Summary
We are interested in a first-principle time-delayed model for the study of active mode-locking. It allows us to access the typical regimes encountered in semiconductor lasers and to perform an extended bifurcation analysis. In particular, close to the harmonic resonances and to the lasing threshold, we recover the Hermite-Gauss solutions. However, the presence of the linewidth enhancement factor induces complex regimes in which even the fundamental solution may become unstable. In addition, we discover a global bifurcation scenario in which a single pulse can jump, over a slow time scale, between the different minima of the modulation potential. Finally, we derive a Haus master equation close to the lasing threshold which shows a good agreement with the original time-delayed model.
