Peng Zengab,
Xiaoyuan Jiac,
Zhiguo Sua and
Songping Zhang*a
aState Key Laboratory of Biochemical Engineering, Institute of Process Engineering, Chinese Academy of Sciences, Beijing 100190, P. R. China. E-mail: spzhang@ipe.ac.cn; Fax: +86 10 82544958; Tel: +86 10 82544958
bUniversity of Chinese Academy of Sciences, Beijing, 100049, P. R. China
cSchool of Pharmaceutical Sciences (Shenzhen), Sun Yat-sen University, Guangzhou 510275, P. R. China
First published on 5th June 2018
A heterogeneous WS2/g-C3N4 composite photocatalyst was prepared by a facile ultrasound-assisted hydrothermal method. The WS2/g-C3N4 composite was used for photocatalytic regeneration of NAD+ to NADH, which were coupled with dehydrogenases for sustainable bioconversion of CO2 to methanol under visible light irradiation. Compared with pristine g-C3N4 and the physical mixture of WS2 and g-C3N4, the fabricated WS2/g-C3N4 composite catalyst with 5 wt% of WS2 showed the highest activity for methanol synthesis. The methanol productivity reached 372.1 μmol h−1 gcat−1, which is approximately 7.5 times higher than that obtained using pure g-C3N4. For further application demonstration, the activity of the WS2/g-C3N4 composite catalyst toward photodegradation of Rhodamine B (RhB) was evaluated. RhB removal ratio approaching 100% was achieved in 1 hour by using the WS2/g-C3N4 composite catalyst with 5 wt% of WS2, at an apparent degradation rate approximately 2.6 times higher than that of pure g-C3N4. Based on detailed investigations on physiochemical properties of the photocatalysts, the significantly enhanced reaction efficiency of the WS2/g-C3N4 composite was considered to be mainly benefiting from the formation of a heterojunction interface between WS2 and g-C3N4. Upon visible-light irradiation, the photo-induced electrons can transfer from the conduction band of g-C3N4 to WS2, thus recombination of electrons and holes was decreased and the photo-harvesting efficiency was enhanced.
Graphitic carbon nitride (g-C3N4), a polymeric semiconductor with a band gap of about 2.7 eV, has attracted significant attention in recent years because of its excellent visible light response,1,13,14 non-toxicity, low cost, and abundant raw materials. As a visible-light active photocatalyst, g-C3N4 has been widely applied for photocatalytic degradation of pollutants, water splitting, and regeneration of NADH since 2009.15,16 Nevertheless, fast recombination of photogenerated electron–hole pairs and low quantum efficiency limits its further applications. In general, there are three routes to improve the photocatalytic efficiency of g-C3N4, which include construction of nanostructure, elemental doping, and hybridization. By fabricating nanosheets,17 diatom frustule structure,18 multishell nanocapsules,19 and some other novel nanostructures,20 more active sites were exposed on g-C3N4 for enhanced light harvesting due to significantly increased specific surface area, and the migration rate of photo-generated electrons was promoted and the recombination of electrons and holes reduced.18–20 Elemental doping was another widely adopted method for reducing the recombination of electron–hole pairs by replacing the lattice defects of g-C3N4.21,22 Nevertheless, fabrication of new nanostructures and elemental doping often involve complicated preparation process and uncontrollable results. Compared with these above two methods, hybridization of g-C3N4 with some other semiconductors was is relative simple but efficient. The hybrid materials, which usually have an unsaturated outer layer electron, can act as a new electron carrier to trap the electrons in the conduction band (CB) of g-C3N4 through formation heterojunction or “Z” scheme electron transfer chain.4,23,24 Nevertheless, either construction of heterojunction or “Z” scheme transfer chain, there are certain requirements for the band structure of hybrid materials, which need a good coordinated relationship with that of g-C3N4.
