Hang
Li
a,
Li
Ling
b,
Shengfa
Li
a,
Feng
Gao
*b and
Qingyi
Lu
*a
aState Key Laboratory of Coordination Chemistry, Coordination Chemistry Institute, Collaborative Innovation Center of Advanced Microstructures, School of Chemistry and Chemical Engineering, Nanjing University, Nanjing 210023, P. R. China. E-mail: qylu@nju.edu.cn
bDepartment of Materials Science and Engineering, Jiangsu Key Laboratory of Artificial Functional Materials, Collaborative Innovation Center of Advanced Microstructures, College of Engineering and Applied Sciences, Nanjing University, Nanjing 210023, P. R. China. E-mail: fgao@nju.edu.cn
First published on 26th September 2023
In recent years, high entropy nanomaterials (HEMs) have become a rapidly developing research field. Due to their multi-element composition and unique high entropy state, HEMs produce four typical effects (high entropy effect, sluggish diffusion, severe lattice distortion and the so-called cocktail effect) that lead to adjustable activity and enhanced stability. These HEMs have received a great deal of attention in catalyst design and exploration. However, this great potential also comes with great challenges, which is called the coexistence of opportunity and crisis. The challenges arise from their broad element composition and complex atomic arrangement configurations, which prevent the thorough and detailed study of HEMs synthesis and their inherent mechanism understanding. Due to the introduction of anions, high entropy compounds usually have more complex high configurational entropy relative to high entropy alloys, which can provide unexpected properties conducive to a wide range of applications in catalysis. Herein, we review the synthesis, structural design and electrocatalytic applications of HEMs electrocatalytic materials in recent years. Firstly, the development and the advanced characterization methods of HEMs are reviewed. Then, the superior properties of the HEMs due to their multi-element properties are discussed in different electrocatalysis applications including oxygen reduction reaction (ORR), oxygen evolution reaction (OER), hydrogen evolution reaction (HER), carbon dioxide reduction reaction (CO2RR) and alcohol oxidation. Finally, we point out the existing challenges and propose solutions to these challenges in order to promote the development of HEMs in the field of electrocatalysis.
The basic principle of HEMs is that forming a single phase material with a high ratio of five or more main elements (equimolar or non-equimolar) will yield a high configurational formation entropy.11 HEMs have been reported to have some unique changes over traditional polymetallic compounds, such as high entropy effect,12 sluggish diffusion,13 severe lattice distortion14 and the so-called cocktail effect,15 which all lead to excellent performances, such as high hardness,16 strong corrosion resistance17 and high catalytic activity.18 The high entropy effect describes multiple principal elements producing a single entropy-stable phase, which may lead to the formation of high performance materials with unexpected/rare phases.12 The sluggish diffusion effect presents that the sluggish diffusion rate makes the HEMs less prone to grain coarsening and recrystallization at high temperature, so the HEMs have good thermal stability.13 In addition, the sluggish diffusion effect also makes it easy for HEMs to obtain supersaturated solid solutions, which is conducive to the acquisition of nanoscale precipitates. The serious lattice distortion effect is caused by the inconsistence of the atomic radius of each element in HEMs and its random distribution property, which affects the active sites of each unit, thermodynamic stability and microstructure of the synthesized HEMs crystal.14 The “cocktail” effect is a phrase first used by Prof. S. Ranganathan. The original intention was “a pleasant, pleasant mixture”. Now, it means a collaborative concoction where the end result is unpredictable and greater than the sum of its parts.19 Unlike other core effects, the cocktail effect is not hypothetical and does not need to be proven. Cocktail effect refers to special material properties, often resulting from unexpected synergies. It is important to note that these effects are not limited to high entropy metal alloys (HEAs),20 but also apply to other HEMs, such as high entropy metal sulfides (HESs),18 high entropy metal nitrides (HENs),12 high entropy metal phosphides (HEPs),21 and high entropy metal oxides (HEOs).1 It has been widely discussed in many recent studies.
