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International Journal of Photoenergy
Volume 2012 (2012), Article ID 198497, 6 pages
http://dx.doi.org/10.1155/2012/198497
Research Article

Hydrothermal Synthesis of Nitrogen-Doped Titanium Dioxide and Evaluation of Its Visible Light Photocatalytic Activity

Key Laboratory for Special Functional Materials, Henan University, Kaifeng 475004, China

Received 14 September 2011; Revised 6 November 2011; Accepted 8 December 2011

Academic Editor: Mietek Jaroniec

Copyright © 2012 Junjie Qian et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

Nitrogen-doped titanium dioxide (N-doped ) photocatalyst was synthesized from nanotube titanic acid (denoted as NTA; molecular formula ) precursor via a hydrothermal route in ammonia solution. As-synthesized N-doped catalysts were characterized by means of X-ray diffraction, transmission electron microscopy, diffuse reflectance spectrometry, X-ray photoelectron spectroscopy, electron spin resonance spectrometry and Fourier transform infrared spectrometry. It was found that nanotube ammonium titanate (NAT) was produced as an intermediate during the preparation of N-doped from NTA, as evidenced by the N1s X-ray photoelectron spectroscopic peak of at 401.7 eV. The catalyst showed much higher activities to the degradation of methylene blue and p-chlorophenol under visible light irradiation than Degussa P25. This could be attributed to the enhanced absorption of N-doped in visible light region associated with the formation of single-electron-trapped oxygen vacancies and the inhibition of recombination of photo-generated electron-hole pair by doped nitrogen.

1. Introduction

Titania, as a currently known most effective photocatalyst, have been widely applied in purifying air and water, deodorization, and many other environmentally related fields [1]. However, TiO2 can only be induced by ultraviolet (UV), due to its large bandgap of ca. 3 eV [2]. As a result, TiO2 in practical application can only utilize a small fraction (~5%) of solar energy [3]. To increase the efficiency for solar energy transformation and utilization, many researchers have attempted to extend the absorption range of TiO2 from UV region to visible light (Vis in short) region by doping various cations [46] and anions [7, 8]. It has been found that N doping induces considerable visible light response of anatase TiO2; the mechanisms for the visible light response of N-doped TiO2, however, still remain disputable. About one decade ago, Asahi et al. reported a visible light active TiO2−x Nx film by sputtering a TiO2 target in the mixture of N2 and Ar (volume ratio 40% : 60%); and they suggested that the incorporation of dopant N atom into the crystal lattice of TiO2 via substituting Ti atom was indispensable for band-gap narrowing and photocatalytic activity generation [9]. In 2003, Irie et al. reported a TiO2−x Nx powder prepared by annealing anatase TiO2 under an ammonia flow; and they supposed that the isolated narrow band formed above the valence band of TiO2 was responsible for the visible light response of N-doped TiO2 [10]. Ihara et al. also prepared a visible light responsive photocatalyst by treating the hydrolysis product of Ti(SO4)2 in ammonia (a precursor for N doping); and they deduced that oxygen-deficient sites formed in grain boundaries gave rise to visible light activity of as-prepared N-doped product, while doped N at oxygen-deficient sites played a key role as a blocker for reoxidation [11]. Zhang et al. observed that the visible-light absorption of vacuum-dehydrated product of NTA was proportional to the intensity of electron spin resonance (ESR) signal [12]. We supposed in our previous researches that the visible light sensitization of N-doped TiO2 was due to the formation of single-electron-trapped oxygen vacancies (SETOVs), and doped-N played a role in preventing photogenerated electrons and holes from recombination [12, 13].

In the present research, we make use of a hydrothermal method to prepare N-doped TiO2 by selecting NTA as a precursor, hoping to harvest TiO2-based photocatalyst with high visible light activity while heat-treatment temperature is considerably lowered as compared with that for calcination of NTA in flowing ammonia [12]. This article reports the preparation and characterization of N-doped TiO2 photocatalyst, as well as its photocatalytic activity for the degradation of methylene blue (MB) and p-chlorophenol (4-CP) under visible light irradiation.

