Abstract
Quantum light–matter interactions of bound electron systems have been studied extensively. By contrast, quantum interactions of free electrons with light have only become accessible in recent years, following the discovery of photon-induced near-field electron microscopy (PINEM). So far, the fundamental free electron–light interaction in all PINEM experiments has remained weak due to its localized near-field nature, which imposes an energy–momentum mismatch between electrons and light. Here, we demonstrate a strong interaction between free-electron waves and light waves, resulting from precise energy–momentum phase-matching with the extended propagating light field. By exchanging hundreds of photons with the field, each electron simultaneously accelerates and decelerates in a coherent manner. Consequently, each electron’s quantum wavefunction evolves into a quantized energy comb, spanning a bandwidth of over 1,700 eV, requiring us to extend the PINEM theory. Our observation of coherent electron phase-matching with a propagating wave is a type of inverse-Cherenkov interaction that occurs with a quantum electron wavefunction, demonstrating how the extended nature of the electron wavefunction can alter stimulated electron–light interactions.
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All data that support the plots and other findings of this study are available from the corresponding author upon reasonable request. Source data are provided with this paper.
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22 January 2021
A Correction to this paper has been published: https://doi.org/10.1038/s41567-021-01178-3.
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Acknowledgements
We thank the IDES Company and especially S.T. Park for illuminating discussions and advice. We are also grateful to I. Goykhman for fruitful discussions. The experiments were performed on the UTEM of the I. K. AdQuanta group installed in the Electron Microscopy Center (MIKA) in the Department of Material Science and Engineering at the Technion. The research was supported by ERC starting grant NanoEP 851780 and the Israel Science Foundation grant 831/19. K.W. is partially supported by a fellowship from the Lady Davis Foundation. I.K. acknowledges the support of the Azrieli Faculty Fellowship.
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R.D. achieved the grazing-angle condition in the transmission electron microscope and led the experimental work including sample preparation. S.N. and R.D. worked on the design before the experiment began. R.D., K.W., M.S., O.B., Y.A. and S.N. carried out the experiments. K.W., S.N., Y.A., R.D., O.R. and Y.K. developed the theory and analysed the results. M.H.L. and X.S. contributed to the discussion of the results. I.K. conceived the research. All authors provided substantial input to all aspects of the project and to the writing of the manuscript.
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Supplementary Discussion and Supplementary Figs. 1–6.
Supplementary Video 1
Finite-difference time-domain simulation of the setup. The simulation assumes a right-angle glass prism with refractive index 1.513 at 700 nm, 15 μm leg size, and base angle of 45°. The laser undergoes total internal reflection inside the prism and generates an evanescent field that interacts with the electron that passes nearby.
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Source Data Fig. 1
Data used to plot Fig. 1b–d. Experimental data points and theoretical data from the classical and quantum mechanical models.
Source Data Fig. 3
Data used to plot Fig. 3. Experimental data points and data from conventional as well as extended PINEM theory.
Source Data Fig. 4
Data used to plot Fig. 4b–e. Experimental and theoretical data points.
Source Data Fig 5
Data used to plot Fig. 5a,b. Experimental data points and theoretical data from the classical and quantum mechanical models.
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Dahan, R., Nehemia, S., Shentcis, M. et al. Resonant phase-matching between a light wave and a free-electron wavefunction. Nat. Phys. 16, 1123–1131 (2020). https://doi.org/10.1038/s41567-020-01042-w
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DOI: https://doi.org/10.1038/s41567-020-01042-w
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