Rajesha Kumar Swain†
,
Aranya Kar†,
Aditi Halder
and
Chullikkattil P. Pradeep
*
School of Chemical Sciences, Indian Institute of Technology Mandi, Mandi, Himachal Pradesh – 175005, India. E-mail: pradeep@iitmandi.ac.in; Fax: +911905267 009; Tel: +91 1905 267 045
First published on 13th August 2025
Enhancing the electrocatalytic performance of metal–organic frameworks (MOFs) remains a key challenge in energy materials research. In this study, the cobalt-based zeolitic imidazolate framework ZIF-67 (Z67) was modified using an all-inorganic coordination polymer, {(H2O)2K-μ-(H2O)3Ni(H2O)3}2n[V10O28]n (NiV10), which introduces both nickel (Ni) centers and decavanadate (V10) polyoxometalate (POM) clusters into the framework. An in situ synthetic approach was employed to generate a series of nanocomposites (25NZ67, 50NZ67, and 75NZ67) by varying the amount of NiV10 added during Z67 synthesis. The integration of Ni2+ and V10 clusters led to a significant structural reorganization in the Z67 framework, leading to the formation of a more open architecture, unlocking coordinatively unsaturated metal active sites (CUMAS), and enriching the material with abundant electroactive centres. Electrochemical evaluation revealed significantly improved oxygen evolution reaction (OER) performance for all composites compared to pristine Z67. The onset potential for all three composites was in the range of 1.44–1.46 V. The composite 75NZ67 exhibited an overpotential of 350 mV at j = 10 mA cm−2, which was ∼200 mV and ∼130 mV lower than Z67 and NiV10, respectively, at the same current density. Further, 75NZ67 exhibited the highest OER activity, with a 3-fold increase in current density compared to pristine Z67. It also displayed an improved Tafel slope of 120 mV dec−1, outperforming most of the control compounds studied and Z67 (144 mV dec−1). The encapsulation of POM within the ZIF cavity reduces the charge transfer resistance, leading to improved electrochemical performance during OER, as evidenced by the linear sweep voltammetry (LSV) curves. Notably, 25NZ67 demonstrated the best long-term stability, maintaining its performance over extended operation, and also the highest intrinsic activity when normalized by electrochemical surface area (ECSA). Control experiments confirmed that the enhanced activity arises from the synergistic effect of Ni doping and V10 encapsulation, achievable only via the in situ synthetic route. This work highlights a room-temperature in situ design strategy for Z67-based electrocatalysts by leveraging transition metal–polyoxometalate hybridization for improved OER performance.
ZIF-67 (Z67) is one of the most widely studied zeolitic imidazolate frameworks (ZIFs) containing cobalt as the metal center and 2-methylimidazole (2-MeIm) as ligands. It serves as a potential candidate for OER electrocatalyst but suffers from poor intrinsic activity. The Co centres in Z67 are coordinatively saturated, hindering the adsorption of water molecules. Various strategies have been adopted to tackle this drawback and fine-tune the electrocatalytic activity of pristine Z67.10,11 These include, synthesizing bi-metallic ZIFs,12,13 thermal treatment,14,15 composite formations,16,17 and encapsulating other catalytically active materials in ZIF cavities.18–20 Such strategies lead to the formation of coordinatively unsaturated metal active sites (CUMAS) in the ZIF framework, boosting its electrocatalytic activity. In terms of incorporating a second metal, Ni-doped ZIFs have been a popular choice. Introduction of Ni modifies the electronic environment of cobalt centres in Z67, improving intrinsic catalytic activity and facilitating the formation of active NiOOH and CoOOH species. Even very low concentrations (0.001 M) of Ni2+ have been reported to significantly boost the OER performance of Z67.21 Li and co-workers designed Co–Ni bimetallic metaphosphate nanoparticles (Co1.6Ni0.4P4O12-C) derived from a Co–Ni ZIF, which showed appreciable alkaline OER activity. Their DFT calculations revealed that Ni doping resulted in facile binding of the oxygenated intermediates to the catalyst surface.22 Liu et al. also reported the synthesis of ZIF-67@Ni@FeOOH composite employing a dual approach of doping Ni in Z67 framework and simultaneous structural defect engineering by FeOOH. The material displayed high electrocatalytic OER activity and also revealed NiOOH and CoOOH formation during the reaction, as the active species.23