In recent years, the synthesis and application of HEAs have been reviewed, but the entropy stabilized systems and structures of high entropy metal compounds are rarely studied. Just as the properties of traditional catalysts are closely related to composition and structure, elucidation of the structure–property relationships of HEMs, especially among different components and structures, is crucial for the use of entropy-enhanced structure–activity relationships for catalysis.22 The rapid development of HEMs also requires a certain degree of generalization and comparison to reveal the correlation between catalyst structures and components. Here, we review the recent progress of HEMs in the field of electrochemical catalysis. This review mainly designs the following aspects: (1) we first introduce the evolution process from traditional HEAs system to entropy-stable HEMs (e.g., HEPs, HEOs, HENs, HESs, etc.) and the corresponding preparation methods from a basic point of view. It is then summarized that a wide range of entropy-stabilized multicomponent systems with tailored components and structures can be obtained using traditional and advanced synthesis methods. (2) Advanced characterization techniques provide detailed information on the surface, electronic structure, lattice, and composition of HEMs, which are important for understanding the related catalytic behaviors. (3) Then, case studies of HEAs and high-entropy compounds are carried out, highlighting the links between structure, component, and electronic properties and the catalytic properties. (4) Finally, we discuss the upcoming opportunities and challenges for HEMs. We hope that the insights provided here will contribute to the future design and development of HEMs with high performance, diversity of structure or components.
In order to achieve this goal, many researchers have proposed different methods to prepare HEMs with single-phase structure. HEMs were first reported by Yeh et al. in 2004, this work is an extraordinary realization of multiple elements (CuCoNiCrAlxFe) co-existing in a single phase by an arc melting method (Fig. 1a).3 Arc melting is a method of electrothermal metallurgy in which electric energy is used to produce an arc between electrodes or between electrodes and materials to be melted.28 Subsequently, Chang et al. followed and reported a composition-adjustable six-element Fe16.7Cr16.7Mn16.7Ni16.7Co16.7M16.7 (M = Nb, Ge, Cu, Ti and V) single-phase alloy materials by casting and melt spinning, in which the six elements have an equal molar ratio. The basic principle of this method is based on heating to melt the raw material into a certain viscosity melt, and finally form a homogeneous solid solution material.4 These two works are recognized as prototypes of HEMs, and HEMs gradually stepped into the materials field.
Fig. 1 Development and evolution of high-entropy materials with varying morphology and adjustable composition through different synthesis strategies. (a) Bulk high entropy alloys (CuCoNiCrAlxFe). Reprinted with permission.3 Copyright 2004 Wiley-VCH. (b) A nanoparticle with adjustable composition and layered distribution of elements was synthesized (without uniformly dispersive elements in the end). Reprinted with permission.30 Copyright 2016 AAAS. (c) Multicomponent NPs (PtPdCoNiFeCuAuSn). Reprinted with permission.31 Copyright 2018 AAAS. (d) High-entropy metal phosphide (NiCoFeMnCrP). Reprinted with permission.32 Copyright 2021, The Royal Society of Chemistry. (e) HEAs with 15 elements by using carbon thermal shock technology and fast moving bed pyrolysis technique. Reprinted with permission.33 Copyright 2021, Elsevier Ltd. (f) HEOs nanosheets ((FeCrCoNiCu)3O4). Reprinted with permission.34 Copyright 2021, Wiley-VCH. (g) Ultra-thin two-dimensional HEA subnanoribbons (SNRs) composed of up to eight metal elements (PtPdIrRuAg). Reprinted with permission.35 Copyright 2022, American Chemical Society. (h) High-entropy Prussian blue materials. Reprinted with permission.36 Copyright 2022, Wiley-VCH. (i) HEOs (CrMnFeCoNiO). Reprinted with permission.37 Copyright 2023, The Royal Society of Chemistry. |
Soon afterwards a nanoparticle with adjustable composition and layered distribution of elements (Au, Ag, Cu, Ni and Co) was synthesized by a novel technique (scanning-probe block copolymer lithography) in 2016 (without uniformly elemental dispersion in the end). The basic principle of the method is that an atoliter-scale volumes of polymers with a metal ion precursor to the desired location on the surface can form as a nanoreactor to convert the precursor into a single site-isolated nanoparticles (NPs) after heat treatment. This work enables the controlled preparation of five different metal components in individual nanoparticle. The researchers extend the element composition to noble and transition metals (Fig. 1b).29 Then Hu et al.30 synthesized a wide range of multicomponent NPs (PtPdCoNiFeCuAuSn) with a desired chemistry (composition), size, and phase (solid solution, phase-separated) by controlling the carbothermal shock (CTS) parameters (substrate, temperature, shock duration, and heating/cooling rate). In this method, NPs can be generated by simply loading a metal precursor onto a carbon substrate and running a short current through the sample to raise the temperature instantaneously (Fig. 1c). In 2021, HEMs are like bamboo shoots after a spring rain, more and more researchers are committed to the development and research of HEMs. Lai et al. prepared a gel containing five kinds of metal species (Fe, Co, Ni, Cr and Mn) and phosphorous species by sol–gel method, and successfully realized the preparation of HEPs after calcining the obtained gel precursor at high temperature (Fig. 1d).31 Hu et al. made a breakthrough in the preparation of HEAs with 15 elements by using carbon thermal shock technology and fast moving bed pyrolysis technique, which showed a solid solution structure with local strain and lattice distortion caused by extreme mixing (Fig. 1e).32
