Chinese Journal of Lasers, Volume. 50, Issue 23, 2301014(2023)

Ultrastable-Cavity-Based PDH Frequency Stabilization for 2 μm DBR Fiber Laser

Xiaobing Liu1,2, Bin Wang3, Bo Yao2,4, Xiumei Yang2,5, Chunge Yue2,5, and Qinghe Mao2,4,5、*
Author Affiliations
  • 1Institute of Physical Science and Information Technology, Anhui University, Hefei 230039, Anhui, China
  • 2Anhui Provincial Key Laboratory of Photonics Devices and Materials, Anhui Institute of Optical and Fine Mechanics, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, Anhui, China
  • 3School of Physical Science, University of Science and Technology of China, Hefei 230026, Anhui, China
  • 4Advanced Laser Technology Laboratory of Anhui Province, Hefei 230037, Anhui, China
  • 5School of Environmental Science and Optoelectronic Technology, University of Science and Technology of China, Hefei 230026, Anhui, China
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    Figures & Tables(7)
    Schematic diagram of our 2 μm single-longitudinal-mode fiber laser and its PDH frequency stabilization structure based on ultra-stable optical cavity. The yellow area represents the DBR fiber resonator located inside a brass block, the light green area represents the polytetrafluoroethylene insulated packaging box, the light yellow area represents the PDH feedback loop, and the gray area represents the temperature feedback circuit
    Measured output characteristics of our single-longitudinal-mode fiber laser. (a) Temperature tuning characteristics of the output laser wavelength; (b) single-longitudinal-mode oscillating characterized by F-P scanning interferometer; (c) response characteristics of PZT frequency tuning mechanism
    Error signals recorded by an oscilloscope. (a) Error signal before frequency locking; (b) error signal after frequency locking
    Frequency noise power spectra and beat spectrum. (a) Measured frequency noise power spectra of the laser before and after its frequency is locked; (b) collected beat spectral data between two frequency-stabilized 1342 nm lasers using an FFT and the Lorentz fitting curve obtained from these data
    Variation of beat frequency signal with time and its Allan variance. (a) Beat frequency signal between two 1342 nm frequency-stabilized lasers as a function of time measured by a frequency counter locked to rubidium atomic clock with a gating time of 100 ms. In the measurement, the output laser from one 1342 nm laser is transmitted to our lab through a 20 km telecommunications optical cable. (b) Allan variance calculated from the frequency jitter data over time recorded in Fig. 5(a)
    PZT control voltage signal and single-longitudinal-mode oscillating behavior of the laser at the moment when the laser frequency just loses the locked state. (a) Recorded PZT control voltage signal when the laser frequency is locked; (b) single-longitudinal-mode oscillating behavior of the laser captured by an F-P scanning interferometer at the moment when the laser frequency just loses the locked state
    Variation of voltage with time. (a) PZT feedback control voltage signal recorded within 160 h with a digital multimeter; (b) variation of voltage over time within 240 h collected at the transmission end of the optical cavity with a digital multimeter following a photodetector
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    Xiaobing Liu, Bin Wang, Bo Yao, Xiumei Yang, Chunge Yue, Qinghe Mao. Ultrastable-Cavity-Based PDH Frequency Stabilization for 2 μm DBR Fiber Laser[J]. Chinese Journal of Lasers, 2023, 50(23): 2301014

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    Paper Information

    Category: laser devices and laser physics

    Received: Apr. 6, 2023

    Accepted: May. 17, 2023

    Published Online: Dec. 7, 2023

    The Author Email: Mao Qinghe (mqinghe@aiofm.ac.cn)

    DOI:10.3788/CJL230690

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