• Chinese Journal of Lasers
  • Vol. 48, Issue 3, 0312002 (2021)
Yabin Dong1、2、*, Jialu Pang1, Li Yang1, and Yaoyao Liu1
Author Affiliations
  • 1College of Physics and Electronic Engineering, Shanxi University, Taiyuan, Shanxi 0 30006, China
  • 2Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan, Shanxi 0 30006, China
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    DOI: 10.3788/CJL202148.0312002 Cite this Article Set citation alerts
    Yabin Dong, Jialu Pang, Li Yang, Yaoyao Liu. Nearly-Resonant Gain Grating in Atomic Media[J]. Chinese Journal of Lasers, 2021, 48(3): 0312002 Copy Citation Text show less
    Energy level structure of atomic system and position relation between fields and atomic system. (a) Four-level N-type atomic system; (b) spatial configuration of probe, modulation, and coupling fields with respect to atomic sample in which zeroth-order, first-order and second-order diffraction directions are indicated
    Fig. 1. Energy level structure of atomic system and position relation between fields and atomic system. (a) Four-level N-type atomic system; (b) spatial configuration of probe, modulation, and coupling fields with respect to atomic sample in which zeroth-order, first-order and second-order diffraction directions are indicated
    Transmission function and corresponding diffraction intensity of probe field when Δc=0, Δm=0.68γ, Δp=-0.05γ, Ωc=0.27γ, Ωm=0.35γ, and L=140z0 . (a) Amplitude and phase of transmission function of probe field versus x; (b) diffraction intensity versus sin θ under different phase modulation conditions; (c) part with zeroth-order diffraction int
    Fig. 2. Transmission function and corresponding diffraction intensity of probe field when Δc=0, Δm=0.68γ, Δp=-0.05γ, Ωc=0.27γ, Ωm=0.35γ, and L=140z0 . (a) Amplitude and phase of transmission function of probe field versus x; (b) diffraction intensity versus sin θ under different phase modulation conditions; (c) part with zeroth-order diffraction int
    Im (χ) versus Rabi frequencies of modulation field and coupling field when Δc=0, Δm=0.68γ, Δp=-0.05γ, and L=140z0. (a) Im (χ) versus Rabi frequency of modulation field; (b) Im (χ) versus Rabi frequency of coupling field
    Fig. 3. Im (χ) versus Rabi frequencies of modulation field and coupling field when Δc=0, Δm=0.68γ, Δp=-0.05γ, and L=140z0. (a) Im (χ) versus Rabi frequency of modulation field; (b) Im (χ) versus Rabi frequency of coupling field
    High-order diffraction intensity versus Ωc and Ωm when Δc=0, Δm=0.68γ, Δp=-0.05γ, and L=140z0.(a) First-order diffraction intensity; (b) second-order diffraction intensity; (c) third-order diffraction intensity
    Fig. 4. High-order diffraction intensity versus Ωc and Ωm when Δc=0, Δm=0.68γ, Δp=-0.05γ, and L=140z0.(a) First-order diffraction intensity; (b) second-order diffraction intensity; (c) third-order diffraction intensity
    High-order diffraction intensity versus Δp and Δm when Δc=0, Ωc=0.27γ, Ωm=0.33γ, and L=140z0. (a) First-order diffraction intensity; (b) second-order diffraction intensity; (c) third-order diffraction intensity
    Fig. 5. High-order diffraction intensity versus Δp and Δm when Δc=0, Ωc=0.27γ, Ωm=0.33γ, and L=140z0. (a) First-order diffraction intensity; (b) second-order diffraction intensity; (c) third-order diffraction intensity
    First-order diffraction intensity versus Ωm for different L when sin θ1=0.25, Δc=0, Δm=0.68γ, Δp=-0.05γ, Ωc=0.27γ, and L=140z0
    Fig. 6. First-order diffraction intensity versus Ωm for different L when sin θ1=0.25, Δc=0, Δm=0.68γ, Δp=-0.05γ, Ωc=0.27γ, and L=140z0
    Yabin Dong, Jialu Pang, Li Yang, Yaoyao Liu. Nearly-Resonant Gain Grating in Atomic Media[J]. Chinese Journal of Lasers, 2021, 48(3): 0312002
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