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Single- and two-mode magnon thermal squeezing

Abstract

Squeezed states play a central role in modern precision measurement and information processing, reducing the noise through manipulating its distributions in phase space. Although squeezing has been explored in various physical systems, realization and characterization in magnetic media remain largely unexplored. Here we demonstrate the single-mode thermal squeezing of the magnetization dynamics in an yttrium iron garnet film using microwave parametric excitation. We also demonstrate two-mode thermal squeezing in the form of correlated fluctuations of magnons concentrated on the top and bottom surfaces of the film. Establishing the control of thermal squeezing in magnetic systems provides insights into the fluctuation dynamics of the magnetic order, and represents a key advance in the quest to observe quantum effects in magnetic films.

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Fig. 1: Squeezing of magnetization fluctuations.
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Fig. 2: Observation of single-mode thermal squeezing of magnetization fluctuations.
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Fig. 3: Observation of two-mode squeezing of the magnetization fluctuations.
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Fig. 4: Localization of magnons under non-degenerate parametric excitation.
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Fig. 5: Numerical simulation of magnon modes.
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Data availability

The data that support the findings of this study are available from the corresponding author upon reasonable request. Due to the size of the datasets and the specialized analysis procedures required, they are not publicly available. Source data are provided with this paper.

Code availability

The codes used in theoretical simulations and calculations are available from the corresponding author upon reasonable request.

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Acknowledgements

We thank B. Hillebrands, A. Serga, V. I. Vasyuchka, K. Kobayashi and T. Kikkawa for fruitful discussions. This work was partially supported by JST CREST (JPMJCR20C1 and JPMJCR20T2), JST PRESTO (JPMJPR24F9), JSPS KAKENHI (JP21K13847, JP22K14584, JP22H04965, JP22H04965, JP23KJ0607, JP24H02231, JP24KJ0927, JP24H02231 and JP25K17943), Advanced Technology Institute Research Grants, Support Center for Advanced Telecommunications Technology Research Grants, SCAT Research Grant, Institute for AI and Beyond of the University of Tokyo, and IBM–UTokyo lab.

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Contributions

T.H. designed the experiments. T.H., S.H. and H.S. prepared the sample. T.H and K.T. performed the experiments and T.H. analysed the data. M.E., and G.E.W.B. developed the theory. K.H. and T.M. supported numerical calculation. T.H., M.E., G.E.W.B. and E.S. discussed the interpretation. T.H. wrote the manuscript with input from all authors. E.S. supervised the research. All the authors discussed the results and contents of the manuscript.

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Correspondence to Tomosato Hioki.

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Nature Physics thanks Hossein Taghinejad for their contribution to the peer review of this work. Peer reviewer reports are available.

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Extended data

Extended Data Fig. 1 Correlation measurement procedure.

The input microwave is generated by combining two channels (Ch.1 and Ch.2) into the pump channel (Ch.3) at the pump frequency \({f}_{{\rm{p}}}\) using a multichannel signal generator (Holtzworth 8990B). Ch.1 is used to finely tune the input microwave power with small increments, while Ch.2 is used for harmonic locking at frequency \(2{f}_{2}\). The signals from Ch.2 and Ch.3 are amplified ( + 35 dB) and combined with the output from Ch.1. The resulting microwave signal is delivered to the sample via the main coplanar waveguide (CPW; orange antenna). The AC signal generated from the YIG/Pt disc (orange circle) is detected by a secondary CPW (blue antenna) and routed, via an RF switch, to either the lock-in amplifier circuit or a spectrum analyser (SA). Before entering the lock-in amplifier, the signal is filtered (providing −80 dB attenuation at \(2f\)) to suppress crosstalk, amplified ( + 35 dB), and mixed with a local oscillator signal from Ch.4 of the signal generator. The mixed signal is then fed into a lock-in amplifier (Zurich UHFLI). FMR absorption spectra and spectra during the non-degenerate process are measured by routing the microwave signal to a vector network analyser (VNA) or spectrum analyser (SA) using an additional RF switch.

Extended Data Fig. 2 Evaluation of temperature increase by microwave pumping.

a, Temperature dependence of the resistance of the Pt film. b, Microwave power dependence of the resistance of the Pt film. c, Detuning frequency dependence of variance of \(I(f)\) and \(Q(f)\) plotted with theoretical curve of amplified noise due to non-degenerate parametric amplification.

Source data

Extended Data Fig. 3 Temperature dependence of S parameters and damping.

a, Temperature dependence of the microwave absorption spectrum (S11). b, Numerically calculated magnon intensity at 31.93 mT at T = 300 K. The calculation was performed for a magnetic disc with a diameter of 100 μm and a thickness of 1.6 μm, using the same material parameters as those used to obtain Fig. 5a–c. c, Magnetic field dependence of microwave absorption spectrum, d, Frequency dependence of microwave absorption spectrum up to 5 GHz, e, Temperature dependence of intrinsic Gilbert damping constant. All data were obtained from repeated measurements (n = 10) of the same sample under identical conditions. These measurements correspond to technical replicates. Error bars represent standard deviation (SD) of the data. Data are presented as mean ± SD.

Source data

Extended Data Fig. 4 Schematics of magnetization dynamics under parametric pumping.

a,b, Schematics of magnetization precession component and AC magnetic field when phase-matching conditions are satisfied. c, Snapshots of the elliptical magnetization (M) precession under an ac magnetic field (bac, pink arrows) and its torque (light blue arrows) that enforce or suppress the torques by the dc magnetic field \(-\gamma {\bf{M}}\times {\bf{B}}\) (black arrows). d, Top view of magnetization precession without AC magnetic field. e, Top view of magnetization precession under parametric pumping as in c. The torque arrow due to AC magnetic field (light blue) directs the same direction as \({\dot{M}}_{Y}\) when \({M}_{Y}\) takes maximum or minimum, while it directs the opposite when \({M}_{Y}=0\), leading to smaller noise along\({M}_{Y}\) and larger noise in \({M}_{X}\).

Extended Data Fig. 5 Two-mode Wigner function below and above threshold.

a,b, Single-mode Wigner functions measured at frequencies \({f}_{1}\) and \({f}_{2}\) at a pump power P = 28.6 mW below the parametric pumping threshold at 220 K under B = 30.14 mT. c,d, Two-mode Wigner functions of the I and Q quadratures measured at the same power as in a,b. e,f, Single-mode Wigner functions measured at \({f}_{1}\) and \({f}_{2}\) for P = 29.1 mW above the threshold. g,h, Two-mode Wigner functions of the I and Q quadratures measured at P = 29.1 mW.

Extended Data Fig. 6 Temperature dependence of two-mode thermal squeezing.

a,d,g, Power dependence of noise intensity (bandwidth = 19 kHz) measured at 300 K at B = 29.84 mT (a), 260 K at B = 30.00 mT (d) and 220 K at B = 30.15 mT, (g). b,e,h, Wigner functions representing correlations between the I (in-phase) components near the nondegenerate parametric excitation threshold at 300 K (b), 260 K (e), and 220 K (h). c,f,i, Wigner functions representing correlations between the Q (quadrature) components near the nondegenerate parametric excitation threshold at 300 K (c), 260 K (f), and 220 K (i).

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Supplementary Figs. 1–12, Sections 1–14 and Table 1.

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Hioki, T., Tojo, K., Elyasi, M. et al. Single- and two-mode magnon thermal squeezing. Nat. Phys. (2026). https://doi.org/10.1038/s41567-026-03294-4

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