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Abstract
Frustrated magnets hold the promise of material realizations of exotic phases of quantum matter, but direct comparisons of unbiased model calculations with experimental measurements remain very challenging. Here we design and implement a protocol of employing many-body computation methodologies for accurate model calculations—of both equilibrium and dynamical properties—for a frustrated rare-earth magnet TmMgGaO4 (TMGO), which explains the corresponding experimental findings. Our results confirm TMGO is an ideal realization of triangular-lattice Ising model with an intrinsic transverse field. The magnetic order of TMGO is predicted to melt through two successive Kosterlitz–Thouless (KT) phase transitions, with a floating KT phase in between. The dynamical spectra calculated suggest remnant images of a vanishing magnetic stripe order that represent vortex–antivortex pairs, resembling rotons in a superfluid helium film. TMGO therefore constitutes a rare quantum magnet for realizing KT physics, and we further propose experimental detection of its intriguing properties.
TmMgGaO4 is one of a number of recently-synthesized quantum magnets that are proposed to realize important theoretical models. Here the authors demonstrate the agreement between detailed experimental measurements and state-of-the-art predictions based on the 2D transverse-field triangular lattice Ising model.
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1 Beihang University, Key Laboratory of Micro-Nano Measurement-Manipulation and Physics (Ministry of Education), School of Physics, Beijing, China (GRID:grid.64939.31) (ISNI:0000 0000 9999 1211)
2 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309); University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419)
3 Beihang University, Key Laboratory of Micro-Nano Measurement-Manipulation and Physics (Ministry of Education), School of Physics, Beijing, China (GRID:grid.64939.31) (ISNI:0000 0000 9999 1211); Ludwig-Maximilians-Universität München, Fakultät für Physik, Arnold Sommerfeld Center for Theoretical Physics, Center for NanoScience, and Munich Center for Quantum Science and Technology, München, Germany (GRID:grid.5252.0) (ISNI:0000 0004 1936 973X)
4 Fudan University, Center for Field Theory and Particle Physics, Department of Physics and State Key Laboratory of Surface Physics, Shanghai, China (GRID:grid.8547.e) (ISNI:0000 0001 0125 2443); Collaborative Innovation Center of Advanced Microstructures, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
5 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309); The University of Hong Kong, Department of Physics and HKU-UCAS Joint Institute of Theoretical and Computational Physics, Hong Kong, China (GRID:grid.194645.b) (ISNI:0000000121742757); Songshan Lake Materials Laboratory, Dongguan, China (GRID:grid.194645.b)
6 Beihang University, Key Laboratory of Micro-Nano Measurement-Manipulation and Physics (Ministry of Education), School of Physics, Beijing, China (GRID:grid.64939.31) (ISNI:0000 0000 9999 1211); Beihang University, International Research Institute of Multidisciplinary Science, Beijing, China (GRID:grid.64939.31) (ISNI:0000 0000 9999 1211)