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铯原子 D 跃迁的Λ增强灰色糖浆。

Λ-enhanced grey molasses on the D transition of Rubidium-87 atoms.

机构信息

LENS European Laboratory for Non-Linear Spectroscopy, and Dipartimento di Fisica e Astronomia, Università di Firenze, Sesto Fiorentino, 50019, Italy.

Istituto Nazionale di Ottica, INO-CNR, Sesto Fiorentino, 50019, Italy.

出版信息

Sci Rep. 2018 Jan 22;8(1):1301. doi: 10.1038/s41598-018-19814-z.

DOI:10.1038/s41598-018-19814-z
PMID:29358635
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5778025/
Abstract

Laser cooling based on dark states, i.e. states decoupled from light, has proven to be effective to increase the phase-space density of cold trapped atoms. Dark-states cooling requires open atomic transitions, in contrast to the ordinary laser cooling used for example in magneto-optical traps (MOTs), which operate on closed atomic transitions. For alkali atoms, dark-states cooling is therefore commonly operated on the D transition nS → nP. We show that, for Rb, thanks to the large hyperfine structure separations the use of this transition is not strictly necessary and that "quasi-dark state" cooling is efficient also on the D line, 5S → 5P. We report temperatures as low as (4.0 ± 0.3) μK and an increase of almost an order of magnitude in the phase space density with respect to ordinary laser sub-Doppler cooling.

摘要

基于暗态的激光冷却,即与光解耦的状态,已被证明可以有效地增加冷捕获原子的相空间密度。与例如用于磁光阱 (MOT) 的普通激光冷却相比,暗态冷却需要开放的原子跃迁,后者则在封闭的原子跃迁上运行。因此,对于碱金属原子,暗态冷却通常在 D 跃迁 nS → nP 上进行。我们表明,对于 Rb,由于大的超精细结构分离,使用此跃迁并非严格必要,并且“准暗态”冷却在 D 线 5S → 5P 上也很有效。我们报告的温度低至 (4.0 ± 0.3) μK,与普通激光亚多普勒冷却相比,相空间密度增加了近一个数量级。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/d3ced7082904/41598_2018_19814_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/303e3c8eb768/41598_2018_19814_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/79b6c7bb4016/41598_2018_19814_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/8439b08a80d1/41598_2018_19814_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/689ea9381088/41598_2018_19814_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/f8d162466edc/41598_2018_19814_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/1a74fd5589a1/41598_2018_19814_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/d3ced7082904/41598_2018_19814_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/303e3c8eb768/41598_2018_19814_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/79b6c7bb4016/41598_2018_19814_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/8439b08a80d1/41598_2018_19814_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/689ea9381088/41598_2018_19814_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/f8d162466edc/41598_2018_19814_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/1a74fd5589a1/41598_2018_19814_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5b2b/5778025/d3ced7082904/41598_2018_19814_Fig7_HTML.jpg

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