Facile Synthesis of Carbon Dots@2D MoS2 Heterostructure with

24 mins ago - Synopsis. CDs@2D MoS2 heterostructure is first constructed by a facile sonication−hydrothermal method. Such heterostructure regulates ...
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Article Cite This: Inorg. Chem. XXXX, XXX, XXX−XXX

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Facile Synthesis of Carbon Dots@2D MoS2 Heterostructure with Enhanced Photocatalytic Properties Ning Li,*,†,‡ Zhengtang Liu,‡ Ming Liu,† Chaorui Xue,† Qing Chang,*,† Huiqi Wang,† Ying Li,†,§ Zhenchao Song,† and Shengliang Hu*,† †

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School of Energy and Power Engineering & School of Material Science and Engineering, North University of China, Taiyuan 030051, P. R. China ‡ State Key Lab of Solidification Processing, Northwestern Polytechnical University, Xi’an 710072, P. R. China § CAS Key Laboratory of Carbon Materials, Institute of Coal Chemistry, Chinese Academy of Sciences, Taiyuan 030001, P. R. China S Supporting Information *

ABSTRACT: To better utilize carbon dots (CDs) as efficient photocatalysts, an excellent strategy of constructing CDs@ MoS2 heterostructure is presented. Here a facile sonication− hydrothermal method is utilized to synthesize CDs@MoS2. Such heterostructure regulates the energy level configuration, and visible light absorption and the separation and transfer of photogenerated charges are enhanced remarkably, which is propitious for the production of more photoinduced charges and improvement of the heterogeneous photocatalytic activity. Meanwhile, the photocatalytic performance of CDs@MoS2 was obviously improved in methylene blue degradation. On the basis of a series of contrast experiments, the possible mechanism of the photocatalytic reaction is proposed. Therefore, this work offers a facile route for the design of a zero-dimensional/twodimensional heterojunction for the adjustment of the energy level structure and the improvement in photocatalytic performance.

1. INTRODUCTION Carbon dots (CDs), due to their photoluminescence, photostability, biocompatibility, nontoxicity, low cost, and potential to capture, transfer, and convert light energy, have attracted a tremendous amount of attention in the fields of fluorescence imaging, sensing, and solar-to-energy conversion.1−13 For one thing, as we know, CDs typically exhibit strong optical absorption in the ultraviolet (UV) region (230−360 nm) with a tail extending into the visible range,14 yet UV light is only 5% of the whole solar spectrum, which restricts the photoabsorption and the amount of photoinduced charge.15 For another, highly efficient charge transfer is fundamental for photocatalytic solar-to-energy conversion. Nevertheless, there are plenty of recombination centers that work against the separation and transfer of the photogenerated charge.9,14 In view of these issues, many methods have been adopted to enhance the visible light absorption and charge transfer efficiency of CDs such as the creation of unique surface states, doping with heteroatoms, construction of heterostructure, etc.1,16−18 As part of these efforts, heterostructure not only can manipulate the absorption of sunlight together with the valence and conduction band positions but also possesses unique interfacial properties for the separation and transfer of photoinduced charges.4,12,19,20 For instance, Kang et al.4 fabricated the CDs-C3N4 composite. The optical properties, valence, and conduction band energies of this composite change, which is beneficial for the improvement of the light © XXXX American Chemical Society

absorbance and photocatalytic efficiency. Moreover, intimate interfacial contact in the layer-by-layer structure of CD-CdS quantum dot heterojunction films facilitates efficient photoinduced charge separation.19 By now, many CD-based heterostructures and hybrid systems such as TiO2, Ag3PO4, ZnFeO4, Fe2O3, C3N4, Bi2WO6, BiOCl, etc., have been designed.1,4,21−24 However, CDs act only as decorated accessories in these composites to heighten the photocatalytic activity of the other compound, which runs counter to the expectation of utilizing CDs adequately. Therefore, how to better utilize and design CDs in the heterostructure is still challenging. Two-dimensional (2D) transition metal dichalcogenides (TMDs) have advantages in terms of their large specific surface area, strong visible light absorption, high-edge active sites, and short migration distance of the photogenerated charge carrier, which can be used to form heterostructures (or composites) by combining with a metal or semiconductor to improve the photocatalytic activity.25−28 Consequently, 2D MoS2 does become the promotor of the CD-based hybridization. For example, Atkin et al.29 synthesized the 2D WS2/CDs hybrids by a two-step method of exfoliation followed by microwave irradiation. These hybrids have enhanced photocatalytic activity for Congo red (CR) dye. Moreover, Fang et al.30 Received: January 13, 2019

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DOI: 10.1021/acs.inorgchem.9b00111 Inorg. Chem. XXXX, XXX, XXX−XXX

