Journal of Colloid and Interface Science 316 (2007) 85–91 www.elsevier.com/locate/jcis Synthesis and photocatalytic activity of mesoporous TiO2 with the surface area, crystallite size, and pore size Dong Suk Kim, Shin Jung Han, Seung-Yeop Kwak ∗ Department of Materials Science and Engineering, Seoul National University, San 56-1, Sillim-dong, Gwanak-gu, Seoul 151-744, South Korea Received 8 March 2007; accepted 20 July 2007 Available online 29 August 2007 Abstract Mesoporous TiO2 materials with various pore-size distributions were synthesized by using diblock copolymers via a sol–gel process in aqueous solution. The properties of these materials were characterized by FE-SEM, HR-TEM, XRD, DRS, BET, and BJH analysis. All particles have spherical morphology with a diameter range of 1–3 µm. The mesoporous TiO2 materials calcined at 400 ◦ C were found to have different specific surface areas—186, 210, and 192 m2 g−1 —and average pore sizes depending on the type of diblock copolymer—5.1, 6.1, and 6.4 nm—and their crystallite sizes were found to be 8.1, 8.3, and 8.8 nm. The photocatalytic activity of each sample was investigated by measuring the photodecomposition of methylene blue (MB), and the small crystallite size, large surface area, and small pore size were found to exhibit better photocatalytic activities. In addition, the photocatalytic activities of all the mesoporous TiO2 materials were found to be better than that of commercial TiO2 . © 2007 Elsevier Inc. All rights reserved. Keywords: Mesoporous TiO2 ; Photocatalytic activity; Calcination temperature; Pore size; Porous structure 1. Introduction Titanium dioxide (TiO2 ) is a very useful semiconducting transition metal oxide material and exhibits unique characteristics such as low cost, easy handling, nontoxicity, and resistance to photochemical and chemical erosion. These advantages make TiO2 a material in solar cell, chemical sensor, hydrogen gas evolution, and environmental purification applications [1–3]. The photocatalytic activity of TiO2 is one of its most distinctive features, and is largely determined by properties such as the crystalline phase, crystallite size, specific surface area, and porous structure. Some studies of the effects of these properties on the photocatalytic activity of TiO2 photocatalysts have been conducted [4]. High photocatalytic activity is associated with crystallite sizes because small crystallite size can lead to quantum size effects in semiconductors. In addition, TiO2 with a large surface area and a porous structure is expected to exhibit outstanding photodegradation properties [5–7], be* Corresponding author. E-mail address: [email protected] (S.-Y. Kwak). 0021-9797/$ – see front matter © 2007 Elsevier Inc. All rights reserved. doi:10.1016/j.jcis.2007.07.037 cause TiO2 with a large surface area has many active sites so that substances can be adsorbed in large quantities onto the TiO2 surface, and porosity facilitates pollutant access, adsorption, and decomposition [8–11]. Peng et al. recently prepared mesoporous TiO2 nanosized powders with high specific surface areas and anatase walls by using cetyltrimethylammonium bromide (CTAB) as a surfactant-directing and pore-forming agent. In their study, it was found that the high photocatalytic activity of the resulting material was related to its large surface area and small anatase crystallites [12]. Zhan et al. fabricated long TiO2 hollow fibers with mesoporous walls and large surface areas by combining a sol–gel process with a two-capillary spinneret electrospinning technique using a triblock copolymer (Pluronic, P123) as a pore-directing agent, and compared the photocatalytic activities of the