Open Access Article
Zhuxin Lyu†
a,
Yunpeng Wang†
ab,
Yueming Sun
a and
Yunqian Dai
*a
aSchool of Chemistry and Chemical Engineering, Southeast University, Nanjing, Jiangsu 211189, P. R. China. E-mail: daiy@seu.edu.cn
bSchool of Materials Science and Engineering, Hebei University of Science and Technology, Shijiazhuang, Hebei 050018, P. R. China
First published on 10th March 2026
High entropy oxides (HEOs) are gaining rapid attention due to densely distributed active centers, tunable surface areas, robust lattices, flexible geometries and self-balanced electronic states. These features give them activity and durability that single- or binary-metal oxides rarely match in thermal, electro- and photo- catalysis. We systematically examine four entropy-driven effects, namely high-entropy stabilization, severe lattice distortion, sluggish diffusion and cocktail-like multi-element synergy, all of which govern phase formation, defect chemistry and functional performance. By simultaneously optimizing the surface area, lattice robustness and scalable processing, we outline how porous architectures, low-temperature integrity, phase control and high-throughput manufacturing are merged into a single framework. Complex disordered structures of HEOs challenge traditional characterization, demanding advanced methods. In situ vibrational spectroscopy, operando X-ray characterization, DFT and artificial-intelligence converge to resolve the dynamic structure–property relationships that underpin HEO catalysis. We hope this review sparks wider interest in high-entropy oxides and accelerates their path from laboratory curiosity to industrial catalysts.
The high-entropy concept opens a broad design space for functional oxides. By mixing five or more cations on one sub-lattice, HEOs can stabilize disordered lattices, widen processing windows, and introduce local strain, charge imbalance, and bonding heterogeneity that are difficult to realize in conventional solids.7–9 These features yield greater thermal robustness, slower ionic inter-diffusion and emergent electronic or catalytic properties that surpass the sum of the parts.10–12 Yet most studies remain empirical or focus on isolated cases; what is still missing is a unified framework that ties high entropy, severe lattice distortion, sluggish diffusion and cocktail-like multi-element cooperativity to measurable performance gains and explains how they act in concert to control structure formation, stability and property emergence.13,14 Establishing a unified framework linking entropy, structure, and catalytic function will accelerate rational design and industrial deployment of high-entropy oxides from laboratory to catalysis and energy technologies.
Anchored in the synergy among configurational entropy, structural disorder, and functional performance, this review establishes an entropy–structure–function paradigm that elucidates how thermodynamic design principles govern the genesis of catalytic properties in high-entropy oxides. Specifically, configurational entropy serves as a tunable thermodynamic variable that expands accessible compositional spaces and entropy-stabilizes single-phase oxides against phase separation, thereby enabling systematic tuning of multication compositions. This entropic stabilization generates structural complexity transcending the average crystal lattice to encompass local coordination environments, strain fields, and oxygen-sublattice distortions, which collectively govern defect formation and redox adaptability, ultimately translating compositional disorder into catalytic function through diverse adsorption strengths and cooperative multi-site reaction pathways. Building upon this foundation, we demonstrate how the high-entropy effect, lattice distortion effect, sluggish diffusion effect, and cocktail effect collectively dictate phase stability and property genesis, consolidating quantitative definitions and structural families of HEOs. We subsequently review advances in synthesis spanning low-temperature and high-surface-area routes, which lock in single-phase compositions while preserving active architectures. Furthermore, we integrate advanced in situ/operando probes, multiscale simulations and machine-learning workflows to decode dynamic structure–property relationships under realistic operating conditions. Finally, these insights are distilled into comprehensive design guidelines covering element selection, synthesis methods, mechanistic investigations, advanced characterization techniques, theoretical considerations, and scalable processing, offering a concise roadmap for translating high-entropy oxides from laboratory curiosities into scalable technologies for energy and environmental applications.
S = kB ln W
| (2-1) |
Here, kB represents the Boltzmann constant and W denotes the number of microscopic states of the system. Conformational entropy describes the diversity of arrangements of different components at equivalent lattice sites. The calculation formula for the configurational entropy of an oxide is
![]() | (2-2) |
Here, R represents the ideal gas constant, and xi and xj respectively denote the mole fraction of the x-th component (where x = i or j) at the cation sites and anion sites. It can be inferred that when the mole fractions of each component are equal, the value of ΔSmix will reach its maximum. As the number of components in the material system increases, the configurational entropy significantly rises. Based on this principle, researchers proposed the concept of high entropy, namely that when multiple metal elements coexist in nearly equal molar ratios, their high configurational entropy can effectively stabilize the solid-solution structure.18 Therefore, high-entropy oxides are defined as: an oxide system of solid solutions composed of five or more metal elements in an equimolar or nearly equimolar ratio. The phase stability of such oxides mainly depends on the high configurational entropy effect.
High-entropy oxides therefore represent a design space in which configurational entropy is treated as an explicit materials design parameter rather than a secondary effect. Studies on high-entropy ceramics and high-entropy oxides have emphasized that rational design requires simultaneous consideration of thermodynamic stability, mixing behavior on different sublattices, and kinetic constraints during synthesis.16,19 This perspective has motivated the development of phase stability maps, descriptor-based screening, and data-driven approaches that couple entropy with enthalpy, electronic structure, and defect chemistry.
