Open Access Article
Athma E.
Praveen
a,
Viplove
Mishra
a,
Aditi
Chandrasekar
*b and
Venkataramanan
Mahalingam
*a
aDepartment of Chemical Sciences, Indian Institute of Science Education and Research (IISER) Kolkata, Mohanpur, 741246, West Bengal, India. E-mail: mvenkataramanan@yahoo.com
bSchool of Arts and Sciences, Azim Premji University, Bangalore 562125, India. E-mail: Aditi.chandrasekar@apu.edu.in
First published on 9th October 2025
Transition metal selenides are considered to be promising electrode materials to catalyze various electrocatalytic reactions. The synthesis of these metal selenides involves harsh synthetic conditions and multistep routes. Herein, a room-temperature ligand-assisted strategy has been developed to synthesize NiSe, CoSe, and NiCoSe in a pure phase. This study delves into the significant impact of ligands on nanoparticle synthesis, with a particular focus on their pivotal role in finely adjusting the crystalline phase of the resulting nanomaterials. We have focused on identifying the specific ligands that can effectively manipulate nucleation and growth processes for the synthesis of specific crystal structures of MSe (M = Ni, Co). The role of functional groups in ligands was probed, and it was found that the carboxylic acid groups play a key role in facilitating the synthesis of pure-phase NiSe, CoSe, and NiCoSe. Through a detailed examination of the existing literature and theoretical calculations, we have investigated the mechanism and role of carboxylate ligands in MSe (M = Ni, Co) formation. Computational investigations suggest that the formation of a metastable metal–carboxylate intermediate complex optimizes the reaction condition, makes it more favorable for reorientation, and allows selenium to approach the nickel center. Furthermore, the synthesis of NiCoSe aims to enhance the electrocatalytic performance of NiSe and CoSe, as the bimetallic (NiCoSe) material exhibits superior electrochemical properties compared to its monometallic counterparts. The electrocatalytic activities of the synthesized transition metal selenides were evaluated for hydrazine-assisted water splitting. Bimetallic NiCoSe displays superior electrocatalytic performance toward hydrazine oxidation and hydrogen evolution reactions compared to the monometallic phases of NiSe and CoSe. The bimetallic component requires a potential of 0.20 V vs. RHE and an overpotential of 0.20 V to attain 10 mA cm−2 for the HzOR and HER, respectively. Moreover, NiCoSe displays excellent activity as a bifunctional catalyst, and it requires a very low cell voltage of 0.45 V to attain a current density of 10 mA cm−2 for H2 production. The free energy profile of the stepwise HzOR has been investigated in detail. The computational results reveal the enhanced feasibility of the HzOR on NiCoSe (1
:
1) compared to NiSe. Therefore, briefly, this work offers an innovative synthesis protocol for the ligand-induced room-temperature synthesis of transition metal selenide nanostructures and their application for hydrazine-assisted hydrogen production.
In recent years, considerable attention has been devoted to understanding the role of ligands in governing nanoparticle phase control.33 Ligands play a crucial role in the nucleation and growth processes owing to their ability to influence nucleation kinetics by acting as either stabilizers or inhibitors, and they can exert control over the subsequent growth of nanoparticles by modifying surface interactions. The interactions between ligands and the nanoparticle surface have a profound impact on the resulting crystal structure and, consequently, the physical and chemical properties of the nanocrystals produced. Ligands can selectively bind to specific facets or crystallographic planes of the growing nanoparticles, thereby modifying the surface energy and surface chemistry. In this manner, they serve as stabilizing agents, lowering the energy barrier for nucleation, or as kinetic inhibitors, impeding the formation of nuclei and subsequently affecting the growth of nanoparticles.33 By carefully selecting appropriate ligands, researchers tailor the synthesis conditions to achieve the desired nanoparticle properties such as size, shape, and surface functionality.34,35 For example, Revaprasadu et al. synthesized various metal chalcogenides and phosphides by tuning different ligands, surfactants, and synthetic conditions.36 Our group has reported how the use of thiol-based ligands leads to the selective synthesis and stabilization of the Ni2P phase, while thiol-free ligands transform the Ni2P phase into the Ni12P5 phase of nickel phosphide.37 Similarly, Pramanik et al. synthesized the NiTe phase using tartaric acid as a ligand.38 Generally, these syntheses involve multiple steps and harsh synthetic conditions. In addition, the exact mechanism explaining why the use of particular ligands leads to the formation of selective phases has not been explored.
