High-aspect-ratio TiO2 nanotubes by anodization of titanium
High-aspect-ratio TiO2 nanotubes by anodization of titanium
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DOI:
10.1002/anie.200462459
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发表时间:
2005-01-01
影响因子:
16.6
通讯作者:
Schmuki, P
中科院分区:
文献类型:
--
作者:
Macák, JM;Tsuchiya, H;Schmuki, P
Nanotubular material surfaces produced by the electrochemical formation of self-organized porous structures on materials such as aluminum [1, 2] and silicon [3, 4] have attracted significant interest in recent years. While scientific thrust is often directed towards the elucidation of the principles of the self-organization phenomena, technological efforts target applications based on the direct use of the high surface area, for example, for sensing [5, 6] or controlled catalysis,[7] exploit the optical properties in photonic crystals,[8] waveguides,[9] or in 3D arranged Bragg-stack type of reflectors.[10] The highly organized structures may be used indirectly as templates [11] for the deposition of other materials such as metals,[12] semiconductors,[13] or polymers.[14] Over the past few years, nanoporous TiO2 structures have also been formed by electrochemical anodization of titanium.[15–17] Although several applications have been proposed,[18, 19] a wider impact of these structures has been hampered by the fact that the layers could only been grown to a limiting thickness of a few hundreds of nanometers.Herein we demonstrate for the first time how high-aspectratio, self-organized, TiO2 films can be grown by tailoring the electrochemical conditions during titanium anodization. Figure1 shows scanning electron microscope (SEM) images of self-organized porous titanium oxide formed to a thickness of approximately 2.5 μm in 1m (NH4) 2SO4 electrolyte containing 0.5 wt.% NH4F. From the SEM images it is evident that the self-organized regular porous structure consists of pore arrays with a uniform pore diameter of approximately 100 nm and an average spacing of 150 nm. It is also clear that pore mouths are open on the top of the layer while on the bottom of the structure the tubes are closed by presence of an about 50-nm thick barrier layer of TiO2. The key to achieve high-aspect-ratio growth is to adjust the dissolution rate of TiO2 by localized acidification at the pore bottom while a protective environment is maintained along the pore walls and at the pore mouth. In our previous work in HF and NaF solutions [15, 20] it was established that the thickness of the porous layer is essentially the result of an equilibrium between electrochemical formation of TiO2 at the pore bottom and the chemical dissolution of this TiO2 in an FÀ ion containing solution (Figure 2). The solubility of TiO2 in