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Inorganic Chemistry

electrode was Pt foil, the reference electrode was the Ag/AgCl reference electrode, and the working electrode was the prepared sample. The working electrodes were prepared by overlaying a slurry of the sample in ethanol onto an indium tin oxide (ITO) glass electrode, and then they were dried under vacuum at 80 °C for 2 h. The electrolyte solution was 0.5 M Na2SO4. Linear potential scans were performed at a rate of 5 mV s−1 within a given potential window. All of the electrochemical measurements were carried out on the BioLogic (SP 120) electrochemical workstation. 2.4. Photocatalysis Experiments. First, a 0.01 mg/mL methylene blue (MB) solution was prepared. Then, 2 mL of the sample (CDs or CDs@MoS2 sample) was added to 25 mL of MB and ceaselessly stirred for 1 h in the dark to establish an adsorption− desorption equilibrium. The solution was irradiated for 5 min with a 300 W xenon lamp placed 30 cm away (wavelengths of 90% (Figure S5a), indicating that the CDs@MoS2 sample remains photocatalytic and stable. As shown in Figures 1−3 and Figure S5b−g, the position and intensity of the (002) preferential peak, the binding energies of Mo 3d and S 2p, and the morphology of the CDs@MoS2 sample were almost the same before and after the photocatalytic experiments. Thus, the stability of CDs@MoS2 could be further validated through the XRD, TEM, and XPS results. In addition, PL spectra of the CDs, CDs@MoS2, and 2D MoS2 were measured. As one can see, an overt emission maximum at ∼415 nm is observed when CDs are excited at 340 nm (Figure S6a). However, the intensity of the emission peak maximum (∼413 nm) decreases significantly (Figure S6b) after combination with 2D MoS2 [the PL peak of the 2D MoS2 sample is extremely low (Figure S6c)], suggesting that the intimate interaction between CDs and 2D MoS2 promotes the effective separation and transfer of the photoinduced electron−hole and inhibits the recombination. This is an indirect explanation for the increment in the photocatalytic efficiency of CDs@MoS2. To thoroughly understand the behaviors of photogenerated charges and the oxidation mechanism, the band alignment [the conduction band minimum (CBM) and the valence band maximum (VBM) levels] and electrochemical property are estimated through linear potential scans and electrochemical impedance spectroscopy (EIS).6−8,45 Panels a and b, c and d, and e and f of Figure 5 show the cathodic and anodic scan results of 2D MoS2, CDs, and CDs@MoS2, respectively. The CBM and VBM values of these three samples are approximately −0.28 and 1.31 V, −1.57 and 0.94 V, and −0.56 and 1.01 V (vs Ag/AgCl), respectively, which are

Figure 5. Cathodic and anodic scans of (a and b) 2D MoS2, (c and d) CDs, and (e and f) CDs@MoS2, respectively. (g) Schematic energy level diagram of the three prepared samples. (h) EIS Nyquist plots of CDs and CDs@MoS2.

equivalent to −0.08 and 1.51 V, −1.37 and 1.14 V, −0.36 and 1.21 V (vs NHE), respectively. The energy gaps of the three samples determined from the potential scan are 1.59, 2.51, and 1.57 eV, respectively. In succession, we plot the schematic energy level diagram of 2D MoS2, CDs, and CDs@MoS2 (Figure 5g). This plot clearly shows that the energy level configuration has been regulated and a typical type II band alignment1,30,42,46−48 is formed between 2D MoS2 and CDs, which facilitates the transfer of photoexcited holes from MoS2 to CDs and photogenerated electrons from CDs to MoS2, resulting in an effective oxidation ability under visible light irradiation. Furthermore, EIS measurements were carried out to further investigate the separation efficiency of the charge carriers. The arc radius on the EIS Nyquist plot of CDs@MoS2 is smaller than that of CDs (Figure 5h), illustrating that the former sample has the lower interfacial charge transfer resistance and subsequently causes the effective separation of photogenerated electron−hole pairs.6−8,45,49 A reasonably theoretical simulation based on density functional theory can study the nature of the material properties and demonstrate experimental results. The just reported work50 can be the auxiliary support for the experimental results of energy level configuration and charge transfer. D

DOI: 10.1021/acs.inorgchem.9b00111 Inorg. Chem. XXXX, XXX, XXX−XXX

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Inorganic Chemistry

can see that the photocatalytic activities are restrained most seriously by the BQ, suggesting that •O2− plays the most important role in photodegradation. Meanwhile, the active species h+ and •OH are also responsible for the final breakdown of the MB. Therefore, MB molecules are degraded by •O2−, •OH, and h+.22,35,47,51−53,55 On the basis of the analysis presented above, the photocatalytic activities of CDs@MoS2 can be significantly enhanced. The modulation of the valence band-edge position (from −0.08 to −0.36 eV vs NHE) enhances the ability to produce •O2− compared with that of 2D MoS2, and the increment in the absorption, separation, and transfer of photoinduced charges boosts the effective MB degradation in contrast to that of CDs. Therefore, we can conclude that the construction of the CDs@MoS2 heterostructure is propitious for the improvement of solar energy absorption and conversion.

