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利用激光冷却原子产生的超冷分子测量电子与质子质量比的变化。

Measurement of the variation of electron-to-proton mass ratio using ultracold molecules produced from laser-cooled atoms.

作者信息

Kobayashi J, Ogino A, Inouye S

机构信息

Department of Physics, Graduate School of Science, Kyoto University, Kyoto, 606-8502, Japan.

PRESTO, Japan Science and Technology Agency, Kyoto, 606-8502, Japan.

出版信息

Nat Commun. 2019 Aug 21;10(1):3771. doi: 10.1038/s41467-019-11761-1.

DOI:10.1038/s41467-019-11761-1
PMID:31434889
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6704166/
Abstract

Experimental techniques to manipulate cold molecules have seen great development in recent years. The precision measurements of cold molecules are expected to give insights into fundamental physics. Here we use a rovibrationally pure sample of ultracold KRb molecules to improve the measurement on the stability of electron-to-proton mass ratio [Formula: see text]. The measurement is based upon a large sensitivity coefficient of the molecular spectroscopy, which utilizes a transition between a nearly degenerate pair of vibrational levels each associated with a different electronic potential. Observed limit on temporal variation of μ is [Formula: see text], which is better by a factor of five compared with the most stringent laboratory molecular limits to date. Further improvements should be straightforward, because our measurement was only limited by statistical errors.

摘要

近年来,用于操控冷分子的实验技术取得了巨大发展。冷分子的精确测量有望为基础物理学提供深刻见解。在此,我们使用超冷KRb分子的振转纯样品来改进对电子与质子质量比稳定性的测量[公式:见原文]。该测量基于分子光谱的高灵敏度系数,利用了一对近乎简并的振动能级之间的跃迁,每个能级与不同的电子势能相关。观测到的μ随时间变化的极限为[公式:见原文],与迄今为止最严格的实验室分子极限相比,提高了五倍。进一步的改进应该很简单,因为我们的测量仅受统计误差限制。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/3db6cdbd39ca/41467_2019_11761_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/bcf403ef9b73/41467_2019_11761_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/4e4f80939d56/41467_2019_11761_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/cbbc1f65bdca/41467_2019_11761_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/3db6cdbd39ca/41467_2019_11761_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/bcf403ef9b73/41467_2019_11761_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/4e4f80939d56/41467_2019_11761_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/cbbc1f65bdca/41467_2019_11761_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b826/6704166/3db6cdbd39ca/41467_2019_11761_Fig4_HTML.jpg

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