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dc.contributor.authorChen, Po-Anen_US
dc.contributor.authorYang, Chao-Yaoen_US
dc.contributor.authorChang, Shu-Juien_US
dc.contributor.authorLee, Min-Hanen_US
dc.contributor.authorTang, Nai-Kuangen_US
dc.contributor.authorYen, Sheng-Chanen_US
dc.contributor.authorTseng, Yuan-Chiehen_US
dc.date.accessioned2014-12-08T15:36:27Z-
dc.date.available2014-12-08T15:36:27Z-
dc.date.issued2014-12-01en_US
dc.identifier.issn0304-8853en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.jmmm.2014.06.027en_US
dc.identifier.urihttp://hdl.handle.net/11536/24796-
dc.description.abstractTwo commercial Nd2Fe14B samples, MQP-B and sintered-NdFeB were investigated using synchrotron based x-ray diffraction and first-order-reversal-curves (FORCs). Despite differing in magnetic and structural properties, the two samples were found to comprise two major ferromagnetic components in FORCs. For the sintered-NdFeB case, the soft component may originate from the intrinsically soft Nd-f site which was coupled with its local Fe atomic environment that differs in magnetic anisotropy from the Nd-g site (intrinsically hard). It may directly originate from the Nd-rich phase or microstructural imperfection, while the former possibility (Nd-f sire) appears greater than the latter While for the MQP-B, the minor second phase resulting from high structural disorder was likely in charge of the presence of the soft component. Sophisticated FORCs analyses revealed the natures of the soft and hard components, soft hard coupling and switching reversibility of the two cases, irrespective of the origins of their two components. This provides insights to the origin of magnetic stability and reversal dynamics of Nd2Fe14B that have not been fully understood by conventional magnetic analyses. The coexistence of the two components led to an incoherent reversal undermining the magnetic stability of Nd2Fe14B. This is a fundamental problem as to why the performance extremity can only be improved finitely through extrinsic tuning. From FORCs simulation we understand that the soft-hard coupling was moderate in a real Nd2Fe14B compound. A stronger soft-hard coupling is necessary to conquer the anisotropic competition to enable a coherent reversal that will promote the magnetic hardness. (C) 2014 Elsevier B.V. All rights reserved,en_US
dc.language.isoen_USen_US
dc.subjectMagnetic propertiesen_US
dc.subjectMagnetic structureen_US
dc.subjectMagnetic materialsen_US
dc.subjectCrystal structureen_US
dc.titleSoft and hard natures of Nd2Fe14B permanent magnet explored by first-order-reversal-curvesen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.jmmm.2014.06.027en_US
dc.identifier.journalJOURNAL OF MAGNETISM AND MAGNETIC MATERIALSen_US
dc.citation.volume370en_US
dc.citation.issueen_US
dc.citation.spage45en_US
dc.citation.epage53en_US
dc.contributor.department材料科學與工程學系zh_TW
dc.contributor.departmentDepartment of Materials Science and Engineeringen_US
dc.identifier.wosnumberWOS:000340051600008-
dc.citation.woscount0-
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