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作 者:SUN Zhen JIA Feng-Dong LV Shuang-Fei RUAN Ya-Ping QING Bo XUE Ping XU Xiang-yuan DAI Xing-Can ZHONG Zhi-Ping
机构地区:[1]School of Physics, University of Chinese Academy of Sciences, Beijing 100049 [2]State Key Laboratory of Low-dimensional Quantum Physics, Department of Physics,Tsinghua University and Collaborative Innovation Center of Quantum M~tter, Beijing 100084 [3]Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900 [4]Department of Physics, Capital Normal University, Beijing 100037
出 处:《Chinese Physics Letters》2014年第4期33-36,共4页中国物理快报(英文版)
基 金:Supported by the National Natural Science Foundation of China under Grant No 11074299, and the Open Research Fund Program of the State Key Laboratory of Low-Dimensional Quantum Physics.
摘 要:The probe transmission spectra around the atomic transition 52S1/2,F = 2 → 52P3/2,F = 2 of 87Rb are measured in a magneto-optical trap by adding a coupling field around the atomic transition 52S1/2, F = 2 → 52 P3/2, F1 = 2. The inversionless amplification is observed in the spectrum over the atomic transition 5 2 S1/2, F = 2 → 52pa/2, Fr = 2. The tripod eleetromagnetically induced transparency is proposed to account for the ampli- fication feature, in which population distributions among these related atomic levels play an important role.The probe transmission spectra around the atomic transition 52S1/2,F = 2 → 52P3/2,F = 2 of 87Rb are measured in a magneto-optical trap by adding a coupling field around the atomic transition 52S1/2, F = 2 → 52 P3/2, F1 = 2. The inversionless amplification is observed in the spectrum over the atomic transition 5 2 S1/2, F = 2 → 52pa/2, Fr = 2. The tripod eleetromagnetically induced transparency is proposed to account for the ampli- fication feature, in which population distributions among these related atomic levels play an important role.
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