ZHANG Ning, LI Qing-shan, ZHAO Bo, WANG Jing-jing, CHEN Da, YANG Ya-jun, ZHENG Xue-gang, SHI Ming-ji, QI Hong-xia. Influence of Annealing on the Structure and Photoluminescence of ZnO Thin Films Made by Sol-gel Method[J]. Chinese Journal of Luminescence, 2006,27(5): 782-786
ZHANG Ning, LI Qing-shan, ZHAO Bo, WANG Jing-jing, CHEN Da, YANG Ya-jun, ZHENG Xue-gang, SHI Ming-ji, QI Hong-xia. Influence of Annealing on the Structure and Photoluminescence of ZnO Thin Films Made by Sol-gel Method[J]. Chinese Journal of Luminescence, 2006,27(5): 782-786DOI:
Zinc oxide with high stability and a direct band gap of 3.37eV has attracted tremendous attention in recent years because of its high potential for application as short wavelength optical devices. Several techniques such as pulsed laser deposition
reactive thermal evaporation
sol-gel have been employed to synthesize high quality ZnO thin films. Sol-gel method was adopted to make ZnO thin films on n-Si (100) and they could be investigated from three parts. The X-ray diffraction spectra indicates that the structure of the ZnO thin films is polycrystal wurtzite structure with
c
axis preferred orientation. The annealing time and the annealing tempe-rature has great effect on the structure and particle size of the films
the proximate annealing temperature is around 500℃ by comprehensive experiments. The surface and profile character of the ZnO thin films can be observed by the Scanning Electrical Microscopy
which indicates that the growth of the films is uniform
the polycrystalline dimensions were determined to be in the range of 70~160 nm
consistent with the X-ray diffraction results. The optical properties of ZnO nanowires were investigated by room-temperature photoluminescence spectroscopy using a Xe lamp with an excitation wavelength of 230 nm. The photoluminescence of the ZnO sol indicates that as the aging time went on
the ultraviolet peak position moved to the short wavelength
from 342 to 340
339 nm. The photoluminescence spectrum of the ZnO thin films at room temperature indicates that the ultraviolet peak positions were at 365
390 nm
and the intensities of the emission were stronger
while the visible emission at 435 nm didn’t change obviously. The stronger peak positions at 460 and 690 nm are twice and three times frequency multiplication of the excitation light. The visible emission showed a weaker deep-level green emission than UV emission without being completely restrained. The PLspectra showed a strong peak around 390 nm at room temperature