research papers\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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RADIATION
ISSN: 1600-5775

In situ X-ray absorption spectroscopic studies of TiO2 photocatalytic active sites for degradation of trace CHCl3 in drinking water

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aDepartment of Environmental Engineering, National Cheng Kung University, Tainan, 70101, Taiwan, and bDepartment of Safety, Health and Environmental Engineering, National United University, Miaoli 36063, Taiwan
*Correspondence e-mail: wanghp@ncku.edu.tw

Edited by R. W. Strange, University of Essex, United Kingdom (Received 8 May 2021; accepted 29 August 2021; online 21 October 2021)

Toxic disinfection byproducts such as trihalo­methanes (e.g. CHCl3) are often found after chlorination of drinking water. It has been found that photocatalytic degradation of trace CHCl3 in drinking water generally lacks an expected relationship with the crystalline phase, band-gap energy or the particle sizes of the TiO2-based photocatalysts used such as nano TiO2 on SBA-15 (Santa Barbara amorphous-15), TiO2 clusters (TiO2–SiO2) and atomic dispersed Ti [Ti-MCM-41 (Mobil Composition of Matter)]. To engineer capable TiO2 photocatalysts, a better understanding of their photoactive sites is of great importance and interest. Using in situ X-ray absorption near-edge structure (XANES) spectroscopy, the A1 (4969 eV), A2 (4971 eV) and A3 (4972 eV) sites in TiO2 can be distinguished as four-, five- and six- coordinated Ti species, respectively. Notably, the A2 Ti sites that are the main photocatalytic species of TiO2 are shown to be accountable for about 95% of the photocatalytic degradation of trace CHCl3 in drinking water (7.2 p.p.m. CHCl3 gTiO2−1 h−1). This work reveals that the A2 Ti species of a TiO2-based photocatalyst are mainly responsible for the photocatalytic reactivity, especially in photocatalytic degradation of CHCl3 in drinking water.

1. Introduction

In order to decrease the risk of water-borne diseases, chlorine is used in the disinfection of drinking water. However, toxic disinfection byproducts (DBPs) such as trihalo­methanes (THMs) are frequently formed in the drinking water chlorination processes. The US National Cancer Institute has suggested that chloro­form (one of the THMs) is carcinogenic in rodents (Boorman, 1999[Boorman, G. A. (1999). Environ. Health Perspect. 107 (Suppl. 1), 207-217.]). Lin & Hoang (2000[Lin, T. F. & Hoang, S. W. (2000). Sci. Total Environ. 246, 41-49.]) found that the level of THM carcinogen exposure could be as high as 47 µg day−1 by drinking or 30 µg day−1 by inhalation. Conventional methods for reduction of DBPs and precursors include chemical coagulation, activated carbon adsorption, membrane separation, ozonation and combined ozonation/bio-treatments (Pan et al., 2016[Pan, Y., Li, H., Zhang, X. & Li, A. (2016). Trends Environ. Anal. Chem. 12, 23-30.]; Sillanpää et al., 2018[Sillanpää, M., Ncibi, M. C. & Matilainen, A. J. (2018). J. Environ. Manage. 208, 56-76.]; Cai et al., 2018[Cai, Z., Dwivedi, A. D., Lee, W.., Zhao, X., Liu, W., Sillanpää, M., Zhao, D., Huang, C. & Fu, J. (2018). Environ. Sci.: Nano, 5, 27-47.]; Abou-Gamra & Ahmed, 2015[Abou-Gamra, Z. M. & Ahmed, M. A. (2015). Adv. Chem. Eng. Sci. 05, 373-388.]). Membrane separation and ozonation also are highly efficienct in the reduction of biologically unstable materials. However, those methods may not be economically attractive in engineering applications (Sillanpää et al., 2018[Sillanpää, M., Ncibi, M. C. & Matilainen, A. J. (2018). J. Environ. Manage. 208, 56-76.]; Cai et al., 2018[Cai, Z., Dwivedi, A. D., Lee, W.., Zhao, X., Liu, W., Sillanpää, M., Zhao, D., Huang, C. & Fu, J. (2018). Environ. Sci.: Nano, 5, 27-47.]).

