Analyzer-free, intensity-based, wide-field magneto-optical microscopy

dc.bibliographicCitation.firstPage031402eng
dc.bibliographicCitation.issue3eng
dc.bibliographicCitation.journalTitleApplied Physics Reviewseng
dc.bibliographicCitation.volume8eng
dc.contributor.authorSchäfer, Rudolf
dc.contributor.authorOppeneer, Peter M.
dc.contributor.authorOgnev, Alexey
dc.contributor.authorSamardak, Alexander
dc.contributor.authorSoldatov, Ivan V.
dc.date.accessioned2022-02-23T12:52:18Z
dc.date.available2022-02-23T12:52:18Z
dc.date.issued2021
dc.description.abstractIn conventional Kerr and Faraday microscopy, the sample is illuminated with plane-polarized light, and a magnetic domain contrast is generated by an analyzer making use of the Kerr or Faraday rotation. Here, we demonstrate possibilities of analyzer-free magneto-optical microscopy based on magnetization-dependent intensity modulations of the light. (i) The transverse Kerr effect can be applied for in-plane magnetized material, as demonstrated for an FeSi sheet. (ii) Illuminating that sample with circularly polarized light leads to a domain contrast with a different symmetry from the conventional Kerr contrast. (iii) Circular polarization can also be used for perpendicularly magnetized material, as demonstrated for garnet and ultrathin CoFeB films. (iv) Plane-polarized light at a specific angle can be employed for both in-plane and perpendicular media. (v) Perpendicular light incidence leads to a domain contrast on in-plane materials that is quadratic in the magnetization and to a domain boundary contrast. (vi) Domain contrast can even be obtained without a polarizer. In cases (ii) and (iii), the contrast is generated by magnetic circular dichroism (i.e., differential absorption of left- and right-circularly polarized light induced by magnetization components along the direction of light propagation), while magnetic linear dichroism (differential absorption of linearly polarized light induced by magnetization components transverse to propagation) is responsible for the contrast in case (v). The domain-boundary contrast is due to the magneto-optical gradient effect. A domain-boundary contrast can also arise by interference of phase-shifted magneto-optical amplitudes. An explanation of these contrast phenomena is provided in terms of Maxwell-Fresnel theory. © 2021 Author(s).eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/8066
dc.identifier.urihttps://doi.org/10.34657/7107
dc.language.isoengeng
dc.publisherMelville, NY : American Inst. of Physicseng
dc.relation.doihttps://doi.org/10.1063/5.0051599
dc.relation.essn1931-9401
dc.rights.licenseCC BY 4.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/eng
dc.subject.ddc530eng
dc.subject.otherBoron compoundseng
dc.subject.otherCircular polarizationeng
dc.subject.otherCobalt compoundseng
dc.subject.otherDichroismeng
dc.subject.otherIron compoundseng
dc.subject.otherLight polarizationeng
dc.subject.otherMagnetizationeng
dc.subject.otherOptical data storageeng
dc.subject.otherOptical microscopyeng
dc.subject.otherSilicon compoundseng
dc.subject.otherUltrathin filmseng
dc.subject.otherCircularly polarized lighteng
dc.subject.otherDifferential absorptioneng
dc.subject.otherLinearly polarized lighteng
dc.subject.otherMagnetic circular dichroismseng
dc.subject.otherMagnetic linear dichroismeng
dc.subject.otherMagnetization componentseng
dc.subject.otherMagneto-optical microscopyeng
dc.subject.otherRight circularly polarizedeng
dc.subject.otherMagnetic domainseng
dc.titleAnalyzer-free, intensity-based, wide-field magneto-optical microscopyeng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorIFWDeng
wgl.subjectPhysikeng
wgl.typeZeitschriftenartikeleng
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