝑚 are estimated. In the second part, the effects of the crystal field 𝐷 𝐽 ⁄ 2𝑏 and four-spins coupling (𝐽4𝑠 𝐽 ⁄ 2𝑏, 𝐽4𝑏 𝐽 ⁄ 2𝑏) has been studied in details. The phase diagrams in the (𝑘𝐵𝑇𝑐 𝐽 ⁄ 2𝑏 ,𝐽2𝑠 𝐽 ⁄ 2𝑏) plane exhibits the special point, for different values of 𝐷 𝐽 ⁄ 2𝑏 and (𝐽4𝑠 𝐽 ⁄ 2𝑏, 𝐽4𝑏 𝐽 ⁄ 2𝑏). Then, we found rich phase diagrams with firstand second-order phase transitions that meet at tricritical points, that are depended on the film thickness N. Finally, this model presents a new partially ordered phase < 𝜎𝑆 >, between the paramagnetic phase and the Baxter phase, which are separated by a second-order phase transition, for positive values of 𝐷 𝐽 ⁄ 2𝑏 and for each film thickness N.
In order to study the nature of phase transitions in magnetic systems, the aim of our research is to explore the S=1 and σ=3/2 states where the ferromagnetism as well as the influence of different crystal fields will be studied by the Monte Carlo method of The Ashken-Teller model which is a coupling of two Ising models with a four-component parameter. We have given some theoretical definitions related to the phase transition as well as the types of magnetism also the spin models and the simulation method. First, we identify the most stable phases in the phase diagrams at temperature T=0 by energy minimization. Then For higher temperatures, we find phase diagrams rich in ordered phases: a 3/2 Baxter phase and a 1/2 Baxter phase as well as a phase that appears neither in spin 1 nor in spin 3/2 ATM, and finally, a <σ> = 1/2 phases with 1st and 2nd order.
L'étude du modèle Ashkin-Teller (ATM) du spin-3/2 sur un réseau cubique est effectuée par la simulation de Monte Carlo (MC). Les diagrammes de phase sont affichés et discutés dans l'espace de paramètres physiques. Des propriétés physiques riches sont récupérées, comme la transition du second ordre et les points multicritiques. Les diagrammes de phase ont étés obtenus en faisant varier l'interaction 4spins et le champ cristallin. Ce modèle montre une nouvelle phase partiellement ordonné à haute température, appelé et une nouvelle phase Baxter 3/2 qui n’existe pas ni dans l'ATM de spin-1/2, ni dans le spin-1 ATM.
We present the Monte Carlo phase diagram of Ising surfaces with intrasurface ( J s ) and surface-bulk ( J 1 ) interactions modified with respect to the bulk exchange interaction J . The new parameter J 1 strongly affects the position of the Binder-Landau multi critical point and the crossover from three-dimensional to two-dimensional behaviour. The surface critical exponents β 1 and ϕ are determined by crossover scaling analysis. A detailed comparison with the results of the mean-field equations is also presented. The Monte Carlo phase diagram shows that stronger modifications of the surface couplings, with respect to those obtained by mean field, are needed to produce an ordered surface phase on a paramagnetic bulk. This is particularly relevant at low values of J s ; in the Monte Carlo simulation the surface is disordered for all values of J 1 when J s < (0.4 ÷ 0.5) J , while the mean field predicts that the ordered phase is present even in the limit J s → 0.
"We used a Monte Carlo simulation to analize the magnetic behavior of Ising model of mixed spins S A i = ß3=2 ; ß1=2 and æ B j = ß 5 = 2 ; ß 3 = 2 ; ß 1 = 2 , on a square lattice. Were studied the possible critical phenomena that may emerge in the region around the multiphase point (D= j J 1 j = ° 3 ;J 2 = j J 1 j = 1) and the dependence of the phase diagrams with the intensities of the anisotropy field of single ion (D= j J 1 j ) and the ferromagnetic coupling of exchange spin S A i (J 2 = j J 1 j). The system displays first order phase transitions in a certain range of the parameters of the Hamiltonian, which depend on D= j J 1 j and j J 2 = j J 1 j . In the plane (D= j J 1 j ;k B T= j J 1 j), the de- crease of j D= j J 1 jj , implies that the critical temperature, T c , increases and the first order transition temperature, T t , decreases. In the plane (J2 = j J 1 j ;k B T= j J 1 j ), T c increases with the increasing of J 2 = j J 1 j , while that T t decreases."
The study of the Ashkin-Teller model (ATM) of spin-3/2 on a hypercubic lattice is undertaken via Monte Carlo simulation.The phase diagrams are displayed and discussed in the physical parameter space.Rich physical properties are recovered, namely the second order transition and multicritical points.The phase diagrams have been obtained by varying the strength describing the four spin interaction and the single ion potential.This model shows a new high temperature partially ordered phase, called 〈S〉 and a new Baxter 3/2 ground state which do not exist either in the spin-1/2 ATM or in the spin-1 ATM.
Two nonperturbative methods by means of the transfer-matrix finite-size-scaling and Monte Carlo simulations are used to investigate the spin-1 Ashkin-Teller model (ATM). We have obtained rich phase diagrams with first- and second-order phase transitions with several multicritical points of higher order. Also this model exhibits a partially ordered phase PO2{\mathrm{PO}}_{2}PO2​ which does not exist in the spin-1/2 Ashkin-Teller model (ATM). Finally, the critical behavior of this model is discussed.