Mingcai Yin*,
Chaojun Wu,
Fangfang Jia,
Lijiao Wang,
Pengfei Zheng and
Yaoting Fan
College of Chemistry and Molecular Engineering, Zhengzhou University, No. 100 of Science Road, Zhengzhou, 450001, P. R. China. E-mail: mcyin@zzu.edu.cn; Fax: +86 371 67766017; Tel: +86 371 67766017
First published on 4th August 2016
MoS2 is considered as a promising alternative to noble metals for H2 evolution. In this work, a MoS2 catalyst was synthesized via a simple and feasible solvothermal process and characterized by XRD, SEM, TEM and XPS techniques. Though the thus-obtained MoS2 was stabilizing agent-free and composed of relatively large agglomerated particles, it shows superior hydrogen production performance under sensitization of eosin Y (EY), significantly different form earlier reports. Under optimized conditions, the hydrogen production rate was high, up to 35 mmol h−1 g−1, much higher than those of previous reports. We attribute this to its relatively high surface roughness and the small thin petal-like nanosheets constituting the MoS2, which result in more active sites for hydrogen evolution. Meanwhile, the obtained MoS2 shows excellent photostability with the H2-evolving activity remaining nearly unchanged after 4 cycles.
18 have gained great interest due to their low cost and better photostability than the above-mentioned biomimetic catalysts.
Molybdenum disulfide (MoS2), acting as a high-performance commercial dehydrosulfurization catalyst,19 has also been exploited in electrochemical and photochemical hydrogen production processes and much progress has been made in recent years.20–26 Although MoS2 itself does not possess photocatalytic H2 generation activity, it has been proven to be an efficient HER catalyst when combined with a semiconductor or photosensitizer. Heretofore, much research has been focused on hydrogen evolution of MoS2 loaded on different supports, such as CdS, TiO2, ZnS and graphene (G).27–32 For example, eosin Y (EY)-sensitized MoS2/RGO (RGO = reduced graphene oxide) showed a hydrogen evolution rate of 88.5 μmol h−1 in 80 mL of 15% (v/v) TEOA aqueous solution (pH = 9.0) under visible light irradiation (λ ≥ 420 nm) with 0.4 mM EY and 20 mg catalyst.33 Furthermore, as far as we know, for the above MoS2-based photocatalytic hydrogen production systems, the highest H2 evolution activity was 9.0 mmol h−1 g−1 over 2.0 wt% MoS2/G-CdS composite.30
In contrast, investigations on employing unsupported MoS2 as H2-evolving catalyst in photochemical systems are rare. In 2009, Zong et al. discussed the hydrogen evolution activity of poly(vinyl pyrrolidone) (PVP)-stabilized colloidal MoS2 nanoparticles (NPs). In a 2
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1 acetonitrile–methanol solution (150 mL), about 900 μmol of H2 was generated within 6 h under visible light irradiation when 12.5 μmol MoS2 and 20 μmol [Ru(bpy)3]2+ were used as catalyst and sensitizer, respectively.34 In addition, in 2014, Yuan et al. also investigated the hydrogen production activity of PVP-stabilized colloidal MoS2 NPs in a 1
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1 methanol–water solution (100 mL) when a series of cyclometalated Ir(III) complexes were used as sensitizers. About 1923 μmol H2 was evolved after 20 h with 100 μM MoS2 and 100 μM sensitizer.35 However, for these two homogeneous systems,34,35 several important points are worth noting. First, similar to previous results,22,23 only “soluble” colloidal MoS2 NPs demonstrated unique catalytic activities, bulk MoS2 did not exhibit any photocatalytic activity. Second, the MoS2 used in the above two systems were both stabilized by PVP and the uncapped large MoS2 clusters (8–10 nm) had no H2-evolving activity at all. Third, not only the above two hydrogen production reactions were conducted in organic solvents, but also the sensitizers were both noble metal complexes.
Besides the above problems, for the synthesis of MoS2, though various methods including ultrahigh-vacuum processing, high-temperature treatment,22 sulfidization using H2S gas,36 electrodeposition37 and photodeposition38 have been developed, it is still a challenge to achieve highly efficient MoS2 catalyst through a relatively facile, environmentally friendly and scalable method. Then in recent years, much research has been focused on the synthesis of MoS2 via simple and feasible hydro(solvo)thermal method.28,30,31,33–35,39 However, more research is necessary because it is well-known that the property of a material is related to its structure, and likewise, the structure is related to the synthetic procedure and parameters, such as the kind and molar ratio of raw materials, the reaction temperature and time, and the solvents, etc.
