论文标题

高对比度干涉测量法原子束源的三维冷却

Three-dimensional cooling of an atom beam source for high-contrast atom interferometry

论文作者

Kwolek, J. M., Fancher, C. T., Bashkansky, M., Black, Adam

论文摘要

我们提出了一个紧凑的两阶段原子束源,该光束源产生连续,狭窄,准直和高频束的rubidium原子,并在三个维度上具有子多普勒温度,这具有沿原子轨迹的近谐和荧光发射非常低的发射。原子束源源于推动的二维磁磁陷阱(2d $^+$ mot),供应一个稍微离轴的三维运动光学糖蜜阶段,该阶段不断冷却并重定向原子束。故意选择移动光学糖蜜的捕获速度为低,$ \ sim 3 $ m/s,以减少荧光,并因谐振的几个原子宽度而降低冷却光,以减少冷却诱导荧光的吸收横截面。 2d $^+$ mot的近谐波和推动梁不会传播到原子轨迹10度弯曲而导致的原子轨迹。从两阶段发射的原子梁的通量高达$ 1.6(3)\ times 10^9 \; \ textrm {atoms/s} $,优化温度为$ 15.0(2)\;μ$ k。我们在原子束输出处采用连续的拉曼 - 拉姆西干扰测量值,以研究在存在连续冷却的情况下的变质来源,并证明原子束源即使在冷却过程中也可以有效地保持高条纹对比度。这种冷原子光束源适合用于原子干涉仪和时钟,在该原子干涉仪和时钟中,连续操作消除了死亡时间,缓慢的原子束速度(6-16 m/s)可提高敏感性,狭窄的3D速度分布可改善边缘对比度,而散射的光线降低的腐蚀性较低,由持续的腐蚀剂引起的连续冷却过程。

We present a compact, two-stage atomic beam source that produces a continuous, narrow, collimated and high-flux beam of rubidium atoms with sub-Doppler temperatures in three dimensions, which features very low emission of near-resonance fluorescence along the atomic trajectory. The atom beam source originates in a pushed two-dimensional magneto-optical trap (2D$^+$ MOT) feeding a slightly off-axis three-dimensional moving optical molasses stage that continuously cools and redirects the atom beam. The capture velocity of the moving optical molasses is deliberately chosen to be low, $\sim 3$ m/s, to reduce fluorescence, and the cooling light is detuned by several atomic linewidths from resonance to reduce the absorption cross-section of cooling-induced fluorescence. Near-resonance light from the 2D$^+$ MOT and the push beam does not propagate to the output atomic trajectory due to a 10 degree bend in the atomic trajectory. The atomic beam emitted from the two-stage source has a flux up to $1.6(3)\times 10^9\;\textrm{atoms/s}$, with an optimized temperature of $15.0(2)\;μ$K. We employ continuous Raman-Ramsey interference measurements at the atom beam output to study the sources of decoherence in the presence of continuous cooling, and demonstrate that the atom beam source effectively preserves high fringe contrast even during cooling. This cold-atom beam source is appropriate for use in atom interferometers and clocks, where continuous operation eliminates dead time, the slow atom beam velocity (6 - 16 m/s) improves sensitivity, the narrow 3D velocity distribution improves fringe contrast, and the low reabsorption of scattered light mitigates decoherence caused by the continuous cooling process.

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