From the analysis presented above, the possible degradation mechanism is shown in Figure 5g. First, samples of CDs, 2D MoS2, and CD@MoS2 could be excited, and simultaneously, the holes (h+) and electrons (e−) were produced under visible light irradiation (λ > 420 nm). However, the abilities of photoinduced e−−h+ pairs are different due to the absorption capacity. The better the absorption ability, the more the photoinduced charges produce. Then, the photogenerated electrons would participate in the following reaction:51,52 O2 + e− → •O2− •

O2− + 2H 2O + 2e− → 3OH− + •OH

(1) (2)

In view of the CBM values of 2D MoS2, CDs, and CDs@ MoS2 (−0.08, −1.37, and −0.36 V vs NHE, respectively), the photogenerated electrons reacted with absorbed O2 on the surface of photocatalysts to form •O2− (O2/•O2−, −0.046 eV vs NHE24). Due to the lower reduction potential of 2D MoS2 and the worse visible absorption of CDs, the capacities of reducing dissolved O2 are both poor. For CDs@MoS2, the separation and transfer of photoinduced charges promote the generation of enough •O2− radicals. To quantify the amount of formed •O2−, the nitro blue tetrazolium (NBT) was used as a probe for •O2− on the basis of the formation of the insoluble formazan dye.53,54 As displayed in panels a and b of Figure S7, the absorption bulge at ∼650 nm refers to the characteristic peak of formazan. When the CDs@MoS2 sample was added to the NBT/NaOH mixture, the adsorption intensity of formazan increased more evidently than those of the CD sample and 2D MoS2, indicating the more beneficial effect of CDs@MoS2 in the generation of •O2−. In addition, •O2− radicals of the three kinds of samples could react with H2O and e− to generate strongly oxidative •OH (•O2−/•OH, 0.9 V vs NHE52). The presence of •OH radicals can be determined by terephthalic acid (TA). After reaction, TA transforms to 2-hydroxyterephthalic acid (TAOH), which emits fluorescence at 426 nm.51 Panels c and d of Figure S7 illustrate the fluorescence spectra of the TA solution irradiated at different times after the addition of samples of CDs, CDs@MoS2, and 2D MoS2. The fluorescence intensity of 426 nm generated from CDs@MoS2 is much stronger than those of the CDs and 2D MoS2. To detect the main active species formed in the CDs@MoS2 samples and comprehend the degradation mechanism, a series of trapping experiments were performed by utilizing different scavengers in the photodegradation process: IPA for •OH, TEOA for h+, and BQ for •O2−.32,55 As shown in Figure 6, one

4. CONCLUSION In summary, we present a facile sonication−hydrothermal method for synthesizing CDs@MoS2 heterostructure. The results show that CDs loaded onto the 2D MoS2 not only can extend and enhance visible light absorption but also can produce higher separation and transfer efficiency of photoinduced charges compared with that of pure CDs. The linear potential scans illustrate that a staggered type II band alignment is formed near the CDs 2D MoS2 interface, and we know that electrons are transferred from the conduction band minimum of CDs to that of 2D MoS2. As a consequence, the proper band-edge positions of CDs@MoS2 are conducive to the production of adequate active radicals to participate in degradation. Meanwhile, the possible mechanism of the photocatalytic reaction is proposed. Finally, we can conclude that the construction of the CDs@MoS2 heterostructure enhances the solar energy absorption and conversion on the basis of this work.



ASSOCIATED CONTENT

S Supporting Information *

The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acs.inorgchem.9b00111.



XRD patterns of MoS2 powder, TEM image of CDs@ MoS2, size distribution of CDs, dark adsorption curve, degradation rates, recycling experiments, XRD, XPS, and TEM images of the CDs@MoS2 sample after photodegradation, PL spectra, and quantification of active species (PDF)

AUTHOR INFORMATION

Corresponding Authors

*E-mail: [email protected]. *E-mail: [email protected]. *E-mail: [email protected]. ORCID

Ning Li: 0000-0002-4046-4825 Huiqi Wang: 0000-0003-1232-7572 Shengliang Hu: 0000-0002-2838-4072 Notes

Figure 6. Trapping of active species during the photocatalytic degradation of MB: IPA for •OH, TEOA for h+, and BQ for •O2−.

The authors declare no competing financial interest. E

DOI: 10.1021/acs.inorgchem.9b00111 Inorg. Chem. XXXX, XXX, XXX−XXX

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ACKNOWLEDGMENTS This work was financially supported by the National Natural Science Foundation of China (U1510125, 51272301, 51502270, and 21703209) and the fund of the State Key Laboratory of Solidification Processing in NWPU (SKLSP201719). The authors also appreciate the financial support by the Shanxi Province Science Foundation (201601D021059), Key Research and Development (R&D) Projects of Shanxi Province (201803D121037 and 201803D421091), the Shanxi Province Science Foundation for Youths (201701D221087, 201701D221085, and 201801D221085), the Specialized Research Fund for Sanjin Scholars Program of Shanxi Province, the Program for the Outstanding Innovative Teams of Higher Learning Institutions of Shanxi, the Fund of CAS Key Laboratory of Carbon Materials (KLCMKFJJ1709), the North University of China Fund for Distinguished Young Scholars, and “333” talent project research. This work was part of the Ph.D. degree of Jin (2017) and North University of China Fund for Scientific Innovation Team.



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DOI: 10.1021/acs.inorgchem.9b00111 Inorg. Chem. XXXX, XXX, XXX−XXX