Zhenhai
Wen
ab,
Wei
Wu
ac,
Zhuang
Liu
a,
Hao
Zhang
a,
Jinghong
Li
*a and
Junhong
Chen
*b
aBeijing Key Laboratory for Analytical Methods and Instrumentation, Tsinghua University, Beijing 100084, China. E-mail: jhli@mail.tsinghua.edu.cn
bDepartment of Mechanical Engineering, University of Wisconsin-Milwaukee, 3200 North Cramer Street, Milwaukee, Wisconsin 53211, USA. E-mail: jhchen@uwm.edu
cKey Laboratory of Jiangxi Province for Ecological Diagnosis-Remediation and Pollution Control, Nanchang Hangkong University, Nanchang 330063, Jiangxi, China
First published on 2nd April 2013
A reliable nanocasting method has been developed to synthesize mesoporous hybrids of platinum (Pt) nanoparticles decorating tungsten trioxide (WO3). The process began with modification of the SBA-15 template with carbon polymers and Pt nanoparticles accompanied by adsorption of W6+, which was then converted into m-Pt–WO3 composites by heat treatment and subsequent template removal. The synthetic strategy can be easily extended to prepare other mesoporous nanohybrids with metal oxide loaded precious metal composites. Comprehensive characterizations suggest that the as-developed m-Pt–WO3 nanohybrid exhibits unique properties with mesoporous structure, excellent crystalline structure, and high surface area. When the photocatalytic properties of m-Pt–WO3 nanohybrids were systematically investigated, it was revealed that the m-Pt–WO3 nanohybrids showed great promise for degrading the organic dye under visible light irradiation, which shows an excellent photocatalytic activity that far exceeded those of pure phase mesoporous WO3 and commercial TiO2 (P25), and was 10-fold more active than that of the bulk Pt–WO3 catalyst. The as-developed synthetic route opens up a new avenue for designing mesoporous hybrid materials for various applications benefiting from the unique porous structure, high surface area, and synergistic effects among constituents.
As an important semiconductor, tungsten oxide (WO3) has been considered as a potential nontoxic, and stable photocatalyst due to its small band gap (2.4–2.8 eV) as well as high oxidation power of valence band (VB) holes (+3.1–3.2 vs. NHE), which makes it possible to efficiently absorb visible light to degrade organic compounds.3 The only drawback of WO3 is its relatively low conduction band (CB) edge (+0.3–0.5 vs. NHE) that is inadequate for O2 reduction and can greatly reduce the photocatalytic efficiency due to rapid recombination of the photo-generated holes and electrons.4 It was reported that this problem can be circumvented by loading platinum (Pt) nanoparticles on WO3 because the introduction of Pt nanoparticles can promote the multi-electron reduction of oxygen, and thus significantly lessen the recombination effect.5 Nevertheless, there is still great potential to optimize the Pt–WO3 composite catalyst associated with its architecture and interactions between Pt and WO3, because the efficiency of the photocatalyst is highly dependent on the surface area, particle size, morphology or structure, and unique surface characteristics. In particular, photocatalysts with mesoporous structure have great potential to achieve significantly enhanced activities due to their porous structure and large surface area.6 However, there is still a lack of effective, reliable, and versatile methods for fabricating mesoporous metal oxide hybrids with precious metals, despite that such nanohybrids endow great potentiality for exploitation and broad application prospects.7
Typically, mesoporous materials can be synthesized through either a soft-template method8 with liquid crystalline phases as a structure-directing agent or a hard-template route9 with mesoporous silica or carbon as a framework. Because the synthesis of mesoporous silica is very well established and can be tuned with morphology ranging from noodle-like, rodlike, to spherical shape,10 mesoporous silica has been widely used as a template for developing other functional mesoporous materials.
We herein describe the use of mesoporous silica as a template in the synthesis of nanohybrid photocatalysts of mesoporous WO3 loaded Pt nanoparticles (m-Pt–WO3) with a high specific surface area. The new nanohybrids are conducive for maximizing the utilization of Pt nanoparticles. The as-developed m-Pt–WO3 exhibited a surprisingly outstanding photocatalytic activity in the photodegradation of methylene blue (blue) dyes with the assistance of visible-light. The synthetic method can be potentially extended to fabricate other mesoporous hybrids with metal oxide loaded highly distributed precious metals.