Notably, another widely used strategy of Z67 activation is encapsulation of other catalytically active materials such as POMs, which are nanosized metal oxide clusters of early transition metals (Mo, W, V and Nb) present in their highest oxidation state.24 They are potential precursors for multifunctional materials due to their nanosized architecture, robust nature, highly polarized oxygen-rich surface, and innate catalytic qualities.25–27 POMs also have significant benefits in electrocatalysis due to their excellent redox properties, ability to act as electron shuttling units, selectivity, and corrosion resistance, which make them useful as adaptable inorganic ligands for OER electrocatalysts.25,27–29 K. Abdelkader et al. successfully synthesized Z67@POM hybrids using a tri-cobalt substituted lacunary Keggin POM ([SiW9Co3O40]). The material exhibited superior OER performance due to the synergistic interaction between POM and Z67 and the structural distortions of Z67 in the material.30 In another notable work, Li and co-workers reported a unique yolk/shell structured Z67@POM catalyst with a Keggin ([PW12O40]3−) POM. The structural arrangement showed POM nanoparticles coated on Z67, and the synergistic effect of the two components resulted in its high activity as an OER electrocatalyst.17 Recently, vanadium(V) based materials have also gained much interest for applications like rechargeable batteries,31 supercapacitors,32 and OER electrocatalysts,31 due to their excellent electrochemical properties and high earth abundance. Among the different POM variants, vanadium-based POM decavanadate (H2[V10O28]4−), has scarcely been explored for electrocatalysis despite its potential.32–34 Meanwhile, Wei and co-workers have reported that the doping of pentavalent V in the spinel oxides (Co3O4 and NiFe2O4) can enhance their activity and stability toward electrocatalytic OER application.35
The above discussions imply that different strategies can activate a metal–organic framework, such as Z67, towards electrocatalytic OER. A combination of such strategies can certainly lead to interesting catalytic materials.36 In this study, we investigate the activation of Z67 for electrocatalytic OER by incorporating a nickel-decavanadate-based all-inorganic coordination polymer, {(H2O)2K-μ-(H2O)3Ni(H2O)3}2n[V10O28]n (NiV10). Here, Z67 host was synthesized in a simple room-temperature in situ method in the presence of pre-dissolved NiV10 polymer. This approach was designed to enable both the doping of heterometal (Ni2+) ions into the Z67 framework and the encapsulation of a POM unit, decavanadate (V10) cluster, within the Z67 cavities simultaneously. The labile aqua ligands coordinating the Ni centres in NiV10 are expected to dissociate under synthetic conditions, facilitating Ni incorporation and cluster encapsulation during Z67 formation. In this way, three composites (25NZ67, 50NZ67, and 75NZ67) were synthesized by varying the amount of NiV10 introduced (25/50/75 mg) into the Z67 synthetic medium (Scheme 1). Structural and spectroscopic analyses confirmed both the doping of Ni2+ and the distribution of V10 clusters within the cavities and on the surface of the Z67 framework. These modifications led to the formation of a more open architecture, unlocked coordinatively unsaturated metal active sites (CUMAS), and enriched the material with abundant Co3+ electroactive centers.18,19 Electrochemical evaluation revealed significantly improved OER performance for all composites compared to pristine Z67, with 75NZ67 exhibiting the highest activity, while 25NZ67 demonstrated the best long-term stability. Our strategy reported here is different from some of the previously employed strategies37–41 to modify ZIFs and its significance is also underscored by the fact that our catalysts (25/50/75NZ67) outperformed some of the previously reported Z67 based OER catalysts (Co-ZIF-9 (510 mV),37 ZIF-67/NPC-2 (410 mV)38 and ZIF-8@ZIF-67@POM (490 mV)16) in terms of overpotential (η) value at 10 mA cm−2 of current density by a margin of ca. 40–140 mV. These results highlight the effectiveness of combining metal substitution and POM encapsulation to engineer MOF-based electrocatalysts with enhanced activity and durability for alkaline OER.
