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In a vacuum environment, when ZnO is prepared using the chemical vapor deposition method and the molecular beam epitaxial growth method, H-gap impurities inevitably remain in the ZnO system, which is often ignored. The study of Zn vacancies under experimental conditions poses a challenge. Second, as an n-type semiconductor, ZnO is characterized by a self-compensation of natural donor defects and poor stability, which severely limit the acquisition of p-type ZnO. Based on the above problems, the conductive properties of S/Se/Te doped and VZn-Hi coexisting ZnO were investigated by first principle to acquire high-stability and high-quality p-ZnO. The study found that Zn35SO35, Zn35SeO35, and Zn35SHiO35 all have good p-type conductivity, which can effectively improve hole mobility and electrical conductivity. Among them, Zn35SO35 has the largest hole concentration at 2.80×1021 cm−3, as well as the best conductivity. The choice of Zn35SO35 provides a reference for obtaining new high-quality p-type ZnO semiconductors.
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Tom
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54--63
Opis fizyczny
Bibliogr. 39 poz., rys., tab.
Twórcy
autor
- College of Science, Inner Mongolia University of Technology, Hohhot, 010051, PR China
autor
- College of Science, Inner Mongolia University of Technology, Hohhot, 010051, PR China
- College of Materials Science and Engineering, Inner Mongolia Key Laboratory of Thin Film and Coatings, Inner Mongolia University of Technology, PR China
autor
- College of Materials Science and Engineering, Inner Mongolia Key Laboratory of Thin Film and Coatings, Inner Mongolia University of Technology, PR China
autor
- College of Science, Inner Mongolia University of Technology, Hohhot, 010051, PR China
autor
- College of Science, Inner Mongolia University of Technology, Hohhot, 010051, PR China
Bibliografia
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- [6] Alfredo BB, Daniel O, Sergio JS. n- to p-type conductivity transition and band-gap renormalization in ZnO: (Cu+Te) codoped films. Phys Rev Mater. 2021;5: 065402–10.
- [7] Zhang T, Li MK, Chen J, Wang Y, Miao LS, Lu YM, et al. Multi-component ZnO alloys: bandgap engineering, hetero-structures, and optoelectronic devices. Mater Sci Eng R Rep. 2022;147: 100661–34.
- [8] Niu WZ, Xu HB, Guo YM, Li YG, Ye ZZ, Zhu LP. The effect of sulfur on the electrical properties of S and N co-doped ZnO thin films: experiment and first-principles calculations. Phys Chem Chem Phys. 2015;17: 16705–4.
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- [10] Cai H, Xu HB, Ye ZZ, Huang JY. Realization of p-type Se–N co-doped ZnO films by radio-frequency magnetron sputtering. Mater Lett. 2013;108: 183–5.
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- [12] Park S, Minegishi T, Oh D, Lee H, Taishi T, Park J, et al. High-quality p-type ZnO films grown by co-doping of N and Te on Zn-Face ZnO Substrates. Appl Phys Express. 2010;3: 031103–3.
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- [14] Hou QY, Qi MD, Li Y. Effects of p-type conductive properties of triaxial strain-regulated ZnO (S, Se, Te) system. Phys Scr. 2021;96: 125815–11.
- [15] Liu YX, Zhang HL, Zhang ZX, Xie YZ, Xie EY. Conversion of p-type to n-type conductivity in undoped ZnO films by increasin operating temperature. Appl Surf Sci. 2010;257: 1236–8.
- [16] Zeng YJ, Ye ZZ, Xu WZ, Lu JG, He HP, Zhao BH, et al. p-type behavior in nominally undoped ZnO thin films by oxygen plasma growth. Appl Phys Lett. 2006;88: 262103–3.
- [17] Gu T, Hu ET, Guo S, Wu Y, Wang J, Wang ZY, et al. Ellipsometric study on optical properties of hydrogen plasma-treated aluminum-doped ZnO thin film. Vacuum. 2019;163: 69–74.
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- [25] Jia XF, Hou QY, Xu ZC, Qua LF. Effect of Ce doping on the magnetic and optical properties of ZnO by the first principle. J Magn Magn Mater. 2018;465: 128–35.
- [26] Guo SQ, Hou QY, Zhao CW, Zhang Y. Study of the effect of Cu heavy doping on band gap and absorption spectrum of ZnO. Chem Phys Lett. 2014;614: 15–20.
- [27] Liu YJ, Hou QY, Sha SL, Xu ZC. Electronic structure, optical and ferromagnetic properties of ZnO co-doped with Ag and Co according to first-principles calculations. Vacuum. 2020;173: 109127.
- [28] Jaballah S, Benamara M, Dahman H, Ly A, Lahem D, Debliquy M, et al. Effect of Mg-doping ZnO nanoparticles on detection of low ethanol concentrations. Mater Chem Phys. 2020;255: 123643–11.
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- [30] Li M, Zhang JY, Zhang Y. First-principles calculation of compensated (2N, W) codoping impacts on band gap engineering in anatase TiO2. Chem Phys Lett. 2012;527: 63–6.
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- [33] Sun PP, Bai LC, Kripalani DR, Zhou K. A new carbon phase with direct bandgap and high carrier mobility as electron transport material for perovskite solarcells. NPJ Comput Mater. 2019;5: 1–7.
- [34] Deb J, Seriani N, Sarkar U. Ultrahigh carrier mobility of penta-graphene: a first-principle study. Physica E. 2021;127: 114507–7.
- [35] Hou QY, Sha SL. Effect of biaxial strain on the p-type of conductive properties of (S, Se, Te) and 2 N co-doped ZnO. Mater Today Commun. 2020;24: 101063–7.
- [36] Janotti A, Van de Walle CG. Fundamentals of zinc oxide as a semiconductor. Rep Prog Phys. 2009;72: 126501–29.
- [37] Yu WL, Zhang JF, Peng TY. New insight into the enhanced photocatalytic activity of N-, C- and S-doped ZnO photocatalysts. Appl Catal B: Environ. 2016;181: 220–7.
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Uwagi
Opracowanie rekordu ze środków MEiN, umowa nr SONP/SP/546092/2022 w ramach programu "Społeczna odpowiedzialność nauki" - moduł: Popularyzacja nauki i promocja sportu (2022-2023).
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-c748545e-8279-4aa9-af98-826c90864b69