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Subterahertz collective dynamics of polar vortices

Abstract

The collective dynamics of topological structures1,2,3,4,5,6 are of interest from both fundamental and applied perspectives. For example, studies of dynamical properties of magnetic vortices and skyrmions3,4 have not only deepened our understanding of many-body physics but also offered potential applications in data processing and storage7. Topological structures constructed from electrical polarization, rather than electron spin, have recently been realized in ferroelectric superlattices5,6, and these are promising for ultrafast electric-field control of topological orders. However, little is known about the dynamics underlying the functionality of such complex extended nanostructures. Here, using terahertz-field excitation and femtosecond X-ray diffraction measurements, we observe ultrafast collective polarization dynamics that are unique to polar vortices, with orders-of-magnitude higher frequencies and smaller lateral size than those of experimentally realized magnetic vortices3. A previously unseen tunable mode, hereafter referred to as a vortexon, emerges in the form of transient arrays of nanoscale circular patterns of atomic displacements, which reverse their vorticity on picosecond timescales. Its frequency is considerably reduced (softened) at a critical strain, indicating a condensation (freezing) of structural dynamics. We use first-principles-based atomistic calculations and phase-field modelling to reveal the microscopic atomic arrangements and corroborate the frequencies of the vortex modes. The discovery of subterahertz collective dynamics in polar vortices opens opportunities for electric-field-driven data processing in topological structures with ultrahigh speed and density.

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Fig. 1: Emergence of the collective dynamics of polar vortices and its experimental detection.
Fig. 2: High-frequency collective modes.
Fig. 3: Tunable vortexon mode.
Fig. 4: Atomistic calculation and dynamical phase-field simulation.

Data availability

The data that support the findings of this study are available from the corresponding author upon request.

Code availability

The codes that support the findings of this study are available from the corresponding author upon request.

References

  1. 1.

    Naumov, I. I., Bellaiche, L. & Fu, H. Unusual phase transitions in ferroelectric nanodisks and nanorods. Nature 432, 737–740 (2004).

    ADS  CAS  PubMed  Google Scholar 

  2. 2.

    Huang, F.-T. & Cheong, S.-W. Aperiodic topological order in the domain configurations of functional materials. Nat. Rev. Mater. 2, 17004 (2017).

    ADS  Google Scholar 

  3. 3.

    Choe, S.-B. et al. Vortex core-driven magnetization dynamics. Science 304, 420–422 (2004).

    ADS  CAS  PubMed  Google Scholar 

  4. 4.

    Büttner, F. et al. Dynamics and inertia of skyrmionic spin structures. Nat. Phys. 11, 225–228 (2015).

    Google Scholar 

  5. 5.

    Yadav, A. K. et al. Observation of polar vortices in oxide superlattices. Nature 530, 198–201 (2016).

    ADS  CAS  Google Scholar 

  6. 6.

    Das, S. et al. Observation of room-temperature polar skyrmions. Nature 568, 368–372 (2019).

    ADS  CAS  PubMed  Google Scholar 

  7. 7.

    Nagaosa, N. & Tokura, Y. Topological properties and dynamics of magnetic skyrmions. Nat. Nanotechnol. 8, 899–911 (2013).

    ADS  CAS  PubMed  Google Scholar 

  8. 8.

    Yadav, A. K. et al. Spatially resolved steady-state negative capacitance. Nature 565, 468–471 (2019).

    ADS  CAS  PubMed  Google Scholar 

  9. 9.

    Íñiguez, J., Zubko, P., Luk’yanchuk, I. & Cano, A. Ferroelectric negative capacitance. Nat. Rev. Mater. 4, 243–256 (2019).

    ADS  Google Scholar 

  10. 10.

    Stoica, V. A. et al. Optical creation of a supercrystal with three-dimensional nanoscale periodicity. Nat. Mater. 18, 377–383 (2019).

    ADS  CAS  PubMed  Google Scholar 

  11. 11.

    Büttner, F., Lemesh, I. & Beach, G. S. D. Theory of isolated magnetic skyrmions: from fundamentals to room temperature applications. Sci. Rep. 8, 4464 (2018).

    ADS  PubMed  PubMed Central  Google Scholar 

  12. 12.

