• Acta Physica Sinica
  • Vol. 69, Issue 16, 164203-1 (2020)
Li-Ya Pei*
Author Affiliations
  • College of Mathematics and Physics, Beijing University of Chemical Technology, Beijing 100029, China
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    DOI: 10.7498/aps.69.20200418 Cite this Article
    Li-Ya Pei. Enhanced third-order nonlinear processes based on Raman resonance[J]. Acta Physica Sinica, 2020, 69(16): 164203-1 Copy Citation Text show less
    D1 line energy-level diagram of 85Rb.
    Fig. 1. D1 line energy-level diagram of 85Rb.
    Experimental setup. DL1 and DL2, diode lasers; PBS, polarizing beam splitter; PD, photodetector; LIA, lock-in amplifier.
    Fig. 2. Experimental setup. DL1 and DL2, diode lasers; PBS, polarizing beam splitter; PD, photodetector; LIA, lock-in amplifier.
    Experimental results for the transmission intensity of the weak probe beam (black solid line) and the FWM signal with narrow linewidth (red solid line) as a function of Δ1: (a) Δ2 = 0; (b) Δ2 = 350 MHz. (Note that in order to see the details clearly, the spectral intensity in Fig. (b) is the result of magnification to 2.5 times the actual situation.)
    Fig. 3. Experimental results for the transmission intensity of the weak probe beam (black solid line) and the FWM signal with narrow linewidth (red solid line) as a function of Δ1: (a) Δ2 = 0; (b) Δ2 = 350 MHz. (Note that in order to see the details clearly, the spectral intensity in Fig. (b) is the result of magnification to 2.5 times the actual situation.)
    Experimental results (red star) and theoretical fitting (black solid line) for the FWM signal. The coupling field intensity I2 = 1.97 mW and the control field intensity I3 = 7.4 mW are used in the experiment. The parameters used in the theoretical simulation are , , , .
    Fig. 4. Experimental results (red star) and theoretical fitting (black solid line) for the FWM signal. The coupling field intensity I2 = 1.97 mW and the control field intensity I3 = 7.4 mW are used in the experiment. The parameters used in the theoretical simulation are , , , .
    (a) FWM (solid line) and SRS (dotted line), and (b) corresponding resonant velocities (solid line) and (dotted line) as a function of when (black), 2.5(red), 4.0(blue).
    Fig. 5. (a) FWM (solid line) and SRS (dotted line), and (b) corresponding resonant velocities (solid line) and (dotted line) as a function of when (black), 2.5(red), 4.0(blue).
    (a) FWM (solid line) and SRS (dotted line), and (b) corresponding resonant velocities (solid line) and (dotted line) as a function of when 50.7 (black), 101.4(red), 202.8(blue).
    Fig. 6. (a) FWM (solid line) and SRS (dotted line), and (b) corresponding resonant velocities (solid line) and (dotted line) as a function of when 50.7 (black), 101.4(red), 202.8(blue).
    Li-Ya Pei. Enhanced third-order nonlinear processes based on Raman resonance[J]. Acta Physica Sinica, 2020, 69(16): 164203-1
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