Role of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet

In order to prove the usefulness of having a structurally disordered precursor to the formation of FePt L1<sub>0</sub> phase and to facilitate the co-existence of exchange coupled hard and soft magnetic phases with optimized magnetic properties in various conditions of annealing, a Fe-Pt...

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Autores principales: Alina Daniela Crisan, Ioan Dan, Ovidiu Crisan
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Publicado: MDPI AG 2021
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spelling oai:doaj.org-article:410393a0d8cb4668b0b080659100b25f2021-11-25T18:12:32ZRole of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet10.3390/magnetochemistry71101492312-7481https://doaj.org/article/410393a0d8cb4668b0b080659100b25f2021-11-01T00:00:00Zhttps://www.mdpi.com/2312-7481/7/11/149https://doaj.org/toc/2312-7481In order to prove the usefulness of having a structurally disordered precursor to the formation of FePt L1<sub>0</sub> phase and to facilitate the co-existence of exchange coupled hard and soft magnetic phases with optimized magnetic properties in various conditions of annealing, a Fe-Pt-Zr-B melt spun alloy has been synthesized and detailed structural and magnetic investigations have been undertaken to probe its phase evolution during annealing. The dynamics of formation of the hard magnetic L1<sub>0</sub> phase during the gradual disorder–order phase transformation has been monitored by using a complex combination of X-ray diffraction methods and <sup>57</sup>Fe Mössbauer spectroscopy methods, over a wide range of annealing temperatures. Multiple phases co-existing in the annealed sample microstructures, observed in XRD, have been reconfirmed by the Mössbauer spectra analysis and, moreover, accurate quantitative data have been acquired in what concerns the relative abundance of each of the observed crystalline phases in every stage of annealing. It is shown that the formation of the hard magnetic phase, emerging from the chemically disordered precursor, is gradual and occurs via complex mechanisms, involving the presence of a disordered Fe-Zr-B-rich intergranular region which contributes to an increase in the abundance of the L1<sub>0</sub> phase for higher annealing temperatures. Magnetic measurements have confirmed the good performances of these alloys in terms of coercivity and remanence. These results contribute to the development of these alloys as the next generation of rare earth, free permanent magnets.Alina Daniela CrisanIoan DanOvidiu CrisanMDPI AGarticlenanocomposite magnetsL1<sub>0</sub> phaseMössbauer spectroscopymagnetic propertiesChemistryQD1-999ENMagnetochemistry, Vol 7, Iss 149, p 149 (2021)
institution DOAJ
collection DOAJ
language EN
topic nanocomposite magnets
L1<sub>0</sub> phase
Mössbauer spectroscopy
magnetic properties
Chemistry
QD1-999
spellingShingle nanocomposite magnets
L1<sub>0</sub> phase
Mössbauer spectroscopy
magnetic properties
Chemistry
QD1-999
Alina Daniela Crisan
Ioan Dan
Ovidiu Crisan
Role of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet
description In order to prove the usefulness of having a structurally disordered precursor to the formation of FePt L1<sub>0</sub> phase and to facilitate the co-existence of exchange coupled hard and soft magnetic phases with optimized magnetic properties in various conditions of annealing, a Fe-Pt-Zr-B melt spun alloy has been synthesized and detailed structural and magnetic investigations have been undertaken to probe its phase evolution during annealing. The dynamics of formation of the hard magnetic L1<sub>0</sub> phase during the gradual disorder–order phase transformation has been monitored by using a complex combination of X-ray diffraction methods and <sup>57</sup>Fe Mössbauer spectroscopy methods, over a wide range of annealing temperatures. Multiple phases co-existing in the annealed sample microstructures, observed in XRD, have been reconfirmed by the Mössbauer spectra analysis and, moreover, accurate quantitative data have been acquired in what concerns the relative abundance of each of the observed crystalline phases in every stage of annealing. It is shown that the formation of the hard magnetic phase, emerging from the chemically disordered precursor, is gradual and occurs via complex mechanisms, involving the presence of a disordered Fe-Zr-B-rich intergranular region which contributes to an increase in the abundance of the L1<sub>0</sub> phase for higher annealing temperatures. Magnetic measurements have confirmed the good performances of these alloys in terms of coercivity and remanence. These results contribute to the development of these alloys as the next generation of rare earth, free permanent magnets.
format article
author Alina Daniela Crisan
Ioan Dan
Ovidiu Crisan
author_facet Alina Daniela Crisan
Ioan Dan
Ovidiu Crisan
author_sort Alina Daniela Crisan
title Role of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet
title_short Role of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet
title_full Role of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet
title_fullStr Role of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet
title_full_unstemmed Role of Disordered Precursor in L1<sub>0</sub> Phase Formation in FePt-Based Nanocomposite Magnet
title_sort role of disordered precursor in l1<sub>0</sub> phase formation in fept-based nanocomposite magnet
publisher MDPI AG
publishDate 2021
url https://doaj.org/article/410393a0d8cb4668b0b080659100b25f
work_keys_str_mv AT alinadanielacrisan roleofdisorderedprecursorinl1sub0subphaseformationinfeptbasednanocompositemagnet
AT ioandan roleofdisorderedprecursorinl1sub0subphaseformationinfeptbasednanocompositemagnet
AT ovidiucrisan roleofdisorderedprecursorinl1sub0subphaseformationinfeptbasednanocompositemagnet
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