In recent years, transition metal dichalcogenides (TMDCs) have emerged and received tremendous attentions. TMDCs such as WS2, MoS2, WSe2, and MoSe2, have various unique electronic, optical, mechanical and chemical properties, promising their potential applications in electronic devices, transistors, energy storage devices and catalysis.25–27 Among TMDCs, the 2H-WS2 has a band gap of about 2.64 V, with conduction band (CB) and valence band (VB) positions at ≈−1.03 V and 1.61 V versus normal hydrogen electrode,26,28 respectively; which means the WS2 possesses energy level of CB and VB both lower than that of g-C3N4, but the CB offset between g-C3N4 and WS2 is much shorter than the band gap of g-C3N4. Therefore, there would be a perfect band structure coordination between WS2 and g-C3N4 to construct a heterojunction structure. The good match for the energy level would possibly enable fast transfer of the photo-induced electrons in the CB of g-C3N4 to the CB of WS2 before recombination with holes in VB of itself, so that the light harvesting efficiency and utilization of photo-induced electrons would be improved largely.29–32
In this present work, a heterogeneous WS2/g-C3N4 composite photocatalyst was prepared via ultrasound assisted hydrothermal method. The photocatalytic performance was evaluated through the regeneration of NADH and degradation of RhB under visible light. Detailed investigations of the physiochemical and photochemical properties of the photocatalysts were performed to elucidate the photoinduced electron-transfer mechanism involved in the heterogeneous WS2/g-C3N4 composite photocatalyst. Therefore, our work highlights the promise of constructing heterojunction based on g-C3N4 for photocatalyzed NADH regeneration and pollutant degradation, and encourages further in-depth investigations of this novel type of heterojunction for artificial photocatalysis.
The organometallic electron mediator (M), [Cp*Rh(phen)H2O]2+, (Cp* = 5-C5Me5, phen = 1,10-phenanthroline) was synthesized as follows. Briefly, 103.01 mg of dichloro (pentamethylcyclopentadienyl) rhodium(III) dimer was added to 10 mL of methylene chloride, where the solid was insoluble. Then, 60.07 mg of 1,10-phenanthroline was added to the mixture. After stirring at room temperature for 3 h, the color of the solution changed from dark orange to orange. After removing the solvent by evaporation under reduced pressure, M was obtained.
WS2/g-C3N4 composites were synthesized via a two-step self-assembly procedure. Herein, 100 mg of g-C3N4 was added into 100 mL deionized water and sonicated for one hour. Into the above suspension, definite amount of WS2 powder was added to obtain a WS2 mass fraction of 1, 5, 10%. The suspension mixture was sonicated for 30 min followed by 36 h mechanical stirring. To consolidate the heterojunction interface in the WS2/g-C3N4 composites, the mixture was sealed into a 100 mL Teflon-lined stainless steel autoclave and heated to 140 °C for 6 h. After cooling down to room temperature and evaporating the solvent, WS2/g-C3N4 composites with different composition proportions were obtained.
XRD were adopted to analyze the composition and structure of as-prepared WS2/g-C3N4 composites. To understand the crystallization of the composite and also mutual interface of each semiconductor over the other during composite formation, the XRD patterns of the following materials were presented in Fig. 3a, which include the obtained WS2, hydrothermally treated WS2 (referred as HT WS2) and ultrasonicated WS2 (referred as US WS2) in absence of g-C3N4; as formed g-C3N4; ultrasonicated 5% WS2/g-C3N4 composite (US 5% WS2/g-C3N4), hydrothermally treated (HT 5% WS2/g-C3N4), as well as the 5% WS2/g-C3N4 composites fabricated through combined ultrasonication-hydrothermal treatments. As shown in Fig. 3a, the XRD pattern of obtained g-C3N4 showed the typical diffraction peaks at 13.1° and 27.3°, perfectly indexed as the (100) and (002) planes, respectively, which were ascribed to in-planar tri-s-triazine unit and the interplanar stacking of aromatic systems.17,40–44 The XRD patterns of the obtained WS2 exhibit many distinct diffraction peaks, indicating its hexagonal structure,28,34 which is consistent with the 2H configuration in the standard card library. The HT WS2 and US WS2 presents the same XRD as that of the obtained WS2, indicating the crystallization of WS2 was not affected by ultrasonication and hydrothermal treatments. For the 5% WS2/g-C3N4 composites, the XRD patterns of all the three composites display the combination of the two sets of diffraction data for both g-C3N4 and WS2 and no other phase is detected, implying that WS2 was not incorporated into the lattice of g-C3N4.
