Magnetic structure determination and putative anisotropic exchange coupling in the hybrid organic-inorganic perovskite (CH5NH2NH2NH3)2MnCl4

09.10.2025, 11:00
15m
Evangelische Akademie Tutzing

Evangelische Akademie Tutzing

Schloßstraße 2+4, 82327 Tutzing, Germany
Talk Low dimensional quantum magnetism Low dimensional quantum magnetism

Sprecher

Lukas Beddrich (JCNS-4, PANDA)

Beschreibung

The interest in low-dimensional magnetism (LDM) is manifold, but can be summarized in two categories. First, it provides a rich test bed for fundamental research in many-body quantum phenomena to study the influences of restricted exchange pathways, frustration and enhanced quantum fluctuations. Second, LDM has been shown to have links with various phenomena such as high-temperature superconductivity, fractional excitations, spin liquids and multiferroicity, which are at the forefront of global solid-state research.
Metal-organic compounds (MOC) serve as an essentially infinite toolbox for building model systems for LDM research. Owing to their modular structure, the strength, type and direction of magnetic exchange can be tuned by the ligand molecules, which connect the magnetic ions. The perovskite Mn-PEA [fully (C$_6$H$_5$CH$_2$CH$_2$NH$_3$)$_2$MnCl$_4$] is considered to be one of the ideal layered 2D antiferromagnets, minimizing out-of-plane interactions by separating magnetically active Mn$^{2+}$ ions by long organic chains.
We have successfully performed neutron diffraction (D10+, ILL) and inelastic neutron scattering experiments at the cold multiplexing spectrometer HODACA (JRR-3) and TAS (JRR-3, HANARO) on non-deuterated Mn-PEA single crystals to determine the magnetic structure and its spin wave excitations. The magnetic moments are antiferromagnetically aligned along the $c$-axis, with a slight canting into the ab-plane. The spin wave dispersion is completely $l$-independent which is characteristic of negligible exchange interactions across the separation layer of organic ligands. Using spinW, we apply linear spin wave theory including exchange coupling up to the next-nearest neighbors and DMI between nearest neighbors to account for the observation of a second dispersion branch along $h$.

Autoren

Dr. Chul-Ho Lee (National Institute of Advanced Industrial Science and Technology (AIST)) Dr. Garam Park (Department of Physics Education, Kongju National University) Dr. Hodaka Kikuchi (Institute for Solid State Physics, The University of Tokyo) Dr. In-Hwan Oh (HANARO, Korea Atomic Energy Research Institute) Dr. Iurii Kibalin (Institut Laue-Langevin) Jitae Park (MLZ, TUM) Karin Schmalzl (JCNS Outstation at ILL, Grenoble) Dr. Kazuhiro Nawa (Institute of Multidisciplinary Research for Advanced Materials, Tohoku University) Dr. Ki-Yeon Kim (HANARO, Korea Atomic Energy Research Institute) Dr. Laura Canadillas-Delgado (ILL) Lukas Beddrich (JCNS-4, PANDA) Dr. Oscar Fabelo Rosa (ILL) Dr. Sungdae Ji (HANARO, Korea Atomic Energy Research Institute) Herr Yunxiao Liu (FRM II, TUM)

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