Chinese Optics, Volume. 18, Issue 3, 661(2025)

Ultralow residual phase noise frequency synthesizer for space gravitational wave detection

Lei-gang WANG1,2, En-xue YUN1,2、*, Xin LUO1,2, Teng-hui YANG1,2, Bi-song WANG1,2, Si-yu SUN1,2, Cheng-yun LI1,2, Jun-liang LIU1,2, Rui-hong GAO2,3,4, Feng ZHAO2,5, and Shou-gang ZHANG1,2
Author Affiliations
  • 1NTSC, Chinese Academy of Science, Xi’an 710600, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Institute of Mechanics, Chinese Academy of Sciences, Beijing 100190, China
  • 4Hangzhou Institute for Advanced Study, UCAS, Hangzhou 310024, China
  • 5Innovation Academy for Precision Measurement Science and Technology, Wuhan 430071, China
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    Figures & Tables(10)
    Structure of frequency synthesizer link
    (a) Principle diagram and (b) spectrum diagram of a 24th-order direct frequency multiplier. Illustration: physical photo of the 24th-order frequency multiplier. The RBW and VBW of the spectrum analyzer are both 91 Hz
    (a) Principle diagram and (b) spectrum diagram of a 2.4 GHz PDRO. Illustration: physical photo of the 2.4 GHz PDRO. The RBW and VBW of the spectrum analyzer are both 91 Hz
    The absolute phase noise of the frequency synthesizer system and key components. Illustration: absolute phase noise test configuration
    Schematic diagram of residual phase noise measurement
    Residual phase noise of the 2.4 GHz frequency synthesizer system
    Residual phase noise of the 75 MHz frequency synthesizer system and key components. Illustration: residual phase noise in the 1 mHz–100 mHz range
    Experimental results of phase temperature sensitivity. (a) and (c) represent temperature variation sequence; (b) temperature sensitivity of the output microwave phase in the 24-order frequency multiplication system; (d) temperature sensitivity of the output microwave phase in the PDRO
    Residual frequency stability of the frequency synthesizer system and the theoretical limit
    • Table 1. Residual phase noise measurement results and Taiji program requirements (rad·Hz\begin{document}${}^{-\frac{1}{2}} $\end{document})

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      Table 1. Residual phase noise measurement results and Taiji program requirements (rad·Hz\begin{document}${}^{-\frac{1}{2}} $\end{document})

      频偏太极计划残余相噪需求2.4 GHz频综残余相噪75 MHz频综残余相噪
      0.1 mHz$ 5.79\times {10}^{-3} $$ \leqslant 1.06\times {10}^{-3} $$ 1.06\times {10}^{-3} $
      1 mHz$ 5.93\times {10}^{-5} $$ \leqslant 8.18\times {10}^{-5} $$ 8.18\times {10}^{-5} $
      10 mHz$ 6.30\times {10}^{-6} $$ 1.19\times {10}^{-6} $$ 7.63\times {10}^{-6} $
      100 mHz$ 6.28\times {10}^{-6} $$ 2.22\times {10}^{-7} $$ 1.30\times {10}^{-6} $
      1 Hz$ 6.28\times {10}^{-6} $$ 6.96\times {10}^{-8} $$ 1.53\times {10}^{-7} $
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    Lei-gang WANG, En-xue YUN, Xin LUO, Teng-hui YANG, Bi-song WANG, Si-yu SUN, Cheng-yun LI, Jun-liang LIU, Rui-hong GAO, Feng ZHAO, Shou-gang ZHANG. Ultralow residual phase noise frequency synthesizer for space gravitational wave detection[J]. Chinese Optics, 2025, 18(3): 661

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    Paper Information

    Category: Special Column on Space-based Gravitational Wave Detection

    Received: Jan. 21, 2025

    Accepted: --

    Published Online: Jun. 16, 2025

    The Author Email:

    DOI:10.37188/CO.2025-0015

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