Gwaza Eric Ayoma,
Malik Dilshad Khan
a,
Rishabh Srivastavab,
Wang Linb,
Ram K. Guptab and
Neerish Revaprasadu
*a
aDepartment of Chemistry, University of Zululand, Private Bag X1001, KwaDlangezwa 3880, South Africa. E-mail: RevaprasaduN@unizulu.ac.za
bDepartment of Chemistry, Pittsburg State University, Pittsburg, KS 66762, USA
First published on 2nd September 2025
To overcome the potential issue of active site blockage by surfactants in colloidal synthesis, alternative synthetic approaches must be explored. In this study, we investigated both solvent-free and colloidal thermolysis routes to synthesize nickel sulfides (NiS and Ni3S2) using sulfur-based Ni complexes, [Ni(S2CO(C2H5))2] (Ni-Xan) and [Ni(S2CN(C2H5)2)2] (Ni-DTC) as precursors. The solvent-free decomposition of these complexes produced ligand-free NiS and Ni3S2 in the absence or presence of triphenylphosphine (TPP), respectively. In contrast, colloidal thermolysis in oleylamine (OLA) led to phase-selective nickel sulfide formation (NiS and Ni3S2), with TPP facilitating desulfurization. The electrochemical performance of the synthesized materials was evaluated in water splitting and supercapacitance applications. Among the tested materials, NiS synthesized from Ni-Xan in OLA exhibited the highest specific capacitance (809.2 F g−1 at 1 A g−1) and energy density (34.9 Wh kg−1), while NiS derived from Ni-DTC in OLA achieved the highest power density (281.7 Wh kg−1). Additionally, the Ni3S2 electrode obtained via the colloidal route demonstrated superior HER performance, requiring only 197 mV (Tafel slope: 159 mV dec−1) to reach a current density of 10 mA cm−2. These findings underscore that simply eliminating surfactants and adopting a solvent-free method is not inherently sufficient to achieve high electrochemical performance. This study provides insights into the limitations of solvent-free synthesis and outlines potential prerequisites that may guide future optimization for improved electrochemical performance.
Transition metal sulfides continually attract attention as potential substitutes for exotic metals in energy conversion and storage technologies. Nickel sulfides have probably drawn more exploration than other sulfides in sustainable energy technologies.9 It has been prepared in different compositions, NiS, NiS2, Ni3S2 and N9iS8.10 NiS which has been more documented amongst the nickel sulfide system probably due to thermodynamic stability11 has been deployed to improve the reaction kinetics of water splitting and in energy storage systems.9 For example, Zhang et al.12 recently fabricated NiS deploying grapefruit peel and Ni(NO3)·6H2O as S and Ni precursors, respectively which was applied as an efficient catalyst in HER and OER. We also have reported NiS obtained from metal–organic compounds towards improving the water-splitting reaction kinetics.10,13,14 The relatively scarcer Ni3S2 phase is an interesting catalyst due to its electronic structure. It has a rhombohedral structure with tetrahedral nickel atoms giving room for Ni–Ni interactions.15 These interactions give Ni3S2 its metallic behavior which makes it an excellent electrical conductor applicable in catalysis.16 The Zhong group17 for example formed Ni3S2 using Ni foam and Na2S·9H2O which demonstrated high OER activity. Also, nickel sulfides such as Ni3S2/NiS18 and NiS19 have been employed as electrode materials in supercapacitor fabrication. Nickel sulfides’ continued appeal to the research community stems from their abundance in earth reserves,20 electrical conductivity17 and versatility in morphology and composition.10
The desire for phase-pure nickel sulfides, considering the multiplicity of phases in the sulfide system, is weighed down by the difficult synthetic protocols. Traditionally, sulfides of nickel have been prepared by high-temperature decomposition of dual or multiple precursors in the absence of any solvents. For instance, Kosmac and colleagues21 formed a mixture of nickel sulfide phases by the mechanical alloying of Ni and S powders in a glove box at high temperatures over an extended period. Other solventless synthetic routes like thermal diffusion,22 solid-to-solid calcination23 and melt decompositions10,24 have also been deployed to fabricate nickel sulfides. These solvent-free routes result not only in poor control of morphology, composition, size and purity of products but also impose high reaction temperatures and time. The use of multiple precursors also makes the synthetic process cumbersome. The colloidal synthetic pathway involving the use of solvents generally yields well-defined particles in terms of dimension, composition and purity.25 For example, different researchers have employed Ni sources like Ni(NO3)2·6H2O, nickel acetate tetrahydrate, Ni foam, Ni foil and S providers like thiourea, Na2S·9H2O and 2-mercaptoethanol to fabricate dimensionally controlled and pure Ni3S2 and NiS exercising colloidal methods like hydrothermal17,26,27 and solvothermal.28–30 Also, other routes like microwave-assisted decompositions,31 electrodeposition32 and product precipitation33 have been deployed in the preparation of desired nickel sulfides similarly employing dual or multiple precursors.
