Molybdenum sulfide modified with nickel or platinum nanoparticles as an effective catalyst for hydrogen evolution reaction

Characterization of TiO2NT/MoS2
Figure 2 shows scanning electron microscopy (SEM) images of MoS2 films obtained from precursor solutions of different compositions (Table 1). In all cases, except for the layer deposited from solution III, the entire surface of the substrate was covered. In the SEM image of the MoS2 layer obtained from (NH4)2MoS2 in water (solution III), the surface of TiO2 nanotubes can be seen. The use of solutions I (NaMoO4, thiourea, water) and solution IV ((NH4)2MoS2, DMF) resulted in a smooth surface of the MoS2 layers; however, cracks in the layer can be observed. A similar layer morphology was obtained from solution II ((NH4)2MoS2, thiourea, water) and solution III ((NH4)2MoS2, water). Despite some similarities, distinct differences in morphology can be observed depending on the raw material used. Each precursor follows a distinct chemical reaction pathway during hydrothermal synthesis. This affects the nucleation and growth rates of MoS2 crystals. Different precursors create different pH and ionic environments during the hydrothermal process. These conditions influence the crystallinity and phase of the resulting MoS2, leading to variations in morphology. For example, the use of Na2MoO4 might lead to a different ionic strength in the solution compared to (NH4)2MoS2, impacting the growth dynamics of MoS2. Moreover, the sulfur source in the precursor material plays a crucial role in the final structure of MoS2. Thiourea and (NH4)2MoS2 provide sulfur differently during the synthesis, impacting how sulfur atoms incorporate into the MoS2 lattice, which in turn affects the morphology.Figure 2SEM images of TiO2NT/MoS2 materials obtained from (a) Na2MoO4, thiourea, water; (b) (NH4)2MoS2, thiourea, water; (c) (NH4)2MoS2, water and (d) (NH4)2MoS2, DMF.The obtained materials were further characterized using transmission electron microscopy (TEM). In the TEM images of TiO2NT/MoS2 at different magnifications (Fig. 3), similar to the SEM analysis, the TiO2 nanotubes (TiO2NT) are not visible. The powder used for analysis was scraped from the surface of the wafer, and only the top layer of MoS2 crystals is observed in the images, without any indication of TiO2 nanotubes.Figure 3TEM images of TiO2NT/MoS2 with different magnifications.Figure 4 shows a comparison of X-ray diffraction (XRD) patterns of layers obtained from precursor solutions of different compositions. The patterns of the layers obtained from solutions II, III, and IV contain peaks corresponding only to pure TiO2 nanotubes. Only in the case of the layer obtained from the aqueous solution containing Na2MoO4 and thiourea (solution I) can be observed additional peaks at ~ 15° and 33°, which correspond to the (002) and (100) planes of MoS2, respectively. Using the XRD technique, it was impossible to confirm the deposition of MoS2 from II, III, and IV solutions. This is related to the fact that the layers were obtained in amorphous form, as no peaks are visible except those from TiO2NT.Figure 4XRD patterns TiO2NT/MoS2 materials obtained from Na2MoO4, thiourea, water; (NH4)2MoS2, thiourea, water; (NH4)2MoS2, water and (NH4)2MoS2, DMF.The elemental mapping (Fig. 5) confirmed the presence of Mo and S on the entire surface of the electrodes studied. When solutions I and IV were used, Mo and S were distributed more uniformly over the entire surface than in the case of solutions II and III layers. In the images of the layers from solutions II and III, areas of increased Mo and S can be observed, and it is worth noting that areas of increased Mo correspond with those where more S can be seen. This indicates the presence of a compound containing both Mo and S, such as MoS2. Table 2 shows the composition of each layer. Assuming that we obtained MoS2 on TiO2 nanotubes, the layers from solutions III and IV were characterized by an excess of Mo and O, which may indicate the formation of molybdenum oxides. A slight excess of Ti can be observed in the layers from solutions I and II; however, these responses are from the substrate, as the nanotubes were obtained directly on the titanium sheet.Figure 5EDX elemental maps for Mo, S, Ti, and O of TiO2NT/MoS2 materials obtained from (a–d) Na2MoO4, thiourea, water; (e–h) (NH4)2MoS2, thiourea, water; (i–l) (NH4)2MoS2, water and (m–p) (NH4)2MoS2, DMF.Table 2 Layers composition determined by EDX analysis.Electrochemical characterization of TiO2NT/MoS2
