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dc.contributor.authorBadía-Romano, L.-
dc.contributor.authorBartolomé, Fernando-
dc.contributor.authorBartolomé, Juan-
dc.contributor.authorLuzón, Javier-
dc.contributor.authorProdius, D.-
dc.contributor.authorTurta, C.-
dc.contributor.authorMereacre, V.-
dc.contributor.authorWilhelm, F.-
dc.contributor.authorRogalev, A.-
dc.date.accessioned2015-07-06T10:56:24Z-
dc.date.available2015-07-06T10:56:24Z-
dc.date.issued2013-
dc.identifierdoi: 10.1103/PhysRevB.87.184403-
dc.identifierissn: 1098-0121-
dc.identifiere-issn: 1550-235X-
dc.identifier.citationPhysical Review B 87: 184403 (2013)-
dc.identifier.urihttp://hdl.handle.net/10261/117607-
dc.descriptionUnder the terms of the Creative Commons Attribution License 3.0 (CC-BY).-
dc.description.abstractThe intramolecular exchange interactions within the single-molecule magnet (SMM) "butterfly" molecule [Fe3Ln(μ3-O) 2(CCl3COO)8(H2O)(THF)3], where Ln(III) represents a lanthanide cation, are determined in a combined experimental [x-ray magnetic circular dichroism (XMCD) and vibrating sample magnetometer (VSM)] and theoretical work. Compounds with Ln=Gd and Dy, which represent extreme cases where the rare earth presents single-ion isotropic and uniaxial anisotropy, on one hand, and with Ln=Lu and Y(III) as pseudolanthanide substitutions that supply a nonmagnetic Ln reference case, on the other hand, are studied. The Dy single-ion uniaxial anisotropy is estimated from ab initio calculations. Low-temperature (T 2.5 K) hard x-ray XMCD at the Ln L 2,3 edges and VSM measurements as a function of the field indicate that the Ln moment dominates the polarization of the molecule by the applied field. Within the {Fe3LnO2} cluster the Ln-Fe3 subcluster interaction is determined to be antiferromagnetic in both Dy and Gd compounds, with values J Dy-Fe3=-0.4 K and J Gd-Fe3=-0.25 K, by fitting to spin Hamiltonian simulations that consider the competing effects of intracluster interactions and the external applied magnetic field. In the uniaxial anisotropic {Fe3DyO2} case, a field-induced reorientation of the Fe3 and Dy spins from an antiparallel to a parallel orientation takes place at a threshold field (μ0H=4 T). In contrast, in isotropic {Fe3GdO2} this reorientation does not occur. © 2013 American Physical Society.-
dc.description.sponsorshipThe financial support of Spanish MINECO Grant No. MAT2011-23791, the Alexander Von Humboldt Foundation (D.P.), and Aragonese DGA-IMANA E34 (cofunded by Fondo Social Europeo) and that received from European Union FEDER funds are also acknowledged. L.B.R. acknowledges the Spanish MINECO FPU 2010 grant.-
dc.publisherAmerican Physical Society-
dc.relation.isversionofPublisher's version-
dc.rightsopenAccess-
dc.titleField-induced internal Fe and Ln spin reorientation in butterfly {Fe3LnO2} (Ln = Dy and Gd) single-molecule magnets-
dc.typeartículo-
dc.identifier.doi10.1103/PhysRevB.87.184403-
dc.relation.publisherversionhttp://dx.doi.org/10.1103/PhysRevB.87.184403-
dc.date.updated2015-07-06T10:56:24Z-
dc.description.versionPeer Reviewed-
dc.language.rfc3066eng-
dc.rights.licensehttp://creativecommons.org/licenses/by/3.0/-
dc.contributor.funderMinisterio de Economía y Competitividad (España)-
dc.contributor.funderEuropean Commission-
dc.contributor.funderDiputación General de Aragón-
dc.contributor.funderAlexander von Humboldt Foundation-
dc.relation.csic-
dc.identifier.funderhttp://dx.doi.org/10.13039/501100003329es_ES
dc.identifier.funderhttp://dx.doi.org/10.13039/501100000780es_ES
dc.identifier.funderhttp://dx.doi.org/10.13039/100005156es_ES
dc.type.coarhttp://purl.org/coar/resource_type/c_6501es_ES
item.fulltextWith Fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.openairetypeartículo-
item.cerifentitytypePublications-
item.grantfulltextopen-
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