TiO2, which possesses unique characteristics such as high photostability, effective band gap and easy availability, has been widely applied in the photocatalytic degradation of toxic organics, splitting of H2O, reduction of NO to N2, and dye-sensitized solar cells (Guo et al., 2018[Guo, J., Liang, J., Yuan, X., Jiang, L., Zeng, G., Yu, H. & Zhang, J. (2018). Chem. Eng. J. 352, 782-802.]; Kang & Wang, 2013[Kang, H. Y. & Wang, H. P. (2013). Environ. Sci. Technol. 47, 7380-7387.]; Yang et al., 2014[Yang, T. C., Chang, F. C., Wang, H. P., Wei, Y. L. & Jou, C. J. (2014). Mar. Pollut. Bull. 85, 696-699.]; Xie et al., 2017[Xie, M. Y., Su, K. Y., Peng, X. Y., Wu, R. J., Chavali, M. & Chang, W. C. (2017). J. Taiwan Inst. Chem. Eng. 70, 161-167.]; Liao et al., 2014[Liao, C. Y., Wang, S. T., Chang, F. C., Wang, H. P. & Lin, H. P. (2014). J. Phys. Chem. Solids, 75, 38-41.]). The photocatalytic activities of TiO2 can be enhanced with dispersed transition metal promoters such as V, Cr, Fe, Cu, Ni, Mn, Ag or Au (Yang et al., 2017[Yang, C., Dong, W., Cui, G., Zhao, Y., Shi, X., Xia, X., Tang, B. & Wang, W. (2017). Electrochim. Acta, 247, 486-495.]; Wang et al., 2017[Wang, Z., Peng, X., Huang, C., Chen, X., Dai, W. & Fu, X. (2017). Appl. Catal. Environ. 219, 379-390.]; Lin et al., 2017[Lin, L., Wang, K., Yang, K., Chen, X., Fu, X. & Dai, W. (2017). Appl. Catal. Environ. 204, 440-455.]; Muñoz-Batista et al., 2014[Muñoz-Batista, M. J., Kubacka, A. & Fernández-García, M. (2014). ACS Catal. 4, 4277-4288.]). Nano TiO2 has been considered a desirable photocatalyst due to its large surface-to-volume ratios (Xu et al., 2019[Xu, C., Ravi Anusuyadevi, P., Aymonier, C., Luque, R. & Marre, S. (2019). Chem. Soc. Rev. 48, 3868-3902.]; Chen et al., 2019[Chen, F., Huang, H., Guo, L., Zhang, Y. & Ma, T. (2019). Angew. Chem. Int. Ed. 58, 10061-10073.]).

Valence and local structure (<1 nm) of select elements in a complicated solid matrix can be studied by synchrotron X-ray absorption spectroscopy. Molecular structure information such as the coordination number (CN), bond distance and oxidation state of elements can be determined by X-ray absorption [extended X-ray absorption fine structure (EXAFS) and X-ray absorption near-edge structure (XANES)] spectroscopy. Using XANES and EXAFS, it was found that copper oxide clusters in the channels of mesopores (2–6.5 nm) [MCM-41 (Mobil Composition of Matter-41)], micropores (0.54–0.56 nm) [e.g. ZSM-5 (Zeolite Socony Mobil-5) and ZSM-48] and TiO2-based photocatalysts were very effective in catalysis (Hsiung et al., 2006a[Hsiung, T. L., Wang, H. P., Lu, Y. M. & Hsiao, M. C. (2006a). Radiat. Phys. Chem. 75, 2054-2057.], 2021[Hsiung, T.-L., Wei, L.-W., Huang, H.-L., Tuan, Y.-J. & Wang, H. P. (2021). J. Synchrotron Rad. 28, 849-853.]; Chien et al., 2001[Chien, Y. C., Wang, H. P. & Yang, Y. W. (2001). Environ. Sci. Technol. 35, 3259-3262.]; Huang et al., 2003[Huang, Y. J., Wang, H. P. & Lee, J. F. (2003). Appl. Catal. Environ. 40, 111-118.]). These molecular-scale data turn out to be very useful in revealing the nature of catalytic active species and the reaction paths involved.