Fig. 3 (a) XRD patterns and (b) FT-IR spectra of obtained g-C3N4, WS2, WS2/g-C3N4 composites; (c) local magnification of the FT-IR spectra at around 810 cm−1 of spectra in (b). |
The FT-IR was also adopted to test the obtained g-C3N4, WS2, and WS2/g-C3N4 composite. As shown in Fig. 3b, pure g-C3N4 has a much stronger IR response than WS2, and the addition of WS2 shows no obvious effect on the IR spectrum of g-C3N4. For the g-C3N4, the strong bands in the region of 1200–1700 cm−1 are assigned to the typical stretching vibration modes of C–N heterocycles. The peaks at 3000–3700 cm−1 represent the N–H and O–H stretching vibration. The sharp peak at 810 cm−1 originates from the characteristic breathing mode of tri-s-triazine units.45–49 For the WS2/g-C3N4 composites, the overall patterns of the spectra are the same as the g-C3N4, confirming the existence of heptazine heterocyclic rings in WS2/g-C3N4 composites. In generally, there is no obvious difference from the FTIR spectrogram before and after doping, but it's not difficult for us to see that the position of the characteristic peak from the tri-s-triazine vibration of g-C3N4 has a certain degree of shift (Fig. 3c), indicating that there might be some interactions between the “nitrogen pots” of g-C3N4 and W species of WS2.24 As a complement to FT-IR, the Raman spectra of the g-C3N4 and the 5% WS2/g-C3N4 were also recorded. As shown in Fig. S1,† the catalysts show several very weak distinctive peaks at 458, 679 and 1220 cm−1, which is basically consistent with the situation of g-C3N4 reported in the literatures.50,51 The formation of 5% WS2/g-C3N4 composite did not lead to apparent new peak, which may be due to the strong photoluminescence effect of g-C3N4 and the small faction of WS2 in the composite.
X-ray photoelectron spectroscopy (XPS) analysis was employed to determine the chemical composition and bonding configuration of the g-C3N4, WS2 and the WS2/g-C3N4 composites (Fig. 4a), with the high-resolution spectrum of each sample were illustrated in Fig. 4b–d. The survey XPS spectra shown in Fig. 4a indicate that the prepared WS2/g-C3N4 samples are composed of C, N, W and S. Specifically, the C1s spectrum (Fig. 4d1) of WS2/g-C3N4 composites show there are two C1s peaks located at 284.7 and 288.2 eV, the former is ascribed to the adventitious hydrocarbon from the XPS instrument, while the latter is assigned to sp2-bonded carbon atom (N–CN) of g-C3N4 in aromatic rings. The high-resolution N1s spectrum of the WS2/g-C3N4 composites could be fitted into four peaks (Fig. 4d2). The peaks centered at 398.7 and 399.5 eV were attributed to sp2-hybridized nitrogen atom (CN–C group) and tertiary nitrogen (N–C3 group or H–N–C2), respectively; the peaks at 401.0 and 404.7 eV derived from amino function groups and charging effect localization in heterocycles, respectively.4,24,52 As compared with the C1s and N1s spectrum (Fig. 4b1 and b2) of pure g-C3N4, all those peaks of the WS2/g-C3N4 composites shifted to a position with a higher binding energy.
