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首页> 外文期刊>The Journal of Chemical Physics >Stark-induced adiabatic Raman passage examined through the preparation of D-2 (v=2, j=0) and D-2 (v=2, j=2, m=0)
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Stark-induced adiabatic Raman passage examined through the preparation of D-2 (v=2, j=0) and D-2 (v=2, j=2, m=0)

机译:通过D-2的制备检查的Stark诱导的绝热拉曼通道(v = 2,j = 0)和d-2(v = 2,j = 2,m = 0)

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摘要

We study the conditions that must be met for successful preparation of a large ensemble in a specific target quantum state using Stark-induced adiabatic Raman passage (SARP). In particular, we show that the threshold condition depends on the relative magnitudes of the Raman polarizability (r(0v)) and the difference of the optical polarizabilities ((00vj)) of the initial (v = 0, j = 0) and the target (v, j) rovibrational levels. Here, v and j are the vibrational and rotational quantum numbers, respectively. To illustrate how the operation of SARP is controlled by these two parameters, we experimentally prepared D-2 (v = 2, j = 0) and D-2 (v = 2, j = 2, m = 0) in a beam of D-2 (v = 0, j = 0) molecules using a sequence of partially overlapping pump and Stokes laser pulses. By comparing theory and experiment, we were able to determine the Raman polarizability r(02) approximate to 0.3 x 10(-41) Cm/(V/m) and the difference polarizabilities (0020) approximate to 1.4 x 10(-41) Cm/(V/m) and (0022) approximate to 3.4 x 10(-41) Cm/(V/m) for the two Raman transitions. Our experimental data and theoretical calculations show that because the ratio r/ is larger for the (0,0) (2,0) transition than the (0,0) (2,2) transition, much less optical power is required to transfer a large population to the (v = 2, j = 0) level. Nonetheless, our experiment demonstrates that substantial population transfer to both the D-2 (v = 2, j = 0) and D-2 (v = 2, j = 2, m = 0) is achieved using appropriate laser fluences. Our derived threshold condition demonstrates that with increasing vibrational quantum number, it becomes more difficult to achieve large amounts of population transfer.
机译:我们研究了使用STARK诱导的绝热拉曼通道(SARP)在特定目标量子状态下成功制备大型集成的条件。特别地,我们表明阈值条件取决于拉曼偏振性(R(0V))的相对幅度,并且初始(v = 0,j = 0)和的光学偏光((00v))的差异目标(v,j)鲁维奇水平。这里,V和J分别是振动和旋转量子数。为了说明SARP的操作是如何通过这两个参数控制的,我们在一束中通过实验制备的D-2(v = 2,j = 0)和d-2(v = 2,j = 2,m = 0) D-2(v = 0,j = 0)使用部分重叠泵和斯托克斯激光脉冲序列的分子。通过比较理论和实验,我们能够确定拉曼偏振性R(02)近似为0.3×10(-41)cm /(v / m),差异偏振率(0020)近似为1.4 x 10(-41) CM /(v / m)和(0022)近似为两个拉曼转换的3.4×10(-41)cm /(v / m)。我们的实验数据和理论计算表明,因为(0,0)(2,0)转换比(0,0)转换的比率R /更大,所以需要更少的光功率大量的人口(v = 2,j = 0)级别。尽管如此,我们的实验表明,使用适当的激光流量将实现对D-2(v = 2,j = 0)和d-2(v = 2,j = 2,m = 0)的大量群体转移。我们的衍生阈值条件表明,随着振动量子数的增加,实现大量人口转移变得更加困难。

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