Effect of Temperature on the Electrical and Current Transport Properties of Au/Nd2O3/n-GaN Metal/Interlayer/Semiconductor (MIS) Junction

被引:0
作者
M. Siva Pratap Reddy
Herie Park
V. Rajagopal Reddy
机构
[1] Kyungpook National University,School of Electronics Engineering
[2] Hanyang University,Division of Electrical and Biomedical Engineering
[3] Sri Venkateswara University,Department of Physics
来源
Applied Physics A | 2021年 / 127卷
关键词
Rare-earth oxide; Nd; O; interlayer; n-GaN; inhomogeneities; Electrical properties; Current conduction mechanism;
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摘要
The Au/Nd2O3/n-type GaN metal/interlayer/semiconductor (MIS) junctions were fabricated with high-k rare-earth oxide interlayer and explored its electrical properties in the wide temperature range of 150–400 K. An anomalous decrease in barrier height and an increase in the ideality factor with a decrease in the temperature were observed. The anomalous barrier height and ideality factor are ascribed to a role of barrier inhomogeneities at the interface of MIS junction assuming a double Gaussian distribution of barrier heights in the temperature ranges of 150–225 K and 225–400 K. Double Gaussian distribution giving mean barrier heights of 0.84 eV and 1.23 eV and standard deviations of 0.0085 V and 0.0187 V for the two temperature regions. A modified conventional energy plot gives mean barrier height Φ¯bo\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\left( {\overline{\Phi }_{bo} } \right)$$\end{document} and Richardson constant (A*) as 0. eV and 13.44 Acm−2 K−2 (150–225 K) and 1.23 eV and 22.85 Acm−2 K−2 (250–400 K), respectively. The estimated A* value in the temperature range of 250–400 K was closely matched with the theoretical value of n-type GaN. Moreover, results express that the obtained interface state density of the MIS junction decreases with increasing temperature. Results explained that the reverse current conduction governed by Poole–Frenkel emission at the temperature range of 150–225 K and Schottky emission at 250–400 K, respectively.
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