Open Access Article
Thi Kim Cuong Phu
a,
Ngoc-Trung Nguyena,
Phi Long Nguyen
ab,
Ngan Nguyen Le
*cd and
Thi Viet Bac Phung
*ae
aCenter for Environmental Intelligence, VinUniversity, Hanoi, Vietnam. E-mail: bac.ptv@vinuni.edu.vn
bSchool of Electrical and Electronic Engineering, Hanoi University of Industry, Hanoi, Vietnam
cInstitute of Applied Science and Technology, Van Lang School of Technology, Van Lang University, Ho Chi Minh City, Vietnam. E-mail: ngan.ln@vlu.edu.vn
dFaculty of Applied Technology, Van Lang School of Technology, Van Lang University, Ho Chi Minh City, Vietnam
eCollege of Engineering and Computer Science, VinUniversity, Hanoi, Vietnam
First published on 15th May 2026
Oxygen vacancies (OV) in metal oxide electrocatalysts are broadly regarded as pivotal factors that improve electrochemical catalytic efficiency in water splitting. However, the intrinsic properties of catalysts also play an important role in the overall catalytic performance. Here, we present a facile synthesis strategy and investigate the interplay between OV content and intrinsic properties in bifunctional electrocatalysts for the hydrogen evolution reaction (HER) and oxygen evolution reaction (OER). Despite being derived from the same class of metal(II) chloride precursors, the three aerogels exhibit distinctly different amorphous porous architectures: sphere-like particles (Fe), flower-like hierarchical nanosheets (Co), and densely packed ultrasmall spheres (Ni). Among the three, OV-rich Co aerogels stand out due to the synergistic combination of the highest OV percentage (89.4%), the largest specific surface area (134.5 m2 g−1), and favorable intrinsic electronic properties of the Co center, which together maximize active site density and facilitate efficient charge transfer for both HER and OER intermediates. Consequently, Co aerogels deliver outstanding bifunctional performance with overpotentials of only 383 mV (OER) and 365 mV (HER) at 100 mA cm−2 in alkaline electrolyte, along with long-term durability over 70 h. Importantly, despite possessing substantial OV content, Fe and Ni aerogels exhibit negligible or poor catalytic activity in neutral electrolyte, demonstrating that OV content alone is insufficient, and intrinsic material properties are equally decisive in governing electrocatalytic performance. This study thus provides mechanistic insights into the relative contributions of OV and intrinsic properties in water splitting electrocatalysis, alongside a scalable synthesis route for high-performance Co-based aerogel electrocatalysts.
In this work, amorphous 3d-VIIIB-metal aerogels featuring significant porous architectures and abundant OV were rapidly synthesized via an ambient facile reduction method, and their electrocatalytic performance toward the anodic OER and cathodic HER was systematically investigated in neutral and alkaline environments. Simultaneously, the contribution of carbon cloth (CC) as a conductive substrate to HER/OER catalytic performance was systematically assessed to elucidate the intrinsic electrocatalytic activity of the as-prepared catalysts. Among the as-prepared catalysts, in alkaline and neutral electrolytes, the OV-rich Co aerogel exhibits the highest OER and HER performance. Besides this, 72-h long-term stability using the OV-rich Co aerogel as the working electrode shows slight degradation with ∼130 mV-decrease in alkaline OER and ∼20 mV-decrease in alkaline HER. Notably, a high OV content alone does not guarantee superior catalytic performance; intrinsic material properties, such as the inherent electronic structure of the metal center, can play an equally decisive role. For instance, despite possessing substantial OV content, OV-rich Fe and OV-rich Ni aerogels exhibit poor catalytic activity for both the HER and OER in neutral electrolyte, highlighting that the interplay between OV and intrinsic material properties governs overall electrocatalytic performance. This study therefore aims to systematically elucidate the relative contributions of OV content and intrinsic material properties to electrocatalytic water splitting under alkaline and neutral conditions.