Herein, a ligand-mediated room-temperature synthesis route is reported for the preparation of NiSe and CoSe in the pure phase. The synthesis involves carboxylic acid-based ligands and elemental Se as a selenide source to facilitate the synthesis of pure-phase NiSe and CoSe. The role of functional groups in ligands is probed by synthesizing NiSe materials using ligands with different functional groups. We have found that the presence of dicarboxylic acid groups in the ligand plays a key role in the synthesis of nickel and cobalt selenides. The precise coordination between ligands and the nanoparticle surface is not fully known due to limited access to the surface structure at the nanoscale. However, our study sheds light on the importance of ligand-surface interactions in controlling the crystal structure of nanocrystals. Understanding these interactions is crucial for synthesizing nanocrystals with the desired properties and gaining insights into crystallization processes in general. In addition, it is known that bimetallic materials often show superior electrochemical performance to monometallic materials due to the synergistic effect of the two metal sites. Therefore, NiCoSe materials with different Ni
:
Co ratios are synthesized to further boost the electrocatalytic performance. The as-synthesized transition metal selenide catalysts are evaluated for hydrazine-assisted water splitting. Bimetallic NiCoSe displays superior electrocatalytic performance to pure-phase NiSe and CoSe. NiCoSe shows excellent activity toward hydrazine oxidation and requires a potential of 0.20 V vs. RHE to attain 10 mA cm−2. To achieve a high current density of 300 mA cm−2, it needs a potential of only 700 mV without the assistance of electrochemically active substrates such as Ni foam or Co foam. Moreover, NiCoSe displays excellent activity as a bifunctional catalyst by requiring a very low cell voltage of 0.45 V to attain a current density of 10 mA cm−2 for H2 production.
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Fig. 1 (a) Synthesis scheme of MSe (M = Ni, Co) synthesized with ligands. (b) PXRD patterns of NiCoSe synthesized with different Ni : Co ratios. | ||
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| Fig. 2 (a) Structures of the ligands used. (b) PXRD patterns of the synthesized materials with different carboxylic acid-containing ligands confirmed the formation of the crystalline NiSe phase. | ||
:
2 and 2
:
1 Ni
:
Co precursor ratios was also synthesized using a similar protocol. For ease of understanding, NiCoSe with Ni
:
Co = 1
:
1, 1
:
2, and 2
:
1 is represented as NiCoSe (1
:
1), NiCoSe (1
:
2), and NiCoSe (2
:
1), respectively.
:
Co ratios, such as NiCoSe (1
:
1), NiCoSe (1
:
2), and NiCoSe (2
:
1), are found to match well with the standard patterns of CoSe and NiSe phases. However, there is no evidence of peak splitting or additional reflections that would suggest the coexistence of distinct NiSe and CoSe phases. Instead, the diffraction pattern displays consistently shifted peak positions relative to the parent phases, indicating the formation of a homogeneous solid solution. This shift is attributed to the substitution of Co2+ ions into the NiSe lattice, which introduces lattice strain and alters the unit cell parameters. Such behavior is consistent with previous reports, including the study by Jiang et al.,39 where the incorporation of Ni into Co-based selenides resulted in noticeable peak shifts, confirming solid solution formation rather than phase separation.
Table S1 shows the binding free energy of formation for the [Ni(TAR)(H2O)4], [Ni(OXAL)(H2O)4], and [Ni(EN)3]2+ complexes from their aqueous complexes in the solution. The experimental conditions were considered, and an aqueous medium was simulated in the initial nickel species and in the medium of the reaction. The equations employed for the calculation of the binding free energy for the three complexes are as follows:
![]() | (1) |
![]() | (2) |
![]() | (3) |
A negative value of the calculated binding energy indicates that the formation of the complex is favorable, and a positive value indicates the opposite. As shown in Table S1, all three complexes have a favorable energy of formation from the aqueous medium. The [Ni(EN)3]2+ complex has the most negative binding energy of approximately −100 kcal mol−1, whereas the carboxylate complexes have about a fourth of that energy. This means that the [Ni(EN)3]2+ complex is highly stable. The reason for this may be that the entropy change associated with the formation (eqn (3)) is significantly different. Six water molecules are released in the formation of the [Ni(EN)3]2+ complex as compared to the two water molecules released in the case of the carboxylate complexes. The positive change in entropy associated with the formation of the former renders it more stable.