Bear all above points in mind, in this paper, a MoS2 catalyst was successfully prepared by the solvothermal method and its hydrogen production performance was evaluated in a noble-metal-free aqueous solution using readily accessible and cheap organic dye, EY as sensitizer. The key factors affecting its hydrogen production activity and the photostability of the obtained MoS2 were investigated in detail. Surprisingly, the results demonstrated that the thus-prepared MoS2 exhibits superior H2-evolving activity and excellent photostability, though it is uncapped and composed of agglomerates up to 1 μm in diameter.
The MoS2 catalyst was synthesized by a solvothermal reaction of Na2MoO4·2H2O and KSCN in a 1
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1 (v/v) DMF/H2O. For a typical synthesis, 1.0 mmol Na2MoO4·2H2O and 3.0 mmol KSCN were dissolved in 60 mL DMF/H2O under continuous stirring, and the pH value of the reaction system was adjusted to 1–2 by 1
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1 HCl. Then the reaction mixture was stirred at room temperature for 2 h before transferred into a 100 mL Teflon-lined autoclave. After heated in an oven at 220 °C for 20 h, a black product was obtained through centrifugation, washing thoroughly with water and anhydrous ethanol, and drying overnight in a vacuum oven at 60 °C.
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1 HCl. Prior to irradiation, the suspension was thoroughly degassed by bubbling nitrogen gas for 20 min to remove the dissolved oxygen. During the whole reaction, a continuous magnetic stirring was used to maintain the homogeneity of the reaction mixture and a water circulation system was used to keep the temperature at about 25 °C. The H2 evolved was measured by a gas chromatograph (GC, Agilent 4890D) equipped with a thermal conductivity detector (TCD) and a porapak Q stainless column. Nitrogen was served as the carrier gas at a flow rate of 20 mL min−1. All of the H2 evolution experiments were repeated three times for reliability of the results (±standard deviation).
| KSCN + 2H2O + HCl = NH3 + H2S + CO2 + KCl | (1) |
| 4Na2MoO4 + 9H2S = 4MoS2 + Na2SO4 + 6NaOH + 6H2O | (2) |
To reveal the surface morphology of the prepared MoS2, SEM measurements were performed at different magnifications. A general view (Fig. 2a) shows that the MoS2 sample displays a nonuniform morphology, which is composed of agglomerated particles with the size ranging from about 100 nm to 1 μm. Higher magnified SEM images (Fig. 2b and c) reveal that these agglomerates are constituted by small NPs of about 10–30 nm in diameter with nonuniform shape and size and their surfaces are quite rough. Simultaneously, we tried our best to characterize the microstructure and morphology of the MoS2 sample by TEM technique. From the TEM and HRTEM images (Fig. 2d–f), on one hand, it can be seen that almost similar to the SEM results, the as-prepared MoS2 is composed of irregularly shaped NPs (around 10–50 nm in diameter). However, the small NPs agglomerate together to form larger clusters. In other words, serious aggregation occurs, which results in a relatively bad dispersion of the sample in the TEM determination. On the other hand, from the HRTEM image (Fig. 2f), lots of short and disordered lattice fringes with a spacing of around 0.66 nm corresponding to (002) plane of hexagonal-phase MoS2 can be observed, which indicate that the obtained MoS2 is layered structure. Then combining TEM results with the above SEM ones, we can infer that the obtained MoS2 is made up of small NPs, which stack each other to form large aggregated particles. In addition, every small NP is composed of small thin and curving nanosheets, looking like petals in morphology. Besides this, the fuzzy feature of lattice fringes shows the low crystallinity of MoS2 agreeing well with the XRD results. However, it is a pity that no more high-quality TEM and HRTEM images were obtained due to the very serious aggregations. Furthermore, the composition of as-prepared MoS2 was preliminarily determined by EDS (see Fig. S2a†), which shows that it is mainly composed of Mo, S and a quantity of C, N and Cl, and the calculated atomic ratio of S to Mo is about 2.01, further verifying the product is MoS2. The element Cl should originate from HCl used to adjust the pH value of the reaction mixture, and the C and N come from the reaction materials of solvothermal process.