2. Experimental Section

2.1. Preparation of Samples

NTA was prepared using the method reported in literature [14]. N-doped TiO2 powders were prepared using a two-step protocol. Firstly, 1 g of NTA and 50 mL of ammonia solution (mass fraction 25%~28%) was added into a Teflon-lined stainless steel autoclave (75 mL) and airproofed and heated at 130, 160 and 210°C for 3 h in an oven. Then, the autoclave was cooled in air down to room temperature after the reaction was completed, followed by filtration, drying at 60°C in vacuum (−0.1 MPa) overnight, and grounding to yield samples denoted as N-NTA-130, N-NTA-160, and N-NTA-210, respectively. Sample H-NTA-210 for a comparative study was also prepared in the same manners except that distilled water was used to replace ammonia solution.

2.2. Characterization

X-ray diffraction (XRD) patterns were measured with a Philips X’Pert Pro X-ray diffractometer (Cu radiation, 2θ range 7~90°, scan step size 0.04°, scanning interval 0.5 s, generator voltage 40 kV, tube current 40 mA). A JEM-100CX transmission electron microscope (TEM; JEOL Ltd., Japan) was performed at an accelerating voltage of 100 kV to observe the morphology and microstructure of various as-prepared photocatalysts. Diffuse reflection spectra (DRS) were obtained with a UV-Vis spectrophotometer (UV-3010; Shimadzu, Japan; reference: BaSO4). An Axis Ultra X-ray photoelectron spectroscope (XPS; Kratos, England) equipped with a multichannel detector was performed to analyze the chemical states of various photocatalysts, where Al radiation was used as the excitation source. All the binding energies were referenced to the C1s peak at 284.8 eV of surface adventitious carbon. Electron spin resonance (ESR) spectra were collected with a Brüker ESP 300E apparatus (reference: diphenyl-picryl hydrazide (DPPH), ). Fourier transform infrared (FTIR) spectra were recorded with a Nicolet 360 spectrometer (Nicolet Company, USA).

2.3. Evaluation of Visible Light Photocatalytic Activity

The photocatalytic activities of various photocatalysts were evaluated by monitoring the degradation of MB and 4-CP under the irradiation of a 500 W xenon lamp as the light source with which a filter and a water cell were attached to eliminate UV and infrared light. Into a quartz reactor (140 mL) charged with 100 mL of the aqueous solution of MB (10 mg/L) or 4-CP (0.15 mM) was added 100 mg of to-be-tested photocatalyst powder. The adsorption equilibrium of aqueous MB or 4-CP on the photocatalyt was reached in the reactor prior to irradiation. The concentration of MB was monitored with a visible light spectrometer (722, Shanghai Jingke Instrument Plant, China) at 664 nm, and that of 4-CP was measured with an UV-Vis spectrometer (752, Shanghai Oppler Instrument Plant, China) at 225 nm.

