Share Email Print
cover

Proceedings Paper

Spontaneous emission of a two-level atom in photonic crystals
Author(s): Lingjiang Yao; Jingcui Peng; Hongjian Li; Gaoming Zhang; Zhijian Jian; Renlong Zhou; Feng Lin; Yufeng Xu; Wenhua Li
Format Member Price Non-Member Price
PDF $14.40 $18.00
cover GOOD NEWS! Your organization subscribes to the SPIE Digital Library. You may be able to download this paper for free. Check Access

Paper Abstract

We investigate spontaneous emission from a two-level atom embedded in photonic crystals. Due to the photon localization and the quantum interference between the two dressed states, some changes of the radiation field happen, and the energy is transferred among the excited atom, the localized field, the propagating field and the diffusion field. If there is a localized field, it appears quasi-oscillation behaves of the population evolution in the excited level. If there isn't a localized field, it appears no quasi-oscillation. Moreover, there have some steady-state trapped atom populations in the excited level, and the spontaneous emission spectrum near the forbidden gap edge is different from that in the vacuum. All these characteristics depend not only on the relative position of the excited level from the band-edge but also on the photon density of states (or the band-edge smoothing parameter) near the band edge.

Paper Details

Date Published: 12 May 2004
PDF: 9 pages
Proc. SPIE 5280, Materials, Active Devices, and Optical Amplifiers, (12 May 2004); doi: 10.1117/12.523226
Show Author Affiliations
Lingjiang Yao, Hunan Univ. (China)
Jingcui Peng, Hunan Univ. (China)
Hongjian Li, Hunan Univ. (China)
Gaoming Zhang, Hunan Univ. (China)
Zhijian Jian, Hunan Univ. (China)
Renlong Zhou, Hunan Univ. (China)
Feng Lin, Hunan Univ. (China)
Yufeng Xu, Hunan Univ. (China)
Wenhua Li, Hunan Univ. (China)


Published in SPIE Proceedings Vol. 5280:
Materials, Active Devices, and Optical Amplifiers
Connie J. Chang-Hasnain; Dexiu Huang; Yoshiaki Nakano; Xiaomin Ren, Editor(s)

© SPIE. Terms of Use
Back to Top