Ea. Hinds et al., ATOMS IN MICRON-SIZED METALLIC AND DIELECTRIC WAVE-GUIDES, Philosophical transactions-Royal Society of London. Physical sciences and engineering, 355(1733), 1997, pp. 2353-2365
Over the past ten years, our group has investigated the effects of con
finement on atoms inside metallic micron-sized cavities in order to el
ucidate some basic phenomena in the field of cavity quantum electrodyn
amics (QED). The first of these was the inhibition of spontaneous emis
sion from an atom inside a cavity. This was followed by a laser spectr
oscopic measurement of the van der Waals interaction between a single
Rydberg atom and a gold cavity, which showed that a simple electrostat
ic model of the atom-cavity interaction is correct when the cavity is
small enough. More recently, the retarded Casimir-Polder force was mea
sured between a ground state sodium atom and a large cavity, demonstra
ting that the van der Waals potential fails at long enough range and t
hat the vacuum fluctuations of the field then have an important role i
n the interaction of the atom with the cavity. Our group is now pushin
g forward these investigations to study cavities whose walls have loss
es and dispersion, where the theory of cavity QED is significantly mor
e complicated. With real surfaces, we have to deal with the complex di
electric response epsilon(omega) of the material, which exhibits frequ
ency-dependent absorption and dispersion. One particularly interesting
case is when a downward transition in the atom is resonant with an ex
citation of the cavity walls. This opens a new branch for the atomic d
ecay: as an alternative to creating a photon within the space surround
ed by the cavity walls the atomic decay can now create an electromagne
tic excitation of the walls themselves. Another novel feature of our e
xperiments is that the Bohr frequencies of the atom are close to the k
(T)/h, where T is room temperature. We therefore expect to be able to
measure effects associated with QED at finite temperature; in other wo
rds, to study how the blackbody radiation affects our experiments. By
conducting experiments with real surfaces, we hope to elucidate and pe
rhaps simplify the theoretical models used to describe these systems.