Sambandam
Anandan
*ab,
Nalenthiran
Pugazhenthiran
b,
Thangavel
Selvamani
b,
Shu-Han
Hsieh
a,
Gang-Juan
Lee
a and
Jerry J.
Wu
*a
aDepartment of Environmental Engineering and Science, Feng Chia University, Taichung 407, Taiwan. E-mail: jjwu@fcu.edu.tw; Fax: +886 4 24517686; Tel: +886 4 24517250 Ext. 5206
bNanomaterials and Solar Energy Conversion Lab, Department of Chemistry, National Institute of Technology, Trichy 620 015, India. E-mail: sanand@nitt.edu; Fax: +91 431 2500133; Tel: +91 431 2503639
First published on 3rd August 2012
A semiconductor photocatalytic process has shown great potential as a low cost, environmentally friendly and sustainable treatment technology for the treatment of wastewater. Hence, a wide band gap Ta2O5 semiconductor nanoparticle was prepared by the hydrothermal method and considerable efforts have been taken to narrow the band gap, i.e., the surface modification has been done with a noble metal (Au0) by a deposition precipitation method. As synthesized, Au–Ta2O5 semiconductor was well characterized by X-ray diffraction (XRD), X-ray photo electron spectroscopy (XPS), transmission electron microscopy (TEM) and diffused reflectance UV-vis spectroscopy (DRS). The photocatalytic potential of Au–Ta2O5 semiconductor was investigated by degrading Methyl Orange in the presence and absence of electron acceptors by illuminating with visible light of intensity 80600 ± 10 Lux.
Among the oxide semiconductors, tantalum oxide (Ta2O5) has many outstanding properties such as a wide band gap (∼3.9 eV), photoactivity in near-UV areas, good thermal and chemical stability, good conductivity, good catalyst for a variety of chemical reactions, etc.8–11 Therefore it is being widely studied and used for a wide variety of applications, e.g. as anti-reflection coating for solar cells, wave guides for surface acoustic devices and capacitor material for dynamic random access memories (DRAM).11–18 Hence, we planned to study visible light assisted photocatalytic degradation of organic pollutant (Methyl Orange, MeOr) in aqueous solution using tantalum oxide (Ta2O5) semiconductor. Ta2O5 semiconductor cannot efficiently utilize the visible light of the solar energy because of its comparably large band gap. To overcome the above problem, considerable efforts have been taken to narrow the band gap, i.e., surface modification with a noble metal (Au0) have been explored in an effort to increase visible light absorption or suppress recombination of photogenerated carriers owing to the unique plasmon absorbance features.19–26 To the best of our knowledge, investigations on the preparation and characterization of gold embedded tantalum oxide (Au–Ta2O5) for photocatalytic degradation of Methyl Orange have never been reported. The activity of Au–Ta2O5 nanoparticle is enhanced further by adding external electron acceptors such as PMS (peroxomonosulphate), PDS (peroxodisulphate) and H2O2 (hydrogen peroxide) which also suppresses the recombination of photogenerated carriers.
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Fig. 1 XRD spectra of Ta2O5 and Au–Ta2O5 nanoparticle. |
The chemical composition of as-prepared Ta2O5 and Au–Ta2O5 nanoparticles was obtained by XPS measurements. No peak of other elements except C, O, Ta and Au indicates the observed product was highly pure (Fig. 2A). In the XPS spectra of the as-prepared Ta2O5 and Au–Ta2O5 nanoparticles, Ta (4f7/2) and Ta (4f5/2) peaks lie at 23.5 and 24.9 eV (Fig. 2B), the C (1s) peak lies at 284 eV (Fig. 2C), the broad peak that lies at 528 eV is assigned to O (1s) (Fig. 2D), and finally Au (4f7/2) peaks lies at 81.2 eV and Au (4f5/2) peak lies at 85.2 eV (Fig. 2E). These energy values correspond to Ta5+ in Ta2O5 and Au(0) in Au–Ta2O5 as reported in the literature.17,32–34
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Fig. 2 XPS spectra of Au–Ta2O5 nanoparticle. (A) Survey spectrum, (B) Ta (4f) line, (C) C(1s) line, (D) O (1s) line and (E) Au (4f) line. |
TEM and HRTEM images of Ta2O5 and Au–Ta2O5 are presented in Fig. 3. As-prepared Ta2O5 exists as sphere like morphology with a uniform grain size in the range 25–30 nm. HRTEM analysis provides further insight into the nanostructure i.e., the observed lattice fringes may belong to the individual nanocrystal of the Ta2O5 sphere, which is consistent with the (200) plane as reported earlier by Agrawal et al.35,36 In addition, the fast Fourier transform (FFT) image (Fig. 3E) of the selected area of HRTEM micrograph, shows a polycrystalline ring diffraction pattern, which may correspond to L-Ta2O5 crystalline phase.31 Upon deposition of Au on the Ta2O5 crystalline phase, the dimensional uniform (sphere morphology) of Ta2O5 is lost, while in addition the particle size increases to 100 nm and above (Fig. 3C). Also the observed HRTEM (Fig. 3D) and the fast Fourier transform (FFT) image (Fig. 3F) are different from the earlier, i.e., the selected area of the HRTEM micrograph shows both polycrystalline diffraction rings and single crystal diffraction dots which correspond to both Ta2O5 and Au nanoparticles. The composition of the prepared material (Au–Ta2O5) was determined by the EDX technique (Fig. 3G), which supports the presence of 8 atomic weight percentage of Au in Ta2O5. The observed TEM image looks big in size after gold doping, which may be due to Ta2O5 particles joined together to form nanosheet-like morphology without any change in the orthorhombic β-phase of Ta2O5.
