Yingying
Xu
ab,
Yingxia
Zhao
bc,
Zihui
Yuan
ab,
Yue
Sun
ab,
Shaomin
Peng
ab,
Yuanhong
Zhong
abc,
Ming
Sun
*abc and
Lin
Yu
*ab
aJieyang Branch of Chemistry and Chemical Engineering Guangdong Laboratory (Rongjiang Laboratory), Jieyang 515200, P. R. China
bGuangDong Engineering Technology Research Center of Modern Fine Chemical Engineering, School of Chemical Engineering and Light Industry, Guangdong University of Technology, 510006 Guangzhou, P. R. China
cGuangdong Yuntao Hydrogen Energy Technology Co., Ltd, 551040 Guangzhou, China
First published on 4th July 2024
Fueled by renewable energy, the paradigm of “green hydrogen” production via water electrolysis stands as an imperative pathway toward the evolution of novel energy frameworks. Proton exchange membrane water electrolysis (PEMWE) emerges as a pivotal route for sustainable power generation, offering substantial advantages. However, the quest to enhance the efficiency of proton exchange membrane water electrolysis (PEMWE) encounters formidable obstacles, prominently centered on attaining a delicate equilibrium between heightened activity and prolonged stability of oxygen evolution reaction (OER) catalysts. The pursuit of OER electrocatalysts that epitomize efficiency, longevity, and cost-effectiveness under high operating potential and corrosive acidic conditions assumes paramount importance in propelling the frontiers of electrochemical water splitting. This review provides a comprehensive overview of recent advancements in both noble and non-noble metal oxides utilized for acidic oxygen evolution reaction (OER). It underscores the significance of analyzing the instability of catalysts based on the OER mechanism, while delving into effective strategies aimed at bolstering the activity and stability of IrO2, RuO2, and transition metal (TM) oxide electrocatalysts. Finally, some insights are provided into the indirect challenges confronting current anode catalysts employed in proton exchange membrane (PEM) electrolyzes, along with perspectives on future research avenues and potential directions.
To date, to realize the vision of green hydrogen production, leveraging renewable energy sources such as wind, solar, and tidal energy to drive water electrolysis for hydrogen production has been a promising approach.16,17 However, traditional alkaline electrolysis has limitations in terms of its dynamic response, especially when coupled with fluctuating renewable energy sources. This can lead to reduced overall efficiency and hinder the effective utilization of sustainable energy. Proton Exchange Membrane Water Electrolysis (PEMWE) holds great promise as a method for hydrogen production.18–20 It utilizes an acidic solid polymer electrolyte membrane, which offers several outstanding advantages over traditional electrolysis methods. One key advantage is its high efficiency. The solid polymer electrolyte membrane enables rapid proton transport, facilitating faster electrochemical reactions at the electrodes.21–23 This results in improved energy efficiency and higher hydrogen production rates compared to conventional alkaline electrolysis. Additionally, PEMWE systems offer greater flexibility and scalability. They can operate under a wide range of operating conditions and can be easily scaled up or down to match varying hydrogen production demands.24–26 This makes them suitable for applications ranging from small-scale distributed hydrogen production to large industrial-scale operations. Furthermore, PEMWE technology allows for better integration with renewable energy sources. The rapid response time of PEMWE systems makes them well-suited for coupling with intermittent renewable energy sources such as solar and wind power. This enables more efficient utilization of renewable energy and helps to address the intermittency challenges associated with these energy sources.27–29
In recent years, significant strides have been made in the development of effective metal oxide catalysts for acidic oxygen evolution reaction (OER), with notable examples including IrO2,30,31 RuO2,28,32–34 and various other transition metal oxides.13,35–38 However, a common challenge encountered by most metal oxides is their susceptibility to metal dissolution in acidic electrolytes, often leading to diminished stability. Previous studies39 have revealed an intriguing phenomenon: while the most reactive oxides in acids (Au ≪ Pt < Ir < Ru < Os) exhibit high reactivity, they paradoxically tend to be the most unstable materials (Au ≫ Pt > Ir > Ru ≫ Os). This intricate interplay between activity and stability is governed by the properties of metal cations and the potential conversion of stable metal cations with a valence state of n = +4 to unstable metal cations with a valence state greater than +4. Therefore, achieving the optimal anode material for proton exchange membrane water electrolysis (PEMWE) necessitates striking a delicate balance between stability and activity, ensuring that the dissolution rate remains neither too fast nor too slow.40,41
In this review, we comprehensively explore the latest developments in the fields of IrO2 based catalysts, RuO2 based catalysts, and non-noble metal oxide catalysts related to acidic oxygen evolution reaction (OER). We first introduced the working mechanism of acidic OER, mainly discussing the complex equilibrium dynamics between catalyst activity and stability. Building upon this understanding, the recent advancements in both noble and non-noble metal oxides as anodic catalysts in acidic environments are comprehensively reviewed. Finally, we analysed the indirect challenges faced by existing anode catalysts in proton exchange membrane (PEM) electrolysis cells and shared insights into future research approaches and potential directions (as shown in Fig. 1).
Fig. 2 (a) Schematic diagram of the AEM pathway of the OER in acids. (b) The concrete path of the AEM. (c) Contour plot of theoretical overpotential as a function of ΔGO*–ΔGOH* and ΔGOH*.42 Copyright 2023, Wiley-VCH. (d) DEMS measurements of 16O18O and 16O16O signals from the reaction products for NiO in 1 M KOH.43 Copyright 2024, Wiley-VCH. |
The OER mechanism dominated by the AEM involves intricate four-electron processes and iterations of intermediates *OH, *O, and *OOH, contributing to overpotential. These steps are intricately dependent on the binding energies involved. According to Sabatier's principle, the ideal oxygen binding energy should be moderate. Excessive binding energy can hinder desorption, while insufficient binding energy leads to inadequate activity. Typically, the step with the largest difference in binding energy is considered the rate-limiting step (RLS) of the reaction. In the current OER, the key overpotential primarily arises from the oxidation of *OH and the formation of *OOH. Optimizing the binding strength of intermediates is pivotal for enhancing OER catalyst performance. To this end, a descriptor for the binding energy difference between *OH and *OOH intermediates, denoted as ΔGOH*–ΔGOOH*, proves valuable for evaluating catalyst performance and predicting OER activity. Theoretical calculations play a crucial role in achieving the optimal binding energy of oxygen intermediates in catalysts, facilitating the precise design of efficient OER catalysts. For instance, Yu et al.42 investigated the binding energy of oxidation intermediates under the interaction between Co doping and cation vacancies using density functional theory calculations. Their findings revealed a scaling relationship between the energy of O* and OOH* provided by metal active sites, expressed as GOOH* = 1.08GOH* + 2.97. Moreover, the overpotential η was found to be related to ΔGO*–ΔGOH*, showing a linear increase. This indicates that Co doping and cationic vacancies can reduce the OER overpotential of NiFe OOH to 0.99 V and 0.82 V, respectively. The identification of AEM pathways relies on monitoring key intermediates, for which effective methods such as in situ Raman spectroscopy, in situ XAS, and isotope-labeled mass spectrometry (DEMs) have been widely employed in recent years. Yan et al.43 labeled the original NiO catalyst with O18 and obtained labeled NiO18 for the OER electrode reaction. In the DEM results, NiO18 exhibited a signal of O,32 indicating that all the generated oxygen originated from water molecules in the electrolyte. This confirmed that the OER performance on the NiO surface is primarily governed by the mechanism of adsorbate evolution.
