Electronic and optical properties of Ga-doped ZnO

被引:32
作者
Lee, Yih-Shing [1 ]
Peng, Yen-Chun [2 ]
Lu, Jong-Hong [2 ]
Zhu, Yu-Ren [2 ]
Wu, Hsuan-Chung [2 ]
机构
[1] Minghsin Univ Sci & Technol, Dept Optoelect Syst Engn, Hsinchu 30401, Taiwan
[2] Ming Chi Univ Technol, Dept Mat Engn, Taishan 24301, New Taipei, Taiwan
关键词
First-principles; DFT plus U; Ga-doped ZnO; Electronic structure; Optical property; THIN-FILMS; ZINC-OXIDE; 1ST-PRINCIPLES; FABRICATION; IMPROVEMENT; POTENTIALS; DEPOSITION; EFFICIENCY; DEVICES; TIO2;
D O I
10.1016/j.tsf.2014.04.037
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
This study adopted density functional theory and the Hubbard-U method in an investigation of the electronic and optical properties of pure ZnO and Ga-doped ZnO. The difference in the lattice constant between calculated results and experimental measurements is less than 1%, while the calculated band gap of pure ZnO is in excellent agreement with experimental values. Three structures, including the substitution of Ga for Zn (Ga-s(Zn)), interstitial Ga in an octahedron (Ga-i(oct)), and interstitial Ga in a tetrahedron (Ga-i(tet)), were considered. Calculations related to formation energy revealed that Ga-s(Zn) forms more easily than Ga-i(oct) and Ga-i(tet). All three of the Ga defect models resulted in an upward shift in the Fermi level into the conduction band, resulting in n-type conductive characteristics and expansion of the optical band gap beyond that of pure ZnO. In the Ga-s(Zn) model, the average transmittance levels in the visible and UV regions were 90.5% and 77.8%, respectively, which are higher than those obtained using the pure ZnO model. However, in both the Ga-i(oct) and Ga-i(tet) models, an increase in effective mass resulted in a decrease in carrier mobility, thereby reducing electrical conductivity. In addition, interestitial Ga atoms within the ZnO crystal reduced transmittance significantly. (C) 2014 Elsevier B.V. All rights reserved.
引用
收藏
页码:464 / 470
页数:7
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