In order to investigate the chemical states of Mo and S in the obtained MoS2 sample, high-resolution XPS spectra of Mo 3d and S 2p were also determined, as given in Fig. 3. For the Mo 3d spectrum (Fig. 3a), peaks located at 229.3 and 232.5 eV can be ascribed to Mo 3d5/2 and Mo 3d3/2, respectively, and the peak at 226.4 eV corresponds to S 2s. The S 2p spectrum (Fig. 3b) consists of a doublet with binding energies of 162.1 (S 2p3/2) and 163.6 eV (S 2p1/2). All this indicates the presence of Mo4+ and S2− in the MoS2 sample.37,40 The surface element contents derived from XPS quantification are 44.3% for S and 22.8% for Mo, respectively, which is close to a Mo to S atomic ratio of 1
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2, consistent with the above EDS result. In addition, UV-vis diffuse reflectance spectrum of the MoS2 prepared was determined and a wide absorption in the region of from 400 to 800 nm was observed (Fig. S4†), consistent with literature result.43
Fig. 4 depicts the time courses of H2 generation with different pH values. It can be seen that the highest rate of 876 μmol h−1 was obtained at pH 7. Either a lower or higher pH value leads to a significant decrease in the H2 evolution efficiency with the maximum H2 evolution rate of 68 μmol h−1 at pH 5 and 380 μmol h−1 at pH 9, respectively, consistent with previous results.33,44 This phenomenon can be explained as follows. At a lower pH value, the protonation of TEOA will reduce its ability to act as an effective electron donor and TEOA+ decomposition will become less facile.45 On the other hand, a higher pH value will make a lower proton concentration in solution, and then the H2 evolution reaction becomes more thermodynamically unfavorable.46
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| Fig. 4 Time courses of photocatalytic H2 evolution as a function of the pH value (MoS2 = 25 mg, EY = 0.4 mM, TEOA = 15 vol%). | ||
The effects of EY and TEOA concentrations were also investigated. As shown in Fig. 5a, the optimal EY concentration is 0.4 mM. A further increasing or decreasing both leads to a decrease in the hydrogen production activity. This phenomenon is probably because that at lower EY concentrations, the EY molecules adsorbed on MoS2 surface increase with EY concentration increasing, which benefits for improving the light absorption efficiency,47,48 however, at relative high EY concentrations, shielding effect of free EY molecules in solution as well as concentration quenching would occur,49 which will result in a decrease in the electron injection efficiency and then in the hydrogen production efficiency.50–53
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| Fig. 5 Time courses of photocatalytic H2 evolution as a function of (a) EY2− (MoS2 = 25 mg, TEOA = 15 vol%, pH = 7) and (b) TEOA (MoS2 = 25 mg, EY = 0.4 mM, pH = 7) concentrations. | ||
Similarly, Fig. 5b indicates that the H2 evolved gradually increases with increasing the TEOA concentration from 10% to 15% and the highest rate of 876 μmol h−1 was achieved at 15%, whereas it decreases to 582 μmol h−1 at 20%, consistent with literature results.45,48,54 According to literatures,55,56 this is probably because that in the present system, TEOA can be oxidized by photo-generated holes (h+) on EY molecules to form TEOA+. As a result, the increase in TEOA concentration makes more electrons transferred from TEOA to EY, and then faster reductive quenching of the excited EY molecules.
In addition, the influence of the catalyst concentration on hydrogen evolution performance was also discussed. As demonstrated in Fig. 6, increasing the catalyst concentration results in an increase in the hydrogen evolution rate, while the amount of H2 evolved does not scale-up linearly with the catalyst amount. Specifically, increasing the MoS2 amount from 12.5 to 25 mg makes an increase of the hydrogen evolution rate from 429 to 876 μmol h−1, while when 50 and 75 mg MoS2 were used, the hydrogen evolution rate was only 1202 and 1380 μmol h−1, respectively. Moreover, the system lifetime was prolonged to some extent when a higher catalyst concentration was used, possibly due to the stability increase of sensitizer EY.57 Except for the above experiments, a series of control experiments were also conducted and the results revealed that no H2 was detected either in the absence of EY, MoS2, TEOA, or when the reaction was performed in the dark, suggesting this reaction is a photocatalytic process.