Photocatalytic degradation of trace THMs or DBPs by nano TiO2 was shown to be not very effective (Diaz-Angulo et al., 2019[Diaz-Angulo, J., Gomez-Bonilla, I., Jimenez-Tohapanta, C., Mueses, M., Pinzon, M. & Machuca-Martinez, F. (2019). Photochem. Photobiol. Sci. 18, 897-904.]; El-Mragui et al., 2019[El Mragui, A., Zegaoui, O. & Daou, I. (2019). Mater. Today Proc. 13, 857-865.]). On the other hand, photocatalytic generation of H2 (from H2O) on atomic dispersed Ti and Zr in the mesoporous molecular sieve (MCM-41) (Ti-MCM-41 and Zr-MCM-41) can be enhanced by 17 and 80 times, respectively (if compared with the bulk states) (Liu et al., 2003[Liu, S. H., Huang, Y. J., Lin, K. S. & Hsiao, M. C. (2003). Energy Sources, 25, 591-596.]). It seems that nano, cluster (<4 nm in diameter) or even atomic dispersed TiO2 may lead to unique enhancements in photocatalytic reactions. However, speciation of photocatalytic active sites in TiO2 has not been well studied particularly during reactions (Hsiung et al., 2006b, 2008[Hsiung, T. L., Wang, H. P. & Lin, S. & H. P. (2008). J. Phys. Chem. Solids, 69, 383-385. .][Hsiung, T. L., Wang, H. P. & Wang, H. C. (2006b). Radiat. Phys. Chem. 75, 2042-2045.]). In order to prepare effective TiO2 photocatalysts, a molecular-scale understanding of their photoactive sites is essential. Thus, the main objective of the present work was to study the chemical structure of Ti species with different TiO2 sizes (i.e. nano, cluster and atomic dispersion) in relation to the photocatalytic degradation of trace CHCl3 in drinking water by in situ XANES and EXAFS.

2. Experimental

The nano TiO2–SiO2 (Ti/Si atomic ratio = 3/7) photocatalyst was prepared by the sol-gel method (Beck et al., 2001[Beck, C., Mallat, T., Bürgi, T. & Baiker, A. (2001). J. Catal. 204, 428-439.]). Typically, 12.8 g of titanium (IV) n-butoxide (Acros, 99%) and 24.3 g of tetra­ethyl­orthosilicate (C8H20OSi, TEOS) (Merck) were well mixed (at the pH value of 7.0) in an ethanol and distilled water (1:2) solution (45 ml). The TiO2–SiO2 solution was heated slowly until the sol-gel became xerogel, and then separated and calcined at 673 K for 1 h. The nano TiO2 photocatalysts were synthesized using a similar procedure.

The TiO2 supported on SBA-15 (Santa Barbara amorphous-15), that has a 2D hexagonal mesoporous structure with long straight channels parallel to the silica skeletons, photocatalysts were prepared by co-condensation of silica, titanium oxide and neutral-charge poly(ethyl­ene oxide)-poly(propyl­ene oxide)-poly(ethyl­ene oxide) [EO20PO70EO20 (P123)] (Aldrich, 99%) nonionic surfactant. Briefly, 0.21 g of titanium n-butoxide [Ti(OBu)4, Aldrich, 97%] and 15 g of sulfuric acid (1.2 M, Merck) were well mixed until the solution became clear; a solution containing 2.75 g of sodium silica [14% NaOH and 27% SiO2 (Aldrich)], 1.25 g of P123 (Aldrich, 99%) and 200 g of distilled water was added. The pH value of the solution was adjusted to 5.0. After separation, the photocatalyst was calcined at 773 K for 6 h.