fibers with those of Degussa P25 and mesoporous TiO2 powders [13]. Jimmy et al. synthesized three-dimensional and thermally stable mesoporous TiO2 without the use of any surfactants via treatment with high intensity ultrasound irradiation, and its high photocatalytic activity was attributed to its high surface area and the three-dimensional connectivity of its mesoporous wormhole frameworks [14]. However, few precise 86 D.S. Kim et al. / Journal of Colloid and Interface Science 316 (2007) 85–91 investigations of the effect of pore-size distribution and porous structure of mesoporous TiO2 on the photocatalytic activity have previously been carried out. In this paper, we report the preparation and characterization of mesoporous TiO2 materials with various pore sizes synthesized by using surfactants with ethylene oxide groups of various lengths, and focus on the effects of the calcination temperature, porous structure, and pore size on their photocatalytic activity. The mesoporous TiO2 materials are synthesized in aqueous solution with a sol–gel process from various diblock copolymers as templates and titanium tetraisopropoxide mixed with 2,4-pentanedione, which is a retarding agent that limits the rate of hydrolysis and condensation. The resulting materials have a spherical morphology with various pore sizes, and exhibit high thermal stabilities up to 600 ◦ C maintaining mesoporous structures. They show better photocatalytic activities compared to commercial TiO2 , Ishihara ST-01. radiation) at room temperature. An accelerating voltage of 50 kV and an emission current of 100 mA were used. The crystallite sizes were calculated with the Scherrer equation (Φ = Kλ/β cos θ ), where Φ is the crystallite size, K is usually taken as 0.89, λ is 0.154 nm, which is the wavelength of the X-ray radiation, β is the full width at half-maximum intensity (FWHM), and θ is the diffraction angle of the (101) peak for anatase (2θ = 25.3◦ ). Nitrogen adsorption–desorption isotherms were collected at 77 K on a Micrometrics ASAP 2000 apparatus after the samples were degassed at 100 ◦ C for 10 h. The specific surface areas were estimated by using the Brunauer–Emmett–Teller (BET) method, and the pore-size distributions were determined with the Barrett–Joyner–Halenda (BJH) method by using the nitrogen desorption branches of the isotherms. Ultraviolet/visible diffuse reflectance spectra (DRS) of the samples were obtained by using a UV–Vis spectrophotometer (Varian Cary5000) with BaSO4 as the reference. 2. Experimental 2.3. Photocatalytic activity 2.1. Preparation of mesoporous TiO2 samples Titanium tetraisopropoxide (Ti(Oi Pr)4 , 97%, Aldrich) and the diblock copolymer surfactants (Lutensol AT 18, Lutensol AT 25, Lutensol AT 50, BASF) were used without further purification. The diblock copolymers (RO(CH2 CH2 O)x H) consist of 16 or 18 carbon units in hydrophobic alkyl groups, where x is the number of ethylene oxide units, for example, x = 18 for Lutensol AT 18. To optimize the synthetic conditions, many parameters including the surfactant concentration, sulfuric acid concentration, Ti precursor to surfactant ratio, and reaction temperature were controlled. First, 3 g of each surfactant (Lutensol AT 18, 2.9 mmol; Lutensol AT 25, 2.2 mmol; Lutensol AT 50, 1.2 mmol) was dissolved in 100 ml of distilled water, and then 1.5 g (15.3 mmol) of sulfuric acid was added. Next, titanium tetraisopropoxide (AT-18, 28.6 mmol; AT-25, 27.7 mmol; AT-50, 27.5 mmol) mixed with 2,4-pentanedione (AT-18, 28.6 mmol, AT-25, 27.7 mmol, AT-50, 27.5 mmol) was dropped into each surfactant solution under magnetic stirring. The resulting solutions were kept at 50 ◦ C. Light yellow powders formed