posted on 2024-05-14, 11:34authored byEvelijn Akerboom, Valerio Di Giulio, Nick J. Schilder, F. Javier García de Abajo, Albert Polman
Tightly confined optical near fields in plasmonic nanostructures
play a pivotal role in important applications ranging from optical
sensing to light harvesting. Energetic electrons are ideally suited
to probing optical near fields by collecting the resulting cathodoluminescence
(CL) light emission. Intriguingly, the CL intensity is determined
by the near-field profile along the electron propagation direction,
but the retrieval of such field from measurements has remained elusive.
Furthermore, the conditions for optimum electron near-field coupling
in plasmonic systems are critically dependent on such field and remain
experimentally unexplored. In this work, we use electron energy-dependent
CL spectroscopy to study the tightly confined dipolar mode in plasmonic
gold nanoparticles. By systematically studying gold nanoparticles
with diameters in the range of 20–100 nm and electron energies
from 4 to 30 keV, we determine how the coupling between swift electrons
and the optical near fields depends on the energy of the incoming
electron. The strongest coupling is achieved when the electron speed
equals the mode phase velocity, meeting the so-called phase-matching
condition. In aloof experiments, the measured data are well reproduced
by electromagnetic simulations, which explain that larger particles
and faster electrons favor a stronger electron near-field coupling.
For penetrating electron trajectories, scattering at the particle
produces severe corrections of the trajectory that defy existing theories
based on the assumption of nonrecoil condition. Therefore, we develop
a first-order recoil correction model that allows us to account for
inelastic electron scattering, rendering better agreement with measured
data. Finally, we consider the albedo of the particles and find that,
to approach unity coupling, a highly confined electric field and very
slow electrons are needed, both representing experimental challenges.
Our findings explain how to reach unity-order coupling between free
electrons and confined excitations, helping us understand fundamental
aspects of light–matter interaction at the nanoscale.