Fig. 1. Schematic of a RTUC-SLs system.

Fig. 2. Intensity time traces (first column), ACF curves (second column), PE (third column). (a1)–(a3) correspond to SL1, (b1)–(b3) correspond to SL2, and (c1)–(c3) correspond to SL3.

Fig. 3. ACF curves evolution (left column) of the intensity time series in the RTUC-SLs when γ∈[15,150]  ns−1. The ACF (middle column) and PE (right column) curves of each laser for γ=15, 30, and 80  ns−1 (from top to bottom for each laser) are presented for comparison.

Fig. 4. The evolution of the ACF curves (left column) of the phase time series in a RTUC-SLs when γ∈[15,150]  ns−1. The ACF (middle column) and PE (right column) curves of each laser for γ=15, 30, and 80  ns−1 (from top to bottom for each laser) are presented for comparison.

Fig. 5. The ACF peak versus γ, where the results for the intensity (|E(t)|2), phase (ϕ(t)=Arg[E(t)]), real (Re[E(t)]), and imaginary (Im[E(t)]) parts of the complex field are contained. (a) corresponds to SL1, (b) corresponds to SL2, and (c) corresponds to SL3.

Fig. 6. Cross-correlation between two lasers versus γ. The insets present the ACF curves for γ=120 and 150  ns−1.