All electrochemical measurements were carried out using a Corrtest C@310M electrochemical workstation in a conventional three-electrode configuration. The catalyst ink was prepared by dispersing 10 mg of the synthesized catalyst in a mixed solvent of isopropanol and ethanol (1
:
1 v/v, total volume 0.98 mL) under ultrasonic treatment for 3 h. Subsequently, 0.02 mL of 5 wt% Nafion solution was added, followed by an additional 1 h of sonication to obtain a uniform suspension. Then, 0.1 mL of the resulting catalyst ink was drop-cast onto a 1 × 1 cm2 carbon cloth substrate (W0S1011) with a catalyst loading of 1 mg cm−2 acting as the working electrode. A 0.5 M phosphate buffer solution (PBS, pH 7) was prepared by dissolving 1.68 g of potassium dihydrogen phosphate (KH2PO4, CAS No. 7778-77-0, GHTECH) and 1.75 g of dipotassium hydrogen phosphate trihydrate (K2HPO4·3H2O, CAS No. 16788-57-1, Xilong) in 200 mL of deionized water (13.1 MΩ cm) under continuous stirring at ambient temperature until complete dissolution. A 1 × 1 cm2 Pt plate was employed as the counter electrode. Ag/AgCl and Hg/HgO electrodes were used as reference electrodes in neutral (0.5 M PBS, pH 7) and alkaline (0.5 M KOH, pH 13.2, CAS No. 1310-58-3, Sigma-Aldrich) electrolytes, respectively.
All cyclic voltammetry (CV) curves recorded at a scan rate of 5 mV s−1 for anodic OER and cathodic HER tests were corrected using iRS compensation. In contrast, no iRS compensation was applied to the chronopotentiometric (CP) measurements. All potentials were converted to the reversible
| E(RHE) = E(Ag/AgCl) + 0.197 V + 0.059 × pH − iRS |
| E(RHE) = E(Hg/HgO) + 0.140 V + 0.059 × pH − iRS |
η = b log|j| + a |
Electrochemical impedance spectroscopy (EIS) tests were carried out under a specific applied potential using an alternative current signal amplitude of 10 mV over a frequency range of 100 kHz–0.1 Hz. The electrochemical double-layer capacitance (Cdl) was evaluated using CV tests at different scan rates (2, 5, 10, 15, 20, and 25 mV s−1) within the non-faradaic potential region. The Cdl values were extracted from the slope of the linear fit of S/(2 × ΔV) as a function of scan rate, where S denotes the enclosed area of the CV curve and ΔV represents the potential window.
Phase identification of the synthesized catalysts was carried out by powder X-ray diffraction (XRD) on a Bruker D8 Advance (Cu Kα, λ = 0.154 nm), over a 2θ window of 10°–90° at a scanning speed of 5° min−1. The specific surface area and pore size were evaluated through nitrogen adsorption measurements based on the Brunauer–Emmett–Teller (BET) method using a Quantachrome NOVA Station C at 77.3 K. The morphology of the obtained catalysts was investigated using a Hitachi S-4800 field emission scanning electron microscope (FE-SEM) operated at an accelerating voltage of 10.0 kV and high-resolution transmission electron microscopy (HR-TEM, JEM2100). The oxidation states of elements were characterized by Al-Kα source X-ray photoelectron spectroscopy (XPS) (JPS-9030 Photoelectron Spectrometer) (C 1s XPS spectra with the C–C peak at 284.7 eV, Fig. S1, SI).
XPS was utilized to gain insights into the surface chemistry of the catalyst such as valence states and chemical composition. Fig. 2a shows the XPS spectrum of Fe 2p with peaks at 711.35 eV and 724.75 eV ascribed to Fe 2p3/2 and Fe 2p1/2 which can be deconvoluted into Fe2+ 2p3/2 (711.21 eV), Fe3+ 2p3/2 (714.02 eV), Fe2+ 2p1/2 (724.8 eV), and Fe3+ 2p1/2 (728.15 eV).24,25 Co 2p XPS spectra can be deconvoluted into six peaks, namely Co3+ 2p3/2 (784.41 eV), Co2+ 2p3/2 (788.61 eV), Co3+ 2p1/2 (799.61 eV), and Co2+ 2p1/2 (801.61 eV), along with a pair of satellite peaks (Fig. 2b).26 Similarly, the Ni 2p XPS spectrum shows peaks at 858.93 eV and 875.93 eV, corresponding to the Ni 2p3/2 and Ni 2p1/2 (Fig. 2c). The Ni 2p signals of the sample can be deconvoluted into six strong peaks, namely Ni2+ 2p3/2 (858.93 eV), Ni3+ 2p3/2 (863.93 eV), Ni2+ 2p1/2 (875.93 eV), and Ni3+ 2p1/2 (879.93 eV), accompanied by a pair of satellite peaks.27 The mixed valence states of metals in synthesized aerogels can be beneficial for enhancing HER and OER performance. The XPS O 1s spectrum of the Fe aerogel reveals two characteristic signals at ∼529.9 eV and ∼531.6 eV, corresponding to the oxygen lattice (OL) and oxygen vacancy (OV), respectively (Fig. 2d).28,29 As shown in Fig. 2e and f, in the Co and Ni aerogels, OL and OV characteristic peaks can be identified at ∼230 eV and ∼533 eV, respectively. Among OV-rich aerogels, the Co aerogel exhibits the highest OV percentage (89.4%) compared to the Ni aerogel (86.1%) and the Fe aerogel (72.9%). The introduction of oxygen vacancies can facilitate charge transfer and balance the adsorption–desorption of intermediates during the reaction process.30 However, under specific conditions, it is necessary to consider carefully the role of OV and intrinsic properties of the as-synthesized materials in catalytic performance.
