Quantum
control of strong interactions between a single atom and one
photon has been achieved within the setting of cavity quantum
electrodynamics (cQED)
[1]. To move beyond proof-of-principle
experiments involving one or two conventional optical cavities to
more complex scalable systems that employ N >> 1 microscopic
resonators requires localization of atoms on distance scales ~100
nm from a resonator’s surface where an atom can be strongly
coupled to a single intracavity photon.
A promising
candidate for the realization of such systems is a system of
microtoroidal resonators that are optically coupled via tapered
nanofibers
[2]. Cavity QED interactions between falling single
atoms and single intracavity photons in such a system has been
achieved in the strong coupling regime
[3], followed by
demonstrations of dynamic regulation of photon transport
[4,5].
Recent study allows observations of perturbative surface effects
mediated by atom’s radiative interactions, due to its proximity to
the dielectric boundary of the resonator, and cQED dynamics in the
strong coupling regime
[6,7]. In this initial step into a new
regime of cQED, we use real-time detection and high-bandwidth
feedback to select and monitor the motion of a single Cesium atom
through the evanescent field of a microtoroid. Direct temporal and
spectral measurements along with simulations reveal the manifestly
quantum nature of strongly coupled atom-cavity dynamics, and the
significant role the Casimir effect and light forces play in the
atom dynamics. This interplay is significant and important in
determining the dynamics of cQED systems involving strongly
interacting single atoms in close proximity to resonator
boundaries, setting the stage for trapping strongly interacting
atoms near micro- and nano-scopic optical resonators. Our research
currently focuses on the realization of single atom trapping in
this new regime of cavity QED.