Wang Juan, Li Quan, Egerton R F
Department of Physics, The Chinese University of Hong Kong, Shatin, New Territory, Hong Kong, China.
Micron. 2007;38(4):346-53. doi: 10.1016/j.micron.2006.06.003. Epub 2006 Jul 18.
Valence electron energy loss spectroscopy in a transmission electron microscope is employed to investigate the electronic structure of ZnO nanowires with diameter ranging from 20 to 100 nm. Its excellent spatial resolution enables this technique to explore the electronic states of a single nanowire. We found that all of the basic electronic structure characteristics of the ZnO nanowires, including the 3.3 eV band gap, the single electron interband transitions at approximately = 9.5, approximately = 13.5,and approximately = 21.8 eV, and the bulk plasmon oscillation at approximately 18.8 eV, resemble those of the bulk ZnO. Momentum transfer resolved energy loss spectra suggest that the 13.5 eV excitation is actually consisted of two weak excitations at approximately = 12.8 and approximately = 14.8 eV, which originate from transitions of two groups of the Zn 3d electrons to the empty density of states in the conduction band, with a dipole-forbidden nature. The energy loss spectra taken from single nanowires of different diameters show several size-dependent features, including an increase in the oscillator strength of the surface plasmon resonance at approximately = 11.5 eV, a broadening of the bulk plasmon peak, and splitting of the O 2s transition at approximately = 21.8 eV into two peaks, which coincides with a redshift of the bulk plasmon peak, when the nanowire diameter decreases. All these observations can be well explained by the increased surface/volume ratio in nanowires of small diameter.
利用透射电子显微镜中的价电子能量损失谱来研究直径范围为20至100纳米的ZnO纳米线的电子结构。其出色的空间分辨率使该技术能够探索单根纳米线的电子态。我们发现,ZnO纳米线的所有基本电子结构特征,包括3.3电子伏特的带隙、在约9.5、约13.5和约21.8电子伏特处的单电子带间跃迁,以及在约18.8电子伏特处的体等离子体振荡,都与块状ZnO的相似。动量转移分辨能量损失谱表明,13.5电子伏特的激发实际上由在约12.8和约14.8电子伏特处的两个弱激发组成,它们源于两组Zn 3d电子向导带中空态密度的跃迁,具有偶极禁戒性质。从不同直径的单根纳米线获取的能量损失谱显示出几个与尺寸相关的特征,包括在约11.5电子伏特处表面等离子体共振的振子强度增加、体等离子体峰变宽,以及在约21.8电子伏特处O 2s跃迁分裂为两个峰,当纳米线直径减小时,这与体等离子体峰的红移相吻合。所有这些观察结果都可以通过小直径纳米线中增加的表面/体积比得到很好的解释。