Fig. 4d3 and d4 display the S2p spectra and the W4f spectra of the WS2/g-C3N4 composites. The peaks at 161.7 and 163 eV can be ascribed to the S2− species, donated as S2p3/2 and S2p1/2, respectively;34 the W4f peaks at 32.1, 34.4, and 37.6 eV can be ascribed to the W4+ species, donated as W4f7/2, W4f5/2 and W5p3/2.28,53 In contrast to the W4f and S2p spectrum (Fig. 4c1 and c2) of WS2, all these above peaks of the WS2 shifted to a position with a lower binding energy after coupling with g-C3N4. Thus, the C1s and N1s peaks of g-C3N4 shifted toward the higher binding energy, while the W4f and S2p peaks of WS2 shifts towards the lower binding energy. It was suggested that there might be some S–C chemical bonds formed between the heterojunction interfaces of WS2/g-C3N4 composites, thus electron transfer could occur from g-C3N4 to WS2 at this interfaces due to their different electron concentration.24,54
The optical properties of WS2, g-C3N4 and the WS2/g-C3N4 composites were revealed by the UV-vis diffuse reflectance spectra (DRS). As shown in Fig. 5a, pure g-C3N4 had absorption from UV to visible region, with an absorption edge at 460 nm, which corresponding to a band gap about 2.7 eV according to the Kubelka–Munk conversion (Fig. 5b).55,56 However, with the coupling of WS2, the absorption range of the composite became wider than that of pure g-C3N4, a remarkable enhanced light-harvesting ability is observed for the WS2/g-C3N4, and the band gap width estimated from the K–M equation became narrower accordingly, which implied that the light absorption ability of the WS2/g-C3N4 composites became stronger. The coupling of WS2 on g-C3N4 may generate an impurity energy level in the valence band (VB) and narrow the band gap. The defect energy levels increased the light absorption efficiency of the materials and thus may exhibit photocatalytic performance superior to that of the individual material. In addition, the DRS spectra of US 5% WS2/g-C3N4 and HT 5% WS2/g-C3N4 composites were also measured and compared with that of the 5% WS2/g-C3N4, it is indicated that the omitting the ultrasonication or hydrothermal treatments during composite formation lead to negligible changes in the band structure (Fig. S2†).
Fig. 6 presents the BET surface areas measurement of 5 wt% WS2/g-C3N4 composites. For comparison, the surface areas of g-C3N4 and the physical mixture of g-C3N4 with 5 wt% WS2 (referred as PM-WS2/g-C3N4 in the following text) were also determined, the results were listed in Table S2.† The specific surface area of g-C3N4 was 7.34 m2 g−1, which is similar to the value reported by He et al.,24 but lower than those reported for most g-C3N4 nanosheets,54,57 which indicates that the g-C3N4 has multi-layered structure. Slight decrease in surface area was observed for the PM-WS2/g-C3N4 (6.87 m2 g−1); while the 5 wt% WS2/g-C3N4 composites exhibited much higher BET values (12.22 m2 g−1), which indicated that some reactions might have occurred between g-C3N4 and WS2 during recombination. This larger specific surface area of WS2/g-C3N4 composites also could supply more reactive sites for light and substrates, improve the whole efficiency of the reaction. It should be noted that the specific surface area of the 5 wt% WS2/g-C3N4 composites are still far lower than the g-C3N4 nanosheets, indicating the ultrasonication and hydrothermal treatments during composite formation still could not result in effective exfoliation of the g-C3N4. After BJH (Barrett–Joyner–Halenda) plotting, the pore size distribution of each samples were analyzed (Fig. 6b). Compared with the pure g-C3N4, coupling of WS2 lead to slight decrease in pore diameter.