![]() | ||
| Fig. 2 High-resolution XPS spectra: (a) Fe 2p of Fe aerogel, (b) Co 2p of Co aerogel, (c) Ni 2p of Ni aerogel; and O 1s XPS spectra of (d) Fe aerogel, (e) Co aerogel, and (f) Ni aerogel. | ||
To elucidate the intrinsic electrocatalytic activity of the as-prepared catalysts, electrochemical measurements for the anodic OER and cathodic HER were conducted using a standard three-electrode configuration in 0.5 M KOH and 0.5 M PBS, serving as alkaline and neutral electrolytes, respectively. As illustrated in Fig. 3a, iR-corrected OER polarization curves recorded in alkaline electrolyte show that the Co aerogel requires an overpotential of only 383 mV to achieve a current density of 100 mA cm−2. This value is significantly lower than those of the Ni aerogel (475 mV) and Fe aerogel (630 mV), demonstrating the superior alkaline cathodic OER performance of the Co aerogel among the investigated catalysts. Besides this, alkaline cathodic OER catalytic activity of the CC substrate is minimal, suggesting that the CC substrate contributes negligibly to the overall alkaline cathodic OER performance. Subsequently, EIS measurements were performed to investigate the electron transfer kinetics of the as-prepared catalysts. The equivalent circuit model used for Nyquist plot fitting is presented in Fig. S3 (SI) which includes uncompensated solution resistance (RS), internal charge transport resistance within the catalyst electrode (Rtr), interfacial charge-transfer resistance between the electrode and electrolyte (Rct), and a constant phase element (CPE).31 According to the fitting results, Nyquist plots obtained under alkaline cathodic OER conditions (Fig. 3b) reveal that the Co aerogel exhibits the smallest Rct (98 Ω), markedly lower than those of the Ni aerogel (189 Ω) and Fe aerogel (7855 Ω), indicating a more efficient charge-transfer process in the Co aerogel. The corresponding Nyquist fitting parameters are summarized in Table S2 (SI). Furthermore, short-term CP tests conducted at different current densities indicate that no noticeable performance degradation in short duration was observed, even at high current densities of 100 and 200 mA cm−2, demonstrating that all as-prepared catalysts exhibit promising stability under alkaline anodic OER conditions (Fig. 3c). Furthermore, Ni and Co aerogels exhibit comparable voltage requirements at low current densities (j = 10, 20, and 50 mA cm−2). However, at higher current densities (j = 100 and 200 mA cm−2), the Co aerogel outperforms the Ni aerogel by requiring a lower applied potential to deliver the same current. In contrast, the Fe aerogel consistently demands substantially higher working potentials to reach comparable current densities, indicating the poorest catalytic activity among synthesized aerogels. Compared to those catalysts, CC exhibits poor short-time performance, suggesting its unstable activity (Fig. S4a, SI).
Subsequently, the 3rd CV polarization curves of the as-prepared catalysts and CC under neutral anodic OER conditions are shown in Fig. 3d. The results indicate that only the Co aerogel exhibits discernible anodic OER activity in a neutral electrolyte, whereas the Fe and Ni aerogels show inactive catalytic activity, as their current densities overlap with those of the bare CC substrate. As presented in Fig. 3e, the obtained Nyquist plot and fitting curves demonstrated that the smallest semicircle radius belongs to the Co aerogel, reflecting the most favorable charge transfer of the Co aerogel. The Nyquist fitted parameters of as-prepared catalysts for neutral cathodic OER are listed in Table S3, SI. Short-term CP measurements confirm the high stability of the Co aerogel, which exhibits negligible current decay during the tests (Fig. 3f). Conversely, the Fe aerogel and CC substrate exhibit aggressive demands on energy consumption (Fig. S4b, SI), due to their poor catalytic activities.