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Fig. 1 Illustration of the preparation process of m-Pt/WO3 and the schematic mechanism of photodegradation of organic dyes by Pt/WO3 photocatalysts under visible light irradiation. |
It is believed that the modification of carbonaceous polymers on the surface of SBA-15 plays a key role in preparation of its replica. On the one hand, the surface properties of the mesoporous silica are highly crucial to achieve uniform and efficient incorporation of targeted material precursors into the voids of the template. On the other hand, in contrast to the silicon alkoxides, it is quite difficult to precisely control the hydrolysis or polymerization of most of the metal precursors. The present work takes advantage of recent synthetic advancements in “painting” –OH/–CO group-rich polymers on the nanochannels of the SBA-15 template. In this way, the precursor can be effectively infiltrated into the pores of the template and subsequently effectively converted to the target material. Moreover, the carbonaceous polymer can function as a reaction reagent for decorating some functional precious metal nanoparticles,13 and the burning off of the carbonaceous polymer can free up adequate space to accommodate the volume change during the conversion process from precursors to target materials.
In the investigation of the evolving processes, transmission electron microscopy (TEM) was conducted to observe the nanostructures of the products at various stages. By comparing the TEM images of SBA-15 (Fig. 2a), it was clearly demonstrated that a film of carbonaceous polymers was formed with distinct Pt nanoparticles in nanochannels of C–Pt–SBA-15 composites (Fig. 2b). Fig. 2c exhibits a typical TEM image of mesoporous Pt–WO3 hybrids after removal of the SBA-15 and carbonaceous polymers, which basically maintained the overall morphology of the well-known monolithic shape of the SBA-15, indicating that the present method can result in a good replicate of the original phase. Fig. 2d presents a representative magnified TEM image of m-Pt–WO3 hybrids, in which one can clearly observe a disordered porous structure constructed by a large number of nanoparticles in the m-Pt–WO3 hybrids, which stands in contrast to ordered mesoporous structure in its parent (SBA-15). This result suggests that the ordered structure was partly damaged during the process of removal of the SBA-15 template, burning out of carbonaceous polymers, and formation or growth of crystalline WO3. It was illustrated that, according to the HRTEM image (Fig. 2e), the WO3 nanoparticles were decorated with many small Pt nanoparticles. Based on analysis of energy-dispersive X-ray spectroscopy (EDS), it was revealed that the m-Pt/WO3 comprised of 73.19 wt% W, 21.08 wt% O and 5.73 wt% Pt, respectively (Fig. S1, ESI†). For comparison, we also prepared mesoporous WO3 (m-WO3) as a reference sample using a similar method without adding the Pt source during the fabrication process, as shown in Fig. 2f. It is worth mentioning that, besides being used for preparing m-Pt/WO3 and m-WO3, the as-developed synthetic strategy can be potentially extended to prepare various mesoporous metal oxides and their composites, which are expected to enhance their performance for practical applications due to their high surface area, tunable pore size, adjustable framework, as well as surface properties. For instance, mesoporous Pt–Fe2O3 and Ag–SnO2 nanohybrids (Fig. S2, ESI†) were also successfully prepared using the same method.
