I. Introduction
In Order to improve transmission distance, transparency, capacity and speed of optical networks, much attention has been paid to investigating practical means for all-optical signal processing, for example all-optical digital logic functions and retiming, reshaping and reamplifying (3R) regenerators [1], [2]. All-optical clock recovery regeneration at 40 Gbit/s and beyond appears to be a crucial element for future transparent networks. One solution to achieve the regeneration is an all-optical clock recovery element combined with a Mach–Zehnder interferometer [2]. In this respect truly all-optical clock recovery is of very high interest as it would supersede the complicated optoelectronic schemes including: a high speed photo-receiver, a high- filter, a power amplifier, and a high speed laser or an integrated laser modulator. Among the different approaches investigated so far, we can mention in particular the one using self-pulsating (SP) lasers.