Dresden 2017 – wissenschaftliches Programm
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MA: Fachverband Magnetismus
MA 65: Poster 2
MA 65.14: Poster
Freitag, 24. März 2017, 09:30–13:00, P2-OG1
The quadratic magnetooptic tensor of cubic materials without inversion symmetry — •Robin Silber1,2, Jan-Oliver Dreessen2, Jaromír Pištora1, Günter Reiss2, Martin Veis3, Jaroslav Hamrle3, and Timo Kuschel2,4 — 1VSB - Technical University of Ostrava, Czech Republic — 2CSMD, Physics Department, Bielefeld University, Germany — 3Charles University, Prague, Czech Republic — 4University of Groningen, The Netherlands
The permittivity tensor of a magnetized crystal could be described by a Taylor series: εij=εij(0)+εij(1)+εij(2)+... , where the superscript denotes the order in magnetization (M). The shape of εij(2) is determined by the so-called quadratic magnetooptic (MO) tensor Gijkl [1]. This quadratic MO tensor for cubic materials with and without inversion symmetry differ in the parameter Δ Γ=(G12−G21) [2], being zero for cubic material with inversion symmetry as G12=G21. The Δ Γ parameter was predicted by symmetry arguments of the structure, but no experimental determination method exists so far. Here, we propose a new measurement procedure of magnetooptic Kerr effect (MOKE), allowing us to separate contribution of ΔΓ to overall MOKE signal.
[1] Š. Višňovský, Czech. J. Phys. B 36, 1424 (1986)
[2] J. Hamrlová et al., Phys. Status Solidi B 250, 2194 (2013)