In rock-salt-type high-entropy oxides (e.g., (MgCoNiCuZn)O), oxygen ions form a face-centered cubic sublattice, while divalent cations occupy octahedral sites (Fig. 1a).3 The random distribution of cations creates a chemically disordered yet topologically simple lattice, where the local environments of individual sites exhibit significant variations, yet long-range cubic symmetry is preserved. These materials have emerged as model systems for studying the formation of entropy-stabilized phases and also serve as functional materials with tunable electrical properties and defect chemistry characteristics. Systematic investigations of the electrical transport properties of rock-salt-type high-entropy oxides and their doped derivatives reveal the coexistence of hopping conduction and polaron conduction. The conductivity and activation energy of these materials can be modulated through cation selection and heterovalent substitution.21
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| Fig. 1 Structural types and four core effects in high-entropy oxides. Common crystal structures: (a) rock-salt, (b) fluorite, (c) perovskite, and (d) spinel structures. Four core effects: (e) high entropy effect, (f) lattice distortion, (g) cocktail effect, and (h) sluggish diffusion. Copyright 2022, Elsevier.46 | ||
The general formula of fluorite-type high-entropy oxides is typically AO2−δ, where A represents a mixture of tetravalent or mixed-valence cations, including rare-earth or transition-metal ions such as zirconium, hafnium, and cerium (Fig. 1b). In this structure, the cations are arranged in a face-centered cubic lattice, while oxygen ions occupy tetrahedral interstitial sites, with each cation having a coordination number of eight. Charge compensation is usually achieved through randomly distributed oxygen vacancies, the presence of which significantly influences ionic transport properties and thermal characteristics. Reported single-phase fluorite-type high-entropy oxides (e.g., Zr0.2Hf0.2Ce0.2Sn0.2Mn0.2O2−δ) exhibit extremely low thermal conductivity, moderate bandgaps, and excellent high-temperature structural stability.22 The combination of cation lattice disorder and mobile oxygen defects not only induces strong phonon scattering effects but also maintains the integrity of the fluorite structure. These materials hold great promise for thermal barrier coatings and multifunctional applications requiring tailored thermal transport properties.23
Perovskite high-entropy oxides extend the classical ABO3 framework to multi-principal cation compositions on the A site, the B site, or both (Fig. 1c). In many high-entropy perovskites, rare-earth and alkaline-earth ions share the A sublattice, whereas several transition metals occupy the B sublattice, which introduces extensive local distortions of the octahedra.24 Studies on high-entropy perovskite cathodes for solid oxide fuel cells have demonstrated that compositions with multiple A-site and B-site cations can still maintain a single perovskite phase with well-defined oxygen octahedra and controllable oxygen non-stoichiometry.25 The disordered cation distribution modifies the bonding environment and regulates the concentration and mobility of oxygen vacancies, which in turn governs electronic conductivity and surface exchange kinetics.
Spinel-type high-entropy oxides typically follow the general formula AB2O4, featuring a cubic crystal structure with the space group Fd
m (Fig. 1d). In this structure, oxygen atoms form a face-centered cubic (fcc) close-packed framework, while A-site ions predominantly occupy tetrahedral interstitial positions and B-site ions reside in octahedral sites under ideal conditions. Both A and B sites exhibit excellent multi-element accommodation, offering greater degrees of freedom for composition design and property modulation than rock-salt or fluorite-type high-entropy oxides. Existing studies have successfully synthesized single-phase spinel high-entropy oxides such as (Mn0.2Fe0.2Ni0.2Mg0.2Zn0.2)3O4, with characterization confirming uniform elemental distribution across the cation sublattices.26 The spinel topology endows A and B sites with rich redox activity and constructs interconnected diffusion channels, which facilitate the transport of both cations and anions. Electrochemical investigations on spinel high-entropy oxides (e.g., (Mg0.2Ti0.2Zn0.2Cu0.2Fe0.2)3O4) for lithium-ion battery applications, particularly as anode materials, have demonstrated that the multi-cation environment significantly accelerates reaction kinetics and enhances cycling stability. Moreover, the underlying spinel framework maintains structural integrity during repeated lithium insertion–extraction and phase transition processes.27
These four structure types provide a common structural basis for most high-entropy oxides reported so far. Rock-salt and fluorite lattices offer simple cation environments and high symmetry, which are advantageous for disentangling the effects of entropic stabilization and lattice distortion. Perovskite and spinel structures introduce multiple crystallographic sites, enabling more complex couplings between charge, spin, orbital, and defect degrees of freedom. Understanding how configurational disorder interacts with each of these structure families is essential for rational design of functional properties and for expanding high-entropy concepts to more complex oxide chemistries.28
Thermodynamically guided synthesis strategies have now made it possible to more precisely quantify the high-entropy effect. Heating can promote the formation of disordered solid solutions, while suppressing ion diffusion during cooling can preserve this disordered state. A recent thermodynamically inspired design study confirmed that by balancing the enthalpy interactions and configurational entropy of the system, it is possible to effectively predict whether a specific cation combination will form a single-phase high-entropy oxide or undergo phase separation. This provides a more predictive theoretical foundation for the compositional design of high-entropy oxides.31
Experimental and atomic simulation results from rare-earth high-entropy silicate model systems demonstrate that, compared to single-component reference materials, high-entropy compositions exhibit significant strain effects and fluctuations in bond strength at the atomic scale. These structural deformations reduce the material's lattice thermal conductivity and modulate its thermophysical properties over a wide temperature range.34 Similar phenomena have been observed in other high-entropy ceramics: the synergistic effects of structural deformation and mass fluctuations can lower thermal conductivity while maintaining phase stability. This characteristic holds significant importance for applications in thermal barrier coatings and thermoelectric fields.35
Similar phenomena also exist in high-entropy calcium titanate oxides. A multi-site calcium titanate La0.5Sr0.5Mn0.15Fe0.15Co0.4Ni0.15Cu0.15O3 electrocatalyst, achieved by B-site co-doping with multiple transition metals, delivers markedly improved oxygen evolution reaction performance, requiring an overpotential of only 309 mV at 10 mA·cm−2, which is lower than the low entropy oxide (396 mV).38 Analysis of the local structure and electronic states confirmed that the mixed B-site environment constructed abundant adsorption sites and reaction pathways, which is the core feature of the “cocktail effect”. Extensive research on high-entropy energy materials further indicates that this kind of synergistic effect is also manifested in dielectric responses, thermoelectric performance, and electrochemical cycling. The complexity of composition enables the materials to possess characteristics such as low thermal conductivity, excellent electrical conductivity, and chemical stability, which are often difficult to achieve simultaneously in traditional oxides and are of great significance for the development of related functional materials.39
