Juying Leia,
Fenghui Liub,
Lingzhi Wangb,
Yongdi Liu*a and
Jinlong Zhang*bc
aState Environmental Protection Key Laboratory of Environmental Risk Assessment and Control on Chemical Process, School of Resources and Environmental Engineering, East China University of Science and Technology, 130 Meilong Road, Shanghai 200237, P. R. China. E-mail: ydliu@ecust.edu.cn
bKey Lab for Advanced Materials, Institute of Fine Chemicals, School of Chemistry and Chemical Engineering, East China University of Science and Technology, 130 Meilong Road, Shanghai 200237, P. R. China. E-mail: jlzhang@ecust.edu.cn
cSuzhou Jukang New Materials Co. Ltd, 558 Fenhu Road, Suzhou, Jiangsu Province 201211, P. R. China
First published on 23rd May 2017
New polymer composites consisting of poly(diphenylbutadiyne) (PDPB) and g-C3N4 have been successfully prepared. UV-vis diffuse reflectance spectra show that the existence of PDPB in composites can clearly increase the visible light absorption of the catalysts. Photoluminescence spectroscopy and photoelectrochemical measurements reveal that PDPB can effectively facilitate the charge carrier separation in the composites. Compared with pure g-C3N4 or pure PDPB, the composite catalysts exhibit observably enhanced visible-light photocatalytic activity for degradation of RhB and phenol. A possible mechanism for the charge separation and transfer in the composite catalysts is proposed. In addition, the composite catalysts show stable catalytic performance after five successive runs, displaying potential for applications in various fields of photocatalysis.
However, the g-C3N4 has many weak points such as the small surface area, high recombination rate of photogenerated electron–hole pairs and low visible light utilization efficiency.15 Hence, various methods have been used to solve these problems, for example, synthesizing different structures,16,17 doping with metal or nonmetal elements,18–21 coupling with other semiconductors,22–26 and modifying by conjugated polymers.27,28 Among these methods, the conjugated polymer modification has attracted many attentions because the conjugated polymer not only can enhance the absorption of the visible light but also can act as a semiconductor. Yan et al. synthesized carbon nitride–poly(3-hexylthiophene) (g-C3N4–P3HT) composite photocatalyst.24 They found that the novel photocatalyst exhibited significantly enhanced photocatalytic activity. Thakare et al. reported on the synthesis of a ternary polymer composite of graphene, carbon nitride, and poly(3-hexylthiophene) (G–g-C3N4–P3HT) which had enhanced photocatalytic activity.29 Ge et al. prepared a novel polyaniline–graphitic carbon nitride (PANI/g-C3N4) composite photocatalyst which had intensive visible light photocatalytic activity.30 Wang et al. prepared an efficient visible-light photocatalyst using g-C3N4 and ordinary polyvinyl chloride (PVC) as main precursors.28 However, to the best of our knowledge, the report about using polymer modified g-C3N4 is still scarce.
Poly(diphenylbutadiyne) (PDPB) is a newly developed polymer semiconductor which was reported by Hynd Remita in 2015.31 The PDPB obtained by π-stacking of oligomers presents a high photocatalytic activity and long-term stability. Recent research has also shown that the composite of PDPB and semiconductor ZnO exhibited high visible light photocatalytic activity,32 due to the visible light harvesting of PDPB. Inspired by this, we speculate that if we combine PDPB with g-C3N4, based on the good visible light absorption of g-C3N4 itself, the combination of g-C3N4 and PDPB will bring a better absorption of visible light, leading to a better visible light activity.
Herein, we prepare a polymer composite photocatalyst consisting of g-C3N4 and PDPB (CN-PDPB). The photocatalytic activity is investigated by evaluating the photocatalytic degradation of Rhodamine B (RhB) and phenol. The results exhibit that the CN–PDPB has higher photocatalytic activity than pure g-C3N4 and PDPB. It is maybe because the existence of PDPB can obviously improve the absorption of g-C3N4 in the visible light range. What's more, the interaction between g-C3N4 and PDPB improves the separation efficiency of the photo-generated charge carriers. In addition, the composites catalysts show stable catalytic performance after five successive runs.