The obtained materials were tested as electrodes for electrocatalytic hydrogen evolution. Figure 6a shows a comparison of the linear sweep voltammetry (LSV) curves of the electrodes at a scanning rate of 5 mV s−1. As can be observed in the inset of Fig. 6a, the material obtained from a solution containing Na2MoO4 with thiourea in water (I) had the lowest overpotential at a current density of − 10 mA cm−2. However, the overpotentials for the other electrodes at this current density were very similar. A comparison of the Tafel slopes of TiO2NT/MoS2 electrodes is shown in Fig. 6b. The calculated slopes indicate that, according to the general HER model, the charge transfer step (Volmer reaction) is the step that determines the rate of the whole reaction26. Layers deposited from solution III ((NH4)2MoS2 in water) had the smallest Tafel slope and thus also the lowest exchange current density. The stability of the electrodes was also tested by applying a current density of − 10 mA cm−2 for 1 h. As shown in Fig. 6c at 1 h, the potential of neither electrode changed significantly. Despite the highest hydrogen evolution overpotential, layers obtained from solution III were chosen for further study. The differences in the overpotentials of the electrodes were insignificant, and the electrode obtained by deposition from an aqueous solution of (NH4)2MoS2 had the most preferable Tafel slope. The chosen synthesis was based on only one compound, without the need to add an additional sulfur precursor. The use of organic solvents was also avoided.Figure 6(a) LSV curves of TiO2NT/MoS2 electrodes obtained from different precursor solutions; inset: zooms of LSV curves from − 0.5 to − 0.2 V, (b) corresponding Tafel slopes, (c) chronopotentiometry curves of TiO2NT/MoS2 electrodes obtained from different precursors at the current density of 10 mA cm−2.Characterization of hybrids TiO2NT/MoS2 with Ni and TiO2NT/MoS2 with PtThe morphology of the obtained nickel and platinum-doped materials was determined by scanning electron microscopy analysis. The top part of Fig. 7 shows the SEM images of the synthesized hybrids of TiO2NT/MoS2 with Ni, and the bottom part of Fig. 7 presents hybrid images of TiO2NT/MoS2 with Pt at the different configurations of Ni and Pt positions. The as-received MoS2 particles are irregular, with the majority having a size of 170 nm. The SEM images show that the distribution of MoS2 particles is relatively homogenous, indicating that the synthesis process facilitated a uniform dispersion of the particles on the TiO2NT surface. The dense distribution of MoS2 particles suggests a strong interaction between the MoS2 and TiO2NT, which is favorable for the desired properties and performance of the hybrid material. In the case of hybrid samples containing nickel, the MoS2 layers structure is more connected and contains only thin ends in some places. In addition, many nodular agglomerated grains are seen on the hybrids with nickel-coating surfaces (TiO2NT/MoS2/Ni and TiO2NT/Ni/MoS2/Ni). For hybrid samples synthesized with platinum in the case of two TiO2NT/MoS2/Pt and TiO2NT/Pt/MoS2/Pt samples, where the platinum particles coat the surface of MoS2, their structure is significantly different from the TiO2NT/Pt/MoS2 sample, where the plantain is only located under the MoS2. The platinum causes the formation of rough and broader ends of MoS2 with a number of small debris pieces. This phenomenon is not visible for TiO2NT/Pt/MoS2 where ends of the surface MoS2 are thinner with no visible thickening and corrugations.Figure 7SEM images of hybrids TiO2NT/MoS2 with (a–c) Ni and (d–f) Pt at three different configurations.A detailed examination using transmission electron microscopy (TEM) revealed that the MoS2 walls are composed of multiple layers distributed throughout the sample volume. The hybrid TiO2NT/MoS2/Ni (Fig. 8a,b) contains nickel particles dispersed irregularly across the structure. In the hybrid TiO2NT/MoS2/Pt (Fig. 8c,d), the presence of platinum metal is confirmed, with the platinum particles showing a tendency to agglomerate into larger clusters at several locations within the sample.Figure 8TEM images of (a, b) TiO2NT/MoS2/Ni and (c, d) TiO2NT/MoS2/Pt with different magnifications.Energy dispersive X-ray (EDX) analysis was performed on two materials, TiO2NT/Ni/MoS2/Ni and TiO2NT/Pt/MoS2/Pt, to determine their elemental composition. The measurements were conducted at various locations on the samples to ensure representative