MoS2@ZnO Nanoheterostructures Prepared by Electrospark Erosion for Photocatalytic Applications

MoS2@ZnO nanoheterostructures were synthesized by electrospark erosion of zinc granules in a hydrogen peroxide solution and simultaneous addition of MoS2 nanostructured powder into the reaction zone. The morphology, size of the crystallites, as well as elemental and phase composition of the prepared structures, were examined using transmission electron microscopy and X-ray diffraction analysis. It was found that the synthesized products represent heterostructures containing MoS2 nanoparticles formed on ZnO nanoparticles. Raman spectroscopy and photoluminescence analysis were also used for characterization of the prepared heterostructures. The obtained MoS2@ZnO nanostructures revealed an intense broad emission band ranging from 425 to 625 nm for samples with different fractions of MoS2. Photocatalytic measurements showed that the maximal hydrogen evolution rate of the prepared nanoheterostructures was about 906.6 μmol·g−1·h−1. The potential of their application in photocatalytic water splitting was also estimated.


Introduction
During recent decades, functional heterostructured metal oxide and sulfide materials received much interest from scientists working in the field of materials for photocatalytic applications [1][2][3][4]. Non-equilibrium fabrication methods like self-propagating high-temperature and mechanochemical synthesis, electrical explosion of wires, and electrospark erosion methods have displayed tremendous potential for synthesizing such materials [5][6][7]. These fabrication methods of such materials yielded structures that revealed high reactivity in various processes. Solar energy is a well-known alternative energy source, and photocatalytic water splitting using sunlight is a promising and eco-friendly approach to produce hydrogen. Semiconductor materials can be used for water splitting if the lowest level of the conduction band (CB) is more negative than the H + /H 2 reduction potential (0 V vs. the normal hydrogen electrode (NHE)), and the highest level of valence band is more positive than the H 2 O/O 2 oxidation potential (1.23 V vs. NHE). [8] Combinations of n-type metal oxides and p-type transition metal dichalcogenides (TMDs) result in a semiconductor n-p heterojunction which can absorb a wide spectrum of solar energy containing both UV and visible light [9][10][11]. the synthesis conditions [34,35]. A schematic diagram of charge generation and transfer process under ultraviolet (UV) and visible (Vis) excitation is proposed to understand the photoluminescence mechanism [34]. The bandgap of MoS 2 /ZnO heterostructures can be adjusted by changing the MoS 2 /ZnO ratio. Photoluminescence spectra have revealed that there is the red shift in the band-edge emission wavelength for the MoS 2 /ZnO heterostructure compared with ZnO, because of a decrease of bandgap [34]. When ZnO is added to MoS 2 , it causes a blue shift due to an increase of the bandgap [27].
The photocatalytic activity of heterostructures depends on the ZnO morphology and MoS 2 content. The preparation method influences the content at which the photocatalytic activity reaches a peak [24,27,36,37]. Nanorods provide the best photocatalytic activity of the ZnO heterostructure [38].
Photocatalytic activity can be adjusted by adding Na 2 S and Na 2 SO 3 to an aqueous solution. In situ formed ZnS slows down the recombination of electron-hole pairs, and therefore increases the photocatalytic H 2 evolution rate [8,37].
The combination of hydrothermal methods with other non-equilibrium fabrication methods listed above creates an additional opportunity to prepare new heterostructures with enhanced characteristics and operating performance (e.g., phase composition, donoracceptor pair recombination, the rate of photocatalytic activity in water splitting reactions). Compared with the methods described, the combination of electrical explosion of molybdenum wires [5], self-propagating high-temperature synthesis of molybdenum sulfide [39] and electrospark erosion of zinc [7,32] provides a technique for preparing heterostructures from simple elements (Mo, S, Zn). It makes the synthesis more ecologically friendly because reduces the amount of waste water.
This work is aimed at fabrication and characterization of MoS 2 @ZnO heterostructures for photocatalytic applications by electrospark erosion (ESE) of zinc granules in a hydrogen peroxide solution and simultaneous addition of MoS 2 nanostructured powder in the reaction zone. MoS 2 as-prepared by self-propagating high-temperature synthesis was added to solution. The main aim was to use the non-equilibrium conditions of the ESE method where newly formed zinc oxide nanoparticles adhered to molybdenum disulfide nanolamellar particles which are separated by the electrosparks. Photoluminescent and hydrogen evolution measurements will be carried out to reveal the application of heterostructures in photocatalytic processes.