Addressing the challenges associated with the adsorbate evolution mechanism requires a thorough investigation into the dynamic behavior of adsorbates on catalyst surfaces under acidic electrolyzed water conditions. The complexity and diversity of the reaction, influenced by protons and oxygen in the solution, necessitate a deeper understanding and control of this mechanism. Moreover, the surface structure and composition of catalysts further complicate the evolution of adsorbates. To overcome these challenges, efficient experimental and theoretical methods must be developed to analyze and predict the evolution process of adsorbates accurately.
Fig. 3 (a) Schematic diagram of the LOM pathway of the OER in acids. (b) The concrete path of the LOM. (c) The electrochemical cell configuration used in DEMS measurements. (d) DEMS signals of 32O2 (16O16O) and 34O2 (16O18O) from the reaction products for 18O-labeled SrRuIr catalysts in H218O aqueous sulfuric acid electrolyte and corresponding CV cycles.44 Copyright 2021, American Chemical Society. |
Advancing the understanding of the lattice oxygen mechanism is paramount for overcoming the challenges posed by the stability of lattice oxygen in acidic electrolyzed water. The dissociation and deactivation of lattice oxygen are exacerbated by the harsh conditions of high temperature and high pressure in acidic environments, further underscoring the complexity of this mechanism. To address these challenges, it is imperative to develop stable lattice oxygen structures, elucidate the active sites involved in lattice oxygen reactions, and explore novel reaction conditions. Leveraging advanced characterization techniques and theoretical calculation methods can facilitate in-depth studies of the active sites and reaction mechanisms of lattice oxygen in acidic electrolyzed water. This knowledge can offer valuable theoretical insights for the rational design of catalysts with enhanced activity and stability.
Fig. 4 (a) Schematic diagram of the OPM pathway of the OER in acids. (b) The concrete path of the OPM. (c) The schematic diagram of dual-site adsorbate evolution mechanisms for coupled O–O bonding during the OER (blue for Co atoms, red for Fe atoms, and yellow for S atoms).47 Copyright 2024, Springer Nature. (d–f) OH− adsorbed surfaces for SFO and CCFO and the corresponding OER mechanism.46 Copyright 2015, Springer Nature. |
Hence, confining the metal active center within a covalent network with symmetric atomic centers (e.g., α-MnO2) stands as one of the effective strategies for designing efficient OER catalysts via the OPM. Lee's team48 utilized a cation exchange method, substituting Ru into MnO2 crystals to form periodic arrangements of Ru atomic chains. XAS and aberration-corrected HAADF-STEM results showed a reduction in the distance between Ru atoms in Ru/MnO2 from the original 3.1 Å to 2.9 Å, facilitating the coupling of O–O radicals. The signal of the key intermediate *O–O* bond directly related to the OPM was demonstrated in electrochemical in situ experiments. Additionally, the authors recorded the changes in the ICP-OES values of Ru and Mn in solution during the OER process. The results indicate the dissolution–redeposition process of Ru, albeit at the expense of Mn dissolution. However, due to in situ self-reconfiguration, the intrinsic OER activity of Ru is more than 600 times higher than that of commercial RuO2. These findings unveil the possibility of triggering the OPM by designing the geometry of the metal active site.
Overall, we have described three typical OER mechanisms in acidic electrolytes: AEM, LOM, and OPM. In the AEM, various oxygen reaction intermediates such as *OH, *O, and *OOH are generated, with their binding energies following a scaling relationship ΔGOOH = ΔGOH + 3.2 ± 0.2 eV, and a theoretical limit of about 370 ± 100 mV. The LOM reduces the theoretical overpotential needed for the OER by avoiding the formation of *OOH intermediates, but it may damage the catalyst lattice structure, posing challenges for long-term stability. New mechanisms like the OPM have emerged in recent years, but specific reaction steps require further research to clarify the intrinsic relationship between activity and stability. It is important to note that these mechanisms are not mutually exclusive, and many new OER mechanisms have evolved from combinations or extensions of the AEM, LOM, and OPM. In Peng's study,49 the structure of Ru-doped Co3O4 was finely tuned at the atomic level, embedding Ru atoms in cation vacancies to activate a proton donor-receptor function (PDAM) mechanism. This optimized mechanism resulted in significantly lower overpotential, with the Ru(anc)–Co3O4 catalyst requiring only 198.5 mV overpotential at 10 mA cm−2 for the OER. In another study by Xu et al.,50 non-catalytic Zn2+ was introduced into CoOOH to alter the OER mechanism from the AEM to the LOM by adjusting the local configuration. They proposed that the OER via the LOM occurs only when two adjacent lattice oxygen ions are oxidized and combined, and two adjacent lattice oxygen vacancies are formed without breaking metal–oxygen bonds. These findings demonstrate how precise control over the catalyst composition and structure can dictate the underlying OER mechanism, leading to enhanced catalytic performance.