In high-entropy oxides, the concept of sluggish diffusion has two primary applications. On the one hand, slow cation diffusion helps maintain a single-phase solid-solution structure during cooling and operation, thereby preserving entropy-stabilized phases and inhibiting grain growth. On the other hand, it facilitates controlled diffusion in solid electrolytes and battery materials, where one species (e.g., Li+ or O2−) must be mobile while the framework cations remain immobile. A recent study demonstrated that a multi-cation framework can create a kinetically stable host lattice while enabling rapid ion transport through a carefully designed defect network.11 Additionally, research on diffusion behavior across a wide compositional range of high-entropy oxides suggests that diffusion properties are better described by a distribution of migration energy barriers rather than a single activation energy, reflecting the complexity of local environments in these materials.42
Rather than acting in isolation, these four high-entropy effects cooperate (Table 1). The high-entropy effect arises from large configurational disorder. This disorder intensifies local lattice distortion as atoms of different sizes and electronic characters occupy the same lattice. The resulting distortion not only helps stabilize single-phase structures but also alters local bond strengths and electronic states.33 The distorted lattice creates a complex landscape of migration for atomic motion. In such a landscape, certain migration pathways have higher energy barriers while other pathways act as traps, slowing down net diffusion rates and reinforcing the sluggish diffusion effect.43 At the same time, the cocktail effect emerges from cooperative interactions among multiple elements. This synergy is modulated by both the degree of lattice distortion and the distribution of mobile species in the distorted lattice.44
| Entropy-driven effect | Core descriptor | Interaction | Experimental readouts | Representative catalytic outcome |
|---|---|---|---|---|
| High entropy effect | Phase stabilization | Amplifies lattice distortion; provides base disorder | XRD (phase purity); STEM-EDS (homogeneity); operando XRD/XAS (phase retention) | Stable activity after aging; suppressed phase separation |
| Lattice distortion | Local coordination dispersion | Reinforces the sluggish diffusion effect; tunes synergy | EXAFS; IR | Broadened adsorption-strength distribution; improved redox flexibility |
| Cocktail effect | Non-linear synergy | Enabled by distortion and distribution of sites | Composition libraries; high-throughput screening maps | Performance beyond linear mixing; co-optimization of activity and stability |
| Sluggish diffusion | Slowed sintering | Results from distortion; impacts species redistribution | Thermal aging and microscopy; diffusion tests; | Enhanced durability; slower deactivation; stable performance |
The roles of the four effects can be summarized as an entropy–structure–function map, where each effect is linked to a core structural descriptor, common experimental readouts, and representative catalytic outcomes (Table 1). Their concerted action flattens the free-energy landscape and frustrates phase separation. A quantitative example is provided by a high-entropy spinel (CoFeNiMnW)3O4, which delivers an OER overpotential of 256 mV at 10 mA cm−2 and maintains >200 h operation at an industrial current density of 500 mA cm−2 in alkaline media, while (CoFeNi)3O4 and Co3O4 display obvious degradation, with overpotentials increasing by 110 and 58 mV over 200 h.45 In a word, HEOs outperform their low- and medium-entropy counterparts in catalytic performance and thermal stability, turning compositional disorder into a systematic performance advantage.
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| Fig. 2 Synthesis strategies of HEOs. (a) Electrospinning route to high-surface-area single-phase spinel, perovskite, and rock-salt HEO nanofibers. Copyright 2024, American Chemical Society.47 (b) Porous high-entropy oxide nanofibers prepared by electrospinning. Copyright 2025, Wiley-VCH.48 (c) Mechanochemical synthesis of porous HE-MgAl2O4-type spinels. Copyright 2021, Elsevier.49 (d) Liquid-metal-assisted low-temperature hydrothermal synthesis of Ga-based high-entropy oxides. Copyright 2025, American Association for the Advancement of Science.53 (e) Magnetron sputtering for high-entropy spinel oxide thin films. Copyright 2025, Science Press.54 (f) The synthesis of ultrathin high-entropy oxides guided by a self-lattice framework, and with a controllable phase state. Copyright 2024, American Chemical Society.61 (g) Crystal-phase modulation of high-entropy perovskite oxides. Copyright 2025, Wiley-VCH.62 | ||
In addition to simply increasing the surface area, porous high-entropy oxide nanofibers can also act as dynamic supports, using configurational entropy to regulate easily sinterable nanoparticles under harsh conditions. In another paper that reported the synthesis of porous spinel-type high-entropy oxide nanofibers using electrospinning (Fig. 2b), the nanofibers were used as a carrier for ultrafine platinum.48 After severe thermal aging at 900 °C and subsequent treatment at 500 °C, entropy-driven platinum would re-disperse from aggregated lumps back to a smaller nanoparticle state, almost restoring the original CO oxidation activity. The high-entropy oxide nanofibers prepared using electrospinning technology were also used as catalysts with high surface area for the selective oxidation of volatile organic compounds. Optimizing spinning parameters and calcination conditions can yield a robust mesoporous network with uniformly distributed multielement active sites and improve the conversion rate and stability. These results collectively indicate that the high surface area and porous structure in fibrous high-entropy oxides not only provide more active sites but also enable entropy-driven metal–support interactions, which are difficult to achieve in traditional single-metal oxides.
In addition, high-entropy oxide powders and films with a high surface area and porous structure can be prepared by mechanical chemical methods and sol–gel methods. First, various metal precursors are subjected to high-energy ball milling (Fig. 2c), followed by calcination at a relatively low temperature to obtain the HE-MgAl2O4 catalyst with a BET surface area of approximately 139 m2·g−1. Its mesopore size distribution is narrow, and it exhibits excellent stability when oxidizing methane in a hot and humid feed, highlighting the ability of configurational entropy to stabilize crystal structures and mesopore frameworks.49 The sol–gel strategy can generate spherical mesoporous high-entropy oxides with surface areas ranging from 42 to 143 m2·g−1 and pore diameters of 5.5 to 8.3 nm. The polymerizable ligands and block copolymer templates define a spinel framework that remains porous even after crystallization.50
By introducing gallium as the reaction medium, gallium-based high-entropy oxides with tunable properties can be synthesized under low-temperature conditions.53 In this method, first, the multi-metal precursors are assembled onto the liquid gallium through the hydrothermal method, and then after calcination at a temperature of only 400 °C (Fig. 2d), single-phase gallium-based high-entropy oxides with rock salt, spinel or perovskite structures can be obtained, depending on the adjustment of the ionic radius and valence. The negative mixing enthalpy between gallium and transition metal species reduces the overall Gibbs free energy of the mixture, and together with the inherent dynamic liquid metal environment, promotes uniform cation distribution and inhibits separation phenomena even below the traditional entropy-stable temperature.