Fig. 6 (a) The N2 adsorption/desorption isotherms, (b) the corresponding pore-size distribution. BET surface area was measured by nitrogen sorption isotherms at 77.5 K and up to 1.03 bar. |
Based on the above photochemical investigations of the g-C3N4 and the WS2/g-C3N4 composites, their performance for visible light-driven photocatalytic NADH regeneration were examined. The reactant solution consisted of 15 wt% TEOA, 0.25 mM electron mediator M, and NAD+ with an initial concentration of 1 mM and an active g-C3N4 content of 1 mg mL−1 was maintained in all the experiments. The photocatalytic activity comparison among pure g-C3N4, WS2, PM-WS2/g-C3N4 and WS2/g-C3N4 composite with WS2 content of 1%, 5% and 10% are presented in Fig. 7a. The monolithic g-C3N4 and WS2 had rather low catalytic efficiency, NADH regeneration yield at 6 h was below 10%. By physically mixing 5 wt% WS2 with g-C3N4, the NADH photo-regeneration yield enhanced to 15%. While the 5 wt% WS2/g-C3N4 composite presents the best performance, a NADH yield of 37.1% was achieved, which were about four times of those obtained by using monolithic g-C3N4 and WS2. With further increasing the WS2 content in the composite to 10 wt%, however, leading to decrement in activity for the photo-regeneration of NADH. Presumably, coupling of high amount WS2 may lead to shielding of active site of g-C3N4 by WS2 or loss of favorable interfaces between g-C3N4 and WS2. Similar phenomenon was also observed on the activity of mesoporous graphitic carbon nitride (mpg-CN) loaded with WS2 towards H2 generation. About 0.3 at% WS2 loading amount was found optimal to reach highest rate of hydrogen evolution, and heavy loading of WS2 led to decrease in activity of the heterojunctions photocatalyst.29
To justify the necessity of multiplicative steps involving ultrasonication, mechanical stirring and hydrothermal treatment for the preparation of WS2/g-C3N4, a series of WS2/g-C3N4 composites were prepared by simpler steps and evaluated for its activity towards NADH photoregeneration. Results presented in Fig. S3 and Table S3† clearly indicated that either omitting of the ultrasonication or hydrothermal treatments, or even the mechanical stirring between these two operations during composite formation, led to significantly lower activity of the fabricated WS2/g-C3N4. The hydrothermal time and temperature did not show remarkable influence on the activity of the composite photocatalyst. Therefore, the two-step sonication and subsequent hydrothermal treatments are necessary, though somewhat tedious, to ensure the photocatalyst a high activity of the 5 wt% WS2/g-C3N4 composite, which presents the highest NADH photo regeneration yield of 37.1%. It was believed that the first step of sonication was to ensure a good dispersion of g-C3N4 particles, the second step of sonication of g-C3N4 and WS2 mixture was for a full contact between these two materials, which was crucial for the subsequent hydrothermal reaction.
In another set of experiment, we tried to address the more challenging question of a potential mediator-free regeneration of NADH. To our surprise, the mediator-free with system with 5 wt% WS2/g-C3N4 composite as photocatalyst was also possible, though the regeneration yield at 6 h was only about half of that obtained in presence of M (Fig. S3, Table S3†). This can be explained from the following two points. Firstly, a mixture of 1,4-NADH and 1,6-NADH would possibly formed, while in presence of M, 1,4-NADH will be unique production; secondly, without a strong redox agent, i.e., mediator, g-C3N4 also catalyzes the back reaction, meaning an equilibrium between NAD+ and NADH.18
We then evaluated the WS2/g-C3N4 composite as a photocatalyst of the artificial photosynthesis system for bioconversion of CO2 to methanol. As expected, the photocatalysts showed higher activity for NADH regeneration also exhibited higher efficiency for methanol synthesis from CO2, when the NADH photoregeneration process was coupled with the biocatalytic process. The highest methanol concentration up to 5.58 mM were obtained by using 5 wt% WS2/g-C3N4 composite as photocatalysts, corresponding to a methanol productivity of 372.1 μmol h−1 gcat−1, which was about 7.5 times higher than that obtained by using g-C3N4 (50.31 μmol h−1 gcat−1). This result clearly indicated that the formation of WS2/g-C3N4 heterojunction generated significant photo-synergistic effect and played key roles in the enhancement in the photocatalytic activity.