Fig. 1a shows the FT-IR spectra of Z67, NiV10, and all three as-prepared composites. The characteristic peaks of 2-MeIm appeared at 694 cm−1 (C–H bending), 752 cm−1 (C–H bending), 994 cm−1 (=C–H in-plane bend), 1380 cm−1 (CH3 asymmetric bend), 1424 cm−1 (CH2 asymmetric bend) and 1585 cm−1 (CN stretch). Additionally, the peak at 421 cm−1 represents the Co–N stretching mode, which confirms the presence of Z67 in all the composites.39,40 The FT-IR spectra of the composites also indicated the presence of V10 clusters, as evident from the peaks at 983 and 840 cm−1, ascribed to the terminal V
O bond stretches, and weaker peaks at 809 and 530 cm−1 corresponding to the symmetric V–O–V vibrations.34 In all the composites, a peak broadening was noticed between 550 and 950 cm−1, indicating the interaction between Z67 and the V10 clusters of NiV10.41 This peak broadening increases from 25NZ67 to 75NZ67, pointing to the increased V10 content in the composites.
The XRD pattern of the as-synthesized Z67 (Fig. 1b) exhibited the characteristic peaks at 7.4°, 10.5°, 12.6°, and 17.8°, corresponding to the (011), (002), (112), and (222) diffraction planes, respectively, confirming the formation of pure phase Z67 (Fig. S1).40,42 The XRD patterns of the composites closely resembled that of Z67, indicating that the Z67 crystal structure remains largely intact during composite formation, as expected. NiV10, due to its labile linkage between Ni and decavanadate centers, forms decavanadate clusters and Ni2+ hydrated species in solution. Given that the decavanadate POM has a size of approximately 0.8–1 nm, it can fit within the 1.16 nm cages of Z67, resulting in its effective encapsulation and preventing the formation of any separate crystalline phase in the composite (especially for lower loading samples like 25NZ67). Additionally, the POM becomes highly dispersed in these composites at a molecular or sub-nanometer scale, which prevents it from exhibiting distinct crystalline peaks in the PXRD pattern. Similar observations have been reported where POM incorporation does not alter the host framework diffraction due to the absence of long-range ordered POM domains.16,19 The average crystallite size of Z67, determined using the Scherrer equation, was 50.11 nm, which decreased to 40 nm in 25NZ67.18,19 In 50NZ67 and 75NZ67, the crystallite sizes were 39 nm and 38 nm, respectively. This decrease in the crystallite size indicates that the interaction between the V10 and Z67 seems to interfere with the growth of Z67 crystals, making them smaller, as reported earlier.18,19 Along with that, the overall crystallinity of the samples also showed a decrease when moved from Z67 to 75NZ67, as evident from the decreased intensity of the PXRD peaks.
To evaluate the surface area and pore sizes of the 25/50/75NZ67 composites, we analysed their N2 adsorption–desorption isotherms, see Fig. 2. The results revealed a consistent decrement in the BET surface area of all composites compared to Z67 (1102.99 m2 g−1). Further, it can be noted that the surface area consistently decreases with increasing feed ratio of NiV10 loading in the composites, from 764.97 m2 g−1 for 25NZ67 to 483.54 m2 g−1 for 50NZ67 and 356.10 m2 g−1 for 75NZ67. These observations are also consistent with the previous reports.17,18 The incorporation of V10 clusters into the pores and the surface of Z67 particles is responsible for this decrease in surface area. Along with the decrement in BET surface area, a gradual decrease in the pore volume of the materials was also observed as the NiV10 loading increased. Furthermore, the average pore diameter showed a gradual increment while moving from Z67 to 75NZ67 (Table S1), which can be attributed to the formation of a more open Z67 framework and also the destruction of the small windows due to POM encapsulation.43
The compositional analyses of Z67 and the nanocomposites were elucidated using ICP-MS, and the results are presented in Table S2. In the composites, as the concentration of NiV10 increases, the amount of vanadium (i.e., mmol of vanadium per gram composite) also increases, with values of 0.84, 1.58, and 1.94 for 25NZ67, 50NZ67, and 75NZ67, respectively. However, the Ni/V ratios observed for the composites (0.008–0.017) were much lower than that in the pristine NiV10 (0.2). This suggests a substantial detachment of Ni units from the NiV10 framework during the composite formation process.
