Second order magnetic phase transition and scaling analysis in iron doped manganite La0.7Ca0.3Mn1-xFexO3 compounds

被引:14
|
作者
Ginting, Dianta [1 ,2 ]
Nanto, Dwi [3 ]
Denny, Yus Rama [4 ]
Tarigan, Kontan [5 ]
Hadi, Syamsul [6 ]
Ihsan, Mohammad [7 ,8 ]
Rhyee, Jong-Soo [1 ,2 ]
机构
[1] Kyung Hee Univ, Dept Appl Phys, Yongin 446701, South Korea
[2] Kyung Hee Univ, Inst Nat Sci, Yongin 446701, South Korea
[3] Syarif Hidayatullah State Islamic Univ, Phys Educ, Jakarta 15412, Indonesia
[4] Univ Sultan Ageng Tirtayasa, Dept Elect Engn, Banten 42435, Indonesia
[5] Mercu Buana Univ, Dept Mech Engn, Jakarta 11650, Indonesia
[6] State Polytech Malang, Dept Mech Engn, East Java 65100, Indonesia
[7] PSTBM BATAN, Tangerang Selatan 15314, Banten, Indonesia
[8] Univ Wollongong, Inst Elect Mat, Wollongong, NSW 2522, Australia
关键词
Second order magnetic transition; Critical behaviors; Iron doped; Manganite; Perovskite; EQUATION-OF-STATE; COLOSSAL MAGNETORESISTANCE; FERROMAGNETISM; CRITERION;
D O I
10.1016/j.jmmm.2015.07.033
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We investigated magnetic properties of La0.7Ca0.3Mn1-xFexO3 (x=0.09 and 0.11) compounds in terms of isothermal magnetization analysis and scaling behavior with various critical exponents. From the Landau theory of magnetic phase transition, we found that the paramagnetic to ferromagnetic phase transition in La0.7Ca0.3Mn1-xFexO3 (x=0.09 and 0.11) compounds is the type of second order magnetic transition (SOMT), which contrary to the first order magnetic transition (FOMT) for low Fe doped compounds (x < 0.09) in previous reports. When we investigate the critical behavior of the compounds near T=T-c by the modified Ai rott plot, Kouvel-Fisher plots, and critical isothermal analysis, the estimated critical exponents beta, gamma, and delta are in between the theoretically predicted values for three-dimensional Heisenberg and mean-held interaction models, It is noteworthy that the scaling relations are obeyed in terms of renormalization magnetization m=epsilon(-beta) M(H,epsilon) and renormalized held h=vertical bar epsilon vertical bar(beta+gamma) H. Temperature-dependent effective exponents beta(eff) and gamma(eff) correspond to the ones of disordered ferromagnets. It is shown that the magnetic state of the compounds is not fully described by the conventional localized-spin interaction model because the ferromagnetic interaction has itinerant character by increasing Fe-doping concentration. (C) 2015 Elsevier B.V. All rights reserved.
引用
收藏
页码:41 / 47
页数:7
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