Optimization of JFET region for 1.2kV SiC HEXFETs with 3D TCAD Simulations

1.2kV 4H-SiC MOSFETs with linear and hexagonal (HEXFET) layouts were fabricated simultaneously with both nominal and heavy doping concentrations in the JFET region. The static electrical characteristics were then compared and evaluated. The HEXFET with heavy JFET doping exhibited the lowest specific on-resistance ($\mathrm{R}_{\mathrm{on}, \mathrm{sp}}$). However, its breakdown voltage (BV) was significantly lower compared to the linear MOSFET with heavy JFET doping, indicating that the degradation in the blocking characteristics stems from a weakness in the HEXFET layout design. To further investigate, 3D TCAD blocking simulations were conducted to directly compare the linear and hexagonal layouts with the same JFET doping. These simulations reveal that the corner created in the JFET region by the hexagonal geometry is the source for the degradation in the blocking characteristics. Not only is the electric field in the gate oxide significantly higher in the center of this corner region, but there is significant electric field crowding underneath the surrounding p-well corners in the SiC.

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Published
2024-11-04
DOI
https://doi.org/10.1109/wipda62103.2024.10773373
Citations
1
Primary Topic
Silicon Carbide Semiconductor Technologies
Type
article
Field-Weighted Citation Impact
0.21

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article

Optimization of JFET region for 1.2kV SiC HEXFETs with 3D TCAD Simulations

Skylar deBoer, Woongje Sung, Adam J. Morgan, Seung Yup Jang
1 citations
Silicon Carbide Semiconductor Technologies
0.21
article

Optimization of JFET region for 1.2kV SiC HEXFETs with 3D TCAD Simulations

Skylar deBoer, Woongje Sung, Adam J. Morgan, Seung Yup Jang
article en
1 citations

Abstract

1.2kV 4H-SiC MOSFETs with linear and hexagonal (HEXFET) layouts were fabricated simultaneously with both nominal and heavy doping concentrations in the JFET region. The static electrical characteristics were then compared and evaluated. The HEXFET with heavy JFET doping exhibited the lowest specific on-resistance ($\mathrm{R}_{\mathrm{on}, \mathrm{sp}}$). However, its breakdown voltage (BV) was significantly lower compared to the linear MOSFET with heavy JFET doping, indicating that the degradation in the blocking characteristics stems from a weakness in the HEXFET layout design. To further investigate, 3D TCAD blocking simulations were conducted to directly compare the linear and hexagonal layouts with the same JFET doping. These simulations reveal that the corner created in the JFET region by the hexagonal geometry is the source for the degradation in the blocking characteristics. Not only is the electric field in the gate oxide significantly higher in the center of this corner region, but there is significant electric field crowding underneath the surrounding p-well corners in the SiC.

University at Albany, State University of New York (US)
U.S. Department of Energy, Office of Energy
Openalex Percentile: Top 45%
Silicon Carbide Semiconductor Technologies
0.21
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Optimization of JFET region for 1.2kV SiC HEXFETs with 3D TCAD Simulations — Skylar deBoer, Woongje Sung, et al. · (2024) | TGRS Research Map | TGRS