Magnetron sputtering technology is a low-temperature vapor-phase synthesis method that can produce high-entropy oxide films with uniform composition, uniform coverage, and a nano-scale grain structure. By sputtering high-entropy alloy target materials onto nickel foam at a low substrate temperature with argon as the protective gas, a uniform multielement layer is formed. This layer spontaneously oxidizes in the air to form a single-phase spinel film ((FeCoNiCrMo)3O4) (Fig. 2e), with the average size of its nano-crystals approaching 2.5 nm.54 The resulting film has an oxygen evolution overpotential of approximately 216 millivolts at a current of 10 microamperes per square centimeter, and can maintain stability for over 200 hours at a current of 100 microamperes per square centimeter. This indicates that the low-temperature sputtering oxidation process can lock in an unstable multi-ion structure while generating a large number of grain boundaries and defect sites. Due to the relatively mild substrate temperature and subsequent treatment, the volatile-driven component drift is minimized, and the cation distribution is mainly controlled by the sputtering jet rather than by high-temperature diffusion, which is beneficial for precisely designed high-entropy compositions.
In addition, the researchers employed a solvothermal–annealing strategy to prepare single-phase spinel high-entropy oxides (Co, Cu, Fe, Mn, Ni)3O4 with an average particle size of approximately 5 nanometers. The synthesis temperature was much lower than that of traditional ceramic processing, and it exhibited excellent activity for water decomposition.55 Due to the enhanced transport and nucleation dynamics of supercritical water, high-entropy spinel nanoparticles with uniform cation mixing and OER activity can be directly generated through supercritical hydrothermal treatment.56 Moreover, this concept of continuous supercritical hydrothermal flow has been extended to continuous flow reactors. In these reactors, this process allows HEO to form at relatively low temperatures within a timescale of seconds. The synthesized perovskite-type HEO natural gas molecules contain 10 metal elements, indicating that by carefully controlling the hydrothermal conditions, extremely complex components can be stabilized without the need for high-temperature sintering methods.57
Taken together, liquid-metal, vapor-phase, and hydrothermal low-temperature methods clarify several core principles for the design of high-entropy oxides. Mixed enthalpy, configurational entropy, and reaction environment must be engineered in a coordinated manner. The thermodynamic driving forces for phase separation and component volatility should be weakened, while the contribution of configurational entropy must remain sufficient to stabilize a single high-entropy phase. When this balance is reached, high-entropy oxides with robust properties, metastable lattices, and precisely preserved multication compositions can be synthesized at relatively low temperatures.
A typical example is the self-lattice framework strategy, in which the coordination preferences of cations are used to pre-design the target structure, while the Ga assistor can effectively reduce the phase's formation energy (Fig. 2f). By combining appropriate cation groups with the Ga assistor, ultra-thin high-entropy oxide nanosheets with phases such as rock salt, spinel, perovskite and fluorite phases have been obtained. This not only enables the controllable synthesis of the target phases but also effectively inhibits the formation of impurity phases.61 The sol–gel method also provides an effective way for precise control of phases in the same composition system (Fig. 2g).62 In the high-entropy LaB5O3 perovskite system, by increasing the complexity of the B-site cation composition, the system can be induced to transform from the tetragonal crystal system to the cubic crystal system, and this crystal transformation process is accompanied by an increase in the lattice distortion degree, an increase in oxygen vacancy concentration, and a synergistic optimization of nitrate reduction and sulfide oxidation performance.
Regulation strategies based on kinetic energy and strain offer diverse approaches for manipulating the phase and enhancing structural stability in HEOs. The flame spray pyrolysis technique enables the fabrication of single-phase high-entropy spinel nanoparticles within a millisecond time scale, where rapid quenching captures distorted spinel lattices with uniform cation distribution, an effect that is difficult to achieve via conventional slow solid-state sintering.63,64
Overall, these strategies show that configurational entropy, lattice distortion, kinetics and strain can be combined to select desired phases and keep them structurally robust under electrochemical and thermal stresses.
Rapid Joule heating synthesis represents a crucial step toward large-scale fabrication of HEOs. By directly applying an electric current to nickel foils coated with a precursor layer, high-entropy rock-salt, spinel, and perovskite oxides can crystallize within tens of seconds rather than hours, while retaining a single-phase structure and a high specific surface area.68 The extremely steep thermal gradients and rapid cooling facilitate the inhibition of phase separation and enable the incorporation of elements that are difficult to stabilize under conventional calcination conditions, thereby expanding the accessible compositional space. Further studies on Joule-heated nanomaterials have demonstrated that this method can produce defect-rich, nanocrystalline high-entropy systems and related multimetallic nanoparticles with tunable grain sizes, highlighting the potential of integrating HEO synthesis with continuous production architectures.69,70
For thin-film architectures and device-oriented HEOs, combinatorial sputtering provides a prototypical high-throughput manufacturing strategy. A notable example is the fabrication of a Ba(Ti, Zr, Ta, Hf, Mo)O3 high-entropy film library on Si using multi-cathode sputtering and a physical mask, which yields one hundred distinct metal–oxide-semiconductor capacitors on a single wafer.71 Beyond single libraries, high-throughput sputtering and related combinatorial approaches are being generalized into modular discovery and scale-up pipelines. Perovskite La(XYZ)O3 thin-film libraries prepared by combinatorial sputter deposition provide dense maps of phase fields and property landscapes, illustrating how multi-dimensional composition spaces can be navigated efficiently before committing to bulk synthesis.72
Researching new materials is often a complex process. High-throughput calculations can provide more accurate results. However, as material structures become more diverse and complex, relying solely on DFT-based high-throughput systems faces many challenges. This greatly limits the exploration of HER electrocatalysts.73 Machine learning is an important modern technology. When combined with high-throughput calculations, it can build prediction models that are more efficient and accurate than DFT calculations.74 This helps to quickly screen catalysts and discover new descriptors. In recent years, machine learning has become widely used as an efficient tool in computational materials science, with reports of its success in many fields.75,76
In summary, the high-throughput, scalable HEO manufacturing technology is evolving from the proof-of-concept stage to a multifunctional toolkit that integrates rapid synthesis, library-scale screening, and precise amplification for energy and electronic applications.