within several minutes, and then hydrothermal treatment was carried out at 90 ◦ C for about 10 h. The solids in the solutions were filtered out, dried in air, and ground to fine powders. The resulting materials are denoted MT-18, MT-25, and MT-50, according to the number of ethylene oxide units in the surfactants. Finally, the materials were calcined at 400, 500, and 600 ◦ C at a rate of 1 ◦ C min−1 in air. 2.2. Characterization The morphologies and pore structures of the mesoporous TiO2 particles were determined from using field emission-gun scanning electron microscope (FE-SEM, JEOL JSM-6330F) and transmission electron microscope (TEM, JEOL JEM2000EXII). The crystal compositions and crystallite sizes of each sample were determined by using wide-angle X-ray diffraction (XRD, MAC/Sci. MXP 18XHF-22SRA with CuKα The photocatalytic activities of the mesoporous TiO2 samples were evaluated by measuring the decomposition rate of methylene blue (MB) at room temperature, and compared with the activity of commercial TiO2 , Ishihara ST-01. A quartz cell containing both aqueous MB solution and TiO2 powder was placed in the center of the reactor, with four UV lamps located at each corner inside the reactor. Each quartz cell contained 25 ml of the aqueous MB solution with 50 ppm dye and 25 mg of the catalyst. In order to provide sufficient UV radiation, four UV lamps providing UV-A (320 < λ < 400 nm) were used as light sources. In each experiment, the reaction solutions were magnetically stirred in the dark for 30 min until adsorption/desorption equilibrium was reached. The solution was then irradiated under UV light with continuous magnetic stirring. A fixed quantity of each MB solution was taken at regular intervals during the illumination period and filtered through a syringe filter to analyze the amount of MB remaining in the solution. The UV–Vis absorption spectra of the taken solutions were obtained using a Shimadzu 2101PC UV–Vis scanning spectrophotometer in the range 500–700 nm, because λmax of methylene blue is approx 664 nm. 3. Results and discussion 3.1. FE-SEM and TEM analyses FE-SEM images of the mesoporous TiO2 materials (MT-18, MT-25, and MT-50) calcined at 400 ◦ C are shown in Figs. 1a, 1b, and 1c, respectively. The particles of these materials all have spherical morphologies, and increase in size with increases in the number of ethylene oxide units. The magnified FE-SEM images of the materials are shown in Figs. 1d, 1e, and 1f. It can be observed that discernible pores are present at the surface of mesoporous TiO2 material among the nanosized TiO2 particles. In order to investigate the properties of the pores, HRTEM images were obtained. The HR-TEM images of MT-18, D.S. Kim et al. / Journal of Colloid and Interface Science 316 (2007) 85–91 87 Fig. 2. HR-TEM images of (a) MT-18, (b) MT-25, and (c) MT-50 calcined at 400 ◦ C and (d) magnified image of MT-18 (the inset is the electron diffraction pattern of MT-18). Fig. 1. FE-SEM images of as-synthesized (a) MT-18, (b) MT-25, and (c) MT-50, and magnified images of mesoporous materials (d) MT-18, (e) MT-25, and (f) MT-50 calcined at 400 ◦ C. MT-25, and MT-50 calcined at 400 ◦ C are shown in Figs. 2a, 2b, and 2c, respectively. The magnified HR-TEM image and electron diffraction pattern of the material are shown Fig. 2d. The pores can be seen as black spots with nonordered wormholelike structures, and the nanosized TiO2 particles appear white. This result is consistent with the FE-SEM images. From FESEM and TEM results, it is found that the pore walls consist of aggregated TiO2 nanoparticles. 