• Laser & Optoelectronics Progress
  • Vol. 62, Issue 3, 0302001 (2025)
Yanzheng Wang*, Bo Wu, Yunqi Fu, and Qiang An
Author Affiliations
  • College of Electronic Science and Technology, National University of Defense Technology, Changsha 410073, Hunan , China
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    DOI: 10.3788/LOP240998 Cite this Article Set citation alerts
    Yanzheng Wang, Bo Wu, Yunqi Fu, Qiang An. Investigation of Electromagnetically Induced Transparency Spectrum in Cesium Atomic Vapor Cell[J]. Laser & Optoelectronics Progress, 2025, 62(3): 0302001 Copy Citation Text show less

    Abstract

    Electromagnetically induced transparency (EIT) is the basis of measuring microwave by Rydberg atom, and the spectral characteristics of EIT affect the measurement accuracy of microwave field directly. The effects of the Rabi frequency of a coupling laser, Rabi frequency of a probe laser, and temperature of an atomic chamber on the electromagnetically induced transparency spectral characteristics of cesium atoms were investigated experimentally in this study. The causes for the variations in optical bistability, atomic collisions, and atomic density are investigated. The research results indicate that as the Rabi frequency of the coupling laser increases, both the width and the degree of asymmetry of the EIT spectrum first increase and then stabilize. In addition, as the Rabi frequency of the probe laser increases, the width of the EIT spectrum increases monotonically. The fitting slope initially increases and then stabilizes as the Rabi frequency of the coupling laser increases, whereas the degree of asymmetry has two trends: increasing, decreasing, and increasing, decreasing, increasing; as the temperature of the atomic chamber increases, both of them first increase and then decrease. This study is beneficial for optimizing the experimental parameters of quantum microwave measurement, improving the sensitivity of microwave measurement, and facilitating the practical application of the technology for quantum microwave measurement.
    ρ˙11=Γ2ρ22+iΩpρ21-ρ12ρ˙22=Γ3ρ33-Γ2ρ22+iΩpρ12-ρ21+iΩcρ32-ρ23ρ˙33=-Γ3ρ33+iΩcρ23-ρ32ρ˙12=-γ12-iΔpρ12-iΩcρ13+iΩpρ22-ρ11ρ˙13=-γ13-iΔp+Δcρ13+iΩpρ23-iΩcρ12ρ˙23=-γ23-iΔcρ23-iΩpρ13+iΩcρ33-ρ22
    ρ21=-iΩp/2γ21-iΔp+(Ωc2/4)γ31-i(Δp+Δc)
    χ=-2Nμ212Ωpρ21
    χ(v)dv=iμ212/ε0γ21-iΔp-iωpcv+Ωc2/4γ31-iΔp+Δc-iωp-ωcv/cN(v)dv
    Ω=2μE/
    I=PΔs=Pπα2
    I=12ncε0E2
    E=2Pπα2ncε0
    Ω=μ2Pπα2ncε0
    W=Δc1-Δc2
    γ=t-t1t-t2