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Fig. 3 In situ vibrational spectroscopy of HEO catalysts and their catalytic performance. (a–d) In situ DRIFTS spectra of CO2 and CH4 adsorption over high-entropy (Ni3MoCoZn)Al12O24 nanofiber catalysts prepared by electrospinning (a and b) and their coprecipitated counterparts (c and d) during dry reforming of methane. Copyright 2024, American Chemical Society.47 (e and f) C3H6 oxidation performance of spinel (Ni0.2Mg0.2Cu0.2Zn0.2Co0.2)Cr2O4 and single-component ACr2O4 (A = Zn, Cu, Ni, Co, Mg) catalysts, (20 000 mL h−1 g−1; the feed gases contain 1vol% C3H6, 99 vol% air). (e) light-off curves under dry feed and (f) long-term stability tests in the presence of water vapor. Copyright 2024, Springer Nature.81 (g–l) In situ DRIFTS spectra for photocatalytic CO2 hydrogenation over ceria-based fluorite-type HEOs and CeO2 at different temperatures and reaction times. Copyright 2024, American Chemical Society.82 | ||
In situ FTIR and Raman spectroscopy were used to probe hydrothermal stability in spinel-type high-entropy oxides.81 Under humid reaction atmospheres, vibrational spectra indicate a significantly reduced accumulation of surface hydroxyl groups compared to those of conventional binary spinels. This suppression of hydroxyl poisoning correlates strongly with improved catalytic stability. When interpreted alongside thermodynamic and structural analysis results, these spectroscopic results revealed that multication disorder lowers water adsorption affinity and facilitates rapid removal of surface hydroxyls. This combination of vibrational evidence provides a mechanistic explanation for why HEO catalysts maintain activity under moisture-rich conditions where conventional oxides deteriorate (Fig. 3e and f).
In situ DRIFTS has also been used to clarify the photocatalytic CO2 hydrogenation mechanisms on fluorite-type HEOs.82 During light-driven reactions, DRIFTS spectra capture the formation of formate, carbonate and CO-associated intermediates (Fig. 3g–l). The evolution process of these substances with changes in temperature and time indicates that the high configurational entropy will increase the concentration and heterogeneity of oxygen vacancy sites. These vacancy-related environments modulate the CO2 adsorption geometry and hydrogenation behavior, resulting in enhanced CO and methanol production. Through operando spectral monitoring, DRIFTS provides mechanistic evidence linking entropy-driven defect chemistry to improved CO2 hydrogenation performance.
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| Fig. 4 Operando and ex situ X-ray absorption spectroscopy of high-entropy oxide anodes. (a–f) Co, Ni, and Cu K-edge XANES spectra in an operating HEO battery as a function of the delivered capacity in the lithiation process. Copyright 2020, American Chemical Society.83 (g–j) Ni, Co, Mn, and Fe K-edge XANES spectra of spinel high-entropy oxide (Ni0.2Co0.2Mn0.2Fe0.2Ti0.2)3O4 (NCMFT). (k) Experimental Fourier transforms of the Ni, Co, Mn, and Fe K-edge EXAFS spectra of NCMFT. Copyright 2020, Royal Society of Chemistry.84 | ||
Complementary operando XRD provides insight into structural transformations during electrochemical cycling. In spinel-type HEO electrodes, operando XRD studies have shown reversible lattice expansions, phase transitions and conversion-to-rock-salt transformations under repeated cycling (Fig. 4g–k).84 These features help explain the high capacity and also the structural fragility of such compositions. The simultaneous presence of multiple metal species leads to multi-step changes in diffraction peak positions, reflecting lattice distortions driven by compositional fluctuations.
After modeling the OER performances of different compositions of AuIrOsPdPtReRhRu using machine learning (ML) models, it was found that AuIrOsPdRu was the best catalyst.87 Then, DFT was utilized to provide a complementary theoretical model with clear assumptions. DFT calculations indicated that most of the activity came from the Ru and Ir active sites, and the addition of Pd enhanced the performance of these sites. Overall, ML can help accelerate the discovery of catalysts, by combining ML models based on experimental data with DFT calculations models, providing important insights into the complex chemistry of OER catalysts.
From a catalytic perspective, DFT screening of adsorption energies and reaction barriers on model HEO surfaces provides mechanistic insight into synergistic effects. Such calculations often rely on reduced-complexity surface models where only a subset of cations is varied explicitly, but recent work is starting to integrate fully random cation distributions combined with configurational averaging to more faithfully represent HEO surfaces.88
ML is particularly well-suited to HEOs because of the vast size of the compositional design space. One recent study used supervised learning models to accelerate the discovery of entropy-stabilized oxide catalysts for oxidation reactions.89 The workflow combined a curated dataset of compositions, phase information and catalytic performance metrics with composition-derived descriptors such as cation electronegativity differences, ionic radius mismatch and valence electron configuration statistics. Models trained on this dataset were used to predict both phase stability and catalytic activity across large composition libraries. The ML-guided predictions identified composition regions with high probability of forming single-phase entropy-stabilized oxides that also exhibited superior oxidation activity. Targeted synthesis and testing confirmed many of these predictions, demonstrating a closed-loop cycle from data to model to experiment (Fig. 5a). This work provides a template for data-driven exploration of HEO catalysts that is significantly more efficient than manual trial-and-error.
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| Fig. 5 Machine-learning strategies for the discovery and design of new HEO nanomaterials. (a) Schematic illustration of the ML approach employed to predict and acquire the structural and catalytic properties of the ACr2Ox system. Copyright 2025, American Chemical Society.89 (b) Operational workflow of the ML-driven analytical process utilized for investigating multicomponent ORR catalysts in alkaline environments. Copyright 2024, Royal Society of Chemistry.90 (c) Hybrid-flow ML framework for designing high-entropy layered Na-ion cathodes. Copyright 2025, Wiley-VCH.91 | ||
ML has also been applied to multicomponent oxide electrocatalysts for the oxygen reduction reaction (ORR). Models trained on compositional and structural features have been used to predict ORR activity trends in multicomponent oxides and to identify compositional descriptors that correlate positively with the current density and onset potential (Fig. 5b).90 These studies reinforce the notion that configurational entropy and cation diversity can be treated as quantitative design variables in catalyst optimization.