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Fig. 2 TEM images of SBA-15 (a), C/Pt/SBA-15 (b), m-Pt/WO3 free of template (c–e), and m-WO3 with a different magnification (f). |
The m-Pt–WO3 nanohybrids were further characterized for their porous structure, composition, and surface properties. Fig. 3a presents the powder X-ray diffraction (XRD) patterns of m-Pt/WO3 and m-WO3, respectively. Well-defined peaks corresponding to (111), (200), and (220) peaks from face-centered cubic (fcc) Pt in m-Pt–WO3 nanohybrids can be clearly identified. The peaks besides the characteristic peaks of Pt in m-Pt–WO3 nanohybrids are consistent with the characteristic peak of WO3, which can be well indexed to the pure monoclinic WO3 with lattice constants of a = 7.306 Å, b = 7.54 Å, c = 7.692 Å, and β = 90.88° (JCPDS card no. 72-0677). Small-angle X-ray powder diffraction (SXRD) was further performed to characterize the products (Fig. S3, ESI†). The SBA-15 exhibited a typical three-peak pattern corresponding to (10), (11), and (20) reflection lines. In contrast, m-Pt/WO3 only displayed a feeble broad peak in the range of 1.5–2.5°, suggesting that the evolved m-Pt/WO3 maintained a porous structure while the highly ordered structure had already collapsed, which is in accordance with structures shown in the TEM images.
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Fig. 3 XRD patterns of m-WO3 and m-Pt–WO3 hybrids (a); and pore size distribution and nitrogen adsorption–desorption isotherms (inset) of m-Pt/WO3 (b). |
The surface area and the porous structure were further investigated through the analysis of nitrogen adsorption–desorption isotherm curves measured at 77 K using the Brunauer–Emmett–Teller (BET) method. m-Pt/WO3 exhibited a curve of the type IV isotherms with a distinct hysteresis loop at the relative pressure P/P0 ranging from 0.4 to 0.8 (inset of Fig. 3b), corresponding to different processes between adsorption onto and desorption from the mesopores according to the IUPAC nomenclature. It was demonstrated that m-Pt/WO3 possessed a BET surface area of 152.7 m2 g−1, which is one order of magnitude higher than that (9.8 m2 g−1) of Pt/bulk-WO3 (Fig. S4, ESI†), and is comparable to that of the mesoporous WO3 (143.0 m2 g−1) reported previously.14 Pore size distributions were calculated from the desorption branch of the N2 adsorption isotherm using the Barrett–Joyner–Halenda (BJH) formula. As shown in Fig. 3b, m-Pt/WO3 exhibits a weak peak at 6.3 nm accompanying a feeble peak at about 3.9 nm, indicating the dual-pore structure in the m-Pt–WO3 hybrids.
The surface composition information of m-Pt/WO3 was analyzed using X-ray photoelectron spectroscopy (XPS). Fig. 4 presents the survey XPS spectra of m-Pt–WO3 nanohybrids; one can observe a series of peaks corresponding to W, Pt and O spectra, respectively, confirming the existence of W, Pt, and O elements in m-Pt/WO3. Fig. 4b–d present high-resolution XPS data of Pt 4f, W 4f, and O 1s in the m-Pt–WO3 nanohybrids, respectively. One can observe that the 4f7/2 and 4f5/2 signals of Pt are positioned at about 71.1 and 74.3 eV, respectively, suggesting the metallic form (zero valence state) for Pt nanoparticles. Two principal peaks of the W element are centered at 35.4 and 37.6 eV, which can be attributed to the oxidation state of tungsten with +6 valency of the W 4f7/2 and W 4f5/2 spectral lines. The O 1s peak at 530.7 eV is attributed to the oxygen of WO3. These results are consistent with the XRD pattern results. According to XPS analyses, the m-Pt–WO3 nanohybrids are comprised of 74.2 wt% W, 19.4 wt% O and 6.4 wt% Pt, respectively.