The Ti-inserted (framework) MCM-41 (Ti-MCM-41) photocatalysts were synthesized by the liquid crystal templating method. Fumed silica (Sigma) and sodium silicate solution were used as silica sources for the preparation of MCM-41. Hexa­decyl­tri­methyl ammonium bromide (CTAB) (Sigma, purity >99%) and tetra­methyl ammonium hydroxide [TMAOH, 25% (Sigma–Aldrich)] were used as a template and mineralizer, respectively. The mole ratio of H2O, CTAB, TMAOH and Si in the mixture was 86:0.27:0.58:1. Titanium n-butoxide (Acros, 99%) was added to the MCM-41 mother liquid for the synthesis of Ti-MCM-41. A diluted sulfuric acid solution was used to adjust the pH values of the solution to between 11 and 12. The mixture was then heated in a Teflon-lined autoclave at 375 K for 24 h. The as-synthesized MCM-41 was filtered, washed with distilled water, dried and calcined at 773 K for 5 h.

The chemical structure of the photocatalysts was characterized by X-ray powder diffraction (XRD) spectroscopy (D8 Advance, Bruker) with Cu Kα (1.542 Å) radiation. Samples were scanned from 10 to 50° (2θ) at a scan rate of 5° min−1. Diffuse reflectance ultraviolet/visible spectra (DR UV–vis) of the photocatalysts were also determined (between 200 and 700 nm) on a UV–vis spectrophotometer (Hitachi U-3010) at a scan speed of 120 nm min−1.

The in situ Ti K-edge (4966 eV) XANES spectra of the photocatalysts were collected at 298 K on the wiggler beamline of the Taiwan National Synchrotron Radiation Research Center. The absorption spectra were collected in ion chambers that were filled with helium and nitro­gen mixed gases. The beam energy was calibrated to the adsorption edge of a Ti foil at the energy of 4966 eV. The electron storage ring was operated at an energy of 1.5 GeV (ring current = 120–200 A). The isolated EXAFS data were normalized to the edge jump and converted to the wavenumber scale. Fitting of data to model compounds was performed using FEFFIT (UWXAFS 3.0) in combination with the multiple scattering code FEFF 8.0 simulation programs (Chiu et al., 2011[Chiu, Y. M., Huang, C. H., Chang, F. C., Kang, H. Y. & Wang, H. P. (2011). Sustain. Environ. Res. 21, 279-282.]). FEFFIT was used to determine the best-fitting results with the minimum Debye–Waller factors (<0.01 Å2). The Fourier transform was performed on k3-weighted EXAFS oscillations in the range 3.8–11.7 Å−1.

Photocatalytic degradation of CHCl3 (500 p.p.b.) was performed on a homemade in situ EXAFS cell (Kang & Wang, 2013[Kang, H. Y. & Wang, H. P. (2013). Environ. Sci. Technol. 47, 7380-7387.]). Typically, 0.15 g of the TiO2 photocatalyst was suspended in H2O containing trace CHCl3 (500 p.p.b.). A 300 W high-pressure Xe arc lamp (Newport, model 6258) was used as the light source (250–800 nm) while the synchrotron X-ray absorption spectra of the TiO2 photocatalysts were determined. Concentrations of CHCl3 were determined using a gas chromatograph (model 3400, Varian) equipped with an electrolytic conductivity detector (model 100, Tracor) and a purge/trap system (model LCS-2000, Tekmar).

3. Results and discussion

The XRD patterns of the TiO2-based photocatalysts are shown in Fig. 1[link]. The Ti-MCM-41 and TiO2–SiO2 photocatalysts have broadened peaks between 17 and 31° (2θ), suggesting the absence of crystalline TiO2, which may be associated with the existence of very small TiO2 nanoparticles or highly atomic dispersed Ti therein. For the TiO2/SBA-15 and nano TiO2, anatase phases [(101), (004) and (200)] are observed with crystalline sizes of about 4.6 and 8.5 nm, respectively (calculated using the Scherrer equation).

[Figure 1]
Figure 1
XRD patterns of (a) Ti-MCM-41, (b) TiO2–SiO2, (c) TiO2/SBA-15 and (d) nano TiO2.