During experiments, it was observed that the [Ni(EN)3]2+ complex is not a good precursor for the formation of the nickel selenide crystal structure at room temperature. On the contrary, the two carboxylate complexes are suitable precursors, enabling the formation of nickel selenide crystals at room temperature. The reason for this is likely to be that the high stability of the [Ni(EN)3]2+ complex, compared with the carboxylate complexes, makes it less favorable to break and allows selenium to approach the nickel center. Interestingly, at elevated temperatures, the [Ni(EN)3]2+ complex has been observed to facilitate nickel selenide crystal formation. If the reaction switches to spontaneous at higher temperatures, this indicates that the reaction relies significantly on entropic factors. In the expression for free energy (ΔG = ΔH − TΔS), the free energy ΔG becomes more negative at higher temperatures when the change in entropy ΔS is positive. The change in entropy is greater when the carboxylate complexes are turned into nickel selenide crystals. Four water molecules and one tartrate/oxalate ligand are displaced in these cases. By contrast, if the [Ni(EN)3]2+ complex breaks, three EN ligands are freed from the complex. Hence, the change in entropy is less in the case of the [Ni(EN)3]2+ complex than in the cases of the two carboxylate complexes. Consequently, only when the temperature is increased, the breaking of the [Ni(EN)3]2+ complex tips the free energy balance from positive to negative, thus rendering this reaction spontaneous at higher temperatures.
Computational studies reveal that the [Ni(EN)3]2+ complex exhibits significantly higher stability than the carboxylate-based complexes. This enhanced thermodynamic stability reduces the likelihood of ligand dissociation, thereby limiting the accessibility of the nickel center to incoming selenium species. As a result, the formation of nickel selenide crystals from this complex is unfavorable under ambient conditions. In contrast, the nickel-tartrate and nickel-oxalate complexes possess moderate binding energies and are further stabilized by hydrogen bonding interactions between coordinated water molecules and carboxylate oxygen atoms. These interactions promote a more flexible coordination environment, facilitating the approach and incorporation of selenium into the nickel coordination sphere. Consequently, these carboxylate complexes act as effective precursors for nickel selenide crystal formation at room temperature. In the absence of dicarboxylic acid ligands, the lack of such stabilizing interactions and poor precursor integrity often result in incomplete reaction pathways, leading to the presence of unreacted elemental selenium in the final product, as confirmed by XRD analysis.
O stretching frequency of the carboxylic group is observed at 1637 cm−1, whereas for the pure ligand, the corresponding peak is observed at 1679 cm−1 (shown in Fig. S7a).33,40 For tartaric acid-capped NiSe, the peak belonging to the –C
O stretching frequency is observed at 1724 cm−1 and that of the ligand is observed at 1740 cm−1 (shown in Fig. S7b).41,42 In oxalic and tartaric acid-capped NiSe, the –C
O peak of the carboxylic acid shifts to relatively lower wavelengths. These spectroscopic changes suggest that oxalic and tartaric acids are attached to the nickel selenide surface through the carboxyl functional moiety.
:
1) (Fig. S9c) is 0.27 nm, corresponding to the (101) plane. To understand the spatial distribution of elements, the elemental mapping (shown in Fig. S9g–j) of the as-synthesized materials was performed. Elemental mapping images show the uniform distribution of elements (Ni, Co, and Se) in nickel cobalt selenide. To determine the elemental compositions, the EDAX analysis of the as-synthesized materials was carried out. The observed experimental ratios obtained from the atomic ratios of cobalt, nickel, and selenium for different samples are similar to the theoretical ratios (Table S2).
:
1) material. As shown in Fig. S10b, the peaks observed at 855.6 eV (Ni 2p3/2) and 873.1 eV (Ni 2p1/2) can be attributed to Ni2+, while the peaks present at 858.4 eV (Ni 2p3/2) and 876 eV (Ni 2p1/2) are attributed to Ni3+.43,44 The peaks at 778 eV (Co 2p3/2) and 793.6 eV (Co 2p1/2) in the Co 2p spectrum (shown in Fig. S10c) are attributed to Co3+. The peaks at 781 eV (Co 2p3/2) and 803 eV (Co 2p1/2) are characteristics of the Co2+ species.23,45 The broad peak at 59 eV in the Se 3d spectrum (shown in Fig. S10d) is associated with the oxidized selenium species (SeOx) as a result of surface oxidation. The two peaks at 54.3 eV and 55.3 eV belong to Se 3d5/2 and Se 3d3/2, respectively.46,47 All these results confirm the coexistence of Ni and Co in the as-synthesized NiCoSe (1
:
1) material.
