I. Introduction
After the development of low-loss and low-dispersion silica fibers, III–V compound lasers, and Ge photodetectors, photonics research has focused on the demonstration of individual devices for wideband and multifunctional optical signal processing [1]. Because the growing photonics market requires more functionality and lower cost, photonic circuitry is desired to be monolithically integrated and to utilize the CMOS processing and low-cost substrates. Germanium and Si CMOS-compatible materials have thus been a natural choice for lower cost platforms [1], [2] and process integration with III–V optoelectronics. Ge emerges as a multifunctional material for the electronic–photonic integration on Si platform, due to its III–V and CMOS compatibility, and direct band-gap energy in the telecommunication wavelengths. The integration of III–V and Ge photonic components onto Si CMOS chips is the shortest route for meeting market expectations.