Magnetic and electrical behaviour of La0.67Ba0.33Mn1-xFexO3 perovskites

被引:60
作者
Baazaoui, M. [1 ]
Zemni, S. [1 ]
Boudard, M. [2 ]
Rahmouni, H. [3 ]
Gasmi, A. [1 ,2 ]
Selmi, A. [4 ]
Oumezzine, M. [1 ]
机构
[1] Dept Phys, Fac Sci Monastir, Lab Phys Chim Mat, Monastir 5019, Tunisia
[2] CNRS, Mat & Genie Phys Lab, UMR 5628, F-38016 Grenoble 1, France
[3] Dept Phys, Fac Sci Gabes, Lab Phys Mat & Nanomat Appl Environm, Gabes 6079, Tunisia
[4] Dept Phys, Fac Sci Monastir, Lab Phys Semicond & Composants Elect, Monastir 5019, Tunisia
关键词
Ceramic manganites; Iron doping; X-ray diffraction; Magnetic and electrical properties; COLOSSAL MAGNETORESISTANCE; TRANSPORT-PROPERTIES; MN-SITE; MAGNETOTRANSPORT PROPERTIES; DOUBLE EXCHANGE; FE; SUBSTITUTION; FIELD;
D O I
10.1016/j.matlet.2009.07.019
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
(La0.67Ba0.33)Mn1-xFexO3 manganites compounds have been prepared by doping up to 20% of Fe at the Mn site. As previously reported in the literature paramagnetic (PM) to ferromagnetic (FM) phase transition has been observed in materials with low Fe doping (<= 10%). In our x = 0 and x = 0.05 compounds the Curie temperature (T-C) is close to room temperature. Above 10% Fe amount, specimens exhibit a glass magnetic behaviour with a spin- or cluster-like freezing process that can be related to a loss of ferromagnetic double exchange interaction. Below 10% of Fe3+ doping electrical-resistivity measurement shows metal - semiconductor transition with a maximum peak of resistivity (rho(max)) at a temperature T-P close to T-C. Above 10% of Fe3+ doping amount the materials exhibit only semiconductor behaviour. Both T-C and T-P decrease with doping rates with an increasing difference in temperature (T-P, being lower than T-C). Results are consistent with a reduction of the number of available hopping sites for the Mn e(g)(up arrow) electron due to substitution of Mn3+ by Fe3+ that suppress the double exchange (DE) interactions. (C) 2009 Elsevier B.V. All rights reserved.
引用
收藏
页码:2167 / 2170
页数:4
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