The single-source precursor route primarily involving metal–organic frameworks to the formation of nickel sulfides bypasses the challenges associated with the use of multiple precursors. This straightforward and facile route to the fabrication of metal sulfides has been deployed in the synthesis of Ni3S2 and NiS. For instance, we have utilized sulfur-based coordination complexes like dithiocarbamates,34,35 xanthates24,36 and dithiophosphonates10,13,14 to form or deposit nickel sulfides. The use of single-source starting materials or any of the other routes to the formation of nickel sulfides is, however, largely inflexible to the formation of more than one pure phase.
Herein, we utilized xanthate, [Ni(S2CO(C2H5))2] (Ni-Xan) and dithiocarbamate, [Ni(S2CN(C2H5)2)2] (Ni-DTC) complexes to prepare different phases of nickel sulfide (NiS and Ni3S2) from a single precursor via a solvent-free and colloidal route. In the solvent-free route, the complexes were pyrolyzed under an inert atmosphere, whereas in colloidal synthesis, oleylamine (OLA) was used as a solvent and capping agent. The study investigates how the choice of starting precursors and the synthetic routes influence the charge storage and water-splitting performance of nickel sulfide phases. This study highlights critical considerations for designing suitable ligands and suggests potential prerequisites that may result in enhancing the performance of materials synthesized via solvent-free routes.
The solvent-less pyrolysis of Ni-Xan/TPP and Ni-DTC/TPP in an inert atmosphere (N2) at 250 °C for an hour yielded hexagonal NiS. The formation of phase-pure NiS (ICDD# 01-075-0613) for Ni-Xan (NiS-3) and Ni-DTC (NiS-4) was confirmed by the powder XRD as matched to the standard reference patterns [Fig. 1(i)]. The facile formation of phase-pure NiS from these precursors is anticipated since nickel is directly bonded to the sulfur in the complexes and their thermal decomposition has been reported to lead to volatile components that are easily removable.36,37 The solvent-free preparation of NiS from Ni-Xan and Ni-DTC is not only straightforward but also scalable. We also explored the fabrication of nickel sulfides from both complexes mediated by TPP via the solvent-free pyrolysis route. This procedure requires the initial homogenization of the desired amounts of TPP with Ni-Xan or Ni-DTC before the pyrolysis reactions. The decomposition of the composite of Ni-Xan with TPP (1:
4) at 250 °C for 1 hour under an N2 atmosphere afforded phase-pure nickel sulfide which matched well to heazlewoodite Ni3S2 (Ni3S2-2) of the rhombohedral crystal system as per the ICDD# 01-085-0775 [Fig. 1(iii)]. Similarly, the pyrolysis of Ni-DTC with TPP (1
:
4) under the same conditions afforded phase-pure heazlewoodite Ni3S2 (ICDD# 01-085-0775) which will be referred to as Ni3S2-4. It is noteworthy that the stoichiometry of the metal complex precursor to TPP in these decomposition reactions is crucial for the successful fabrication of Ni3S2. For instance, the pyrolysis of a 1
:
3 composite of Ni-DTC with TPP yielded a mixture of nickel sulfides identified as rhombohedral Ni3S2 (ICDD# 01-073-0698) and orthorhombic Ni9S8 (ICDD# 01-078-1886) as shown in Fig. S2. Though the Ni3S2 material is highly desired due to its excellent catalytic activity,38,39 synthetic protocols have been largely limited to the colloidal routes.15,40 In addition, dual or multiple precursors have dominated the colloidal pathway to Ni3S2 fabrication hence their formation procedures are usually complex and time-consuming.40 Therefore, the use of cheap, readily available, and chemically stable TPP to mediate the solvent-free formation of Ni3S2 from single-source precursors offers a significant advantage over conventional methods.