In general, some reactive oxygen species including hydroxyl radicals (˙OH) and superoxide radicals (˙O2−), as well as holes (h+) are expected to be involved in the photocatalytic process of RhB degradation.55,58 To investigate the role of these reactive species, the effects of some radical scavengers and N2 purging on the photodegradation of RhB were studied to propose the possible photocatalytic mechanism. Results in Fig. 8c indicate that the addition of IPA (˙OH scavengers) had almost no effect on RhB degradation. While addition of TEOA (h+ scavengers) and KI (scavenger of both ˙OH and h+) led the degradation rate after 1 h's irradiation decreased to about 70% and 58%, respectively. When N2 purging was conducted which acts as ˙O2− scavenger, the degradation rate decreased dramatically to about only 22%. These results suggested that the ˙O2− plays major roles in the photodegradation of RhB catalyzed by the WS2/g-C3N4 heterojunction photocatalyst, which is consistent with results in other reports.55,58
Reusability of photocatalyst is a very important parameter from an economical viewpoint. The reusability and stability of the 5 wt% WS2/g-C3N4 composites was examined by measuring the RhB degradation during repeated usages. As shown in Fig. 8d, after five successive runs, there is no remarkable decrease in its activity. Hence, the photocatalyst has a good stability during the photocatalytic reactions.
To further demonstrate the photoinduced electron-transfer mechanism, as well as elucidate the effect of amount of WS2 in WS2/g-C3N4 heterojunction on the overall reaction efficiency, detailed investigations of the photochemical properties were performed on WS2/g-C3N4 heterojunction hybridized with different amount of WS2 ranging from 1 wt% to 10 wt%. For most semiconductors, photogenerated electrons and holes can bind after the excitation by incident light, leading to the transfer of partial energy to fluorescence. In general, the binding efficiency and photoelectron lifetime can be measured by monitoring fluorescence intensity and lifetime.17,57,59,60 Fig. 10a presents the fluorescence spectrum of pure g-C3N4, which shows strong fluorescence intensity at 437 nm. However, the physical mixing WS2 and g-C3N4 (PM-WS2/g-C3N4) and the WS2/g-C3N4 heterojunction all show a decremental effect on the fluorescence spectra. More interesting, the WS2/g-C3N4 heterojunction with 5 wt% WS2 presents the lowest fluorescence intensity, which means more electrons on the CB of g-C3N4 transfer to WS2 instead of recombining with the holes in the VB of g-C3N4. The suppressed recombination of electron–hole pairs of g-C3N4 may attribute to the fast electron transfer from CB of g-C3N4 to the CB of WS2, which also demonstrate the electron transfer mechanism and explain the highest activity of 5 wt% WS2/g-C3N4 heterojunction.
Fig. 10 (a) PL spectra of g-C3N4, WS2 and WS2/g-C3N4 composite photocatalysts. (b) Excited state electron radioactive decay of g-C3N4, WS2 and WS2/g-C3N4 composite. |
In order to confirm the suppressed recombination of electron–hole pairs in 5 wt% WS2/g-C3N4 heterojunction, time-resolved fluorescence decay analysis was carried out. The excited state electron radioactive decay lifetime (Fig. 10b) show that the 5 wt% WS2/g-C3N4 heterojunction owns the longest fluorescence lifetime (11.080 ns) compared with that of 10 wt% WS2/g-C3N4 (10.549 ns), 1 wt% WS2/g-C3N4 (10.368 ns), PM-WS2/g-C3N4 (10.554 ns), and g-C3N4 (10.487 ns), indicating that the incorporation of WS2 increased the photoelectron lifetime of WS2/g-C3N4. This result further certified that 5 wt% WS2/g-C3N4 heterojunction has the best coordination between g-C3N4 and WS2 for the most efficient and fastest photo-excited electrons transfer.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8ra02807a |
This journal is © The Royal Society of Chemistry 2018 |