:
1) requires a potential of 0.20 V vs. RHE to reach a 10 mA cm−2 current density. The corresponding potential values for CoSe and NiSe are 0.30 and 0.40 V vs. RHE, respectively. These results show that the bimetallic NiCoSe phase shows superior activity to individual NiSe and CoSe phases. Among the as-synthesized NiCoSe materials, NiCoSe (1
:
1) requires the lowest potential to attain 10 mA cm−2 compared to NiCoSe (1
:
2) (0.30 V vs. RHE) and NiCoSe (2
:
1) (0.38 V vs. RHE). Furthermore, a high current density of 300 mA cm−2 is attained at a potential of 700 mV without the use of any electrochemically active substrate, like Ni foam. Further electrochemical measurements were carried out using the NiCoSe (1
:
1) catalyst because it shows the best activity. The higher activity of NiCoSe is supported by a low Tafel slope of 65 mV dec−1 compared to CoSe (113 mV dec−1) and NiSe (184 mV dec−1) (shown in Fig. 3c). The observed lower Tafel slope for NiCoSe (1
:
1) suggests the faster kinetics of the electrochemical reactions on the NiCoSe catalyst.
Electrochemical impedance spectroscopic (EIS) analysis was performed at 0.3 V vs. RHE in 0.5 M hydrazine to understand the possible origin of the higher activity of the NiCoSe electrocatalyst. The observed charge transfer resistance (RCT) of NiCoSe (∼11.5 Ω) is lower than that of CoSe (∼50.5 Ω) and NiSe (∼71.5 Ω) (Fig. 3d). The ECSA measurement was performed to get a better insight into the developed catalyst.48,49 It is generally believed that the electrocatalytic activity of materials increases with an increase in their ECSA. However, due to the limitations of all the existing methods, the accurate determination of the ECSA is extremely challenging. Therefore, a qualitative comparison of the ECSA of the as-synthesized materials was obtained from the double-layer capacitance (Cdl) of materials measured in the non-faradaic region. The calculated Cdl value of NiSe (11.8 mF cm−2) is higher than those of CoSe (6.8 mF cm−2) and NiCoSe (2.0 mF cm−2) (shown in Fig. S11a–d). To find the intrinsic activity, the LSV curves were normalized by the ECSA (shown in Fig. S11e). Despite having the lowest ECSA, NiCoSe exhibits the highest current density when normalized by the ECSA, indicating superior intrinsic catalytic activity towards hydrazine oxidation compared to both NiSe and CoSe. This enhanced performance is attributed to the synergistic effect between Ni and Co in the bimetallic structure, which improves the electronic environment and reaction kinetics.50 Thus, we believe that the enhanced activity of NiCoSe is very likely due to the presence of more potent catalytic centers that can catalyze reactions with higher efficiency. Further, the durability of NiCoSe for the HzOR was analyzed using chronopotentiometry measurements. As shown in Fig. S12a, NiCoSe shows excellent stability of 32 h at a current density of 10 mA cm−2. The HzOR performance shows a significant rise in the potential requirement in 16 h. As previously noted in the literature, the rise in potential requirements may result from either the electrocatalyst deterioration or the consumption of hydrazine during the HzOR.12,51 After 16 hours, the electrolytic solution was swapped for a fresh one to confirm the reason for the increment in the potential requirement. The electrochemical performance of NiCoSe for the HzOR is restored and displays a similar trend for another 16 hours. To further validate the stability of the hydrazine oxidation reaction (HzOR), the linear sweep voltammetry (LSV) curves were recorded before and after the chronopotentiometry test in a fresh electrolyte containing 0.5 M Hz + 1 M KOH. The negligible change in the LSV profile confirms the excellent electrochemical stability of the NiCoSe catalyst during prolonged HzOR operation (shown in Fig. S12b). It confirms that the consumption of hydrazine leads to a decrease in activity; however, the electrocatalyst is stable
To further support the higher activity of NiCoSe compared with that of NiSe and CoSe, electrochemical impedance spectroscopy was performed at −0.20 V vs. RHE. The observed charge transfer resistance (RCT) value is lower for NiCoSe (∼9.1 Ω) than for NiSe (∼11 Ω) and CoSe (∼16.5 Ω) catalysts (see Fig. 4c). These results show that the superior activity of NiCoSe is due to faster kinetics, as reflected by the low RCT and Tafel slope. Additionally, the intrinsic activity of the synthesized catalyst toward the HER was calculated by ECSA-normalized LSV. Fig. S11f shows the electrochemically active surface area (ECSA)-normalized polarization curves for the hydrogen evolution reaction. NiCoSe exhibits the highest current density when normalized by the ECSA, indicating superior intrinsic catalytic activity compared to both NiSe and CoSe. Further, the durability of the best-performing HER electrocatalyst (NiCoSe) was evaluated by performing a 24 h chronopotentiometric analysis at 10 mA cm−2geo in 1 M KOH (Fig. 4d). The HER performance of NiCoSe (1
:
1) under continuous usage displays a negligible decrease even after 24 h, demonstrating the prominent durability.
