We demonstrate a thermally stable titanium silicide/titanium nitride (TiSi <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><i>x</i></sub> /TiN) full metal gate (FMG) for dual-channel gate-first high- <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$k$ </tex-math></inline-formula> /metal gate complementary metal–oxide–semiconductor technology. Unlike prior tungsten-based FMG, the simple TiSi <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><i>x</i></sub> /TiN gate electrode does not require any additional barrier layer preventing oxygen down-diffusion during high-temperature processing, as the TiSi <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><i>x</i></sub> itself blocks oxygen. With HfO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -based gate dielectrics and without any oxygen scavenging scheme, we thus demonstrate a capacitance-equivalent thickness in inversion ( <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$T_{\mathrm {inv}})$ </tex-math></inline-formula> of 1.11 nm, corresponding to an equivalent oxide thickness of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\sim 0.7$ </tex-math></inline-formula> nm. Silicon channel nFET and silicon germanium channel pFET parametrics are similar to those of control devices utilizing a conventional a-Si/TiN metal-inserted poly-Si stack (MIPS) gate, while providing superior gate sheet resistance. By supplanting MIPS with such an FMG, we anticipate that contacted gate pitch can be scaled aggressively via reduced gate height and borderless source/drain contacts.
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