2021
DOI: 10.1103/physreva.103.053524
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Stable-unstable switching dynamics in semiconductor lasers with external cavities

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Cited by 8 publications
(3 citation statements)
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“…is the nonlinear carrier relaxation rate, 𝐽𝐽 ̃ is the normalized bias current above the threshold, and b is the linewidth enhancement factor. The parameters are extracted from a commercial communication laser [28][29][30]: γc = 5.36×10 11 s −1 , γs = 5.96×10 9 s −1 , γn = 7.53×10 9 s −1 , γp = 1.91×10 10 s −1 , J ̃ = 1.222, and b = 3.2. Second-order Runge-Kutta integration is conducted on Eqs.…”
Section: Chaos Generation and Detectionmentioning
confidence: 99%
“…is the nonlinear carrier relaxation rate, 𝐽𝐽 ̃ is the normalized bias current above the threshold, and b is the linewidth enhancement factor. The parameters are extracted from a commercial communication laser [28][29][30]: γc = 5.36×10 11 s −1 , γs = 5.96×10 9 s −1 , γn = 7.53×10 9 s −1 , γp = 1.91×10 10 s −1 , J ̃ = 1.222, and b = 3.2. Second-order Runge-Kutta integration is conducted on Eqs.…”
Section: Chaos Generation and Detectionmentioning
confidence: 99%
“…The Hopf-bifurcation boundary between the stable state and the period-one state was demonstrated in red color in Figure 2, indicating a fluctuation feature; when L was in a short-cavity region, the short-cavity region corresponded to the Hopf-bifurcation boundary with obvious fluctuation (e.g., L < 0.9 m). However, with the increase of L, the fluctuation of the Hopf-bifurcation boundary was gradually stabilized [12,[28][29][30] and tended to a constant feedback strength (e.g., κ c = 0.0011 for current system parameter settings) when L was larger than the critical external cavity length denoted by L c (e.g., 0.9 m shown in Figure 2). We, hence, set the switching status for this SLOF with L larger than L c , and κ near the Hopf-bifurcation boundary as the system operating condition.…”
Section: A Semiconductor Laser With Optical Feedback (Slof) At a Switching Statusmentioning
confidence: 99%
“…The region magnified in the inset allows the identification of oscillations of constant frequency f RO that characterize the oscillatory region and a sharp transition to the stable regime. The coexistence of stable and unstable dynamics is a common feature of SL with low optical feedback [43,45,46].…”
Section: Low Feedback Ratementioning
confidence: 99%