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dc.contributor.authorMartínez Boubeta, Carlos-
dc.contributor.authorClavero Pérez, César-
dc.contributor.authorGarcía-Martín, José Miguel-
dc.contributor.authorArmelles Reig, Gaspar-
dc.contributor.authorCebollada, Alfonso-
dc.contributor.authorBalcells Argemi, Lluis-
dc.contributor.authorMenéndez, José Luis-
dc.contributor.authorPeiró, F.-
dc.contributor.authorCornet, Albert-
dc.date.accessioned2009-11-30T10:29:48Z-
dc.date.available2009-11-30T10:29:48Z-
dc.date.issued2005-01-06-
dc.identifier.citationPhysical Review B 71, 014407 (2005)en_US
dc.identifier.issn1098-0121-
dc.identifier.urihttp://hdl.handle.net/10261/19136-
dc.description.abstractDifferent aspects of the structure-magnetism and morphology-magnetism correlation in the ultrathin limit are studied in epitaxial Fe films grown on MgO(001). In the initial stages of growth the presence of substrate steps, intrinsically higher than an Fe atomic layer, prevent the connection between Fe islands and hence the formation of large volume magnetic regions. This is proposed as an explanation to the superparamagnetic nature of ultrathin Fe films grown on MgO in addition to the usually considered islanded, or Vollmer-Weber, growth. Using this model, we explain the observed transition from superparamagnetism to ferromagnetism for Fe coverages above 3 monolayers (ML). However, even though ferromagnetism and magnetocrystalline anisotropy are observed for 4 ML, complete coverage of the MgO substrate by the Fe ultrathin films only occurs around 6 ML as determined by polar Kerr spectra and simulations that consider different coverage situations. In annealed 3.5 ML Fe films, shape or configurational anisotropy dominates the intrinsic magnetocrystalline anisotropy, due to an annealing induced continuous to islanded morphological transition. A small interface anisotropy in thicker films is observed, probably due to dislocations observed at the Fe∕MgO(001) interface.en_US
dc.description.sponsorshipThe Spanish Commission of Science and Technology, and Comunidad de Madrid are acknowledged for financial support. Portions of this research were carried out at the Stanford Synchrotron Radiation Laboratory, a national user facility operated by Stanford University on behalf of the U.S. Department of Energy, Office of Basic Energy Sciences. One of the authors (J. M. G. M.) thanks the Spanish Ministry of Science and Technology for his present “Ramón y Cajal” contract.en_US
dc.format.extent370629 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoengen_US
dc.publisherAmerican Physical Societyen_US
dc.rightsopenAccessen_US
dc.subjectMagnetismen_US
dc.subjectUltrathin filmsen_US
dc.titleCoverage effects on the magnetism of Fe∕MgO(001) ultrathin filmsen_US
dc.typeartículoen_US
dc.identifier.doi10.1103/PhysRevB.71.014407-
dc.description.peerreviewedPeer revieweden_US
dc.relation.publisherversionhttp://link.aps.org/doi/10.1103/PhysRevB.71.014407en_US
dc.relation.publisherversionhttp://dx.doi.org/10.1103/PhysRevB.71.014407en_US
dc.type.coarhttp://purl.org/coar/resource_type/c_6501es_ES
item.languageiso639-1en-
item.fulltextWith Fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.cerifentitytypePublications-
item.grantfulltextopen-
item.openairetypeartículo-
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