The electrocatalytic anodic HER performance of as-prepared aerogels was first evaluated under alkaline conditions. As shown by the iR-corrected polarization curves in Fig. 4a, overpotentials required to reach a current density of 100 mA cm−2 are 526 mV for the Fe aerogel, 365 mV for the Co aerogel, and 463 mV for the Ni aerogel. These results demonstrate that the Co aerogel exhibits superior alkaline cathodic HER catalytic activity compared with Fe and Ni aerogels. Moreover, the current density delivered by CC is substantially lower than those of the as-synthesized catalysts within the same working potential window, indicating that the observed alkaline cathodic HER activity predominantly arises from the intrinsic catalytic properties of the synthesized materials. As illustrated in Fig. 4b, the Nyquist plot and corresponding fitted curves of the as-prepared aerogels exhibit similar semicircular shape but markedly different radii. The Nyquist fitting parameters for alkaline cathodic HER, summarized in Table S4 (SI), reveal that the Co aerogel exhibits a relatively low Rct (2.89 Ω), which is significantly smaller than those of the Ni aerogel (23.15 Ω) and the Fe aerogel (28.55 Ω), suggesting the favorable charge transfer of the Co aerogel. In addition, under alkaline cathodic HER conditions, Ni and Co aerogels maintain good short-term stability across the entire range of tested current densities, whereas the performance of the Fe aerogel and CC substrate deteriorates significantly due to inevitable corrosion at high required potentials (Fig. 4c and Fig. S4c, SI). These observations indicate that all as-prepared catalysts exhibit alkaline cathodic HER activity, with the Co aerogel demonstrating the highest overall performance among the synthesized materials.
As shown in Fig. 4d, neutral cathodic HER catalytic activities of the as-prepared catalysts and CC substrate were evaluated in 0.5 M PBS where Fe, Co, and Ni aerogels require overpotentials of 623, 464, and 526 mV, respectively, to achieve a current density of 100 mA cm−2. The relatively high overpotentials observed indicate sluggish cathodic HER kinetics in neutral media, which can be attributed to the limited availability of protons and hydroxide ions. The overlap of current densities of the Fe aerogel and CC substrate highlights the non-catalytic activities of the Fe aerogel. To further evaluate interfacial charge-transfer resistance Rct of the as-prepared catalysts under neutral conditions, EIS measurements were performed in 0.5 M PBS at −0.5 V vs. RHE, revealing a single semicircular feature for all samples (Fig. 4e). As a result, the Co aerogel has the lowest Rct (3.9 Ω), which is slightly lower than that of the Ni aerogel (3.97 Ω) and substantially lower than that of the Fe aerogel (7.85 Ω) (Table S5, SI), suggesting that the Co aerogel possesses the fastest electron-transfer rate and more favorable interfacial reaction kinetics among the mentioned aerogels. As shown in Fig. 4f, neutral cathodic HER short-term stability tests were performed at various cathodic current densities ranging from 5 to 100 mA cm−2. Particularly, Co and Ni aerogels exhibit minimal potential variations even at a high current density of −100 mA cm−2, whereas the Fe aerogel degrades early at a low current density of −10 mA cm−2 and demands significantly high potentials in subsequent current densities. These results demonstrate the high stability of Co and Ni aerogels under neutral cathodic HER conditions. The poor short-term stability of the CC substrate under neutral cathodic HER conditions is illustrated in Fig. S4d (SI). The alkaline/neutral anodic OER and cathodic HER CV curves of as-synthesized catalysts without iR correction are presented in Fig. S5 (SI).
