C4: Ultrastrong matter-magnon coupling phenomena
Joachim Deisenhofer, Marcus Kollar
In this project we will explore ultrastrong coupling (USC) effects in the polar magnets A2Mo3O8 with A = Fe, Co, Mn, Zn and in the rare-earth orthoferrites REFeO3 (RE = Tm, Er, Y) using THz-time-domain spectroscopy in external magnetic fields. We will identify further material classes to clarify the origin of the USC and the involved bosonic states. New non-equilibrium phenomena will be investigated using intense coherent THz fields. We will develop a theoretical description in terms of quantum Rabi-type models using input from the THz data. Their complexity will depend on the importance of counter-rotating terms and the presence of asymmetric terms due to broken inversion symmetry. Numerical and analytical studies of these models will help to clarify the origin of the USC.
Publications
2024 |
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Vasin, K. V.; Strinić, A.; Schilberth, F.; Reschke, S.; Prodan, L.; Tsurkan, V.; Nurmukhametov, A. R.; Eremin, M. V.; Kézsmárki, I.; Deisenhofer, J. Optical magnetoelectric effect in the polar honeycomb antiferromagnet Fe2Mo3O8 Journal Article Phys. Rev. B 110, 054401, 2024. @article{vasin_optical_2024, The lack of both time-reversal and spatial inversion symmetry in polar magnets is a prerequisite for the occurrence of optical magnetoelectric effects such as nonreciprocal directional dichroism, i.e., a difference in refractive index and absorption for two counter-propagating electromagnetic waves, which has the potential for the realization of optical diodes. In particular, antiferromagnetic materials with magnetic excitations in the THz range such as Fe2Mo3O8 are promising candidates for next-generation spintronic applications. In a combined experimental and theoretical effort we investigated the THz excitations of the polar honeycomb antiferromagnet Fe2Mo3O8 in external magnetic fields and their nonreciprocal directional dichroism, together with the temperature dependence of the electronic transitions in the mid- and near-infrared frequency range. Using an advanced single-ion approach for the Fe ions, we are able to describe optical excitations from the THz to the near-infrared frequency range quantitatively and model the observed nonreciprocal directional dichroism in the THz regime successfully. | |
2023 |
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Ghara, S.; Barts, E.; Vasin, K. V.; Kamenskyi, D.; Prodan, L.; Tsurkan, V.; Kézsmárki, I.; Mostovoy, M.; Deisenhofer, J. Magnetization reversal through an antiferromagnetic state Journal Article Nat. Commun. 14, 5174, 2023. @article{ghara_magnetization_2023, Magnetization reversal in ferro- and ferrimagnets is a well-known archetype of non-equilibrium processes, where the volume fractions of the oppositely magnetized domains vary and perfectly compensate each other at the coercive magnetic field. Here, we report on a fundamentally new pathway for magnetization reversal that is mediated by an antiferromagnetic state. Consequently, an atomic-scale compensation of the magnetization is realized at the coercive field, instead of the mesoscopic or macroscopic domain cancellation in canonical reversal processes. We demonstrate this unusual magnetization reversal on the Zn-doped polar magnet Fe2Mo3O8. Hidden behind the conventional ferrimagnetic hysteresis loop, the surprising emergence of the antiferromagnetic phase at the coercive fields is disclosed by a sharp peak in the field-dependence of the electric polarization. In addition, at the magnetization reversal our THz spectroscopy studies reveal the reappearance of the magnon mode that is only present in the pristine antiferromagnetic state. According to our microscopic calculations, this unusual process is governed by the dominant intralayer coupling, strong easy-axis anisotropy and spin fluctuations, which result in a complex interplay between the ferrimagnetic and antiferromagnetic phases. Such antiferro-state-mediated reversal processes offer novel concepts for magnetization control, and may also emerge for other ferroic orders. |