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.)
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
,
,
,
.
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).
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).