Wang Zhenling, Lin Cuikun, Liu Xiaoming, Li Guangzhi, Luo Yan, Quan Zewei, Xiang Hongping, Lin Jun
Key Laboratory of Rare Earth Chemistry and Physics, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P R China.
J Phys Chem B. 2006 May 18;110(19):9469-76. doi: 10.1021/jp057214t.
ZnO and ZnO:Zn powder phosphors were prepared by the polyol-method followed by annealing in air and reducing gas, respectively. The samples were characterized by X-ray diffraction (XRD), field emission scanning electron microscopy (FESEM), X-ray photoelectron spectra (XPS), electron paramagnetic resonance (EPR), and photoluminescence (PL) and cathodoluminescence (CL) spectra, respectively. The results indicate that all samples are in agreement with the hexagonal structure of the ZnO phase and the particle sizes are in the range of 1-2 microm. The PL and CL spectra of ZnO powders annealed at 950 degrees C in air consist of a weak ultraviolet emission band (approximately 390 nm) and a broad emission band centered at about 527 nm, exhibiting yellow emission color to the naked eyes. When the sample was reduced at the temperatures from 500 to 1050 degrees C, the yellow emission decreased gradually and disappeared completely at 800 degrees C, whereas the ultraviolet emission band became the strongest. Above this temperature, the green emission ( approximately 500 nm) appeared and increased with increasing of reducing temperatures. According to the EPR results and spectral analysis, the yellow and green emissions may arise from the transitions of photogenerated electron close to the conduction band to the deeply trapped hole in the single negatively charged interstitial oxygen ion (Oi(-)) and the single ionized oxygen vacancy (V.O) centers, respectively.
采用多元醇法分别制备了ZnO和ZnO:Zn粉末荧光粉,随后分别在空气中退火和在还原气体中退火。分别通过X射线衍射(XRD)、场发射扫描电子显微镜(FESEM)、X射线光电子能谱(XPS)、电子顺磁共振(EPR)以及光致发光(PL)和阴极发光(CL)光谱对样品进行了表征。结果表明,所有样品均与ZnO相的六方结构一致,粒径在1 - 2微米范围内。在空气中950℃退火的ZnO粉末的PL和CL光谱由一个弱的紫外发射带(约390nm)和一个以约527nm为中心的宽发射带组成,肉眼观察呈现黄色发射。当样品在500至1050℃的温度下还原时,黄色发射逐渐减弱并在800℃时完全消失,而紫外发射带变得最强。高于此温度,绿色发射(约500nm)出现并随着还原温度的升高而增强。根据EPR结果和光谱分析,黄色和绿色发射可能分别源于导带附近的光生电子跃迁到单负电荷间隙氧离子(Oi(-))和单电离氧空位(V.O)中心的深捕获空穴。