High-Current E-Mode InGaN/GaN p-FET on p-GaN Gate HEMT Platform

The low current density in E-mode GaN p-FET presents a severe challenge for its application in complementary logic (CL) circuits. In this work, a high-current E-mode InGaN/GaN p-FET is demonstrated on a p-GaN gate HEMT platform with p-InGaN/p-GaN/AlGaN/GaN heterostructure. The proposed heterostructure introduces a net polarization charge at the InGaN/GaN interface, leading to an enhanced 2DHG. With a negative gate bias, a buried 2DHG channel is formed prior to the surface MIS channel. As a result, the recess-gate InGaN/GaN p-FET with <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${L}_{\text {G}} = 2~\mu $ </tex-math></inline-formula> m achieves a large maximum current (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${I}_{\max }\text {)}$ </tex-math></inline-formula> exceeding −20 mA/mm. The InGaN/GaN p-FET obtains a low <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${R}_{\text {ON}}$ </tex-math></inline-formula> of 0.64 k<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\Omega \cdot $ </tex-math></inline-formula> mm and 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">${I}_{\text {ON}}$ </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">${I}_{\text {OFF}}$ </tex-math></inline-formula> ratio exceeding <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$10^{{7}}$ </tex-math></inline-formula>. The device presents E-mode operation with a threshold voltage (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V}_{\text {TH}}\text {)}$ </tex-math></inline-formula> of −1.8 V and a low subthreshold swing (SS) of 144 mV/dec. Furthermore, an E-mode n-channel GaN HEMT is fabricated on the same platform, validating the potential of the proposed InGaN/GaN p-FET for GaN CL circuits.

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Publication Details

Journal
IEEE Electron Device Letters
Published
2024-12-20
DOI
https://doi.org/10.1109/led.2024.3520582
Citations
14
Primary Topic
GaN-based semiconductor devices and materials
Type
article
Field-Weighted Citation Impact
4.35
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article

High-Current E-Mode InGaN/GaN p-FET on p-GaN Gate HEMT Platform

Teng Li, Jingjing Yu, Xuelin Yang, Jiawei Cui et al.
14 citations
IEEE Electron Device Letters
GaN-based semiconductor devices and materials
4.35
article

High-Current E-Mode InGaN/GaN p-FET on p-GaN Gate HEMT Platform

Teng Li, Jingjing Yu, Xuelin Yang, Jiawei Cui, Maojun Wang, Junjie Yang, Han Yang, Jin Wei, Yingming Song, Sihang Liu, Bo Shen
article en
14 citations

Abstract

The low current density in E-mode GaN p-FET presents a severe challenge for its application in complementary logic (CL) circuits. In this work, a high-current E-mode InGaN/GaN p-FET is demonstrated on a p-GaN gate HEMT platform with p-InGaN/p-GaN/AlGaN/GaN heterostructure. The proposed heterostructure introduces a net polarization charge at the InGaN/GaN interface, leading to an enhanced 2DHG. With a negative gate bias, a buried 2DHG channel is formed prior to the surface MIS channel. As a result, the recess-gate InGaN/GaN p-FET with <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${L}_{\text {G}} = 2~\mu $ </tex-math></inline-formula> m achieves a large maximum current (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${I}_{\max }\text {)}$ </tex-math></inline-formula> exceeding −20 mA/mm. The InGaN/GaN p-FET obtains a low <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${R}_{\text {ON}}$ </tex-math></inline-formula> of 0.64 k<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$\Omega \cdot $ </tex-math></inline-formula> mm and 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">${I}_{\text {ON}}$ </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">${I}_{\text {OFF}}$ </tex-math></inline-formula> ratio exceeding <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$10^{{7}}$ </tex-math></inline-formula>. The device presents E-mode operation with a threshold voltage (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${V}_{\text {TH}}\text {)}$ </tex-math></inline-formula> of −1.8 V and a low subthreshold swing (SS) of 144 mV/dec. Furthermore, an E-mode n-channel GaN HEMT is fabricated on the same platform, validating the potential of the proposed InGaN/GaN p-FET for GaN CL circuits.

IEEE Electron Device LettersVol. 46(2)
Peking University (CN)
Affordable and clean energy
Openalex Percentile: Top 4%
GaN-based semiconductor devices and materials
4.35
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