PDPB was synthesized following the previously method published by Hynd Remita.31
The composite catalysts of g-C3N4 and PDPB were prepared by impregnating g-C3N4 (0.5 g) with an ethanol solution of PDPB for a night, and then the solvent was vapored in oil bath at 363 K. The resultant samples were labeled as 50:x CN–PDPB, where 50:x was the mass ratio of g-C3N4 and PDPB in the above-mentioned process for preparation of CN–PDPB photocatalysts.
Fig. 2 shows the wide-angle XRD patterns of pure PDPB, pure g-C3N4 and CN–PDPB photocatalysts. The peak at 27.7° in the XRD pattern of g-C3N4 coming from the interlayer stacking of aromatic segments can be indexed as the (002) planes. Another pattern at 13.1° indexed as (100) planes is due to the in-plane structural packing motif.5,33,34 From the XRD patterns of CN–PDPB photocatalysts, we can see that the two characteristic peaks of g-C3N4 are clearly observed, indicating that PDPB does not change the crystalline structure of g-C3N4. However, the characteristic patterns of PDPB are not observed at first because of its low content in the composites but with the increase of content of PDPB, the XRD of 50:4 CN–PDPB displays patterns at 14°, 20.4°, 23.6°, 24.7°, which are ascribed to the characteristic patterns of PDPB.31 This results further confirm the existence of PDPB in the CN–PDPB composites.
The surface chemical environment of the catalysts is analyzed by XPS. Fig. 3a and b show the C 1s XPS spectra of g-C3N4 and 50:2 CN–PDPB, respectively. In Fig. 3b, the C 1s has two peaks at 284.8 and 288.1 eV. The C peak at 284.8 eV corresponds to graphitic carbon, which is usually observed in the XPS spectrum of carbon nitrides.35 The peak at 288.1 eV is ascribed to the sp2-bonded carbon (N–CN) from carbon nitride and carbon atoms in conjugated structure (–CC–) from PDPB.28,36–39 Compared with Fig. 3a, the intensity ratio of the peaks at 284.8 eV and 288.1 eV in Fig. 3b reduces, indicating the existence of –CC– on the surface of 50:2 CN–PDPB. This further confirms the existence of PDPB in the composite CN–PDPB.
Fig. 4 shows the FTIR spectra of PDPB, g-C3N4 and 50:2 CN–PDPB. For g-C3N4, the strong bands at 1241, 1322, 1406, 1571, and 1631 cm−1 are corresponding to the typical stretching modes of CN heterocycles and the band at 806 cm−1 is attributed to the characteristic breathing mode of triazine units. Compared with the FTIR of PDPB and g-C3N4, the FTIR band at 685 cm−1 and 787 cm−1 can be found in 50:2 CN–PDPB which is consistence with the previous report31 but the intensities of the peaks are weak. That is because the low content of PDPB in 50:2 CN–PDPB. All of these prove the existence of PDPB in 50:2 CN–PDPB.
The UV-vis diffuse reflectance spectrum for the catalysts in Fig. 5 shows that the absorption of the CN–PDPB composites is higher than that of pure g-C3N4 in the range of 360–800 nm due to the existence of PDPB. Furthermore, the absorption intensity of the CN–PDPB increases with the increase of PDPB content. This improved absorption is helpful to the improvement of the photocatalytic activity of g-C3N4.
Fig. 6 Photocatalytic degradation of RhB over different catalysts (a) under simulated sunlight (with AM 1.5), (b) under visible light irradiation (λ > 420 nm). |
Fig. 7 The UV-vis spectra of the degraded RhB using the 50:2 CN–PDPB under simulated sunlight (with AM 1.5). |
In addition, we use TOC measurement to further confirm the degree of mineralization of RhB solution. The RhB solution is almost decolorized after 60 min irradiation (in Fig. 6a) and about 30% removal of TOC has been seen in Fig. 8, manifesting that RhB has been not only decolorized but also mineralized partly.