results. The EDX analysis confirmed the presence of platinum, nickel, molybdenum, sulfur, titanium, and oxygen in both materials. The presence of nickel and platinum in TiO2NT/Ni/MoS2/Ni and TiO2NT/Pt/MoS2/Pt (Fig. 9), respectively, is consistent with the intended design and synthesis of these hybrids. The incorporation of molybdenum and sulfur can be attributed to the presence of MoS2, while titanium and oxygen are inherent to the TiO2NT substrate. These findings validate the successful integration of the desired elements into the hybrid structures. Importantly, the EDX analysis was conducted at multiple locations on the samples, ensuring that any potential variations in composition across the material were taken into account. The results indicate no significant differences in the quantity or distribution of the materials based on the location of the sample. This uniformity in composition further supports the successful synthesis and uniform distribution of the elements within the TiO2NT/Ni/MoS2/Ni and TiO2NT/Pt/MoS2/Pt hybrid structures.Figure 9EDX spectra of (a) TiO2NT/Ni/MoS2/Ni and (b) TiO2NT/Pt/MoS2/Pt.The XRD results were obtained for the TiO2NT/MoS2 hybrids with the inclusion of platinum or nickel in different configurations, as depicted in Fig. 10. The positions and intensities of dominant peaks corresponded well with the known crystallographic data for TiO2, confirming the presence of TiO2 in the hybrid structures and crystalline nature of the substrate. Regarding MoS2, due to its amorphous nature, characteristic peaks corresponding to MoS2 crystal lattice planes were not observed in the XRD patterns. This suggests the MoS2 component might exist in a disordered or poorly crystalline state. However, it is worth noting that the XRD results did show some additional broadening or slight shifts in the TiO2 peaks when comparing the different configurations of Pt or Ni. This could be indicative of interactions between the TiO2 substrate and the Pt or Ni dopants, potentially affecting the crystalline structure or lattice parameters of TiO2. Additionally, the remaining diffraction peaks that were not assigned to TiO2 likely originate from metallic titanium, corresponding to the substrate material27.Figure 10XRD patterns of hybrids TiO2NT/MoS2 with (a) Ni and (b) Pt at three different configurations were compared.Due to the lack of clear XRD peaks from MoS2 in the obtained results, an additional investigative method, X-ray Photoelectron Spectroscopy (XPS), was employed to confirm the presence of MoS2 in the samples.To confirm the presence of molybdenum disulfide, nickel, and platinum, X-ray Photoelectron Spectroscopy measurements were conducted for three selected samples, pristine TiO2NT/MoS2 material and their hybrid with the addition of nickel TiO2NT/Ni/MoS2/Ni and the addition of platinum TiO2NT/MoS2/Pt. Figures 11, 12 and 13 shows spectra for the Mo 3d, S 2p, O 1s, Ni 2p, and Pt 4f regions. The spectrum in the Mo 3d region (Figs. 11a, 12a, 13a) was fitted with four doublets (d5/2–d3/2 separation of 3.13 eV), with the first main line of 3d5/2 at a binding energy of 228.6 eV, indicating the presence of molybdenum sulfide in the 1T phase. The second line of 3d5/2 at a binding energy of 229.1 eV suggests the presence of molybdenum sulfide in the 2H phase28. The third line of 3d5/2 at a binding energy of 230.2 eV indicates the presence of molybdenum(IV) oxide, and the last line of 3d5/2 at a binding energy of 232.3 eV points to the presence of molybdenum(VI) oxide (MoO3)29.Figure 11High-resolution XPS spectrum of (a) Mo 3d, (b) S 2p, and (c) O 1s of TiO2NT/MoS2.Figure 12High-resolution XPS spectrum of (a) Mo 3d, (b) S 2p, (c) O 1s, and (d) Ni 2p of TiO2NT/Ni/MoS2/Ni.Figure 13High-resolution XPS spectrum of (a) Mo 3d, (b) S 2p, (c) O 1s, and (d) Pt 4f of TiO2NT/MoS2/Pt.An additional line at around 226 eV in binding energy originates from the S 2s line. The S 2p spectra (Figs. 11b, 12b, 13b) were fitted with three doublets (p3/2–p1/2 separation of 1.16 eV), with the first main line of 2p3/2 at a binding energy of 161.5 eV, indicating the presence of sulfur in molybdenum sulfide in the 1T phase. The second line of 2p3/2 at a binding energy of 163.2 eV indicates the presence of sulfur in molybdenum sulfide in the 2H phase. The last line of 2p3/2 at a binding energy of 168.8 eV signifies the presence of sulfur in sulfate (VI)28,30.The spectra in the oxygen region (Figs. 11c, 12c, 13c) were fitted with three peaks. The first peak, located at an