Abstract
Collective excitations presenting nonlinear dynamics are fundamental phenomena with broad applications. A prime example is nonlinear optics, where diverse frequency-mixing processes are central to communication and attosecond science, and extreme (>sixth-order) harmonic generation provides broad wavelength conversion. Leveraging recent progress in van der Waals magnetic semiconductors, we demonstrate nonlinear optomagnonic coupling. In the layered antiferromagnetic semiconductor CrSBr, we observe exciton states dressed by up to 20 harmonics of magnons, resulting from their extreme nonlinearities. We also create tunable optical sidebands via sum- and difference-frequency generation between two optically bright magnon modes under symmetry-breaking magnetic fields. Moreover, we can tune the observed difference-frequency generation mode into resonance with one of the fundamental magnons, which results in parametric amplification of magnons. Our findings realize the modulation of the optical-frequency exciton with the extreme nonlinearity of magnons at microwave frequencies, which could find applications in magnonics and hybrid quantum systems, and provide a method for optomagnonic neuromorphic computing devices.
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Data availability
The datasets generated during and/or analysed during this study are provided with this paper. All other data that support the plots within this paper and other findings of this study are available from the corresponding author upon reasonable request. Source data are provided with this paper.
References
Cramer, J. et al. Magnon detection using a ferroic collinear multilayer spin valve. Nat. Commun. 9, 1089 (2018).
Chumak, A. V. et al. Advances in magnetics roadmap on spin-wave computing. IEEE Trans. Magn. 58, 0800172 (2022).
Pirro, P., Vasyuchka, V. I., Serga, A. A. & Hillebrands, B. Advances in coherent magnonics. Nat. Rev. Mater. 6, 1114–1135 (2021).
Zheng, S. et al. Tutorial: nonlinear magnonics. J. Appl. Phys. 134, 151101 (2023).
Flebus, B., Rezende, S. M., Grundler, D. & Barman, A. Recent advances in magnonics. J. Appl. Phys. 133, 160401 (2023).
Lachance-Quirion, D., Tabuchi, Y., Gloppe, A., Usami, K. & Nakamura, Y. Hybrid quantum systems based on magnonics. Appl. Phys. Express 12, 070101 (2019).
Bae, Y. J. et al. Exciton-coupled coherent magnons in a 2D semiconductor. Nature 609, 282–286 (2022).
Diederich, G. M. et al. Tunable interaction between excitons and hybridized magnons in a layered semiconductor. Nat. Nanotechnol. 18, 23–28 (2023).
Först, M. et al. Nonlinear phononics as an ultrafast route to lattice control. Nat. Phys. 7, 854–856 (2011).
Chumak, A. V., Serga, A. A. & Hillebrands, B. Magnon transistor for all-magnon data processing. Nat. Commun. 5, 4700 (2014).
Rodrigues, D. R. et al. Nonlinear dynamics of topological ferromagnetic textures for frequency multiplication. Phys. Rev. Appl. 16, 014020 (2021).
Schubert, O. et al. Sub-cycle control of terahertz high-harmonic generation by dynamical Bloch oscillations. Nat. Photon. 8, 119–123 (2014).
Demidov, V. E. et al. Generation of the second harmonic by spin waves propagating in microscopic stripes. Phys. Rev. B 83, 054408 (2011).
Hermsdoerfer, S. J. et al. A spin-wave frequency doubler by domain wall oscillation. Appl. Phys. Lett. 94, 223510 (2009).
Zhang, Z. et al. Terahertz-field-driven magnon upconversion in an antiferromagnet. Nat. Phys. 20, 788–793 (2024).
Zhang, Z. et al. Terahertz field-induced nonlinear coupling of two magnon modes in an antiferromagnet. Nat. Phys. 20, 801–806 (2024).
Telford, E. J. et al. Coupling between magnetic order and charge transport in a two-dimensional magnetic semiconductor. Nat. Mater. 21, 754–760 (2022).
Telford, E. J. et al. Layered antiferromagnetism induces large negative magnetoresistance in the van der Waals semiconductor CrSBr. Adv. Mater. 34, 2205639 (2020).
Wilson, N. P. et al. Interlayer electronic coupling on demand in a 2D magnetic semiconductor. Nat. Mater. 20, 1657–1662 (2021).
Sun, Y. et al. Dipolar spin wave packet transport in a van der Waals antiferromagnet. Nat. Phys. 20, 794–800 (2024).
Dirnberger, F. et al. Magneto-optics in a van der Waals magnet tuned by self-hybridized polaritons. Nature 620, 533–537 (2023).
Huang, C. et al. Extreme terahertz magnon multiplication induced by resonant magnetic pulse pairs. Nat. Commun. 15, 3214 (2024).
Kapteyn, H. C., Murnane, M. M. & Christov, I. P. Extreme nonlinear optics: coherent X rays from lasers. Phys. Today 58, 39–46 (2005).
Lee, K. et al. Magnetic order and symmetry in the 2D semiconductor CrSBr. Nano Lett. 21, 3511–3517 (2021).
Cham, T. M. J. et al. Anisotropic gigahertz antiferromagnetic resonances of the easy-axis van der Waals antiferromagnet CrSBr. Nano Lett. 22, 6716–6723 (2022).
MacNeill, D. et al. Gigahertz frequency antiferromagnetic resonance and strong magnon–magnon coupling in the layered crystal CrCl3. Phys. Rev. Lett. 123, 047204 (2019).
Ferray, M. et al. Multiple-harmonic conversion of 1064 nm radiation in rare gases. J. Phys. B 21, L31 (1988).
Ghimire, S. et al. Observation of high-order harmonic generation in a bulk crystal. Nat. Phys 7, 138–141 (2011).