With the development of HEMs, researchers are no longer satisfied with the component regulation of HEMs, and more and more people pay attention to the morphological and structural regulation of HEMs. Wang et al. reported a low-temperature plasma strategy towards the synthesis of HEOs nanosheets with rich oxygen vacancies. Compared with the traditional high-temperature calcination/reduction method, the low-temperature plasma has the advantages of operation at room temperature, non-equilibrium property and low power, which can solve the problems of grain aggregation, sublimation and structure collapse in the traditional preparation processes, and realize the unconventional preparation of materials (Fig. 1f).33 Guo et al. developed a new cryogenically general synthesis method (ion exchange method) to prepare ultra-thin HEA subnanoribbons (SNRs) composed of up to eight metal elements with a layer thickness of only 0.8 nm, achieving the thinnest HEA metal material in the world, using Ag nanowires (NWs) as a template (Fig. 1g).34 Du et al. expanded the family of HEMs and successfully prepared high-entropy Prussian blue materials with cubic morphology by simple coprecipitation method (Fig. 1h).35 Recently, our research group proposed a universal precursor oxidation method to simultaneously achieve the synthesis and structure regulation of HEOs.36 Different metal sources are uniformly integrated into amorphous carbon spheres through a hydrothermal process. The resulted carbon spherical precursor are transformed to crystalline HEMOs after an oxidation process and by controlling ion diffusion and oxidation rates, HEMOs with different structures including solid, core–shell and hollow spheres can be controllably achieved.
Fig. 2 Advanced characterization techniques for high-entropy materials: (a) schematic summarizing the diffraction, microscopy, and spectroscopy techniques for the characterization of HEMs. (b) FT-EXAFS spectra of CoZnCuNiFeZrCeOx. Reprinted with permission.53 Copyright 2018, American Chemical Society. (c) HAADF-STEM, ABF and atomic EDS mapping of La(Cr0.2Mn0.2Fe0.2Co0.2Ni0.2)O3. Reprinted with permission.54 Copyright 2022 Springer Nature. (d) AC-HAADF-STEM image of Al0.3CoCrFeNi. Reprinted with permission.55 Copyright 2018, Elsevier Ltd. (e) Atomic electron tomography. Reprinted with permission.56 Copyright 2019, Springer Nature. (f) In situ synchrotron X-ray nano-tomography. Reprinted with permission.57 Copyright 2021, Springer Nature. |
Powder X-ray diffraction (XRD) can help determine the basic phase structure to make sure whether the material is homogeneous.38 Electron-coupled plasma atomic emission spectrometry (ICP-AES) can accurately determine the molar ratio of each metal element in HEMs,39 and X-ray photoelectron spectroscopy (XPS) can help determine the valence states of basic elements.40 XPS not only provides information about molecular structure and valence states for chemical research, but also provides information about elemental composition and content, chemical state, molecular structure and chemical bond of various compounds. But these characterization techniques may lack the resolution needed to analyze the more elemental mixing. Synchrotron X-ray technology has been widely used in materials research, mainly because the technology can provide shorter wavelengths, which can better characterize the atomic arrangement, bonding coordination and electronic properties of HEMs.41 For example, synchrotron XRD has high resolution and diffraction intensity and is suitable for studying long range and/or short range ordered crystal and amorphous materials.42 Therefore, synchrotron XRD can more accurately detect the overall phase structure and possible immiscible phase and impurities in HEMs. X-ray intensity attenuates after passing through the sample, and the degree of attenuation is closely related to the structure and composition of the sample. This study of the relationship between transmission intensity and incident X-ray intensity is called X-ray absorption spectroscopy (XAS).43 Because its transmitted light intensity is related to atomic number and atomic mass, for solid (crystal or amorphous), liquid, gas and other types of samples it can be used for qualitative and quantitative analysis of relevant test elements. Thus, XAS can be used to study the atomic and/or local coordination environment of each element, which is critical for understanding multi-element mixing and possible short-range or local ordering in HEMs.44