Moreover, ML methodologies have been extended to high-entropy cathodes for sodium-ion batteries and related energy-storage systems.91 In these workflows (Fig. 5c), composition descriptors are combined with structural stability data and electrochemical performance metrics to train models that predict capacity retention, voltage profiles and structural robustness. The models highlight specific combinations of s-block and transition-metal cations that favor layered or polyanionic frameworks with good cycling stability.
ML interatomic potentials enable atomistic simulations of high-entropy oxides over supercell sizes and timescales that are prohibitive for conventional DFT. In one study, a machine-learning potential was constructed to reproduce energies and forces across a wide range of compositions and configurations for rock-salt HEOs.92 The resulting model was then used to map mixing enthalpies, bond-length distributions and structural stability for thousands of candidate compositions. This approach identified known entropy-stabilized compositions and predicted additional stable or metastable candidates, illustrating the power of ML potentials for high-throughput computational screening. Combined with thermodynamic modelling and experimental validation, such tools can greatly expand the accessible HEO design space.
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| Fig. 6 High entropy oxide catalysts for thermally driven reactions. (a) Schematic illustration of in situ exsolution and dissolution of CoFeCuNi alloy nanoparticles from the high-entropy Zr0.5(NiFeCuMnCo)0.5Ox host under H2 reduction and oxidative treatment. (b) Catalytic performance of Zr0.5Cu0.5Ox, Zr0.5Mn0.5Ox, Zr0.5Co0.5Ox, Zr0.5Ni0.5Ox, Zr0.5Fe0.5Ox, Zr0.5(CuMn)0.5Ox, and Zr0.5(NiFeCuMnCo)0.5Ox in CO2 hydrogenation at 400 °C. Copyright 2021, Springer Nature.94 (c) The effect of the CuCeOx-HEO hetero-structure on the outstanding high-temperature stability during CO oxidation. (d) The temperature-dependent conversion of CO for CuO-CeO2, ZnO-CeO2 and Cu-ZnOx-CeO2. Copyright 2020, Elsevier.100 | ||
The same design philosophy appears in other redox active HEOs. Spinel type Co3MnNiCuZnOx nanoparticles can generate CuCoNi nanoalloys at the surface under reducing conditions and re-incorporate them when the gas feed becomes oxidizing. This dynamic exchange maintains a high density of metal–oxide interfaces and protects small particles from coalescence, which leads to sintering resistant performance in CO2 conversion and related redox reactions.95
In parallel, fluorite structured high entropy oxides containing Zr, Y, and multiple transition metals have been used as hosts for isolated Pd species. In these materials, configurational entropy stabilizes atomically dispersed Pd–O complexes that hydrogenate CO2 to formate through a non-classical pathway, achieving high turnover frequency and selectivity to formic acid under relatively mild conditions.96
A complementary strategy uses a family of high entropy oxides in which the relative amount of Fe is systematically varied. Non equimolar compositions based on Cr, Co, Mn, Ni, and Fe form highly crystalline oxides with controlled oxygen vacancy concentrations. These materials afford high methane yields and maintain their structures after long term CO2 methanation, which is attributed to the balance between reducible Fe rich motifs and more stable cation environments.97
Heterostructured architectures that combine HEO domains with conventional oxides provide additional ways to regulate oxygen mobility. In the CuO–CeO2 system, a high entropy (NiMgCuZnCo)O support can be interfaced with ceria to form a multiscale composite.100 The entropy stabilized oxide anchors copper species and restrains their sintering, while the CeO2 phase offers fast oxygen transport. After aging at 900 °C, the heterostructured catalyst retains high CO conversion and displays delayed deactivation compared with low entropy references. The high-entropy (NiMgCuZnCo)O layer encapsulates the CeCuOx aggregates and restricts their mobility during the high-temperature treatment process (Fig. 6c). The CO conversion rate curve indicates that the composite material based on HEO has superior stability compared to the traditional CuO–CeO2 catalyst (Fig. 6d).
HEOs serve as thermally stable oxygen activation platforms, achieving low activation temperatures and sintering resistance through the configuration of entropy, high oxygen vacancies, and engineered HEO-oxide interfaces, thereby reducing reliance on precious metals.
In electrocatalytic reactions, the multi-component cation sublattice allows synchronous optimization of metal–oxygen covalency, thereby tuning the distribution of key intermediates such as *OH, *O, and *OOH. Rock-salt, spinel, perovskite, and layered HEOs have demonstrated correlated behaviors in the OER, ORR, nitrate reduction reaction (NO3−RR), and battery electrode performance.103 This design strategy is equally applicable to rechargeable battery systems, wherein lattice distortion, sluggish diffusion kinetics, and the “cocktail effect” markedly influence redox potentials, ion diffusion pathways, and mechanical stability during repeated intercalation processes. The following sections will focus on the mechanistic insights and performance of HEOs in oxygen electrocatalysis, nitrate reduction reactions, as well as lithium-, sodium-, and zinc-based battery systems.
