Structural and Optical Properties of Group III Doped Hydrothermal ZnO Thin Films

被引:0
作者
Asad J. Mughal
Benjamin Carberry
James S. Speck
Shuji Nakamura
Steven P. DenBaars
机构
[1] University of California Santa Barbara,Materials Department
[2] University of Florida,Department of Electrical and Computer Engineering
[3] University of California Santa Barbara,Department of Electrical and Computer Engineering
来源
Journal of Electronic Materials | 2017年 / 46卷
关键词
Hydrothermal deposition; ZnO; TCO; thin films; ALD; Burstein-Moss Effect;
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摘要
In this work, we employ a simple two-step growth technique to deposit impurity doped heteroepitaxial thin films of (0001) ZnO onto (111) MgAl2O4 spinel substrates through a combination of atomic layer deposition (ALD) and hydrothermal growth. The hydrothermal layer is doped with Al, Ga, and In through the addition of their respective nitrate salts. We evaluated the effect that varying the concentrations of these dopants has on both the structural and optical properties of these films. It was found that the epitaxial ALD layer created a ⟨111⟩MgAl2O4⟨0001⟩ZnO\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \langle 111\rangle_{{{\rm{MgAl}}_{2} {\rm{O}}_{4} }} \left\| {\;\langle 0001\rangle_{\rm{ZnO}} } \right. $$\end{document} out-of-plane orientation and a ⟨1¯1¯2⟩MgAl2O4⟨011¯0⟩ZnO\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \langle \bar{1}\bar{1}2\rangle_{{{\rm{MgAl}}_{2} {\rm{O}}_{4} }} \left\| {\;\langle 01\bar{1}0\rangle_{\rm{ZnO}} } \right. $$\end{document} in-plane orientation between the film and substrate. The rocking curve line widths ranged between 0.75° and 1.80° depending on dopant concentration. The optical bandgap determined through the Tauc method was between 3.28 eV and 3.39 eV and showed a Burstein-Moss shift with increasing dopant concentration.
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页码:1821 / 1825
页数:4
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共 113 条
  • [21] Barquinha P(2012)undefined CrystEngComm 14 1232-undefined
  • [22] Aguas H(2003)undefined J. Cryst. Growth 259 103-undefined
  • [23] Pereira L(2000)undefined Appl. Phys. Lett. 76 245-undefined
  • [24] Goncalves G(2011)undefined J. Cryst. Growth 322 45-undefined
  • [25] Ferreira I(2006)undefined Opt. Mater. 29 100-undefined
  • [26] Klingshirn C(1966)undefined Phys. Status Solidi B 15 627-undefined
  • [27] Ozgur U(2015)undefined Phys. Status Solidi 252 1700-undefined
  • [28] Hofstetter D(1998)undefined J. Appl. Phys. 83 5447-undefined
  • [29] Morkoc H(1954)undefined Phys. Rev. 93 632-undefined
  • [30] Janotti A(undefined)undefined undefined undefined undefined-undefined