Similar reactions were also carried out via a colloidal method to gain further insight into the role of TPP in the formation of nickel sulfides. The decomposition of Ni-Xan (NiS-1) or Ni-DTC (NiS-2) in oleylamine (OLA) by the heat-up protocol at 250 °C for 1 hour formed nickel sulfide which matched well with hexagonal NiS (ICDD# 01-075-0613), as shown in Fig. 1(ii).
Table 1 summarizes the precursors, experimental conditions, phases obtained, and codes used in this study as well as the average crystallite sizes of the synthesized catalysts.
Complexes/composites | Synthetic route | Reaction conditions | Phase formed | Code | Average crystallite size (nm) |
---|---|---|---|---|---|
[Ni{S2CO(C2H5)}2] (Ni-Xan) | Colloidal | 250 °C, in oleylamine, 1 h | NiS | NiS-1 | 33 ± 5 |
[Ni{S2CN(C2H5)2}2] (Ni-DTC) | Colloidal | 250 °C, in oleylamine, 1 h | NiS | NiS-2 | 22.5 ± 4 |
[Ni{S2CO(C2H5)}2] (Ni-Xan) | Solventless | 250 °C, 1 h | NiS | NiS-3 | 23 ± 7 |
[Ni{S2CN(C2H5)2}2] (Ni-DTC) | Solventless | 250 °C, 1 h | NiS | NiS-4 | 49 ± 3 |
[Ni{S2CO(C2H5)}2] (Ni-Xan)/triphenylphosphine (TPP) | Colloidal | 250 °C, in oleylamine, 1 h | Ni3S2 | Ni3S2-1 | 12 ± 8 |
[Ni{S2CO(C2H5)}2] (Ni-Xan)/triphenylphosphine (TPP) | Solventless | 250 °C, 1 h | Ni3S2 | Ni3S2-2 | 16 ± 2 |
[Ni{S2CN(C2H5)2}2] (Ni-DTC)/triphenylphosphine (TPP) | Colloidal | 250 °C, in oleylamine, 1 h | Ni3S2 | Ni3S2-3 | 26 ± 14 |
[Ni{S2CN(C2H5)2}2] (Ni-DTC)/triphenylphosphine (TPP) | Solventless | 250 °C, 1 h | Ni3S2 | Ni3S2-4 | 28 ± 8 |
There are limited reports on the fabrication of NiS in OLA via the heat-up method employing single-source precursors and mostly involving the use of a combination of solvents or additives.41–44 The preparation of NiS in OLA, as presented, is facile and straightforward. The thermolysis of composites of Ni-Xan or Ni-DTC with TPP in OLA, formed Ni3S2 just like the solvent-less pyrolysis reactions. The synthetic protocol for these reactions entailed the initial homogenization of the required complex and the desired amount of TPP by grinding before decomposition in OLA by the heat-up method at 250 °C for 1 hour under N2. The thermolysis of the composite of Ni-Xan and TPP in 1:
2 stoichiometry resulted in Ni3S2 (Ni3S2-1) of the cubic crystal system as per (ICDD# 01-076-1813) as shown in Fig. 1(iv). Similarly, the decomposition of Ni-DTC/TPP (1
:
3) in OLA at 250 °C resulted in nickel sulfide, which matched well with Ni3S2 (ICDD# 01-076-1813), referred to as Ni3S2-3, as shown in Table 1. The stoichiometry of the complex to TPP is critical in the formation of Ni3S2 in the colloidal route just like in the solvent-free pyrolysis path stated above. For example, the thermolysis of Ni-DTC/TPP (1
:
2) in OLA at 250 °C yielded a mixture of nickel sulfides that matched rhombohedral NiS (ICDD# 01-086-2280) and the non-stoichiometric hexagonal Ni0.96S (ICDD# 00-050-1791) as shown in Fig. S3. It is worth noting that the colloidal synthesis of Ni3S2 is often carried out using dual or multiple precursors and typically relies on the time-intensive hydrothermal route.40 In our previous work, we reported the use of single-source precursors in colloidal synthesis with trioctylphosphine (TOP) to obtain the Ni3S2 phase and proposed the role of TOP in achieving a sulfur-deficient composition.35,45 The use of single-source precursors and the heat-up method in preparing Ni3S2 simplifies most documented protocols.