High-entropy oxides with tailored oxygen vacancies have been synthesized through non-equilibrium thermal shock. The FeCoNiCrCuO HEO with an oxygen-vacancy-rich surface exhibited an overpotential of about 256 mV at 10 mA cm−2 in alkaline media (Fig. 7b) and a small Tafel slope (Fig. 7c). The four-electron transfer process of the OER was calculated using density functional theory to determine its free energy change (Fig. 7a). The results proved that the presence of oxygen deficiency is beneficial to the OER process.106
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| Fig. 7 HEOs for electrocatalysis. (a) OER mechanism on the oxygen-vacancy-rich FeCoNiCrCuO in alkaline medium (1 M KOH; Fe: purple spheres, Co: blue spheres, Ni: blue-gray spheres, Cr: gray spheres, Cu: orange spheres, and O: red spheres). (b) Linear sweep voltammetry scans for FeCoNiCrCuO, FeCoNiCrCuO-A1 and FeCoNiCrCuO-A2. (c) Comparison of overpotentials at 10 mA cm−2 for the three catalysts ([1] FeCoNiCrCuO, [2] FeCoNiCrCuO-A1, and [3] FeCoNiCrCuO-A2). Copyright 2025, Elsevier.106 (d) Characteristics of low-entropy spinel oxide with integrated single octahedral sites and high-entropy spinel oxide with bipolar dual-active sites for the OER/ORR. (e) ORR/OER performances of spinel oxides and commercial catalysts (Pt/C and RuO2) in 1 M KOH at a rotating speed of 1600 rpm. Copyright 2024, Wiley-VCH.108 (f) FENH3 values of p-(CoMnFeNiCu)3O4, meso-(CoMnFeNiCu)3O4 and meso-Co3O4. (g) Tandem electrocatalytic NO3−-to-NH3 mechanism of meso-(CoMnFeNiCu)3O4. Copyright 2025, Wiley-VCH.110 | ||
HEOs are frequently used as model systems to investigate the structure–activity relationships of the OER. Research on high-entropy OER catalysts based on oxide frameworks shared by multiple transition metals demonstrates that the coexistence of various cations can broaden the d-orbital range, reduce orbital degeneracy, and optimize the distribution characteristics of surface binding energy. This results in their significantly enhanced intrinsic activity and stability in overall water splitting compared to those of their single-metal or binary-metal-based counterparts.107
HEOs can also decouple oxygen redox reactions from structural degradation. A recent study on high-entropy-induced electric dipole transitions constructed bipolar dual-active sites in multi-component oxides (Fig. 7d), achieving reversible oxygen redox reactions (Fig. 7e) while mitigating the coupling effect between surface lattice oxygen oxidation and bulk structural collapse.108 The dual-active site design balances the redox processes of transition metal centers and oxygen centers. This mechanism is not only closely related to the OER but also applicable to the cathode operation of oxygen redox-active batteries. In catalysis, such bipolar sites can facilitate adsorption and desorption in oxygen electrocatalysis, providing a new approach to simultaneously enhance the OER and ORR on the same high-entropy oxide surface.
For the ORR, high-entropy spinel-type oxides have been reported as efficient cathode catalysts in metal–air configurations. In multicomponent spinels designed for the alkaline ORR, homogeneous distribution of several transition metals in octahedral and tetrahedral sites improves the number and accessibility of redox-active centers, while the strong lattice distortion maintains structural integrity under large potential windows.109 When integrated into zinc–air battery cathodes, such HEOs deliver high half-wave potentials (E1/2) and superior cycling stability compared with conventional perovskites or noble-metal catalysts, demonstrating the promise of HEOs as bifunctional air electrodes coupling the ORR and OER.
In the field of oxygen electrocatalysis, the mapping of composition–activity relationships has progressively advanced through high-throughput experiments and computational simulations of the HEO space. A recent study systematically explored the composition-combination space of polycationic oxides, revealing intrinsic correlations among the local structure, electronic occupation states, and OER activity across numerous HEO systems.87 Such data-driven research methodologies are well-suited to the inherently high-dimensional design space of HEOs, potentially accelerating the screening of optimal compositions for the ORR, OER, and related electrocatalytic processes.
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| Fig. 8 High-entropy oxide electrodes for rechargeable batteries. (a) Schematic illustration of the lithium-storage mechanism of the spinel-type 6-SHEO anode, showing the reversible evolution among highly crystalline spinel, distorted spinel, and distorted rock-salt phases during the first discharge/charge process. (b) Long-term cycling performance and coulombic efficiency of the 6-SHEO anode at 0.2 A·g−1. (c) Rate capability of 6-SHEO at different current densities. Copyright 2022, MDPI.112 (d) Schematic comparison of structural evolution and solid-electrolyte interphase formation for NHEO-PVDF and NHEO-PAN500 electrodes upon repeated lithiation. (e) Radar plot comparing capacity, rate performance, cycling stability and related metrics of NHEO-PAN500 with representative conversion-type anodes. Copyright 2024, Wiley-VCH.115 (f) Schematic configuration of a solid-state sodium-ion battery employing an O3-type Na0.95Li0.06Ni0.25Cu0.05Fe0.15Mn0.49O2 high-entropy layered cathode and a PVDF-HFP/SiO2/PC polymer solid electrolyte. (g) Rate performance of the Na0.95LNCFM polymer solid-state battery at various C-rates. (h and i) Long-term cycling performance and coulombic efficiency of the Na0.95LNCFM PSE battery at 2C and 5C. Copyright 2023, Springer.117 | ||
Moreover, HEO structures shorten lithium-ion diffusion pathways, expand the contact area between electrodes and electrolytes, and increase internal voids. Such voids effectively mitigate volume expansion during cycling. The high-entropy lattice constructs a spatial support network for lithium insertion/extraction processes, safeguarding structural integrity throughout material cycling and ultimately conferring exceptional cycling stability.113,114
Polyacrylonitrile (PAN) was employed as a binder to form a cyclised polyacrylonitrile (cPAN) outer layer on the NHEO surface (NHEO-cPAN) via an in situ thermochemical cyclisation reaction (Fig. 8d).115 The in situ-formed cyclic polyacrylonitrile coating not only enhances electrical conductivity but also improves structural and interfacial stability. The resulting NHEO-cPAN electrode exhibits significantly enhanced rate performance and cycling stability (Fig. 8e). This study demonstrates that combining the high-entropy design of bulk materials with tailored surface layers represents an effective pathway for developing commercially viable HEO-based lithium-ion battery anodes.
These concepts have been applied to practical cathode designs. A high-entropy O3-Na0.95Li0.06Ni0.25Cu0.05Fe0.15Mn0.49O2 cathode for solid-state SIBs (Fig. 8f) delivered high reversible capacity, exceptional rate capability and long-term cycling stability (Fig. 8g–i).117 Incorporating multiple transition metals and Li+ into the O3 lattice alleviates lattice stress and boosts ionic conductivity. This enables rapid, reversible O3−P3 phase transition while inhibiting irreversible structural alterations. Structural characterization techniques such as high-resolution electron microscopy and in situ monitoring uncovered homogeneous element distribution and robust lattice evolution under high-rate cycling. These features represent the signature advantages of high-entropy design.
High-entropy layered oxide cathodes for SIBs have been shown to combine high Na content, favorable redox potentials and improved structural integrity, making them promising candidates for large-scale stationary applications where cost and resource abundance are crucial. Design guidelines emerging from these studies stress the importance of carefully selecting transition-metal combinations and dopants to balance charge compensation, oxygen redox participation and mechanical stability.118
000 cycles at 2 A·g−1.119The concept of high entropy has been further extended to the design principles of ZIB materials, encompassing both electrode and electrolyte components. The high-entropy material design philosophy for ZIBs indicates that high-entropy doping or multi-cationic frameworks can optimize diffusion pathways, regulate solvation structures, and alleviate local stresses.120 When combined with in situ characterization, these designs reveal that distributing redox and structural roles among multiple cations reduces the likelihood of catastrophic phase transitions and allows more homogeneous Zn2+ insertion, which is essential for long-term durability in aqueous environments.