Fig. 5 (a) SEM image showing the uniform distribution of the IrO2NR. (b) A typical long IrO2NR with a length of 22.53 μm.51 Copyright 2023, Springer Nature. (c) TEM image of IrO2 nanoneedles. (d) Initial OER performance of IrO2.57 Copyright 2017, Wiley-VCH. (e) The SEM image of 1T-IrO2, showing its ultrathin morphology. (f) Polarization curves of 1T-IrO2, rutile-IrO2, and commercial catalysts (C-IrO2 and C-Ir/C) in O2-saturated 0.1 M HClO4 electrolyte with iR-correction.58 Copyright 2021, Springer Nature. (g–i) The nanosheet structure of 2D IrIrOx/C-20. (j) Water oxidation polarization curves recorded with a linear scan of potential at 2 mV s−1 for Ir–IrOx/C, commercial crystalline c-IrO2, Ir/C, and carbon black.59 Copyright 2022, American Chemical Society. |
Furthermore, extensive studies have been conducted on two-dimensional materials made of IrO2. Shao et al.58 reported the synthesis of 1T-phase-IrO2 nanosheets in strongly alkaline media through a combination of mechanochemical and heat treatment methods, as depicted in Fig. 5e. Atomic force microscopy (AFM) analysis revealed that the thickness of the ultra-thin IrO2 nanosheets was in the range of 3–5 nm. Linear sweep voltammetry (LSV) results (shown in Fig. 5f) indicated that 1T-IrO2 exhibited an ultralow overpotential of 197 mV (at 10 mA cm−2), which was 100 mV lower than that of rutile-IrO2. Further extended X-ray absorption fine structure (EXAFS) analysis suggested that the optimized 1T phase Ir active sites and ultra-thin 2D structure were crucial for achieving high-performance acidic OER catalysis. Zhao et al.59 synthesized ultrathin Ir–IrOx/C nanosheets with ordered interlayer spaces through a nano-self-assembly effect, as illustrated in Fig. 5g and h. On these nanosheets, IrO2 particles were well dispersed, forming a state of Ir/IrO2 coexistence. Due to the abundant pore structure of Ir–IrOx/C and the electronic interaction between Ir and IrO2, the prepared Ir–IrOx/C electrocatalysts exhibited the lowest overpotential (η) of 198 mV at 10 mA cm−2 for the OER in acidic media. This report is of significant importance for the application of two-dimensional materials in acidic OER. In general, apart from nano-self-assembled materials, the morphology of most materials relies on the carrier to prevent sintering. Uniform nucleation points are formed on the carrier with the help of other additives. The interaction between the support and the catalytic metal will be discussed in a later section.
Moreover, the unique structure of perovskite-type iridium oxides has also recently garnered widespread attention. Zou et al.61 recently reported a honeycomb layered strontium iridium salt (SrIr2O6) and demonstrated its potential as an efficient OER electrocatalyst with strong structural stability in acids. In stark contrast to conventional iridium-based catalysts, SrIr2O6 distinguishes itself by upholding the crystalline integrity of both its bulk and surface structures throughout the OER process, thus sidestepping the formation of an amorphous active phase. Among them, the short Sr–O bond and strong Sr–O interaction are fundamental factors contributing to the excellent structural stability of SrIr2O6 (Fig. 6a). Impressively, SrIr2O6 outperforms the benchmark catalyst IrO2 by a factor of ten in terms of efficiency, showcasing an exceedingly low total iridium leaching rate of a mere 0.03% during extended open electrolytic reduction tests, while maintaining catalytic activity for over 300 hours. Friedrich62et al. reported the development of an anode catalyst utilizing Sr2CaIrO6, boasting a loading density of merely 0.2 mg cm−2, a striking ten-fold reduction compared to commercially available catalyst-coated membranes (CCMs) laden with iridium. In practical proton exchange membrane water electrolysis (PEMWE) cells integrating this innovative anode, exceptional performance was achieved, with a voltage of 1.78 V recorded at a current density of 2 A cm−2, operating at 80 °C under ambient pressure conditions. Impressively, this remarkable performance was sustained for over 1000 hours, underscoring the catalyst's robust stability. Following this extended operational period, the surface morphology underwent a notable transformation, adopting a sponge-like structure attributed to the rapid leaching of calcium and strontium. Interestingly, this altered morphology featured small nanoscale domains of Ir–O–H, attributed to the small amorphous region of about 2 nm, believed to contribute significantly to the catalyst's superior oxygen evolution reaction (OER) performance. Koper et al.31 introduced a groundbreaking oxygen evolution catalyst featuring iridium double-perovskite. Double perovskites (DPs) are compounds with the generic formula A2BB′O6, with A denoting a large cation and B and B′ smaller cations (Fig. 6d). A wide range of compounds can be prepared by different combinations of A, B and B′ cations, which allows fine tuning of DPs. Remarkably, this catalyst boasts a 32 wt% reduction in iridium content compared to IrO2, yet demonstrates over three-fold higher activity in acidic environments. The 3D network of corner sharing octahedra is a necessary prerequisite for enhancing the activity of Ir DPs and their chemical stability under anode working conditions. Moreover, this double-perovskite strategy holds promise for extension to other noble metal oxide systems, such as ruthenium (Ru), platinum (Pt), and beyond.
Fig. 6 (a) Sr–O bond length, the integrated −ICOHP values of the Sr–O bond, and the Bader charge analysis of SrIr2O6 and Sr2IrO4. (b) Schematic showing the key factors controlling the structural stability of SrIr2O6 and Sr2IrO4. (c) Linear polarization curves for the OER of SrIr2O6, Sr2IrO4, and IrO2 at 1 mV s−1 in a 0.1 M HClO4 electrolyte, with the corresponding Tafel slopes in the inset.61 Copyright 2023, American Chemical Society. (d) Crystal structure of a generic Ba2MIrO6 DP. (e) OER activity in 0.1 M HClO4 of Ba2MIrO6, compared with the benchmark activity of IrO2 nanoparticles; the dotted lines show Tafel slopes of 60 and 120 mV per decade.31 Copyright 2016, Springer Nature. (f) OER catalytic mechanism diagram of the Co doped SrIrO3 catalyst. (g) Adsorbate evolution mechanism (AEM) diagram. (h) OER performance of the samples.63 Copyright 2024, Springer Nature. |
In addition to the dissolution of the A site, the evolution of the B site also significantly influences the activity of IrO2, which contributes to understanding the mechanism of acidic OER in perovskite-type Ir oxides. Gao et al.63 elucidated the crucial role of Co dissolution in acidic OER and the impact of surface and bulk Co on IrOx sites. Using in situ experiments and DFT calculations, it was revealed that Co initially dissolves on the catalyst surface under acidic conditions, leading to decreased stability of surface oxygen in SrIrO3 and removal of some bridging lattice oxygen, ultimately resulting in the formation of a low-coordination IrOx structure. Subsequently, adsorbent filling and the LOM reach a dynamic equilibrium, forming a unique mechanism called lattice oxygen promoted acidic evolution mechanism (LOPAEM) that is dominated by the adsorbate evolution mechanism (AEM) and promoted by the LOM.
All in all, limiting IrO2 to perovskite structures can effectively reduce the loading of traditional IrO2-based materials while achieving high-quality activity. The high activity is mainly attributed to the dissolution of the IrOx phase, typically accompanied by the collapse of the perovskite structure. Thus, ensuring the long-term stability of perovskite-type iridium oxides remains a significant challenge. To address this, effective characterization or computational methods are essential to further understanding the catalyst deactivation mechanism. Approaches such as combining Pourbaix plots with in situ data can aid in comprehending the working mechanism of IrO2 and offer crucial insights for the design and synthesis of high-performance perovskite-type iridium oxides.
