We present our recent experimental and theoretical results on polarization nonlinear dynamics in Vertical-Cavity Surface -Emitting Lasers (VCSELs) for the cases of optical injection and current modulation. In the first part of this work, we investigate the case of orthogonal optical injection, i.e. the injected field has a linear polarization (LP) orthogonal to that of the free-running VCSEL. The experiments are carried out on oxide-confined AlGaAs-GaAs quantum well VCSELs for a large frequency detuning range: from -82 to 180 GHz [1]. As the injection strength increases the VCSEL switches to the master laser polarization. Such polarization switching (PS) is observed either accompanied or not by injection locking and often by a rich nonlinear dynamics, including limit cycles, wave mixing, subharmonic resonance and possibly a period doubling route to chaos [1,2]. Theoretically, we unveil the bifurcations underlying polarization switching and injection locking based on two models of VCSELs: the spin-flip model (SFM) [3] and a phenomenological two-mode rate equation model [4]. For the last case a considerable simplification of the model is possible [5], which allows the continuation of the more complicated bifurcation curves by using the continuation package AUTO [6] and clarifies in such a way the corresponding more complicated dynamics predicted by the SFM model. In Fig.1 the bifurcations are continued in the 2D plane given by the injection strength κ and the frequency detuning Δν. The branching FIG. 1: Mapping of the bifurcation lines in the plane of the injection strength κ vs. frequency detuning Δν. The saddlenode bifurcation on the x-LP injection-locked solution are plotted in black and denoted as SNx. The Hopf bifurcation on the same single mode (x-LP) solution are plotted in blue and labeled H1x. The Hopf bifurcation on the two-mode solution are plotted in blue and red and labeled H1xy and H2 xy. Branching solutions are plotted in green and denoted as Br. The numerically calculated values of the injection strength necessary to observe PS are plotted as black triangles.(Br) between a two-mode and a single-mode solution is responsible for the continuous PS and shutting down of the y-LP mode, as indicated by the fact that the uppermost triangle marking PS lies exactly along 138 TuB2.3 (Invited) 11:30 -12:00 978-1-4244-2611-9/09/$25.00 IEEE