So far, the detection techniques of material structure are generally based on the diffraction phenomenon of crystalline ordered structures, and XAFS (X-Ray absorption fine structure spectrum) is an exception.45 XAFS includes both XANES (X-ray absorption near edge structure)46 and EXAFS (extended X-ray absorption fine structure)47 technologies. In the X-ray absorption spectrum, the low-energy spectrum above the threshold within 60 eV shows strong absorption characteristics, which is called XANES.48 It is caused by the multiple scattering of excited photoelectrons by surrounding atoms. It not only reflects the geometric configuration of atoms in the surroundings of absorbing atoms, but also reflects the structure of electron states in the low energy near the Fermi level, so it becomes a useful tool for studying HEMs. As a powerful tool to study and characterize catalysts, XANES can determine valence states, characterize D-band properties, measure coordination charges, and provide structural information including orbital hybridization, coordination number and symmetry.49 With the development of synchrotron radiation source, the application of XANES in the study of HEMs has increased significantly. EXAFS is the oscillation of the X-ray absorption coefficient of the element in the range of 30–1000 eV on the high-energy side of the absorption edge.50 The production of EXAFS is related to the scattering of absorbing atoms and other atoms around them, that is, they are all structure-dependent. Therefore, the nearest neighbor structure around the absorption atoms can be studied by EXAFS, and the parameters such as atomic spacing, coordination number and mean azimuth shift can be obtained.51 The main feature of EXAFS method is that it can measure different kinds of atoms respectively, give the nearest neighbor structure of the specified element, and distinguish the types of the nearest neighbor atom. It is also possible to use strong X-ray sources to study the neighboring structures of atoms in very small quantities, and to study both ordered and disordered matter. In this way, EXAFS can be used to solve structural problems that are difficult or impossible to solve with other methods.52 As shown in Fig. 2b, Liu et al. proved that there are certain differences among the elements Co, Zn, Cu, Ni, Fe, Zr, and Ce in HEMs through FT-EXAFS spectra and EXAFS.53 There are obvious differences in the relative strength, coordination number and bond distance of each metal element in the FT-EXAFS curves, which reveal the different local structure and chemical environment of each element.
Advanced electron microscopy technology is needed to better understand the particle size, morphology and distribution of each element of HEMs. Electron microscopy mainly includes scanning electron microscopy (SEM),58 transmission electron microscopy (TEM)59 and scanning transmission electron microscopy (STEM),60 which rely on the interaction between electrons and samples and are widely used to obtain local information such as the morphology and size of materials. SEM has the features of large depth of field, high resolution, intuitive imaging, strong stereo sense, wide magnification range, and the sample to be tested can rotate and tilt in three-dimensional space. In addition, it has the advantages of rich sample types, almost no damage or contamination of the original sample, and the morphology, structure, composition and crystallographic information can be obtained at the same time On the other hand, STEM has a broader function. STEM enables the characterization and analysis of the microstructure and fine chemical components of materials at the nano and atomic scale.61 In recent years, with the introduction of spherical correction, the spatial resolution of STEM has reached the level of sub-angstrom, and the imaging observation of a single atomic column can be realized. As show Fig. 2c, Suet al. displays the HAADF image and EDS maps of La(CrMnFeCoNi0.2)O3, respectively, confirming its chemical compositions. EDS maps show that La is uniformly distributed on the A-site, and the five transition-metal cations, namely Fe, Mn, Cr, Ni, and Co, are in the B-site. Oxygen is observed in the ABF image, distributed between two neighboring B-site atoms. From the EDS maps the intensity variations of the five B-site TM cations can be clearly observed.53 Xu et al. clearly demonstrated the dissociated (a/2) 〈110〉 dislocation taken along the [110] direction through HAADF-STEM characterization (Fig. 2d).54 Annular dark field STEM (ADF-STEM) allows atomic resolution visualization of HEMs that explicitly determine the positions of different atoms.62 Elemental diagrams of STEM combined with energy dispersive X-ray spectroscopy (EDS)63 or electron energy loss spectroscopy (EELS)64 can specify the local chemical composition, which is important for evaluating the structural uniformity of HEMs. STEM-EDS elemental maps are more commonly applied to HEMs because of their high sensitivity to metallic elements with higher atomic numbers. EELS are able to identify the oxidation state of the target element and more sensitive detect light elements such as C, N and O. TEM is usually more focused on smaller areas with higher resolution.