Fig. 7 (a) Schematic illustration of Au@MnO2–IrOx core–shell nanoparticle-enhanced Raman spectroscopy for an in situ electrochemical study. (b) DFT-calculated Gibbs free energies of OER pathways on MnO2–IrO2 and IrO2. (c) LSV polarization curves of Au@MnO2–IrOx, Au@Ir, Au@MnO2 NPs, and commercial IrO2.66 Copyright 2023, Royal Society of Chemistry. (d) Schematic structure of Ir/Nb2O5−x. (e) In situ Ir L3-edge XANES spectra of Ir/Nb2O5−x at different potentials. (f and g) Electrocatalytic performance of Ir/Nb2O5−x.67 Copyright 2022, Wiley-VCH. (h) The illustration of oxygen diffusion in the ZrOx/TaOx interface. (i) Chronopotentiometry curve of the PEM electrolyzer with Ir–ZrTaOx as the anode operated at 1 A cm−2 at 80 °C with a Nafion 117 membrane.68 Copyright 2023, Elsevier. |
Indeed, an acidic environment imposes limitations on the use of traditional carbon-based supports due to their solubility in acid. Consequently, inert carriers such as Nb2O5, TiO2,69,70 SnO2,71–73 and TaOx74 have garnered significant attention. These supports remain stable under acidic conditions, providing a robust support platform for catalysts without undergoing dissolution or degradation. As a result, IrO2 catalysts supported on these inert supports exhibit enhanced stability and longevity, making them ideal candidates for various electrochemical applications in acidic media. Xing et al.67 conducted a comprehensive study using Nb2O5−x supported iridium (Ir/Nb2O5−x) as a model catalyst, where they monitored the dynamic evolution of the catalyst under operating conditions and uncovered the robust interaction between the carrier and metal. In the Ir/Nb2O5−x system, oxygen migration from the carrier to the metal Ir nanoparticles facilitated the formation of Ir–O coordination structures. Additionally, excess Ir–O species could be re-incorporated into Nb4+ ions within the Nb2O5−x support. This dynamic migration of interfacial oxygen enabled the prepared catalyst to effectively maintain the oxidation state of Ir–O even at high potentials, thus ensuring the stability of IrOx. In practical performance tests, the catalyst achieved a remarkable current density of 3 A cm−2 at a potential of 1.839 V in proton exchange membrane water electrolysis (PEMWE) cells and demonstrated stability for over 2000 hours at a current density of 2 A cm−2 (Fig. 7d–g).
The continuous triggering of the lattice oxygen mechanism (LOM) by the carrier/metal catalyst inevitably leads to the destruction of the carrier's crystal structure. In addition to selecting carriers with high acid insolubility, modifying the carrier through composite formation is employed to enhance the stability of the carrier. For instance, Zhang et al.68 discovered that the formation of heterogeneous interfaces (Fig. 7h) between ZrOx and TaOx in the support could potentially construct an oxygen diffusion pathway, thereby enhancing the stability. Leveraging this insight, they synthesized a supported catalyst (Ir–ZrTaOx), exhibiting mass-specific activity two orders of magnitude higher than conventional IrO2, capable of sustaining electrolysis for 1000 hours under operating conditions. In a PEMWE single cell, only 1/4 of the conventional Ir dosage was required to operate for over 200 hours (Fig. 7i), with a decay rate of only 4.7 μV h−1. In situ Raman and XAS analyses revealed that oxygen diffusion pathways between ZrOx/TaOx interfaces protected the carriers from over-oxidation and detrimental structural re-modelling, thus enhancing operational stability.
At present, the exploration of supported IrO2-based catalysts remains a forefront area of research, and understanding the interaction between the carrier and metal is crucial for designing OER-friendly IrO2 catalysts. While attributing the support-induced metal–support interaction (SMSI) effect solely to electron interaction may be oversimplified, it poses an important challenge to leverage existing characterization techniques to comprehensively address the promotion of acidic OER by support/metal interaction in IrO2-based catalysts. Building upon current characterization levels involves employing advanced techniques such as in situ spectroscopy, X-ray absorption spectroscopy75 (XAS), X-ray photoelectron spectroscopy (XPS), and transmission electron microscopy (TEM) to elucidate the structural and electronic changes occurring at the support/metal interface during OER operation. Additionally, computational methods like density functional theory (DFT) calculations can provide valuable insights into the nature of support/metal interactions and their influence on OER activity. By integrating experimental and theoretical approaches, researchers can gain a deeper understanding of the mechanisms underlying the enhanced OER performance of supported IrO2 catalysts, paving the way for the rational design of more efficient catalysts for acidic electrolysis applications.
Overall, although the oxygen evolution reaction (OER) activity of IrO2 is lower than that of RuO2, its excellent long-term stability makes it more widely used in acidic OER catalysis. The traditional AEM of IrO2-based catalysts has been reported in a large amount of literature (Table 1); DFT simulations and in situ characterization techniques have been employed to investigate this mechanism, highlighting the formation of OOH* intermediates as the main limiting factor contributing to the high overpotential of IrO2. Consequently, researchers have explored various synthetic methods to reduce the iridium load while preparing catalysts with high acidic OER activity and thermal stability. Future research will be pivotal in balancing the activity and stability of IrO2 catalysts by investigating their reaction mechanisms more thoroughly.