Fig. 2[link] shows the DR UV–vis spectra of the photocatalysts. The band-gap energies for the TiO2–SiO2 and Ti-MCM-41 are 3.38 and 3.42 eV, respectively. Beck et al. (2001[Beck, C., Mallat, T., Bürgi, T. & Baiker, A. (2001). J. Catal. 204, 428-439.]) also found blue shifts for the band-gap absorption edge with highly dispersed Ti in the SiO2 framework. The absorption feature (<260 nm) for the Ti-MCM-41 can be attributed to the ligand-to-metal charge transfer between TiIV and the amorphous SiO2 framework. It seems that Ti is well dispersed in the Ti-MCM-41 photocatalyst.

[Figure 2]
Figure 2
DR UV–vis spectra of (a) Ti-MCM-41, (b) TiO2–SiO2, (c) nano TiO2 and (d) TiO2/SBA-15.

The EXAFS spectra best-fitted by the Fourier transformation and k3-weighted for the TiO2-based photocatalysts in the ranges 0–4 and 4–11 Å, respectively, are shown in Fig. 3[link]. The speciation parameters for the Ti in those photocatalysts are also listed in Table 1[link]. The bond distances for the Ti—(O)—Si species (in the second shells) in the Ti-MCM-41 and TiO2–SiO2 photocatalysts are 3.13 and 3.31 Å, respectively. It is worth noting that the Ti-MCM-41 has a greater CN for the Ti—(O)—Si bonding than does the TiO2–SiO2, demonstrating that more Ti atoms are dispersed in the amorphous SiO2 framework for the Ti-MCM-41, and that the TiO2–SiO2 one has more TiO2 aggregates on the SiO2 surfaces with a metal–support interaction related to its relatively low CN. It seems that the TiO2–SiO2 contains sub-nano TiO2 (supported on the SiO2) that is not observed by XRD, which may behave like a TiO2 cluster. The Ti—O—Si species are, in contrast, not found in the TiO2/SBA-15. It seems that the TiO2 nanoparticles may be formed in the hexagonally ordered mesoporous channels (an opening of 5.7 nm) of the SBA-15. Note that the averaged diameter of the TiO2 nanoparticles in the SBA-15 is approximately 4.6 nm (see Table 2[link]).

Table 1
Speciation parameters of titanium in the photocatalysts for degradation of trace CHCl3 in drinking water

  Shell Bond distance (Å) Coordination number Debye–Waller factor (Å2)
Ti-MCM-41 Ti—Oeq 1.75 0.9 0.0058
Ti—Oax 1.99 2.6 0.0029
Ti—(O)—Si 3.13 2.9 0.0103
TiO2–SiO2 Ti—Oeq 1.77 1.9 0.0023
Ti—Oax 2.32 2.5 0.0030
Ti—(O)—Si 3.31 1.1 0.0027
Nano TiO2 Ti—Oeq 1.92 1.5 0.0004
Ti—Oax 2.03 3.1 0.0045
Ti—(O)—Ti 3.03 3.5 0.0049
TiO2/SBA-15 Ti—Oeq 1.90 2.0 0.0038
Ti—Oax 1.99 3.3 0.0044
Ti—(O)—Ti 3.03 2.1 0.0043

Table 2
Characterization and reactivity of the photocatalysts for degradation of trace CHCl3 in drinking water

TiO2 chemical structure was determined by XRD. Crystalline size was calculated using the Scherrer equation. Band-gap absorption edge was determined by DR UV–vis. Photocatalytic degradation of CHCl3 was determined in a total UV–vis reflectance system under UV–vis irradiation for 4 h [initial CHCl3 concentration = 500 p.p.b. (in H2O)]. Ti species were determined by XANES [A1: TiO4; A2: (Ti=O)O4; A3: TiO6]. Fractions of the Ti species (i.e. A1, A2 and A3) related to the photocatalytic degradation of CHCl3 determined by the linear regression analysis are well fitted for A2 (R2 > 0.9) while the R2 values for A1 and A3 are 0.37 and 0.64, respectively.