3.2. XRD analysis Figs. 3a, 3b, and 3c show XRD patterns of as-synthesized MT-18, MT-25, and MT-50, and of MT-18, MT-25, and MT-50 calcined at various temperatures in the range of 400–600 ◦ C. Relatively broad diffraction peaks due to anatase structures are present for all these materials, even for the as-synthesized materials. As the calcination temperature increases, the diffraction peak (101) due to the anatase structure becomes sharper with increases in all the samples in the crystallite size [15]. Table 1 represents crystallite sizes of as-synthesized mesoporous TiO2 and mesoporous TiO2 calcined at various temperatures. It was estimated with the Scherrer equation, and the crystallite sizes of the as-synthesized MT-18, MT-25, and MT-50 are about 6.9, 7.1, and 7.5 nm, respectively; i.e., the crystallite sizes gradually increase with increases in the calcination temperature (Table 1). Hydrothermal treatment at 90 ◦ C for 10 h is used to ensure the formation of an anatase structure before calcination [16,17]. The phase transformation from anatase to rutile does not occur in TiO2 materials during calcination at high temperatures, so only the anatase phase is present at 600 ◦ C, without any other crystalline by-products. In addition, thermodynamic phase stability is generally dependent on particle size, and the anatase structure is more stable thermodynamically than the rutile structure at particle sizes below approx 14 nm [18], which is similar to the crystal sizes of MT-18, MT-25, and MT-50 calcined at 600 ◦ C, as shown in Table 1. Thus it is possible that the three mesoporous TiO2 materials are thermally stable up to 600 ◦ C because of these effects [19]. 3.3. N2 adsorption–desorption analysis N2 adsorption–desorption isotherms of all the samples calcined at various temperatures are shown in Fig. 4. All the isotherms of the samples are of classical type IV with H2 hysteresis between the adsorption and the desorption curves, indicating the existence of ink-bottle-type pore structure with a narrow entrance and a large cavity [20,21]. For MT-18, MT-25, and MT-50 calcined at 400 ◦ C, the surface areas determined with the BET method are similar: 186, 210, and 192 m2 g−1 , respectively. When the calcination temperature is 600 ◦ C, the specific surface areas of these materials decrease to approx 90 m2 g−1 due to the crystallization of TiO2 , subsequent crystal growth, and the collapse of the mesoporous structure [12]. However, a 88 D.S. Kim et al. / Journal of Colloid and Interface Science 316 (2007) 85–91 Fig. 4. N2 adsorption–desorption isotherms of (a) MT-18, (b) MT-25, and (c) MT-50 calcined at various temperatures. Fig. 3. XRD patterns of (a) MT-18, (b) MT-25, and (c) MT-50 as-synthesized and calcined at various temperatures. large proportion of the mesopores is maintained because all the samples have isotherms with well-defined hysteresis loops up to 600 ◦ C, which indicates their thermal stability [6]. The thermal stability of mesoporous TiO2 can be achieved with hydrothermal treatment [16,17,22], which results in a higher degree of polymerization of the inorganic precursors [23] and the crys- tallization of the mesoporous wall into anatase so that there is no phase transformation during the calcination process. As the calcination temperature is increased, the hysteresis loop of a given sample shifts to the high pressure (P /P0 ) range and its slope becomes steeper. It is well known that the average pore diameter increases with increases in the TiO2 crystallite size, as confirmed by the XRD analysis, and the pore-size distribution becomes narrower with increases in the calcination temperature, indicating that the pores formed from the assembly of TiO2 nanoparticles have similar sizes [24]. Fig. 5 shows the pore-size