I. Introduction
Optically injected semiconductor lasers have recently been used in photonic microwave generation [1]. In a master–slave configuration with a sufficient injection power, the optical frequency of the slave laser is injection locked to that of the master laser. By properly adjusting the injection strength and the frequency detuning, instability occurs through Hopf bifurcation into the period-one dynamical state. The result is a tunable microwave oscillation in the optical power of the slave laser [2]. This method of photonic microwave generation offers many advantages due to its single-sideband (SSB) spectrum, broad-frequency tuning range, and ease of stabilization.