Phenol was chosen as another model pollutant to eliminate the sensitization effect of RhB.5 Fig. 9 presents the results of photocatalytic degradation of phenol catalyzed by pure g-C3N4 and 50:2 CN–PDPB under visible light irradiation. We can see that the photocatalytic degradation efficiency of phenol with 50:2 CN–PDPB is obviously higher than that of pure g-C3N4, further illustrating that the composite has increscent photocatalytic activity. In addition, we use TOC measurement to further confirm the degree of mineralization of phenol solution. From Fig. 10, it can be seen that the TOC removal values are increased. The degradation of phenol takes time until being finally mineralized.
Fig. 9 Photocatalytic degradation of phenol over different catalysts under visible light irradiation. |
Besides the photoluminescence measurement, electrochemical impedance spectroscopy (EIS) is also applied to investigate the charge transfer resistance of the catalysts.43–45 The EIS results of prepared samples are presented in Fig. 12 in the form of Nyquist plots. It can be clearly found that the g-C3N4 has the highest charge transport resistance for its biggest arc radius and the arc radius of CN–PDPB is significantly smaller than that of the pure g-C3N4. In addition, the 50:2 CN–PDPB has the smallest arc radius among the prepared materials, revealing an effective separation of photogenerated electron–hole pairs and faster charge transfer occurred on 50:2 CN–PDPB.
To further investigate the photocatalytic mechanism of the CN–PDPB, the transient photocurrent responses of pure g-C3N4 and 50:2 CN–PDPB were tested by on–off cycles of irradiation.
Transient photocurrent analysis is also a widely used typical method to investigate the electron–hole separation effect for a material.46 In Fig. 13, it can be seen that the photocurrent of 50:2 CN–PDPB is much larger than the photocurrent of pure g-C3N4, indicating higher separation and transfer efficiency of photo-generated electrons and holes due to the synergetic effect of g-C3N4 and PDPB.
The effects of benzoquinone (BQ, a typical ˙O2− scavenger) and disodium oxalate (Na2C2O4, a typical hole scavenger) on the photodegradation of RhB in the presence of 50:2 CN–PDPB are investigated. From the Fig. 14, we can see that the BQ clearly inhibits the photodegradation of RhB, but the Na2C2O4 lightly decreases the photodegradation of RhB, indicating that the ˙O2− and the holes are all effective for the degradation of RhB but the ˙O2− is the main active species for the RhB degradation.
On the basis of the above experiments and results, the mechanism is explained in Fig. 15. With irradiation of light, both g-C3N4 and PDPB can be excited to produce photo-generated electrons and holes. The conduction band (CB) position of PDPB (−1.78 eV) is more negative than that of g-C3N4 (−1.13 eV), and the valence band (VB) position of g-C3N4 (+1.57 eV) is more positive than that of PDPB (+0.18 eV).31 Hence, the photo-generated electrons of PDPB can easily transfer to the conduction band (CB) of g-C3N4, while the holes of g-C3N4 can transfer to the valence band (VB) of PDPB. Thus, the recombination of photo-generated electrons and holes can be inhibited and an effective charge separation is achieved, resulting in a remarkable enhancement of the photocatalytic activity. Moreover, the major possible reactions can be displayed as follows:
CN–PDPB + hv → g-C3N4*–PDPB* |
g-C3N4*–PDPB* → g-C3N4 (e−e−/h+h+)–PDPB (e−e−/h+h+) |
g-C3N4 (e−e−/h+h+)–PDPB (e−e−/h+h+) → g-C3N4 (e−e−e−/h+)–PDPB (e−/h+h+h+) |
e− + O2 → ˙O2− |
˙O2− + organic pollutants → degradation products |
h+ + organic pollutants → degradation products |
The stability of photocatalyst is another important issue for a photocatalyst. The recycling runs in the photodegradation of RhB in the presence of 50:2 CN–PDPB are carried out. Fig. 16 shows that the photocatalytic degradation degree of RhB still remains high after 5 cycles, manifesting the catalyst has good photocatalytic stability.
Fig. 16 Effect of cycling runs on RhB degradation in the presence of 50:2 CN–PDPB under visible-light irradiation. |
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