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Quadratic-in-magnetization permittivity and conductivity tensor in cubic crystals

dc.contributor.authorHamrlová, Jana
dc.contributor.authorHamrle, Jaroslav
dc.contributor.authorPostava, Kamil
dc.contributor.authorPištora, Jaromír
dc.date.accessioned2013-11-28T09:19:08Z
dc.date.available2013-11-28T09:19:08Z
dc.date.issued2013
dc.identifier.citationphysica status solidi (b) – basic solid state physics. 2013, vol. 250, issue 10, p. 2194-2205.cs
dc.identifier.issn0370-1972
dc.identifier.issn1521-3951
dc.identifier.urihttp://hdl.handle.net/10084/101291
dc.description.abstractWe present diagonal and off-diagonal elements of the permittivity and conductivity tensor up to the second order in magnetization for cubic crystals. We express all tensor elements as a function of a general sample orientation, for arbitrary magnetization direction and for (001), (011), and (111) surface orientations. Finally, we discuss, how to extract values of quadratic elements G of the second-order permittivity tensors for different sample surface orientations from both experiment and ab initio calculations.cs
dc.language.isoencs
dc.publisherWiley-VCHcs
dc.relation.ispartofseriesphysica status solidi (b) – basic solid state physicscs
dc.relation.urihttp://dx.doi.org/10.1002/pssb.201349031cs
dc.rights© 2013 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheimcs
dc.subjectanisotropic magnetoresistancecs
dc.subjectcubic crystalscs
dc.subjectmagnetic linear dichroismcs
dc.subjectmagneto-optical Kerr effectcs
dc.titleQuadratic-in-magnetization permittivity and conductivity tensor in cubic crystalscs
dc.typearticlecs
dc.identifier.doi10.1002/pssb.201349031
dc.type.statusPeer-reviewedcs
dc.description.sourceWeb of Sciencecs
dc.description.volume250cs
dc.description.issue10cs
dc.description.lastpage2205cs
dc.description.firstpage2194cs
dc.identifier.wos000325484300037


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