Scaling Challenges of Nanosheet Field-Effect Transistors Into Sub-2 nm Nodes
Murad Ghazy Khalaf Alabdullah, Muhammad A. Elmessary, Daniel Nagy, Natalia Seoane, Antonio J. García‐Loureiro, K. Kálna
Abstract
The scaling of nanosheet (NS) field effect transistors (FETs) from the 12 nm gate length to the ultimate gate length of 10 nm for sub-2 nm nodes brings additional technological challenges. Here, 3D finite element Monte Carlo simulations are employed to explore how to alter the NS architecture to increase the drive current (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${I}_{\mathrm {\mathbf { DD}}}$ </tex-math></inline-formula>) because the gate scaling to 10 nm results in a decline of the current (by <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\mathbf {10.7}$ </tex-math></inline-formula>%). <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${I}_{\mathrm {\mathbf {DD}}}$ </tex-math></inline-formula> of the 10 nm gate length NS FET will increase by 11% if the maximum n-type source/drain doping reaches <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1\times 10^{20} \mathrm {cm^{-3}}$ </tex-math></inline-formula>, or increase by <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\mathbf {3.8}$ </tex-math></inline-formula>% if the high-<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\kappa $ </tex-math></inline-formula> dielectric layer equivalent oxide thickness (EOT) is less than <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\mathbf {1.0}$ </tex-math></inline-formula> nm. The reduction in the channel width below 40 nm or the reduction in the channel thickness below 5 nm will substantially decrease IDD. The sub-threshold figures of merit like the sub-threshold slope (SS) will decrease from 75 to 73 mV/dec, while the drain-induced barrier lowering (DIBL) will increase from 32 to 77 mV/V. Finally, the effect of strain to increase the drive current is strongly limited by quantum confinement. <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${I}_{\mathrm {\mathbf {DD}}}$ </tex-math></inline-formula> will increase by 3% and by 14% in the 10 nm gate NS FET with the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\langle 110\rangle $ </tex-math></inline-formula> and <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\langle 100\rangle $ </tex-math></inline-formula> channel orientations, respectively, when a strain of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\mathbf {0.5}$ </tex-math></inline-formula>% is applied to the channel, with a negligible increase for larger strain values (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\mathbf {0.7}$ </tex-math></inline-formula>% and <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\mathbf {1.0}$ </tex-math></inline-formula>%).