Critical behavior and magnetocaloric simulation of La0.7Ba0.2Ca0.1Mn1-xSnxO3 near room temperature

被引:1
|
作者
Dhahri, Jamila [1 ]
Lefi, Ramzi [2 ]
Bouzidi, Souhir [3 ]
Essid, Manel [4 ]
Abdulaziz, Fahad [5 ]
Alsehli, Amal H. [6 ]
Alsowayigh, Marwah M. [7 ]
机构
[1] Univ Monastir, Fac Sci Monastir, Dept Phys, Lab Phys Chem Mat, Monastir 5019, Tunisia
[2] Univ Sfax, Fac Sci Sfax, Lab Mat Energy & Environm & Modeling LMEEM, Sfax, Tunisia
[3] Univ Monastir, Fac Sci Monastir, Dept Phys, Lab Matiere Condensee & Nanosci, Monastir, Tunisia
[4] King Khalid Univ KKU, Coll Sci, Chem Dept, POB 9004, Abha, Saudi Arabia
[5] Univ Hail, Coll Sci, Dept Chem, Hail 81451, Saudi Arabia
[6] Taibah Univ, Coll Sci, Chem Dept, Madinah 42353, Saudi Arabia
[7] King Faisal Univ, Coll Sci, Chem Dept, Al Hasa 31982, Saudi Arabia
来源
关键词
Iterative process; Magnetization; Modified Arrott plot; Critical exponent; EQUATION-OF-STATE; MAGNETORESISTANCE; MANGANITES; NICKEL; ORDER; FIELD;
D O I
10.1007/s00339-023-07003-3
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
In this article, we focus on the critical behavior of La0.7Ba0.2Ca0.1Mn1-xSnxO3 samples (x = 0.00 and 0.01) around the PM-FM phase transition by measuring the magnetization M (mu H-0) versus magnetic field. The study is based on an iterative process using modified Arrott plots. We then use other techniques to confirm the critical parameters obtained for our manganites, such as the Kouvel-Fisher (KF) method and the critical isotherm (CI) around Tc. Our samples are characterized by a second-order phase transition. The critical parameters determined (beta, gamma and delta) have no known universal classes. Moreover, Widom's scaling formula delta = 1 + gamma/beta, demonstrates the accuracy of the critical exponent parameters. In addition, we employ the scaling equation M(H,epsilon)=epsilon beta f +/-(H epsilon beta+gamma)M(H,epsilon)=epsilon(beta)f(+/-)(H/epsilon(beta+gamma)) with epsilon = (T-T-C)/T-C to further verify the reasonableness of the critical exponent in which the curves (M-mu 0H-T) split into two distinct branches under and over the T-C. Furthermore, the simulated M (H, T) plots were generated to determine the - S-M (T) plots; according to the Gibbs free energy within the obtained critical exponent.
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页数:10
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