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hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorMAYER, Charlotte
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorGORSSE, Stéphane
hal.structure.identifierLaboratoire national des champs magnétiques intenses - Grenoble [LNCMI-G]
dc.contributor.authorBALLON, Géraldine
hal.structure.identifierInstituto de Ciencia de Materiales de Sevilla [ICMSE]
dc.contributor.authorCABALLERO-FLORES, Rafael
hal.structure.identifierInstituto de Ciencia de Materiales de Sevilla [ICMSE]
dc.contributor.authorFRANCO, Victor
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCHEVALIER, Bernard
dc.date.issued2011
dc.identifier.issn0021-8979
dc.description.abstractEnThe series of glassy ribbons Gd60M30In10 (M = Mn, Co, Ni, Cu) was synthesized by melt-spinning. The change of transition element M in these Gd-based metallic glasses was proven to induce huge variations of the Curie temperature TC, magnetic entropy change peak values ΔSm<sup>peak</sup>, and widths at half maximum values of the magnetic entropy change δT. When M is non magnetic (M = Co, Ni, Cu), the samples behave similarly: they display high values of ΔSm<sup>peak</sup> (between -6.6 and -8.2 J/kg K in a magnetic field variation of 4.6 T), average δT values (between 77 and 120 K) and no magnetic hysteresis. On the contrary, when M carries a magnetic moment (M = Mn), some irreversibility appears at low temperature, ΔSm<sup>peak</sup> is lower (only 3.1 J/kg K for μ0H = 4.6 T) and the magnetic transition is very large (δT = 199 K for μ0H = 4.6 T). These features are explained by some antiparallel coupling between Mn atoms randomly located in the metallic glass. This leads to the occurrence of a cluster-glass behavior at low temperature (35 K), following the ferromagnetic transition observed at 180 K when the temperature is decreased. Also, power law fittings of ΔSm<sup>peak</sup> and δT versus μ0H were performed and show that δT is less field dependent than ΔSm<sup>peak</sup>. We could then identify an interesting way of improving the refrigeration capacity of the material at low magnetic field.
dc.language.isoen
dc.publisherAmerican Institute of Physics
dc.subject.enNickel alloys
dc.subject.enCurie temperature
dc.subject.enCobalt alloys
dc.subject.enCopper alloys
dc.subject.enEntropy
dc.subject.enGadolinium alloys
dc.subject.enIndium alloys
dc.subject.enMagnetic transitions
dc.subject.enMagnetocaloric effects
dc.subject.enManganese alloys
dc.subject.enMelt spinning
dc.title.enTunable magnetocaloric effect in Gd-based glassy ribbons
dc.typeArticle de revue
dc.identifier.doi10.1063/1.3632983
dc.subject.halChimie/Matériaux
bordeaux.journalJournal of Applied Physics
bordeaux.page053920 (7 p.)
bordeaux.volume110
bordeaux.issue5
bordeaux.peerReviewedoui
hal.identifierhal-00626201
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00626201v1
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