Further, we have compared the catalytic performance of the NiCoSe catalyst with commercial Pt/C for the HzOR and HER. The polarization curves of commercial Pt/C in both the hydrazine oxidation reaction (HzOR) and hydrogen evolution reaction (HER) are shown in Fig. S13a and c. The NiCoSe catalyst exhibits a higher overpotential than Pt/C. Also, Pt/C exhibits a lower Tafel slope of 43 mV dec−1 in the HER compared to the 122 mV dec−1 measured for NiCoSe, suggesting faster HER kinetics in the case of Pt/C (shown in Fig. S13b). However, in the case of the HzOR, NiCoSe demonstrates a Tafel slope of 65 mV dec−1, which is reasonably close to the 48 mV dec−1 observed for Pt/C (shown in Fig. S13d). This suggests that NiCoSe possesses competitive intrinsic activity for the HzOR. Also, NiCoSe is composed of earth-abundant and low-cost materials, offering a more economically viable alternative for scalable applications. NiCoSe can be a promising alternative for scalable energy systems due to its high durability and affordability.
Furthermore, we have checked the OER performance of the NiCoSe catalyst. The LSV curve shows that the anodic potential for water oxidation is 1.62 V vs. RHE at 10 mA cm−2. An excess potential of 1.42 V is required for water oxidation in the conventional water electrolysis system (Fig. 5a). However, the HzOR can deliver a much higher current density than the OER at a low work potential, which depicts the significantly enhanced energy efficiency by replacing the OER with the HzOR. The above results depict that the NiCoSe catalyst is an efficient catalyst for the HzOR and HER. Thus, we checked the bifunctional activity of NiCoSe toward hydrazine-assisted water splitting (OHzWS) and compared its activity with the traditional overall water splitting system (OWS). For the electrochemical measurements, we used a NiCoSe electrode as the cathode and anode in a two-electrode setup for the overall water splitting. To attain a current density of 10 mA cm−2geo, the NiCoSe||NiCoSe couple requires a cell potential of 0.45 V in an electrolyte containing 0.5 M hydrazine and 1 M KOH and outperforms OWS (an electrolyte containing 1 M KOH), which requires 1.81 V (shown in Fig. S14). To understand the durability of the NiCoSe catalyst, a chronopotentiometry test was employed for 48 h at 10 mA cm−2. The bifunctional activity of NiCoSe under continuous usage shows a negligible decrease even after 48 h, demonstrating good durability in the two-electrode system (shown in Fig. 5b). To determine the rate of hydrogen production, the chronoamperometry (CA) measurement was performed at 0.85 V using the NiCoSe||NiCoSe couple, and hydrogen was detected at different reaction times with the help of an online gas chromatography setup. The hydrogen production rate is initially measured as 27 mL h−1 (2 min), which decreases to 22.1 mL h−1 (32 min) and 18.6 mL h−1 (56 min) with an increase in the reaction time, which is due to the consumption of hydrazine during the reaction, a common phenomenon observed in the case of hydrazine oxidation-assisted hydrogen production (Table S4 and Fig. S15). The above results show that the NiCoSe system, under alkaline conditions, is a promising electrocatalyst to promote hydrazine-assisted hydrogen production. Additionally, NiCoSe shows better electrochemical performance and stability than most of the reported chalcogenide-based bifunctional catalysts for OHzWS (Table S5).
