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基于光钟的长达数月的时间尺度实时生成。

Months-long real-time generation of a time scale based on an optical clock.

作者信息

Hachisu Hidekazu, Nakagawa Fumimaru, Hanado Yuko, Ido Tetsuya

机构信息

National Institute of Information and Communications Technology, 4-2-1 Nukui-kitamachi, Koganei, Tokyo, 184-8795, Japan.

出版信息

Sci Rep. 2018 Mar 9;8(1):4243. doi: 10.1038/s41598-018-22423-5.

DOI:10.1038/s41598-018-22423-5
PMID:29523792
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5844947/
Abstract

Time scales consistently provide precise time stamps and time intervals by combining atomic frequency standards with a reliable local oscillator. Optical frequency standards, however, have not been applied to the generation of time scales, although they provide superb accuracy and stability these days. Here, by steering an oscillator frequency based on the intermittent operation of a Sr optical lattice clock, we realized an "optically steered" time scale TA(Sr) that was continuously generated for half a year. The resultant time scale was as stable as International Atomic Time (TAI) with its accuracy at the 10 level. We also compared the time scale with TT(BIPM16). TT(BIPM) is computed in deferred time each January based on a weighted average of the evaluations of the frequency of TAI using primary and secondary frequency standards. The variation of the time difference TA(Sr) - TT(BIPM16) was 0.79 ns after 5 months, suggesting the compatibility of using optical clocks for time scale generation. The steady signal also demonstrated the capability to evaluate one-month mean scale intervals of TAI over all six months with comparable uncertainties to those of primary frequency standards (PFSs).

摘要

时间尺度通过将原子频率标准与可靠的本地振荡器相结合,始终如一地提供精确的时间戳和时间间隔。然而,光学频率标准尽管如今已具备超高的精度和稳定性,但尚未应用于时间尺度的生成。在此,通过基于锶光学晶格钟的间歇运行来控制振荡器频率,我们实现了一个持续生成半年的“光学控制”时间尺度TA(Sr)。所得时间尺度与国际原子时(TAI)一样稳定,其精度达到10^-18量级。我们还将该时间尺度与TT(BIPM16)进行了比较。TT(BIPM)每年1月根据使用一级和二级频率标准对TAI频率评估的加权平均值在延迟时间内计算得出。5个月后,时间差TA(Sr) - TT(BIPM16)的变化为0.79纳秒,这表明使用光学时钟生成时间尺度具有兼容性。该稳定信号还展示了在所有六个月内评估TAI一个月平均尺度间隔的能力,其不确定性与一级频率标准(PFS)相当。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/2d66bc1b64c0/41598_2018_22423_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/649910caf4eb/41598_2018_22423_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/7ba8ede6054f/41598_2018_22423_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/00ca93e72812/41598_2018_22423_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/4f9ea3d6db77/41598_2018_22423_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/8e8f2296904f/41598_2018_22423_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/af4b2e82f8e1/41598_2018_22423_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/2d66bc1b64c0/41598_2018_22423_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/649910caf4eb/41598_2018_22423_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/7ba8ede6054f/41598_2018_22423_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/00ca93e72812/41598_2018_22423_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/4f9ea3d6db77/41598_2018_22423_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/8e8f2296904f/41598_2018_22423_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/af4b2e82f8e1/41598_2018_22423_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81e3/5844947/2d66bc1b64c0/41598_2018_22423_Fig7_HTML.jpg

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