“…[1−4] Compared with traditional Fabry-Perot two-section type mode-locked configurations, of which typical schemes incorporate a gain section and a saturable absorber (SA) that is integrated on a single substrate sharing the same multiple quantum well active region, [5−8] colliding pulse mode-locked (CPM) lasers place the SA section at the center of the laser cavity, taking advantage of the collision of two counter-propagating pulses in the SA section, which results in an absorption grating, leading to an enhancement of the saturable absorption and therefore more effective pulse shortening. [9−12] CPM lasers with 40-GHz repetition rate have been realized earlier in bulk [13] and multi-quantum well InGaAsP lasers [14] with picosecond pulses obtained. However, both the structures employed an all-active configuration, which would introduce potentially too much quantum noise resulting from amplified spontaneous emission (ASE) of the gain section, [15] leading to broad rf 3-dB line widths of several hundreds of kilohertz, deteriorating the device performance in pragmatic applications.…”