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

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 sensiti...

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Main Authors: Yang Bai, Xinliang Wang, Junru Shi, Fan Yang, Jun Ruan, Ruifang Dong, Shougang Zhang
Format: Article
Language:English
Published: MDPI AG 2021-12-01
Series:Sensors
Subjects:
Online Access:https://www.mdpi.com/1424-8220/21/24/8333
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author Yang Bai
Xinliang Wang
Junru Shi
Fan Yang
Jun Ruan
Ruifang Dong
Shougang Zhang
author_facet Yang Bai
Xinliang Wang
Junru Shi
Fan Yang
Jun Ruan
Ruifang Dong
Shougang Zhang
author_sort Yang Bai
collection DOAJ
description 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 × 10<sup>−15</sup>, with the uncertainty of 0.10 × 10<sup>−15</sup>.
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spelling doaj.art-babf802fd6504cdfb696d471ff13cdb22023-11-23T10:30:00ZengMDPI AGSensors1424-82202021-12-012124833310.3390/s21248333The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency ShiftYang Bai0Xinliang Wang1Junru Shi2Fan Yang3Jun Ruan4Ruifang Dong5Shougang Zhang6National Time Service Center, Chinese Academy of Sciences, Shu Yuan Road, Xi’an 710600, ChinaNational Time Service Center, Chinese Academy of Sciences, Shu Yuan Road, Xi’an 710600, ChinaNational Time Service Center, Chinese Academy of Sciences, Shu Yuan Road, Xi’an 710600, ChinaNational Time Service Center, Chinese Academy of Sciences, Shu Yuan Road, Xi’an 710600, ChinaNational Time Service Center, Chinese Academy of Sciences, Shu Yuan Road, Xi’an 710600, ChinaNational Time Service Center, Chinese Academy of Sciences, Shu Yuan Road, Xi’an 710600, ChinaNational Time Service Center, Chinese Academy of Sciences, Shu Yuan Road, Xi’an 710600, ChinaSecond-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 × 10<sup>−15</sup>, with the uncertainty of 0.10 × 10<sup>−15</sup>.https://www.mdpi.com/1424-8220/21/24/8333cesium atomic fountain clocksecond-order Zeeman frequency shiftlow-frequency transition
spellingShingle Yang Bai
Xinliang Wang
Junru Shi
Fan Yang
Jun Ruan
Ruifang Dong
Shougang Zhang
The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency Shift
Sensors
cesium atomic fountain clock
second-order Zeeman frequency shift
low-frequency transition
title The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency Shift
title_full The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency Shift
title_fullStr The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency Shift
title_full_unstemmed The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency Shift
title_short The Application of Low-Frequency Transition in the Assessment of the Second-Order Zeeman Frequency Shift
title_sort application of low frequency transition in the assessment of the second order zeeman frequency shift
topic cesium atomic fountain clock
second-order Zeeman frequency shift
low-frequency transition
url https://www.mdpi.com/1424-8220/21/24/8333
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