Open Access Article
Kai Taoa,
Mingxiao Hanb,
Li Jiang
b,
Shangzhong Jinb,
Tommaso Giovannini
c,
Denis Garoli
*bd,
Zhefei Zhao
e,
Qiang Linf and
Huaizhou Jin*a
aKey Laboratory of Quantum Precision Measurement, School of Physics and Optical Engineering, Zhejiang University of Technology, Hangzhou 310014, China. E-mail: jinhuaizhou@zjut.edu.cn
bCollege of Optical and Electronic Technology, China Jiliang University, Hangzhou 310018, China
cDepartment of Physics, University of Rome Tor Vergata, INFN, Via della Ricerca Scientifica 1, I-00133, Rome, Italy
dDipartimento di Scienze e Metodi dell’Ingegneria, Università degli Studi di Modena e Reggio Emilia, Viale Amendola 2, Reggio Emilia, Italy. E-mail: denis.garoli@unimore.it
eDepartment of Applied Chemistry, Petroleum and Chemical Industry Key Laboratory of Organic Electrochemical Synthesis, State Key Laboratory of Green Chemical Synthesis and Conversion, Zhejiang University of Technology, Hangzhou 310014, China
fState Key Laboratory of Ocean Sensing, Institute of Quantum Sensing, School of Physics, Zhejiang University, Hangzhou, 310058, China
First published on 15th May 2026
Understanding the mechanisms for improving hydrogen oxidation reaction (HOR) activity on Pt-based catalysts in alkaline environments is challenging due to the lack of directly observed intermediates. Understanding the role of oxophilic metal additives is also crucial for designing advanced catalysts. In this study, we use in situ surface-enhanced Raman spectroscopy (SERS) to investigate the HOR on Au@PtRuNi nanoparticles. Electrochemical measurements show improved HOR activity with little change in hydrogen binding energy (HBE), whereas Raman results show the 740 cm−1 peak for hydroxyl adsorption on Ru, as well as a new peak at 565 cm−1, which can likely be attributed to the formation of nickel hydroxide (Ni(OH)2) during the catalytic process, starting from 0.3 to 0.5 V vs. RHE. This suggests that nickel hydroxide and the hydroxyl groups on ruthenium likely collaborate to facilitate hydrogen oxidation.
To understand the HOR in alkaline media, we first start with its reaction equation. The HOR in alkaline media consists of a few basic steps: Tafel, Heyrovsky, and Volmer steps, with the first step being the Tafel or Heyrovsky process, and the second being the Volmer process.17,21 The reaction equations of Tafel, Heyrovsky and Volmer steps are shown in (1)–(3), with the total reaction equation shown in eqn (4):
| Tafel step: * + H2 → 2Had | (1) |
| Heyrovsky step: * + H2 + OH− → Had + H2O + e− | (2) |
| Volmer step: Had + OH− → * + H2O + e− | (3) |
| Total equation: 2* + H2 + 2OH− → 2* + 2H2O + 2e− | (4) |
In this study, we aim to utilize SERS to investigate the behavior of adsorbed hydroxyl intermediates on Pt and PtRu based catalysts by using Au@Pt, Au@PtRu and Au@PtRuNi core–shell structures.35 The Au@PtRuNi structure is used to investigate the role of Ni in the HOR process, and that whether Ni can act in synergy with Ru to improve HOR activity. The Au@PtRuNi core–shell structure is shown in Fig. 1. This comparative analysis with multiple catalysts using both electrocatalytic measurement and SERS allows for a nuanced understanding of how different oxophilic elements influence the interfacial interactions in the HOR, and allows us to discover possible nickel hydroxide formation which facilitates the HOR process.
Reductive agents including sodium borohydride (NaBH4), ascorbic acid and sodium citrate were employed for the synthesis; ethanol, potassium hydroxide, and ultrapure water (18.2 MΩ cm) were used for solution preparation and cleaning procedures.
All reagents above were purchased from various domestic providers, such as Adamas-beta, Macklin and Aladdin, all from Hangzhou and Shanghai, China. They were all of analytical grade and were used without further purification. Vulcan carbon XC-72 was utilized as the catalyst support material, obtained from Cabot Corporation, Boston, United States.