Photocatalyst TiO2 chemical structure Crystalline size (nm) Band-gap absorption edge (eV) Photocatalytic degradation of CHCl3 (p.p.m. gTiO2−1 h−1) Ti species (%)
A1 A2 A3
Ti-MCM-41 Amorphous 3.42 7.2 7 49 44
TiO2–SiO2 Amorphous 3.38 0.9 25 33 42
Nano TiO2 Anatase 8.5 3.25 0.7 22 32 46
TiO2/SBA-15 Anatase 4.6 3.30 5.6 19 40 41
[Figure 3]
Figure 3
Ti K-edge XANES spectra of (a) TiO2–SiO2, (b) nano TiO2, (c) TiO2/SBA-15 and (d) Ti-MCM-41.

Photocatalytic degradation of trace CHCl3 (500 p.p.b. in drinking water) by the nano, cluster and atomic dispersed TiO2 photocatalysts under UV–vis radiation (250–800 nm) is shown in Fig. 4[link]. An enhanced photocatalytic degradation of trace CHCl3 by the Ti-MCM-41 is observed. After a 4 h UV–vis radiation, accumulated 28.8 p.p.m. CHCl3 gTiO2−1 are photocatalytically degraded by Ti-MCM-41. The nano TiO2 shows relatively low activity for photocatalytic degradation of CHCl3 when compared with the Ti-MCM-41. Note that the TiO2–SiO2 containing TiO2 clusters also shows much less activity for the photocatalytic degradation than the TiO2/SBA-15 that has larger TiO2 nanoparticles (an average size of 4.6 nm). It appears that the reactivity with respect to photocatalytic degradation of trace CHCl3 in drinking water may not be related to the crystalline phase, band-gap absorption edge or particle size of the TiO2-based photocatalysts.

[Figure 4]
Figure 4
Time dependence for photocatalytic degradation of trace CHCl3 in H2O effected by (a) Ti-MCM-41, (b) TiO2/SBA-15, (c) TiO2–SiO2 and (d) nano TiO2.

To reveal the key factor that influences the photocatalytic degradation reactivity of the TiO2-based photocatalysts, Table 2[link] summarizes the characterization of the TiO2-based photocatalysts, the related photocatalytic degradation reactivity and the photoactive sites involved. It seems that the photocatalysts, i.e. Ti-MCM-41 and TiO2/SBA-15, possessing meso-pore channel systems have greater photocatalytic degradation conversions than the other ones that have nano and cluster TiO2 on SiO2. Apparently, the mesopores in the MCM-41 and SBA-15 have a large enough pore opening for free diffusion of small CHCl3 molecules to the TiO2 photoactive sites. Thus, there may exist other factors such as different loadings of TiO2 and hardness or toxic ions in real drinking water that may also disturb the photocatalysis.

In Fig. 5[link], A1 (4969 eV), A2 (4971 eV) and A3 (4972 eV) sites can be resolved in the pre-edge XANES spectra [between the absorption threshold (4966 eV) and jump (4984 eV)] of the photocatalysts. The A1, A2 and A3 species in TiO2 may be attributed to four- (TiO4), five- [(Ti=O)O4] and six- (TiO6) coordinated Ti species, respectively (Hsiung et al., 2006a[Hsiung, T. L., Wang, H. P., Lu, Y. M. & Hsiao, M. C. (2006a). Radiat. Phys. Chem. 75, 2054-2057.], 2008[Hsiung, T. L., Wang, H. P. & Lin, S. & H. P. (2008). J. Phys. Chem. Solids, 69, 383-385. .]). The B and C features (at 4974 and 4980 eV, respectively) are due to the interactions of the central Ti 4p orbitals hybridized with the near Ti or O atoms. The Ti K post-edge at 4980–5020 eV can be assigned to 3s-to-np dipole-allowed transitions. The insertion of Ti atoms into the SiO2 matrix may cause distortion of the Ti–O octahedron structure. It is worth noting that the broadened white line absorption (4987 eV) for Ti-MCM-41 and TiO2–SiO2 is observed, suggesting the existence of highly dispersed Ti atoms in the SiO2 matrix.

