Nano-quantum size effect in sol–gel derived mesoporous titania layers deposited on soda-lime glass substrate
Introduction
Titanium dioxide TiO2 is a wide energy band gap n-type semiconductor with wide application due to its optical and electrical properties. Titanium dioxide films are very versatile from the view point of their potential applications such as photocatalyst [1], [2], [3], self-cleaning glasses [4], antireflection [5] or high reflection coatings [6], electrochromic films [7], solar cell [8], [9], [10], transparent conductors [11], protective layers [12], and gas sensitive layers [13], [14], [15]. Titanium dioxide is a component used in planar optical waveguide technology [16], [17]. Many different technological procedures for the fabrication of thin films of titania have been reported, such as e-beam evaporation [14], magnetron sputtering [1], [18], ultrasonic spray pyrolysis [19], chemical vapor deposition [20], metal organic chemical vapor deposition [21], pulsed laser deposition [22], and sol–gel method [3], [4], [5], [6], [7], [10], [13], [15], [23]. The sol–gel method has advantages, such as low temperature processing, easy coating of large area, and being suitable for preparation of porous films and homogeneous multi-component oxide films. In contrast to the other, the sol–gel method is very efficient and does not require expensive technological equipment. The most important advantage of sol–gel over other coating methods is the ability to tailor the microstructure of deposited films [23], so using the sol–gel method titania films of controlled structure can be produced. The properties of sol–gel derived titania films depend on applied technological processes as well as applied substrates. Different procedures of fabrication technology of titania layer with the sol–gel method as well as the properties of the obtained layers have been widely reported in the literature [3], [4], [5], [6], [7], [10], [13], [15], [23], [24]. The influence of substrate type on photocatalytic properties of titania dioxide was discussed in the literature in the past [25], [26], [27]. However, to the best of our knowledge, the problem involving the influence of substrate type on the width of energy gap of the titania layer has not been discussed so far. While investigating thin titania films fabricated on soda-lime glass substrates, we found that there was a non-monotonic dependence of the indirect energy band gap on layer thickness. And that finding stimulated us to undertake the research presented here in order to clarify the origin of the effect. To the best of our knowledge such non-monotonous dependence of indirect energy band gap on layer thickness was not explored earlier. In this paper we present results of our studies of the influence of soda-lime glass substrate on the quantum size effect in sol–gel derived mesoporous titania layers which are demonstrated as blue-shift of optical energy band gap. Fabricated by us via sol–gel route titania layers on soda-lime glass (SLG) substrate exhibit both direct and indirect optical energy band gaps. For the indirect transitions we obtain non monotonic dependence of the energy band gap versus layer thickness while for the direct transition we obtain monotonic one. We present both results for titania layers on SLG substrates pre-coated with the silica films of different thicknesses. The objective of the work was to define the influence of the thickness of the buffer silica layer on the properties of titania layers. The data presented here show that the buffer silica layers are an effective barrier for Na+ ions. However, this layer is simultaneously a cluster of Si ions, which difunds to the TiO2 layer. The concentration of Si4+ in the TiO2 has an influence on the Urbach energy magnitude. The resulting titania layers were characterized by monochromatic ellipsometry, UV–vis spectrophotometry and atomic force microscopy (AFM). The work consists of two main sections. Section 2 of the work contains the description of technological procedures, the applied measurement methods and measurement apparatus, and the results of the carried out research and discussion are presented in Section 3.
Section snippets
Substrates
The titania layers have been fabricated on SLG substrates (microscope slides, Menzel–Glaser) and on soda-lime glass substrates precoated with a SiO2 layer (SLGC). Ultra clean SLG substrates, cleaned as per the procedure described elsewhere [17], were used for titania and silica thin film depositions. The SLG substrates used in the studies contain 14.3 wt % of Na2O as its component. At high temperature the sodium ions Na+ in SLG have high mobility and diffuse to the titania layer coated onto
Titania and silica layers
Fig. 1 presents the influence of withdrawal speed on thickness d and refractive index n of titania layers fabricated on SLG substrate. The experimental dependence of the refractive index on the substrate withdrawal speed was approximated with the linear dependence n=0.00154×v+2.04475 (v in cm/min). It can be observed that the refractive index slightly increases with the rise of substrate withdrawal speed v from the sol. By changing the substrate withdrawal speed v from 3.6 cm/min to 16.7 cm/min,
Summary
The paper presents the results of investigation studies involving the influence of soda-lime glass substrate on the properties of TiO2 layers fabricated via the sol–gel route with the use of dip-coating method. In the studies on the TiO2 layer, optical methods and atomic force microscopy AFM were applied. In the TiO2 layers fabricated on soda-lime glass substrate there occurs quantum size effect, which was used to determine the diameters of anatase nanocrystals. In the TiO2 layers on SLG
Acknowledgments
This work was supported by the National Science Centre on the basis of decision DEC-2011/03/B/ST7/03538.
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