Introducing artificial length scales to tailor magnetic properties

dc.bibliographicCitation.journalTitleNew Journal of Physicseng
dc.bibliographicCitation.volume11
dc.contributor.authorFassbender, J.
dc.contributor.authorStrache, T.
dc.contributor.authorLiedke, M.O.
dc.contributor.authorMarkó, D.
dc.contributor.authorWintz, S.
dc.contributor.authorLenz, K.
dc.contributor.authorKeller, A.
dc.contributor.authorFacsko, S.
dc.contributor.authorMönch, I.
dc.contributor.authorMcCord, J.
dc.date.accessioned2018-06-12T16:44:15Z
dc.date.available2019-06-28T12:39:57Z
dc.date.issued2009
dc.description.abstractMagnetism is a collective phenomenon. Hence, a local variation on the nanoscale of material properties, which act on the magnetic properties, affects the overall magnetism in an intriguing way. Of particular importance are the length scales on which a material property changes. These might be related to the exchange length, the domain wall width, a typical roughness correlation length, or a length scale introduced by patterning of the material. Here we report on the influence of two artificially created length scales: (i) ion erosion templates that serve as a source of a predefined surface morphology (ripple structure) and hence allow for the investigation of roughness phenomena. It is demonstrated that the ripple wave length can be easily tuned over a wide range (25–175 nm) by varying the primary ion erosion energy. The effect of this ripple morphology on the induced uniaxial magnetic anisotropy in soft magnetic Permalloy films is studied. Only below a ripple wavelength threshold (≈60 nm) is a significant induced magnetic anisotropy found. Above this threshold the corrugated Permalloy film acts as a flat film. This cross-over is discussed in the frame of dipolar interactions giving rise to the induced anisotropies. (ii) Ion implantation through a lithographically defined mask, which is used for a magnetic property patterning on various length scales. The resulting magnetic properties are neither present in non-implanted nor in homogeneously implanted films. Here new insight is gained by the comparison of different stripe patterning widths ranging from 1 to 10 μm. In addition, the appearance of more complicated magnetic domain structures, i.e. spin-flop domain configurations and head-on domain walls, during hard axis magnetization reversal is demonstrated. In both cases the magnetic properties, the magnetization reversal process as well as the magnetic domain configurations depend sensitively on the artificially introduced length scale.eng
dc.description.versionpublishedVersioneng
dc.formatapplication/pdf
dc.identifier.urihttps://doi.org/10.34657/1563
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/4366
dc.language.isoengeng
dc.publisherMilton Park : Taylor & Franciseng
dc.relation.doihttps://doi.org/10.1088/1367-2630/11/12/125002
dc.rights.licenseCC BY-NC-SA 3.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by-nc-sa/3.0/eng
dc.subject.ddc530eng
dc.subject.otherCollective phenomenaeng
dc.subject.otherCross-overeng
dc.subject.otherDipolar interactioneng
dc.subject.otherDomain configurationseng
dc.subject.otherDomain wall widtheng
dc.subject.otherExchange lengtheng
dc.subject.otherFlat filmseng
dc.subject.otherInduced magnetic anisotropyeng
dc.subject.otherIon erosioneng
dc.subject.otherLength scaleeng
dc.subject.otherLocal variationseng
dc.subject.otherMagnetic domain structureseng
dc.subject.otherMagnetization reversal processeng
dc.subject.otherMaterial propertyeng
dc.subject.otherNano scaleeng
dc.subject.otherPermalloy filmseng
dc.subject.otherRipple structureeng
dc.subject.otherRipple wavelengtheng
dc.subject.otherRoughness correlationeng
dc.subject.otherSoft magneticseng
dc.subject.otherSpin flopseng
dc.subject.otherUniaxial magnetic anisotropyeng
dc.titleIntroducing artificial length scales to tailor magnetic propertieseng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorIFWDeng
wgl.subjectPhysikeng
wgl.typeZeitschriftenartikeleng
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