distributions of MT-18, MT-25, and MT-50 calcined at 400 ◦ C, as estimated with the BJH method from the desorption branches. As the number of ethylene oxide units in the surfactants is increased, the average D.S. Kim et al. / Journal of Colloid and Interface Science 316 (2007) 85–91 89 Table 1 Crystallite sizes, surface areas, and pore sizes of the mesoporous TiO2 materials (MT-18, MT-25, and MT-50) calcined at various temperatures Sample MT-18 MT-25 MT-50 Surface area (m2 g−1 ) Crystallite size (nm) Pore size (nm) 400 ◦ C 500 ◦ C 600 ◦ C 400 ◦ C 500 ◦ C 600 ◦ C 400 ◦ C 500 ◦ C 8.1 8.3 8.8 10.0 11.1 16.5 15.8 16.5 17.6 186 210 192 135 145 177 95 99 96 5.1 6.1 6.4 6.0 7.1 9.7 600 ◦ C 9.2 9.7 11.7 Fig. 5. Pore-size distributions of MT-18, MT-25, and MT-50 calcined at 400 ◦ C. pore sizes of the mesoporous TiO2 materials increase: MT-18 (5.1 nm), MT-25 (6.1 nm), and MT-50 (6.4 nm). The change of pore size with increase of the ethylene oxide units may be considered as the influence of the hydrophilic ethylene oxide units of the copolymer which is dependent on the temperature [25]. At the reaction temperature of 50 ◦ C, the surfactant can form a micelle in aqueous solution, and the ethylene oxide units are expected to interact more strongly with the titanium species and thus be more closely associated with the TiO2 nanoparticles than the hydrophobic alkyl chain. However, at the higher temperature of 90 ◦ C, the ethylene oxide units become more hydrophobic, resulting in increased hydrophobic domain volumes, and increased pore sizes. As increases in the lengths of the PEO chains in the surfactants result in increases during the hydrothermal treatment in the size of the hydrophobic portions, the pore sizes of the mesoporous TiO2 vary. The results for the surface areas and pore sizes of the samples calcined at various temperatures are shown in Table 1. Fig. 6. UV–Vis diffuse reflectance spectra of (a) MT-18 calcined at various temperatures, and (b) MT-18, MT-25, and MT-50 calcined at 400 ◦ C. quantum size effects of semiconductors. In the quantum size effect, the band-gap energy decreases as the crystallite size increases [28]. 3.5. Photocatalytic activities of the mesoporous TiO2 samples 3.4. DRS analysis To investigate the absorption band shifts of TiO2 , DRS was analyzed. Fig. 6 shows DRS of MT-18 materials calcined at various temperatures and mesoporous TiO2 materials calcined at 400 ◦ C, respectively. The Kubelka-Munk formula was used for the analysis of diffuse reflectance spectra obtained from absorbing samples [26]. The absorption band shifts toward the shorter wavelength region with decreases in the crystallite sizes of the samples, which indicates an increase in the band-gap energy [4, 27]. As found in the XRD results, the crystallite sizes increase as the calcinations temperature increases. The absorption band shifts toward the longer wavelength region with the increase in the crystallite sizes of samples, which indicates a decrease in the band-gap energy. This phenomenon could be caused by the The photocatalytic activity of TiO2 is evaluated by measuring the amount of methylene blue remaining in solutions under UV illumination at regular intervals. In each experiment, prior to UV irradiation, the reaction solution was magnetically stirred in the dark for 30 min until adsorption/desorption equilibrium was reached. The MB solutions containing the mesoporous TiO2 samples were almost fully degraded and became transparent within 45 or 60 min under UV light as shown in Fig. 7. In plots of ln(C/C0 ) versus UV irradiation time, straight lines were found for all materials, indicating that the degradation of methylene blue is a first-order process. The