Fabrication of Nanostructured MoS 2 by Self-Propagating High-Temperature Synthesis
Nanostructured MoS 2 was synthesized by a self-propagating high-temperature reaction using mixtures of molybdenum nanopowder and pure elemental sulfur (99.90%, ZAO "Soyuzhimprom", Novosibirsk, Russia) [39]. Molybdenum nanopowder was prepared using the method of electrical explosion of wires in argon, described in [6]. A 0.25 mm diameter Mo wire (99.96%, OOO "GK "SMM", Moscow, Russia) was used. The following parameters were applied in the electrical explosion: voltage-28 kV, the exploded wire distance between the electrodes-100 mm, argon pressure-1 atm. According to BET measurements, the surface area A S and surface-average particle size D S of the powders were 4.6 m 2 ·g −1 and 130 nm, respectively.
In the synthesis of the nanostructured MoS 2 , stoichiometric mixtures of electroexplosive molybdenum nanopowder and pure elemental sulfur were used. These were then compacted into cylindrical pellets of 30 mm diameter and 10 mm height and placed into the sample holder in a special high pressure reactor described in [39]. The process of selfpropagating synthesis was initiated by point-heating of the pellet top using a Nichrome wire connected to a direct current (DC) power supply. Once started, a wave of exothermic self-propagating reaction sweeps through the remaining pellet material. The process temperature was controlled by a W/W-Re thermocouple connected to an oscilloscope employed for recording the thermo-emf signal. After completion of the self-propagating high-temperature synthesis (SHS) reaction, the final products were cooled in the reaction chamber. The SHS products represented silver gray packets of nanostructured molybdenum disulfide, according to X-ray diffraction phase analysis conducted.

Synthesis of MoS 2 -ZnO Heterostructures
The electrospark erosion method was used for the synthesis of the MoS 2 @ZnO nanoheterostructures [7]. In our case, a 38% aqueous solution of hydrogen peroxide was employed. MoS 2 @ZnO nanoheterostructures were synthesized by electrospark erosion of zinc granules (analytic grade, ZAO "Soyuzhimprom", Novosibirsk, Russia) in the hydrogen peroxide solution (OOO "INNOVATSIIA", Voronezh, Russia) and simultaneous addition of MoS 2 nanostructured powder in the reaction zone. Figure 1 shows the scheme of the electrospark erosion experiment for the fabrication of MoS 2 @ZnO heterostructures. The reactor represents a porcelain vessel very resistant to electric current pulses. 185 g of zinc granules were placed into the reactor and then 200 mL of hydrogen peroxide solution were poured. Two zinc electrodes were immersed in the hydrogen peroxide solution until the complete electric contact with the zinc granules. After this procedure, electric current pulses were applied to the electrodes from the power supply within 30 s for each experiment. The experimental conditions were the following: the electrode separation distance was 10 cm, the voltage was 500 V, the current was 150 A. After the experiment, the prepared suspension was separated into two fractions by decantation. Both fractions were then maintained at 80 • C in a drying oven for 1 h. self-propagating high-temperature synthesis (SHS) reaction, the final products were cooled in the reaction chamber. The SHS products represented silver gray packets of nanostructured molybdenum disulfide, according to X-ray diffraction phase analysis conducted.

