Abstract
Magneto-optical (MO) effects have a pivotal role in modern photonic devices for light manipulation and sensing, but the study of these effects has so far been limited to the MO Faraday and Kerr effects. Conventional MO systems encounter considerable intrinsic losses, markedly hampering their ability to amplify the MO effects. Here we introduce a loss-enhanced MO effect to sublinearly amplify the frequency response of a non-Hermitian optical cavity under different background magnetic fields. This exceptional MO effect relies on an architecture of MO material embedded in a Fabry–Pérot cavity, accompanied by a polarization-dependent optical absorption, that is, linear dichroism, to construct a reconfigurable exceptional point. The experimental results show that two eigenmodes of the Fabry–Pérot cavity exhibit sublinear frequency splitting. By electrically reconfiguring the absorber, the eigenfrequency shift can be adaptively enhanced under different background magnetic fields. Using this effect, we demonstrate the detection of subtle magnetic field variations in a strong background, with the system’s response magnified by a factor exceeding 10 and sensitivity increased threefold compared with its conventional Hermitian counterpart. Our study leverages exceptional physics to study the MO effect and develops a new class of reconfigurable MO devices equipped with enhanced sensitivity for potential integration with photonic systems.
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Data availability
The data that support the plots within this paper are available via figshare at https://doi.org/10.6084/m9.figshare.25998517(ref. 60). All other data used in this study are available from the corresponding authors upon reasonable request.
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Acknowledgements
This work was supported by the National Natural Science Foundation of China (grant nos. 92365107, 12334012, 12234012, 12305020, 11935006 and 12421005), the National Key R&D Program of China (grant nos. 2019YFA0308700, 2019YFA0308704, 2022YFA1405000, 2021YFA1400900, 2021YFA0718300 and 2024YFE0102400), the Innovation Program for Quantum Science and Technology (grant nos. 2021ZD0301400 and 2021ZD0301500), the Program for Innovative Talents and Teams in Jiangsu (grant no. JSSCTD202138), the Natural Science Foundation of Jiangsu Province, Major Project (grant no. BK20212004), the Hunan Major Sci-Tech Program (grant no. 2023ZJ1010), the China Postdoctoral Science Foundation (grant no. 2023M731613) and Jiangsu Funding Program for Excellent Postdoctoral Talent (grant no. 2023ZB708). C.-W.Q. acknowledges the support from National Research Foundation (grant no. NRF2021-QEP2-03-P09 with WBS number A-8000708-00-00 and grant no. NRF-CRP26-2021-0004).
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K.X. conceived the original idea and the research, and supervised the project. W.L., H.J., Y.-Q.L. and C.-W.Q. contributed to the idea and co-supervised the project. Y.-P.R. conducted the experiment and performed the data analysis and processing. J.-S.T., Z.L., Y.-P.R., W.L., H.J., C.-W.Q. and K.X. contributed to the theoretical model and interpretation of experimental results. K.X. presented the electric constitutive relation and solely derived the interaction Hamiltonian. H.W., W.Z. and H.Z. contributed to the experimental implementation and details. S.-J.G. and W.H. fabricated the LC cell. J.C., Z.L., Y.-Q.L., W.L., H.J., C.-W.Q. and K.X. developed the underlying physics. Y.-P.R., Z.L., J.C., W.L., H.J., J.-S.T., C.-W.Q. and K.X. contributed to manuscript writing. All authors contributed to discussion of experimental data and results.
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Extended data
Extended Data Fig. 1 Spherical coordinate system for the magnetization M in the (x, y, z)-coordinate.
The angle φ represents the orientation of M with respect to the z axis, and γ is the angle between M projected on the x-y plane and the x axis50.
Extended Data Fig. 2 Verdet constant of the TGG crystal.
Black dots represent the experimental results and red curve represents the fitting from ref. 59.
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Ruan, YP., Tang, JS., Li, Z. et al. Observation of loss-enhanced magneto-optical effect. Nat. Photon. 19, 109–115 (2025). https://doi.org/10.1038/s41566-024-01592-y
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DOI: https://doi.org/10.1038/s41566-024-01592-y