Catalyst | In a three-electrode system | In a PEMWE | Ref. | |||
---|---|---|---|---|---|---|
η 10 (mV) | Stability | Pathway | Stability | T (°C) | ||
M–RuIrFeCoNiO2 | 189 | 120 h @ 10 mA cm−2 | AEM | 500 h @ 1 A cm−2 | 80 | 76 |
SI6C1 | 280 | — | AEM/LOM | 10 h @ 200 mA cm−2 | 85 | 63 |
Mn0.98Ir0.02O2 | 100 | 48 h @ 100 mA cm−2 | AEM | — | — | 77 |
IrO2@TaB2 | 288 | 120 h @ 10 mA cm−2 | AEM | 100 h @ 1 A cm−2 | 80 | 74 |
IrCo@CNT/CC | 241 | 90 h @ 10 mA cm−2 | AEM | — | — | 56 |
SrIr2O6 | 303 | 300 h @ 10 mA cm−2 | AEM | — | — | 61 |
Sr2CaIrO6 | — | — | — | 100 h @ 1 A cm−2 | 80 | 62 |
Ir/D-ATO | 293 | 20 h @ 10 mA cm−2 | — | 250 h @ 1 A cm−2 | 80 | 72 |
M–RuIrFeCoNiO2 | 190 | 120 h @ 10 mA cm−2 | AEM | 500 h @ 1 A cm−2 | 80 | 76 |
Ir/Nb2O5−x | 218 | 100 h @ 10 mA cm−2 | LOM | 2000 h @ 2 A cm−2 | 80 | 67 |
1T-IrO2 | 197 | 50 h @ 50 mA cm | — | — | — | 58 |
Fig. 8 (a) Schematic diagram of the structural evolution of RuO2 under acidic conditions.81 Copyright 2024, Springer Nature. (b–d) Dissolution of Ru, Ir, and Pt under steady-state galvanostatic conditions.80 Copyright 2014, Wiley-VCH. (e) Calculated Pourbaix diagrams of RuO2; the potentials are referenced to the standard hydrogen electrode (SHE).83 (f) Ru3+ and Ru4+ content ratios corresponding to the in situ Ru 3d XPS spectra recorded at applied potentials ranging from 1.00 to 2.00 V vs. RHE.83 Copyright 2022, Springer Nature. |
Catalyst | In a three-electrode system | In a PEMWE | Ref. | |||
---|---|---|---|---|---|---|
η 10 (mV) | Stability | Pathway | Stability | T (°C) | ||
Ru/Ti4O7 | 150 | 500 h @ 10 mA cm−2 | — | 200 h @ 200 mA cm−2 | 80 | 84 |
Mn–RuO2-450 | 168 | 150 h @ 10 mA cm−2 | — | 150 h @ 50 mA cm−2 | 60 | 85 |
MnxRu1−xO2/MnO2/CFs | 161 | 600 h @ 10 mA cm−2 | — | 24 h @ 500 mA cm−2 | 70 | 86 |
RuO2–CeO2 | 180 | 1000 h @ 10 mA cm−2 | AEM/OPM | — | — | 87 |
RuO2/BNNS | 180 | 350 h @ 10 mA cm−2 | AEM | 200 h @ 200 mA cm−2 | 80 | 88 |
Ru3PbOx | 201 | 72 h @ 10 mA cm−2 | — | 300 h @ 100 mA cm−2 | 25 | 89 |
RuO2/Ag | 690 (η2A) PEM | 120 h @ 200 mA cm−2 | — | 100 h @ 1 A cm−2 | 90 | |
SnRuOx | 194 | 250 h @ 100 mA cm−2 | AEM | 1300 h @ 1 A cm−2 | 50 | 91 |
Nb0.1Ru0.9O2 | 204 | 360 h @ 200 mA cm−2 | — | 100 h @ 300 mA cm−2 | 80 | 92 |
(Ru–W)Ox | 170 | 300 h @ 10 mA cm−2 | AEM | 500/300/50 h @ 0.1/0.5/1.0 A cm−2 | 80 | 93 |
Ni–RuO2 | 214 | 200 h @ 10 mA cm−2 | AEM | 1000 h @ 200 mA cm−2 | 25 | 94 |
SrRuIr | 190 | 1500 h @ 10 mA cm−2 | AEM | 150 h @ 1 A cm−2 | 80 | 44 |
W0.2Er0.1Ru0.7O2−δ | 168 | 500 h @ 10 mA cm−2 | AEM | 120 h @ 100 mA cm−2 | — | 95 |
InRuO2/G | 187 | — | — | 350 h @ 100 mA cm−2 | — | 96 |
Si–RuO2-0.1 | 224 | 800 h @ 10 mA cm−2 | AEM | — | — | 81 |
Fig. 9 (a–c) OER performance of the prepared NbxRu1−xO2 in a three-electrode system and PEM electrolyzer. (d and e) EXAFS and XPS characterization of Nb0.1Ru0.9O2.92 Copyright 2023, Elsevier. (f) RuO6 octahedron before and after lithium intercalation. (g) The charge density distribution of the O* absorbed on the (110) surface of RuO2 (up) and Li0.5RuO2 (down) and the charge density distribution of the OOH* absorbed on the (110) surface of RuO2 (up) and Li0.5RuO2 (down).98 Copyright 2022, Springer Nature. |
However, most of the doping strategies activate the lattice oxygen mechanism (LOM) of RuO2, which inherently increases the covalency of Ru–O bonds. As previously discussed, this tendency poses challenges for the long-term stability of RuO2. Therefore, it is imperative to stabilize the RuO2 lattice bonds both before and after the reaction while optimizing the reaction pathway. Wang94 reported a nickel-stabilized RuO2 (Ni–RuO2) catalyst exhibiting high activity and durability in acidic oxygen evolution reaction (OER) for proton exchange membrane (PEM) water electrolysis. The original RuO2 demonstrated poor stability in acid OER and degraded rapidly, whereas the RuO2 lattice was significantly stabilized by the addition of nickel, extending its durability by more than an order of magnitude. When utilized as the anode of a PEM water electrolyzer, the prepared Ni–RuO2 catalyst exhibited stability exceeding 1000 hours at a water decomposition current of 200 mA cm−2, indicating its potential for practical applications. Wei et al.81 introduced a novel gap silicon doping strategy aimed at stabilizing the RuO2 lattice and inhibiting the direct involvement of lattice oxygen in the acidic oxygen evolution reaction (OER) process. The resulting Si–RuO2 electrode exhibited remarkable activity and stability in acid. As shown in Fig. 10a and b, the overpotential of the catalyst at 10 mA cm−2 was 226 mV. Moreover, after continuous oxygen evolution for up to 800 hours, the degradation rate of the catalyst does not exceed 52 μV per hour. Furthermore, metallized silicon demonstrates excellent acid resistance and possesses a suitable ionic radius for insertion into the interstitial positions of the RuO2 lattice. Additionally, the bond dissociation energy of the Si–O bond (798 kJ mol−1) surpasses that of the Ru–O bond (481 kJ mol−1), effectively reducing the covalency of the Ru–O bond (Fig. 10d–f). These strong Si–O bonds favor the inhibition of the lattice oxygen mechanism (LOM) pathway and enhance the associative elementary mechanism (AEM) pathway (Fig. 10g). The effective doping strategy proposed in this study, which attenuates the covalency of Ru–O bonds while preserving the quantity of Ru–O structures, carries profound implications. It emphasizes the necessity of evaluating the covalent characteristics of Ru–O bonds and the precise delineation of oxygen evolution reaction (OER) mechanisms as pivotal considerations in the design of acidic OER catalysts. This highlights the need for more sophisticated characterization methodologies like synchrotron radiation, along with the adoption of online in situ techniques such as in situ electrochemical mass spectrometry.
