Revert stable p-type ZnO with LimN complex co-doping from the first-principles study

被引:2
|
作者
Huang, Xiaowei [1 ,2 ]
Liu, Liangliang [1 ,2 ]
Zeng, Zaiping [1 ,2 ]
Jia, Yu [1 ,2 ,3 ,4 ]
Du, Zuliang [1 ,2 ]
机构
[1] Henan Univ, Collaborat Innovat Ctr Nano Funct Mat & Applicat, Key Lab Special Funct Mat, Minist Educ, Kaifeng 475001, Henan, Peoples R China
[2] Henan Univ, Sch Mat Sci & Engn, Kaifeng 475001, Henan, Peoples R China
[3] Zhengzhou Univ, Int Lab Quantum Funct Mat Henan, Zhengzhou 450001, Henan, Peoples R China
[4] Zhengzhou Univ, Sch Phys & Engn, Zhengzhou 450001, Henan, Peoples R China
关键词
Zinc oxide; p-Type conductivity; Density functional theory; LITHIUM;
D O I
10.1016/j.commatsci.2020.109894
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Although lithium-nitrogen dual acceptor (LimN) co-doping has been experimentally applied successfully for the realization of p-type conductibility in bulk ZnO, the observed p-type conductivity usually suffers instability issues. In this contribution, we have employed first-principles method within the framework of density functional theory to explore the driving mechanism of p-type conductivity in LimN-doped ZnO with an emphasis on the lithium concentration (i.e., m = 1-4). Through examining the formation energy of different doping configurations and corresponding band structures, we find that Li2N complex doping (i.e., with a Li interstitial bound to a Li-N dual-acceptor co-doping center) is responsible for the p-type conductivity. However, such a complex is energetically meta-stable. Excess Li-interstitial in bulk ZnO sample could easily cross the energy barrier (similar to 0.39 eV) and bind to the Li2N doping center, and form a stable but neutral Li3N cluster, causing the disappearance of p-type conductivity. This therefore explains the experimental instability phenomenon observed in the (Li, N)-doped ZnO. This work can be interesting and useful for designing electronic and optoelectronic devices based on p-type ZnO.
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页数:5
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