J4 ›› 2011, Vol. 28 ›› Issue (6): 682-686.

• 激光技术与器件 • 上一篇    下一篇

480nm激光器的双光子DAVLL谱稳频

许鹏1,2,3, 陈曦1,2,3, 王谨1,2,詹明生1,2   

  1. 1中国科学院武汉物理与数学研究所波谱与原子分子国家重点实验室-武汉光电国家实验室, 湖北 武汉 430071; 
    2中国科学院冷原子物理中心, 湖北  武汉 430071 ;
    3 中国科学院研究生院, 北京 100049
  • 收稿日期:2010-11-05 修回日期:2010-11-16 出版日期:2011-11-28 发布日期:2011-11-14
  • 通讯作者: 詹明生(1961- )研究员, 研究方向为冷原子物理与量子信息。 E-mail:mszhan@wipm.ac.cn
  • 基金资助:

    This work was supported by the National Basic Research Program of China under Grant No. 2006CB921203, by the National Natural Science Foundation of China under Grant Nos. 10827404 and 10804124, and also by funds from the Chinese Academy of Sciences

Frequency stabilization of 480 nm laser using two-photon DAVLL

XU Peng 1,2,3, CHEN Xi 1,2,3, WANG Jin 1,2 , ZHAN Ming-sheng 1,2   

  1. 1 State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan National Laboratory for Optoelectronics, Wuhan 430071, China;
    2 Center for Cold Atom Physics, Chinese Academy of Sciences, Wuhan 430071, China;
    3 Graduate University of  Chinese Academy of Sciences, Beijing 100049, China
  • Received:2010-11-05 Revised:2010-11-16 Published:2011-11-28 Online:2011-11-14

摘要:

480nm激光的稳频对于实现铷原子从基态双光子相干激发到里德堡态必不可少。本工作基于梯形构型下的电磁诱导透明现象,一种新的480nm激光器稳频技术采用偏振谱稳频的780nm激光作为探测光而480nm激光则作为耦合光,在外加偏置磁场作用下产生的双光子双色原子气体激光锁频(DAVLL)谱方法,将该谱信号通过比例-积分-微分电路后反馈回480nm激光器即可实现稳频。在频率锁定后,480nm激光器和780nm激光器长时间稳频的总线宽为1MHz左右。

关键词: 激光技术, 激光稳频, 双光子双色原子气体激光锁频, 里德堡态跃迁

Abstract:

Frequency stabilization of a diode laser at 480nm is crucial for coherently exciting rubidium atoms to Rydberg states. Here reported is a laser laser frequency stabilization experimenttechnique techniques based on electromagnetically induced transparency in a ladder con?guration with a polarization spectroscopy stabilized 780nm diode laser as the probe laser and a 480nm laser as the coupling laser. With a uniform magnetic ?eld, a two-photon dichroic atomic vapor laser lock (DAVLL) spectroscopy iswas generated. Then this spectroscopy was and fed back through two proportion -integral -differential circuits to lock the 480nm diode laser. A combined linewidth of about 1MHz is achieved during the locking period.

Key words: laser techniques, laser frequency stabilization, two-photon dichroic atomic vapor laser lock, Rydberg transition

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