One-atom
laser.

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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).
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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.
- About 14000 photons are produced by each atom on average
- 2-photon events are suppressed by over twenty-fold relative
to a weak coherent state. This is limited by rare events in which
we load 2 atoms into the trap.
- Our overall escape, propagation and detection efficiency is
between 2 and 3%, in agreement with the fraction of attempts in which
we detect a photon.
- Our system enables coherent reversibility and
user-controlled pulse shapes, which we are working to improve in
ongoing experiments.
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.