    Seidel, J. Domain walls as nanoscale functional elements. J. Phys. Chem. Lett. 3, 2905–2909 (2012).

    CAS  Google Scholar 

  13. 13.

    Gu, Z. et al. Resonant domain-wall-enhanced tunable microwave ferroelectrics. Nature 560, 622–627 (2018).

    ADS  CAS  PubMed  Google Scholar 

  14. 14.

    Cochard, C., Spielmann, T. & Granzow, T. Dielectric tunability of ferroelectric barium titanate at millimeter-wave frequencies. Phys. Rev. B 100, 184104 (2019).

    ADS  CAS  Google Scholar 

  15. 15.

    Catalan, G., Seidel, J., Ramesh, R. & Scott, J. F. Domain wall nanoelectronics. Rev. Mod. Phys. 84, 119–156 (2012).

    ADS  CAS  Google Scholar 

  16. 16.

    Wu, X. et al. Low-energy structural dynamics of ferroelectric domain walls in hexagonal rare-earth manganites. Sci. Adv. 3, e1602371 (2017).

    ADS  PubMed  PubMed Central  Google Scholar 

  17. 17.

    Luk’yanchuk, I., Sené, A. & Vinokur, V. M. Electrodynamics of ferroelectric films with negative capacitance. Phys. Rev. B 98, 024107 (2018).

    ADS  Google Scholar 

  18. 18.

    Hlinka, J., Paściak, M., Körbel, S. & Marton, P. Terahertz-range polar modes in domain-engineered BiFeO3. Phys. Rev. Lett. 119, 057604 (2017).

    ADS  Google Scholar 

  19. 19.

    Gui, Z. & Bellaiche, L. Terahertz dynamics of ferroelectric vortices from first principles. Phys. Rev. B 89, 064303 (2014).

    ADS  Google Scholar 

  20. 20.

    Zhang, Q., Herchig, R. & Ponomareva, I. Nanodynamics of ferroelectric ultrathin films. Phys. Rev. Lett. 107, 177601 (2011).

    ADS  Google Scholar 

  21. 21.

    Ogawa, N., Seki, S. & Tokura, Y. Ultrafast optical excitation of magnetic skyrmions. Sci. Rep. 5, 9552 (2015).

    ADS  CAS  PubMed  PubMed Central  Google Scholar 

  22. 22.

    Hong, Z. et al. Stability of polar vortex lattice in ferroelectric superlattices. Nano Lett. 17, 2246–2252 (2017).

    ADS  CAS  PubMed  Google Scholar 

  23. 23.

    Scott, J. F. Soft-mode spectroscopy: experimental studies of structural phase transitions. Rev. Mod. Phys. 46, 83–128 (1974).

    ADS  CAS  Google Scholar 

  24. 24.

    Li, X. et al. Terahertz field-induced ferroelectricity in quantum paraelectric SrTiO3. Science 364, 1079–1082 (2019).

    ADS  CAS  PubMed  Google Scholar 

  25. 25.

    Nova, T. F., Disa, A. S., Fechner, M. & Cavalleri, A. Metastable ferroelectricity in optically strained SrTiO3. Science 364, 1075–1079 (2019).

    ADS  CAS  PubMed  Google Scholar 

  26. 26.

    Bargheer, M. et al. Coherent atomic motions in a nanostructure studied by femtosecond X-ray diffraction. Science 306, 1771–1773 (2004).

    ADS  CAS  PubMed  Google Scholar 

  27. 27.

    Zhu, H. et al. Observation of chiral phonons. Science 359, 579–582 (2018).

    ADS  MathSciNet  CAS  PubMed  Google Scholar 

  28. 28.

    Qi, T., Shin, Y.-H., Yeh, K.-L., Nelson, K. & Rappe, A. Collective coherent control: synchronization of polarization in ferroelectric PbTiO3 by shaped THz fields. Phys. Rev. Lett. 102, 247603 (2009).

    ADS  PubMed  Google Scholar 

  29. 29.

    Chen, F. et al. Ultrafast terahertz-field-driven ionic response in ferroelectric BaTiO3. Phys. Rev. B 94, 180104 (2016).

    ADS  Google Scholar 

  30. 30.