Electrochemical measurements were performed using a DHElecchem electrochemical workstation with a standard three-electrode setup, using the built-in DHElecchem software to record electrochemical data. A Gauss Union C031-4 in situ electrochemical flow cell was used for all electrochemical and in situ Raman measurements. The flow cell was equipped with a standard tri-electrode setup, including a platinum wire counter electrode, a mercury/mercurous oxide (Hg/HgO) reference electrode, and a glassy carbon working electrode, with all potentials referenced against the reversible hydrogen electrode (RHE) in 0.1 M KOH solution.
For Raman measurements, we used a Horiba XploRA Raman Spectrometer (Horiba Jobin Yvon, Paris, France). A 638 nm laser was used as the excitation laser. Strong fluorescent interference was present for SERS measurements when a 532 nm laser was used; on the other hand, the signals we obtained when using a 785 nm laser were too weak.
After the synthesis of these Au@catalyst core–shell nanoparticles, transmission electron microscopy (TEM) was used to characterize their morphology and size distribution, with elemental composition and mapping characterized by energy-dispersive X-ray spectroscopy (EDS). Additionally, electrochemical techniques such as cyclic voltammetry (CV) and linear sweep voltammetry were employed to evaluate the catalytic activity with the aforementioned DHElecchem electrochemical workstation. In situ Raman spectroscopy measurements were conducted under constant potential conditions (such as −0.015 V, 0.035 V, 0.085 V, 0.135 V, etc.) to investigate intermediates during the electrochemical processes.
EDS elemental mapping reveals the spatial distribution of Au, Pt, Ru, and Ni throughout the nanoparticles. Fig. 2(c) shows the distribution of the four individual metals. The Au and Pt signals are concentrated in the center of the figure, this suggests more continuous distribution of Au and Pt, whereas the Ru and Ni signals are spread more sparsely over the nanoparticle. Quantitative EDS analysis of Au, Pt, and Ru shows atomic percentages of 77.80%, 21.01%, and 1.18%, respectively (normalized for Au, Pt and Ru only). Nickel content could not be accurately quantified by EDS; however, the presence of nickel content is confirmed in XPS results in Fig. 3(c) and (d). In fact, X-ray photoelectron spectroscopy (XPS) was used to characterize the surface chemical states of the Au@PtRuNi nanoparticles, as shown in Fig. 3. The Pt 4f spectrum displays two prominent peaks at binding energies of 71.2 eV (Pt 4f7/2) and 74.5 eV (Pt 4f5/2), which correspond to metallic Pt, with a minor shoulder at ∼72.3 eV suggesting the presence of partially oxidized Pt species Pt(II). The Ru 3p3/2 peak is observed at 462.9 eV, consistent with metallic Ru, while the broadening toward higher binding energy indicates a small fraction of RuOx, which is in agreement with the role of Ru as an oxophilic site for OH adsorption. XPS spectra of Ni 2p are taken both before and after the HOR. In Fig. 3(c), two main Ni 2p3/2 peaks appear at 856.0 eV and 852.7 eV corresponding to Ni(II) and metallic Ni, respectively. XPS results further show that the deposition of Pt, Ru and Ni on the Au core is successful. In addition, as shown in Fig. 3(d), the XPS curve changes after HOR electrocatalysis. The 852.7 eV peak corresponding to metallic Ni disappears while the 855.6 eV peak, which corresponds to Ni(II), becomes the main nickel peak in the spectrum. The shift of the satellite peak from 860.3 to 862.3 eV also suggests that nickel species are oxidized during the HOR process.
The CV curves in Fig. 4(a) also show that Au@PtRuNi exhibits a higher double-layer capacitance (Cdl) compared to Au@PtRu and Au@Pt; the increased Cdl may arise from enhanced surface roughness and/or hydrophilicity from Ni(OH)2 formation.