Fig. 10 (a and b) OER performance of the prepared Si–RuO2 in acidic electrolyte. (c) Comparison of the number of leached Ru ions during the OER process observed for Si–RuO2. (d) Normalized Ru K-edge XANES spectra of Si–RuO2−0.1 and com-RuO2. (e) Fourier-transform EXAFS spectra of Si–RuO2−0.1 and com-RuO2. (f) Schematic diagram of the band structures of Si–RuO2 and RuO2 based on Ru and O atoms on the (110) plane. (g) Schematic diagram of the enhanced stability caused by interstitial Si doping.81 Copyright 2024, Springer Nature. |
In addition to introducing insoluble doped metals to stabilize the RuO2 lattice and reduce the covalency of Ru–O, Hao et al.95 reduced/avoided the dissolution of RuO2 by decreasing the formation energy (ΔG) of oxygen vacancies (VO). They co-doped tungsten (W) and erbium (Er) into RuO2 to adjust its electronic structure. The introduction of W and Er significantly increased the formation energy of oxygen vacancies (VO) compared to the redox reaction of H2O/O2, which prevented the dissolution of Ru. As a result, the overpotential of W and Er co-doped RuO2 under acidic conditions was reduced to 168 mV at 10 mA cm−2, and it remained stable for at least 500 hours without apparent decay even at a high current density of 100 mA cm−2.
Additionally, heterometallic doping also benefits the asymmetric structure of metal–O–Ru, thereby disrupting the traditional adsorption or lattice oxygen mechanism. For instance, Wu et al.96 prepared In–RuO2 catalysts (In–RuO2/G) on graphene to enhance the oxidation of acidic water. By breaking the Ru–O–Ru symmetry in conventional RuO2, the electronic microenvironment and the local RuO bond strength of the catalyst were optimized, resulting in a significant improvement in acid OER performance. The overpotential was reduced to 187 mV at 10 mA cm−2, and persistent stability reached 350 hours at 100 mA cm−2. Further theoretical calculations revealed that the asymmetric structure of Ru–O–In disrupts the thermodynamic activity limit of the traditional adsorption evolution mechanism and notably weakens the formation energy barrier of OOH*, thus leading to a new rate-determining step for OH* adsorption. Similarly, in the work of Peng et al.93 asymmetric Ru–O–W active units were created around the interface of (Ru–W)Ox heterostructures, inducing valence oscillations at the Ru site. This cyclic transformation of the oxidation state of the active metals promoted the continuous operation of the active sites. The prepared catalyst demonstrated excellent stability for 300 hours in acidic electrolyte and showed potential for practical application in proton exchange membrane water electrolysis (PEMWE), maintaining stability for 300 hours at 0.5 A cm−2. In summary, the heterometallic doping strategy effectively adjusts the electronic structure of RuO2, stabilizes the crystal lattice, reduces the covalency of Ru–O bonds, enhances the formation energy of oxygen vacancies, and breaks the symmetry of Ru–O–Ru. These adjustments enable unconventional OER mechanisms and reduce barriers, ultimately improving the OER activity and stability of RuO2.
Fig. 11 (a) Operando synchrotron FTIR spectra were recorded in a cyclic potential range from 0.8 to 1.6 V versus RHE for Ru-MOF-400. (b) The free energy diagrams of the OER process at VRHE = 0 V (via the AEM) for RuCoOx, Co3O4, and RuCoOx/Co3O4 (upper pattern) and the calculated free energy diagrams of the OER process (via the OPM) for RuCoOx and RuCoOx/Co3O4 (lower pattern). (c) LSV curves of Ru-MOF-400, RuCoOx-Z, RuCoOx-B, RuO2, and Co3O4.100 Copyright 2023, Wiley-VCH. (d and e) Charge density difference of a two-dimensional slice on the RuS2–Ru model. (f) LSV curves with iR correction.102 Copyright 2021, Wiley-VCH. (g and h) Differential charge density analysis of RuO2–CeO2. (i and j) OER performance in 0.5 M H2SO4.87 Copyright 2024, American Chemical Society. |
Indeed, beyond the electronic effect, the lattice effect of a heterogeneous interface can induce lattice distortion or the formation of new lattice structures, both of which can significantly alter the surface activity of the catalyst. Lu et al.87 recently constructed RuO2–CeO2 heterojunction electrocatalysts using a lattice matching strategy. At the interface of the Ru–O–Ce heterostructure, a pathway for electron transfer between Ru and Ce is established (Fig. 11h), inducing lattice stress and distorting the local structure of RuO2. This resulted in a catalyst that demonstrated remarkable stability, maintaining OER activity for at least 1000 hours in 0.5 M H2SO4 with negligible degradation and an overpotential of merely 180 mV at 10 mA cm−2 (Fig. 11i and j). In situ ATR-SEIRAS and DEMS analyses revealed that both the interface and non-interface sites of RuO2–CeO2 underwent the oxide path mechanism (OPM) and adsorbate evolution mechanism (AEM) during the OER. In essence, the introduction of CeO2 initially distorts the RuO2 lattice, facilitating the deprotonation of *OH at the Ru site, thereby promoting stable *OOH adsorption. Consequently, the energy barrier of the AEM reaction pathway is lowered. Additionally, the unique electronic structure at the interface further promotes the direct coupling of hydrogen peroxide radicals in the OER process. Overall, Ru-based heterointerfaces serve as pivotal components in acidic electrolyzed water, substantially enhancing the performance of the electrocatalytic oxygen evolution reaction through diverse pathways such as component effects, electronic effects, band modulation effects, and lattice effects.
Fig. 12 (a) Illustration of the strategies for enhancing the performance of electrocatalytic water splitting via vacancy engineering.103 Copyright 2020, Royal Society of Chemistry. (b) A schematic illustration of the role of defects in the modulation of electrocatalytic performance.8 Copyright 2021, Royal Society of Chemistry. (c) STEM image of a CVD-grown monolayer MoS2 flake film after etching. The yellow dotted circles represent the S-vacancies. (d) The projected electronic density of states of the d-band for the Mo atoms of P-MoS2, MoS2-FGJK, and MoS2-EGMO.104 Copyright 2020, American Chemical Society. (e and f) Two-dimensional volcano plot constructed using the descriptors of ΔGO*–ΔGOH* and ΔGOOH*–ΔGO* and a schematic showing the origin of OER activity improvement upon introducing a Ru vacancy. Insets show the configurations of O-terminated RuO2(110) and RuO2(100) surfaces.28 Copyright 2020, Royal Society of Chemistry. |
Firstly, metal vacancies have garnered widespread attention and experienced rapid development in recent years, primarily due to their unique electronic structure and high surface activity density. The presence of metal vacancies typically results in the formation of additional active sites on the catalyst surface, thereby enhancing the adsorption and activation of reactants. Furthermore, the change in the electronic structure of the catalyst induced by metal vacancies, particularly the shift in the position of the d-band center, can optimize the adsorption energy of reaction intermediates. The introduction of a metal vacancy can alter the reaction pathway and mechanism of the catalyst, thereby accelerating the chemical kinetics. Metal vacancies can lower the energy barrier of the reaction, facilitating easier reaction processes. Although the incorporation of metal vacancies can introduce structural defects, careful design and optimization can significantly enhance the stability of the catalyst. Overall, the role of metal vacancies in electrocatalysis is profound, demonstrating substantial potential by modulating the electronic structure, enhancing catalytic activity, promoting chemical kinetics, and improving catalyst stability.
