Abstract

Slow swift electrons with low self-inertia interact differently with matter and light in comparison with their relativistic counterparts: they are easily recoiled, reflected, and also diffracted form optical gratings and nanostructures. As a consequence, they can be also better manipulated into the desired shape. For example, they get bunched quite fast in interaction with acceleration gratings in presence of an external electromagnetic radiation, a phenomenon which can be desirable in development of superradiant coherent light sources. Here, I examine the spatiotemporal behavior of pulsed electron wave packets at low energies interacting with pulsed light and optical gratings, using a quantum-mechanical self-consistent numerical toolbox which is introduced here. It will be shown that electron pulses are accelerated very fast in interaction with the near-field of the grating, demanding that a synchronicity condition is met. To prevent the electrons to be transversely deflected from the grating a symmetric double-grating configuration is necessary. It is found that even in this configuration, diffraction due to the interaction of the electron with the standing-wave light inside the gap between the gratings, is a source of defocusing. Moreover, the longitudinal broadening of the electron pulse directly affects the final shape of the electron wave packet due to the occurrence of multiple electron-photon scatterings. These investigations pave the way towards the design of more efficient electron-driven photon sources and accelerators.

Highlights

  • Electron-photon interactions have been the subject of intense studies

  • When an external laser field is applied to the grating, an electron traveling adjacent to the grating may gain energy by absorbing photons, a phenomenon referred to as inverse Smith‒Purcell effect [40]

  • The time threshold ts 2m0WL2,t is related to the square of longitudinal broadening, which means that, for a sufficiently long pulse, the change in the carrier energy should be not pronounced, but the electron wave packet experiences bunching, as we will see in the following. It is already apparent from the results presented above that coherent electron wave packets do interact in a different way with optical gratings in comparison with monolithic classical electrons at an equivalent centre of mass energy

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Summary

Introduction

Electron-photon interactions have been the subject of intense studies. Several spontaneous and stimulated mechanisms of radiation from electrons have been hitherto detected; i.e. Larmor radiation [1], Cherenkov radiation [2], bremsstrahlung [3], transition radiation [2], Smith‒Purcell effect [4], and stimulated Compton‒Raman scattering [5], which have found applications in particle detectors [6], efficient electron-driven photon sources [7,8,9], and spectroscopy techniques [10]. A combined system of laser beams and electron wave packet in the presence of matter which mediates the electron‒ photon interaction, causes the electrons to absorb photons. This has been perfectly demonstrated in the recent field of photon-induced near-field electron microscopy (PINEM) [11,12,13,14]. ˆ is a unitary vector along the grating axis, is the period of the grating, and m is an integer denoting the diffraction order This mapping is the reason behind the Smith‒Purcell radiation into the far-field. When an external laser field is applied to the grating, an electron traveling adjacent to the grating may gain energy by absorbing photons, a phenomenon referred to as inverse Smith‒Purcell effect [40]

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