In order to assess the catalytic performance of the three catalysts, we also performed polarization experiments. Fig. 4(b) shows the polarization curves of Au@Pt, Au@PtRu and Au@PtRuNi catalysts obtained from linear sweeping voltammetry in 0.1 M KOH with saturated H2 at a sweeping rate of 10 mV s−1 and rotating speed of 1600 rpm, with the inset of Fig. 4(b) showing the micro-polarization regions of −4 to 4 mV. Fig. 4(c) shows the Tafel plot obtained from the LSV data from Fig. 4(b). Current densities increase faster for Au@PtRuNi than for Au@PtRu and Au@Pt, with Au@Pt having the slowest increasing of current density. At a fixed current density of 1 mA cm−2, Au@PtRuNi requires an overpotential of 38.9 mV, compared to 52.5 mV for Au@PtRu and 65.5 mV for Au@Pt. This 13.6 mV and 26.6 mV improvement over Au@PtRu and Au@Pt, respectively, demonstrates that the catalytic enhancement arises from electronic and chemical effects of Ni(OH)2, rather than the increase of surface area and hydrophilicity alone.
These results demonstrate that the inclusion of Ni in the catalyst provides genuine catalytic enhancement. The mechanisms of this enhancement are revealed by in situ SERS analysis in the next section.
The changes to the spectra of the HOR on Au@PtRuNi nanoparticles from −0.015 V to 0.535 V (−15 to 535 mV) vs. RHE are shown in Fig. 5(b). In these experiments, we also found another peak at 566 cm−1 that becomes stronger as potential increases. In the Au@PtRu results shown in Fig. 5(c), a peak is also observed near 566 cm−1. However, the 566 cm−1 peak obtained from the Au@PtRu catalyst becomes weaker as the potential increases, and disappears before 0.2 V, which is attributed to the oxidation of RuOx and is consistent with previous results.33 On the other hand, for experiments on Au@PtRuNi nanoparticles, the intensity of 566 cm−1 increases as the potential increases, especially at and above 0.385 V vs. RHE. Hence, the increasing 566 cm−1 peak on Au@PtRuNi nanoparticles is associated primarily with Ni compounds. Nickel has two primary (oxy)hydroxide species in electrochemistry: nickel hydroxide, Ni(OH)2, where Ni is predominantly in the +2 oxidation state, or Ni(II), and nickel oxyhydroxide, NiOOH, which contains nickel in the +3 oxidation state, or Ni(III). Our post-reaction XPS result in Fig. 3(d) shows a prominent Ni(II) peak at 855.6 eV; the metallic Ni peak, which is present in the pre-reaction XPS curve in Fig. 3(c) and disappears in Fig. 3(d), suggesting that most Ni species are oxidized. We performed peak fitting on the post-reaction XPS result, and the fit could not converge when a Ni(III) peak was added. This suggests that the contribution of Ni(III) is non-existent or extremely minimal, and that Ni(II) is the dominant nickel species in the HOR process. In the literature, the formation of NiOOH or Ni(III) typically requires higher potentials; 1.2 V to 1.4 V vs. RHE are the minimum potentials required for NiOOH formation, whereas Ni(OH)2 can form at lower potentials, such as at 0.5 V vs. RHE.41,42 According to recent studies, the transition of α-Ni(OH)2 to β-Ni(OH)2 can take place at low potentials, which is a phenomenon consistent with the two distinct oxidation peaks observed in the cyclic voltammetry curve of Au@PtRuNi; moreover, Hall et al. assigned the peak around 566 cm−1 to β-Ni(OH)2, and α-Ni(OH)2 exhibits no such peaks near that region.38,43 Xue et al. also showed that in a RuNi/C catalyst, Ni species are present as oxidized Ni(II) under operating conditions.44 Given these pieces of evidence, we attribute the 566 cm−1 peak on Au@PtRuNi to Ni(OH)2. The distinct behavior of the 566 cm−1 peak in the Au@PtRuNi system, intensifying with increasing potential, suggests the potential involvement of nickel hydroxide species that may enhance the HOR catalytic activity.
We also performed peak-fitting for the 740 cm−1 peak on Au@PtRuNi and Au@PtRu catalysts; the results (SI Fig. S2) show that the area of the 740 cm−1 peak on Au@PtRuNi is larger at lower potentials and gradually decreases as the potential increases, whereas the 740 cm−1 band on Au@PtRu remains similar over the same potential range. This potential-dependent decrease in the 740 cm−1 peak area on Au@PtRuNi, while remaining constant on Au@PtRu, indicates that the addition of nickel fundamentally modifies the OHad adsorption dynamics.