In addition to the characterization techniques mentioned above, various simulation methods and calculation methods have also been applied to study the structure, composition and active site of HEMs.65 In order to better understand the structure and atom-related information of HEMs, researchers are trying to find more advanced representations to explore the deeper structural information of HEMs. Atomic electron tomography (AET) is a powerful method for determining the three-dimensional (3D) atomic structure of materials without assuming the degree of crystallization, and has been applied to the study of dislocation, stratification, grain boundaries, atomic displacement, strain tensors, chemical order/disorder, and point defects in unprecedented details.66 Miao et al.56 reported a four-dimension (including time) study of early nucleation using atomic electron tomography (AET). Using iron base alloy NPs as a model system, the researchers found that the early nuclei were formed irregularly. Each core was composed of one to several atoms with maximum order parameter, and the order parameter varied gradiently from the core to the edge of nucleation. The structural and dynamical changes of early nucleation during growth, decomposition and fusion were also captured, and it was found that these processes were regulated by the distribution and gradient changes of order parameters (Fig. 2e). This technique provides a new angle for studying the fundamental issues of materials science. The real-time change of material structure can help us to understand more clearly the internal structure formation mechanism of the material itself. Ronne et al. reported a novel characterization technique (in situ synchrotron X-ray nano-tomography) for the real-time detection of unique physicochemical properties and unique morphological evolution of nanomaterials (Fig. 2f).57
In addition to experimental characterizations, various computational methods have been applied to predict the synthesis of HEMs and to interpret the catalytic behavior of HEMs. Density functional theory (DFT) calculations can evaluate atomic configuration, electron distribution and energy parameters of HEMs.67 The birth of artificial intelligence has a great impact on the field of material synthesis. The derived machine learning technique can achieve high throughput screening of possible structures and compositions in HEMs.8 The advent of this technology has greatly accelerated the process of material discovery and design. In addition, based on computer simulation techniques, researchers used molecular dynamics and Monte Carlo methods to achieve controllable prediction of the composability and stability of HEMs.68 With the innovation of artificial intelligence and computer technology, these computational tools can not only produce results that complement experimental data, but also guide the progress of experiments.
Fig. 3 Examples of HEMs in ORR: (a) Convex cube-shaped Pt34Fe5Ni20Cu31Mo9Ru HEA catalysts: high angle annular dark field TEM image and the corresponding elemental mapping of Pt34Fe5Ni20Cu31Mo9Ru and electrocatalytic performance of samples (polarization curves). Reprinted with permission.80 Copyright 2022, Wiley-VCH. (b) PdCuPtNiRu core@shell NPs: atomistic simulations of the phase stability of the quinary HEA NPs, electrocatalytic performance of samples (polarization curves). Reprinted with permission.81 Copyright 2022, American Chemical Society. (c) Fourteen-component high-entropy alloy@oxide electrocatalyst: characterization (SEM, TEM, HAADF-STEM and STEM-EDS mapping) of the HEA cluster@HEO and electrocatalytic performance of samples. Reprinted with permission.25 Copyright 2022, The Royal Society of Chemistry. (d) HEAs spatial heterostructure electrocatalyst: structural characterizations (HAADF STEM image and EDS mapping images of HEA@Pt) and electrocatalytic performance for ORR. Reprinted with permission.82 Copyright 2023, Wiley-VCH. |
Synthesis of heterogeneous catalysts is one of the important strategies to improve catalytic performance. Bueno et al.81 reported the synthesis of quinary higher order HEAs (PdCuPtNiM, M = Co, Ir, Rh, Fe, Ru and Rh) through thermal conversion of core@shell NPs. Core@shell HEA NPs were prepared by the seed-mediated co-reduction. And then, the NPs were dispersed on carbon support and annealed to promote the mixing and formation of single-phase PdCuPtNiCo NPs. For NPs containing Ir and Ru, intra-particle heterogeneity, i.e., subdomains within a single NPs with different metal distributions, was observed. The resulted core@shell HEA NPs show better activity and durability than commercial Pt (Fig. 3b). In this work, the electron controllable modulation and the adsorption energy optimization of the active site for intermediates of HEA materials were realized based on the heterostructural regulation of HEA.