    Kozina, M. et al. Terahertz-driven phonon upconversion in SrTiO3. Nat. Phys. 15, 387–392 (2019).

    CAS  Google Scholar 

  31. 31.

    Kubacka, T. et al. Large-amplitude spin dynamics driven by a THz pulse in resonance with an electromagnon. Science 343, 1333–1336 (2014).

    ADS  CAS  PubMed  Google Scholar 

  32. 32.

    Damodaran, A. R. et al. Phase coexistence and electric-field control of toroidal order in oxide superlattices. Nat. Mater. 16, 1003–1009 (2017).

    ADS  CAS  PubMed  Google Scholar 

  33. 33.

    Li, Q. et al. Quantification of flexoelectricity in PbTiO3/SrTiO3 superlattice polar vortices using machine learning and phase-field modeling. Nat. Commun. 8, 1468 (2017).

    ADS  CAS  PubMed  PubMed Central  Google Scholar 

  34. 34.

    Yang, T., Wang, B., Hu, J.-M. & Chen, L.-Q. Domain dynamics under ultrafast electric-field pulses. Phys. Rev. Lett. 124, 107601 (2020).

    ADS  CAS  PubMed  Google Scholar 

  35. 35.

    Trigo, M. et al. Probing unfolded acoustic phonons with X rays. Phys. Rev. Lett. 101, 025505 (2008).

    ADS  CAS  PubMed  Google Scholar 

  36. 36.

    Zhang, L. & Niu, Q. Angular momentum of phonons and the Einstein–de Haas effect. Phys. Rev. Lett. 112, 085503 (2014).

    ADS  Google Scholar 

  37. 37.

    von Hoegen, A., Mankowsky, R., Fechner, M., Först, M. & Cavalleri, A. Probing the interatomic potential of solids with strong-field nonlinear phononics. Nature 555, 79–82 (2018).

    ADS  Google Scholar 

  38. 38.

    Tamura, S., Hurley, D. C. & Wolfe, J. P. Acoustic-phonon propagation in superlattices. Phys. Rev. B 38, 1427–1449 (1988).

    ADS  CAS  Google Scholar 

  39. 39.

    Daranciang, D. et al. Ultrafast photovoltaic response in ferroelectric nanolayers. Phys. Rev. Lett. 108, 087601 (2012).

    ADS  PubMed  Google Scholar 

  40. 40.

    Chollet, M. et al. The X-ray Pump–Probe instrument at the Linac Coherent Light Source. J. Synchrotron Radiat. 22, 503–507 (2015).

    CAS  PubMed  PubMed Central  Google Scholar 

  41. 41.

    Kozina, M. et al. Ultrafast X-ray diffraction probe of terahertz field-driven soft mode dynamics in SrTiO3. Struct. Dyn. 4, 054301 (2017).

    CAS  PubMed  PubMed Central  Google Scholar 

  42. 42.

    Sato, T. et al. A simple instrument to find spatiotemporal overlap of optical/X-ray light at free-electron lasers. J. Synchrotron Radiat. 26, 647–652 (2019).

    CAS  PubMed  PubMed Central  Google Scholar 

  43. 43.

    Glownia, J. M. et al. Pump–probe experimental methodology at the Linac Coherent Light Source. J. Synchrotron Radiat. 26, 685–691 (2019).

    CAS  PubMed  PubMed Central  Google Scholar 

  44. 44.

    Sepliarsky, M., Asthagiri, A., Phillpot, S. R., Stachiotti, M. G. & Migoni, R. L. Atomic-level simulation of ferroelectricity in oxide materials. Curr. Opin. Solid State Mater. Sci. 9, 107–113 (2005).

    ADS  CAS  Google Scholar 

  45. 45.

    Sepliarsky, M. & Cohen, R. E. First-principles based atomistic modeling of phase stability in PMN–xPT. J. Phys. Condens. Matter 23, 435902 (2011).

    ADS  CAS  PubMed  Google Scholar 

  46. 46.

    Stachiotti, M. G. & Sepliarsky, M. Toroidal ferroelectricity in PbTiO3 nanoparticles. Phys. Rev. Lett. 106, 137601 (2011).

    ADS  CAS  PubMed  Google Scholar 

  47. 47.