Synthesis of MoS2-ZnO Heterostructures
The electrospark erosion method was used for the synthesis of the MoS2@ZnO nanoheterostructures [7]. In our case, a 38% aqueous solution of hydrogen peroxide was employed. MoS2@ZnO nanoheterostructures were synthesized by electrospark erosion of zinc granules (analytic grade, ZAO "Soyuzhimprom", Novosibirsk, Russia) in the hydrogen peroxide solution (OOO "INNOVATSIIA", Voronezh, Russia) and simultaneous addition of MoS2 nanostructured powder in the reaction zone. Figure 1 shows the scheme of the electrospark erosion experiment for the fabrication of MoS2@ZnO heterostructures. The reactor represents a porcelain vessel very resistant to electric current pulses. 185 g of zinc granules were placed into the reactor and then 200 mL of hydrogen peroxide solution were poured. Two zinc electrodes were immersed in the hydrogen peroxide solution until the complete electric contact with the zinc granules. After this procedure, electric current pulses were applied to the electrodes from the power supply within 30 s for each experiment. The experimental conditions were the following: the electrode separation distance was 10 cm, the voltage was 500 V, the current was 150 A. After the experiment, the prepared suspension was separated into two fractions by decantation. Both fractions were then maintained at 80 °C in a drying oven for 1 h.

Characterization Techniques
X-ray diffraction (XRD) measurements were performed using a Shimadzu-7000S diffractometer (CuKα radiation, λ = 1.5418 Å, Shimadzu, Kyoto, Japan). The phase composition and the crystallite size (coherent scattering region) of the prepared structures were determined. Transmission electron microscopy (TEM) analysis was performed on a JEOL JEM-2100F (JEOL Ltd., Тоkyo, Japan) in order to examine the morphology of the prepared nanoheterostructures. Raman spectroscopy measurements were conducted using a Centaur I HR spectrometer (OOO "Nano Scan Technology", Dolgoprudny, Russia) at a wavelength of 538.8 nm. This instrument combines a scanning probe microscope, as well as a confocal microscope/spectrometer with double dispersion for obtaining Raman scattering and fluorescence spectra and spectral images. The diameter of laser spot in Raman scattering measurements was 3 μm. The acquisition time was 10 min per sample. The number of investigated areas was varied from 3 to 5.

Characterization Techniques
X-ray diffraction (XRD) measurements were performed using a Shimadzu-7000S diffractometer (CuKα radiation, λ = 1.5418 Å, Shimadzu, Kyoto, Japan). The phase composition and the crystallite size (coherent scattering region) of the prepared structures were determined. Transmission electron microscopy (TEM) analysis was performed on a JEOL JEM-2100F (JEOL Ltd., Tokyo, Japan) in order to examine the morphology of the prepared nanoheterostructures. Raman spectroscopy measurements were conducted using a Centaur I HR spectrometer (OOO "Nano Scan Technology", Dolgoprudny, Russia) at a wavelength of 538.8 nm. This instrument combines a scanning probe microscope, as well as a confocal microscope/spectrometer with double dispersion for obtaining Raman scattering and fluorescence spectra and spectral images. The diameter of laser spot in Raman scattering measurements was 3 µm. The acquisition time was 10 min per sample. The number of investigated areas was varied from 3 to 5.
The spectral power distribution of the total radiant flux of the PL spectra was measured by using an integrating sphere that was connected to a CCD detector (AvaSpec-3648, (Avantes, Apeldoorn, The Netherlands). Samples were prepared in such a way that the surface area was~1 cm 2 . The energy efficiency of the phosphors was evaluated as the ratio of the radiation flux of the blue chip and the radiation flux of the phosphors. All measurements were carried out at room temperature. The LED source parameters were 395 nm, 3.25 V, 0.03 A. The hydrogen production rate was measured using a special measurement scheme. 60 mg of the prepared nanostructured powder was dissolved in 100 mL aqueous solution containing 0.1 M Na 2 S and 0.05 Na 2 SO 3 as the sacrificial reagents. The samples were treated under full spectra irradiation by a 150 W Xe lamp (or deuterium lamp (30 W)) in order to start the photocatalytic reaction. The flask with the sample was connected with a tube to a scaled hermetic burette with which the amount of released hydrogen was measured. using a special measurement scheme. 60 mg of the prepared nanostructured powder was dissolved in 100 mL aqueous solution containing 0.1 M Na2S and 0.05 Na2SO3 as the sacrificial reagents. The samples were treated under full spectra irradiation by a 150 W Xe lamp (or deuterium lamp (30 W)) in order to start the photocatalytic reaction. The flask with the sample was connected with a tube to a scaled hermetic burette with which the amount of released hydrogen was measured.

