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Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite

The orthorhombic Pr(0.8)Na(0.2)MnO(3) ceramic was prepared in polycrystalline form by a Pechini sol–gel method and its structural, magnetic, electrical and dielectric properties were investigated experimentally. A structural study confirms that the sample is single phase. Magnetic measurements show...

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Autores principales: Ouni, I., Ben Khlifa, H., M'nassri, R., Nofal, Muaffaq M., Rahmouni, H., Cheikhrouhou, W., Chniba-Boudjada, N., Khirouni, K., Cheikhrouhou, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9074664/
https://www.ncbi.nlm.nih.gov/pubmed/35528058
http://dx.doi.org/10.1039/c9ra05414f
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author Ouni, I.
Ben Khlifa, H.
M'nassri, R.
Nofal, Muaffaq M.
Rahmouni, H.
Cheikhrouhou, W.
Chniba-Boudjada, N.
Khirouni, K.
Cheikhrouhou, A.
author_facet Ouni, I.
Ben Khlifa, H.
M'nassri, R.
Nofal, Muaffaq M.
Rahmouni, H.
Cheikhrouhou, W.
Chniba-Boudjada, N.
Khirouni, K.
Cheikhrouhou, A.
author_sort Ouni, I.
collection PubMed
description The orthorhombic Pr(0.8)Na(0.2)MnO(3) ceramic was prepared in polycrystalline form by a Pechini sol–gel method and its structural, magnetic, electrical and dielectric properties were investigated experimentally. A structural study confirms that the sample is single phase. Magnetic measurements show that the sample is a charge ordered manganite. The sample undergoes two successive magnetic phase transitions with the variation of temperature: a charge ordering transition occurred at T(CO) = 212 K followed by a paramagnetic (PM) to ferromagnetic (FM) transition around T(C) = 115 K. From an electrical point of view, a saturation region was marked in the conductivity as a function of temperature σ(T) curves at a specific temperature. The dc-conductivity (σ(dc)) reaches a maximum value at 240 K. The obtained results are in good agreement with the temperature dependence of the average normalized change (ANC). We found that the conduction mechanism was governed by small polaron hopping (SPH) in the high temperature region and by variable range hopping (VRH) in the low temperature region. Complex impedance analysis indicates the presence of a non-Debye relaxation phenomenon in the system. Also, the compound was modeled by an electrical equivalent circuit. Then, the contribution of the grain boundary in the transport properties was confirmed.
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spelling pubmed-90746642022-05-06 Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite Ouni, I. Ben Khlifa, H. M'nassri, R. Nofal, Muaffaq M. Rahmouni, H. Cheikhrouhou, W. Chniba-Boudjada, N. Khirouni, K. Cheikhrouhou, A. RSC Adv Chemistry The orthorhombic Pr(0.8)Na(0.2)MnO(3) ceramic was prepared in polycrystalline form by a Pechini sol–gel method and its structural, magnetic, electrical and dielectric properties were investigated experimentally. A structural study confirms that the sample is single phase. Magnetic measurements show that the sample is a charge ordered manganite. The sample undergoes two successive magnetic phase transitions with the variation of temperature: a charge ordering transition occurred at T(CO) = 212 K followed by a paramagnetic (PM) to ferromagnetic (FM) transition around T(C) = 115 K. From an electrical point of view, a saturation region was marked in the conductivity as a function of temperature σ(T) curves at a specific temperature. The dc-conductivity (σ(dc)) reaches a maximum value at 240 K. The obtained results are in good agreement with the temperature dependence of the average normalized change (ANC). We found that the conduction mechanism was governed by small polaron hopping (SPH) in the high temperature region and by variable range hopping (VRH) in the low temperature region. Complex impedance analysis indicates the presence of a non-Debye relaxation phenomenon in the system. Also, the compound was modeled by an electrical equivalent circuit. Then, the contribution of the grain boundary in the transport properties was confirmed. The Royal Society of Chemistry 2019-11-01 /pmc/articles/PMC9074664/ /pubmed/35528058 http://dx.doi.org/10.1039/c9ra05414f Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/
spellingShingle Chemistry
Ouni, I.
Ben Khlifa, H.
M'nassri, R.
Nofal, Muaffaq M.
Rahmouni, H.
Cheikhrouhou, W.
Chniba-Boudjada, N.
Khirouni, K.
Cheikhrouhou, A.
Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite
title Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite
title_full Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite
title_fullStr Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite
title_full_unstemmed Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite
title_short Structural, magnetic, electrical and dielectric properties of Pr(0.8)Na(0.2)MnO(3) manganite
title_sort structural, magnetic, electrical and dielectric properties of pr(0.8)na(0.2)mno(3) manganite
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9074664/
https://www.ncbi.nlm.nih.gov/pubmed/35528058
http://dx.doi.org/10.1039/c9ra05414f
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