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Fig. 3 TEM and HRTEM image of Ta2O5 (A, B) and Au–Ta2O5 (C, D) nanoparticle. FFT image of Ta2O5 (E) and Au–Ta2O5 (F). EDX pattern (G) and elemental composition of Au–Ta2O5 nanoparticle are provided. |
The UV-vis diffused absorbance spectrum of Ta2O5 and Au–Ta2O5 are shown in Fig. 4. Pure Ta2O5 nanoparticles show an absorption onset band in the UV region at approximately 340 nm (band gap calculated is ∼3.55 eV from Tauc plot, see inset of Fig. 4), which may be indexed to the presence of Ta species as Ta5+ due to the electronic excitation of the valence band O (2P) electron to the conduction band Ta (5d) level.17,37,38 However in the case of prepared Au–Ta2O5 nanoparticles, a new absorption band (around 580 nm) is seen in the visible region and may be due to the surface plasmon resonance of Au0 nanoparticles impregnated on the surface of Ta2O5 nanoparticles. The band gap calculated for Au–Ta2O5 nanoparticles is ∼3.09 eV from the Tauc plot (see inset of Fig. 4).
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Fig. 4 Solid state diffuse reflectance UV-vis spectra of Ta2O5 and Au–Ta2O5 nanoparticle. Inset shows the corresponding Tauc plots. |
Under visible light irradiation, the photocatalytic degradation of Methyl Orange (MeOr) was performed using prepared Au–Ta2O5 nanoparticles. After confirming that there is no appreciable degradation of MeOr with Au–Ta2O5/visible light irradiation alone, we studied photocatalytic degradation of MeOr (5 × 10−5 M) in the presence of both Au–Ta2O5 nanoparticles (0.2 to 1.8 g L−1) and visible light (80600 ± 10 Lux) by monitoring the decrease in the absorption maxima of MeOr (λmax 493 nm) as a function of irradiation time in 1 h using UV-vis absorption spectroscopy. First order rate constants were evaluated from the slopes of the -ln[C/Co] vs. time plots (Fig. 5). The optimum concentration of Au–Ta2O5 nanocatalysts provides maximum photocatalytic efficiency at 1 g L−1 (1.2 × 10−4 s−1; see inset of Fig. 5) which is comparatively higher than the rate obtained for bare Ta2O5 nanocatalyst (0.3 × 10−4 s−1) with the same concentration. Generally, the photocatalytic activity depends on the optimal amount of the catalyst loading and the total number of incident photons available in the reaction medium. This can be rationalized in terms of availability of active sites on Au–Ta2O5 surface and the light penetration into the suspension. The availability of the active sites increases with an increase in the catalyst loading up to 1 g L−1 of Au–Ta2O5 nanoparticles. However, increasing the catalyst loading beyond 1 g L−1, the light scattering effect induced by the Au–Ta2O5 catalyst also increased, which reduced the number of photons available for photocatalytic reactions and as a consequence, the rate of photocatalytic activity got reduced (inset of Fig. 5). Therefore, 1 g L−1 of Au–Ta2O5 catalyst loading was considered as the optimum quantity for the photocatalytic degradation of Methyl Orange. Furthermore, the photoexcited semiconductor nanoparticles undergo charge equilibration when they are in contact with metal nanoparticles by shifting the Fermi level to more negative potentials. The negative shift in the Fermi level is an indication of better electron and hole charge separation and more reductive power towards the degradation of pollutants. This may be due to the surface plasmon resonance of Au0 nanoparticles impregnated on the surface of Ta2O5 nanoparticles which absorbs a higher number of photons at that concentration. That is, gold present in the Au–Ta2O5 can enhance the photocatalytic activity by creating a local electric field (oxygen vacancy and crystal defects) and in addition the optical vibration of the gold surface plasmon can make a reasonable alternation in the Fermi level equilibration, which leads to easier electronic transition from the valence band O (2P) electron to the conduction band Ta (5d) level.38
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Fig. 5 Plot of variation of Au–Ta2O5 nanoparticle ((■) 0.2 g L−1, (●) 0.6 g L−1, (▲) 1.0 g L−1, (▼) 1.4 g L−1, (◆) 1.8 g L−1) upon irradiation time in the presence of fixed initial concentration of MeOr (5 × 10−5 M). Inset shows a plot of the photodegradation rate of various concentrations of Au–Ta2O5 nanoparticles. |