X-ray Phase and Structural Analysis of the Prepared MoS2@ZnO Heterostructures
X-ray diffraction measurements were performed in order to determine the phase composition and crystalline properties of the prepared nanoheterostructures, as shown in Figure

Raman Analysis of the Prepared MoS2@ZnO Heterostructures
In order to determine the composition of the produced nano man spectroscopy was also used for the characterization of the p structures. The Raman spectrum of MoS2@ZnO is shown in Figur  MoS2@ZnO showed peaks at 330, 360, 812, 838, 864, 897 and 950 cm −1 ∼330-360 cm −1 are related to molybdenum sulfide vibration modes o vibration modes of bridging and terminal S2 2− , as well as vertex sulfi to the quasi-amorphous state of the MoSx formed during the electros The Raman peaks at 950 cm −1 was assigned to molybdenum sulfid the possible presence of molybdenum oxysulfide MoSxOy due to the process of electrospark erosion of the zinc granules in the hydroge The latter can act as a source of oxygen-containing defects forming i nanostructured molybdenum disulfide.
The multi-phonon bands at 775-838 cm −1 , including the peaks correspond to zinc oxide [41,42]. The anomalous mode detected at 8 to the influence of MoS2 at their interface. Moreover, a special non-equilibrium conditions under which the MoS2@ZnO nanoh prepared during electrospark erosion in the medium of hydrogen origin of some of the observed anomalies in their Raman spectrum. The nanoheterostructure MoS 2 @ZnO shows the main characteristic peaks from both MoS 2 and ZnO. This can be attributed to the successful formation of nanoheterostructures during the process of electrospark erosion of the zinc granules in the hydrogen peroxide solution with simultaneous addition of the nanostructured molybdenum disulfide. The XRD pattern of MoS 2 and ZnO also demonstrates the presence of traces of Mo 2 S 3 and ZnS phases, which were not found in the final products of the SHS and ESE processes. Presumably, they form at the interface between the newly formed ZnO and dispersed MoS 2 particles. These phases are then condensed on the surface of the ZnO particles as interfacial layers, because of the simultaneous reactions between ZnO and MoS 2 .

Raman Analysis of the Prepared MoS 2 @ZnO Heterostructures
In order to determine the composition of the produced nanoheterostructures, Raman spectroscopy was also used for the characterization of the prepared nanoheterostructures. The Raman spectrum of MoS 2 @ZnO is shown in Figure 3. The synthesized MoS 2 @ZnO showed peaks at 330, 360, 812, 838, 864, 897 and 950 cm −1 . The Raman peaks at ∼330-360 cm −1 are Nanomaterials 2021, 11, 157 6 of 11 related to molybdenum sulfide vibration modes of ν(Mo-S) [40]. These vibration modes of bridging and terminal S 2 2− , as well as vertex sulfide centers are related to the quasi-amorphous state of the MoS x formed during the electrospark erosion process. The Raman peaks at 950 cm −1 was assigned to molybdenum sulfide defects, suggesting the possible presence of molybdenum oxysulfide MoS x O y due to the extreme energetical process of electrospark erosion of the zinc granules in the hydrogen peroxide solution. The latter can act as a source of oxygen-containing defects forming in the structure of the nanostructured molybdenum disulfide.
MoS2@ZnO showed peaks at 330, 360, 812, 838, 864, 897 and 950 cm . The Raman peaks at ∼330-360 cm −1 are related to molybdenum sulfide vibration modes of ν(Mo-S) [40]. These vibration modes of bridging and terminal S2 2− , as well as vertex sulfide centers are related to the quasi-amorphous state of the MoSx formed during the electrospark erosion process. The Raman peaks at 950 cm −1 was assigned to molybdenum sulfide defects, suggesting the possible presence of molybdenum oxysulfide MoSxOy due to the extreme energetical process of electrospark erosion of the zinc granules in the hydrogen peroxide solution. The latter can act as a source of oxygen-containing defects forming in the structure of the nanostructured molybdenum disulfide.
The multi-phonon bands at 775-838 cm −1 , including the peaks at 812 and 832 cm −1 , correspond to zinc oxide [41,42]. The anomalous mode detected at 832 cm −1 could be due to the influence of MoS2 at their interface. Moreover, a special role of the extreme non-equilibrium conditions under which the MoS2@ZnO nanoheterostructures were prepared during electrospark erosion in the medium of hydrogen peroxide can be the origin of some of the observed anomalies in their Raman spectrum.  The multi-phonon bands at 775-838 cm −1 , including the peaks at 812 and 832 cm −1 , correspond to zinc oxide [41,42]. The anomalous mode detected at 832 cm −1 could be due to the influence of MoS 2 at their interface. Moreover, a special role of the extreme nonequilibrium conditions under which the MoS 2 @ZnO nanoheterostructures were prepared during electrospark erosion in the medium of hydrogen peroxide can be the origin of some of the observed anomalies in their Raman spectrum.

