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Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles

Nd(0.78)Sr(0.22)CoO(3) nanoparticles having 89 nm average particle size are synthesized by standard sol–gel techniques. Structural and morphological characterization is performed by X-ray diffraction and FESEM images. DC magnetization studies in the range 1.6 K to 300 K reveal the disordered magneti...

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Autores principales: Giri, Neepamala, Biswas, Bohnni Shikha, Sengupta, Payal, Ray, Ruma
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9478994/
https://www.ncbi.nlm.nih.gov/pubmed/36275144
http://dx.doi.org/10.1039/d2ra04454d
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author Giri, Neepamala
Biswas, Bohnni Shikha
Sengupta, Payal
Ray, Ruma
author_facet Giri, Neepamala
Biswas, Bohnni Shikha
Sengupta, Payal
Ray, Ruma
author_sort Giri, Neepamala
collection PubMed
description Nd(0.78)Sr(0.22)CoO(3) nanoparticles having 89 nm average particle size are synthesized by standard sol–gel techniques. Structural and morphological characterization is performed by X-ray diffraction and FESEM images. DC magnetization studies in the range 1.6 K to 300 K reveal the disordered magnetic phase below 36 K. Existence of this disordered magnetic phase is substantiated by the magnetic memory effect. A significant upturn in the ZFC magnetization below 4.5 K, which is a signature of a dominant ferromagnetic (FM) component, is observed. This FM component may be attributed to the uncompensated (UC) spins at the surface of Nd(0.78)Sr(0.22)CoO(3) nanoparticles. The presence of the interface of these two magnetic components with significantly different anisotropy results in the exchange bias effect.
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spelling pubmed-94789942022-10-20 Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles Giri, Neepamala Biswas, Bohnni Shikha Sengupta, Payal Ray, Ruma RSC Adv Chemistry Nd(0.78)Sr(0.22)CoO(3) nanoparticles having 89 nm average particle size are synthesized by standard sol–gel techniques. Structural and morphological characterization is performed by X-ray diffraction and FESEM images. DC magnetization studies in the range 1.6 K to 300 K reveal the disordered magnetic phase below 36 K. Existence of this disordered magnetic phase is substantiated by the magnetic memory effect. A significant upturn in the ZFC magnetization below 4.5 K, which is a signature of a dominant ferromagnetic (FM) component, is observed. This FM component may be attributed to the uncompensated (UC) spins at the surface of Nd(0.78)Sr(0.22)CoO(3) nanoparticles. The presence of the interface of these two magnetic components with significantly different anisotropy results in the exchange bias effect. The Royal Society of Chemistry 2022-09-16 /pmc/articles/PMC9478994/ /pubmed/36275144 http://dx.doi.org/10.1039/d2ra04454d Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/
spellingShingle Chemistry
Giri, Neepamala
Biswas, Bohnni Shikha
Sengupta, Payal
Ray, Ruma
Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles
title Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles
title_full Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles
title_fullStr Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles
title_full_unstemmed Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles
title_short Exchange bias and magnetic memory effect in hole doped Nd(0.78)Sr(0.22)CoO(3) nanoparticles
title_sort exchange bias and magnetic memory effect in hole doped nd(0.78)sr(0.22)coo(3) nanoparticles
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9478994/
https://www.ncbi.nlm.nih.gov/pubmed/36275144
http://dx.doi.org/10.1039/d2ra04454d
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