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具有双AlGaN势垒设计的凹槽栅AlGaN/GaN MIS-HEMT增强模式特性研究

Investigation of Recessed Gate AlGaN/GaN MIS-HEMTs with Double AlGaN Barrier Designs toward an Enhancement-Mode Characteristic.

作者信息

Wu Tian-Li, Tang Shun-Wei, Jiang Hong-Jia

机构信息

International College of Semiconductor Technology, National Chiao Tung University, Hsinchu 30010, Taiwan.

出版信息

Micromachines (Basel). 2020 Feb 3;11(2):163. doi: 10.3390/mi11020163.

DOI:10.3390/mi11020163
PMID:32028702
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7074664/
Abstract

In this work, recessed gate AlGaN/GaN metal-insulator-semiconductor high-electron-mobility transistors (MIS-HEMTs) with double AlGaN barrier designs are fabricated and investigated. Two different recessed depths are designed, leading to a 5 nm and a 3 nm remaining bottom AlGaN barrier under the gate region, and two different Al% (15% and 20%) in the bottom AlGaN barriers are designed. First of all, a double hump trans-conductance ()-gate voltage () characteristic is observed in a recessed gate AlGaN/GaN MIS-HEMT with a 5 nm remaining bottom AlGaN barrier under the gate region. Secondly, a physical model is proposed to explain this double channel characteristic by means of a formation of a top channel below the gate dielectric under a positive . Finally, the impacts of Al% content (15% and 20%) in the bottom AlGaN barrier and 5 nm/3 nm remaining bottom AlGaN barriers under the gate region are studied in detail, indicating that lowering Al% content in the bottom can increase the threshold voltage () toward an enhancement-mode characteristic.

摘要

在本工作中,制备并研究了具有双AlGaN势垒设计的凹槽栅AlGaN/GaN金属-绝缘体-半导体高电子迁移率晶体管(MIS-HEMT)。设计了两种不同的凹槽深度,使得栅极区域下方剩余5nm和3nm的底部AlGaN势垒,并设计了底部AlGaN势垒中两种不同的Al%(15%和20%)。首先,在栅极区域下方剩余5nm底部AlGaN势垒的凹槽栅AlGaN/GaN MIS-HEMT中观察到双峰跨导( )-栅极电压( )特性。其次,提出了一个物理模型,通过在正 下在栅极电介质下方形成顶部沟道来解释这种双通道特性。最后,详细研究了底部AlGaN势垒中Al%含量(15%和20%)以及栅极区域下方5nm/3nm剩余底部AlGaN势垒的影响,表明降低底部Al%含量可使阈值电压( )朝着增强型特性增加。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/66cbad608615/micromachines-11-00163-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/55af56a30ebc/micromachines-11-00163-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/90c8cee5eaeb/micromachines-11-00163-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/5ccf23fb2bab/micromachines-11-00163-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/68859272ae10/micromachines-11-00163-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/f127687c8939/micromachines-11-00163-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/9667cbb4181b/micromachines-11-00163-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/3e4949b642fe/micromachines-11-00163-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/cef413b47e7d/micromachines-11-00163-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/7c0eb8e81eb5/micromachines-11-00163-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/66cbad608615/micromachines-11-00163-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/55af56a30ebc/micromachines-11-00163-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/90c8cee5eaeb/micromachines-11-00163-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/5ccf23fb2bab/micromachines-11-00163-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/68859272ae10/micromachines-11-00163-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/f127687c8939/micromachines-11-00163-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/9667cbb4181b/micromachines-11-00163-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/3e4949b642fe/micromachines-11-00163-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/cef413b47e7d/micromachines-11-00163-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/7c0eb8e81eb5/micromachines-11-00163-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e95f/7074664/66cbad608615/micromachines-11-00163-g010.jpg

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