TGA was conducted on all samples to assess their thermal stability and validate their successful synthesis (Fig. S6). Notably, two distinct weight-loss regions were observed across all composites. The initial weight reduction observed up to 250 °C is attributed to the loss of solvated or coordinated water molecules in all composites. The pristine Z67 exhibited weight loss in the 550 to 750 °C temperature range due to framework collapse. This phenomenon occurs at lower temperatures, i.e., between 450 and 550 °C, for all the composites, which indicates the opening of the Z67 framework in these composites due to interactions between V10 and Z67. Further, as the concentration of V10 increases in the composites, a corresponding decrease in the overall weight loss % was noted, resulting in a higher residual mass of 25/50/75NZ67 than Z67, as expected.
Following this, TEM images of the materials were acquired to gain further insights into their structural features. The Z67 particles displayed a characteristic hexagonal morphology with a smooth, finely textured surface (Fig. 5a). In comparison, the particles in all three composites (25/50/75NZ67) exhibited a notably rougher and more rugged surface texture than the original Z67 particles, which can be attributed to incorporating V10 POM from NiV10. With increasing concentration of NiV10, some sheet-like aggregates were observed inside the Z67 units and on their surface, fewer in 25NZ67 (Fig. 5b), more in 50NZ67 (Fig. 5c) and maximum in 75NZ67 (Fig. 5d). These are speculated to be the POMs, confirmed by the high-resolution TEM (HRTEM) images and elemental mapping at these positions, as discussed later. Images of individual particles from each composite (Fig. 5e-h) reveal the retained hexagonal morphology of Z67, along with rough edges and areas of dark contrast within the particles, further indicating the incorporation of POM units. The TEM analysis results of 50NZ67 and 75NZ67, corroborated with their FESEM analysis, revealed an open structure of Z67 particles with POM units distributed both inside the pore and on the surface of the particles (Fig. 5g and h). Elemental mapping showed that the sheet-like aggregates inside and on the surface of Z67 particles in these composites contained a significant % of V and O, suggesting that these are the POM units (Fig. 5i–l). As shown in Fig. S14–S19, elemental mapping clearly revealed the V, Ni, Co, K and O distribution in all these composites. Notably, the POM-enriched regions, identified as bright spots in the V mapping, are distinctly distinguishable from the nearly POM-free zones. Compared to V and O, the Ni patterns seem scattered in the whole region, similar to Co but in much less concentration, suggesting the presence of Ni along with Co in the whole Z67 framework. The HRTEM images of the 25/50/75NZ67 revealed lattice fringes with a d-spacing of 0.24 nm, equal to that of the V10 POM (0.24 nm) (see Fig. S20). Additional TEM images of the materials are given in Fig. S21. Moreover, these fringes were exclusively found in the highlighted (blue circle) region of the composites. The observed d-spacings have also been confirmed by analyzing the selected area electron diffraction (SAED) patterns of the materials, as shown in Fig. S22. Based on all the structural and morphological analyses carried out, it can be concluded that all three composites show similar structural features. In all of them, some amounts of V10 clusters are encapsulated inside the Z67 cavities, along with the distribution of excess POMs on the surface of the Z67 particles, as revealed by the SEM and TEM data. This can also be seen from the BET data, which shows a decrease in surface area with increasing concentration of NiV10 in the composite. Apart from this, incorporating a few Ni centres in the Z67 framework is anticipated from the ICP data, which shows the Ni/V ratio is much lower than it should be if the NiV10 structure were intact in the composites. More indication of the same can be seen in the XPS data, where a higher % of the mixed valent state of Co (resulting from the formation of CUMAS) and the presence of Ni can be observed as a result of V10 encapsulation and Ni incorporation. Further, the HRTEM analysis of the composites showed d-spacing values matching with the decavanadate POM, proving its distribution inside and outside the Z67 framework. Alongside, the elemental mapping of the composites showed that the distribution of V was concentrated in the regions where the outgrowths were mainly observed, while the distribution of Ni appeared uniformly all over the framework. This again supports the fact that the Ni centres have uniformly replaced some Co centres in the Z67 framework in the composites.