To further compare the electrocatalytic activity in alkaline and neutral media, the Tafel slopes of the best-performing catalyst, Co aerogel, were derived. As shown in Fig. 5a, the Co aerogel exhibits a substantially lower anodic OER Tafel slope in alkaline electrolyte (76.8 mV dec−1) than in neutral electrolyte (254.2 mV dec−1), indicating more favorable anodic OER kinetics under alkaline conditions. Tafel slopes of all as-prepared catalysts in neutral and alkaline environments are illustrated in Fig. S6 (SI). We note, however, that Tafel analysis for the Fe aerogel in neutral HER – and for Fe and Ni aerogels in neutral OER – is not physically meaningful, as their polarization curves overlap with those of the bare CC substrate (Fig. 3d and 4d), confirming the absence of intrinsic electrocatalytic activity. In comparison with the Tafel slope and overpotential at j = 100 mA cm−2 for anodic OER performance in an alkaline environment to other reported Co-based catalysts, the Co aerogel exhibits promising anodic OER performance even when using a lower concentration of the electrolyte (Fig. 5b and Table S6, SI). Additionally, cathodic HER kinetics are explored as shown in Fig. 5c, where the Co aerogel exhibits a lower Tafel slope in alkaline electrolyte (135.9 mV dec−1) than in neutral electrolyte (221.8 mV dec−1), further confirming its more favorable cathodic HER kinetics under alkaline conditions compared with neutral media.32 Subsequently, cathodic HER performance of the Co aerogel via Tafel slope and overpotential at j = −100 mA cm−2 in an alkaline environment demonstrates acceptable performance compared with state-of-the-art Co-based catalysts (Fig. 5d and Table S7, SI).
To assess the electrochemically active surface areas (ECSA) of the as-synthesized catalysts, the electrochemical double-layer capacitance (Cdl) was obtained. As shown in Fig. S7 and S8 (SI), Cdl values were derived from CV curves recorded in the non-faradaic region at various scan rates (2–25 mV s−1). Notably, all catalysts show higher ECSA values in 0.5 M KOH than those measured in 0.5 M PBS (Fig. S9, SI). This variance is fundamentally attributed to the difference in the Cdl of the electrode–electrolyte interfaces. The smaller hydrated radii and strong specific adsorption of OH− ions in KOH lead to a higher Cdl compared to the bulkier phosphate anions in PBS. Therefore, the ECSA values in this study are primarily utilized to compare the relative electrochemically active surface areas among different catalysts within the same electrolyte medium, rather than making cross-electrolyte absolute ECSA comparisons. Using a nominal Cs value of 40 µF cm−2 for this relative estimation (ECSA = Cdl/Cs), the calculated ECSA values under alkaline conditions follow the order: Co aerogel (30.5 cm2) > Ni aerogel (27.0 cm2) > Fe aerogel (10.6 cm2). A similar trend is observed under neutral conditions: Co aerogel (4.2 cm2) > Ni aerogel (4.1 cm2) > Fe aerogel (2.4 cm2) (Fig. S9, SI). These results consistently indicate that the Co aerogel possesses a higher density of electrochemically accessible active sites than the Ni and Fe aerogels, regardless of the examined electrolyte.
Aside from the catalytic activity, the long-term durability of the Co aerogel in alkaline cathodic HER and alkaline anodic OER was assessed by sequential CV sweeps at a scan rate of 5 mV s−1. As exhibited in Fig. 6b and c, alkaline cathodic OER CV curves of the Co aerogel show a slight deterioration whereas in alkaline cathodic HER, the current densities remained almost unchanged after 200 cycles. To further assess the long-term stability of the Co aerogel for the HER and OER, a 70-h CP analysis was conducted within a three-electrode system. In Fig. 6d, the lowest overpotential for the anodic OER is measured as 697 mV (without iR correction) at a current density of 100 mA cm−2. Over time, this overpotential shows an increase to 130 mV after 70 h, which can be attributed to a combination of intrinsic material properties and the extrinsic limitations of the batch-type testing system. Intrinsically, the amorphous nature of the aerogel, while providing abundant active defect sites, is thermodynamically metastable and thus more prone to structural degradation or surface reconstruction under harsh continuous polarization compared to its crystalline counterparts. Extrinsically, the vigorous evolution of O2 and H2 gases at 100 mA cm−2 and −100 mA cm−2 in turn leads to severe bubble accumulation on the electrode surface, physically blocking active sites and increasing mass-transport resistance.33 Additionally, testing in an undivided batch cell without pH correction inevitably results in local and bulk pH fluctuations over time, which further contributes to the apparent increase in the measured potential.34 In contrast, for the cathodic HER process (Fig. 6e), the overpotential at j = −100 mA cm−2 remains nearly constant, exhibiting only a 20 mV decrease after 70 h, which indicates excellent stability of the Co aerogel electrode during the HER.
Experimental details and further electrochemical tests are available from https://doi.org/10.5281/zenodo.19103624.
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