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肖特基C-V法研究Al_xGa_(1-x)N/GaN异质结界面二维电子气 被引量:2

Investigation on Two-Dimensional Electron Gas in Al_xGa_(1-x) N/GaN Heterostructures by Using Schottky C-V Measurement
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摘要 通过对 Pt/ Al0 .2 2 Ga0 .78N/ Ga N肖特基二极管的 C- V测量 ,研究分析了 Al0 .2 2 Ga0 .78N/ Ga N异质结界面二维电子气 (2 DEG)浓度及其空间分布 .测量结果表明 ,Al0 .2 2 Ga0 .78N/ Ga N异质结界面 2 DEG浓度峰值对应的深度在界面以下 1.3nm处 ,2 DEG分布峰的半高宽为 2 .3nm ,2 DEG面密度为 6 .5× 10 1 2 cm- 2 .与 Alx Ga1 - x As/ Ga As异质结相比 ,其 2 DEG面密度要高一个数量级 ,而空间分布则要窄一个数量级 .这主要归结于 Alx Ga1 - x N层中~ MV / cm量级的压电极化电场和自发极化电场对 Alx Ga1 - x N/ Ga N异质结能带的调制和 Alx Ga1 - x N/ Ga Concentration and spatial distribution of the two dimensional electron gas (2DEG) near the Al 0.22 Ga 0.78 N/GaN heterointerface are investigated by using Schottky C V measurement.The peak value of the 2DEG concentration occurs at 1 3nm beneath the heterointerface.The full width at half maximum (FWHM) of the 2DEG peak is 2 3nm and the sheet density of the 2DEG is 6 5×10 12 cm -2 .The sheet density of the 2DEG is one order higher and the FWHM is one order lower than those in Al x Ga 1-x As/GaAs heterostructures,because of the piezoelectrically induced polarization field in the order of ~MV/cm,which will strongly modulate the conduction band of Al x Ga 1-x N/GaN heterostructure,as well as the much larger conduction band discontinuity in the Al x Ga 1-x N/GaN heterointerface.
机构地区 南京大学物理系
出处 《Journal of Semiconductors》 EI CAS CSCD 北大核心 2001年第11期1420-1424,共5页 半导体学报(英文版)
基金 国家重点基础研究专项基金 ( G2 0 0 0 0 6 83) 国家自然科学基金 ( 6 980 6 0 0 6 6 9976 0 14及 6 99870 0 1) 国家"八六三"高技术研究发展计划基金资助~~
关键词 异质结 肖特基C-V法 二维电子气 半导体材料 Al xGa 1-x N/GaN heterostructure Schottky contacts two dimensional electron gas
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参考文献3

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同被引文献12

  • 1王晓亮,王翠梅,胡国新,王军喜,刘新宇,刘键,冉军学,钱鹤,曾一平,李晋闽.RF-MBE生长的高Al势垒层AlGaN/GaN HEMT结构(英文)[J].Journal of Semiconductors,2005,26(6):1116-1120. 被引量:1
  • 2王晓亮,刘新宇,胡国新,王军喜,马志勇,王翠梅,李建平,冉军学,郑英奎,钱鹤,曾一平,李晋闽.输出功率密度为2.23W/mm的X波段AlGaN/GaN功率HEMT器件(英文)[J].Journal of Semiconductors,2005,26(10):1865-1870. 被引量:3
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