The redox behaviours of the materials in a 0.1 M KOH medium were analyzed using CV scans at a scan rate of 10 mV s−1 (Fig. S23). For all the materials under investigation, a characteristic distinct anodic peak around 1.12–1.18 V was observed, attributed to the Co2+ to Co3+ transition, while the corresponding reduction peak was observed around 1.02 V.52,53 Compared to the characteristic Co2+/Co3+ oxidation peak of Z67, all three composites exhibited a shift to lower potential, which could probably be related to electron transfer between Z67 and decavanadate POM units, indicating a synergistic interaction between the two components as previously been shown in the XPS analysis. The encapsulation of the V10 clusters inside Z67 cavities induced structural modifications to the Z67 framework, resulting in the opening of Z67 frameworks, leading to an increased number of Co centres undergoing redox processes. This also enhanced the electrochemical activity, as more intense and wider redox couples for the composites can be observed compared to those in pristine Z67.
For a better understanding of the synergistic interactions within the composites, we prepared a control sample, Z67+NiV10, as a physical mixture of Z67 and NiV10 through a simple room-temperature grinding method. The CV scans for Z67, NiV10, 25NZ67 and Z67+NiV10 are presented in Fig. 6a. The Co2+/Co3+ couple in Z67 and 25NZ67 is denoted as A1/C1 and A5/C5, respectively, while the Ni2+/Ni3+ couple in NiV10 is denoted as A2/C2. Notably, in Z67+NiV10, two distinct redox couples A3/C3 and A4/C4 were observed. The A3/C3 couple corresponds to the A2/C2 couple seen for NiV10, while the A4/C4 couple is analogous to the A1/C1 couple of Z67. This observation confirms that Z67 and NiV10 exist as separate components in Z67+NiV10. In contrast, 25NZ67 displays a single redox couple (A5/C5) shifted to a lower potential than the A1/C1 couple, a behaviour not present in the physical mixture. This indicates that the in situ prepared composites facilitate a reorganization of the NiV10 components, where some V10 clusters become encapsulated in the pores of Z67, and some Ni centres are incorporated into the Z67 framework. Such unique arrangements are not achievable through simple physical mixing, highlighting that the synergistic effects of the components can only be realized when the composite is synthesized in situ. The less resolved Ni2+/Ni3+ peak in the composites is not visible in the CV scans. This could be due to the large current density in the same potential region due to catalytic water oxidation, which masks the weaker Ni2+/Ni3+anodic peak. As anticipated, the Ni2+ to Ni3+ oxidative peaks in all three 25/50/75NZ67 composites are resolved in the DPV, as shown in Fig. S24.
We also prepared several control samples to assess the roles of the proposed Ni doping and in situ synthetic procedure in determining the OER activity of the composites 25/50/75NZ67. First, we prepared a control sample, 25VZ67, using only the sodium salt of decavanadate (Na6[V10O28]) instead of NiV10 and keeping all other synthetic conditions unaltered. Therefore, in 25VZ67, any possible Ni doping of Z67 is prevented. Our second control sample was Z67+NiV10, a physical mixture of Z67 and NiV10. This control compound was used to understand the potential role of the in situ synthetic conditions in composites 25/50/75NZ67. Finally, to investigate the role of low-concentration nickel in the composites, we prepared two additional control samples by introducing nickel salt directly into the Z67 and 25VZ67 systems, resulting in composites 25NiZ67 and 25(Ni+V)Z67. Fig. 6c compares the LSV scans of 25NZ67 with the control samples, where the in situ prepared 25NZ67 composite showed a much better current density, lower onset, and a lower overpotential than all four control samples (25VZ67, Z67+NiV10, 25NiZ67 and 25(Ni+V)Z67). This observation confirms that better electrocatalytic activity of the in situ synthesized composites stems from the synergy of three components, i.e., Z67, V10 and Ni centres. Such a synergy is not achievable by combining Z67 with V10 alone, even under in situ conditions, or by physically mixing Z67 and NiV10, or by introducing Ni separately into Z67 and 25VZ67 systems. The observed increment in the current density of the in situ generated composites 25/50/75NZ67 could be attributed to the generation of more undercoordinated Co and Ni centres in the modified Z67 framework. Alongside this, the encapsulation of the V10 POMs in the Z67 pores could be responsible for lowering the overpotential for OER. The characterization data for the control samples (FT-IR, XRD, and XPS) are given in Fig. S26–S33.
