I. Introduction
IN recent years, advances in silicon fabrication technology and in particular the development of multi-user silicon fabrication facilities have enabled the development of low-cost optical microelectromechanical systems (MEMS) for laser applications. Most notably, scanning micromirrors have been integrated inside solid-state laser cavities as active mechanical Q-switches, enabling the generation of cavity-limited pulse durations at average powers exceeding 100 mW [1] . Compared to more traditional active Q-switching techniques using acousto-optic modulators (AOM) or electro-optic modulators (EOM), this MEMS-based approach provides significant advantages in miniaturization, reduction of power-consumption and cost. This technique particularly benefits from recent intense developments in optical MEMS generating new directions in optics [2]. Finally, the possibility of developing MEMS micromirror arrays will enable multiple, individually controlled, beam emission from the same laser gain medium impacting many applications in defense, industry and biology.