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东南大学, 电子科学与工程学院,江苏 南京,210096
收稿日期:2007-08-25,
修回日期:2007-11-24,
纸质出版日期:2008-05-20
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屈科, 张晓兵, 雷威, 侯凯, 李驰, 杨夏喜. 四针氧化锌制备及其场致发射特性[J]. 发光学报, 2008,29(3): 542-546
QU Ke, ZHANG Xiao-bing, LEI Wei, HOU Kai, LI Chi, YANG Xia-xi. Synthesis of Tetrapod-like Zinc Oxide and Its Field Emission Characteristic[J]. Chinese Journal of Luminescence, 2008,29(3): 542-546
采用了VS(Vapor-Solid)的方法制备了四针状ZnO
以此作为场致电子发射的冷阴极材料。并对材料进行了扫描电镜(SEM)和X射线粉末衍射(XRD)测试分析
揭示其表面形态和晶体结构。同时将阴极与印刷有荧光粉的阳极板组装成二极管结构场致发射显示屏
并进行了场致发射特性实验。该二极管结构的开启电压为3.6V/μm
其阈值电压为6.6V/μm
相应的电流密度为0.2mA/cm
2
并且具有稳定的电流密度和均匀的显示效果。实验证明ZnO是一种优良的场致发射冷阴极材料
具有广阔的应用前景。
Much effort has been devoted to the development of cold cathodes in field emission flat panel display and vacuum microelectronic devices. Electron field emission from various nanostructure materials has drawn significant attention of the industrial and scientific communities over world wide. One of the cold cathodes is zinc oxide (ZnO). ZnO-based nanostructure materials have attracted great interest recently due to their potential applications such as ultraviolet nanowire nanolasers
gas sensors
solar cells and field emission (FE) devices. Zinc oxide is a Ⅱ-Ⅳ compound semiconductor with a direct wide bandgap (3.37 eV) and large exciton binding energy (60 meV). Several methods have been reported for the synthesis of one-dimensional (1D) ZnO nanostructures such as nanowires
nanorods
and nanobelts. Comparing to carbon-based materials
the ZnO nanostructure has a unique advantage. Using carbon-based materials
we have to encounter a strict requirement on vacuum. If not
it will be oxidized with the growth of vacuum and temperature. ZnO nanostructure would last longer under the same vacuum for carbon-based FE device. The tetrapod-like zinc oxide synthesized by Vapor-Solid method was applied to the field emission display as the cold cathode material. Our ZnO nanostructures were prepared by oxidizing Zn vapor in a horizontal tube furnace. The source material was Zn (99.9%) powder
which was loaded in a horizontal quartz tube placed in the constant temperature zone of the tube furnace. Ar at a flow rate of 300 sccm was used first to purge the reactor for 30 min. Then the furnace was heated to 850℃ at a heating rate of 25℃/min and kept at 850℃ for 30 min at a flow rate of 70 sccm Ar and 40 sccm O
2
. Finally
after cooling down the furnace naturally to room temperature under the protection of an Ar flow
the fluffy
white ZnO was collected from the quartz tube. We introduced SEM and XRD to show the morphology and structure of the tetrapod-like zinc oxide.The field emission characteristics are evaluated by the simplified Fowler-Nordheim (FN) equation
J
=
A
(β
2
V
2
/Φ
d
2
)exp(-
B
Φ
3/2
d
/β
V
)
where
J
is the current density
A
and
B
are constants with values of
A
=1.56×10
-10
A·V
-2
·eV
B
=6.8×10
3
V·eV
-3/2
·μm
-1
respectively
β is a field enhancement factor which quantifies the field enhancement due to microstructure roughness
Φ is the work function of ZnO (5.3 eV)
d is a distance between the anode and cathode and V is the applied voltage. The characteristic of the diode structure was researched and the anode display image was presented. The turn-on field was 3.6 V·μm
-1
and the threshold field was 6.6 V/μm with the current density of 0.2 mA·cm
-2
. From the stable field emission and uniform display image
we can conclude that the tetrapod-like zinc oxide is an excellent cold cathode material for field emission and has a potential application in the vacuum nano-electronics.
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