:
1) has been simulated using density functional theory calculations. In NiCoSe (1
:
1), half the Ni atoms are replaced by Co in the lattice. The simulations elaborate on the experimental findings pertaining to the electrochemical properties of the material surfaces. Based on the XRD results, the [1 0 1] planes of NiSe and NiCoSe (1
:
1) have been considered as the catalytic plane.
The experiments have demonstrated the feasibility of the HzOR on the NiSe and NiCoSe (1
:
1) surfaces. Calculations were performed to investigate the free energy associated with the stepwise mechanism of the HzOR on both surfaces. The two energy profiles are overlaid in Fig. 6 for effective comparison. The [1 0 1] planes of NiSe (blue) and NiCoSe (1
:
1) (pink) have been considered for the binding of hydrazine and its oxidized successors. Fig. 6 shows the reaction pathways and corresponding energy changes for the HzOR on the two surfaces. The free energy profiles of the HzOR on the NiSe (blue) and NiCoSe (1
:
1) (pink) surfaces as a function of the reaction coordinate are shown. The profile labels are shown in the inset. Optimized geometries focused on the active site of binding are provided along the reaction pathway for both surfaces. The experiments have been performed under high-pH conditions. The following equations have been employed for the free energy calculations in alkaline media:
| N2H4 + *→ *N2H4 | (1) |
| *N2H4 + OH− → *N2H3 + H2O + e− | (2) |
| *N2H3 + OH− → *N2H2 + H2O + e− | (3) |
| *N2H2 + OH− → *N2H1 + H2O + e− | (4) |
| *N2H1 + OH− → *N2 + H2O + e− | (5) |
| *N2 → N2+* | (6) |
The materials are similar to each other in terms of their structures and unit cell geometries. The differences between the two are that in NiCoSe (1
:
1) (pink), half of the Ni atoms are replaced by Co. It is evident from Fig. 6 that a step with a rise in free energy is a rise for both, and a step with a drop is so for both. As observed in the experiments, both are viable and good materials for the HzOR. This matches the result obtained in the calculations, showing a net negative free energy change for both materials. In nearly all the steps of the mechanism, the potential for NiCoSe (1
:
1) is lower than that for NiSe. Additionally, the adsorption of N2H4 onto the catalytic surface is more favorable in the case of NiCoSe (1
:
1). In turn, the desorption of N2 in the last step requires more energy in the case of NiCoSe (1
:
1). These are reflected in the changes in the free energy between the adsorbed and desorbed species in both cases. The step of *N2H2 becoming *N2H1 is of particular interest. At this transition, in the case of NiSe, the rise in the energy is high, whereas for NiCoSe (1
:
1), the ΔG difference is lower. These three factors combined render the overall HzOR mechanism to be more favorable on the NiCoSe (1
:
1) surface as compared to the NiSe surface. These results corroborate the experimental findings.
:
1) electrodes were subjected to post-catalytic analyses after 10 h of chronopotentiometry. The post-catalytic PXRD pattern of NiCoSe (1
:
1) illustrated in Fig. S16a confirms the retention of the phase after the durability test. The XPS spectra of the Ni 2p, Co 2p, and Se 3d regions of NiCoSe (1
:
1) do not show any shift in the binding energy compared to the pre-catalytic sample (Fig. S16b–d). All these results confirm that NiCoSe is a robust and efficient catalyst for hydrazine oxidation.
:
1) compared to NiSe. The thermodynamic advantages lie in the stronger adsorption of species on the NiCoSe (1
:
1) surface, the lowered energy for each step, and the less drastic energy changes between one step and the next in the case of NiCoSe (1
:
1).
The supplementary information file consists of instrumentation details, material details, synthesis details, electrochemical measurement details, and computational details. PXRD, SEM, TEM, HRTM, EDS, FTIR, TGA, XPS analysis for materials used for control studies, optimized geometries of nickel complexes used in computational analysis, computed binding free energy for the formation of the nickel complexes, Cdl and CV plot of different catalyst, table for calculated ECSA, ECSA normalized LSV for HzOR and HER, CP curve for HzOR stability, LSV after stability for HzOR, electrochemical performance of Pt/C for HzOR and HER, table for calculated H2 production values, comparison of OHzWS and OWS for the NiCoSe || NiCoSe couple, PXRD and XPS analysis of post-catalytic samples, comparison table for NiCoSe OHzWS performance with other reported transition metal chalcogenide-based bifunctional OHzWS electrocatalysts. See DOI: https://doi.org/10.1039/d5nr02653a.
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