Magnetic Dichroism in the Reflectivity of Linearly Polarized Synchrotron Radiation from a Ti(10 nm)/Gd{sub 0.23}Co{sub 0.77}(250 nm)/Ti(10 nm) Sample

The dichroic effect (“rotated” polarization) in the reflectivity from a magnetically ordered sample is experimentally studied at the station PHASE of the Kurchatov Synchrotron Radiation Source. The experiments are performed for the Gd{sub 0.23}Co{sub 0.77} film, which has a compensation temperature...

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Published inJournal of experimental and theoretical physics Vol. 126; no. 6
Main Authors Andreeva, M. A., Baulin, R. A., Borisov, M. M., Gan’shina, E. A., Kurlyandskaya, G. V., Mukhamedzhanov, E. Kh, Repchenko, Yu. L., Svalov, A. V.
Format Journal Article
LanguageEnglish
Published United States 15.06.2018
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Summary:The dichroic effect (“rotated” polarization) in the reflectivity from a magnetically ordered sample is experimentally studied at the station PHASE of the Kurchatov Synchrotron Radiation Source. The experiments are performed for the Gd{sub 0.23}Co{sub 0.77} film, which has a compensation temperature T{sub comp} ≈ 433 K, using linearly polarized radiation of the photon energy of 7930 eV (L{sub 2} absorption edge of gadolinium) at room temperature. The developed theory of reflectivity accounted for the magnetic contributions to the scattering amplitude predicts the appearance of a peak for the orthogonal (to the incident polarization) polarization of the reflected radiation near the critical angle of the total external reflection. The experiment reveals the significant difficulties because of the incomplete σ polarization of the synchrotron beam, the beam instability, and so on. Therefore, a rotated-polarization peak has been detected near the critical angle but at the limits of the measurement accuracy. In principle, our experimental technique could be an alternative to circular polarization experiments, which are widely used at synchrotrons to study magnetic ordering. However, as we have shown, it makes high demands of the radiation source parameters.
ISSN:1063-7761
1090-6509
DOI:10.1134/S1063776118050102