Dual acceptor (N, Cu) doping effects on the electronic and optical properties of ZnO

This study reports on the dual-acceptor doping effects on ZnO for obtaining p-type conductivity and effectively tuning the band gap. The electronic and optical properties of undoped, mono-(N, Cu) and dual-(N-Cu) doped ZnO have been investigated using first-principles calculations based on the densit...

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Published inMaterials chemistry and physics Vol. 242; p. 122463
Main Authors Huda Liton, Md Nurul, Mohammad Farid Ul Islam, Abu Kalam, Kamruzzaman, Md, Rahman Khan, Md Khalilur, Al Helal, Md, Rahman, Md Mozibur
Format Journal Article
LanguageEnglish
Published Lausanne Elsevier B.V 15.02.2020
Elsevier BV
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Summary:This study reports on the dual-acceptor doping effects on ZnO for obtaining p-type conductivity and effectively tuning the band gap. The electronic and optical properties of undoped, mono-(N, Cu) and dual-(N-Cu) doped ZnO have been investigated using first-principles calculations based on the density functional theory (DFT) in the framework of generalized gradient approximation (GGA). The substitution of N, Cu and N-Cu into ZnO leads to the acceptor levels arise above the valance band insight the p-type conduction nature of ZnO. The electronic and optical properties revealed that the band gap narrowing of ZnO is possible by these elementals doping. However, the heavy dual doping is an effective way leads to create shallower impurity level below Fermi level. Therefore, the dual-doped ZnO can be a potential candidate for stable p-type ZnO for future experiment and optoelectronic devices applications. •Mono (N,Cu) & dual (N-Cu) doping effect on electronic and optical properties of ZnO.•P-type conductivity nature of ZnO obtained by (N,Cu) & dual (N-Cu) doping.•Band gap narrowing is occurred in mono (N,Cu) and dual (N-Cu) doping ZnO.•Dual (N-Cu) doping is an effective way to create shallow accepter level in ZnO.•Absorption edge is red shifted for the incorporation of N, Cu and N-Cu inside ZnO.
ISSN:0254-0584
1879-3312
DOI:10.1016/j.matchemphys.2019.122463