• Acta Photonica Sinica
  • Vol. 53, Issue 8, 0814003 (2024)
Junchao GAO, Junjie CHEN, Liuxian YE, Bing CHENG..., Bin WU, Helin WANG*, Xiaolong WANG and Qiang LIN|Show fewer author(s)
Author Affiliations
  • Zhejiang Provincial Key Laboratory of Quantum Precision Measurement, College of Science, Zhejiang University of Technology, Hangzhou 310023, China
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    DOI: 10.3788/gzxb20245308.0814003 Cite this Article
    Junchao GAO, Junjie CHEN, Liuxian YE, Bing CHENG, Bin WU, Helin WANG, Xiaolong WANG, Qiang LIN. Research on Fiber Raman Laser Source for Mobile Quantum Gravimeter[J]. Acta Photonica Sinica, 2024, 53(8): 0814003 Copy Citation Text show less
    Low phase noise and narrow linewidth Raman fiber laser system
    Fig. 1. Low phase noise and narrow linewidth Raman fiber laser system
    Noise model of optical phase-locked loop in the narrow linewidth Raman fiber laser
    Fig. 2. Noise model of optical phase-locked loop in the narrow linewidth Raman fiber laser
    The influence of Raman phase noise on the sensitivity of gravimeter under different T and τ value
    Fig. 3. The influence of Raman phase noise on the sensitivity of gravimeter under different T and τ value
    Power spectral density of phase noise of Raman beat signal. Illustration : beat signal diagram
    Fig. 4. Power spectral density of phase noise of Raman beat signal. Illustration : beat signal diagram
    The gravity sensitivity limit and total phase noise at different beat optical power ratios
    Fig. 5. The gravity sensitivity limit and total phase noise at different beat optical power ratios
    The phase noise power spectral density of the laser system with different 7G signal sources and different 7G sources is analyzed.
    Fig. 6. The phase noise power spectral density of the laser system with different 7G signal sources and different 7G sources is analyzed.
    Phase noise spectral density of Raman laser system and different devices in the system.
    Fig. 7. Phase noise spectral density of Raman laser system and different devices in the system.
    Phase noise and gravity sensitivity in different frequency bands
    Fig. 8. Phase noise and gravity sensitivity in different frequency bands
    Stability of phase noise and gravity sensitivity of Raman fiber laser
    Fig. 9. Stability of phase noise and gravity sensitivity of Raman fiber laser
    Frequency stability of beat light in Raman laser system
    Fig. 10. Frequency stability of beat light in Raman laser system
    Allen variance of beat frequency stability of Raman laser system under different integration time
    Fig. 11. Allen variance of beat frequency stability of Raman laser system under different integration time
    Noise sourceTransfer function
    Reference signal sourceTref(s)=ϕRamϕref=NG(s)
    Phase detectorTPFD(s)=ϕRamϕPFD=NKdG(s)
    Low-pass filterTLF(s)=ϕRamϕLF=Ne-sτKdF(s)G(s)
    LaserTL(s)=ϕRamϕL=G(s)H(s)
    Frequency dividerT/N(s)=ϕRamϕ/N=-NG(s)
    Photoelectric probeTPD(s)=ϕRamϕPD=-G(s)
    7 GHz signal sourceT7G(s)=ϕRamϕ7G=G(s)
    MixerTMix(s)=ϕRamϕMix=-G(s)
    Table 1. Noise transfer function of each device
    Noise sourceNoise power spectral density
    Reference signal sourceSϕreff=10-12.58759+10-9.59512f+10-6.59232f2  10 Hzf100 kHz10-14.06524+10-2.59547f2               100 kHzf10 MHz
    Phase detectorSϕPFDf=10-15.2752+10-12.89131f
    Low-pass filterSϕLFf=4kbTR
    LaserSϕLf=102.82978f2+106.54404f3+109.19809f4
    Frequency dividerSϕ/Nf=10-15.43998+10-11.98159f
    Photoelectric probeSϕPDf=10-11.5f
    7 GHz signal sourceSϕ7Gf=10-12.28186+10-5.79388f2+10-3.596072f3 10 Hzf100 kHz10-13.94731+10-2.28974f2        100 kHzf10 MHz
    MixerSϕMixf=10-17+10-14f
    Table 2. Noise power spectral density of each device
    Junchao GAO, Junjie CHEN, Liuxian YE, Bing CHENG, Bin WU, Helin WANG, Xiaolong WANG, Qiang LIN. Research on Fiber Raman Laser Source for Mobile Quantum Gravimeter[J]. Acta Photonica Sinica, 2024, 53(8): 0814003
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