The role of TPP in the formation of Ni3S2 by colloidal as well as solvent-free routes employing sulfur-based coordination complexes is interesting and needs further probing. Trialkylphosphines have been used as desulfurization agents as well as a source of phosphorus for metal phosphide formation. For example, colloidal or solvent-less thermolysis of various chalcogen-based metal–organic precursors in the presence of trialkyl/arylphosphines at high temperatures resulted in the formation of metal phosphide nanomaterials.10,13,14,46 In addition, they have been used for the desulfurization of metal chalcogenides to yield metallic (Ag, Sb, Bi) or bi-/intermetallic (AgBi, Ag3Sb) compounds.47–49 TPP therefore mediates the formation of the non-stoichiometric Ni3S2 in solvent-free and colloidal routes by partial desulfurization. The partial desulfurization by TPP also explains the formation of the sulfur-rich Ni0.96S phase for the lower TPP composite amount (Ni-DTC/TPP; 1:
2) compared to the sulfur-deficient Ni3S2 (Ni-DTC/TPP; 1
:
3) in the colloidal decompositions of Ni-DTC/TPP composite (Fig. 1 & S3). The mediating role of trialkylphosphines in the formation of functional materials can therefore be explored to prepare desirable but scarcely available metal chalcogenide analogues.
The microstructure of the formed NiS and the TPP-assisted fabricated Ni3S2 via the solvent-less and colloidal routes was examined by employing scanning electron microscopy (SEM), energy-dispersive X-ray (EDX), transmission electron microscopy (TEM) and selected area electron diffraction (SAED). The SEM images of the nickel sulfides indicate agglomerated particles without any defined shape at such low magnification (Fig. 2 & S4). However, Ni3S2 particles obtained in OLA (Fig. 2c) and the NiS and Ni3S2 formed from the solvent-less pyrolysis of complex 2 (Fig. S4b and d) showed sheet-like morphologies.
![]() | ||
Fig. 2 SEM images of NiS obtained from the decomposition of (a) Ni-Xan and (b) Ni-DTC and Ni3S2 obtained from the decomposition of (c) Ni-Xan/TPP and (d) Ni-DTC/TPP all in OLA. |
TEM analysis of nickel sulfides provided further insight into these materials’ microstructure. The TEM images (Fig. 3 & S5) of the prepared sulfides confirm the agglomeration and compact arrangement of the particles. It also revealed that these materials have a non-uniform morphology consisting of spherical and elongated-shaped particles. The elemental mapping images of the fabricated sulfides indicate exclusively the presence of Ni and S which were well distributed as shown in Fig. 2 & S3. Also, the experimental atomic percentage composition (EDX) of nickel sulfides agreed with the theoretical values (Table S1).