In order to further adjust catalytic performance and versatility, the design and manufacture of multi-component high entropy nanocomposites such as HEA@HEO should be very promising. Jin et al.25 designed a two-step alloy-dealloying strategy to synthesize ultra-small HEA nanoclusters (∼2 nm) loaded on nanoporous HEO nanowire, and realized the composition of HEA and HEO that could be individually controllable adjusted. The combined experimental results and first-principles DFT calculations clearly show that better oxygen evolution (OER) performance can be obtained by optimizing the composition of HEO carriers, and that, compared with pure Pt clusters, due to the modified optimized surface electronic structure, the seven-component HEA nanoclusters show more excellent catalytic activity for ORR (Fig. 3c). However, we believe that another unique advantage of HEAs is the adjustable proportion distribution of each element, which may greatly increase the catalytic activity of HEAs. Recently, Zhang et al.82 reported an effective strategy to accelerate the ORR/OER dynamics of Li–O2 batteries by constructing a unique, well-designed HEAs spatial heterogeneous electrocatalyst (HEA@Pt) as a cathode. The core–satellite structure promotes the rapid transfer of interfacial electrons and exposes active heterogeneous interfaces for catalytic reactions, thus increasing the intrinsic catalytic activity of ORR (Fig. 3d).
Fig. 4 Examples of HEMs in OER: (a) HEP NiCoFeMnCrP NPs: TEM images, corresponding element mappings and overpotentials for OER of the samples. Reprinted with permission.31 Copyright 2021, The Royal Society of Chemistry. (b) STEM-HAADF image with corresponding EDX mappings for Fe (red), Ni (blue), Co (green), Cr (yellow), Mn (cyan), and V (magenta) of FeNiCoCrMnV HEO catalysts. Reprinted with permission.90 Copyright 2022, Wiley-VCH. (c) HAADF-STEM image of a (CrMnFeCoNi)Sx nanoparticle and the corresponding EDS elemental mappings. Reprinted with permission.91 Copyright 2021, Wiley-VCH. (d) Schematic illustration of the synthetic procedures for nanoporous NiFeCoMnAl oxide grown on carbon paper and corresponding EDS elemental mapping of Ni, Fe, Co, Mn, Al, O for etched NiFeCoMnAl. Reprinted with permission.92 Copyright 2022, Elsevier Ltd. (e) TEM images and the corresponding element EDS mappings of the CrMnFeCoNiO. Reprinted with permission.36 Copyright 2023, The Royal Society of Chemistry. |
Similarly, high entropy sulfides and high entropy oxides have also been reported for OER, both exhibiting excellent catalytic properties (Fig. 4b and c). Abdelhafiz et al. reported in situ synthesis of non-noble metal HEO catalysts on carbon fiber by rapid Joule heating and quenching.90 Compared with the noble metal IrO2, the different compositions of three- to six-membered (FeNiCoCrMnV) HEO NPs are more active catalysts for oxygen evolution. Alloying elements Cr, Mn and V affect OER activity by promoting different oxidation states of the catalytic activity TM (Fe, Ni and Co). The introduction of more metal elements resulted in the serious distortion of crystal structure, which may be the reason for the excellent catalytic performance of HEMs. Cui et al.91 first reported the synthesis of high entropy metal sulfide ((CrMnFeCoNi)Sx) solid solution NPs through a pulse thermal decomposition method to overcome the immiscibility of multiple metallic constituents in 2021. The obtained (CrMnFeCoNi)Sx NPs were used as electrocatalysts for OER in 1 M KOH solution, and showed a very low overpotential of 295 mV and a good operating stability for 10 hours at 100 mA cm−2 current density.
