Lei Yang, Wei Pan, Lianshan Yan, Bin Luo, Penghua Mu, Nianqiang Li, "Loss of time-delay signature in a ring of three unidirectionally coupled semiconductor lasers," Chin. Opt. Lett. 13, 041403 (2015)

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- Chinese Optics Letters
- Vol. 13, Issue 4, 041403 (2015)

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.
![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.](/Images/icon/loading.gif)
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.
![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.](/Images/icon/loading.gif)
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.
![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.](/Images/icon/loading.gif)
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 .

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