Effect of Non-magnetic Ti4+ Ion Doping at Mn-site on Magnetocaloric Properties and Critical Behavior in AMn1-xTixO3 (0 ≤ x ≤ 0.2) Compounds
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作者:
Aref Omri
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机构:University Campus Agricultural City,Research Unit of Valuation and Optimization of Resource, Faculty of Science and Technology of Sidi Bouzid
Aref Omri
E. Dhahri
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机构:University Campus Agricultural City,Research Unit of Valuation and Optimization of Resource, Faculty of Science and Technology of Sidi Bouzid
E. Dhahri
E. K. Hlil
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机构:University Campus Agricultural City,Research Unit of Valuation and Optimization of Resource, Faculty of Science and Technology of Sidi Bouzid
E. K. Hlil
机构:
[1] University Campus Agricultural City,Research Unit of Valuation and Optimization of Resource, Faculty of Science and Technology of Sidi Bouzid
[2] University of Kairouan,Laboratory of Applied Physics, Sfax Faculty of Science
[3] University of Sfax,Institut Néel
[4] CNRS - Université J. Fourier,undefined
来源:
Journal of Low Temperature Physics
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2021年
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204卷
关键词:
Perovskite;
Magnetic entropy change;
Critical exponents;
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摘要:
In this paper, we present a thorough study for the critical behavior of AMn1-xTixO3 (A = La0.5Pr0.2Sr0.3, x = 0.0 and 0.2) polycrystalline samples by analysing their isothermal magnetization data using various technique such us modified Arrott plots, Kouvel-Fischer method, and critical magnetisation isotherms M(TC,H). The critical exponent values for the undoped compound allowed us to assign a mean field universality class with long-range interactions (β = 0.509,γ = 1.094,δ = 3.14). The non-magnetic Ti-substitution does not affect the class of universality. The analysis shows that the critical exponents of all compounds were close to those of the mean field model with long-range interaction. The field dependence of the magnetic entropy change is also analyzed using-ΔSM=aHn\documentclass[12pt]{minimal}
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\begin{document}$$\Delta S_{M} = a\left( H \right)^{n}$$\end{document} power law, where the exponent n values ranging between 0.68 and 0.74 are close to those obtained from the theoretical relation n(TC)=1+β-1/β+γ\documentclass[12pt]{minimal}
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\begin{document}$$n(T_C) = 1 + \left(\left( \beta - 1\right)/\left(\beta + \gamma \right)\right)$$\end{document}. The second-order nature of the magnetic phase transition has been confirmed by constructing the universal magnetic entropy change curves. The spontaneous magnetization values determined using the magnetic entropy change (∆SM vs. M2) are in good agreement with those obtained from the classical extrapolation of Arrott curves (H/M vs. M2).