Here, we propose that Ni(OH)2 acts as a dual-function modifier. First, it facilitates water activation and supplies additional OHad species through its inherent oxophilic character; second, it creates favorable interfacial sites at the Ni(OH)2–RuOx perimeter for efficient OHad consumption. At lower potentials (−0.015 to 0.235 V vs. RHE), the enhanced OHad generation dominates, resulting in a larger 740 cm−1 peak on Au@PtRuNi compared to Au@PtRu. However, at higher potentials (above 0.235 V vs. RHE), OHad is consumed more rapidly through the interfacial Volmer step at Pt–RuOx sites promoted by Ni(OH)2, causing the 740 cm−1 peak to decrease. The potential role of Ni(OH)2 will be further discussed in the Discussions section.
Under this hypothesis, the active surface of Au@PtRuNi can be viewed as a Pt–RuOx–Ni(OH)2 ensemble. In our electrochemical experiments, the HOR has higher reaction activity on Au@PtRuNi than on Au@PtRu; our DFT results (Note #2 and Fig. S2 in SI) also show that the Pt–RuOx–Ni(OH)2 ensemble has modestly more favorable Gibbs free energies for OH adsorption and for Had + OHad → H2O formation at the Ni(OH)2/RuOx interface, compared to the RuOx surface alone. In addition, we performed RT-TDDFTB simulations of four core–shell nanoparticle models: Au561, Au309@Pt252, Au309@Pt216Ru36, and Au309@Pt116Ni116Ru20 (Note #3 and Fig. S3 in SI). The results show that alloying the Au surface with Pt, Ru, and Ni does not produce a distinct new visible resonance, but instead broadens and damps the optical response of the Au core. This suggests that the enhanced HOR activity and the appearance of the 566 cm−1 Raman band are unlikely to originate from a stronger plasmonic or optical antenna effect. The optimized multi-metal clusters also exhibit significant structural relaxation upon incorporation of Ru and Ni, which may support the formation and stabilization of catalytically relevant species.
The role of Ni(OH)2 can be rationalized by the Pt/Ni(OH)2 system studied by Markovic's group in both HOR and hydrogen evolution reaction (HER) electrocatalysis.27,47 Tian et al.'s research also reported a synergistic interaction between RuOx and Ni(OH)2 in their system.48 In both Markovic and Tian's systems, Ni(OH)2 acts as a promoter that accelerates water activation and the production of OHad while Ru/RuOx act as active sites for further reaction steps involving OHad. The spectroscopic evidence from the potential-dependent decrease in the 740 cm−1 OHad peak on Au@PtRuNi also validates our proposed multi-site bifunctional mechanism. Rather than simply increasing the total OHad availability, Ni(OH)2 actively regulates the supply-consumption network at the Pt–RuOx sites. These results are consistent with DFT predictions of more favorable OHad reduction energetics at the Ni(OH)2/RuOx interface. To summarize, we successfully found spectroscopic evidence of Ni(II) forming in situ that correlates with increased HOR activity. Our in situ electrochemical SERS results, together with prior work on Pt/Ni(OH)2 and Ru–NiOx systems, support a multi-site bifunctional mechanism for the HOR on Au@PtRuNi in which Ni(OH)2, RuOx, and Pt play distinct yet complementary roles. In our Pt–RuOx–Ni(OH)2 framework formed in situ from the Au@PtRuNi catalyst, Pt provides sites for H adsorption, Ni(OH)2 contributes to water activation and the supply of OHad, and RuOx provides thermodynamically optimal adsorption sites for OHad to react with Had in the Volmer step. The Ni(OH)2–Pt and Ni(OH)2–RuOx perimeters increase the number of interfacial Had/OHad pairs and establish a coupled OHad supply and consumption network. Taken together, our results support a multi-site, bifunctional mechanism and highlight a general strategy for future alkaline HOR catalyst design that not only promotes OH adsorption, but also focuses on the synergistic effect of different oxophilic components for coupled supply and consumption of OHad.
Supplementary information (SI) is available. See DOI: https://doi.org/10.1039/d6na00164e.
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