[Figure 5]
Figure 5
Ti K-edge XANES spectra of (a) TiO2–SiO2, (b) nano TiO2, (c) TiO2/SBA-15 and (d) Ti-MCM-41.

The Ti species (A1, A2 and A3) in the photocatalysts were distinguished (in the XANES spectra). As shown in Table 2[link], the well dispersed Ti in Ti-MCM-41 has a much better performance for photocatalytic degradation of trace CHCl3 in drinking water. The A2 Ti species (fivefold-coordinated TiIV) possesses a square-pyramid structure, consisting of a double bond (Ti=O) and four Ti—O bonds, which is predominant generally on the surfaces of the very small (<10 nm) TiO2 nanoparticles. Fractions of the Ti active species related to the photocatalytic degradation of CHCl3 determined by the linear regression analysis are well fitted (R2 > 0.9) while the R2 values for A1 and A3 are 0.37 and 0.64, respectively. The A2 Ti species make a major contribution (75% approximately) to the photocatalytic degradation of trace CHCl3 in H2O. Note that about 95% of the photocatalytic conversion (7.2 p.p.m. CHCl3 gTiO2−1 h−1) is associated with the A2 Ti active species in Ti-MCM-41.

4. Conclusions

The A1 (TiO4), A2 [(Ti=O)O4] and A3 (TiO6) Ti species in TiO2 were observed and distinguished by component fitted pre-edge XANES spectra of the nano TiO2 (TiO2/SBA-15), TiO2 cluster (TiO2-SiO2) and highly atomic dispersed Ti (Ti-MCM-41) photocatalysts. It appears that the photocatalytic degradation of trace CHCl3 in drinking water may not be related to the crystalline phase, band-gap absorption edge or the particle size of the TiO2-based photocatalysts. Nevertheless, the A2 Ti species in the TiO2-based photocatalysts may make a major contribution (75% approximately) to the overall photocatalytic performance. In the photocatalytic degradation of trace CHCl3, for example, the higher A2 Ti species in the atomic dispersed Ti (Ti-MCM-41) may account for 95% of the accumulated photocatalytic conversion. This work reveals that the A2 Ti species of a TiO2-based photocatalyst are associated significantly with its photocatalytic reactivity, especially in photocatalytic degradation of CHCl3.

Acknowledgements

We thank Y. W. Yang and Jyh-Fu Lee of the NSRRC for their assistance with X-ray absorption experiments.

Funding information

The financial support of the Taiwan Ministry of Science and Technology, Bureau of Energy, and National Synchrotron Radiation Research Center (NSRRC) are gratefully acknowledged.

