• Infrared and Laser Engineering
  • Vol. 50, Issue 11, 20210155 (2021)
Nuerlan Tuerdahong1, Lianqing Zhu1、2、3, Guangwei Chen1、2, Huiyu Li1、3, and Jing Zhu2、3
Author Affiliations
  • 1Beijing Laboratory of Optical Fiber Sensing and System, Beijing Information Science & Technology University, Beijing 100016, China
  • 2Key Laboratory of the Ministry of Education for Optoelectronic Measurement Technology and Instrument, Beijing Information Science & Technology University, Beijing 100192, China
  • 3Beijing Key Laboratory of Optoelectronic Measurement Technology, Beijing Information Science & Technology University, Beijing 100192, China
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    DOI: 10.3788/IRLA20210155 Cite this Article
    Nuerlan Tuerdahong, Lianqing Zhu, Guangwei Chen, Huiyu Li, Jing Zhu. Structure of Fabry-Perot cavity type weak magnetic sensitivity enhancement vapor cell[J]. Infrared and Laser Engineering, 2021, 50(11): 20210155 Copy Citation Text show less
    (a) Mechanism of SERF atomic magnetometer; (b) Measurement of setup of SERF atomic magnetometer
    Fig. 1. (a) Mechanism of SERF atomic magnetometer; (b) Measurement of setup of SERF atomic magnetometer
    Resonance spectrum linewidth features under the cell temperature varying from 120 °C to 210 °C
    Fig. 2. Resonance spectrum linewidth features under the cell temperature varying from 120 °C to 210 °C
    Schematic structure of FP cavity
    Fig. 3. Schematic structure of FP cavity
    Influence of (a) absorption and (b) off-resonance parameter on output light rotation angle
    Fig. 4. Influence of (a) absorption and (b) off-resonance parameter on output light rotation angle
    Relationship between the laser interaction distance and output light rotation angle in three conditions, from top to bottom are α=0, Δφ=0; α=0.04 m−1, Δφ=0; α=0, Δφ=π/32, respectively
    Fig. 5. Relationship between the laser interaction distance and output light rotation angle in three conditions, from top to bottom are α=0, Δφ=0; α=0.04 m−1, Δφ=0; α=0, Δφ=π/32, respectively
    Evolution of amplification factor along with the laser transmission distance under two sets: the off-resonance Δφis π/64 and π/32 respectivitly for different absorption coefficients
    Fig. 6. Evolution of amplification factor along with the laser transmission distance under two sets: the off-resonance Δφis π/64 and π/32 respectivitly for different absorption coefficients
    (a) Dynamic diagram of output light rotation angle ψ with the parameters of α and Δφ; (b) Decline of output light rotation angle with increase of absorption coefficients
    Fig. 7. (a) Dynamic diagram of output light rotation angle ψ with the parameters of α and Δφ; (b) Decline of output light rotation angle with increase of absorption coefficients
    ParametersValue
    Power reflectivity(R) 90%
    Length of cell(l)/cm 1
    Alkali number density(n)/cm−35×1013
    Radius of electron(re) 2.8×10−13
    Speed of light in vacuum(c)/m·s−13×108
    Resonance strength(f) 1/3
    FWHM of resonance(D(v))/GHz 30.4
    Power of laser (P)/mW 10
    Table 1. Numerical calculation parameters of optical field
    Nuerlan Tuerdahong, Lianqing Zhu, Guangwei Chen, Huiyu Li, Jing Zhu. Structure of Fabry-Perot cavity type weak magnetic sensitivity enhancement vapor cell[J]. Infrared and Laser Engineering, 2021, 50(11): 20210155
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