The crystallinity of the formed materials was examined by SAED and HRTEM analysis (Fig. 3 & S5). SAED images show well-defined spots that match well with the respective XRD and ICDD standard patterns, indicative of good crystallinity. The SAED results were affirmed by the clear lattice fringes of the formed sulfides that were in agreement with the standard patterns, as shown in the HRTEM results. We also calculated the crystallite size of our formed sulfides from our XRD results via the Debye–Scherrer equation (; L = sulfide's average crystallite size, λ = X-ray wavelength, β = full width at half maximum, and θ = Bragg's angle) to check the effect of the synthetic route on particle size as given in Table 1. NiS particles from the colloidal route were relatively smaller and less agglomerated than those from the solventless method, due to better morphology control and surface capping by the solvent (Fig. 3 & S4). Likewise, pure NiS made without TPP was larger than TPP-containing Ni3S2, indicating TPP's role as a capping agent that limits particle growth.
X-ray photoelectron spectroscopy (XPS) spectra of the formed and transformed sulfides were employed to examine the surface chemistry of our materials (Fig. 4 & S6). The survey spectrum of the colloidally formed NiS (NiS-1) indicated a composition of Ni, S, C, O and N. Apart from the expected Ni, S and residual C, O and N were attributed to surface oxidation and the capping amine group (OLA), respectively. The deconvoluted Ni 2p peaks at 855.2 and 873.2 eV (Fig. 4b) are assigned to 2P3/2 and 2p1/2, respectively, characteristic of Ni2+ of the sulfide.50,51 Additional Ni 2p peaks at 852.5 and 869.4 eV are assigned to Ni+ and metallic Ni0 while the satellite peak at 860.8 and shakeup peak at 878.8 eV are typical of nickel.50 The S 2p region showed two peaks (Fig. 4c), including 160.8 (2p3/2) and 162.2 eV (2p1/2) attributed to S of the sulfide. Other regions with peaks at 398.8, 284.4 and 530.7 eV (Fig. 4d & S6Ib and c) are assigned to N, C and O, respectively. The colloidally transformed sulfide (Ni3S2-2) had similar XPS results as expected (Fig. 4e-I & S6Id–f) with the presence of the P 2p region, the major exception (Fig. 4i). The peaks at 2p3/2 (129.2) and 2p1/2 (132.7 eV) are typical of metal phosphides and are due to residual amorphous nickel phosphide formed in the transformation of NiS to Ni3S2.52 Also, all the deconvoluted XPS regions of Ni3S2-2 had slightly higher binding energies compared to NiS-1, indicative of phase transformation.
![]() | ||
Fig. 4 XPS spectra of formed sulfides. Survey spectrum (a) and Ni 2p (b), S 2p (c) N 1s (d) regions of NiS-1. Survey spectrum (e) and Ni 2p (f), S 2p (g) N 1s (h), P 2p (i) regions of Ni3S2-1. |
The XPS analysis of the solventless formed sulfides (Fig. S6II) is similar to the ones from the colloidal route except for the absence of the N 1s region since no solvents were employed. The minor P 2p signal observed in the XPS spectrum, in all the transformed sulfides, i.e. Ni3S2 as given in Fig. 4 & S6, may originate from residual TPP or surface-bound phosphorus-containing intermediate species formed during the phase transformation.
NiS + OH− ↔ NiSOH + e− | (1) |
Ni3S2 + 3OH− ↔ Ni3S2(OH)3 + 3e− | (2) |
To gain further insight into the charge transfer kinetics of these materials, a comparison of the CV curves for the NiS and Ni3S2 samples at a scan rate of 10 mV s−1 was delineated as shown in Fig. 5g and h. These comparative curves clearly show that among the NiS and Ni3S2 samples, NiS-1, NiS-2 and Ni3S2-3 have more enclosed areas which are a pointer to their superior electrochemical kinetics. Also, the anodic potential (Ea) and cathodic potential (Ec) of the samples were noted where NiS-1 and NiS-2 had lower differences between Ea and Ec compared to Ni3S2-1 and Ni3S2-2, all formed via the colloidal route. On the other hand, the samples obtained via the solvent-free method showed a different result. Here, Ni3S2-3 and Ni3S2-4 showed higher peak potential differences than NiS-3 and NiS-4. It is important to note that the lower potential difference between the peaks shows better electronic transmission movement and ion fusibility due to low charge transfer resistance. NiS-2 and Ni3S2-3 offered the least ion resistance among the electrodes and hence amplified ion mobility suggestive of better charge storage capacity among all the electrodes. It is also important to note that a lower potential difference means faster redox processes which also enrich the power density and energy density of a material.