To enhance the photocatalytic activity of Au–Ta2O5 nanocatalysts further, experiments were carried out with external electron acceptors such as PMS, PDS and H2O2, and the observed rate constants (Table 1) are in the following order, i.e., PMS (10.09 × 10−4 s−1) > PDS (3.89 × 10−4 s−1) > H2O2 (3.21 × 10−4 s−1) (experimental conditions are as follows: MeOr (5 × 10−5 M); Au–Ta2O5 (1 g L−1) and PMS = PDS = H2O2 (0.25 mM) (Fig. 6). The use of these electron acceptors alone in the absence of Au–Ta2O5 nanocatalysts did not degrade the MeOr dye. Such an enhanced rate constant may be due to the (i) generation of surface active radicals by a reaction between electron acceptors and Au–Ta2O5 nanocatalysts23,34,38,39 and (ii) immediate trapping of the photogenerated electrons by the electron acceptors.23,39 Finally, the extent of photocatalyzed mineralization of MeOr was measured in the presence of Au–Ta2O5 and electron acceptors after 8 h illumination of visible light (Fig. 7). With Au–Ta2O5 and electron acceptor (PMS) about 57% of the TOC was removed after discoloration of MeOr. However with bare Au–Ta2O5 the mineralization of MeOr took place at a much lower rate and TOC was reduced to only 28%, while the rate of mineralization is 42 and 37% in the case of PDS and H2O2. Thus, the addition of electron acceptors to the Au–Ta2O5 nanocatalyst accelerates the mineralization process, which may be due to the generation of surface active radicals by a reaction between electron acceptors and Au–Ta2O5. Hence in the available literature,23,34,38 it is considered that the embedded Au on Ta2O5 upon illumination by visible light can promote the transfer of electrons (e−) in the Ta2O5 conduction band to outer oxygen, which is dissolved in water and meanwhile it degrades the MeOr. However the electrons would be promptly transported in the case of added electron acceptors, which avoid recombination of e−/h+ pairs. Thus, these studies clearly indicate that excitation of surface plasmons may play a major role for the visible light assisted photocatalytic activity. Linic et al.40 explained the role of surface plasmon mediated chemical transformations by predicting three different possible mechanisms, however many different factors affect the overall performance. Therefore, further research is ongoing in our lab to predict the perfect mechanism.
S. No. | Name of catalyst | Name of oxidant | Presence of light | Absence of light | Rate constant × 10−4 (s−1) |
---|---|---|---|---|---|
1 | — | — | Yes | — | 0.000012 |
2 | Ta2O5 | — | Yes | — | 0.31 |
3 | Ta2O5 | PMS | Yes | — | 0.71 |
4 | Ta2O5 | PDS | Yes | — | 0.45 |
5 | Ta2O5 | H2O2 | Yes | — | 0.42 |
6 | Au-Ta2O5 | — | — | Yes | 0.0000667 |
Yes | — | 1.2 | |||
7 | Au-Ta2O5 | PMS | — | Yes | 0.000765 |
Yes | — | 10.09 | |||
8 | Au-Ta2O5 | PDS | — | Yes | 0.0000987 |
Yes | — | 3.89 | |||
9 | Au-Ta2O5 | H2O2 | — | Yes | 0.000087 |
Yes | — | 3.21 |
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Fig. 6 Comparison of the photocatalytic degradation rate of MeOr in the presence of Ta2O5, Au–Ta2O5 nanoparticles with and without electron transfer agents. Concentrations are maintained as follows: MeOr (5 × 10−5 M), PMS = PDS = H2O2 (0.25 mM), Ta2O5 = Au–Ta2O5 = 1 g L−1. Bar diagram notations A1, B1, C1 and D1 are Au–Ta2O5/PMS, Au–Ta2O5/PDS, Au–Ta2O5/H2O2 and Au–Ta2O5 alone respectively under illumination of visible light whereas under dark conditions are indicated as notations A2, B2, C2 and D2. Illumination experiments with bare Ta2O5 alone, Ta2O5/PMS, Ta2O5/PDS and Ta2O5/H2O2 are indicated as E, F, G and H respectively. Notations I is a control experiment in the presence of visible light only without any catalyst and electron transfer agents. |
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Fig. 7 Comparison of the photomineralization rate of MeOr in the presence of Au–Ta2O5 nanoparticle without any electron transfer agents (◆), Au–Ta2O5with PMS (■), PDS (▲) and H2O2 (×). Concentrations are maintained as follows: MeOr (5 × 10−5 M), PMS=PDS = H2O2 (0.25 mM), Au–Ta2O5 = 1 g L−1. |
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