energy of 530.5 eV, corresponds to the presence of X-O bonds (where X = Mo, Ni, S or Ti). The second peak, at a binding energy of 532.0 eV, indicates the presence of both metal oxides (oxygen in non-stoichiometric oxides), organic groups such as O=C, and bonds such as O–S. The third peak, located at 533.5 eV, indicates the presence of bonds such as O–C and/or –OH31,32. The spectrum in the nickel 2p3/2 region (Fig. 12d) was fitted with five lines. The first line, located at a binding energy of 856.6 eV, indicates the presence of nickel in the + 2 oxidation state in oxide or hydroxide compounds33. The remaining lines in the binding energy range of 858 to 865 eV are associated with multiplet splitting effects and further confirm the + 2 oxidation state of nickel. The spectrum in the Pt 4f region (Fig. 13d) was fitted with a doublet (the f7/2–f5/2 separation is 3.33 eV) with the main 4f7/2 line lying at a binding energy of 71.2 eV indicating the presence of platinum metal34.Electrochemical performance of hybrids TiO2NT/MoS2 with Ni and TiO2NT/MoS2 with PtThe hybrids obtained in this study were evaluated for their catalytic performance in the hydrogen evolution reaction under specific conditions. The measurements were conducted in a 0.2 M H2SO4 electrolyte using a three-electrode setup, employing a scan rate of 5 mV s−1. To facilitate comparison, we also tested bare TiO2 nanotubes and Pt as reference materials. The HER polarization curves of the commercial Pt and Ni discs, pure TiO2 nanotubes, and the hybrids obtained in this study, both with and without the addition of metal, are presented in Fig. 14. The obtained hybrids exhibited promising catalytic activity for the hydrogen evolution reaction, as evident from the linear sweep voltammograms shown in Fig. 14a,b. However, it is worth noting that the overpotential values for achieving a current density of jHER = 10 mA cm−2 were lower for the commercial Pt disc electrode compared to the hybrids but better than those observed for the commercial Ni disc electrode. This observation is summarized in Table 3, which presents the overpotential values for all the tested electrodes. Despite the slightly higher overpotential values, it is noteworthy that incorporating a small amount of metal resulted in an improvement of the hydrogen evolution overpotential compared to the TiO2 nanotubes/MoS2 electrode (see Fig. 7, Table 3). This suggests that the addition of the metal component positively influenced the catalytic performance of the hybrids.Figure 14LSV curves (HER reaction) of hybrids TiO2NT/MoS2 with (a) Pt and (b) Ni in 0.2 M H2SO4.Table 3 Electrochemical parameters determined from LSV curves and Tafel plots.However, a phenomenon occurred where the TiO2NT/Pt/MoS2/Pt configuration, with a higher quantity of platinum, exhibits poorer HER performance compared to than the TiO2NT/MoS2/Pt configuration. This discrepancy can potentially be attributed to the intricate synergy between TiO2NT and MoS2. One plausible hypothesis arises from the examination of TiO2NT/Pt/MoS2 and TiO2NT/MoS2 configurations. In these cases, the composite with platinum demonstrated lower catalytic activity compared to the platinum-free composite. It suggests that the presence of platinum between the layers of semiconductor materials has a detrimental effect on the catalytic activity of the composite. The negative impact of platinum presence between TiO2NT and MoS2 layers could be elucidated through various factors: (1) Platinum may disrupt the synergistic effects between TiO2NT and MoS2. The optimal interaction between TiO2NT and MoS2, crucial for enhanced catalytic activity, might be compromised by the introduction of platinum between them. (2) The presence of platinum could alter the charge transfer dynamics between TiO2NT and MoS2, influencing the electron flow required for the hydrogen evolution reaction negatively. (3) Platinum nanoparticles may physically block active sites on either TiO2NT or MoS2, hindering the accessibility of reactants and affecting the overall catalytic efficiency. Moreover, a similar phenomenon can be observed when nickel is used instead of platinum. In this case, when nickel is between the layers, the composites exhibit inferior activity, suggesting that the introduction of nickel between TiO2NT and MoS2 layers may also disrupt the balance and synergies, akin to the observed effects with platinum. Overall, while the obtained results were favorable, it is important to acknowledge that the catalytic activity of