High Voltage Design Strategies for Gallium Oxide Power Devices

This study employs drift-diffusion simulation to investigate key factors influencing the performance of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 FinFETs, demonstrating that enhancement-mode behavior (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm { th}} \gt 0$ </tex-math></inline-formula>) is achievable for <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 FinFET using a Fin width <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}\leq 0.5~\mu $ </tex-math></inline-formula>m and doping concentration <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$N_{d}\leq 1\times 10{^{{16}}}$ </tex-math></inline-formula> cm-3. Breakdown voltage and output/transfer characteristics are calculated by using drift-diffusion methodology calibrated by experiments. We found that the metal work function (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\boldsymbol {\varnothing }_{m}$ </tex-math></inline-formula>), dielectric constant <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>, and unintentional negative interface charge density (-Qf) at the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3/dielectric interface significantly impact Vth, with a high <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\varnothing _{m}$ </tex-math></inline-formula> being necessary for enhancement mode (E-mode) operation. To achieve 5kV breakdown, a <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}$ </tex-math></inline-formula> of 200 nm requires a fin thickness <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$(T_{FIN})$ </tex-math></inline-formula> of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$0.8~\mu $ </tex-math></inline-formula>m, a <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}$ </tex-math></inline-formula> of 400 nm requires <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$T_{FIN} {\gt }$ </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">$1.2~\mu $ </tex-math></inline-formula>m, and a <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}\ {\gt }$ </tex-math></inline-formula> 600 nm requires <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$T_{FIN}\ {\gt }$ </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">$2~\mu $ </tex-math></inline-formula>m. From <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}\ $ </tex-math></inline-formula>of 200 nm to 400 nm, DIBL (drain induced barrier lowering, i.e., Vth /Vds) increases by 300%, while from 400 to 600 nm, it rises by only 100%. The presence of -Qf enhances the breakdown voltage by mitigating DIBL-related failure mechanisms and by redistributing the electric potential away from the gate dielectric and deeper into the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 drift region. A controllable and relatively defect-free process was developed for Ga2O3 metal-insulator-semiconductor (MIS) structures, enabling improved interface quality. Capacitance–voltage measurements and progressive annealing studies demonstrate enhanced device stability and reduced hysteresis for the proposed FinFET application. Finally, an optimized <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 fin etch process was developed on the KLA SPTS SynapsEtch™ module for Ga2O3 technology integration.

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IEEE Transactions on Semiconductor Manufacturing
Published
2025-08-12
DOI
https://doi.org/10.1109/tsm.2025.3597872
Primary Topic
Ga2O3 and related materials
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article
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article

High Voltage Design Strategies for Gallium Oxide Power Devices

David A. Goodwin, J. Evans, M. Vellvehı́, John H. Burnett et al.
IEEE Transactions on Semiconductor Manufacturing
Ga2O3 and related materials
article

High Voltage Design Strategies for Gallium Oxide Power Devices

David A. Goodwin, J. Evans, M. Vellvehı́, John H. Burnett, Saptarsi Ghosh, Jacob J. Mitchell, Finn Monaghan, Ariane Tomas, Michael R. Jennings, E. Chikoidze, Owen James Guy, A. Martı́nez, Hafiz Muhammad Ashraf, J. Asher, Craig A. Fisher, Ned C. Edwards, C. Colombier
article en

Abstract

This study employs drift-diffusion simulation to investigate key factors influencing the performance of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 FinFETs, demonstrating that enhancement-mode behavior (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm { th}} \gt 0$ </tex-math></inline-formula>) is achievable for <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 FinFET using a Fin width <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}\leq 0.5~\mu $ </tex-math></inline-formula>m and doping concentration <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$N_{d}\leq 1\times 10{^{{16}}}$ </tex-math></inline-formula> cm-3. Breakdown voltage and output/transfer characteristics are calculated by using drift-diffusion methodology calibrated by experiments. We found that the metal work function (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\boldsymbol {\varnothing }_{m}$ </tex-math></inline-formula>), dielectric constant <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>, and unintentional negative interface charge density (-Qf) at the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3/dielectric interface significantly impact Vth, with a high <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\varnothing _{m}$ </tex-math></inline-formula> being necessary for enhancement mode (E-mode) operation. To achieve 5kV breakdown, a <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}$ </tex-math></inline-formula> of 200 nm requires a fin thickness <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$(T_{FIN})$ </tex-math></inline-formula> of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$0.8~\mu $ </tex-math></inline-formula>m, a <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}$ </tex-math></inline-formula> of 400 nm requires <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$T_{FIN} {\gt }$ </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">$1.2~\mu $ </tex-math></inline-formula>m, and a <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}\ {\gt }$ </tex-math></inline-formula> 600 nm requires <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$T_{FIN}\ {\gt }$ </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">$2~\mu $ </tex-math></inline-formula>m. From <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$W_{FIN}\ $ </tex-math></inline-formula>of 200 nm to 400 nm, DIBL (drain induced barrier lowering, i.e., Vth /Vds) increases by 300%, while from 400 to 600 nm, it rises by only 100%. The presence of -Qf enhances the breakdown voltage by mitigating DIBL-related failure mechanisms and by redistributing the electric potential away from the gate dielectric and deeper into the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 drift region. A controllable and relatively defect-free process was developed for Ga2O3 metal-insulator-semiconductor (MIS) structures, enabling improved interface quality. Capacitance–voltage measurements and progressive annealing studies demonstrate enhanced device stability and reduced hysteresis for the proposed FinFET application. Finally, an optimized <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\beta $ </tex-math></inline-formula>-Ga2O3 fin etch process was developed on the KLA SPTS SynapsEtch™ module for Ga2O3 technology integration.

IEEE Transactions on Semiconductor ManufacturingVol. 38(4)
Swansea University (GB), Gemalto (France) (FR), Groupe d’Étude de la Matière Condensée (FR), Compound Semiconductor Centre (United Kingdom) (GB), SPTS Technologies (United Kingdom) (GB), Institut de Microelectrònica de Barcelona (ES), MTS Systems (United States) (US), Cardiff Metropolitan University (GB)
UK Research and Innovation, Swansea University, Agence Nationale de la Recherche
Affordable and clean energy
Openalex Percentile: Top 87%
Ga2O3 and related materials
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