Atoms in micron-sized metallic and dielectric waveguides

被引:19
作者
Hinds, EA [1 ]
Lai, KS
Schnell, M
机构
[1] Univ Sussex, Sussex Ctr Opt & Atom Phys, Brighton BN1 9QH, E Sussex, England
[2] Yale Univ, Sloan Phys Lab, New Haven, CT 06520 USA
[3] Univ Konstanz, Fak Phys, D-78434 Constance, Germany
来源
PHILOSOPHICAL TRANSACTIONS OF THE ROYAL SOCIETY A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES | 1997年 / 355卷 / 1733期
关键词
D O I
10.1098/rsta.1997.0132
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
Over the past ten years, our group has investigated the effects of confinement on atoms inside metallic micron-sized cavities in order to elucidate some basic phenomena in the field of cavity quantum electrodynamics (QED). The first of these was the inhibition of spontaneous emission from an atom inside a cavity. This was followed by a laser spectroscopic measurement of the van der Waals interaction between a single Rydberg atom and a gold cavity, which showed that a simple electrostatic model of the atom-cavity interaction is correct when the cavity is small enough. More recently, the retarded Casimir-Polder force was measured between a ground state sodium atom and a large cavity, demonstrating that the van der Waals potential fails at long enough range and that the vacuum fluctuations of the field then have an important role in the interaction of the atom with the cavity. Our group is now pushing forward these investigations to study cavities whose walls have losses and dispersion, where the theory of cavity QED is significantly more complicated. With real surfaces, we have to deal with the complex dielectric response epsilon(omega) of the material, which exhibits frequency-dependent absorption and dispersion. One particularly interesting case is when a downward transition in the atom is resonant with an excitation of the cavity walls. This opens a new branch for the atomic decay: as an alternative to creating a photon within the space surrounded by the cavity walls the atomic decay can now create an electromagnetic excitation of the walls themselves. Another novel feature of our experiments is that the Bohr frequencies of the atom are close to the k(T)/h, where T is room temperature. We therefore expect to be able to measure effects associated with QED at finite temperature; in other words, to study how the blackbody radiation affects our experiments. By conducting experiments with real surfaces, we hope to elucidate and perhaps simplify the theoretical models used to describe these systems.
引用
收藏
页码:2353 / 2365
页数:13
相关论文
共 21 条
[1]   QUANTUM-ELECTRODYNAMIC LEVEL SHIFTS BETWEEN PARALLEL MIRRORS - ANALYSIS [J].
BARTON, G .
PROCEEDINGS OF THE ROYAL SOCIETY OF LONDON SERIES A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 1987, 410 (1838) :141-174
[2]   QUANTUM-ELECTRODYNAMIC LEVEL SHIFTS BETWEEN PARALLEL MIRRORS - APPLICATIONS, MAINLY TO RYDBERG STATES [J].
BARTON, G .
PROCEEDINGS OF THE ROYAL SOCIETY OF LONDON SERIES A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 1987, 410 (1838) :175-200
[3]  
Berman P. R., 1994, CAVITY QUANTUM ELECT
[4]  
Casimir H. B. G., 1948, Proc. Kon. Ned. Akad. Wet, V51, P793, DOI DOI 10.4236/WJNSE.2015.52007
[5]   THE INFLUENCE OF RETARDATION ON THE LONDON-VANDERWAALS FORCES [J].
CASIMIR, HBG ;
POLDER, D .
PHYSICAL REVIEW, 1948, 73 (04) :360-372
[6]   TABLES FOR THE COMPUTATION OF RADIAL INTEGRALS IN THE COULOMB APPROXIMATION [J].
EDMONDS, AR ;
PICART, J ;
TRANMINH, N ;
PULLEN, R .
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 1979, 12 (17) :2781-2787
[7]  
Edwards D.F., 1985, Handbook of optical constants of solids
[8]   VACUUM RADIATIVE LEVEL SHIFT AND SPONTANEOUS-EMISSION LINEWIDTH OF AN ATOM IN AN OPTICAL-RESONATOR [J].
HEINZEN, DJ ;
FELD, MS .
PHYSICAL REVIEW LETTERS, 1987, 59 (23) :2623-2626
[9]  
HINDS EA, 1994, ADV AT MOL OPT PHY S, V2, P1
[10]  
IBACH H, 1995, SOLID STATE PHYS, P287