CV scans of Z67 and 25/50/75NZ67 were recorded in a non-faradaic region at variable scan rates (100 mV s−1 to 600 mV s−1) to calculate electrical double layer capacitance (Cdl), as shown in Fig. S34 and S35. The estimated Cdl values for the 25/50/75NZ67 composites were 0.29, 0.38, and 0.48 mF cm−2, respectively. In contrast to Z67, which has a Cdl value of 0.14 mF cm−2, all composites demonstrated higher Cdl values. The observed rise in the Cdl values of the composites suggests rougher areas on the electrode and more active sites within the composites.55 The intrinsic activity of the electrocatalysts was evaluated by normalizing the average current densities from their LSV curves to their respective electrochemical surface area (ECSA). ECSA was calculated from the obtained Cdl values and considering a standard specific capacitance (Cs) value of 0.040 mF cm−2 according to similar reports56 (Fig. S36). From this analysis, we observed that 25NZ67 exhibits the highest intrinsic activity among all composites, suggesting that the synergistic interactions between the three components (Z67, POM and Ni centres) in 25NZ67 enhance the activity of cobalt centres in the composite. For the higher loading composites (50NZ67 and 75NZ67), although they showed better intrinsic activity than pristine Z67, their intrinsic activity was lower than 25NZ67. This indicates that in higher loading composites (50- and 75NZ67), the enhanced overall current density arises predominantly from new active sites created by POM encapsulation and increased nickel content.
To get an insight into the kinetics of OER, the Tafel slopes (TS) of the materials were calculated from their LSV scans (Fig. S37). Among all the materials tested, 75NZ67 exhibited the lowest TS value of 120 mV dec−1, compared to 50NZ67 (126 mV dec−1) and 25NZ67 (133 mV dec−1). For OER electrocatalysis, a low TS value suggests faster reaction kinetics. As reported earlier, high TS values signify sluggish rate-determining steps involving the adsorption of OH− on active sites, as in the case of Z67 and other control samples. Consequently, the lower TS values suggest facile adsorption of OH− groups onto the active sites, which is a direct consequence of the more open structures in the composites.18 These results confirm that faster OER kinetics depends on the concentration of decavanadate POM and the Ni centres within the composites. Additionally, the faster kinetics observed for the composites 25/50/75NZ67, compared to the control samples, underscores the importance of component synergy for achieving improved kinetics. A comparative plot of the overpotential @ j = 10 mA cm−2 and Tafel slope values of all the materials studied are given in Fig. 6d.
To investigate the electron transport capabilities of the composites 25/50/75NZ67, electrochemical impedance spectroscopy (EIS) measurements were conducted at a steady potential of 1.55 V (Fig. 7). The impedance data were analysed using a Randles equivalent circuit, depicted in the inset of Fig. 7. In this model, Rs represents the solution resistance, while Rct and Cdl correspond to the charge transfer resistance and the double-layer capacitance, respectively. The addition of a constant phase element (CPE) in the circuit arises from the non-ideal behaviour and complexity of the electrode/electrolyte interface.57 In the Nyquist plot, the diameter of the semicircles corresponds to the charge transfer resistance (Rct). Notably, the 25NZ67 composite exhibited a considerably lower Rct of 50.05 Ω compared to the pristine Z67, which has an Rct of 172.60 Ω. In the case of higher POM-loaded composites 50NZ67 and 75NZ67, the Rct values decreased further to 47.61 Ω and 44.06 Ω, respectively. These findings suggest that the encapsulation of POM within the ZIF cavity reduces the charge transfer resistance, leading to improved electrochemical performance during OER, as evidenced by the LSV curves. Other circuit fitting parameters are given in Table S4. Using the Rs value obtained from the EIS circuit fitting, the iR-corrected LSV plot was calculated (Fig. S38), which showed that 75NZ67 was the most active electrocatalyst for OER. A comparison plot of the η values at j = 10 and 20 mA cm−2 is given in Fig. S39.