Structural and Compositional Analysis
The morphology of the as-synthesized photocatalytic nanomaterials was studied with transmission electron microscopy (TEM). Figure 4a shows the TEM image of the MoS 2 @ZnO nanoheterostructures prepared using the method of electrospark erosion. It can be seen that the synthesized material represents two different types of nanoscale overlapping particles. The faceted spherical particles of 20-40 nm in size represent wurtzite type hexagonal zinc oxide (ZnO). The black elongated and also hexagonal particles are nanosized sheets of molybdenum disulfide adhering to ZnO nanoparticles.

Structural and Compositional Analysis
The morphology of the as-synthesized photocatalytic nanomaterials was studied with transmission electron microscopy (TEM). Figure 4a shows the TEM image of the MoS2@ZnO nanoheterostructures prepared using the method of electrospark erosion. It can be seen that the synthesized material represents two different types of nanoscale overlapping particles. The faceted spherical particles of 20-40 nm in size represent wurtzite type hexagonal zinc oxide (ZnO). The black elongated and also hexagonal particles are nanosized sheets of molybdenum disulfide adhering to ZnO nanoparticles. Energy-dispersive X-ray spectroscopy (EDS) helps to find the purity and elemental composition of the prepared materials. The EDS spectra in Figure 4b show the elemental composition of the prepared MoS2@ZnO material. The peaks of Mo, S, Zn and O are Energy-dispersive X-ray spectroscopy (EDS) helps to find the purity and elemental composition of the prepared materials. The EDS spectra in Figure 4b show the elemental composition of the prepared MoS 2 @ZnO material. The peaks of Mo, S, Zn and O are clearly visible.
The very small size of the ZnO particles is related to the extreme conditions of the electrospark erosion process [7]. The formation of the ZnO nanoparticles can consist of two simultaneous processes. Firstly, melting of Zn granules and the electrodes when applying voltage pulses with the subsequent release of the material as molten metal droplets with an initial temperature of approximately 2200 K, occurs. Secondly, evaporation of the materials of the medium and the electrodes with plasma formation takes place. Surface interaction of the molten zinc with the hydrogen peroxide aqueous solution occurs during the fast cooling of the particles with a cooling rate of about 10 9 K·s −1 . When the process is finished, this interaction results in particles consisting of a metal core coated with a film of interaction products of the metal with the dispersion medium, as well as single particles formed due to radiation-chemical and thermal decomposition of the dispersion medium.
The plasma formation results in atomization of the medium with subsequent recombination and formation of the decomposition products, which then interact with products of the first process to form a highly dispersed composite material. When applying current pulses, a hydromechanical effect accompanied by strong cavitation occurs. Finally, the particles forming are well distributed in the total volume of the suspension. At the same time, the particles start to disperse from the submicron S-Mo-S sandwich packets into nanoplatelets with a thickness of a few layers to form centers onto which newly formed ZnO nanoparticles can adhere. Process behavior under highly non-equilibrium conditions leads to the formation of nanocomposite structures with a high volume and surface deficiency which consequently display a high chemical reactivity in various processes.

