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Abstract
Ultrastrong and deep-strong coupling are two coupling regimes rich in intriguing physical phenomena. Recently, hybrid magnonic systems have emerged as promising candidates for exploring these regimes, owing to their unique advantages in quantum engineering. However, because of the relatively weak coupling between magnons and other quasiparticles, ultrastrong coupling is predominantly realized at cryogenic temperatures, while deep-strong coupling remains to be explored. In our work, we achieve both theoretical and experimental realization of room-temperature ultrastrong magnon-magnon coupling in synthetic antiferromagnets with intrinsic asymmetry of magnetic anisotropy. Unlike most ultrastrong coupling systems, where the counter-rotating coupling strength g2 is strictly equal to the co-rotating coupling strength g1, our systems allow for highly tunable g1 and g2. This high degree of freedom also enables the realization of normalized g1 or g2 larger than 0.5. Particularly, our experimental findings reveal that the maximum observed g1 is nearly identical to the bare frequency, with g1/ω0 = 0.963, indicating a close realization of deep-strong coupling within our hybrid magnonic systems. Our results highlight synthetic antiferromagnets as platforms for exploring unconventional ultrastrong and even deep-strong coupling regimes, facilitating the further exploration of quantum phenomena.
Deep-strong coupling in hybrid magnonic systems is yet to be explored. Here, the authors unveil unconventional coupling properties in synthetic antiferromagnets. The systems’ high degree of freedom enables a near-realization of deep-strong coupling.
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Details
; Zhang, Yu 2
; Li, Chaozhong 3 ; Wei, Jinwu 3 ; He, Bin 1 ; Xu, Hongjun 4 ; Xia, Jihao 1 ; Luo, Xuming 1 ; Li, Jiahui 1 ; Dong, Jing 4 ; He, Wenqing 1 ; Yan, Zhengren 1 ; Yang, Wenlong 1 ; Ma, Fusheng 2
; Chai, Guozhi 3
; Yan, Peng 5
; Wan, Caihua 1
; Han, Xiufeng 6
; Yu, Guoqiang 6
1 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309); University of Chinese Academy of Sciences, Center of Materials Science and Optoelectronics Engineering, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419)
2 Nanjing Normal University, Jiangsu Key Laboratory of Opto-Electronic Technology, School of Physics and Technology, Nanjing, China (GRID:grid.260474.3) (ISNI:0000 0001 0089 5711)
3 Lanzhou University, Key Laboratory for Magnetism and Magnetic Materials of the Ministry of Education, Lanzhou, China (GRID:grid.32566.34) (ISNI:0000 0000 8571 0482)
4 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309); Songshan Lake Materials Laboratory, Dongguan, China (GRID:grid.511002.7)
5 University of Electronic Science and Technology of China, School of Electronic Science and Engineering and State Key Laboratory of Electronic Thin Films and Integrated Devices, Chengdu, China (GRID:grid.54549.39) (ISNI:0000 0004 0369 4060)
6 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309); University of Chinese Academy of Sciences, Center of Materials Science and Optoelectronics Engineering, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419); Songshan Lake Materials Laboratory, Dongguan, China (GRID:grid.511002.7)




