The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency Shift

被引:0
|
作者
Bai, Yang [1 ,2 ,3 ]
Wang, Xinliang [1 ,2 ]
Shi, Junru [1 ,2 ,3 ]
Yang, Fan [1 ,2 ,3 ]
Ruan, Jun [1 ,2 ]
Dong, Ruifang [1 ,2 ]
Zhang, Shougang [1 ,2 ]
机构
[1] Chinese Acad Sci, Natl Time Serv Ctr, Shu Yuan Rd, Xian 710600, Peoples R China
[2] Chinese Acad Sci, Natl Time Serv Ctr, Key Lab Time & Frequency Primary Stand, Xian 710600, Peoples R China
[3] Univ Chinese Acad Sci, Yu Quan Rd, Beijing 100049, Peoples R China
基金
中国国家自然科学基金;
关键词
cesium atomic fountain clock; second-order Zeeman frequency shift; low-frequency transition; ACCURACY EVALUATION; CESIUM FOUNTAIN; CLOCK;
D O I
10.3390/s21248333
中图分类号
O65 [分析化学];
学科分类号
070302 ; 081704 ;
摘要
Second-order Zeeman frequency shift is one of the major systematic factors affecting the frequency uncertainty performance of cesium atomic fountain clock. Second-order Zeeman frequency shift is calculated by experimentally measuring the central frequency of the (1,1) or (-1,-1) magnetically sensitive Ramsey transition. The low-frequency transition method can be used to measure the magnetic field strength and to predict the central fringe of (1,1) or (-1,-1) magnetically sensitive Ramsey transition. In this paper, we deduce the formula for magnetic field measurement using the low-frequency transition method and measured the magnetic field distribution of 4 cm inside the Ramsey cavity and 32 cm along the flight region experimentally. The result shows that the magnetic field fluctuation is less than 1 nT. The influence of low-frequency pulse signal duration on the accuracy of magnetic field measurement is studied and the optimal low-frequency pulse signal duration is determined. The central fringe of (-1,-1) magnetically sensitive Ramsey transition can be predicted by using a numerical integrating of the magnetic field "map". Comparing the predicted central fringe with that identified by Ramsey method, the frequency difference between these two is, at most, a fringe width of 0.3. We apply the experimentally measured central frequency of the (-1,-1) Ramsey transition to the Breit-Rabi formula, and the second-order Zeeman frequency shift is calculated as 131.03 x 10(-15), with the uncertainty of 0.10 x 10(-15).
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页数:10
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