AlGaN/GaN HEMT-Based MHM Ultraviolet Phototransistor With Bent-Gate Structure

We have designed an AlGaN/GaN-based metal-heterostructure-metal (MHM) ultraviolet (UV) phototransistor (PT) with bent-Gate Structure. After partial etching of the AlGaN/GaN layer, an interdigital Ti/Al/Ni/Au metal stack was deposited on the GaN absorber layer to form an ohmic contact, which is in lateral contact with the AlGaN/GaN heterojunction to form a MHM structure. A bent gate was embedded between the interdigital ohmic electrodes to control the switching state of the two-dimensional electron gas (2DEG) channel. More importantly, benefiting from the strong polarization electric field in the lengthwise direction and the 2DEG high mobility channel in the lateral direction at the AlGaN/GaN heterojunction interface of the device, the device shows excellent photodetection performance: a peak responsivity (R) of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$6 \times 10^{{4}}$ </tex-math></inline-formula> A/W can be obtained under 265 nm UV irradiation, with a corresponding detectivity (D<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\ast }$ </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">$8.28 \times 10^{{16}}~\text {cm}\cdot \text {W}^{-{1}}\cdot \text {Hz}^{\text {1/2}}$ </tex-math></inline-formula>; and a responsivity of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1.8 \times 10^{{4}}$ </tex-math></inline-formula> A/W can be obtained under 360 nm UV irradiation, with a corresponding D<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\ast }$ </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">$2.48 \times 10^{{16}}~\text {cm}\cdot \text {W}^{-{1}} \cdot \text {Hz}^{\text {1/2}}$ </tex-math></inline-formula>. In addition, we have analyzed and investigated the operating principle of the designed device and the control mechanism of the bent gate using the theoretically simulated results of the device.

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Publication Details

Journal
IEEE Electron Device Letters
Published
2024-10-18
DOI
https://doi.org/10.1109/led.2024.3483730
Citations
11
Primary Topic
GaN-based semiconductor devices and materials
Type
article
Field-Weighted Citation Impact
3.42

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article

AlGaN/GaN HEMT-Based MHM Ultraviolet Phototransistor With Bent-Gate Structure

Mei Ge, Guofeng Yang, Bingjie Ye, Junjun Xue et al.
11 citations
IEEE Electron Device Letters
GaN-based semiconductor devices and materials
3.42
article

AlGaN/GaN HEMT-Based MHM Ultraviolet Phototransistor With Bent-Gate Structure

Mei Ge, Guofeng Yang, Bingjie Ye, Junjun Xue, Biao Gong, И. Н. Пархоменко, Ф. Ф. Комаров, Yu Liu, Xiao Wang, Jin Wang
article en
11 citations

Abstract

We have designed an AlGaN/GaN-based metal-heterostructure-metal (MHM) ultraviolet (UV) phototransistor (PT) with bent-Gate Structure. After partial etching of the AlGaN/GaN layer, an interdigital Ti/Al/Ni/Au metal stack was deposited on the GaN absorber layer to form an ohmic contact, which is in lateral contact with the AlGaN/GaN heterojunction to form a MHM structure. A bent gate was embedded between the interdigital ohmic electrodes to control the switching state of the two-dimensional electron gas (2DEG) channel. More importantly, benefiting from the strong polarization electric field in the lengthwise direction and the 2DEG high mobility channel in the lateral direction at the AlGaN/GaN heterojunction interface of the device, the device shows excellent photodetection performance: a peak responsivity (R) of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$6 \times 10^{{4}}$ </tex-math></inline-formula> A/W can be obtained under 265 nm UV irradiation, with a corresponding detectivity (D<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\ast }$ </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">$8.28 \times 10^{{16}}~\text {cm}\cdot \text {W}^{-{1}}\cdot \text {Hz}^{\text {1/2}}$ </tex-math></inline-formula>; and a responsivity of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$1.8 \times 10^{{4}}$ </tex-math></inline-formula> A/W can be obtained under 360 nm UV irradiation, with a corresponding D<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$^{\ast }$ </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">$2.48 \times 10^{{16}}~\text {cm}\cdot \text {W}^{-{1}} \cdot \text {Hz}^{\text {1/2}}$ </tex-math></inline-formula>. In addition, we have analyzed and investigated the operating principle of the designed device and the control mechanism of the bent gate using the theoretically simulated results of the device.

IEEE Electron Device LettersVol. 45(12)
Jiangnan University (CN), University of Copenhagen (DK), Nantong University (CN), Belarusian State University (BY), Nanjing University of Posts and Telecommunications (CN)
National Natural Science Foundation of China
Affordable and clean energy
Openalex Percentile: Top 6%
GaN-based semiconductor devices and materials
3.42
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