Photoluminescent Measurements
The room temperature PL spectra of MoS 2 -coated ZnO nanocomposites are shown in Figure 5a. There is an intense broad emission band ranging from 425 to 625 nm for the samples with different fractions of MoS 2 . The mass of MoS 2 in the composite MoS 2 @ZnO varies from 1 to 2 g. The broad band at around 503 nm strongly decreases when the MoS 2 content increased. The reflection also decreased when the MoS 2 content increased ( Figure 5b). The reflection measurement accuracy was ±1%. An obvious quenching effect is observed for defect emission after the ZnO nanoparticle is coated with MoS 2 . The nature of this band is possibly connected with defects emission of the ZnO [43]. The nature of the green emission is contradictory. In [44] it was demonstrated that the green luminescence induced by an oxygen vacancy peaks at 490 nm, while the typical emission of the ZnO nanocomposite located around 503 nm corresponds to a donor-acceptor pair recombination. The cause of the deep level emission in the ZnO is controversial, although it is well accepted that the visible luminescence has multiple centers and pathways [45][46][47]. The emission bands represent a complex composition and could possibly be due to superposition of MoS 2 and ZnO emissions. We recently have demonstrated the emission of MoS 2 nanocrystals excited by electrons of nanosecond duration with different energy densities in [48]. With increasing energy densities from 6 up to 200 mJ·cm −2 the cathodoluminescence intensity strongly increases in the range of 450-675 nm. The authors suggested that luminescence is attributed to excess electrons in the conduction band. The bandgap of the nanopowder exhibits a high density of states. emission bands represent a complex composition and could possibly be due to superposition of MoS2 and ZnO emissions. We recently have demonstrated the emission of MoS2 nanocrystals excited by electrons of nanosecond duration with different energy densities in [48]. With increasing energy densities from 6 up to 200 mJ⋅cm −2 the cathodoluminescence intensity strongly increases in the range of 450-675 nm. The authors suggested that luminescence is attributed to excess electrons in the conduction band. The bandgap of the nanopowder exhibits a high density of states. The result obtained suggests that the recombination rate of photogenerated carriers is significantly reduced and that the charge transfer between the interface of ZnO and MoS2 is evidently facilitated. The reduced emission in the "green" spectral region for the MoS2 and ZnO mixture reported in reference [49] supports our assumption.

Hydrogen Evolution Measurements
The photocatalytic H2 production activities of the synthesized MoS2@ZnO nanoheterostructures were tested in an aqueous solution containing 0.1 M Na2S and 0.05 M Na2SO3 as the sacrificial reagents while applying full spectra irradiation by a 150 W Xe lamp (or deuterium lamp (30 W)). Sodium salts of analytic grade were used to make a solution (Na2S·9H2O, 97.8%, LC "VEKTON", Moscow, Russia; Na2SO3, 98.0%, LC "Karpov chemical plant", Mendeleyevsk, Russia). A plot of the variation in activities of the MoS2-ZnO nanoheterostructures irradiated by the different types of light source (dif- The result obtained suggests that the recombination rate of photogenerated carriers is significantly reduced and that the charge transfer between the interface of ZnO and MoS 2 is evidently facilitated. The reduced emission in the "green" spectral region for the MoS 2 and ZnO mixture reported in reference [49] supports our assumption.

