I. Introduction
It is well established that the electron mobility in nMOSFETs can be enhanced by applying uniaxial tensile stress to the channel. The desired stress levels can be achieved by forming embedded epitaxial source/drain junctions, which provide a smaller lattice constant than the Si substrate [1]–[4]. In order to take full advantage of the strain-induced mobility enhancement, the MOSFET parasitic series resistance must be limited to a small fraction of the channel resistance. The contact resistance, which emerges as the most critical component of this resistance, is an exponential function of the metal–semiconductor barrier height and the doping density at the interface. Since the doping density is limited by the solid solubility of dopant atoms, the barrier height remains as the only parameter that can be engineered to reduce the contact resistivity.