SiO₂/β-Ga₂O₃ (001) MIS Capacitors With Ideal Flat Band Voltage, Small Hysteresis, and Low Interface Traps

In this study, we have fabricated a high-performance SiO2/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) metal-insulator–semiconductor (MIS) capacitor. Its high-temperature thermal stability was investigated in detail. No significant frequency dispersion was observed by the bidirectional frequency-dependent C–V characteristics. The SiO2/<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) MIS capacitor with postdeposition annealing (PDA) at 1000 °C demonstrates an ideal flat band voltage (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V}_{\text {FB}}$ </tex-math></inline-formula>) of 1.0 V, low flat band hysteresis voltage of 40 mV, as well as low interface state density (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${D}_{\text {it}}$ </tex-math></inline-formula>) of below <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5\times 10^{{11}}$ </tex-math></inline-formula> cm−2 eV−1. However, for the sample annealed at 1100 °C, the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V}_{\text {FB}}$ </tex-math></inline-formula> increased to 2.1 V, indicating a high density of fixed charge in SiO2 film. The gate leakage current density remains below <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1\times 10^{-{6}}$ </tex-math></inline-formula> A/cm−2 for 1000 °C-annealed SiO2/<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) MIS capacitor until hard breakdown occurs. The <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${D}_{\text {it}}$ </tex-math></inline-formula> values of SiO2/<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) interfaces with PDA at 800 °C, 900 °C, and 1000 °C are lower than <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5\times 10^{{11}}$ </tex-math></inline-formula> cm−2 eV−1 within the trap energy level range of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$0.2\le {E}_{C}-{E}_{t} \le 0.6$ </tex-math></inline-formula> eV. However, the sample after annealing at 1100 °C, the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${D}_{\text {it}}$ </tex-math></inline-formula> values are higher than that of the other three capacitors. High-angle annular dark field scanning transmission electron microscope (HAADF-STEM) was performed to investigate interface characteristics of the SiO2/<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) MIS capacitor with PDA at 1100 °C. The depth profiles of Ga and Si in SiO2 films and at the surface 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 after PDA at 1000 °C and 1100 °C were measured by dynamic secondary ion mass spectrometry measurements. These results indicate the formation of high-quality SiO2 film on the (001) oriented<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 after high-temperature annealing, 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
2025-03-11
DOI
https://doi.org/10.1109/ted.2025.3547295
Primary Topic
Ga2O3 and related materials
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article
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article

SiO₂/β-Ga₂O₃ (001) MIS Capacitors With Ideal Flat Band Voltage, Small Hysteresis, and Low Interface Traps

Qihao Zhang, Jiwu Lu, Dongyuan Zhai, Min He
IEEE Transactions on Electron Devices
Ga2O3 and related materials
article

SiO₂/β-Ga₂O₃ (001) MIS Capacitors With Ideal Flat Band Voltage, Small Hysteresis, and Low Interface Traps

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

Abstract

In this study, we have fabricated a high-performance SiO2/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) metal-insulator–semiconductor (MIS) capacitor. Its high-temperature thermal stability was investigated in detail. No significant frequency dispersion was observed by the bidirectional frequency-dependent C–V characteristics. The SiO2/<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) MIS capacitor with postdeposition annealing (PDA) at 1000 °C demonstrates an ideal flat band voltage (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V}_{\text {FB}}$ </tex-math></inline-formula>) of 1.0 V, low flat band hysteresis voltage of 40 mV, as well as low interface state density (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${D}_{\text {it}}$ </tex-math></inline-formula>) of below <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5\times 10^{{11}}$ </tex-math></inline-formula> cm−2 eV−1. However, for the sample annealed at 1100 °C, the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V}_{\text {FB}}$ </tex-math></inline-formula> increased to 2.1 V, indicating a high density of fixed charge in SiO2 film. The gate leakage current density remains below <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1\times 10^{-{6}}$ </tex-math></inline-formula> A/cm−2 for 1000 °C-annealed SiO2/<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) MIS capacitor until hard breakdown occurs. The <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${D}_{\text {it}}$ </tex-math></inline-formula> values of SiO2/<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) interfaces with PDA at 800 °C, 900 °C, and 1000 °C are lower than <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5\times 10^{{11}}$ </tex-math></inline-formula> cm−2 eV−1 within the trap energy level range of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$0.2\le {E}_{C}-{E}_{t} \le 0.6$ </tex-math></inline-formula> eV. However, the sample after annealing at 1100 °C, the <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${D}_{\text {it}}$ </tex-math></inline-formula> values are higher than that of the other three capacitors. High-angle annular dark field scanning transmission electron microscope (HAADF-STEM) was performed to investigate interface characteristics of the SiO2/<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) MIS capacitor with PDA at 1100 °C. The depth profiles of Ga and Si in SiO2 films and at the surface 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 after PDA at 1000 °C and 1100 °C were measured by dynamic secondary ion mass spectrometry measurements. These results indicate the formation of high-quality SiO2 film on the (001) oriented<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 after high-temperature annealing, 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 Natural Science Foundation of China, Natural Science Foundation of Hunan Province
Affordable and clean energy
Openalex Percentile: Top 98%
Ga2O3 and related materials
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