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| Fig. 6 Time courses of H2 evolution as a function of MoS2 amount (EY = 0.4 mM, TEOA = 15 vol%, pH = 7). | ||
Furthermore, in view of photosensitizer (PS) also plays a crucial role in the dye-sensitized H2-generating systems,58 other four xanthene dyes, eosin B (EB), rose bengal (RB), erythrosin B disodium salt (EB2−) and rhodamine B (RhB) with different substitutions on the xanthene ring have also been employed to investigate the effect of PS species on the hydrogen-evolving activity of MoS2. As demonstrated in Fig. 7, the PS species significantly affect the H2 generation activity and the highest H2 evolution rate of 876 μmol h−1 was obtained for EY. Concretely, the activity order is EY > EB2− > RB > EB > RhB, similar to the results reported in literatures.46,48,59 In addition, under the optimal condition of 25 mg MoS2, 0.4 mM EY, 15% TEOA and pH 7.0, the quantum yield at 460 nm achieved to 22.8%.33,60
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| Fig. 7 (a) Time courses of hydrogen production and (b) the amounts of hydrogen evolved in 2.5 h with different sensitizer species (MoS2 = 25 mg, sensitizer = 0.4 mM, TEOA = 15 vol%). | ||
From the above results, we also found that for the EY–MoS2–TEOA system, hydrogen generation ceased after about 5 h. To elucidate the deactivation reasons, more experiments were performed and the results are displayed in Fig. 8. Firstly, the photocatalytic stability of MoS2 was determined by a recycling test (Fig. 8a). It can be seen that after four consecutive cycles, there is no significant decrease in the H2-evolving activity and more than 90% of the activity is still retained with respect to the first cycle, indicating that the MoS2 catalyst is stable during the photocatalytic reaction.
To further clarify this, the MoS2 sample recovered after four cycles was also characterized by SEM, XPS and EDS, and the results were compared with those of freshly prepared MoS2. It can be found that no significant changes occurred in the size and morphology of the MoS2 catalyst after the photocatalytic reaction, though a little more aggregations happened, as demonstrated in Fig. S1a–c.† In addition, the EDS and XPS results showed that the atomic ratio of S to Mo was also unchanged (see Fig. S2 and S3†). Concretely, for the recovered MoS2 sample, the elemental contents determined by XPS are 41.6% for S and 21.2% for Mo respectively, namely, the atomic ratio of Mo to S is still 1
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2. Furthermore, no obvious changes were observed for the UV-vis spectrum of the MoS2 recovered after reaction (see Fig. S4†). So the deactivation of the present photocatalytic system could be mainly attributed to the loss of EY under the irradiation of visible light.58 This assumption was further supported by the changes on the absorption spectra of the solutions before and after reaction. As indicated in Fig. 8b, the absorption intensity of EY decreases drastically together with an obvious blue shift of the characteristic absorption peak after reaction, which is associated with the loss of Br atoms from EY molecule,33 namely, the photodegradation of EY molecules happened. On the other hand, the color change from red to green-yellow of the reaction solution during the photocatalysis process further verified the above assumption.
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| Scheme 1 Proposed photocatalytic H2 evolution mechanism under visible light irradiation (a) and energy level (b) for the EY–MoS2–TEOA system. | ||
In order to verify the above hypothesis, photoluminescence (PL) spectra of EY and EY–MoS2 in TEOA solution were determined. It can be seen that the fluorescence (FL) intensity of EY–MoS2 is much weaker than that of EY (Fig. S5†), whereas the FL of EY can't be quenched by adding TEOA,33 implying an efficient electron transfer from the singlet excited state 1*EY to MoS2, namely, an oxidative quenching occurs. However, on the other hand, according to literature,33 the lowest-lying triplet excited state 3*EY, generated form singlet excited state 1*EY via efficient intersystem crossing, can be reductively quenched by TEOA and produce EY−˙ with reductive potential of −0.8 V (vs. NHE),33,63 which can also transfer electrons to the CB of MoS2 (ca. −0.50 V vs. NHE).64 So in the present EY–MoS2–TEOA H2-evolving system, the electron transfer involves both oxidative quenching and reductive quenching.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra14710k |
| This journal is © The Royal Society of Chemistry 2016 |