3. Results and Discussion

The XRD patterns of undoped TiO2 and three N-doped TiO2 samples are compared in Figure 1. Samples N-NTA-130 and N-NTA-160 still retain the orthorhombic form (inset in Figure 1) and nanotubular morphology of precursor NTA (Figure 2). This differs from our previous finding in that the tubular shape of orthorhombic NTA is destroyed in association with conversion into anatase TiO2 when NTA is heated in distilled water at 130°C or 160°C [15]. However, sample N-NTA-210 shows strong diffraction peaks of anatase TiO2 as well as additional diffraction peaks of rutile phase (27.4, 36.1, 39.2, 41.2, 44.1, and 56.6°), which indicates that hydrothermal treatment of orthorhombic NTA in ammonia solution at an elevated temperature of 210°C also facilitates its transformation to TiO2. In the meantime, all the XRD peaks of sample H-NTA-210 can be well indexed as anatase TiO2 (25.4, 37.9, 48.2, 54.1, and 55.2°); and both H-NTA-210 and N-NTA-210 have diamond shapes, but the size of the former is a little bit smaller than that of the latter (Figure 2). We assume that nanotube ammonium titanate (NAT) is formed as an intermediate through a simple acid-base reaction (1) when NTA is hydrothermally treated in ammonia at 130°C or 160°C, but it is transformed to TiO2 at 210°C (reacthion (2)). This supposition is supported by corresponding FTIR data shown in Figure 3. Namely, both N-NTA-130 and N-NTA-160 show a broad band at 3400 cm−1 and a sharp peak at 1630 cm−1 attributed to the stretching vibration and flexural vibration of hydroxyl groups [16] as well as a broad band within 750~400 cm−1 corresponding to the flexural vibration of Ti–O and Ti–O–Ti groups. Particularly, they also show the stretching and flexural vibration bands of N-H at 3140 cm−1 and 1400 cm−1 [17], which confirms that intermediate NAT is indeed generated during hydrothermal treatment of NTA in ammonia at 130°C or 160°C. However, no stretching and flexural vibration bands of N-H are observed for N-NTA-210, which is due to the decomposition of intermediate NAT at an elevated temperature of 210°C: XPS spectra of NTA and various N-doped TiO2 samples were measured to further elucidate the chemical states of N. As shown in Figure 4, precursor NTA shows no N1s XPS signal; but samples N-NTA-130, N-NTA-160, and N-NTA-210 show N1s XPS peaks at 400.0 eV and 401.7 eV. It is usually recognized that N1s XPS peak of N-doped TiO2 at 397.0 eV is assigned to atomic Ti–N [12, 1820]; but the assignment of the N1s XPS peaks at 400.0 eV and 401.7 eV are still under argument. Asahi et al. assigned them as molecularly chemisorbed γ-N2, but Sato et al. argued that molecular N2 could not be adsorbed on metal oxide like TiO2 at room temperature and suggested that the N1s core level of N-doped TiO2 at 400.0 eV was attributed to N–O bonding (i.e., Ti–O–N), possibly at interstitial site [20]. Irie et al. assigned the N1s XPS peak of N-doped TiO2 at 400.0 eV as NO [10]. In the present research, the N1s XPS peak at ca. 401.7 eV confirms the presence of N in a third chemical state. Since this N1s XPS peak is only observed for N-NTA-130 and N-NTA-160 but not for N-NTA-210, we tentatively assign it as of intermediate NAT, as evidenced by relevant FTIR analyses.

198497.fig.001
Figure 1: XRD patterns of (a) H-NTA-210 and (b) N-NTA-210. The inset shows the XRD patterns of orthorhombic systems of (c) NTA, (d) N-NTA-130, and (e) N-NTA-160.
fig2
Figure 2: TEM images of (a) NTA, (b) N-NTA-130, (c) N-NTA-160, (d) H-NTA-210, and (e) N-NTA-210.
198497.fig.003
Figure 3: FTIR spectra of (a) N-NTA-130, (b) N-NTA-160, (c) N-NTA-210, and (d) reference (NH4)2SO4.
198497.fig.004
Figure 4: XPS spectra of (a) N-NTA-130, (b) N-NTA-160, and (c) N-NTA-210.

Photocatalytic tests indicate that samples NTA, N-NTA-130, and N-NTA-160 have no photocatalytic activity for the discoloration of MB; but sample N-NTA-210 is able to effectively catalyze the discoloration reaction of MB, following the first-order reaction kinetics model (the kinetic constants are ranked as k(N-NTA-210) > k(H-NTA-210) > k(P25), see Figure 5. In the meantime, NTA, N-NTA-130, and N-NTA-160 are inert to the degradation of colorless organic pollutant 4-CP under visible light irradiation; but H-NTA-210 and N-NTA-210 can well accelerate the degradation of 4-CP under the same conditions, and N-NTA-210 possesses better photocatalytic activity than H-NTA-210 (Figure 6).

198497.fig.005
Figure 5: Kinetics of the photocatalytic decomposition of MB on different TiO2 powders under visible light irradiation: (a) P25, (b) H-NTA-210, and (c) N-NTA-210.
198497.fig.006
Figure 6: Photocatalytic degradation of p-chlorophenol on P25, H-NTA-210, and N-NTA-210.

