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Electrons herald non-classical light

MPS-Authors
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Arend,  Germaine       
Department of Ultrafast Dynamics, Max Planck Institute for Multidisciplinary Sciences, Max Planck Society;

/persons/resource/persons270783

Feist,  Armin
Department of Ultrafast Dynamics, Max Planck Institute for Multidisciplinary Sciences, Max Planck Society;

/persons/resource/persons270780

Henke,  Jan-Wilke
Department of Ultrafast Dynamics, Max Planck Institute for Multidisciplinary Sciences, Max Planck Society;

/persons/resource/persons301908

Jeng,  Hao
Department of Ultrafast Dynamics, Max Planck Institute for Multidisciplinary Sciences, Max Planck Society;

/persons/resource/persons292481

Haindl,  Rudolf
Department of Ultrafast Dynamics, Max Planck Institute for Multidisciplinary Sciences, Max Planck Society;

/persons/resource/persons270504

Ropers,  Claus       
Department of Ultrafast Dynamics, Max Planck Institute for Multidisciplinary Sciences, Max Planck Society;

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2409.11300v1.pdf
(Preprint), 2MB

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Citation

Arend, G., Huang, G., Feist, A., Yang, Y., Henke, J.-W., Qiu, Z., et al. (2024). Electrons herald non-classical light. arXiv. doi:10.48550/arXiv.2409.11300.


Cite as: https://hdl.handle.net/21.11116/0000-000F-DDB4-D
Abstract
Free electrons are a widespread and universal source of electromagnetic fields. The past decades witnessed ever-growing control over many aspects of electron-generated radiation, from the incoherent emission produced by X-ray tubes to the exceptional brilliance of free-electron lasers. Reduced to the elementary process of quantized energy exchange between individual electrons and the electromagnetic field, electron beams may facilitate future sources of tunable quantum light. However, the quantum features of such radiation are tied to the correlation of the particles, calling for the joint electronic and photonic state to be explored for further applications. Here, we demonstrate the coherent parametric generation of non-classical states of light by free electrons. We show that the quantized electron energy loss heralds the number of photons generated in a dielectric waveguide. In Hanbury-Brown-Twiss measurements, an electron-heralded single-photon state is revealed via antibunching intensity correlations, while two-quantum energy losses of individual electrons yield pronounced two-photon coincidences. The approach facilitates the tailored preparation of higher-number Fock and other optical quantum states based on controlled interactions with free-electron beams.