the hybrids, although enhanced by the presence of metal, still fell short of the performance exhibited by the commercial Pt disc electrode. However, utilizing a small amount of platinum and nickel in the hybrids offers a significant advantage in terms of cost-effectiveness. The cost of platinum, in particular, is relatively high, and its extensive use in industrial applications may not always be economically viable. By incorporating only a small quantity of these precious metals, the hybrids become a more practical and cost-effective alternative.Impedance spectra obtained for TiO2NT, TiO2NT/Ni/MoS2, TiO2NT/Pt/, TiO2NT/MoS2/Ni, TiO2NT/MoS2/Pt, TiO2NT/MoS2 are presented in Fig. 15. EIS spectra were taken at an onset potential for unmodified and modified electrodes. In each case where the metal was located on the outer layer, it was observed that these materials exhibited significantly lower charge transfer resistance compared to the other materials. Furthermore, the Nyquist plots for these materials showed a steeper slope, indicating more capacitive behaviour. The EIS results clearly show a noticeable improvement in electron transfer properties upon depositing the metal on the MoS2 surface. The lower charge transfer resistance observed in TiO2NT/MoS2/Ni and TiO2NT/MoS2/Pt indicates a more efficient electron transfer process, which is crucial for catalytic applications such as HER. Additionally, the steeper slope in the Nyquist plot suggests a more capacitive nature, indicating an increased electrochemical surface area and availability of active sites. Interestingly, when the metal is located between TiO2 and MoS2, higher charge transfer resistance was observed in the EIS curve. This higher value indicates a relatively lower electron transfer rate in the material, suggesting limited electrocatalytic activity. These studies confirm the hypotheses (1), (2) and (3) mentioned above regarding the reasons for poorer HER performance for materials where the metal was located between the layers.Figure 15EIS spectra of obtained catalysts: TiO2NT, TiO2NT/Ni/MoS2, TiO2NT/Pt/, TiO2NT/MoS2/Ni, TiO2NT/MoS2/Pt, TiO2NT/MoS2.Figure 16 illustrates the Tafel plots of hybrids TiO2NT/MoS2 with Pt and hybrids TiO2NT/MoS2 with Ni, which provide valuable insights into the kinetic behavior of the electrodes during the hydrogen evolution reaction. At high overpotentials, the HER is primarily kinetically controlled, and its behavior can be described by the Tafel equation:Figure 16Tafel plots of hybrids TiO2NT/MoS2 with (a) Pt and (b) Ni determined from LSV in 0.2 M H2SO4.here η (V) represents the overpotential, a (V) corresponds to the cathodic intercept associated with the exchange current density, b (V dec−1)) represents the cathodic Tafel slope, and j (A cm−2) denotes the catalytic current density. By analyzing the linear portion of the potential versus the logarithmic value of the current density, it becomes possible to calculate the Tafel slope values, which provide essential kinetic metrics of the catalyst.These Tafel slope values offer valuable information about the electrocatalytic activity of the tested electrodes. They indicate the rate at which the catalytic current density changes with variations in the overpotential. The magnitude of the Tafel slope provides insights into the reaction mechanism and the effectiveness of the catalyst in promoting the desired electrochemical process. The Tafel plots reveal interesting trends among the tested hybrids containing different metals. It is observed that almost all the hybrids incorporating metals exhibited lower Tafel slopes compared to the pure TiO2 nanotubes. This indicates a more efficient catalytic performance for the hybrids, as smaller Tafel slopes correspond to faster kinetics and better electrocatalytic activity. Notably, the hybrids with the addition of nickel stood out with significantly reduced Tafel slopes. These hybrids displayed a Tafel slope of 63 mV dec−1, whereas the commercial Pt disc electrode exhibited a Tafel slope of 38 mV dec−1, and the pure TiO2 nanotubes demonstrated a much higher Tafel slope of 229 mV dec−1. It is worth noting that the measured Tafel slope for the Ni disc was 171 mV dec−1. This finding is particularly noteworthy because a lower Tafel slope signifies a higher catalytic reaction rate and improved performance in the hydrogen evolution reaction. Comparatively, the commercial Pt disc electrode, which serves as a benchmark due to its excellent catalytic activity, exhibits a lower