photodecomposition rate constants are shown in Table 2. In comparison with MT-18 calcined at different temperature, MT-18 calcined at 400 ◦ C has the highest photodecomposition rate constant 90 D.S. Kim et al. / Journal of Colloid and Interface Science 316 (2007) 85–91 Fig. 7. Kinetics of the photocatalytic degradation of MB solutions containing (a) MT-18 calcined at various temperatures and (b) MT-18, MT-25, and MT-50 calcined at 400 ◦ C and Ishihara ST-01. Table 2 Photodecomposition rate constants of mesoporous TiO2 and the commercial TiO2 material, ST-01 Sample MT-18 MT-25 MT-50 ST-01 Calcination temperature (◦ C) 400 500 600 400 400 – Degradation rate (min−1 ) Degradation rate per surface area (g m−2 min−1 )a R2 0.093 0.091 0.067 0.081 0.066 0.016 0.50 × 10−3 0.99 0.99 0.98 0.99 0.98 0.99 0.67 × 10−3 0.70 × 10−3 0.38 × 10−3 0.34 × 10−3 0.06 × 10−3 we performed the photocatalytic activity of MT-18, MT-25, and MT-50, which were similar in surface area and crystallite size except for different pore-size distributions (Table 1). The ordering of decreasing photodecomposition rate constants of the mesoporous TiO2 materials is MT-18, MT-25, and MT50 (Fig. 7b and Tables 1 and 2), indicating that small pore size has a much greater photocatalytic activity. This result indicates that the adsorption of MB onto the active sites of the pore walls closer is enhanced, and so photocatalysts with small pore sizes decompose adsorbed substances more readily and effectively. In comparison with photocatalytic activity of commercial TiO2 , Ishihara ST-01, all samples calcined at 400 ◦ C have better photocatalytic activity. Fig. 7b shows the kinetics of the photocatalytic degradation of MB of these TiO2 materials. The photodecomposition rate constants were found to be 0.093 min−1 (MT-18), 0.081 min−1 (MT-25), and 0.066 min−1 (MT-50), which were higher than that of ST-01 (0.016 min−1 ). It is considered that the differences in their rate constants are attributed to the crystallite, pore size, and surface area of the mesoporous TiO2 materials. If the surface area is only considered, ST-01 (ca. 290 m2 g−1 ) has a larger surface area than MT-18 (ca. 186 m2 g−1 ), indicating that the ST-01 should have better photocatalytic activity. However, the crystallite size of ST-18 is 8.7 nm, which is larger than that of MT-18 (ca. 8.1 nm). In addition, the pore size of ST-01 (ca. 7.6 nm) is larger than that of MT-01 (5.1 nm), indicating that the photocatalytic activity of MT-18 can be higher than that of ST-01. Therefore, we think that the photocatalytic activity of mesoporous TiO2 is strongly dependent on the crystallite size, pore size, and surface area, but the effects of these factors on the photocatalytic activity are interdependent. Further investigation of how the porous structure of ST-01 and MT-18 affects the photocatalytic activity is necessary. 4. Conclusions a Degradation rate is divided into surface area. (Fig. 7a and Table 2). This result can be explained in terms of surface area, crystallite size, and pore-size distribution. A large surface area means that many substances are adsorbed onto the active sites of the catalysts which can decompose them [27,29]. Regarding the effect of pore size, smaller pore size shows higher photocatalytic activity (Tables 1 and 2). It has been commonly accepted that smaller crystallite size corresponds to more powerful redox ability because smaller crystallite size induces a larger band gap, which agrees with XRD results for crystallite sizes (Table 1) and DRS results for the absorption band edges (Fig. 6). Furthermore, in the effect of the pore size, mesoporous TiO2 with smaller pore size is likely to exhibit better