用塞曼调谐技术制造慢原子的超窄速度分布

S. Zilio, V. Bagnato
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引用次数: 0

摘要

我们报道了在慢速原子束中使用受激拉曼跃迁来产生选定电子状态下原子的窄速度分布,这可用于低温状态下的原子碰撞研究(1)。速度选择是减速过程的一部分,在这个意义上它是独一无二的。反传播激光束施加在原子上的辐射压力使原子束减速。由于塞曼用空间不均匀磁场调谐电子子电平(2)来补偿多普勒频移的变化,因此沿减速路径保持了共振条件。在慢化过程结束时,初始麦克斯韦-玻尔兹曼分布被压缩为一个以v = 0附近为中心的窄速度分布(Δv ~ 50 m/s)。这种速度聚集(3)大大增加了每个速度类别中的原子数量,从而允许使用速度选择技术作为研究低速碰撞的可行方法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Ultra-Narrow Velocity Distributions of Slow Atoms Produced with the Zeeman Tuning Technique
We report on the use of a stimulated Raman transition in a slowed atomic beam to produce a narrow velocity distribution of atoms in a selected electronic state, which could be used for atomic collisions studies in the low temperature regime(1). The velocity selection is part of the deceleration process and in this sense it is unique. The atomic beam is decelerated by the radiation pressure force exerted on the atoms by a counter- propagating laser beam. The resonance condition is maintained along the deceleration path because the changing Doppler shift is compensated by Zeeman tuning the electronic sublevels(2) with a spatialy inhomogneous magnetic field. At the end of the slowing process, the initial Maxwell-Boltzman distribution is compressed to a narrow velocity distribution (Δv ~ 50 m/s), centered close to v = 0. This velocity bunching(3) increases considerably the number of atoms in each velocity class, allowing the use of velocity selection techniques as a feasible way of studying low velocity collisions.
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