Zobrazit minimální záznam

dc.contributor.authorSilber, Robin
dc.contributor.authorTomíčková, Michaela
dc.contributor.authorRodewald, Jari
dc.contributor.authorWollschläger, Joachim
dc.contributor.authorPištora, Jaromír
dc.contributor.authorVeis, Martin
dc.contributor.authorKuschel, Timo
dc.contributor.authorHamrle, Jaroslav
dc.date.accessioned2018-10-16T07:54:01Z
dc.date.available2018-10-16T07:54:01Z
dc.date.issued2018
dc.identifier.citationPhotonics and Nanostructures - Fundamentals and Applications. 2018, vol. 31, p. 60-65.cs
dc.identifier.issn1569-4410
dc.identifier.issn1569-4429
dc.identifier.urihttp://hdl.handle.net/10084/132745
dc.description.abstractIn most of the cases the magnetooptic Kerr effect (MOKE) techniques rely solely on the effects linear in magnetization (M). Nevertheless, a higher-order term being proportional to M-2 and called quadratic MOKE (QMOKE) can additionally contribute to experimental data. Handling and understanding the underlying origin of QMOKE could be the key to utilize this effect for investigation of antiferromagnetic materials in the future due to their vanishing first order MOKE contribution. Also, better understanding of QMOKE and hence better understanding of magnetooptic (MO) effects in general is very valuable, as the MO effect is very much employed in research of ferro- and ferrimagnetic materials. Therefore, we present our QMOKE and longitudinal MOKE spectroscopy setup with a spectral range of 0.8-5.5 eV. The setup is based on light modulation through a photoelastic modulator and detection of second-harmonic intensity by a lock-in amplifier. To measure the Kerr ellipticity an achromatic compensator is used within the setup, whereas without it Kerr rotation is measured. The separation of QMOKE spectra directly from the measured data is based on measurements with multiple magnetization directions. So far the QMOKE separation algorithm is developed and tested for but not limited to cubic (001) oriented samples. The QMOKE spectra yielded by our setup arise from two quadratic MO parameters G(s) and 2G(44), being elements of quadratic MO tensor G, which describes perturbation of the permittivity tensor in the second order in M.cs
dc.language.isoencs
dc.publisherElseviercs
dc.relation.ispartofseriesPhotonics and Nanostructures - Fundamentals and Applicationscs
dc.relation.urihttp://doi.org/10.1016/j.photonics.2018.05.007cs
dc.rights© 2018 Elsevier B.V. All rights reserved.cs
dc.subjectquadratic magnetooptic Kerr effectcs
dc.subjectmagnetooptic spectroscopycs
dc.subjectmagnetooptic tensorscs
dc.subjectmagnetitecs
dc.subjectphotoelastic modulatorcs
dc.titleQuadratic magnetooptic spectroscopy setup based on photoelastic light modulationcs
dc.typearticlecs
dc.identifier.doi10.1016/j.photonics.2018.05.007
dc.type.statusPeer-reviewedcs
dc.description.sourceWeb of Sciencecs
dc.description.volume31cs
dc.description.lastpage65cs
dc.description.firstpage60cs
dc.identifier.wos000445716900008


Soubory tohoto záznamu

SouboryVelikostFormátZobrazit

K tomuto záznamu nejsou připojeny žádné soubory.

Tento záznam se objevuje v následujících kolekcích

Zobrazit minimální záznam