• Chinese Optics Letters
  • Vol. 22, Issue 1, 011401 (2024)
Yibo Wang1,2, Hongwei Zhang1,2, Chenhao Zhao1,2, Gang Zhao1,2,*..., Xiaojuan Yan1,2 and Weiguang Ma1,2,**|Show fewer author(s)
Author Affiliations
  • 1State Key Laboratory of Quantum Optics & Quantum Optics Devices, Institute of Laser Spectroscopy, Shanxi University, Taiyuan 030006, China
  • 2Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
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    DOI: 10.3788/COL202422.011401 Cite this Article Set citation alerts
    Yibo Wang, Hongwei Zhang, Chenhao Zhao, Gang Zhao, Xiaojuan Yan, Weiguang Ma, "Dual-mode stabilization for laser to radio-frequency locking by using a single-sideband modulation and a Fabry–Pérot cavity," Chin. Opt. Lett. 22, 011401 (2024) Copy Citation Text show less
    Principle of the proposed dual-mode stabilization.
    Fig. 1. Principle of the proposed dual-mode stabilization.
    Schematic diagram of the experimental setup. EDFL, erbium-doped fiber laser; f-AOM, fiber-coupled acoustic optic modulator; f-EOM, fiber-coupled electro-optic modulator; f-S, fiber splitter; f-SSM, fiber-coupled single-sideband modulator; f-C, fiber collimator; MML, mode-matching lens; λ/2, half-wave plate; λ/4, quarter-wave plate; PBS, polarization beam splitter; VCO, voltage-controlled oscillator; PD1,2, photodetector; FG, frequency generator; PID, proportional-integral-derivative servo; SG, signal generator; PS, phase shift; LP, low-pass filter.
    Fig. 2. Schematic diagram of the experimental setup. EDFL, erbium-doped fiber laser; f-AOM, fiber-coupled acoustic optic modulator; f-EOM, fiber-coupled electro-optic modulator; f-S, fiber splitter; f-SSM, fiber-coupled single-sideband modulator; f-C, fiber collimator; MML, mode-matching lens; λ/2, half-wave plate; λ/4, quarter-wave plate; PBS, polarization beam splitter; VCO, voltage-controlled oscillator; PD1,2, photodetector; FG, frequency generator; PID, proportional-integral-derivative servo; SG, signal generator; PS, phase shift; LP, low-pass filter.
    Error signals for the two PDH locking processes. (a) Without and (c) with locking for the first laser; (b) without and (d) with locking for the second laser.
    Fig. 3. Error signals for the two PDH locking processes. (a) Without and (c) with locking for the first laser; (b) without and (d) with locking for the second laser.
    PSD of the frequency deviation for (a) the first laser and (b) the second laser.
    Fig. 4. PSD of the frequency deviation for (a) the first laser and (b) the second laser.
    Locking performance for the phase locking: the phase noise (a) without and (b) with locking; (c) the PSD result of the frequency deviation retrieved from the phase noise.
    Fig. 5. Locking performance for the phase locking: the phase noise (a) without and (b) with locking; (c) the PSD result of the frequency deviation retrieved from the phase noise.
    Laser frequency stability evaluated by the frequency comb: the long-term laser frequency (a) with and (b) without phase locking and (c) their Allan deviation.
    Fig. 6. Laser frequency stability evaluated by the frequency comb: the long-term laser frequency (a) with and (b) without phase locking and (c) their Allan deviation.
    Yibo Wang, Hongwei Zhang, Chenhao Zhao, Gang Zhao, Xiaojuan Yan, Weiguang Ma, "Dual-mode stabilization for laser to radio-frequency locking by using a single-sideband modulation and a Fabry–Pérot cavity," Chin. Opt. Lett. 22, 011401 (2024)
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