首页> 外文会议>International school on quantum electronics: laser physics and applications >Multiple peaks due to EIT and Autler-Townes effect in Lambda-probing of the strongly driven 5P_(3/2) manifold of cold (85)~Rb atoms in MOT
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Multiple peaks due to EIT and Autler-Townes effect in Lambda-probing of the strongly driven 5P_(3/2) manifold of cold (85)~Rb atoms in MOT

机译:MOT中冷(85)〜Rb原子的强驱动5P_(3/2)流形的Lambda探测中,由于EIT和Autler-Townes效应而导致的多个峰

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Electromagnetically induced transparency (EIT) and Autler-Townes (A-T) effect were studied under conditions of strong coupling of the hyperfine manifold 5p_(3/2)(F') with the 5S_(1/2)(F=2) ground state of cold (85)~Rb atoms in MOT. Transmission spectra of a weak probe beam, at the frequency scanned in the vicinity of the 5S_(1/2)(F=3)→5P(3/2)(F') resonances were registered at various frequency settings of the coupling beam. The spectra were interpreted by applying optical Bloch equations. As a starting point, a 5-level model, accounting for F=2, 3 and F'=1, 2, 3 states was assumed (the non-coupled state F'=4 being neglected, but the F'=1 state, coupled but not directly probed, included, as its presence was found to be imprinted in the spectra). Such a model alone does not reproduce all the spectral features observed. Therefore we have considered the existence of the polarized light induced transitions between Zeeman substates, involving (F'=2, m') and (F'=3, m') upper states. In order to indirectly account for the m→m' absorption transitions to the non-coupled m' states, and to the pairs of states with incomplete coupling, we have complemented the results of the 5-level model with the ones of its reduced versions. Satisfactory agreement of the positions of respective modeled and experimental spectral peaks was achieved.
机译:在超细歧管5p_(3/2)(F')与5S_(1/2)(F = 2)基态强耦合的条件下,研究了电磁感应透明度(EIT)和奥特勒-唐纳斯(AT)效应MOT中的冷(85)〜Rb原子数。在耦合光束的各种频率设置下,记录了在5S_(1/2)(F = 3)→5P(3/2)(F')共振附近扫描的频率下的弱探测光束的透射光谱。 。通过应用光学Bloch方程来解释光谱。首先,假设一个五级模型,说明了F = 2、3和F'= 1、2、3个状态(忽略了非耦合状态F'= 4,但是F'= 1状态包括耦合但未直接探测到的,因为发现它的存在已在光谱中留下了印记)。单独这样的模型并不能再现观察到的所有光谱特征。因此,我们考虑了在(F'= 2,m')和(F'= 3,m')上态之间在Zeeman子态之间存在偏振光诱导的跃迁。为了间接地解释m→m'到非耦合m'态以及不完全耦合的状态对的吸收跃迁,我们用其简化形式对5级模型的结果进行了补充。各个建模和实验光谱峰的位置均令人满意。

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