![]() | ||
Fig. 7 EIS data of Z67 and 25-75NZ67 measured at a steady potential of 1.55 V vs. RHE (inset: the fitted circuit model). |
Chronoamperometry was employed to evaluate the stability of the composites as OER electrocatalysts. The oxygen bubbles formed on the electrode surface are the source of the distinctive local current density reductions seen in the chronoamperometric plots shown in Fig. S40. Rotation of the electrode causes the bubbles to release, regaining some or all of the prior current density values.58,59 As shown in Fig. 8a–c, the 25NZ67 composite demonstrated an approximately 8% increase in current density after an 8-hour chronoamperometry test, while the 50NZ67 composite exhibited a negligible 1% decrease. In contrast, the 75NZ67 composite experienced a significant decrease of 23% in current density. Regarding overpotentials at j = 10 mA cm−2, the 25NZ67 composite maintained the same overpotential, whereas the 50NZ67 composite showed an increase of 10 mV, and the 75NZ67 composite exhibited a 40 mV increase compared to the values before chronoamperometry (Fig. 8d). These variations in behaviour among the composites can be attributed to their distinct structural arrangements. The results indicate that the overall stability of the composites under OER conditions decreases as the POM content increases, highlighting the critical role of POM concentration for the long-term OER performance of these composites.
Due to the instability of POMs in the alkaline media, pristine NiV10 showed a decrease in current density (∼8%), an increase in overpotential, and thus a poor overall stability after 8 h chronoamperometry, as reported earlier.34 With 25NZ67, we successfully addressed the instability issue that was faced in the case of pristine NiV10, as we didn't observe any decrease in current density or change in overpotential during the 8 h chronoamperometry. For the other two composites, 50NZ67 and 75NZ67, we hypothesize that due to comparatively more open polyhedral geometry and excess POMs on the surfaces of the Z67 framework, there is a high possibility of POM leaching from the surface, resulting in a decrease in current density and an increase in overpotential, as observed. To prove our hypothesis, we recorded the UV-vis spectra of the recovered electrolytes of 25/50/75NZ67 post-chronoamperometry (Fig. S41). The UV-Vis spectrum of NiV10 in a 0.1 M KOH solution was taken as a reference sample, which displayed two peaks around 220 nm and 265 nm, assigned to the charge-transfer transition of the type π(O) → d(V) of the decavanadate POM.60,61 Notably, the recovered electrolytes of 50NZ67 and 75NZ67 after the 8 h chronoamperometry experiment also showed a broad peak around 220 nm, indicating the leaching of vanadium species from the surface, which likely caused the reduction in OER activity. However, such leaching was not observed with the 25NZ67 composite, suggesting it is sufficiently stable under the given conditions.
To assess the post-OER stability of 25NZ67, we conducted extensive analyses using FT-IR, XRD, XPS, SEM and TEM on the recovered sample after chronoamperometry. FT-IR spectra of the fresh and recovered 25NZ67 (Fig. 9a) revealed a decrease in the peak intensity, probably due to the very low amount of the sample recovered and used for IR studies and also due to the presence of acetylene black in the ink used for sample preparation for chronoamperometry. Apart from the decreased peak intensity, nearly all the peaks of the recovered 25NZ67 matched with the fresh catalyst, suggesting the catalyst's unaltered structure. The XRD pattern of the recovered catalyst (Fig. 9b) exhibited similarities to that of the fresh catalyst, with a higher signal-to-noise ratio attributable to amorphous acetylene black and a small amount of sample. This observation indicates no significant structural changes in the composite. The XPS results also indicated a similar elemental composition of the recovered and fresh catalysts. Furthermore, the deconvoluted Co 2p scan of the recovered 25NZ67 composite clearly depicted characteristic peaks of Co2+ (798.56 and 783.24 eV) and Co3+ (796.55 and 780.80 eV), along with their satellite peaks (Fig. S42). Despite some noise in the deconvoluted V 2p scan due to the limited sample recovery, the characteristic peak of V5+ remained discernible (Fig. S43). The FESEM images of the recovered catalyst (Fig. S44) showed mostly the morphology of acetylene black as spherical particles; however, some Z67 polyhedra were still identifiable. The TEM and HRTEM images of the recovered catalyst showed a much clearer presence of the Z67 particles and revealed a d-spacing of 0.24 nm, as seen for the fresh catalyst (Fig. 9c and d). These post-catalytic experiments demonstrate that the 25NZ67 composite retains its structural integrity and activity under OER conditions.
