39th Annual Meeting of the APS Division of Atomic, Molecular, and Optical Physics
Volume 53, Number 7
Tuesday–Saturday, May 27–31, 2008;
State College, Pennsylvania
Session U2: Focus Session: Strongly Correlated Photons
8:00 AM–10:24 AM,
Saturday, May 31, 2008
Kern Building
Room: 112
Chair: Matt Mackie, Temple University
Abstract ID: BAPS.2008.DAMOP.U2.1
Abstract: U2.00001 : Strong Interactions of Photon Pairs in Cavity QED*
8:00 AM–8:36 AM
Preview Abstract
Abstract
Author:
H.J. Kimble
(California Institute of Technology)
The charge and spin degrees of freedom of massive particles have
relatively
large long-range interactions, which enable nonlinear coupling
between pairs
of atoms, ions, electrons, and diverse quasi-particles. By
contrast, photons
have vanishingly small cross-sections for direct coupling.
Instead, photon
interactions must be mediated by a material system. Even then,typical
materials produce photon-photon couplings that are orders of
magnitude too
small for nontrivial dynamics with individual photon pairs. The
leading
exception to this state of affairs is cavity quantum
electrodynamics (cQED),
where strong interactions between light and matter at the
single-photon
level have enabled a wide set of scientific advances [1].
My presentation will describe two experiments in the Caltech
Quantum Optics
Group where strong interactions of photon pairs have been
observed. The work
in Ref. [2] provided the initial realization of photon blockade
for an
atomic system by using a Fabry-Perot cavity containing one atom
strongly
coupled to the cavity field. The underlying blockade mechanism
was the
quantum anharmonicity of the ladder of energy levels for the
composite
atom-cavity system. Beyond this \textit{structural} effect, a new
\textit{%
dynamical} mechanism was identified in Ref. [3] for which photon
transport
is regulated by the conditional state of one intracavity atom,
leading to an
efficient mechanism that is insensitive to many experimental
imperfections
and which achieves high efficiency for single-photon transport. The
experiment utilized the interaction of an atom with the fields of a
microtoroidal resonator [4]. Regulation was achieved by way of an
interference effect involving the directly transmitted optical
field, the
intracavity field in the absence of the atom, and the
polarization field
radiated by the atom, with the requisite nonlinearity provided by the
quantum character of the emission from one atom.\smallskip
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[1] R. Miller, T. E. Northup, K. M. Birnbaum, A. Boca, A. D.
Boozer, and H. J. Kimble, J. Phys. B: At. Mol. Opt. Phys.
\textbf{38}, S551-S565 (2005).
\newline
[2] K. M. Birnbaum, A. Boca, R. Miller, A. D. Boozer, T. E.
Northup, and H. J. Kimble, Nature \textbf{436}, 87 (2005).
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[3] B. Dayan, A. S. Parkins, T. Aoki, H. J. Kimble, E. Ostby,
and K. J. Vahala, Science (in press, 2008).
\newline
[4] Takao Aoki, B. Dayan, E. Wilcut, W. P. Bowen, A. S.
Parkins, H. J. Kimble, T. J. Kippenberg, and K. J. Vahala, Nature
\textbf{443}, 671 (2006).
*This research is supported by the National Science Foundation \#PHY-0652914, by IARPA, and by Northrop Grumman Space Technology.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2008.DAMOP.U2.1