Acta Optica Sinica, Volume. 43, Issue 13, 1306005(2023)

Design and Experimental Study of Mid-Infrared TDLAS System Based on Anti-Resonant Hollow Core Fiber

Yali Sun1,2, Xinyue Zhu1, Dakun Wu1,3, Cheng Wu1,4, Fei Yu1,3、*, Renjie Li5,6, Xin Lin5、**, and Wenkai Zhao7
Author Affiliations
  • 1Laboratory of Materials for High Power Laser Optical Components, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3School of Physics and Optoelectronic Engineering, Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, Zhejiang, China
  • 4School of Physical Sciences, University of Science and Technology of China, Hefei 230026, Anhui, China
  • 5State Key Laboratory of High-Temperature Gas Dynamics, Institute of Mechanics, Chinese Academy of Sciences, Beijing 100190, China
  • 6School of Engineering Science, University of Chinese Academy of Sciences, Beijing 100049, China
  • 7Research Center of Infrared Optical Materials, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
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    Figures & Tables(11)
    Anti-resonant waveguide schematic. (a) Transmission of the light field when the resonant wavelength is satisfied; (b) transmission of the light field when the resonant wavelength is not satisfied
    AR-HCF drawing flow chart. (a) Drawing glass capillary; (b) stacking capillary; (c) drawing optical fiber preform; (d) drawing optical fiber
    AR-HCF parameters. (a) Scanning electron microscopy image of fiber cross section (outer diameter of the fiber is 220 μm and core diameter is 43 μm); (b) fiber loss spectrum (0.06 dB/m@2.5 μm)
    Simulation results of mode field characteristics and transmission characteristics of ice cream type AR-HCF. (a) HE11 mode and second order mode with a transmission wavelength of 2.5 μm in the fiber; (b) loss of the fundamental mode and second order mode
    Principle of absorption spectrum
    Near-infrared and mid-infrared linestrengths of H2O and CO2 at 2000 K (from HITRAN2016). (a) H2O; (b) CO2
    TDLAS system diagram
    Spots at different distances after collimation
    High temperature water vapor absorption signal of different transmission fibers. (a) High-temperature water vapor absorption signal when ZBLAN optical fiber is used as the transmission medium, and 4029.52 cm-1 is the high-temperature water vapor absorption line; (b) high temperature water vapor absorption signal when AR-HCF is used as the transmission medium,and 4029.78 cm-1 and 4029.52 cm-1 are the water vapor absorption lines at room temperature and high temperature, respectively
    Comparison of baseline fitting before and after vacuum pumping of AR-HCF
    • Table 1. Measurement results of spot diameter at different distances after collimating the output beam of ZBLAN fiber and AR-HCF

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      Table 1. Measurement results of spot diameter at different distances after collimating the output beam of ZBLAN fiber and AR-HCF

      L /cmD1 /mmD2 /mm
      101.40.7
      202.61.0
      304.61.4
      407.21.9
      509.32.5
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    Yali Sun, Xinyue Zhu, Dakun Wu, Cheng Wu, Fei Yu, Renjie Li, Xin Lin, Wenkai Zhao. Design and Experimental Study of Mid-Infrared TDLAS System Based on Anti-Resonant Hollow Core Fiber[J]. Acta Optica Sinica, 2023, 43(13): 1306005

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    Paper Information

    Category: Fiber Optics and Optical Communications

    Received: Jan. 16, 2023

    Accepted: Mar. 6, 2023

    Published Online: Jul. 12, 2023

    The Author Email: Yu Fei (yufei@siom.ac.cn), Lin Xin (linxin_bit@imech.ac.cn)

    DOI:10.3788/AOS230483

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