Tafel slope of 38 mV dec−1. However, it is noteworthy that the hybrids with the addition of nickel approached this level of performance, showcasing their potential as cost-effective alternatives to the platinum-based catalysts. Overall, these findings highlight the superiority of the hybrids containing metal additives, particularly nickel, in terms of their electrocatalytic performance. Furthermore, an interesting trend was observed regarding the positioning of the metal within the hybrids. It was noticed that when the metal was located on the surface of the MoS2 rather than beneath it, the resulting hybrids exhibited superior catalytic performance. This observation suggests that the proximity of the metal to the active sites of MoS2 plays a crucial role in enhancing the electrocatalytic activity. Placing the metal on the surface of MoS2 facilitates better electron transfer and promotes synergistic effects between the metal and the MoS2, leading to improved catalytic efficiency in the hydrogen evolution reaction. The trend of surface positioning of the metal as a contributing factor to enhanced performance provides valuable insights for designing and developing efficient electrocatalysts. By strategically controlling the arrangement of metal and MoS2, it becomes possible to optimize the catalytic properties and achieve superior performance in various electrochemical processes. To compare the catalytic performance of the tested materials, the Tafel slope values were compiled and tabulated in Table 3.In Table 4, literature-based Tafel slope results for MoS2-based materials are presented. As observed, some of the catalysts synthesized in this work fall within the range of values reported in the literature.Table 4 Literature-based Tafel slope values for MoS2-based.This consistency with literature values suggests that the electrocatalytic performance of the developed catalysts aligns with the trends and characteristics observed in prior research. The comparison provides additional validation and context for the obtained results, indicating that the catalysts exhibit Tafel slopes that are consistent with or comparable to those reported for similar materials in the existing body of scientific literature.The stability of the tested materials was evaluated using chronopotentiometry measurements over a duration of 3600 s. The results revealed that almost all the materials, except pure TiO2 nanotubes, exhibited excellent stability under the applied experimental conditions (see Fig. 17). Chronopotentiometry is a reliable technique for assessing the long-term stability of electrocatalytic materials. By applying a constant current (− 10 mA cm−2) to the electrodes and monitoring the corresponding potential changes over time, it is possible to evaluate the durability and performance of the catalyst. In this study, except for the pure TiO2 nanotubes, nearly all materials demonstrated remarkable stability during the 3600-s chronopotentiometry measurements. The absence of significant potential fluctuations or degradation suggests that these materials retained their catalytic activity and structural integrity over an extended period, reinforcing their suitability for practical applications. Material stability is crucial for successful utilization in various electrochemical devices and processes. The observed stability in the chronopotentiometry measurements confirms the robustness and reliability of the tested materials, providing a solid foundation for their potential implementation in real-world applications.Figure 17Stability of hybrids TiO2NT/MoS2 with (a) Pt and (b) Ni at a current density of − 10 mA cm−2. (c) Stability measurement for TiO2NT/MoS2/Pt and Pt disk during 100 h.Additionally, stability measurements were conducted at a current density of − 10 mA/cm2 for 100 h for both the TiO2NT/MoS2/Pt electrode and, for comparison, the Pt disk electrode. The results indicate minor changes in potential for both the synthesized material and the commercial disk electrode. It can be stated that the materials exhibit stability over time during electrochemical measurements. An unexpected increase in potential was observed around 80 h for both materials (measurements were performed simultaneously using the same instrument, as the potentiostat–galvanostat has multiple measurement channels). Unfortunately, explaining the events after this hour is challenging, and an issue with the measurement setup likely occurred.

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