It is well known that photocatalytic activity is dependent on light absorption efficiency and separation efficiency of photogenerated electrons and holes. Figure 7 shows the UV-Vis spectra of various photocatalysts. Precursor NTA does not show any absorption in visible light region, but samples H-NTA-210 and N-NTA-210 both show broadened absorptions at , which corresponds to their enhanced ESR signals at (Figure 8) and accounts for better visible photocatalytic activity of N-NTA-210 as compared with Degussa P25. Besides, the present research once again provides evidence to the supposition that SETOV density in TiO2 lattice is proportional to the absorption intensity of the photocatalyst in visible light region (Figure 9) [12, 2123].

198497.fig.007
Figure 7: DRS of H-NTA-210, N-NTA-210 and P25.
198497.fig.008
Figure 8: ESR spectra of (a) H-NTA-210, (b) N-NTA-210, and (c) P25 (reference compound: diphenyl picryl hydrazyl (DPPH), ).
198497.fig.009
Figure 9: The relation between intensity of value signal and visible light absorption of three TiO2 samples; h(ESR) refers to the signal intensity at g = 2.003, h(F(R′)) refers to the absorption intensity at 450 nm, F(R′) = (1−)2/(2), F(R′) and refer to absorptivity and reflectance at λ = 450 nm.

Aside from the light absorption efficiency, the separation efficiency of electrons and holes is another important factor to influence the activity of photocatalysts. Ordinarily, photoinduced electrons and holes can be generated in photocatalysts under light excitation; and the photoinduced electrons and holes can be separated on the surface of photocatalysts to take part in chemical reactions or recombine. Some researchers have reported that the mixed crystal effect and high crystallinity in a semiconductor is in favor of retarding the recombination of photogenerated electrons and holes [24, 25], resulting in enhanced photocatalytic activity. This, however, does not seem to be dominant in the present research. Namely, although H-NTA-210 has a stronger SETOV intensity and broader visible light absorption than N-NTA-210, the former possesses poorer photocatalytic activity than the latter. The enhanced photocatalytic activity of N-NTA-210 as compared with that of H-NTA-210, that we suppose, may be attributed to N doping which retards the recombination of photoinduced electrons and holes in TiO2 matrix. This can be described using equations (3)–(5) [13]. Briefly, photoinduced electrons in TiO2 matrix arrive at the intraband contributed by SETOV ((3); refers to SETOV), but they tend to jump back and recombine with holes. When nitrogen atoms are doped into TiO2 lattices, the back-jumping routes are forbidden and the recombination is reduced greatly, allowing more photoinduced electrons to take part in the chemical reactions. In the meantime, N atoms in Ti–O–N bond occupy interstitial sites and allow their electron clouds to transfer towards O atom with a higher electronegativity. As a result, dopant N in N-doped TiO2 possesses a higher chemical valence than the N in and is able to entrap another electron from ((4); refers to double-electron-trapped oxygen vacancy). Nevertheless, interstitial N atom with an excessive electron is unstable and allows its electron could to transfer towards O2 molecule in gas or solution medium (5). Although Ti–O–N bond also exists in samples N-NTA-130 and N-NTA-160 as in N-NTA-210, N-NTA-130 and N-NTA-160 without SETOV do not possess visible light photocatalytic activity:

4. Summary

A simple and mild hydrothermal method has been established to prepare nanoscale N-doped TiO2 photocatalyst with good visible light catalytic activity, where heat treatment of precursor NTA in ammonia solution at 210°C for 3 h facilitates structural transformation from orthorhombic NTA to N-doped TiO2. Heat treatment of the same precursor at lowered temperature of 130°C and 160°C gives rise to intermediate NAT deserving further research, a potential precursor for fabricating novel N-doped TiO2. As-prepared N-NTA-210 possesses better photocatalytic performance than Degussa P25 for the degradation of MB and 4-CP under visible light irradiation, which is attributed to the formation of a large number of SETOV on the surface of N-doped TiO2 and the occupation of interstitial sites in the crystal lattice of TiO2 by dopant N as Ti–O–N.

Acknowledgments

The authors thank the National Natural Science Foundation of China (no. 20973054) for financial support.

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