The far off-resonant trap: a tool for confining atoms in cavities

Cold cesium atoms, released from a magneto-optical trap, fall through our cavity and interact with the standing-wave field between its two mirrors.  In order to extend this interaction time, we use a classical standing-wave dipole force trap, with a trap lifetime of 2-3 seconds within the cavity demonstrated in 2003.  The trap's standing wave is supported by a mode of the cavity which is several free spectral ranges away from the cesium resonance; laser beams perpendicular to the cavity axis cool the atom into the trap.  A single atom confined within the far off-resonant trap (FORT) is then available for strongly coupled interaction with a series of photons.  This has made possible a series of recent experimental achievements:
One-atom laser.
Schematic for single atom laser.
One atom trapped between a pair of mirrors and optically pumped from the side: this is the fundamental "conceptual" lower limit on the size of a laser.  The basic idea is not really to build a device that will be used for any practical application, nor is it an exercise in miniaturization of lasers.  It's more of an exploration of a fundamental limit, in a particularly quantum & strongly-coupled regime.  The output of our device is non-classical, meaning our photodetection data can only come from a quantized field.  Although the properties of the system are not typical for a laser, that is a result of the strong coupling of the atom to the field (or equivalently, the very small size of our cavity) which effectively causes each photon to leave the cavity as soon as it is "created" by the driven atom (at random moments). 

Single photons on demand.
Using a pulsed sequence of side beams, we are able to generate single photons deterministically from atoms trapped in a cavity. 
Cavity QED "by the numbers."
Atoms leave the cavity one at a time.
Continuous observation of the cavity via a weak probe beam allows us to determine the number of trapped atoms in real time.  In the image to the left, N > 4 atoms are loaded into the trap and subsequently leave one at a time, altering the transmission of the probe beam in a "stair step" cascade.   This technique could be used to choose the precise number of atoms interacting with a cavity in our experiments.
Vacuum-Rabi spectrum.
Vacuum-Rabi spectrum. For an individual trapped atom, we have mapped out the vacuum-Rabi splitting, a signature of the atom-cavity system's eigenvalue spectrum in the strong coupling regime.  While previous measurements required 103-105 atoms to obtain a single spectrum, we were able to interleave our probing sequences with atomic cooling in order to perform an extended series of measurements on the system.  A new Raman sideband scheme for cooling the trapped atom was an integral part of this experiment.
Photon blockade.
Analagous to the condensed-matter phenomenon of Coulomb blockade, photon blockade occurs when the absorption of a first input photon by an optical device blocks the absorption of a second one.  In the context of cavity QED, this blockade is due to the anharmonicity of the Jaynes-Cummings ladder of eigenstates.   We have observed photon blockade by probing on the lower vacuum-Rabi sideband of a cavity and measuring the nonclassical statistics of the outgoing photon stream.  In addition, these photon statistics give us information about the temperature of the atoms, which we estimate to be ~250 microKelvin.

Ground-state cooling.
We have demonstrated resolved Raman sideband cooling of a trapped atom to its ground state along the cavity axis. This cooling technique, adapted from the ion trap community, allows us for the first time to access the quantum regime for atomic center-of-mass motion.
Trapping single atoms with single photons

Atom-cavity microscope.The experiments above rely on an external red-detuned classical field in order to trap atoms, but it is also possible to use the atom-cavity interaction itself.  By making the coupling energy of the atom to the cavity, g, greater than kinetic energy of the atom, we were able to trap single atoms with a single-photon-strength laser field for the first time. Quicktime movies of individual atom trajectories from this atom-cavity microscope are available here.  One exciting prospect is that by observing atoms passing through the standing wave structure of the cavity mode, it should be possible to approach the standard quantum limit for measurement of the atomic position.  We have designed and analyzed the performance of feedback algorithms which would actively stablilize the motion of the atom in real time.

Microsphere in fabrication.Fabry-Perot alternatives

Driven by the quest for yet higher cavity finesse in combination with small mode volume, we have investigated alternatives to Fabry-Perot cavities as possible settings for extending our work with cold atoms.  In the past, we have studied microsphere cavities, shown on the left during fabrication, and measured microsphere resonator quality factors of 2-3 billion. 

A current experiment in our research group explores the use of microtoroidal resonators for cavity QED interactions.