By Topic

Atomic motional states in an optical cavity field

Sign In

Cookies must be enabled to login.After enabling cookies , please use refresh or reload or ctrl+f5 on the browser for the login options.

Formats Non-Member Member
$31 $13
Learn how you can qualify for the best price for this item!
Become an IEEE Member or Subscribe to
IEEE Xplore for exclusive pricing!
close button

puzzle piece

IEEE membership options for an individual and IEEE Xplore subscriptions for an organization offer the most affordable access to essential journal articles, conference papers, standards, eBooks, and eLearning courses.

Learn more about:

IEEE membership

IEEE Xplore subscriptions

4 Author(s)
Doherty, A.C. ; Dept. of Phys., Auckland Univ., New Zealand ; Parkins, A.S. ; Tan, S.M. ; Walls, D.F.

Summary form only given. A new regime in cavity QED is realized in which single atoms interact with the cavity field for very long times (i.e., many Rabi cycles) and in which the atomic kinetic energy is comparable to or smaller than the dipole coupling energy. The mechanical effects of just a few-photon light field should therefore enable single atoms to be trapped in effective potential wells. We consider such a situation in the far detuned dispersive regime of cavity QED, where a single atom is confined in the lower (quantized) bound states of the effective optical potential formed around an antinode of the standing wave cavity field.

Published in:

Quantum Electronics Conference, 1998. IQEC 98. Technical Digest. Summaries of papers presented at the International

Date of Conference:

8-8 May 1998