Electrostatic Discharge and Failure Model of Carbon Nanotube Field-Effect Transistors

The electrostatic discharge (ESD) and failure mechanisms of carbon nanotube field-effect transistors (CNT FETs) were thoroughly investigated via transient current tests and numerical simulations. Experiments demonstrated that CNT FETs have a three-stage ESD process according to transmission-line pulse (TLP) and human-body model (HBM) measurements, vastly different from the snapback phenomenon in conventional Si CMOS transistors. As the drain bias (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V} _{\text {DS}}$ </tex-math></inline-formula>) increases from 2 to 12 V, the ESD mechanism of CNT FETs changes from thermionic emission (first stage) to band-to-band tunneling (second stage), which results in a dynamic discharge impedance. The soft breakdown of the drain-to-gate isolation dielectric contributes to the discharge current in the third stage when <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V} _{\text {DS}} \gt 12$ </tex-math></inline-formula> V. The breakdown current-induced heating of CNT FETs can cause critical damage to the drain-to-gate isolation dielectric and the metal contacts and eventually result in device failure. Therefore, the drain-to-gate isolation dielectric is identified as the weak spot, requiring optimization to enhance the reliability of CNT FETs.

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Publication Details

Journal
IEEE Transactions on Electron Devices
Published
2025-03-04
DOI
https://doi.org/10.1109/ted.2025.3545011
Citations
1
Primary Topic
Carbon Nanotubes in Composites
Type
article
Field-Weighted Citation Impact
0.52

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article

Electrostatic Discharge and Failure Model of Carbon Nanotube Field-Effect Transistors

Yichao Sun, Bo Li, Yachi Duan, Jia Si et al.
1 citations
IEEE Transactions on Electron Devices
Carbon Nanotubes in Composites
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article

Electrostatic Discharge and Failure Model of Carbon Nanotube Field-Effect Transistors

Yichao Sun, Bo Li, Yachi Duan, Jia Si, Peng Lu, Jianhui Bu, Xiaojing Li, Dong Zhang, Can Yang, Yuepeng Gao
article en
1 citations

Abstract

The electrostatic discharge (ESD) and failure mechanisms of carbon nanotube field-effect transistors (CNT FETs) were thoroughly investigated via transient current tests and numerical simulations. Experiments demonstrated that CNT FETs have a three-stage ESD process according to transmission-line pulse (TLP) and human-body model (HBM) measurements, vastly different from the snapback phenomenon in conventional Si CMOS transistors. As the drain bias (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V} _{\text {DS}}$ </tex-math></inline-formula>) increases from 2 to 12 V, the ESD mechanism of CNT FETs changes from thermionic emission (first stage) to band-to-band tunneling (second stage), which results in a dynamic discharge impedance. The soft breakdown of the drain-to-gate isolation dielectric contributes to the discharge current in the third stage when <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V} _{\text {DS}} \gt 12$ </tex-math></inline-formula> V. The breakdown current-induced heating of CNT FETs can cause critical damage to the drain-to-gate isolation dielectric and the metal contacts and eventually result in device failure. Therefore, the drain-to-gate isolation dielectric is identified as the weak spot, requiring optimization to enhance the reliability of CNT FETs.

IEEE Transactions on Electron DevicesVol. 72(4)
Chinese Academy of Sciences (CN), Peking University (CN), Institute of Microelectronics (CN)
National Natural Science Foundation of China, Youth Innovation Promotion Association of the Chinese Academy of Sciences, National Key Research and Development Program of China
Openalex Percentile: Top 41%
Carbon Nanotubes in Composites
0.52
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