High-Performance ZrO₂/β-Ga₂O₃ (001) Metal–Insulator–Semiconductor Capacitors

In this study, we have fabricated high-performance metalinsulatorsemiconductor (MIS) capacitor using atomic layer-deposited ZrO2/beta-gallium oxide (<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) (001) heterojunction. The energy band alignment for the ZrO2/<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 heterojunction and electrical properties for the ZrO2/<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 MIS capacitor are investigated. Valence band offset (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\Delta {E}_{V}$ </tex-math></inline-formula>) and conduction band offset (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\Delta {E}_{C}$ </tex-math></inline-formula>) for the ZrO2/<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 heterojunction, determined by X-ray photoelectron spectroscopy (XPS) technique, are −0.42 and 1.42 eV, respectively. Its band alignment configuration exhibits a type II (staggered gap) structure. Gate leakage current and frequency-dependent capacitancevoltage (C–V) characteristics for the ZrO2/<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 MIS capacitor are investigated. The ZrO2/<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 MIS capacitor demonstrates a low gate leakage current. The PooleFrenkel (PF) conduction model is employed to elucidate the gate leakage current mechanism. No significant frequency dispersion is observed based on the frequency-dependent C–V characteristics. The fixed charge and trapped charge densities in the ZrO2 film are calculated to be <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$7.9\times 10^{{12}}$ </tex-math></inline-formula> and <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1.27\times 10^{{12}}$ </tex-math></inline-formula> cm<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{-{2}}$ </tex-math></inline-formula>, respectively. The minimum interface trapped charged density is extracted to be <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$4.1\times 10^{{10}}$ </tex-math></inline-formula> cm<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{-{2}}\cdot \text { eV}^{-{1}}$ </tex-math></inline-formula> at an energy of 0.6 eV below the conduction band 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, representing the lowest reported value for the dielectric/<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 (001) interface. These results indicate the formation of high-quality ZrO2 film on 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, making it a potential candidate as gate dielectrics in <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 power devices.

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Journal
IEEE Transactions on Electron Devices
Published
2025-03-22
DOI
https://doi.org/10.1109/ted.2025.3549382
Primary Topic
Ga2O3 and related materials
Type
article
Field-Weighted Citation Impact
0.00

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article

High-Performance ZrO₂/β-Ga₂O₃ (001) Metal–Insulator–Semiconductor Capacitors

Qihao Zhang, Jiangwei Liu, Jiwu Lu, Dongyuan Zhai et al.
IEEE Transactions on Electron Devices
Ga2O3 and related materials
article

High-Performance ZrO₂/β-Ga₂O₃ (001) Metal–Insulator–Semiconductor Capacitors

Qihao Zhang, Jiangwei Liu, Jiwu Lu, Dongyuan Zhai, Min He
article en

Abstract

In this study, we have fabricated high-performance metalinsulatorsemiconductor (MIS) capacitor using atomic layer-deposited ZrO2/beta-gallium oxide (<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) (001) heterojunction. The energy band alignment for the ZrO2/<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 heterojunction and electrical properties for the ZrO2/<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 MIS capacitor are investigated. Valence band offset (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\Delta {E}_{V}$ </tex-math></inline-formula>) and conduction band offset (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\Delta {E}_{C}$ </tex-math></inline-formula>) for the ZrO2/<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 heterojunction, determined by X-ray photoelectron spectroscopy (XPS) technique, are −0.42 and 1.42 eV, respectively. Its band alignment configuration exhibits a type II (staggered gap) structure. Gate leakage current and frequency-dependent capacitancevoltage (C–V) characteristics for the ZrO2/<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 MIS capacitor are investigated. The ZrO2/<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 MIS capacitor demonstrates a low gate leakage current. The PooleFrenkel (PF) conduction model is employed to elucidate the gate leakage current mechanism. No significant frequency dispersion is observed based on the frequency-dependent C–V characteristics. The fixed charge and trapped charge densities in the ZrO2 film are calculated to be <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$7.9\times 10^{{12}}$ </tex-math></inline-formula> and <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1.27\times 10^{{12}}$ </tex-math></inline-formula> cm<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{-{2}}$ </tex-math></inline-formula>, respectively. The minimum interface trapped charged density is extracted to be <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$4.1\times 10^{{10}}$ </tex-math></inline-formula> cm<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{-{2}}\cdot \text { eV}^{-{1}}$ </tex-math></inline-formula> at an energy of 0.6 eV below the conduction band 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, representing the lowest reported value for the dielectric/<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 (001) interface. These results indicate the formation of high-quality ZrO2 film on 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, making it a potential candidate as gate dielectrics in <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 power devices.

IEEE Transactions on Electron DevicesVol. 72(5)
Hunan University (CN), National Institute for Materials Science (JP)
Natural Science Foundation of Hunan Province
Affordable and clean energy
Openalex Percentile: Top 97%
Ga2O3 and related materials
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