2005 36th Meeting of the Division of Atomic, Molecular and Optical Physics
Tuesday–Saturday, May 17–21, 2005;
Lincoln, Nebraska
Session P1: Hot Topics
9:00 AM–12:00 PM,
Saturday, May 21, 2005
Burnham Yates Conference Center
Room: Ballroom I
Chair: Kate Kirby, ITAMP, Harvard-Smithsonian Center for Astrophysics
Abstract ID: BAPS.2005.DAMOP.P1.5
Abstract: P1.00005 : Observation of the Vacuum-Rabi Spectrum for One Trapped Atom
11:24 AM–12:00 PM
Preview Abstract
Abstract
Author:
H. J. Kimble
(California Institute of Technology)
\begin{document}
A cornerstone of optical physics is the interaction of a single
atom with
the electromagnetic field of a high quality resonator. Of particular
importance is the regime of strong coupling, for which the
frequency scale $g
$ associated with reversible evolution for the atom-cavity system
exceeds
the rates $(\gamma ,\kappa )$ for irreversible decay of atom and
cavity
field, respectively. In the domain of strong coupling, a photon
emitted by
the atom into the cavity mode is likely to be repeatedly absorbed and
re-emitted at the single-quantum Rabi frequency $2g$ before being
irreversibly lost into the environment. This oscillatory exchange of
excitation between atom and cavity field results from a normal-mode
splitting in the eigenvalue spectrum of the atom-cavity system,
and has been
dubbed the vacuum-Rabi splitting.
Without exception experiments related to the vacuum-Rabi
splitting in cavity
QED with single atoms have required averaging over trials with
many atoms ($%
\gtrsim 10^{3}$) to obtain quantitative spectral information. By
contrast,
the implementation of complex algorithms in quantum information
science
requires the capability for repeated manipulation of an
individual quantum
system. With this goal in mind, we have succeeded in recording
the entire
vacuum-Rabi spectrum for one-and-the-same atom strongly coupled
to the field
of a high-finesse optical resonator [1]. These measurements are
made possible by a new Raman scheme for cooling atomic motion
along the
cavity axis for single atoms trapped within a state-insensitive
intracavity
FORT [2], with inferred atomic localization $\Delta
z_{axial}\simeq 33~\mathrm{nm}$. Our measurements represent an
important
milestone towards the realization of more complex tasks in quantum
computation and communication [3].
\begin{thebibliography}{9}
\bibitem{boca04} A. Boca, R. Miller, K. M. Birnbaum, A. D. Boozer, J.
McKeever, and H. J. Kimble, Phys. Rev. Lett. \textbf{93}, 233603
(2004).
\bibitem{mckeever03} J. McKeever, J.R. Buck, A.D. Boozer, A. Kuzmich,
H.-C.Nagerl, D.M. Stamper-Kurn, H.J. Kimble, Phys. Rev. Lett.
\textbf{90},
133602 (2003).
\bibitem{ack} This work was carried out in collaboration with A.
Boca, R.
Miller, K.~M. Birnbaum, A.~D. Boozer, and J. McKeever, and was
supported by
the Caltech MURI Center for Quantum Networks, by the National Science
Foundation, and by the Advanced Research and Development Activity
(ARDA).
\end{thebibliography}
\end{document}
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2005.DAMOP.P1.5