Li et al.28 employed a molten salt method to fabricate ultra-thin RuO2 nanosheets abundant in Ru vacancies, yielding numerous multi-scale defects including dislocations and grain boundaries. The presence of Ru vacancy phases on the surface substantially diminishes the binding energy of O*, consequently reducing the energy barrier for the conversion of O* to OOH* and significantly enhancing the performance of acidic OER. Remarkably, at a current density of 10 mA cmgeo−2 and 125 μg cmgeo−2 loading, an exceptionally low overpotential of 199 mV was achieved along with the demonstrated stability (Fig. 12e and f). Similarly, Li et al.107 reported defect-rich amorphous/crystalline RuO2 porous particles, showcasing outstanding OER performance under acidic conditions with a low overpotential of 165 mV at a current density of 10 mA cm−2.
On the one hand, the presence of oxygen vacancies can activate neighboring metal atoms, inducing high reactivity, by shifting the density of states (DOS) closer to the Fermi level, thereby facilitating electron transfer. On the other hand, electrons residing on the vacancies can be excited into the conduction band (CB), introducing fresh sites conducive to hydrogen adsorption within the CB. Cho et al.108 introduced a novel modification to amorphous/crystalline RuO2 (a/c-RuO2) by incorporating oxygen-enriched vacancy sodium. Through DFT calculations, they demonstrated that the introduction of oxygen vacancies leads to an increased separation between the d-band center of RuO2 and the Fermi energy level. This effect weakens the chemical bond between oxygen intermediates and the RuO2 surface, consequently enhancing both the activity and stability of RuO2 in electrocatalytic applications. Li et al.109 devised a novel oxygen-enriched RuO2 nanoparticle–carbon coupled hybrid aerogel (VO-RuO2@CA), demonstrating that oxygen vacancies (VO) can notably diminish the binding energy of O* relative to OOH*, thereby enhancing the oxidation activity and anti-peroxidation capability of RuO2 in natural water. Notably, the representative VO-RuO2@CA achieved an ultra-low overpotential of 207 mV under acidic water oxidation conditions at 10 mA cm−2. Additionally, the emergence of metal-induced oxygen vacancies has garnered significant attention. For instance, Qi et al.110 devised a distinctive array of Mo-doped ruthenium–cobalt oxide (Mo–RuCoOx) nanoplates. During surface reconstruction in the oxygen evolution reaction (OER), these nanoplates generate oxygen vacancies, optimizing the adsorption energy of hydrogen/oxygen intermediates. As a result, the kinetics of both the hydrogen evolution reaction (HER) and OER in acidic conditions are greatly accelerated.
While vacancy engineering has showcased remarkable activity in electrocatalysis, the unsaturated coordination and heightened reactivity of the defective catalyst make it unable to withstand prolonged continuous operation under harsh electrolytic conditions.34 Consequently, the catalyst is prone to restructuring during the reaction. In situ characterization becomes imperative to monitor the catalyst's state under operational conditions, necessitating techniques such as in situ Raman spectroscopy, in situ infrared spectroscopy, in situ XPS, and in situ synchrotron radiation. Moreover, structural evolution may lead to mechanistic shifts, warranting further characterization, such as in situ electrochemical mass spectrometry, and computational methods to elucidate the mechanism of the defective catalyst. This aids in gaining a deeper understanding of the relationship between defects and activity and stability.
In conclusion, the dominant AEM restricts the further enhancement of RuO2 catalytic activity. At the same time, the traditional LOM related to lattice oxygen, although helpful to enhance the catalytic activity, initiated the structural variation and dissolution of RuO2, which significantly reduced its long-term stability. It is necessary to carry out the effective coordination and management between the AEM and LOM mechanisms, therefore balance the activity and stability of RuO2 electrocatalysts. This optimization not only helps to improve the application of RuO2 in acidic electrolyzed water, but also provides an important design idea and method for developing new efficient and stable electrocatalysts.
In addition to noble metal doping, the incorporation of non-noble metals into Co3O4 has emerged as a promising avenue. Lou et al.114 explored the introduction of 13 different metals as isolated metal sites within ultrathin Co3O4 nanosheets. Their investigation revealed that Fe-doped Co3O4 significantly enhanced the electrocatalytic activity for the oxygen evolution reaction (OER). Leveraging their advantageous structure and composition, the Fe-doped Co3O4 laminated nanosheets demonstrated remarkable electrocatalytic performance in the OER. At an overpotential of 262 mV at 10 mA cm−2, these nanosheets exhibited excellent stability even under high current density conditions of 100 mA cm−2, maintaining their performance for 50 hours.
The addition of Mn into the spinel lattice of Co3O4 represents a significant advancement in improving the stability of non-noble metal-based OER catalysts under acidic conditions. Xiao et al.'s work115 demonstrated a remarkable increase in the catalyst's lifetime, extending from just a few hours to hundreds or even thousands of hours. Theoretical calculations revealed that the stability of the Mn–O bond played a crucial role in preventing the dissolution of lattice oxygen, thereby enhancing the catalyst's stability. This breakthrough represents a promising development in the field of Co3O4-based OER catalysts, showing their potential for practical applications in acidic electrolysis systems. By addressing the stability limitations at high current densities, this research opens up new possibilities for the design of robust and efficient non-noble metal-based catalysts for water electrolysis. Zhai et al.116 applied a coating of Mn-doped Co3O4 with N (Mn–CO3O4@CN) layers. Through in situ isotopic labeling spectroscopy and electron localization function (ELF) evaluation, they unveiled the presence of hydrogen bond interactions between CN units and H2O molecules, forming a continuous hydrogen bond network at the catalyst–electrolyte interface (Fig. 13h and i). Additionally, strong charge regulation between Mn/CN and Co sites was observed to reduce the OER barrier. The results demonstrated that the Co3O4-based electrode exhibited a low overpotential of 395 mV (at 10 mA cm−2) in acidic media, surpassing the activity of RuO2 even at high current densities (100 mA cm−2 @ ∼538 mV). In addition, the acidic OER properties of Co3O4-based catalysts in recent years are listed in Table 3.
