Abstract

The interaction of swift, free-space electrons with confined optical near fields has recently sparked much interest. It enables a new type of photon-induced near-field electron microscopy, mapping local optical near fields around nanoparticles with exquisite spatial and spectral resolution and lies at the heart of quantum state manipulation and attosecond pulse shaping of free electrons. The corresponding interaction of optical near fields with slow electrons has achieved much less attention, even though the lower electron velocity may enhance electron-near-field coupling for small nanoparticles. A first-principle theoretical study of such interactions has been reported very recently by N Talebi (2020 Phys. Rev. Lett. 125 080401). Building up on this work, we investigate, both analytically and numerically, the inelastic scattering of slow electrons by near fields of small nanostructures. For weak fields, this results in distinct angular diffraction patterns that represent, to first order, the Fourier transform of the transverse variation of the scalar near-field potential along the direction perpendicular to the electron propagation. For stronger fields, scattering by the near-field component along the electron trajectory results in a break-up of the energy spectrum into multiple photon orders. Their angular diffraction patterns are given by integer powers of the Fourier transform of the transverse potential variation and are shifting in phase with photon order. Our analytical model offers an efficient approach for studying the effects of electron kinetic energy, near field shape and strength on the slow-electron diffraction pattern and thus may facilitate the experimental observation of these phenomena by, e.g. ultrafast low-energy point-projection microscopy or related techniques. This could provide simultaneous access to different vectorial components of the optical near fields of small nanoparticles.

Highlights

  • When free swift electrons pass an optically excited nanostructure at close distance, their wave function acquires a phase modulation

  • For sufficiently strong fields this phase modulation can be used to tailor the quantum state of free electron wave functions [6], opening up exciting new ways for the creation of attosecond electron pulse trains [7], or to directly measure the quantum state of nanolocalized optical fields [8]. Inducing such a phase modulation of the electron wave function is most efficient if phase matching between the localized field and the passing electron wave is satisfied: In this case, the optical wave vector component parallel to the propagation direction of the electron matches the ratio of optical frequency and electron velocity [3]

  • A diffraction pattern is seen in the transverse direction, which becomes even more pronounced for slow electrons with ~100 eV kinetic energies

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Summary

Introduction

When free swift electrons pass an optically excited nanostructure at close distance, their wave function acquires a phase modulation This phase modulation lies at the heart of photon induced optical near field microscopy (PINEM) [1-3] and resulted in the development of electron energy gain spectroscopy (EEGS) [4, 5]. For sufficiently strong fields this phase modulation can be used to tailor the quantum state of free electron wave functions [6], opening up exciting new ways for the creation of attosecond electron pulse trains [7], or to directly measure the quantum state of nanolocalized optical fields [8]. Since the electron beam width employed in transmission electron microscopes (TEM) typically is on the order of only a few nm, the spatial variation of the optical field across the electron beam can be neglected and the phase modulation is described reasonably well in one-dimensional models [3] Due to their high velocities, electrons in a TEM pass the optical field around particles with dimensions below 100 nm within less than an optical cycle. The experimental investigation of these interferograms could pave the way towards a full vectorial characterization of optical near-field dynamics of individual nanostructures with few-femtosecond time resolution

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