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dc.contributor.authorSilva, Franciscarlos Gomes dapt_BR
dc.contributor.authorDepeyrot, J.pt_BR
dc.contributor.authorRaikher, Yuriypt_BR
dc.contributor.authorStepanov, Victorpt_BR
dc.contributor.authorPoperechny, Igorpt_BR
dc.contributor.authorSouza, Renata Aquino da Silva dept_BR
dc.contributor.authorBallon, Geraldinept_BR
dc.contributor.authorGeshev, Julian Penkovpt_BR
dc.contributor.authorDubois, Emmanuellept_BR
dc.contributor.authorPerzynski, Réginept_BR
dc.date.accessioned2021-06-25T04:26:16Zpt_BR
dc.date.issued2021pt_BR
dc.identifier.issn2045-2322pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/222872pt_BR
dc.description.abstractExchange bias properties of MnFe2O4@γ–Fe2O3 core–shell nanoparticles are investigated. The measured feld and temperature dependencies of the magnetization point out a well-ordered ferrimagnetic core surrounded by a layer with spin glass-like arrangement. Quasi-static SQUID magnetization measurements are presented along with high-amplitude pulse ones and are cross analyzed by comparison against ferromagnetic resonance experiments at 9GHz. These measurements allow one to discern three types of magnetic anisotropies afecting the dynamics of the magnetic moment of the well-ordered ferrimagnetic NP’s core viz. the easy-axis (uniaxial) anisotropy, the unidirectional exchange-bias anisotropy and the rotatable anisotropy. The uniaxial anisotropy originates from the structural core–shell interface. The unidirectional exchange-bias anisotropy is associated with the spin-coupling at the ferrimagnetic/spin glass-like interface; it is observable only at low temperatures after a feld-cooling process. The rotatable anisotropy is caused by partially pinned spins at the core/shell interface; it manifests itself as an intrinsic feld always parallel to the external applied magnetic feld. The whole set of experimental results is interpreted in the framework of superparamagnetic theory, i.e., essentially taking into account the efect of thermal fuctuations on the magnetic moment of the particle core. In particular, it is found that the rotatable anisotropy of our system is of a uniaxial type.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofScientific reports. London. Vol. 11 (Mar. 2021), 5474, 10 p.pt_BR
dc.rightsOpen Accessen
dc.subjectAnisotropia magnéticapt_BR
dc.subjectNanopartículas de ferropt_BR
dc.subjectPolarização por intercâmbiopt_BR
dc.titleExchange‑bias and magnetic anisotropy felds in core–shell ferrite nanoparticlespt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb001125607pt_BR
dc.type.originEstrangeiropt_BR


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