Boyd, R. W. Nonlinear Optics (Academic, 2008).
Kamimaki, A., Iihama, S., Suzuki, K. Z., Yoshinaga, N. & Mizukami, S. Parametric amplification of magnons in synthetic antiferromagnets. Phys. Rev. Appl. 13, 044036 (2020).
Fu, H., Huang, K., Watanabe, K., Taniguchi, T. & Zhu, J. Gapless spin wave transport through a quantum canted antiferromagnet. Phys. Rev. X 11, 021012 (2021).
Koerner, C. et al. Frequency multiplication by collective nanoscale spin-wave dynamics. Science 375, 1165–1169 (2022).
Pawbake, A. et al. Raman scattering signatures of strong spin–phonon coupling in the bulk magnetic van der Waals material CrSBr. Phys. Rev. B 107, 075421 (2023).
Fiebig, M., Pavlov, V. V. & Pisarev, R. V. Second-harmonic generation as a tool for studying electronic and magnetic structures of crystals: review. J. Opt. Soc. Am. B 22, 96–118 (2005).
Bai, Y. et al. High-harmonic generation from topological surface states. Nat. Phys. 17, 311–315 (2021).
Li, X. F., L’Huillier, A., Ferray, M., Lompré, L. A. & Mainfray, G. Multiple-harmonic generation in rare gases at high laser intensity. Phys. Rev. A 39, 5751–5761 (1989).
Jungwirth, T., Marti, X., Wadley, P. & Wunderlich, J. Antiferromagnetic spintronics. Nat. Nanotechnol. 11, 231–241 (2016).
Au, Y. et al. Resonant microwave-to-spin-wave transducer. Appl. Phys. Lett. 100, 182404 (2012).
Roslyak, O. & Mukamel, S. Photon entanglement signatures in difference-frequency-generation. Opt. Express 17, 1093–1106 (2009).
Acknowledgements
We thank L. Fu, M. Rudner and G. Refael for discussions. This work was mainly supported by the Department of Energy, Basic Energy Sciences, Materials Sciences and Engineering Division (DE-SC0012509). Sample fabrication and optical measurements are partially supported by AFOSR FA9550-19-1-0390 and FA9550-21-1-0460. Synthesis of the CrSBr crystals is supported by the NSF MRSEC on Precision-Assembled Quantum Materials (DMR-2011738). Structural and magnetic characterization measurements were conducted as part of the Programmable Quantum Materials, an Energy Frontier Research Center, funded by the US Department of Energy (DOE), Office of Science, Basic Energy Sciences, under award DE-SC0019443. X.X. acknowledges support from the State of Washington-funded Clean Energy Institute and from the Boeing Distinguished Professorship in Physics.
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X.X., D.X., Y.R. and G.M.D. conceived the project. G.M.D. performed the measurements with help from M.N., S.P., J.C. and J.F. M.N., S.P. and J.C. fabricated the samples. G.M.D., M.N., J.C., Y.J.B., X.Z., Y.R., D.X. and X.X. analysed the data and interpreted the results. Y.R. and D.X. built the model and performed the simulations. D.G.C. and X.R. grew the CrSBr crystals. G.M.D., M.N., X.Z., Y.R., D.X. and X.X. wrote the manuscript with input from all authors. All authors discussed the results.
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Extended data
Extended Data Fig. 1 Field dependent transient reflectivity data.
a, Raw transient reflectivity data corresponding to the spectrum presented in Fig. 1d. b, Linecut taken from (a) at µoH ≈ 0.45 T. c, Same data as in (a) with the exponential decay removed. d, Linecut taken from (c) at µoH ≈ 0.45 T.
Extended Data Fig. 2 Magnon HHG under c axis field.
a, Transient reflectivity data from CrSBr under a field applied along the c (hard) crystal (magnetic) axis. b, Corresponding magnon spectrum presenting the first few harmonic orders.
Extended Data Fig. 3 Field angle dependent transient reflectivity data.
a, Raw transient optical reflectivity data corresponding to the spectrum presented in Fig. 3a. b, Same data as in (a) with the exponential decay removed.
Extended Data Fig. 4 Comparison of field angle dependent data with simulations.
a, Same measured magnon spectrum presented in Fig. 3b. b, Simulated magnon spectrum. c, Additional dataset showing the DFG mode at positive and negative field angles.
Extended Data Fig. 5 HHG spectrum from an additional CrSBr sample.
a, Magnon spectrum presenting HHG from a ~ 90 nm thick flake, roughly half the thickness of the sample shown in the main text.
Extended Data Fig. 6 Model calculation of HHG.
The amplitude of the Fourier components as a function of frequency is shown. The amplitude first decays, then reaches a plateau, and then decays again. Both even and odd harmonics exist. The model parameters used to produce this spectrum are ω = 1 = 10ω0, v3 = 1, \({v}_{4}=\frac{1}{2}\), Γ = 10, and F(t) = 0.5sin (ω0t).
Source data
Source Data Fig. 1
Raw transient reflectivity data for Fig. 1.
Source Data Fig. 2
Raw transient reflectivity data and numerical data for Fig. 2.
Source Data Fig. 3
Raw transient reflectivity data for Fig. 3.
Source Data Fig. 4
Raw transient reflectivity data for Fig. 4.
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Diederich, G.M., Nguyen, M., Cenker, J. et al. Exciton dressing by extreme nonlinear magnons in a layered semiconductor. Nat. Nanotechnol. 20, 617–622 (2025). https://doi.org/10.1038/s41565-025-01890-8
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DOI: https://doi.org/10.1038/s41565-025-01890-8
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