Influence of Non-magnetic Ti4+ Doped on Critical Behavior of La0.55Pr0.1Sr0.35Mn1 − xTixO3 (x = 0.00, 0.05) Manganites

被引:0
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作者
Abdelabki Guedri
Aref Omri
Safa Mnefgui
Abdessalem Dhahri
机构
[1] University of Monastir,Laboratory of Physical Chemistry of Materials, Faculty of Science of Monastir, Department of Physics
[2] Université of Gabes,Faculty of sciences of Gabes
[3] University of Kairouan,Research Unit of Valuation and Optimization of Resource, Faculty of Science and Technology of Sidi Bouzid, Campus Agricultural City
[4] National Center for Nuclear Sciences and Technology,Laboratory of Energy and Matter research for Nuclear Science Developments 2LR16CNSTN02
来源
Journal of Superconductivity and Novel Magnetism | 2021年 / 34卷
关键词
Perovskite; Manganites; Second-order phase transition; Critical behavior;
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中图分类号
学科分类号
摘要
Our central focus in this research work is upon the study of the effect of lightly Ti4+ doping ions on the critical behavior of La0.55Pr0.1Sr0.35Mn1 − xTixO3 (x = 0.0 and 0.05) perovskite compounds synthesized by the modified sol-gel Pechini method. The two samples underwent a second-order paramagnetic to ferromagnetic transition as temperature decreased. The critical exponents (beta, gamma, and delta) were determined using various methods based all on the measure of magnetization around the Curie temperature TC. With the Modified Arrot plot method, the critical exponents were found to be β = 0.254, γ = 0.934 at TC = 308.9 K and β = 0.347, γ = 1.29 at TC = 287.8 K for xTi = 0.0 and xTi = 0.05 samples, respectively. Thus, the magnetic interactions satisfied with the prediction of 3-D Tricritical mean field model for xTi = 0.0 and the Heisenberg model forxTi = 0.05. Therefore, the universality class was affected by Ti doping. This result was confirmed by the Kouvel-Fisher method which gave values of β = 0.269, γ = 1.024 at TC = 309.0 K and β = 0.356, γ = 1.31 at TC = 288.3 K for xTi = 0.0 and xTi = 0.05 samples, respectively. These values were checked by the Widom’s scaling equation δ = 1 + γ/β and the Stanley’s scaling equation MHε=εβf±Hεβ+γ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ M\left(H,\varepsilon \right)={\varepsilon}^{\beta }{f}_{\pm}\left(\frac{H}{\varepsilon^{\beta +\gamma }}\right) $$\end{document}. The coupling between critical exponents and magnetocaloric effect was studied by analysis of the field dependence of magnetic entropy change which showed the law dependence, namely, ∆SM ∝ Hn.
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页码:1875 / 1884
页数:9
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