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1. 哈尔滨学院, 物理与电子工程系,黑龙江 哈尔滨,150086
2. 集美大学, 计算科学与应用物理系,福建 厦门,361021
收稿日期:2002-08-20,
修回日期:2002-12-04,
纸质出版日期:2003-07-20
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宋国利, 刘慧英, 孙凯霞, 杨幼桐, 陈保久. 纳米ZnO胶体可见发射机制的研究[J]. 发光学报, 2003,24(4): 348-352
SONG Guo-li, LIU Hui-ying, SUN Kai-xia, YANG You-tong, CHEN Bao-jiu. Study on the Visible Emission Mechanism of Nanocrystalline ZnO Colloids[J]. Chinese Journal of Luminescence, 2003,24(4): 348-352
关于ZnO可见发射机制的讨论目前尚无定论。本文研究了不同颗粒尺寸的纳米晶ZnO胶体的发射性质
观测到两个发射带
其中之一是激子发射
另一个是可见发射;发现两个发射带的峰值能量之间存在线性关系
并由此提出了可见发射机制是来自导带的电子到深陷阱的跃迁。
The mechanism behind the visible luminescence of ZnO is still a question of debate. To find out the mechanism
the emission properties of nanocrystalline ZnO colloids with different particle sizes were studied in the present paper. The preparation procedure of nanocrystalline ZnO colloids consists of two major steps:(1) preparation of precursor and (2) hydrolysis of the precursor to form the colloid. Zinc acetate and methanol were used to prepare the precursor without further purification
and NaOH was used to hydrolyze the precursor
respectively. The sizes of ZnO particles increase with the reaction time. The emission spectra were taken at different times during the growth of ZnO particles in methanol at room temperature. In this way one can study nanocrystalline ZnO particles with different sizes. Two emission bands were observed
one being an exciton emission and the other being visible emission. The energetic positions of the maxima of both emission bands depend on the size of the ZnO particles. We found that the two emission bands shift to lower energies positions upon particle growth. This is a quantum size effect and can be understood in terms of confinement of charge carriers. Contrary to the nanocrystalline ZnO powder
the emission intensities of the nanocrystalline ZnO colloids increases as the sizes of ZnO particles are decreased. Studies on the variation of the energetic positions of the maxima of both the UV and visible emission band of ZnO as a function of particle size provide novel information on the nature of the visible emission transition
which is valid for ZnO in general. The energetic positions of both band edges can be calculated as a function of particle size. A linear relationship between the maximum energetic positions of the two emission bands was given both from our experiments and from our calculation in this paper. Accordingly we attribute the visible emission to the transition of an electron from the conduction band to a deep trap.
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