中国物理B ›› 2023, Vol. 32 ›› Issue (4): 44211-044211.doi: 10.1088/1674-1056/aca39b

• • 上一篇    下一篇

Spontaneous emission from Λ-type three-level atom driven by bichromatic field in anisotropic double-band photonic crystals

Kai Ling(凌凯)1, Li Jiang(姜丽)1,†, Ren-Gang Wan(万仁刚)2,‡, and Zhi-Hai Yao(姚治海)1   

  1. 1 Changchun University of Science and Technology, Changchun 130000, China;
    2 School of Physics and Information Technology, Shaanxi Normal University, Xi'an 710062, China
  • 收稿日期:2022-08-30 修回日期:2022-11-15 接受日期:2022-11-17 出版日期:2023-03-10 发布日期:2023-03-30
  • 通讯作者: Li Jiang, Ren-Gang Wan E-mail:jiangli@cust.edu.cn;wrg@snnu.edu.cn
  • 基金资助:
    Project supported by the Natural Science Foundation of Jilin Province of China (Grant No. 20220101031JC).

Spontaneous emission from Λ-type three-level atom driven by bichromatic field in anisotropic double-band photonic crystals

Kai Ling(凌凯)1, Li Jiang(姜丽)1,†, Ren-Gang Wan(万仁刚)2,‡, and Zhi-Hai Yao(姚治海)1   

  1. 1 Changchun University of Science and Technology, Changchun 130000, China;
    2 School of Physics and Information Technology, Shaanxi Normal University, Xi'an 710062, China
  • Received:2022-08-30 Revised:2022-11-15 Accepted:2022-11-17 Online:2023-03-10 Published:2023-03-30
  • Contact: Li Jiang, Ren-Gang Wan E-mail:jiangli@cust.edu.cn;wrg@snnu.edu.cn
  • Supported by:
    Project supported by the Natural Science Foundation of Jilin Province of China (Grant No. 20220101031JC).

RichHTML

2

PDF (PC)

162

赞

摘要： The spontaneous emission property of Λ-type three-level atom driven by the bichromatic field in the anisotropic double-band photonic crystal is calculated by n-times iteration method. The influence of different parameters on atomic spontaneous emission is studied, and the phenomena of atomic spontaneous emission are explained in the dressed state representation. It is found that the spontaneous emission spectra of the atom driven by the bichromatic field presents a multi-peak comb structure. The position of the emission peak is determined by the initial state of the atom, and the interval between the neighboring emission peaks is the detuning δ of the bichromatic field. When the ratio between Rabi frequency intensity and the detuning δ of the bichromatic field remains unchanged, the intensity of each emitted peak remains invariant. The spontaneously emitted peak can be annihilated in the band gap and enhanced near the band edge in the anisotropic photonic crystals. Meanwhile, we also observe the fluorescence quenching phenomenon in the spontaneous emission spectra. The research in this paper provides the theoretical guidance for the control of atomic spontaneous emission.

关键词: photonic crystal, bichromatic field, spontaneous emission spectra, dressed state

Abstract: The spontaneous emission property of Λ-type three-level atom driven by the bichromatic field in the anisotropic double-band photonic crystal is calculated by n-times iteration method. The influence of different parameters on atomic spontaneous emission is studied, and the phenomena of atomic spontaneous emission are explained in the dressed state representation. It is found that the spontaneous emission spectra of the atom driven by the bichromatic field presents a multi-peak comb structure. The position of the emission peak is determined by the initial state of the atom, and the interval between the neighboring emission peaks is the detuning δ of the bichromatic field. When the ratio between Rabi frequency intensity and the detuning δ of the bichromatic field remains unchanged, the intensity of each emitted peak remains invariant. The spontaneously emitted peak can be annihilated in the band gap and enhanced near the band edge in the anisotropic photonic crystals. Meanwhile, we also observe the fluorescence quenching phenomenon in the spontaneous emission spectra. The research in this paper provides the theoretical guidance for the control of atomic spontaneous emission.

Key words: photonic crystal, bichromatic field, spontaneous emission spectra, dressed state

中图分类号:  (Photonic bandgap materials)

  • 42.70.Qs
32.80.Qk (Coherent control of atomic interactions with photons) 42.50.Gy (Effects of atomic coherence on propagation, absorption, and Amplification of light; electromagnetically induced transparency and Absorption)