Hydrogen Evolution Measurements
The photocatalytic H 2 production activities of the synthesized MoS 2 @ZnO nanoheterostructures were tested in an aqueous solution containing 0.1 M Na 2 S and 0.05 M Na 2 SO 3 as the sacrificial reagents while applying full spectra irradiation by a 150 W Xe lamp (or deuterium lamp (30 W)). Sodium salts of analytic grade were used to make a solution (Na 2 S·9H 2 O, 97.8%, LC "VEKTON", Moscow, Russia; Na 2 SO 3 , 98.0%, LC "Karpov chemical plant", Mendeleyevsk, Russia). A plot of the variation in activities of the MoS 2 -ZnO nanoheterostructures irradiated by the different types of light source (different powers of irradiation) is shown in Figure 6. The sample prepared by electrospark erosion of Zn granules in the peroxide solution with the maximal addition of 2.0 g of MoS 2 nanolamellar powder exhibits a photocatalytic activity with a H 2 evolution rate (HER) of 906.6 and 114.9 µmol·g −1 ·h −1 when exposed to the irradiation of the xenon or deuterium lamp, respectively. The accuracy of the hydrogen evolution rate measurements is within standard deviation. According to the error analysis for the HER measurements, the standard deviations depend on the amount of MoS 2 added to the reaction zone and were in the ranges of 8.3-10.7 µmol·g −1 ·h −1 and 25.9-30.1 µmol·g −1 ·h −1 for the experiments with the use of the deuterium and xenon lamp, respectively. Therefore, it was demonstrated that the hydrogen evolution rate depends on the amount of nanostructured MoS 2 added into the reaction zone and the lamp irradiation power as a light source as well. These excellent photocatalytic properties ensure a great potential of the prepared nanoheterostructures to be used for efficient photoelectrochemical water splitting. zone and were in the ranges of 8.3-10.7 μmol·g ·h and 25.9-30.1 μmol·g ·h for the experiments with the use of the deuterium and xenon lamp, respectively. Therefore, it was demonstrated that the hydrogen evolution rate depends on the amount of nanostructured MoS2 added into the reaction zone and the lamp irradiation power as a light source as well. These excellent photocatalytic properties ensure a great potential of the prepared nanoheterostructures to be used for efficient photoelectrochemical water splitting.

Conclusions
The present study demonstrated the successful preparation and synthesis of MoS2@ZnO nanoheterostructures by using electrospark erosion of zinc granules in a hydrogen peroxide aqueous solution with the simultaneous addition of nanostructured MoS2 powder in the reaction zone. Furthermore, TEM analysis proved that the as-prepared materials have binary heterostructures consisting mostly of MoS2 nanoparticles adhered to ZnO. The room temperature PL spectra of MoS2-coated ZnO nanoheterostructures showed an intense broad emission band ranging from 425 to 625 nm for the samples with different fractions of MoS2. The result obtained suggests that the recombination rate of photogenerated carriers is significantly reduced and that the charge transfer between the interface of ZnO and MoS2 is evidently facilitated. Finally, photocatalytic measurements showed that the prepared nanoheterostructures produced an attractively high hydrogen evolution rate of 906.6 μmol⋅g −1 ⋅h −1 and thus have great potential to be used for efficient photoelectrochemical water splitting.

Conclusions
The present study demonstrated the successful preparation and synthesis of MoS 2 @ZnO nanoheterostructures by using electrospark erosion of zinc granules in a hydrogen peroxide aqueous solution with the simultaneous addition of nanostructured MoS 2 powder in the reaction zone. Furthermore, TEM analysis proved that the as-prepared materials have binary heterostructures consisting mostly of MoS 2 nanoparticles adhered to ZnO. The room temperature PL spectra of MoS 2 -coated ZnO nanoheterostructures showed an intense broad emission band ranging from 425 to 625 nm for the samples with different fractions of MoS 2 . The result obtained suggests that the recombination rate of photogenerated carriers is significantly reduced and that the charge transfer between the interface of ZnO and MoS 2 is evidently facilitated. Finally, photocatalytic measurements showed that the prepared nanoheterostructures produced an attractively high hydrogen evolution rate of 906.6 µmol·g −1 ·h −1 and thus have great potential to be used for efficient photoelectrochemical water splitting.