In-situ contact formation for ultra-low contact resistance NiGe using carrier activation enhancement (CAE) techniques for Ge CMOS

Abstract

We first achieved ultra-low NiGe specific contact resistivities (ρ <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</sub> 's) of 2.3×10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-9</sup> Ωcm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> and 1.9×10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-8</sup> Ωcm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> , which were both reduced from the best values ever reported by one order of magnitude, for Ge P- and N-MOS, respectively. The keys to the excellent performance were carrier activation enhancement (CAE) techniques using Ge pre-amorphization implant (PAI) or laser anneal (LA) followed by an in-situ contact process. Impact of ultra-low ρ <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">c</sub> 's on saturation drive current (Id <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">sat</sub> ) was also simulated for ITRS 2015 HP nFinFET.