Guang Zhu*a,
Hongyan Wanga,
Gaoxia Yanga,
Liangwei Chena,
Peijun Guob and
Li Zhang*a
aAnhui Key Laboratory of Spin Electron and Nanomaterials, Suzhou University, Suzhou 234000, P. R. China. E-mail: zhlisuzh@163.com; guangzhu@ahsztc.edu.cn; Fax: +86-557-2871003; Tel: +86-557-2871006
bDepartment of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, USA
First published on 21st August 2015
Novel carbon nanotube (CNT) and hierarchical ZnO microsphere composites were prepared via a facile chemical deposition route and their photocatalytic performance in the degradation of methylene blue (MB) was investigated. The results indicate that the as-prepared ZnO/CNT hierarchical microsphere composite with 1.1 wt% CNT shows optimized photocatalytic activity. The photocatalytic performance improvement can be attributed to the triple effects of high surface area, enhanced light absorption and suppression of charge carrier recombination resulting from the interaction between ZnO and CNT.
Carbon nanotubes (CNTs), an important member in carbon family, has potential applications in photocatalysis, energy storage, solar cells, and transparent electrodes due to their low cost, large surface area, superior chemical stability, and good catalytic activity.25–29 Recently, many works have demonstrated that CNTs incorporated with metal oxide semiconductor, show high activity for photocatalytic applications.30–35 The enhanced performance can be attributed to the improved electron transfer from the conduction band of semiconductor to the CNTs in the process of photocatalysis.36–38 Among metal oxide semiconductor catalysts, ZnO has been getting increased attention due to its suitable band gap of 3.37 eV and high electron mobility of 115–155 cm−2 V−1 s−1.39,40 So far, a few publications focus on the research of the CNTs doped ZnO composites and show a enhanced photocatalytic performance. Ahmad et al. prepared ZnO/CNTs nanocomposite by using sol method and used as-prepared nanocomposites as catalysts to photodegrade RhB dye.31 The results indicated that ZnO/CNTs nanocomposite has a superior photodegradation efficiency of RhB in comparison with the pure ZnO nanoparticle due to enhanced the electron–holes separation at the hetero-interface. Lv et al. reported that the ZnO/RGO/CNTs were prepared by microwave assisted method and used to photodegrade methylene blue (MB), and a degradation efficiency of 96% was achieved under UV light irradiation.41 Gao et al. prepared ZnO nanoparticles coated multi-walled carbon nanotubes for the photocatalytic degradation of MB, and results indicated that as-prepared composites have a higher photocatalytic activity than ZnO bulk material or the mechanical mixture of MWCNTs and ZnO.42 Despite the above progress to date, as promising hybrid materials for photocatalysis, the exploration on ZnO–CNTs composites is not nearly enough so far. It is well known that the photocatalytic performance strongly depends on the morphology of materials. Recently, hierarchically structured ZnO has been fabricated and used to enhance photocatalytic performance due to large surface area and higher electron transport of organic pollutants.43–45 Although superior photocatalytic performance can be improved for the hierarchically ZnO mircostructured, to our knowledge, there are rare research reports on enhanced photocatalytic performance of hierarchical structured ZnO/CNTs composites.
In our recent works, we have fabricated hierarchical structured TiO2/Ag microspheres using a facile chemical deposition route and applied in photocatalytic degradation of MB.46 In this work, we further explore the application of this method in the one-step fabrication of novel hierarchical structured ZnO/CNTs microsphere composites for photocatalytic degradation of MB. The novel hierarchical ZnO/CNTs microsphere composite with 1.1 wt% CNTs achieves a maximum degradation efficiency of 92.3% and 76% under UV and visible light irradiation for 60 min, compared with pure ZnO microspheres (70.4% and 37%), respectively. The enhanced photocatalytic performance is attributed to the triple effects of high surface area, enhanced light absorption and suppression of charge carriers recombination resulting from the interaction between ZnO and CNTs.
The morphology and structure of as-prepared samples were characterized by an scanning electronic microscopy (SEM, HATICH 4800), a JEOL-2010 high-resolution transmission electron microscope (HRTEM), X-ray diffraction (XRD, Japan MAC Science Co.), and Raman spectrometer (HORIBA Scientific) with an excitation of 532 nm laser light, respectively. The UV-Vis absorption spectra of as-prepared samples were detected using a UV-Vis spectrophotometer (Hitachi U-3900). Photoluminescence (PL) spectra were recorded on a HORIBA Jobin Yvon fluoromax-4 fluorescence spectrophotometer, using the 350 nm excitation line of a Xe lamp as light source. Brunauer–Emmett–Teller (BET) surface area was measured by ASAP 2020 Accelerated Surface Area and Porosimetry System (Micrometitics, Norcross, GA).