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Fig. 4 XPS spectra of m-Pt–WO3 nanohybrids (a), high-resolution XPS of Pt4f (b), W4f (c) and O 1s in m-Pt/WO3. |
The photocatalytic activity was obtained by studying photocatalytic oxidation of methyl blue (MB) as a model reaction under visible-light (λ > 400 nm) irradiation with m-Pt/WO3, Pt/bulk-WO3 (Fig. S5, ESI†), P25, and m-WO3 as photocatalysts, respectively. The normalized temporal concentration changes (C/C0) of MB upon photodegradation were proportional to the normalized maximum absorbance (A/A0), which can be derived from the changes in the dye's absorption profile (λ = 665 nm) during photocatalytic processes. Fig. 5a presents the temporal concentration changes of MB over different photocatalysts, from which the following fundamental information can be extracted. At first, the MB concentration for various samples decreased in a stepwise manner at different rates during the degradation processes, suggesting that there were remarkable differences in photocatalytic activity among these samples. Secondly, the m-Pt–WO3 nanohybrids showed a drastic decline in C/C0 compared with other samples, as evidenced by a C/C0 value of 0.33 in 2 min, which showed a striking contrast to Pt/bulk-WO3 that degraded MB to a C/C0 value of 0.72 within 2 min. Thirdly, almost all MB dyes were degraded in 5 min and 60 min for m-Pt/WO3 and Pt/bulk-WO3 catalysts, respectively, while both P25 and m-WO3 showed an insignificant change even after exposure to visible-light irradiation for 90 min. The photocatalytic activity of these catalysts can also be directly reflected in digital photographs of the MB solution after irradiating with visible light for different durations (Fig. 5b). The m-Pt/WO3 exhibited a very quick color change from blue, to light blue, and then to colorless during the initial periods, which outperformed the Pt/bulk-WO3 and was far better than P25 and m-WO3.
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Fig. 5 Concentration variation (a) and digital photographs (b) of the MB solutions during the photodegradation under visible light (λ > 400 nm) over m-Pt/WO3, Pt/bulk-WO3, P25, and m-WO3, respectively. |
Considering that m-Pt/WO3 showed much higher photocatalytic activity than Pt/bulk-WO3 and m-WO3, it is reasonable to conclude that mesoporous structure and loading of Pt nanoparticles are two key factors that improve the photocatalytic activity. It is generally acknowledged that the performance of a photocatalyst is highly dependent on the following three factors, namely the adsorption of dye molecules, the light absorption, and the charge transport and separation.1a,15 The synergy between Pt nanoparticles and WO3 can be foreseen to be present in the mesoporous structure due to the porous architecture and interactions between WO3 and Pt nanoparticles, endowing superior catalytic properties in the as-prepared m-Pt/WO3. As is well known, the major issue in the WO3 photocatalyst is the low conduction band (CB) edge (+0.3–0.5 vs. NHE), which is not enough to transfer the electron to the oxidant (e.g. oxygen), leading to the recombination of photogenerated electrons and holes. One of the effective strategies is to introduce Pt nanoparticles that can efficiently take away the photogenerated electrons and reduce the recombination effect.5 Obviously, the mesoporous structures can be beneficial to achieve uniform loading of Pt nanoparticles onto the WO3 surface and thus advance the synergistic effects between the two components, as was schematically shown in Fig. 1. First, mesoporous structures can effectively absorb more light since the porous structure can enhance the utilization of scattered light;16 second, the m-Pt/WO3 may enhance the capability for enrichment of MB on the surface of photocatalysts and offer more catalytic sites for photocatalytic reaction greatly due to the high surface area;6c,17 third, the Pt nanoparticles are uniformly decorated on the surface of WO3, which is conducive for achieving optimum performance to make the best of Pt nanoparticles upon suppression of the charge carrier recombination and thus maximizing the performance for degradation of MB. It should be noted that the pure phase m-WO3 had a similar BET surface area (137.6 m2 g−1) while it displayed a quite weak activity for photodegradation of MB, implying that Pt nanoparticles play a key role in promoting the electron transfer and transport and significantly reduce the charge carrier recombination.3a
It should be noted that, in addition to the ultra-high activity, the as-developed m-Pt/WO3 catalysts also showed excellent stability in repeated running cycles. The durability of the m-Pt/WO3 catalyst was investigated for the degradation of MB under visible light (Fig. S6, ESI†), which was monitored for three consecutive cycles with a period of 20 min. After each cycle, m-Pt/WO3 was collected by centrifuging the catalysts used in previous experiments followed by washing and drying, and the fresh MB solution was used for each cycle of photocatalytic experiments. There was no significant change in the photodegradation rate during the three consecutive cycles, and almost all the MB could be degraded in 5 min, indicating the good stability of the prepared m-Pt/WO3 photocatalyst.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c3cp50647a |
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