Photonics Research, Volume. 12, Issue 11, 2741(2024)

Reducing statistical noise in frequency ratio measurement between Ca+ and Sr optical clocks with a frequency-synthesized local oscillator from a Sr optical clock

Haosen Shi1、†, Bingkun Lu2,3,4、†, Huaqing Zhang5,6、†, Ruming Hu5,6,7, Yuan Qian5,6,7, Yao Huang5,6, Tao Yang2,4, Yuan Yao1, Hongfu Yu1, Zhanjun Fang2,4, Kelin Gao5,6, Hua Guan5,6,8,9、*, Yige Lin2,4,10、*, Yanyi Jiang1,11、*, and Longsheng Ma1
Author Affiliations
  • 1State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062, China
  • 2Division of Time and Frequency Metrology, National Institute of Metrology, Beijing 100029, China
  • 3Key Laboratory of Atomic Frequency Standards, Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences, Wuhan 430071, China
  • 4Key Laboratory of State Administration for Market Regulation (Time Frequency and Gravity Primary Standard), Beijing 100029, China
  • 5Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences, Wuhan 430071, China
  • 6Department of Precision Instrument, Tsinghua University, Beijing 100084, China
  • 7University of Chinese Academy of Sciences, Beijing 100049, China
  • 8Wuhan Institute of Quantum Technology, Wuhan 430206, China
  • 9e-mail: guanhua@apm.ac.cn
  • 10e-mail: linyige@nim.ac.cn
  • 11e-mail: yyjiang@phy.ecnu.edu.cn
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    Figures & Tables(5)
    Timing control sequence for (a) Ca+ optical clock and (b) Sr optical lattice clock.
    (a) Schematic of the experiment setup. AOM, acoustic-optic modulator; NCF, noise canceled fiber link; DDS, direct digital synthesizer; OFD, optical frequency divider. The red straight line and the black dashed line stand for the optical path and electric control path, respectively. (b) Noise cancelation scheme for frequency noise of the comb used in OFD. The method to generate the optically referenced time base fCLK is also shown on the right side.
    Measured Rabi spectra of the Ca+ clock transition with 100 times averaging at each frequency point. The probe time is 160 ms (green circles), 320 ms (blue circles), and 640 ms (purple dots), respectively. The dashed lines and shaded regions are the corresponding fits to the measured data using the Rabi model and their 1−σ confidence intervals.
    Overlapping Allan deviation of the frequency ratio measurement. The LO of Ca+ clock is frequency-synthesized from the Sr clock by OFD (red dots and blue squares for Tp=80 ms and 160 ms, respectively). The dashed lines are weighted 1/τ fits to the measured frequency ratio data for an averaging time greater than 100 s. Error bars indicate 1−σ confidence intervals. A previous result with independent LOs for the Ca+ and Sr clocks is shown for reference (purple circles) [36].
    Frequency instability of a single Ca+ clock measured by the time-interleaved self-comparison method with a probe time of 80 ms (red triangles), 160 ms (purple dots), and 320 ms (blue squares). The LO of the Ca+ clock is frequency-synthesized from the cavity-stabilized 698 nm laser with the OFD. The dashed lines are the weighted 1/τ fits to Tp=80 ms, 160 ms, and 320 ms data for an averaging time greater than 100 s. Error bars indicate 1−σ confidence intervals.
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    Haosen Shi, Bingkun Lu, Huaqing Zhang, Ruming Hu, Yuan Qian, Yao Huang, Tao Yang, Yuan Yao, Hongfu Yu, Zhanjun Fang, Kelin Gao, Hua Guan, Yige Lin, Yanyi Jiang, Longsheng Ma, "Reducing statistical noise in frequency ratio measurement between Ca+ and Sr optical clocks with a frequency-synthesized local oscillator from a Sr optical clock," Photonics Res. 12, 2741 (2024)

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    Paper Information

    Category: Instrumentation and Measurements

    Received: Aug. 20, 2024

    Accepted: Sep. 22, 2024

    Published Online: Nov. 1, 2024

    The Author Email: Hua Guan (guanhua@apm.ac.cn), Yige Lin (linyige@nim.ac.cn), Yanyi Jiang (yyjiang@phy.ecnu.edu.cn)

    DOI:10.1364/PRJ.539892

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