The photocatalytic activities of as-prepared samples were evaluated via decomposing methylene blue (MB) dye solution at room temperature. The concentration of MB and photocatalyst were set as 30 mg L−1 and 0.17 g L−1, respectively. Prior to irradiation, the suspensions were magnetically stirred in the dark for 30 min to establish an adsorption/desorption equilibrium. The dispersions were kept under constant air-equilibrated conditions before and during irradiation. The photocatalytic degradation process was observed by the change of the absorbance maximum in optical absorption spectra of MB dye. A 500 W Hg lamp and 500 W Xe lamp equipped with a 420 nm cutoff filter were employed as UV and visible light sources, and located 20 cm away from the reactor to trigger the photocatalytic reaction, respectively. A certain volume of suspension were drawn at selected times for analysis. The absorbance spectra of the temporal variations of the MB dye were recorded by a Shimadzu UV-3310 spectrometer.
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| Fig. 1 FESEM images of (a) ZC-0 microspheres, (b) and (c) ZC-1.1 composite, and (d) magnified image of the black pane area in (c). | ||
The high-resolution transmission electron microscope (HRTEM) images of as-prepared ZC-1.1 composite are shown in Fig. 3. The synthesized composite show a nearly mono-dispersed spherical shape with sizes of ca. 2 μm (as shown in Fig. 3a and b). Fig. 3c and d show that the high-magnification HRTEM images of as-prepared ZC-1.1 composite. The crystallites connecting to the CNTs have a lattice fringe of 0.28 nm which is ascribed to the (1 0 0) plane of ZnO (JCPDS 36-1451).
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| Fig. 3 (a) and (b) low-magnification HRTEM images, and (c) and (d) high-magnification HRTEM images of as-prepared ZC-1.1 composite. | ||
The XRD patterns of as-prepared ZC-0, ZC-0.8, ZC-1.1, ZC-1.5 and ZC-2.3 are shown in Fig. 4. The characteristic diffraction peaks at 31.8°, 34.4°, 36.3°, 47.5°, 56.6°, 62.9°, 66.6°, 68.1°, and 69.2° are indexed to (100), (002), (101), (102), (110), (103), (200), (112) and (201) crystal planes of the wurtzite-structure (JPCDS 36-1451) of ZnO, which demonstrates that the presence of CNTs does not result in the development of new crystal orientations or changes in preferential orientations of ZnO. The XRD analysis further shows that the main diffraction peaks of ZnO/CNTs composites are similar to those of pure ZnO, which demonstrates that the presence of CNTs does not result in the development of new crystal orientations or changes in preferential orientations of ZnO. It is noted that no typical diffraction peaks of carbon species are observed, which may be due to the low amount and relatively low diffraction intensity of CNTS in the composites.48
The Raman spectra of as-prepared ZC-0 and ZC-1.1 are shown in Fig. 5. The pure ZnO exhibits a strong Raman peak at 435 cm−1 corresponds to E2 mode of ZnO crystal. A small peaks at 326 cm−1 is assigned to zoneboundary phonons 3E2H–E2L for wurtzite ZnO single crystals which is matched up with Raman peak of bulk ZnO crystals.49 In addition, a longitudinal-optical (LO) mode at 573 cm−1, together with its overtones at 1146 cm−1 are observed for pure ZnO microspheres. Compared with pure ZnO, characteristic D peak at 1343 cm−1 and G peak at 1575 cm−1 are observed for ZC-1.1 composite. The G peak is the response of the in-plane stretching motion of symmetric sp2 C–C bonds, whereas the D peak results from the disruption of the symmetrical hexagonal graphitic lattice.50 This results further confirm that ZnO/CNTs composites have been prepared by the facile chemical deposition method.
The UV-Vis absorption spectra of ZC-0, ZC-0.8, ZC-1.1, ZC-1.5 and ZC-2.3 composites are displayed in Fig. 6. The absorption edges are derived from the intersection of the sharply decreasing region of a spectrum.51 Compared to the absorption edge of pure ZnO (ca. 400 nm), there is not a obvious change for the composites. The band gaps of the pure ZnO and composites obtained from the absorption edge are about 3.1 eV. Because ZnO and CNTs in the ZnO/CNTs composite are different two phases, their band-gap energies are not changed.53 However, compared with pure ZnO, the visible light absorption of ZnO/CNTs composites gradually increases with the increase of CNTs content in the composites, which can be ascribed to the presence of the black CNTs.54 The enhanced light absorption can increase the number of photo-generated electrons and holes to participate in the photocatalytic reaction and improve the photocatalytic performance.
