Almost fifty years after the first experiment by Stover [1], optical injection has been the subject of intense analysis in the last decade, especially for single-frequency laser [2,3]. This paper focuses on the properties of a single-mode quantum dash laser emitting at 1.55 !-1m, submitted to optical injection. Recent results concern mainly multi-frequency quantum dot or dash lasers emitting at 1.55 !-1m [4] or single-mode quantum-dot laser emitting at 1.3 !-1m [5,6]. However, our devices, DFB quantum-dash laser emitting at 1.55 !-1m [7], doesn't reveal the same behaviour as the one described in [5]. The general properties of this DFB quantum-dash laser are close to the ones of quantum-well lasers [3]. Nevertheless the strong damping factor associated to the quantum-dash lasers modifies totally the response with respect to the pumping parameter of the slave laser. In a conventional laser (bulk or quantum wells), close to threshold, the laser behaves like an optical amplifier, while at a larger pump current, more regimes appear as illustrated in the figure 1, which compares the different regimes in the chart "detuning"-"injected power". On the contrary, for quantum-dash laser, the tendency is opposite as shown in figure 2. We propose in this communication to detail these trends experimentally and theoreticalJy.Oetuning (GHz) • Chaos • Locklng C W;M! rnill ng • Period doubling o R Relaxation Deluning (GHz) Fig. 1 Injection map at l.3 Ith (left figure) and 41th (figure at right) for a conventional DFB laser, showing an amplifier behaviour at low pump current with less dynamical regimes. [3) Increasing detuning Cl.1 times of t", Decreasing detuning @3 times 'Ih 10 locking Ml = E '" Chaos 3 ·10 3 ·s � ·10 M2 i · IS i! 1: t ·IS II � rela.allon :? ·20 ·20 M4 ·25 ·25 3J .3) ·10 -5 10 ·10 ·S 10 Dctunlng (GHz) DClUning (GHz) Fig. 2 Injection map at 1.1 Ith (left figure) and 31th (figure at right) for a quantum-dash DFB laser, showing a richness of regimes at low pump current.