Jul 7 – 11, 2025
Europe/Bratislava timezone
NEWS: The full scientific programme has been released.

A Frustrated Antipolar Analogue to the Classical Spin Liquid in Triangular Lattice EuAl$_{12}$O$_{19}$

I-09
Jul 8, 2025, 2:00 PM
30m
INVITED ORAL Topic 6 - Low-dimensional magnetic materials, molecular magnets and ferrofluids Section S6

Speaker

Ross Colman (Department of Condensed Matter Physics, Charles University, Prague, Czech Republic)

Description

The ground-state of the $S =1/2$ Ising 2D Triangular Lattice AntiFerroMagnet (ITLAFM) is the go-to example of a frustrated magnet, and was calculated by Wannier over $70$ years ago [1]. In the absence of strong quantum fluctuations, this ground-state is called a classical spin liquid with a large number of energy-degenerate spin configurations that share the minimum energy. It is expected to have spin-dynamics governed by Arrhenius behavior, with spinons required to transform between each topologically protected configuration [2]. Despite interest in investigating this type of system experimentally, model magnetic materials are hard to come by, with magnetic moments typically deviating from the Ising limit or displaying significant quantum fluctuations.

The rare-earth hexaaluminates with the magnetoplumbite structure are a promising family for the investigation of ITLAFM physics, and I will present our investigations of the compound EuAl$_{12}$O$_{19}$. Despite the well separated triangular layers of magnetic ions, the Eu$^{2+}$ magnetic interactions drive the material to ferromagnetism with a $T_C = 1.3$ K [3].

Instead, we find the sought-after classic-liquid physics of the ITLAFM ground-state not within its magnetic lattice, but within a lattice of antiferroelectrically coupled dipoles. The material contains a triangular lattice of dynamically disordered, but antiferroelectrically correlated, charge displacive dipoles built from Al$^{3+}$ ions sitting off-centre within their bipyramid oxygen cages. Electric dipoles have an advantage over spins that they can be intrinsically Ising, and we label this model instead the Ising Triangular Lattice AntiFerroElectric (ILAFE). I will present our recently published structural, spectroscopic, and thermodynamic measurements on EuAl$_{12}$O$_{19}$, comparing the observed properties to those expected for the ITLAFM [4].

References

[1] G. H. Wannier, “Antiferromagnetism. The Triangular Ising Net,” Physical Review, vol. 79, no. 2. American Physical Society (APS), pp. 357–364, Jul. 15, 1950. https://doi.org/10.1103/physrev.79.357
[2] Z. Zhou et al., “Quantum dynamics of topological strings in a frustrated Ising antiferromagnet,” npj Quantum Materials, vol. 7, no. 1. Springer Science and Business Media LLC, Jun. 08, 2022. https://doi.org/10.1038/s41535-022-00465-3
[3] G. Bastien et al.,"Quasi-two-dimensional ferromagnetism in the triangular magnet EuAl12⁢O19" Physical Review B, vol. 110, no. 9. American Physical Society (APS), Sep. 24, 2024. https://doi.org/10.1103/physrevb.110.094436
[4] G. Bastien et al., “A Frustrated Antipolar Phase Analogous to Classical Spin Liquids,” Advanced Materials, vol. 36, no. 50. Wiley, Oct. 23, 2024. https://doi.org/10.1002/adma.202410282

Primary author

Gael Bastien (Department of Condensed Matter Physics, Charles University, Prague)

Co-authors

Dalibor Repček (Institute of Physics of the Czech Academy of Sciences) Adam Eliáš (Department of Condensed Matter Physics, Charles University, Prague) Andrej Kancko (Department of Condensed Matter Physics, Charles University, Prague) Quentin Courtade (Department of Condensed Matter Physics, Charles University, Prague) Tetiana Haidamak (Department of Condensed Matter Physics, Charles University, Prague) Maxim Savinov (Institute of Physics of the Czech Academy of Sciences) Viktor Bovtun (Institute of Physics of the Czech Academy of Sciences) Martin Kempa (Institute of Physics of the Czech Academy of Sciences) Karel Carva (Department of Condensed Matter Physics, Faculty of Mathematics and Physics, Charles University) Michal Valiska (Department of Condensed Matter Physics, Charles University, Prague) Petr Doležal (Department of Condensed Matter Physics, Charles University, Prague) Marie Kratochvílová (Department of Condensed Matter Physics, Charles University, Prague) Petr Proschek (Department of Condensed Matter Physics, Charles University, Prague) Jan Prokleška (Department of Condensed Matter Physics, Charles University, Prague) Christelle Kadlec (Institute of Physics of the Czech Academy of Sciences) Petr Kužel (Institute of Physics of the Czech Academy of Sciences) Ross Colman (Department of Condensed Matter Physics, Charles University, Prague, Czech Republic) Stanislav Kamba (Institute of Physics of the Czech Academy of Sciences)

Presentation materials

There are no materials yet.