Although a full explanation of the underlying mechanism is unclear, our initial studies provide some insights into the characteristics of active sites in the OER process. Wu et al. reported that there are four sequential electron-transfer phases in the OER mechanism in alkaline media, as follows:
OH− + * → OH* + e− |
OH* + OH− → O* + H2O + e− |
O* + OH− → OOH* + e− |
OOH* + OH− → O2 + H2O + e− |
According to their report, for Z67, the rate-determining step (RDS) is the formation of OOH* from O*, which has a high energy barrier. They also documented, by DFT calculations, that upon the incorporation of a second transition metal ion into the Z67 framework (Zn, Ni or Cu), the adsorption of O*, OH*, and OOH* is strengthened altogether, which facilitates the decrement of energy barrier for the RDS. This aids in better electrocatalytic OER activity for the modified Z67.62 Fernandez and co-workers have reported a bidirectional synergy upon encapsulating a Keggin POM inside Z67. The encapsulation resulted in the generation of CUMAS, which served as active centres for electrocatalytic OER.19 In the same line of discussion, Co and a low concentration of Ni were identified as active metals in the present case. This was evidenced by the enhanced OER activity observed for all synthesized composites containing Ni compared to Z67, which lacks Ni. Also, the composites 25/50/75NZ67 showed better OER activity in terms of overpotential, current density and TS values than 25VZ67, a control compound prepared by replacing NiV10 with simple V10 clusters during synthesis. A physical mixture of these components (Z67+NiV10) further demonstrated that the mere presence of NiV10 is not enough for enhanced activity, which is achieved by the in situ synthesis. Thus, in 25NZ67, the incorporation of a second metal center (Ni) in the Z67 framework increases the overall active sites for electrocatalytic OER, which is evident from the integrated area of the LSV scans (Fig. S25). Also, the presence of Ni could make the adsorption of OH− more feasible onto the catalyst surface, thus making the reaction easier. The second component of our composite, V10 clusters, on the other hand, plays the crucial role of modulating the local coordination environments in Z67 framework, thus generating CUMAS, which helps in shifting the oxidation potential of the Co2+ centres to lower values, and also decreasing the overpotential for OER by facilitating a better charge transfer in the composites. Thus, the overall activity observed for the 25NZ67 is proposed to be a cumulative effect of the two strategies: (i) incorporation of a second transition metal in the Z67 framework and (ii) encapsulation of POMs inside the Z67 pores that were used for modification of Z67. Further, incorporating V10 clusters in the composite helps to reduce its charge transfer resistance, as revealed by the RCT values calculated from the impedance measurements, contributing to the enhanced electrocatalytic OER activity of the composite.
A comparison of the current results with the OER parameters of similar ZIF and POM-based catalysts is given in Table S5. In a large number of strategies employed to enhance Z67's OER activity,63 researchers rely on high-temperature annealing, which destroys its inherent porous framework.15,64 Other common approaches employed for activating ZIFs include metal ion doping,13,65 POM hybridization,66–68 carbonization, and forming composites with conductive supports.69 While metal doping improves intrinsic activity by tuning the electronic structure, it risks distorting the ZIF framework. Simple POM hybridization introduces additional redox-active sites but often suffers from leaching issues. Carbonization enhances conductivity but sacrifices porosity and structural integrity, while conductive composites improve electron transport but usually require complex multi-step synthesis. In contrast, our approach uses NiV10 as a single precursor to simultaneously incorporate both nickel centres and decavanadate POM units at room temperature, without using any harsh reaction conditions. This strategy maintains the original Z67 structure with only minor modifications (especially at lower loading of NiV10), avoids harsh processing, and achieves strong synergistic electronic and redox interactions with low Ni content, offering a simpler and more effective route to enhance the electrocatalytic OER performance.
The same synthetic protocol was employed to synthesize the 50NZ67 and 75NZ67 composites as well, using 0.050 and 0.075 g of NiV10, respectively.
During the synthesis of the composites 25/50/75NZ67, the amounts of Co2+ salt and 2-MeIm (used for obtaining Z67) were kept constant in all the cases; only the NiV10 amount was varied to increase the loading amount sequentially. In that sense, the increasing amounts of NiV10 incorporated in these composites are with respect to the weight of the Z67 counterpart.
Footnote |
† These authors contribute equally to the manuscript. |
This journal is © The Royal Society of Chemistry 2025 |