A Model of Dual Fabry-Perot Etalon-Based External-Cavity Tunable Laser Us...
Internal motion within pulsating pure-quartic soliton molecules in a fibe...
Enhanced light emission of germanium light-emitting-diode on 150 mm germa...
The Fabrication of GaN Nanostructures Using Cost-Effective Methods for Ap...
Negative-to-Positive Tunnel Magnetoresistance in van der Waals Fe3GeTe2/C...
Quantum Light Source Based on Semiconductor Quantum Dots: A Review
A High-Reliability RF MEMS Metal-Contact Switch Based on Al-Sc Alloy
Development of a Mode-Locked Fiber Laser Utilizing a Niobium Diselenide S...
Development of Multiple Fano-Resonance-Based All-Dielectric Metastructure...
Traffic Vibration Signal Analysis of DAS Fiber Optic Cables with Differen...
官方微信
友情链接

Optimization of selective-area regrown n-GaN via MOCVD for high-frequency HEMT

2022-02-24

 

Author(s): Zhang, L (Zhang, Lian); Cheng, Z (Cheng, Zhe); He, YW (He, Yawei); Xu, JX (Xu, Jianxing); Jia, LF (Jia, Lifang); Wang, XY (Wang, Xinyuan); Zhang, SY (Zhang, Shiyong); Tan, W (Tan, Wei); Zhang, Y (Zhang, Yun)

Source: APPLIED PHYSICS LETTERS Volume: 119 Issue: 26 Article Number: 262104 DOI: 10.1063/5.0077937 Published: DEC 27 2021

Abstract: The selective-area regrowth (SAG) n-type GaN source/drain electrode has been widely used in high electron mobility transistors (HEMTs) for high-frequency applications. Previous studies focused only on device performances, but not on SAG n(+)-GaN in devices. This paper studies electron concentration and mobility of SAG n(+)-GaN on InAlN/GaN HEMTs via metal-organic chemical vapor deposition (MOCVD). It is revealed that electron mobility of SAG GaN is significantly affected by thickness. The decrease in mobility in a thin GaN may be attributed to regrowth interface defects. A gas flow model on the regrowth region is proposed to guide the regrowth of SAG GaN for improving the electron mobility. A high electron mobility of 138cm(2)/Vs with an electron concentration of 5.2x10(19)/cm(3) is obtained from an 80-nm n(+)-GaN with the regrowth width of 10 mu m. Due to the high doping level, the nonalloy metal-semiconductor contact resistance (Rm-GaN) is as low as 0.041 Omega mm. The interface resistance (R-int) between GaN and 2DEG is extracted using transfer length measurement (TLM) models and found to be 0.106 Omega mm. The on-resistance (R-on) is 0.753 Omega mm for InAlN/GaN HEMT with a source-drain metal spacing (L-sd metal) of 2 mu m. Published under an exclusive license by AIP Publishing.

Accession Number: WOS:000755254700021

ISSN: 0003-6951

eISSN: 1077-3118

Full Text: https://aip.scitation.org/doi/10.1063/5.0077937



关于我们
下载视频观看
联系方式
通信地址

北京市海淀区清华东路甲35号(林大北路中段) 北京912信箱 (100083)

电话

010-82304210/010-82305052(传真)

E-mail

semi@semi.ac.cn

交通地图
版权所有 中国科学院半导体研究所

备案号:京ICP备05085259-1号 京公网安备110402500052 中国科学院半导体所声明