    Gale, J. D. & Rohl, A. L. The General Utility Lattice Program (GULP). Mol. Simul. 29, 291–341 (2003).

    CAS  MATH  Google Scholar 

Download references

Acknowledgements

We acknowledge discussions with M. Trigo, D. Xiao, Z. Hong, I. Luk’yanchuk and V. M. Vinokur. This work was primarily supported by the US Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division: experimental design, data collection, data analysis, and part of simulations by Q.L. and H.W. were supported under the DOE Early Career Award; ultrafast measurements and sample synthesis by V.A.S., Y.Y., S.P., L.W.M., C.D., S.Y., A.L., L.-Q.C., V.G., J.W.F. and H.W. were supported under award no. DE-SC-0012375; ancillary ultrafast X-ray measurements by H.L., S.M., Y.A. and P.E. were supported under award no. DE-FG02-04ER46147. M.M., S.D., and R.R. acknowledge support for part of sample synthesis through the Quantum Materials programme (KC 2202) funded by the US Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences Division under contract no. DE-AC02-05-CH11231. J.H. and M.P. were supported by the Czech Science Foundation (project no. 19-28594X) and acknowledge the access to computing facilities owned by parties and projects contributing to the National Grid Infrastructure MetaCentrum, provided under programme no. Cesnet LM2015042. T.Y. and L.-Q.C. acknowledge partial support from the US Department of Energy, Office of Science, Basic Energy Sciences, under award n0. DE-SC0020145 as part of the Computational Materials Sciences Program and from NSF under award DMR-1744213. Y.Z. and H.W. acknowledge support by ANL-LDRD for preliminary X-ray measurements. Q.L. acknowledges support by the Basic Science Center Project of NSFC under grant no. 51788104 for completing phase-field simulations at Tsinghua University. S.M. acknowledges support from the Office of Science Graduate Student Research (SCGSR) programme (DOE contract no. DE‐SC0014664) and from the UW-Madison Materials Research Science and Engineering Center (NSF DMR-1720415). H.L. acknowledges support by the National Research Foundation of Korea under grant 2017R1A6A3A11030959. Use of the Linac Coherent Light Source is supported by the US Department of Energy, Office of Science, Office of Basic Energy Sciences under contract no. DE-AC02-76SF00515. Use of the Advanced Photon Source is supported by the US Department of Energy, Office of Science, Office of Basic Energy Sciences under contract no. DE-AC02–06CH11357.

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Contributions

Q.L., V.A.S., Y.Y., M.R.M., S.P., H.J.L., Y.A., S.D.M., T.S., M.C.H., M.C., M.E.K., S.N., D.Z., A.M.L., P.G.E., V.G., J.W.F. and H.W. performed the experiment at the Linac Coherent Light Source. Y.Z., V.A.S., D.A.W. and H.W. performed preliminary experiments at the Advanced Photon Source. M.P. and J.H. performed atomistic modelling. Q.L., C.D., T.Y. and L.-Q.C. performed phase-field simulation. T.Y., L.-Q.C. and. J.H. developed the analytical model. S.D., M.R.M., A.K.Y., L.W.M. and R.R. prepared the samples. S.Y. and C.K. performed THz spectroscopy measurements. Q.L. and H.W. wrote the manuscript with input from all authors. H.W. conceived and supervised the project.

Corresponding author

Correspondence to Haidan Wen.

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Peer review information Nature thanks Igor Luk’yanchuk, Daniel Schick and the other, anonymous, reviewer(s) for their contribution to the peer review of this work.

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Extended data figures and tables

Extended Data Fig. 1 Diffraction patterns of probed Bragg peaks and the corresponding diffraction geometry.

a, Diffraction patterns of 023, 113 and 004 peaks in logarithmic scale as recorded by a two-dimensional X-ray area detector. The projected q-axis labels indicate the approximate directions in reciprocal space. b, Schematics of diffraction geometry for probing the 023, 113 and 004 peaks. The dashed circle represents the horizontal plane. The red and blue stripes represent vortex structure with opposite vorticities. The THz field is polarized vertically.

