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Influence of Na Addition on Magnetic and Magnetocaloric Effects of La0.67Pb0.13Na0.2MnO3 Ceramics
Authors:Asma?Zaidi,Ahmed?Dhahri  author-information"  >  author-information__contact u-icon-before"  >  mailto:jemai_@outlook.fr"   title="  jemai_@outlook.fr"   itemprop="  email"   data-track="  click"   data-track-action="  Email author"   data-track-label="  "  >Email author,J.?Dhahri,E.?K.?Hlil,M.?Zaidi
Affiliation:1.Laboratoire de la matière condensée et des nanosciences,Université de Monastir,Monastir,Tunisia;2.Laboratoire de Physique Appliquée, Faculté des Sciences de Sfax,Université de Sfax,Sfax,Tunisia;3.Institut Neel,CNRS et Université Joseph Fourier,Grenoble,France;4.College of Science of Zulfi,Majmaah University,Al Majma’ah,Saudi Arabia
Abstract:Structural, magnetic, magnetocaloric, and electrical properties are reported for mixed-valence manganite La0.67Pb0.13Na0.2MnO3. X-ray diffraction reveals that the sample crystallizes in the rhombohedric structure with the R-3c space group. The magnetic properties of the polycrystalline La0.67Pb0.13Na0.2MnO3 compound are discussed in detail, based on the susceptibility, magnetization, and isotherm. The sample presents a ferromagnetic property with T C= 275 K and a Griffiths phase at T G= 325 K which gives the existence of ferromagnetic clusters in the paramagnetic domain. A large deviation is usually observed between field cooled (FC) and zero field cooled (ZFC). M(T) is a low temperature below the blocking temperature. At 40 K, a spin-glass or a cluster-glass state is seen to arise from a ferromagnetic state. This is caused by the competition between the antiferromagnetic and ferromagnetic interactions. The electrical properties show the presence of a metal–semiconductor transition at T M?Sc. To understand the dependence of disorder with the transport mechanism, we used the phenomenological equation for resistivity under a percolation approach, which is dependent on the phase segregation of a paramagnetic semiconductor and ferromagnetic metallic regions.
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