By merging high-entropy structural design with detailed mechanistic understanding from operando methods, HEO-based ZIB cathodes are moving toward practical performance targets for grid-scale storage.
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| Fig. 9 High-entropy oxide photocatalysts for visible-light H2O2 production and antibiotic degradation. (a and b) Charge density difference plots for water and oxygen adsorption on representative cation sites of an octonary rutile-type TiVCrNbMoWCuAl high-entropy oxide. The visualized electron accumulation and depletion regions highlight how Mo and W sites favor water activation while V and Cu sites facilitate oxygen activation through distinct adsorption configurations. (c) Photocatalytic H2O2 production with TVCNMWCA-HEO, other septenary high-entropy oxides, and TiO2 in pure water under visible light irradiation (λ ≥ 420 nm, 300 mW cm−2). Copyright 2024, Springer Nature.125 (d) Schematic band structure and reaction pathway for visible-light-driven degradation of antibiotic pollutants over spinel (FeCoNiCuZn)aOb_550 NPs. Visible light-induced photocatalytic degradation of (e) sulfamethoxazole (SMX) and (f) ofloxacin (OFX) by FeCoNiCuZn and (FeCoNiCuZn)aOb NPs. Copyright 2024, Royal Society of Chemistry.130 | ||
(La0.2Ce0.2Gd0.2Zr0.2Fe0.05)O2 nanoparticles confirmed that the material exhibits photocatalytic degradation of tetracycline hydrochloride. Its superior performance provides another route to improve photocatalytic degradation, as controlled introduction of Fe cations and associated oxygen vacancies produces higher carrier densities and more adsorption sites for pollutants.128 Layered bismuth-based high-entropy oxides extend this concept to two-dimensional architectures. These materials offer internal electric fields and exposed bismuth-oxygen motifs that cooperate to accelerate photogenerated carrier separation, leading to efficient degradation of methyl orange.129 Across these investigations, the multicomponent oxide matrix expands the absorption range. It provides diverse adsorption configurations for pollutants and reactive oxygen intermediates, enabling multiple oxidative pathways to proceed simultaneously.
Magnetic high-entropy spinel oxides offer promising potential for practical water treatment. Spinel (FeCoNiCuZn)aOb nanoparticles, synthesized via thermal decomposition, exhibit strong visible-light absorption, abundant surface oxygen defects, and enhanced charge separation and transfer.130 Under visible light, these nanoparticles effectively degrade sulfamethoxazole and ofloxacin within ninety minutes. Band structure analysis shows that the conduction and valence bands align with the redox potentials necessary for ˙O2− and ˙OH. As reactions take place on the surface, ˙O2− and ˙OH along with holes act on the antibiotic molecules adsorbed on the HEO NPs, finally breaking them down into simpler compounds (Fig. 9d). Photodegradation tests indicate that the high-entropy spinel outperforms both the parent multimetal alloy and simple oxide references. Concentration–time profiles demonstrate negligible pollutant loss in the dark, followed by rapid degradation under light, confirming a photocatalytic reaction rather than adsorptive processes (Fig. 9e and f).
These examples illustrate how compositional complexity, defect engineering, and magnetic functionality can be integrated within HEOs to deliver photocatalysts that couple strong and tunable light absorption with robust redox activity and convenient separation. Insights from water splitting, hydrogen peroxide generation, and pollutant degradation point to common design principles. These include constructing high-entropy lattices that stabilize dense oxygen vacancies, distributing multiple cation species to create a spectrum of adsorption sites for reactants and intermediates, and using band-gap engineering to align semiconductor levels with targeted redox couples.
However, despite these advantages, several challenges still need to be addressed to realize the potential of HEOs.
(1) Phase stability under operating conditions is still a key risk. Because the chemical potential of oxygen and surface adsorbates changes, the entropy-stabilized phases at synthesis temperature may transform during catalysis. Surface reconstruction, cation leaching, and redox-driven segregation can occur even when the bulk remains a single phase. Future work needs stability criteria that match operating, not only synthesis phase purity.
(2) Machine learning is becoming essential, but model transferability is a major challenge for HEOs. It can accelerate the exploration of HEO configuration space by learning structure–property relationships and by guiding where to sample next. Recent work also shows the potential of machine-learning interatomic potentials to study disorder and stability beyond conventional DFT limits. Still, robust performance requires curated datasets, physically meaningful descriptors, and validation across synthesis routes and measurement platforms.
(3) HEOs often require tight control over composition uniformity, oxidation states, and defect populations. These targets become harder to maintain when synthesis is scaled up from milligram powders to gram-scale batches, or when materials are transferred from thin-film libraries to bulk catalysts. Small changes in precursor chemistry, heating profiles, and mass transport can cause composition drift, local segregation, or morphology collapse. These variations reduce reproducibility across laboratories and limit practical translation. Future work should focus on process–structure mapping and on reporting synthesis windows with clear tolerances. It is also important to validate that the composition, phase, and defect descriptors remain consistent after scale-up and after shaping into electrodes or devices. This scale-up validation is increasingly viewed as a key step for moving HEOs from discovery to application.
The future of HEOs holds great promise, particularly as advancements in synthesis techniques and mechanistic understanding continue. Looking forward, further investigation into the atomic-level structure and active sites by integrating advanced characterization techniques with computational tools such as DFT and ML will provide new insights into understanding their outstanding catalytic performance. Understanding these mechanisms will enable the rational design of HEOs tailored to specific applications, from catalysis to energy storage. At the same time, developing low-temperature and high-throughput synthesis methods will be essential for scaling up the production of HEOs, making them more cost-effective and widely accessible. HEOs also present an exciting opportunity for sustainable technologies, where they could replace expensive noble metals. As the stability and scalability of HEOs improve, their integration into industrial applications will become more feasible, helping to address both environmental and energy challenges.
Footnote |
| † These authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2026 |