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Dropout dynamics in pulsed quantum dot lasers due to mode jumping

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Figure

FIG. 1. Experimental time traces (a)–(c) and optical spectra (d)–(f) of the op-tical output for a range of pump currents: (a) and (d) 0:6 A; (b) and (e) 1:2 A;and (c) and (f) 1:4 A: The solid line represents the total output
FIG. 3. Unfiltered (a) and (b) and filtered (d) and (c) time traces illustratingthe transition from the unstable maximum gain mode to (a) and (c) anothersingle mode (b ¼ 0:2Þ or to (b) and (d) a two mode beating (b ¼ 0:5Þ
FIG. 5. Bifurcation diagram of the CMs showing two Hopf bifurcationpoints corresponding to the jump-down and jump-up transition (as indicatedgby the arrows) as we either increase or decrease a; respectively

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