Compared with HEAs, the shape control of HEMs is more difficult to achieve, mainly because the compound phase of different metals is more complex, and it is difficult to achieve consistent kinetic diffusion among each element in the preparation process. Han et al.92 introduced the concept of high entropy to the self-supporting HEO catalyst, which was prepared using a simple and scalable electrodeposition method. In this work, binary NiFe was selected as the initial component of the highly active OER catalyst, and the effect of the composition cutting on the performance of OER was studied by doping Co, Mn and Al. All elements are evenly distributed in the amorphous structure. It was found that the doping of Co and high Mn could improve the conductivity of the catalyst. Doped Al as a sacrificial template is dealloyed in alkaline solution to form nanopore structure, resulting in an increase in electrochemical active surface area. This work is more in line with the previous review article: amorphous materials have unique short-range atomic ordered and long-range disordered structures, which have attracted more and more attention in electrocatalysis,69 especially in water splitting catalysis. This work provides a compelling demonstration of HEMs as effective OER catalysts, a comprehensive understanding of multi-element synergies, and potential guidance for self-supporting HEMs electrocatalyst design (Fig. 4d). Obviously, structural adjustment is an effective strategy to improve the electrochemical performances of HEMs. However, none of the reported non-precious metal HEMs has achieved the morphology control of nanomaterials, which further indicates that the morphology control of HEMs is a very important scientific direction. Lai et al.36 achieved the controllable preparation of HEOs with different structures by controlling ionic diffusion and oxidation rate. The work was carried out with a simple hydrothermal technique through which five kinds of metal species are uniformly integrated into amorphous carbon spheres that are converted to HEOs by calcination. As shown in Fig. 4e, this work successfully achieved structural regulation from a solid sphere to a core–shell sphere to a hollow sphere. Importantly, the obtained HEOs have a single-crystalline structure, all the elements of HEOs with different structures are evenly distributed and the five metal components can be exchanged at will. Core–shell CrMnFeCoNiO shows the best performance due to its component and structural advantages. This work expands the synthesis of HEMs and provides a rational approach for structural regulation, which makes it have great potential as a high-performance energy storage and conversion material.
Fig. 5 Examples of HEMs in HER: (a) TEM image, EDX mappings and electrocatalytic performance of np-UHEAs (Al87Ag1Au1Co1Cu1Fe1Ir1Mo1Ni1Pd1Pt1Rh1Ru1Ti1). Reprinted with permission.95 Copyright 2021, The Royal Society of Chemistry. (b) Fabrication schematic illustration, TEM image and corresponding EDX mappings and electrocatalytic performance of the FeCoNiCuPd film. Reprinted with permission.96 Copyright 2022, Elsevier Ltd. (c) Electron microscopic characterization of high-entropy alloy PdMoGaInNi nanosheets. Reprinted with permission.97 Copyright 2022, American Chemical Society. (d) Schematic illustration of selective Zn dealloying through vapor dealloying process and EDX mappings of ZnNiCoIrMn). Reprinted with permission.98 Copyright 2023, Wiley-VCH; (e) Schematic illustration of PtPdRhRuCu mesoporous nanospheres and electrocatalytic performance of samples (polarization curves). Reprinted with permission.99 Copyright 2023, Springer Nature. |
On the other hand, HER applications always require some supporting substrate, and the traditional adhesive fixing method will greatly reduce the performance of the catalyst. Therefore, it is very necessary to fix HEMs on the supporting substrate efficiently and easily. Wang et al.96 deposited FeCoNiCuPd with single face-centered cubic structure on carbon fiber cloth (CFC) by magnetron sputtering technology. The FeCoNiCuPd/CFC module exhibits a remarkable electrocatalytic performance with a low overpotential of 29 mV for HER at 10 mA cm−2, superior to commercially available Pt/C. In addition, the novel electrocatalyst also shows impressive HER stability under high current density conditions. This work provides a feasible method for producing high performance HEMs catalysts for water decomposition (Fig. 5b).
Similarly, the morphology regulation of HEMs is also very challenging in HER catalysts, because the catalysts need to have certain acid and alkaline resistance, and their working environment may be more harsh, which may lead to the adverse effect of structural regulation on the catalytic performance. As shown in Fig. 5c, Fuet al.97 reported the discovery of PdMoGaInNi, a Pt-free group with optimal hydrogen binding energy values, by computer aided screening. As an exploratory example of a two-dimensional HEA for HER, PdMoGaInNi HEA nanosheets have been synthesized to achieve a predicted Pt-free combination with an optimal hydrogen binding energy. The HEA nanosheets were prepared by a traditional oil bath reduction process. PdMoGaInNi HEA nanosheets show high HER activity, with a low overpotential of 13 mV at 10 mA cm−2, superior to commercial Pd/C and Pt/C catalysts. Given the high entropy, lattice distortion and slow diffusion effects of HEA, PdMoGaInNi shows good long-term durability of at least 200 hours in proton exchange membrane water electrolytic cells.