Fig. 13 (a) Frequency at which each element appears in acid-stable oxides. Elements with zero frequency are shaded in gray. Lanthanoids and actinoids are omitted for clarity because no oxide containing these elements was predicted to be stable.111 Copyright 2020, American Chemical Society. (b) Calculated Pourbaix diagram of CoOx.83 Copyright 2022, Springer Nature. (c) Activity trends towards oxygen evolution for rutile, anatase, Co3O4, and MnxOy oxides.117 Copyright 2011, Wiley-VCH. (d and e) Identification of the Ruoct–O–Cooct coordination environment in RuCoOx. (f) Simulative structural model of a Ruoct–O–Cooct unit with two adsorbed oxygen radicals. (g) Geometric LSV curves of RuO2, Co3O4 and RuCoOx.113 Copyright 2023, American Chemical Society. (h) Schematic illustration of Mn–Co3O4@CN with a hydrophilous CN layer to tailor the local chemical environment at the interface for optimum OER in acidic electrolyte. (i) In situ Raman spectra of interfacial water. (j) Tafel curves obtained from the polarization curves.116 Copyright 2024, Wiley-VCH. |
Catalyst | In a three-electrode system | In a PEMWE | Ref. | |||
---|---|---|---|---|---|---|
η 10 (mV) | Stability | Pathway | Stability | T (°C) | ||
Mn–Co3O4@CN | 395 | — | — | 50 h @ 200 mA cm−2 | 80 | 116 |
RuCoOx | 200 | 100 h @ 10 mA cm−2 | DOM | 10 h @ 100 mA cm−2 | 85 | 113 |
Co3−xBaxO4 | 278 | 110 h @ 10 mA cm−2 | OPM | — | — | 118 |
Co9S8/Co3O4 | 275 | 40 h @ 10 mA cm−2 | OPM | 50 h @ 50 mA cm−2 | 80 | 119 |
Ir–Co3O4 | 236 | 30 h @ 10 mA cm−2 | — | — | — | 120 |
Co3O4@C/GPO | 360 | 40 h @ 10 mA cm−2 | — | — | — | 121 |
Co2MnO4 | — | 1600 h @ 200 mA cm−2 | LOM | — | — | 115 |
γ-MnO2 | 428 | 8000 h @ 10 mA cm−2 | — | 400 h @ 10 mA cm−2 | 25 | 122 |
LiMnP2O7 | 680 | — | — | — | — | 123 |
Certainly, as with all transition metal oxides in acidic environments, catalysts featuring MnO2 as the anode unavoidably confront dissolution in acidic electrolytes. Previous studies123,126,127 have suggested that the higher overpotential observed for MnO2 catalysts could be attributed to the instability arising from charge disproportionation caused by Mn3+ intermediates. Recently, several effective strategies have been proposed to mitigate the dissolution of Mn under acidic conditions.
For instance, Nakamura128 investigated the oxygen evolution reaction (OER) of rutile-type MnO2 with (101) and (110) crystal faces. Through in situ monitoring of Mn3+ intermediates, a linear relationship between the quantity and activity of Mn3+ intermediates was revealed. It was found that the presence of Mn3+ intermediates could enhance stability, a characteristic determined by the surface electronic structure of MnO2. While much of the development of MnO2 catalysts still occurs at low current densities, recent work by Xiao et al.129 achieved a remarkable improvement in stability. By increasing the proportion of planar oxygen in the MnO2 lattice, they enhanced stability by 40 times. Additionally, they achieved a current density of 2 amperes at 2 volts, with catalytic activity comparable to that of iridium. Overall, research on MnO2-based acidic OER catalysts remains in its nascent stages. One pressing issue to address is the alteration of MnO2 valence states at high potentials, which can result in instability in MnO2 performance. Additionally, the intrinsic activity of MnO2 requires further enhancement through strategies such as doping, introducing defects, and inducing strain, among others. The rational utilization of Pourbaix diagrams and other theoretical verification methods can offer guidance for screening non-noble metal elements stable in acids.
Overall, the high activity and stability of noble metal-based catalysts in acidic oxygen evolution reaction (OER) currently make them the most effective choice. However, their high cost and scarcity limit their large-scale application. Non-noble metal-based catalysts have significant potential for application due to their low cost and abundant resources, but their activity and stability require further enhancement. Future research should prioritize improving the performance of non-noble metal-based catalysts through nanostructure design, doping, and alloying, and developing new catalytic materials that balance high efficiency and cost control. These efforts are essential to achieving comprehensive advances in acid water electrolysis technology.
The advancement of earth-abundant OER catalysts with high activity and stability in acidic environments remains a formidable challenge. Progress in this direction requires a deeper comprehension of these catalysts' operational states and the characteristics of their active sites to enable precise control and adjustment of their properties. The integration of theoretical insights, computational modelling, and sophisticated in situ/operational characterization techniques will be instrumental in addressing these pivotal challenges. From the foregoing discussion, several key points emerge. Firstly, regarding IrO2-based catalysts, current research focuses on achieving low loading, high stability, and intrinsic activity. Strategies such as leveraging the structure effect, support effect, interface effect, defect effect, and molecular self-assembly effect show promise in enhancing the stability of IrO2 catalysts. Secondly, a significant challenge lies in reducing the dissolution rate of RuO2 at high potential. Effective approaches such as incorporating sacrificial components have been widely explored. Additionally, RuO2-based catalysts are emerging as the preferred alternative to Ir-based catalysts. Furthermore, research on non-noble metal acidic OER catalysts is still in its nascent stages. While practical application remains challenging at present, the field holds considerable potential for development. Lastly, it is crucial to underscore the importance of in situ characterization techniques such as in situ XPS, in situ synchrotron radiation X-ray absorption spectrometry (XAS), operando differential electrochemical mass spectrometry (DEMS), and in situ Raman analysis. These methods play a vital role in tracing catalyst evolution during OER processes. When combined with mechanism elucidation and catalyst design strategies, they enable more efficient catalyst design, leading to high-performance catalytic acidic OER under high current densities. Overall, the high activity and stability of noble metal-based catalysts in acidic oxygen evolution reaction (OER) currently make them the most effective choice. However, their high cost and scarcity limit their large-scale application. Non-noble metal-based catalysts, due to their low cost and abundant resources, hold significant potential for application, but their activity and stability require further enhancement. Future research should prioritize improving the performance of non-noble metal-based catalysts through nanostructure design, doping, and alloying, as well as developing new catalytic materials that balance high efficiency and cost control. These efforts are essential to achieving comprehensive advancements in acidic water electrolysis technology. The further development of advanced anode oxide-based electrocatalysts for proton exchange membrane water electrolyzers (PEMWEs) in acidic environments needs to address several key areas.
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