The anodic and cathodic peak current density of the electrodes was plotted against the scan rate as shown in Fig. 5i–l to probe into the charge storage capacity of nickel sulfides. No linear correlation between the anodic and cathodic peak current density as a function of scan rate is observed for all the electrodes indicating that charge storage has pseudocapacitance characteristics and not an absorption mechanism which is in agreement with the CV results. The charge storage mechanism for all the electrodes was probed further using the Sevcik equation.57 The linear plots of the current density vs. the scan rates for all the electrodes indicated a diffusion-assisted mechanism of the electrochemical oxidation and reduction processes as shown in Fig. 6a–d. The linear fitting of these plots resulted in the highest anodic slope of 4.81 for NiS-2 (Fig. 6a) among all the NiS samples whereas for the Ni3S2 electrodes, Ni3S2-3 had the highest slope of 3.03 (Fig. 6b). These results suggest that NiS-2 and Ni3S2-3 electrodes with faster oxidation processes have the best storage capacity with the highest rate of permeation of ions compared to their regression rate. Furthermore, cathodic intercepts were also plotted as shown in Fig. 6c and d with NiS-2 and Ni3S2-3 similarly having the better reduction processes (i.e. the slopes and intercepts). NiS-2 (prepared by the colloidal route) and Ni3S2-3 (obtained by the solvent-less protocol) therefore show the best charge transfer rate and storage capability potentials compared to all the electrodes.
The specific capacitance of the samples was calculated using the CV curves employing eqn (3) and (4):58
![]() | (3) |
![]() | (4) |
The specific capacitance (Cs) of the electrodes was also calculated by the following eqn (5) using GCD measurements.
Cs = I*Δt/(m*ΔV) | (5) |
Herein, Cs is the specific capacitance (F g−1), I is the current (A), Δt is the discharge time (s), m is the mass of the active material (g) and ΔV is the potential window. From the calculated results, the specific capacitance vs. current density plots for all the electrodes were done and are shown in Fig. S9a and b. NiS-2 showed the highest specific capacitance of 809.2 F g−1 compared to NiS-1 & NiS-3 (with an average of 600 F g−1) and NiS-4 (50 F g−1) at 1 A g−1 of current density. For the Ni3S2 electrodes, the ones prepared by the solvent-less route (Ni3S2-3 & Ni3S2-4) had the best specific capacitance (about 500 F g−1) in comparison to the samples formed by the colloidal method (Ni3S2-1 & Ni3S2-2) with 300 F g−1 at the current density of 1 A g−1. Therefore, the specific capacitance of the NiS samples formed by the colloidal method and the Ni3S2 ones fabricated by the solvent-free protocol was better than the respective other electrodes. The energy storage capacity of synthesized materials compares well with other recently documented Ni-based electroactive materials, as shown in Table S2.
