4.5 Article

Laser frequency stabilization based on a universal sub-Doppler NICE-OHMS instrumentation for the potential application in atmospheric lidar

Journal

ATMOSPHERIC MEASUREMENT TECHNIQUES
Volume 12, Issue 3, Pages 1807-1814

Publisher

COPERNICUS GESELLSCHAFT MBH
DOI: 10.5194/amt-12-1807-2019

Keywords

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Funding

  1. National Key R&D Program of China [2017YFA0304203]
  2. Changjiang Scholars and Innovative Research Team in University of Ministry of Education of China [IRT_17R70]
  3. Fund for Shanxi 1331 Project Key Subjects Construction
  4. National Natural Science Foundation of China [61675122, 61875107, 61875108, 11704236, 61475093, 61775125]
  5. Shanxi Scholarship Council of China [2017-016]
  6. Program for the Outstanding Innovative Teams of Higher Learning Institutions of Shanxi
  7. Open Research fund of Key Laboratory of Atmospheric Optics, Chinese Academy of Sciences [JJ-2018-02]
  8. Swedish Research Foundation (Vetenskapsradet) [621-2015-04374]
  9. 111 project [D18001]

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Lidar is an effective tool for high-altitude atmospheric measurement in which a weak absorption line for the target gas is selected to ensure a large optical depth. The laser frequency stabilization to the line center is required, and a sub-Doppler (sD) spectroscopy of the target line is preferred as a frequency reference. In this paper, a novel universal sD noise-immune cavity-enhanced optical heterodyne molecular spectroscopy (NICE-OHMS) instrumentation based on a fiber-coupled optical single-sideband electro-optic modulator (f-SSM) for the potential application in atmospheric lidar for different target gases with different types of lasers is reported. The f-SSM can replace all frequency actuators in the system, so as to eliminate the individual design of feedback servos that often are tailored for each laser. The universality of the instrumentation was demonstrated by the alternative use of either an Er-doped fiber laser or a whispering-gallery mode laser. Then the instruments based on both lasers were used to produce the sD signals of acetylene, which worked as a frequency reference to stabilize the laser. By performing the lockings, relative frequency stabilizations of 8.3 x 10(-13) and 7.5 x 10(-13) at an integration time of 240 s were demonstrated.

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