Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide Thickness

A 27 nm gate oxide thickness has been successfully used for manufacturing high performance 650V 4H-SiC planar-gate, inversion-channel power JBSFETs in a 6-inch commercial foundry with three (Linear, Hexagonal, and Octagonal) cell topologies. The 27 nm gate oxide thickness allows operation of these J...

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Main Authors: Aditi Agarwal, Kijeong Han, B. J. Baliga
Format: Article
Language:English
Published: IEEE 2021-01-01
Series:IEEE Journal of the Electron Devices Society
Subjects:
Online Access:https://ieeexplore.ieee.org/document/9270278/
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spelling doaj-827d9af738d74fa2bd18f2dbbe318a4b2021-03-29T18:52:57ZengIEEEIEEE Journal of the Electron Devices Society2168-67342021-01-019798810.1109/JEDS.2020.30403539270278Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide ThicknessAditi Agarwal0https://orcid.org/0000-0003-4594-3398Kijeong Han1https://orcid.org/0000-0002-1006-0694B. J. Baliga2https://orcid.org/0000-0001-9171-0080Electrical and Computer Engineering Department, North Carolina State University, Raleigh, NC, USAElectrical and Computer Engineering Department, North Carolina State University, Raleigh, NC, USAElectrical and Computer Engineering Department, North Carolina State University, Raleigh, NC, USAA 27 nm gate oxide thickness has been successfully used for manufacturing high performance 650V 4H-SiC planar-gate, inversion-channel power JBSFETs in a 6-inch commercial foundry with three (Linear, Hexagonal, and Octagonal) cell topologies. The 27 nm gate oxide thickness allows operation of these JBSFETs at a gate bias of 15 V compared with 20 V used in previous reports for devices with 55 nm gate oxide thickness. The width for the Schottky contact was varied to optimize the performance of the JBS diode in the third quadrant for each cell topology. An on-state voltage drop of 2.5 V or less was achieved in the third quadrant for all the cell topologies by current flow through the integrated JBS diode, satisfying the objective of effectively by-passing the MOSFET body diode. The best breakdown voltage was achieved using the Octagonal cell topology with a half-cell Schottky contact width of 1.1 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>. It had a breakdown voltage of 850 V with a low leakage current of less than 5 nA at 650 V. The Linear cell (with half-cell Schottky contact width of 1.0 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>) and the Octagonal cell (with half-cell Schottky contact width of 2.8 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>) had blocking voltages of 800 V. The hexagonal cell topology (with half-cell Schottky contact width of 1.5 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>) had the worst blocking voltage of 715 V. Numerical simulation results are provided to show that the leakage current in all cell topologies begins to increase when the electric field at the Schottky contact exceeds 1.5 MV/cm. The lowest specific on-resistance was obtained with the hexagonal cell topology but its gate-drain charge was <inline-formula> <tex-math notation="LaTeX">$2\times $ </tex-math></inline-formula> larger than the conventional Linear cell design. The Octagonal cell topology with half-cell Schottky contact width of 1.1 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula> had the same specific on-resistance as the Linear cell case with <inline-formula> <tex-math notation="LaTeX">$2\times $ </tex-math></inline-formula> smaller gate-drain charge. This work demonstrates for the first time that excellent High-Frequency Figures-of-Merit can be achieved with a reduced gate drive voltage of 15 V for 650 V SiC JBSFETs by using a smaller gate oxide thickness of 27 nm and the Octagonal cell topology.https://ieeexplore.ieee.org/document/9270278/Silicon carbide4H-SiCinversionJBSFETcell topologylinear
collection DOAJ
language English
format Article
sources DOAJ
author Aditi Agarwal
Kijeong Han
B. J. Baliga
spellingShingle Aditi Agarwal
Kijeong Han
B. J. Baliga
Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide Thickness
IEEE Journal of the Electron Devices Society
Silicon carbide
4H-SiC
inversion
JBSFET
cell topology
linear
author_facet Aditi Agarwal
Kijeong Han
B. J. Baliga
author_sort Aditi Agarwal
title Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide Thickness
title_short Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide Thickness
title_full Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide Thickness
title_fullStr Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide Thickness
title_full_unstemmed Assessment of Linear, Hexagonal, and Octagonal Cell Topologies for 650 V 4H-SiC Inversion-Channel Planar-Gate Power JBSFETs Fabricated With 27 nm Gate Oxide Thickness
title_sort assessment of linear, hexagonal, and octagonal cell topologies for 650 v 4h-sic inversion-channel planar-gate power jbsfets fabricated with 27 nm gate oxide thickness
publisher IEEE
series IEEE Journal of the Electron Devices Society
issn 2168-6734
publishDate 2021-01-01
description A 27 nm gate oxide thickness has been successfully used for manufacturing high performance 650V 4H-SiC planar-gate, inversion-channel power JBSFETs in a 6-inch commercial foundry with three (Linear, Hexagonal, and Octagonal) cell topologies. The 27 nm gate oxide thickness allows operation of these JBSFETs at a gate bias of 15 V compared with 20 V used in previous reports for devices with 55 nm gate oxide thickness. The width for the Schottky contact was varied to optimize the performance of the JBS diode in the third quadrant for each cell topology. An on-state voltage drop of 2.5 V or less was achieved in the third quadrant for all the cell topologies by current flow through the integrated JBS diode, satisfying the objective of effectively by-passing the MOSFET body diode. The best breakdown voltage was achieved using the Octagonal cell topology with a half-cell Schottky contact width of 1.1 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>. It had a breakdown voltage of 850 V with a low leakage current of less than 5 nA at 650 V. The Linear cell (with half-cell Schottky contact width of 1.0 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>) and the Octagonal cell (with half-cell Schottky contact width of 2.8 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>) had blocking voltages of 800 V. The hexagonal cell topology (with half-cell Schottky contact width of 1.5 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula>) had the worst blocking voltage of 715 V. Numerical simulation results are provided to show that the leakage current in all cell topologies begins to increase when the electric field at the Schottky contact exceeds 1.5 MV/cm. The lowest specific on-resistance was obtained with the hexagonal cell topology but its gate-drain charge was <inline-formula> <tex-math notation="LaTeX">$2\times $ </tex-math></inline-formula> larger than the conventional Linear cell design. The Octagonal cell topology with half-cell Schottky contact width of 1.1 <inline-formula> <tex-math notation="LaTeX">$\mu \text{m}$ </tex-math></inline-formula> had the same specific on-resistance as the Linear cell case with <inline-formula> <tex-math notation="LaTeX">$2\times $ </tex-math></inline-formula> smaller gate-drain charge. This work demonstrates for the first time that excellent High-Frequency Figures-of-Merit can be achieved with a reduced gate drive voltage of 15 V for 650 V SiC JBSFETs by using a smaller gate oxide thickness of 27 nm and the Octagonal cell topology.
topic Silicon carbide
4H-SiC
inversion
JBSFET
cell topology
linear
url https://ieeexplore.ieee.org/document/9270278/
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AT kijeonghan assessmentoflinearhexagonalandoctagonalcelltopologiesfor650v4hsicinversionchannelplanargatepowerjbsfetsfabricatedwith27nmgateoxidethickness
AT bjbaliga assessmentoflinearhexagonalandoctagonalcelltopologiesfor650v4hsicinversionchannelplanargatepowerjbsfetsfabricatedwith27nmgateoxidethickness
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