TY - JOUR
T1 - Germanium-tin p-channel tunneling field-effect transistor
T2 - Device design and technology demonstration
AU - Yang, Yue
AU - Han, Genquan
AU - Guo, Pengfei
AU - Wang, Wei
AU - Gong, Xiao
AU - Wang, Lanxiang
AU - Low, Kain Lu
AU - Yeo, Yee Chia
PY - 2013/12
Y1 - 2013/12
N2 - We report the demonstration of germanium-tin (GeSn) p-channel tunneling field-effect transistor (p-TFET) with good device performance in terms of on-state current (I-{on}). With the incorporation of Sn, the conduction band minima at \Gamma-point of GeSn alloy shift down, increasing the direct band-to-band tunneling (BTBT) generation rate at the source-channel tunneling junction in TFET. In addition, n-type dopant activation temperature of below 400^{\circ}{\rm C} can be used in GeSn, which is much lower than that in Ge (700^{\circ}{\rm C} ). Therefore, n-type dopant diffusion in GeSn is suppressed leading to an abrupt {\rm n}+ tunneling junction that is favorable for the source junction of a p-TFET. Lateral {\rm Ge}-{0.958}{\rm Sn} 0.042 p-TFETs were fabricated and high Ion of 29 \mu{\rm A}/\mu{\rm m} at V-{\rm GS}=V-{\rm DS}=-2~{\rm V} and 4.34 \mu{\rm A}/\mu{\rm m} at V-{\rm GS}=V-{\rm DS}=-1~{\rm V} is achieved.
AB - We report the demonstration of germanium-tin (GeSn) p-channel tunneling field-effect transistor (p-TFET) with good device performance in terms of on-state current (I-{on}). With the incorporation of Sn, the conduction band minima at \Gamma-point of GeSn alloy shift down, increasing the direct band-to-band tunneling (BTBT) generation rate at the source-channel tunneling junction in TFET. In addition, n-type dopant activation temperature of below 400^{\circ}{\rm C} can be used in GeSn, which is much lower than that in Ge (700^{\circ}{\rm C} ). Therefore, n-type dopant diffusion in GeSn is suppressed leading to an abrupt {\rm n}+ tunneling junction that is favorable for the source junction of a p-TFET. Lateral {\rm Ge}-{0.958}{\rm Sn} 0.042 p-TFETs were fabricated and high Ion of 29 \mu{\rm A}/\mu{\rm m} at V-{\rm GS}=V-{\rm DS}=-2~{\rm V} and 4.34 \mu{\rm A}/\mu{\rm m} at V-{\rm GS}=V-{\rm DS}=-1~{\rm V} is achieved.
KW - Band-to-band tunneling
KW - direct bandgap
KW - germanium-tin
KW - p-channel tunneling field-effect transistor (p-TFET)
UR - http://www.scopus.com/inward/record.url?scp=84889594368&partnerID=8YFLogxK
U2 - 10.1109/TED.2013.2287031
DO - 10.1109/TED.2013.2287031
M3 - Article
AN - SCOPUS:84889594368
SN - 0018-9383
VL - 60
SP - 4048
EP - 4056
JO - IEEE Transactions on Electron Devices
JF - IEEE Transactions on Electron Devices
IS - 12
M1 - 6656859
ER -