Extended Data Fig. 2 The response of the FE (a1/a2) structure upon THz field excitation.

a, 3D schematic of diffraction peaks of the film around the 023 or 113 substrate peaks in reciprocal space. The dashed arrows indicate the reciprocal axes through the centres of the FE or vortex SL peaks that are offset along the qy-axis owing to the lattice constant difference along the y-axis. Only two SL and their satellite peaks are shown for simplicity. b, Normalized change of diffraction intensity of the 113 FE satellite peak (red curve) measured at the delay of 4 ps indicated by the red arrow in e, and normalized change of diffraction intensity of the 004 FE SL peak (blue curve) measured at the delay of 35 ps indicated by the blue arrow in g, as a function of the applied THz peak field. Lines are linear and quadratic fits to the measured data, in agreement with the field-driven structure factor modulation and the THz-induced Bragg peak shift (heating), respectively. c, Rocking curve of 023 FE SL peak. d, Normalized change of diffraction intensity as a function of delay measured at various incident angles indicated by the magenta, grey and blue arrows in c. e, Normalized change of diffraction intensity of the 113 FE SL peak and its satellites as a function of delay. The curves are vertically offset for clarity. f, Fourier spectra of e. g, Normalized change of diffraction intensity as a function of delay measured at the lower-angle side of the 004 FE SL peaks, indicated by the green arrow in h. h, Rocking curves of 004 FE SL peak measured at the delay of 35 ps with and without THz excitation. The peak shift shows a strain of 2.5 × 10−5, corresponding to a 2 K temperature rise as calibrated by the temperature-dependent X-ray diffraction measurements shown in Extended Data Fig. 7b.

Extended Data Fig. 3 The dielectric properties of vortex structures as a function of strain and frequency from atomistic calculations.

a, Frequency–strain diagram with the diagonal oscillator strength (Sii) of each mode reflected in the size of the markers (the area is proportional to log(Sii + 1 THz2)), where i represents x, y or z. The dielectric strength of the mth mode (\(\Delta {{\epsilon }}_{ii,m}\)) is directly related to the oscillator strength via \(\Delta {{\epsilon }}_{ii,m}={S}_{ii,m}/{\omega }_{m}^{2}\), where ωm is the mode’s frequency. The 15 lowest-frequency modes are considered; the zz signal is multiplied 5 times for better visibility. The orange area indicates the high-frequency regime. b, Frequency-dependent permittivity for two different strain values, εx = −0.25% and 0.2%. The imaginary part is presented in the main plots, while the left-hand insets show diagonal components \({{\epsilon }}_{xx}^{{\prime\prime} }\), \({{\epsilon }}_{yy}^{{\prime\prime} }\), \({{\epsilon }}_{zz}^{{\prime\prime} }\) and the right-hand insets present off-diagonal spectra \({{\epsilon }}_{xy}^{{\prime\prime} }\), \({{\epsilon }}_{xz}^{{\prime\prime} }\), \({{\epsilon }}_{yz}^{{\prime\prime} }\). The arrows indicate modes that are analysed in the Extended Data Fig. 4. All dielectric properties are calculated for the PTO layer only.

Extended Data Fig. 4 Decomposition of selected modes with strain εx = −0.25% in the atomistic model.

The modes are characterized by the highest oscillator strengths in the x-direction (below the frequency of 0.41 THz, marked by the arrows in Extended Data Fig. 3b), and the first two of them are also described in the main text. ad, Each column contains microscopic configurations at t = τ/4 of (a) Pb and Ti displacements; (b) O displacements of the mode’s eigenvectors; (c) change in polarization caused by these atomic displacements (overlaid on a \(\nabla \times {\bf{P}}\) map of the equilibrium structure); (d) polarization patterns and the respective \(\nabla \times {\bf{P}}\) map of a structure subjected to the mode’s perturbation. The origin O and vector R in a are related to the calculation of the angular momentum of the vortexon in the boxed region detailed in Supplementary Note 1B. The displacement vectors are scaled arbitrarily, while perturbed (P) configurations are calculated for maximum ionic displacements of 30 pm. We note that there are additional modes with the y-component of the oscillator strength that contribute to the diversity of the collective dynamics in the frequency range 0.3–0.4 THz.

