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1.Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
2.University of Chinese Academy of Sciences, Beijing 100049, China
3.Theoretical Materials Physics, Q-MAT, Université de Liège, Liège B-4000, Belgium
4.Beijing Academy of Quantum Information Sciences, Beijing 100193, China
5.State Key Laboratory for Mesoscopic Physics and Frontiers Science Center for Nano-optoelectronics, School of Physics, Peking University, Beijing 100871, China
6.Beijing National Center for Electron Microscopy and Laboratory of Advanced Materials, Department of Materials Science and Engineering, Tsinghua University, 100084 Beijing, China
Kui-juan Jin (kjjin@iphy.ac.cn)
Received:03 December 2024,
Revised:08 March 2025,
Accepted:24 March 2025,
Published Online:22 April 2025,
Published:30 June 2025
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Xu, S. et al. Characterizing G-type antiferromagnetism quantitatively with optical second harmonic generation. Light: Science & Applications, 14, 1718-1726 (2025).
Xu, S. et al. Characterizing G-type antiferromagnetism quantitatively with optical second harmonic generation. Light: Science & Applications, 14, 1718-1726 (2025). DOI: 10.1038/s41377-025-01849-3.
Antiferromagnetism has become a promising candidate for the next generation electronic devices due to its thermal stability
low energy consumption
and fast switching speed. However
the canceling of the net magnetic moment in antiferromagnetic order presents great challenge on quantitative characterization and modulation
hindering its investigation and application. In this work
utilizing the optical second harmonic generation (SHG) in a wide temperature range
the integrated differential phase contrast scanning transmission electron microscopy
and first-principles calculations
we performed a quantitative study on the evolution of non-collinear antiferromagnetic order in BiFeO
3
films with a series of strains. We found that the antiferromagnetic coupling was significantly enhanced
featured by the increase of Néel temperature from 428 K to 646 K
and by one order of enhancement of SHG intensity contributed from the G-type antiferromagnetic order by strain manipulation from -2.4% to +0.6%. We attributed the enhancement of the antiferromagnetic coupling to the enhancement of the superexchange interaction as the Fe-O-Fe bond angle approaches 180° when the in-plane lattice co
nstants increase
which might also result in a tendency from a non-collinear antiferromagnetic order to a collinear one. Our work not only bridges the antiferromagnetic order and the strain manipulation in epitaxial multiferroics
more importantly
also paves a way for quantitative characterization by SHG technology and the precise manipulation of antiferromagnetism.
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