Since the energy and power density of a capacitor are crucial to estimating its practical application, they were calculated using eqn (6) and (7):62
E = 0.5CV2 (Wh kg−1) | (6) |
P = 3.6 × E/Δt (kW kg−1) | (7) |
The electrochemical stability of an energy storage device is another key pointer towards its practical application and was evaluated through the cycling processes. The coulombic efficiency of the two best-performing electrodes was evaluated in terms of energy storage i.e. NiS-2 and Ni3S2-3 as shown in Fig. S9e and f. NiS-2 and Ni3S2-3 remarkably showed 100% coulombic efficiency over 5000 cycles indicative of cycling stability. NiS-2 and Ni3S2-3 electrodes also showed exceptional capacitance retention of 91.3% and 80.2%, respectively over 5000 cycles of testing. Therefore, energy storage testing parameters like CV, electrochemical kinetics, and capacitance derived using CV area and that obtained by GCD evaluations collectively indicate that colloidally prepared NiS and solvent-free formed Ni3S2 with NiS-2 and Ni3S2-3 materials showed the best performance among all the electrodes. This then means that the high carbon content of the solventless prepared NiS limited its energy storage performance more than the OLA capping agent blocking the active sites. Contrarily, OLA's adsorption on Ni3S2 had less of a negative impact on its storage functionality compared to the carbon content.
The performance of all materials towards OER was also investigated in an alkaline environment. Rare earth and exotic elemental oxides like IrO2 and RuO2 are the benchmark catalysts for OER, which restricts the practical application of these technologies. Readily available substitutes like nickel sulfides are therefore highly sought after. The OER performance of the fabricated electrodes was examined by polarization curves, as shown in Fig. 7. To attain 10 mA cm−2 current density, Ni3S2-1, Ni3S2-2, Ni3S2-3 and Ni3S2-4 required 275, 298, 272, and 256 mV with Tafel slopes of 73, 66, 88 and 71 mV dec−1, respectively. Also, the NiS samples needed overpotentials/Tafel slopes of 257/81 (NiS-1), 257/72 (NiS-2), 267/90 (NiS-3) and 290/45 (NiS-4) to reach the same current density. RuO2, the benchmark OER catalyst, demanded 333 mV to reach 10 mA cm−2. Ni3S2-4, NiS-1, NiS-2, and Ni3S2-4, NiS-4 are, therefore, better OER catalysts in terms of overpotential lowering and intrinsic reaction kinetics (Tafel slopes), respectively. Sulfides with relatively larger crystallite sizes tended to show better water splitting activity. For example, the sample with the highest HER performance and the one with the most favorable HER kinetics both fell into the group with larger particle sizes. Notably, surface morphology did not show a clear correlation with performance, as samples with distinct morphologies displayed comparable reaction kinetics. These findings suggest that intrinsic factors, such as crystallinity, conductivity, phase composition, or defect chemistry, may play a more decisive role in determining electrochemical behavior than particle size alone. The OER performance of synthesized nickel sulfides compares well with recently reported similar materials (Table S4). The HER and OER results indicate that the synthetic route had no major influence on the sulfide's performance.
The ion diffusion kinetics of an electrode sheds light on its charge/mass transfer processes, which are crucial to its practical application. We, therefore, investigated this property by electrochemical impedance spectroscopy (EIS) measurements. Fig. 8 gives the EIS measurements as Nyquist plots with linear behavior at low frequency and semicircle shape at higher frequency in congruence with other reports.65 The charge transfer resistance of electroactive species is a function of the semicircle's diameter, with resistance increasing with an increase in diameter.8,66 Ni3S4-4 showed the lowest charge transfer resistance of 0.6 Ω cm−2 among all the samples, which correlates with the OER results. Apart from the charge transfer resistance, the stability and ruggedness of an electrode are crucial to its long-term application. The durability of the materials was assessed by employing the polarization curves before and after 1000 CV cycles and long-term chronoamperometry (CA) curves for 24 h. Fig. S10 and S11 give the HER and OER stability polarization curves of all the electrodes. These curves for the 1st and 1000th cycles matched well indicative of the synthesized materials’ ruggedness and stability. CA curves for all the nickel sulfides were also employed to probe further into their durability and are given in Fig. S12. All the sulfides showed good stability of current density over an extended period of 24 h with NiS-1, NiS-4 and Ni3S4-4 having the best results. The EIS and CA results are suggestive of the feasibility of synthesized nickel sulfides for practical application. The fabricated nickel sulfides have therefore been shown as suitable electrode materials applicable in lowering the constraining energy thermodynamics in HER and OER.
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