photocatalytic activity. To precisely investigate the effect of pore size, This paper has shown the synthesis and photocatalytic activity of mesoporous TiO2 with various surface area, crystallite size, and pore-size distributions. The sol–gel synthesis with diblock copolymer and titanium precursor in aqueous solution gave a spherical morphology of mesoporous TiO2 with different pore sizes, crystallite sizes, and surface areas according the calcination temperature. The photocatalytic activity was increased with decrease of crystallite size, larger surface area, and smaller pore-size distribution. In comparison with commercial TiO2 , Ishihara ST-01, the mesoporous TiO2 materials exhibit better photocatalytic activities in the decomposition of MB. Acknowledgment This study was supported by the Ministry of Environment, Republic of Korea, through the Eco-Technopia 21 project. References [1] M.R. Hoffmann, S.T. Martin, W. Choi, D.W. Bahnemann, Chem. Rev. 95 (1995) 69–96. D.S. Kim et al. / Journal of Colloid and Interface Science 316 (2007) 85–91 [2] G. Calleja, D.P. Serrano, R. Sanz, P. Pizzaro, A. Garcia, Ind. Eng. Chem. Res. 43 (2004) 2485–2492. [3] V.F. Stone Jr., R.J. Davis, Chem. Mater. 10 (1998) 1468–1474. [4] Z. Li, B. Hou, Y. Xu, D. Wu, Y. Sun, J. Colloid. Interface. Sci. 288 (2005) 149–154. [5] B. Ohtani, Y. Ogawa, S. Nishimoto, J. Phys. Chem. B 101 (1997) 3746– 3752. [6] K. Cassiers, T. Linssen, M. Mathieu, Y.Q. Bai, H.Y. Zhu, P. Cool, E.F. Vansant, J. Phys. Chem. B 108 (2004) 3713–3721. [7] Y. Sakatani, D. Grosso, L. Nicole, C. Boissière, G.J. de A.A. Soler-Illia, C. Sanchez, J. Mater. Chem. 16 (2006) 77–82. [8] C.T. Kresge, M.E. Leonowicz, W.J. Roth, J.C. Vartuli, J.S. Beck, Nature 359 (1992) 710–712. [9] D.M. Antonelli, J.Y. Ying, Angew. Chem. Int. Ed. Engl. 34 (1995) 2014– 2017. [10] Q. Huo, D. Margolese, U. Ciesla, P. Feng, T.E. Cier, P. Sieger, R. Leon, P. Petroff, F. Schüth, G.D. Stucky, Nature 368 (1994) 317–321. [11] Y. Zhang, A. Weidenkaff, A. Reller, Mater. Lett. 54 (2002) 375–381. [12] T. Peng, D. Zhao, K. Dai, W. Shi, K. Hirao, J. Phys. Chem. B 109 (2005) 4947–4952. [13] S. Zhan, D. Chen, X. Jiao, C. Tao, J. Phys. Chem. B 110 (2006) 11199– 11204. [14] J.C. Yu, L. Zhang, J. Yu, New J. Chem. 26 (2002) 416–420. [15] J.-G. Yu, H.-G. Yu, B. Cheng, X.-J. Zhao, J.C. Yu, W.-K. Ho, J. Phys. Chem. B 107 (2003) 13871–13879. [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] 91 C. Wang, Q. Li, R.-D. Wang, Mater. Lett. 58 (2004) 1424–1426. Y. Yue, Z. Gao, Chem. Commun. (2000) 1755–1756. H. Zhang, J.F. Banfield, J. Mater. Chem. 8 (1998) 2073–2076. (a) A.S. Barnard, P. Zapol, J. Phys. Chem. B 108 (2004) 18435–18440; (b) A.S. Barnard, P. Zapol, Phys. Rev. B 70 (2004) 235–403. K.S.W. Sing, D.H. Everett, R.A.W. Haul, L. Moscow, R.A. Pierotti, J. Rouquerol, T. Siemieniewska, Pure Appl. Chem. 57 (1985) 603–619. F. Dumeignil, K. Sato, M. Imamura, N. Matsubayashi, E. Payen, H. Shimada, Appl. Catal. A 241 (2003) 319–329. Q. Huo, D.I. Margolese, G.D. Stucky, Chem. Mater. 8 (1996) 1147–1160. P. Yang, D. Zhao, D.I. Margolese, B.F. Chmelka, G.D. Stucky, Chem. Mater. 11 (1999) 2813–2826. T.-Z. Ren, Z.-Y. Yuan, B.-L. Su, Chem. Phys. Lett. 374 (2003) 170–175. D. Zhao, J. Feng, Q. Huo, N. Melosh, G.H. Fredrickson, B.F. Chmelka, G.D. Stucky, Science 279 (1998) 548–552. H. Lin, C.P. Huang , W. Li, C. Ni, S. Ismat Shah, Y.-H. Tseng, Appl. Catal. B 68 (2006) 1–11. Z. Wang, L. Mao, J. Lin, J. Photochem. Photobiol. A Chem. 177 (2006) 261–268. M. Anpo, T. Shima, S. Kodama, Y. Kubokawa, J. Phys. Chem. 91 (1987) 4305–4310. M. Miyauchi, A. Ikezawa, H. Tobimatsu, H. Irie, K. Hashimoto, Phys. Chem. Chem. Phys. 6 (2004) 865–870.
© Copyright 2026 Paperzz