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| Fig. 6 UV-Vis absorption spectra of as-prepared ZC-0, ZC-0.8, ZC-1.1, ZC-1.5, and ZC-2.3 composites. | ||
The photoluminescence (PL) emission spectra of ZC-0, ZC-0.8, ZC-1.1, ZC-1.5 and ZC-2.3 composites are shown in Fig. 7. The results display that a broad emission band in the range of 380–650 nm, which is ascribed to luminescence from localized surface states due to recombination of photogenerated electron–hole pairs.55 The PL intensity decreases with the increase of CNTs content, suggesting that the introduction of CNTs could quench the fluorescence from ZnO. The quenching mechanism of the PL spectra may because electron transfers from the excited ZnO.56 It may be possible to increase electron transfer and interfacial interaction between ZnO and CNTs, and reduce the electron–hole pair recombination, which can increase the photocatalytic activity. However, ZG-2.3 exhibits a significant increase of intensity compared to that of other composites, which is because that the excessive CNTs on ZnO can act as a kind of recombination center instead of providing an electron pathway.57,58
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| Fig. 7 Room-temperature PL emission spectra of as-prepared ZC-0, ZC-0.8, ZC-1.1, ZC-1.5, and ZC-2.3 composites. | ||
The photocatalytic degradation of MB under UV and visible light irradiation is used to evaluate the photocatalytic performance of as-prepared pure ZnO and ZnO/CNTs composites.
Fig. 8a shows the absorption spectrum of MB using as-prepared ZC-1.1 composite with reaction time under UV light radiation, which indicates that the MB content decreases with the increase of the light irradiation time. Fig. 8b shows the photocatalytic performance of as-prepared pure ZnO and ZnO/CNTs composites under UV light irradiation. The normalized temporal concentration changes (C/C0) of MB during photodegradation are proportional to the normalized maximum absorbance (A/A0). The photocatalytic activity of as-prepared ZC-0.8 composites (72.8%) is higher than that of pure ZnO (ZC-0) (70.4%). When CNTs amount is increased, the degradation efficiency is increased, and reaches a maximum value of 92.3% for ZC-1.1. However, when the CNTs loading is further increased, the photocatalytic performance will decrease, which is due to the following two reasons: (1) light harvesting competition between CNTs and ZnO appears with increase of CNTs amount,53 (2) the excessive CNTs can act as a kind of recombination center instead of providing an electron pathway.57,58 The photocatalytic performance of as-prepared pure ZnO and ZnO/CNTs composites under visible light irradiation indicates a similar trend as the photocatalytic degradation of MB under UV light irradiation (as shown in Fig. 8c). Under visible irradiation, the photocatalytic activity of as-prepared ZC-1.1 composite reaches a maximum value of 76%. According to above results, the enhanced photocatalytic performance of as-prepared ZnO/CNTs composites suggests that the introduction of CNTs play an important role in the photocatalytic performance. The stability of as-prepared composite with ZC-1.1 as catalyst under UV light irradiation is also studied (as shown in Fig. 8d). It can be seen that the photocatalytic activity of composite do not decrease conspicuously after six successive cycles of degradation tests, indicating that this composite is fairly stability.
Based on the experimental results, the higher photocatalytic activity of ZnO/CNTs composites could be summarized as follows: (1) higher surface area. The BET surface area of as-prepared ZC-0 and ZC-1.1 was carried out, and the results indicate that the surface area of ZC-1.1 (26.1 m2 g−1) is higher than that of pure ZnO (17.6 m2 g−1) due to loading CNTs with higher surface area. The higher surface areas result in the large contact areas between the active sites and the target substrate, which can increase the photocatalytic activity. (2) Increased visible light absorption. The strong absorption of visible light can be produced due to the introduction of CNTs (as shown in Fig. 6), which increases the number of photo-generated electrons and holes to participate in the photocatalytic reaction and improve the photocatalytic performance. (3) The reduced electron–hole pair recombination and increased electron transfer. The photocatalytic degradation of MB by ZnO/CNTs composites under light irradiation involves two mechanisms. The work function of excited MB, CNTs, and conduction band (CB) of ZnO are −3.60, −4.80 eV and −4.05 eV (vs. vacuum),52,59 respectively, as shown in Fig. 9. Under the UV light irradiation, the electrons are excited from the valence band (VB) of ZnO to CB, and then these photo-induced electrons transfer from the CB of ZnO to CNTs. On the other hand, the dye can acts as a sensitizer of visible light, and excited electrons transfer to the CB of ZnO via CNTs. In the whole electron transfer process, CNTs could efficiently increase electron transfer and reduce the electron–hole pair recombination,60,61 which is confirmed by the results from PL emission spectra (as shown in Fig. 7), leading to a enhanced photocatalytic performance.
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