Strong atom-field coupling for Bose-Einstein condensates in an optical cavity on a chip

被引:592
作者
Colombe, Yves
Steinmetz, Tilo
Dubois, Guilhem
Linke, Felix
Hunger, David
Reichel, Jakob
机构
[1] Univ Paris 06, CNRS, ENS, Lab Kastler Brossel, F-75005 Paris, France
[2] LMU, Max Planck Inst Quantenopt, D-80799 Munich, Germany
关键词
D O I
10.1038/nature06331
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
An optical cavity enhances the interaction between atoms and light, and the rate of coherent atom-photon coupling can be made larger than all decoherence rates of the system. For single atoms, this 'strong coupling regime' of cavity quantum electrodynamics(1,2) has been the subject of many experimental advances. Efforts have been made to control the coupling rate by trapping(3,4) the atom and cooling(5,6) it towards the motional ground state; the latter has been achieved in one dimension so far(5). For systems of many atoms, the three-dimensional ground state of motion is routinely achieved(7) in atomic Bose-Einstein condensates (BECs). Although experiments combining BECs and optical cavities have been reported recently(8,9), coupling BECs to cavities that are in the strong-coupling regime for single atoms has remained an elusive goal. Here we report such an experiment, made possible by combining a fibre-based cavity(10) with atom-chip technology(11). This enables single-atom cavity quantum electrodynamics experiments with a simplified set-up and realizes the situation of many atoms in a cavity, each of which is identically and strongly coupled to the cavity mode(12). Moreover, the BEC can be positioned deterministically anywhere within the cavity and localized entirely within a single antinode of the standing-wave cavity field; we demonstrate that this gives rise to a controlled, tunable coupling rate. We study the heating rate caused by a cavity transmission measurement as a function of the coupling rate and find no measurable heating for strongly coupled BECs. The spectrum of the coupled atoms-cavity system, which we map out over a wide range of atom numbers and cavity-atom detunings, shows vacuum Rabi splittings exceeding 20 gigahertz, as well as an unpredicted additional splitting, which we attribute to the atomic hyperfine structure. We anticipate that the system will be suitable as a light-matter quantum interface for quantum information(13).
引用
收藏
页码:272 / U9
页数:6
相关论文
共 34 条
[1]   Bose-Einstein condensation of atomic gases [J].
Anglin, JR ;
Ketterle, W .
NATURE, 2002, 416 (6877) :211-218
[2]   Observation of strong coupling between one atom and a monolithic microresonator [J].
Aoki, Takao ;
Dayan, Barak ;
Wilcut, E. ;
Bowen, W. P. ;
Parkins, A. S. ;
Kippenberg, T. J. ;
Vahala, K. J. ;
Kimble, H. J. .
NATURE, 2006, 443 (7112) :671-674
[3]   Cooling to the ground state of axial motion for one atom strongly coupled to an optical cavity [J].
Boozer, A. D. ;
Boca, A. ;
Miller, R. ;
Northup, T. E. ;
Kimble, H. J. .
PHYSICAL REVIEW LETTERS, 2006, 97 (08)
[4]   COHERENCE IN SPONTANEOUS RADIATION PROCESSES [J].
DICKE, RH .
PHYSICAL REVIEW, 1954, 93 (01) :99-110
[5]   Atom-chip Bose-Einstein condensation in a portable vacuum cell -: art. no. 053606 [J].
Du, SW ;
Squires, MB ;
Imai, Y ;
Czaia, L ;
Saravanan, RA ;
Bright, V ;
Reichel, J ;
Hänsch, TW ;
Anderson, DZ .
PHYSICAL REVIEW A, 2004, 70 (05) :053606-1
[6]   Long-distance quantum communication with atomic ensembles and linear optics [J].
Duan, LM ;
Lukin, MD ;
Cirac, JI ;
Zoller, P .
NATURE, 2001, 414 (6862) :413-418
[7]  
Fischer T, 2001, NEW J PHYS, V3, P111
[8]   Magnetic microtraps for ultracold atoms [J].
Fortagh, Jozsef ;
Zimmermann, Claus .
REVIEWS OF MODERN PHYSICS, 2007, 79 (01) :235-289
[9]   Quasi-1D Bose-Einstein condensates in the dimensional crossover regime [J].
Gerbier, F .
EUROPHYSICS LETTERS, 2004, 66 (06) :771-777
[10]   Collapse and revival of the matter wave field of a Bose-Einstein condensate [J].
Greiner, M ;
Mandel, O ;
Hänsch, TW ;
Bloch, I .
NATURE, 2002, 419 (6902) :51-54