References

First citationAbou-Gamra, Z. M. & Ahmed, M. A. (2015). Adv. Chem. Eng. Sci. 05, 373–388.  CAS Google Scholar
First citationBeck, C., Mallat, T., Bürgi, T. & Baiker, A. (2001). J. Catal. 204, 428–439.  CrossRef CAS Google Scholar
First citationBoorman, G. A. (1999). Environ. Health Perspect. 107 (Suppl. 1), 207–217.  Google Scholar
First citationCai, Z., Dwivedi, A. D., Lee, W.., Zhao, X., Liu, W., Sillanpää, M., Zhao, D., Huang, C. & Fu, J. (2018). Environ. Sci.: Nano, 5, 27–47.  CrossRef CAS Google Scholar
First citationChen, F., Huang, H., Guo, L., Zhang, Y. & Ma, T. (2019). Angew. Chem. Int. Ed. 58, 10061–10073.  CrossRef CAS Google Scholar
First citationChien, Y. C., Wang, H. P. & Yang, Y. W. (2001). Environ. Sci. Technol. 35, 3259–3262.  CrossRef PubMed CAS Google Scholar
First citationChiu, Y. M., Huang, C. H., Chang, F. C., Kang, H. Y. & Wang, H. P. (2011). Sustain. Environ. Res. 21, 279–282.  CAS Google Scholar
First citationDiaz-Angulo, J., Gomez-Bonilla, I., Jimenez-Tohapanta, C., Mueses, M., Pinzon, M. & Machuca-Martinez, F. (2019). Photochem. Photobiol. Sci. 18, 897–904.  CAS PubMed Google Scholar
First citationEl Mragui, A., Zegaoui, O. & Daou, I. (2019). Mater. Today Proc. 13, 857–865.  CrossRef CAS Google Scholar
First citationGuo, J., Liang, J., Yuan, X., Jiang, L., Zeng, G., Yu, H. & Zhang, J. (2018). Chem. Eng. J. 352, 782–802.  CrossRef CAS Google Scholar
First citationHsiung, T. L., Wang, H. P. & Lin, S. & H. P. (2008). J. Phys. Chem. Solids, 69, 383–385. .  Google Scholar
First citationHsiung, T. L., Wang, H. P., Lu, Y. M. & Hsiao, M. C. (2006a). Radiat. Phys. Chem. 75, 2054–2057.  CAS Google Scholar
First citationHsiung, T. L., Wang, H. P. & Wang, H. C. (2006b). Radiat. Phys. Chem. 75, 2042–2045.  CAS Google Scholar
First citationHsiung, T.-L., Wei, L.-W., Huang, H.-L., Tuan, Y.-J. & Wang, H. P. (2021). J. Synchrotron Rad. 28, 849–853.  CrossRef CAS IUCr Journals Google Scholar
First citationHuang, Y. J., Wang, H. P. & Lee, J. F. (2003). Appl. Catal. Environ. 40, 111–118.  CrossRef CAS Google Scholar
First citationKang, H. Y. & Wang, H. P. (2013). Environ. Sci. Technol. 47, 7380–7387.  Web of Science CrossRef CAS PubMed Google Scholar
First citationLiao, C. Y., Wang, S. T., Chang, F. C., Wang, H. P. & Lin, H. P. (2014). J. Phys. Chem. Solids, 75, 38–41.  CrossRef CAS Google Scholar
First citationLin, L., Wang, K., Yang, K., Chen, X., Fu, X. & Dai, W. (2017). Appl. Catal. Environ. 204, 440–455.  CrossRef CAS Google Scholar
First citationLin, T. F. & Hoang, S. W. (2000). Sci. Total Environ. 246, 41–49.  CrossRef PubMed CAS Google Scholar
First citationLiu, S. H., Huang, Y. J., Lin, K. S. & Hsiao, M. C. (2003). Energy Sources, 25, 591–596.  CrossRef CAS Google Scholar
First citationMuñoz-Batista, M. J., Kubacka, A. & Fernández-García, M. (2014). ACS Catal. 4, 4277–4288.  Google Scholar
First citationPan, Y., Li, H., Zhang, X. & Li, A. (2016). Trends Environ. Anal. Chem. 12, 23–30.  CrossRef CAS Google Scholar
First citationSillanpää, M., Ncibi, M. C. & Matilainen, A. J. (2018). J. Environ. Manage. 208, 56–76.  PubMed Google Scholar
First citationWang, Z., Peng, X., Huang, C., Chen, X., Dai, W. & Fu, X. (2017). Appl. Catal. Environ. 219, 379–390.  CrossRef CAS Google Scholar
First citationXie, M. Y., Su, K. Y., Peng, X. Y., Wu, R. J., Chavali, M. & Chang, W. C. (2017). J. Taiwan Inst. Chem. Eng. 70, 161–167.  CrossRef CAS Google Scholar
First citationXu, C., Ravi Anusuyadevi, P., Aymonier, C., Luque, R. & Marre, S. (2019). Chem. Soc. Rev. 48, 3868–3902.  CrossRef CAS PubMed Google Scholar
First citationYang, C., Dong, W., Cui, G., Zhao, Y., Shi, X., Xia, X., Tang, B. & Wang, W. (2017). Electrochim. Acta, 247, 486–495.  CrossRef CAS Google Scholar
First citationYang, T. C., Chang, F. C., Wang, H. P., Wei, Y. L. & Jou, C. J. (2014). Mar. Pollut. Bull. 85, 696–699.  CrossRef CAS PubMed Google Scholar

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