Extended Data Fig. 5 Polarization dependent response and analysis of the vortexon mode.

a, Normalized change of diffraction intensity of 004 vortex Bragg peak as a function of time when the THz field is applied parallel to and perpendicular to the crystalline x-axis. b, Baseline-subtracted normalized change of diffraction intensity of the 004 vortex superlattice peak (red curve) as a function delay. Raw data shown in grey are from Fig. 4b. The green curve shows a sinusoidal wave (see Supplementary Note 5), with its minima (green arrows) deviating from the data (red arrows) at later times. The vertical dashed line indicates the time when the THz field turns on.

Extended Data Fig. 6 Dynamical phase-field simulation results.

a, b, Fourier transform of the simulated polarization dynamics, which is represented by spatially averaged (a) \({P}_{z}^{2}\) and (b) \({P}_{x}^{2}\) in the simulation box on application of the THz-field pulse aligned along the x-, y- or z-axis. c, Calculated frequency spectra of \({P}_{x}^{2}\) with various values of the direct-current (DC) electric field along the x-axis. d, Frequency and amplitude of the vortexon mode as a function of the applied electric field (Ex). Such an in-plane electric field can be applied using a pair of coplanar electrodes, as schematically shown in the inset to d. e, Histograms of the Pb and Sr ionic displacement u away from its equilibrium positions along the x- and z-axes, corresponding to the maximum diffraction intensity change of 4% of 004 SL peak at a delay of 9 ps in the simulation.

Extended Data Fig. 7 Equilibrium characterizations of (PbTiO3)16/(SrTiO3)16 superlattice.

a, Room-temperature RSM of the superlattice grown on DSO substrate, cutting through the substrate specular 004 peak, which shows vortex (V) and FE superlattice diffraction peaks in the qxqz plane. The satellites (V Sat) due to the in-plane vortex ordering appear along the qx direction around the corresponding superlattice (V) peaks. b, The measured average lattice parameters with linear fits for the vortex and FE structures as a function of temperature. The error bars represent systematic errors of the measurement. c, Room-temperature RSM of the superlattice grown on Sr2Al0.3Ga0.7TaO6 (SAGT) substrate, cutting through the substrate specular 002 peak, which shows the vortex SL diffraction peaks and satellites. d, Room-temperature imaginary dielectric constant extracted from the THz time-domain absorption spectroscopy measurements of superlattices grown on DSO and SAGT substrates. The error bars represent the estimated experimental errors in the frequency ranges of the shaded and unshaded regimes.

Extended Data Fig. 8 X-ray diffraction simulations based on dynamical phase-field modelling.

a, Model geometry of the PTO/STO superlattice film and the DSO substrate. The colour scale denotes the vorticity of the polarization vectors. The boundary conditions (Methods) are marked on the right. b, Schematics for the method used to map the phase-field modelling output to atomistic configurations, based on which kinematic X-ray scattering intensities are calculated (Supplementary Note 2). CoM, center ofmass; V and C denote the vortex and cubic phases of PbTiO3, respectively. c, Measured and simulated H0L-cut (along the qxqz plane in reciprocal lattice units (r.l.u)) RSMs near the 004 reflection with the intensity shown on a logarithmic colour scale. The fringes in the simulated RSM are due to the finite lateral size of the simulation box.

Extended Data Fig. 9 Structural dynamics excited by 400-nm optical pulses.

a, Normalized changes of 004-vortex peak intensity as a function delay. b, Fourier spectra of a. L and T represent the acoustic waves that travel along the out-of-plane direction with longitudinal and transverse sound speeds, respectively. c, Calculated phonon dispersion curves. The vertical dashed line indicates the boundary of the folded Brillouin zones. The shaded region corresponds to the scattering vectors probed in the experiment. The solid circles show the measured modes upon 400-nm excitation, while the stars show the measured modes upon THz excitation. The error bars show the full-width at half-maximum of the peaks in the Fourier spectra. dSL, superlattice periodicity.

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This file contains Supplementary text, Supplementary Notes 1 to 7, Supplementary Tables 1 – 3 and Supplementary References.

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Li, Q., Stoica, V.A., Paściak, M. et al. Subterahertz collective dynamics of polar vortices. Nature 592, 376–380 (2021). https://doi.org/10.1038/s41586-021-03342-4

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