I. Introduction
The DEVELOPMENT of future electronic–photonic integrated circuits based on silicon (Si) technology critically depends on the availability of complementary metal–oxide–semiconductor (CMOS)-compatible high-speed modulators that enable the interaction of electronic and optical signals. (a) Externally biased MZ modulator with coplanar RF feeder. (b) Split-ridge waveguide pin-phase modulator with single-mode intensity profile. Si-based phase modulators using the plasma dispersion effect in a -structure have been proposed for Si-based optoelectronic phase and amplitude modulators [1]. Switching speeds up to 10 MHz [2] have been demonstrated and up to 1 GHz are predicted [3]. The speed of the response in these devices is limited by carrier recombination. Very recently a modulator based on an MOS structure has been proposed [4] operating at 1-GHz speed. However, this device needs an applied voltage of 10 V for achieving a phase shift within 1-cm length and showed 6.7-dB loss due to the doped polysilicon rib-waveguide. Much lower drive voltage in the order of 1–5 V is needed, when fed by CMOS circuitry. The same is true for top contacted rib-waveguides of previously proposed pin-structures [1].