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Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds

In this study, our central focus is to investigate the magnetocaloric characteristics of a La(1−x)□(x)MnO(3) (x = 0.1, 0.2 and 0.3) series prepared by a sol–gel technique published in Prog. Mater. Sci., 93, 2018, 112–232. The crystallographic study revealed that our compounds crystallize in a rhombo...

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Autores principales: Henchiri, C., Mnasri, T., Benali, A., Hamdi, R., Dhahri, E., Valente, M. A., Costa, B. F. O.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9050008/
https://www.ncbi.nlm.nih.gov/pubmed/35497833
http://dx.doi.org/10.1039/c9ra10469k
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author Henchiri, C.
Mnasri, T.
Benali, A.
Hamdi, R.
Dhahri, E.
Valente, M. A.
Costa, B. F. O.
author_facet Henchiri, C.
Mnasri, T.
Benali, A.
Hamdi, R.
Dhahri, E.
Valente, M. A.
Costa, B. F. O.
author_sort Henchiri, C.
collection PubMed
description In this study, our central focus is to investigate the magnetocaloric characteristics of a La(1−x)□(x)MnO(3) (x = 0.1, 0.2 and 0.3) series prepared by a sol–gel technique published in Prog. Mater. Sci., 93, 2018, 112–232. The crystallographic study revealed that our compounds crystallize in a rhombohedral structure with R3̄c. Ferromagnetic (FM) and paramagnetic (PM) characters were detected from the variation in magnetization as a function of magnetic fields at different temperatures. The second order transition was verified from the Arrott plots (M(2)vs. (μ(0)H/M)), where the slopes have a positive value. In order to verify the second order, we traced the variation of magnetization vs. temperature at different magnetic fields for x = 0.2. This revealed a ferromagnetic (FM)–paramagnetic (PM) transition when temperature increases. Relying on the indirect method while using the Maxwell formula, we determined the variation in the entropy (−ΔS(M)) as a function of temperature for different magnetic fields for the three samples. We note that all the studied systems stand as good candidates for magnetic refrigeration with relative cooling power (RCP) values of around 131.4, 83.38 and 57.26 J kg(−1) with magnetic fields below 2 T, respectively. Subsequently, the magnetocaloric effect was investigated by a phenomenological model for x = 0.2. The extracted data confirm that this phenomenological model is appropriate for the prediction of magnetocaloric properties. The study also demonstrated that this La(0.8)□(0.2)MnO(3) system exhibits a universal behaviour.
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spelling pubmed-90500082022-04-29 Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds Henchiri, C. Mnasri, T. Benali, A. Hamdi, R. Dhahri, E. Valente, M. A. Costa, B. F. O. RSC Adv Chemistry In this study, our central focus is to investigate the magnetocaloric characteristics of a La(1−x)□(x)MnO(3) (x = 0.1, 0.2 and 0.3) series prepared by a sol–gel technique published in Prog. Mater. Sci., 93, 2018, 112–232. The crystallographic study revealed that our compounds crystallize in a rhombohedral structure with R3̄c. Ferromagnetic (FM) and paramagnetic (PM) characters were detected from the variation in magnetization as a function of magnetic fields at different temperatures. The second order transition was verified from the Arrott plots (M(2)vs. (μ(0)H/M)), where the slopes have a positive value. In order to verify the second order, we traced the variation of magnetization vs. temperature at different magnetic fields for x = 0.2. This revealed a ferromagnetic (FM)–paramagnetic (PM) transition when temperature increases. Relying on the indirect method while using the Maxwell formula, we determined the variation in the entropy (−ΔS(M)) as a function of temperature for different magnetic fields for the three samples. We note that all the studied systems stand as good candidates for magnetic refrigeration with relative cooling power (RCP) values of around 131.4, 83.38 and 57.26 J kg(−1) with magnetic fields below 2 T, respectively. Subsequently, the magnetocaloric effect was investigated by a phenomenological model for x = 0.2. The extracted data confirm that this phenomenological model is appropriate for the prediction of magnetocaloric properties. The study also demonstrated that this La(0.8)□(0.2)MnO(3) system exhibits a universal behaviour. The Royal Society of Chemistry 2020-02-26 /pmc/articles/PMC9050008/ /pubmed/35497833 http://dx.doi.org/10.1039/c9ra10469k Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/
spellingShingle Chemistry
Henchiri, C.
Mnasri, T.
Benali, A.
Hamdi, R.
Dhahri, E.
Valente, M. A.
Costa, B. F. O.
Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds
title Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds
title_full Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds
title_fullStr Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds
title_full_unstemmed Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds
title_short Structural study and large magnetocaloric entropy change at room temperature of La(1−x)□(x)MnO(3) compounds
title_sort structural study and large magnetocaloric entropy change at room temperature of la(1−x)□(x)mno(3) compounds
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9050008/
https://www.ncbi.nlm.nih.gov/pubmed/35497833
http://dx.doi.org/10.1039/c9ra10469k
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