In addition, how to tailor the electronic structure in HEA is also a big challenge. Kwon et al.98 designed Ir-based electrocatalysts using a ZnNiCoIrX HEA platform with two elements (X: Fe and Mn). They achieved easy dealloying through a vacuum system in which Zn was used as a sacrificial element to construct a nanoporous HEA structure with high crystallinity. This work found that the incorporation of Mn into HEA would adjust the electronic structure of Ir site, causing the d-band center to move away from the Fermi level. The downward movement of the d-band center weakens the adsorption energy with the reaction intermediates, which is conducive to catalyzing the reaction. When in the case of low Ir content of the catalyst, HER overpotential is only 50 mV at −50 mA cm−2. ZnNiCoIrMn shows almost constant voltage for HER for 100 h and high stability number of 3.4 × 105 nhydrogen nIr−1, demonstrating exceptional durability of HEA platform. The results provide one of the means for the practical preparation of low-cost and efficient nanoporous HEMs electrocatalysts.
At present, more and more researchers believe that it is necessary to design HEMs with specific morphology and composition of nanostructures in order to increase the richness of nanostructures and explore the structure-performance relationship. Recently, Kang et al. designed a one-pot wet-chemical reduction approach to synthesize core–shell motif PtPdRhRuCu mesoporous nanospheres (PtPdRhRuCu MMNs) using a diblock copolymer as the soft template (Fig. 5e).99 Due to the unique morphology and structure, the material with adjustable composition has exposed porous structure and is rich in high entropy alloy potential, and thus exhibits robust electrocatalytic hydrogen evolution reaction (HER) activities and low overpotentials of 10, 13, and 28 mV at a current density of 10 mA cm−2 in alkaline (1.0 M KOH), acidic (0.5 M H2SO4), and neutral (1.0 M phosphate buffer solution) electrolytes, respectively. This work closely links the concept of HEMs and mesoporous, and further expands the application range of HEMs.
Compared to the above electrocatalytic studies (e.g. HER, OER and ORR), the design of high entropy ECR catalysts is more difficult, the challenge is that more metal elements may cause the product selectivity disorder. Therefore, the design of a suitable HEMs catalyst requires extremely precise coordination between the components, which is difficult to achieve at the current atomic level of chemical control. Pedersen et al.104 predicted CO and hydrogen (H) adsorption energies at all surface sites on disordered CoCuGaNiZn and AgAuCuPdPt HEAs (111) surfaces by combining DFT with supervised machine learning (Fig. 6a). Through their simulation and calculation, they found that necessary (but by no means sufficient) criteria were used for weak H adsorption and strong CO adsorption. This work presented a framework for unbiased discovery of new catalyst candidates for CO2RR and CORR, using two disordered HEAs CoCuGaNiZn and AgAuCuPdPt as starting points. Knowing only the catalytic properties of Cu, the model can suggest, for example, that GaNi as a locally optimal catalyst candidate for CO2RR/CORR is known experimentally to exhibit a degree of selectivity for highly reduced carbon products. This demonstrates the model's ability to predict effective catalyst candidates without prior knowledge of catalyst performance, and provides a method for probabilistically optimizing disordered alloy composition for optimal catalytic performance.
Fig. 6 Examples of HEMs in CO2RR: (a) schematic diagram of catalytic reaction of HEA (AgAuCuPdPt) and selectivity–activity plots (plot of the CO2RR/CORR selectivity and CORR activity space achievable of HEA (AgAuCuPdPt). Reprinted with permission.104 Copyright 2020, American Chemical Society. (b) The active surface of HEAs (Fe0.2Co0.2Ni0.2Cu0.2Mo0.2 (111)), structures of the designed three active sites and adsorption configuration of CHO* on Ni–Mo and Ni–Cu sites of HEAs with the charge density difference and simulated reaction of CO2RR on HEAs. Reprinted with permission.105 Copyright 2022, American Chemical Society. (c) Schematic of the catalysis reaction, XRD pattern of HEA alloy NPs (AuAgPtPdCu) and mapping of an atom probe microscope. Reprinted with permission.106 Copyright 2022, American Chemical Society. (d) Schematic illustration of the preparation and STEM-EDS elemental mappings of PdCuAuAgBiIn HEAAs. Reprinted with permission.107 Copyright 2022, Wiley-VCH. |
In order to further improve the ECR catalytic performance of HEMs, Chen et al.105 proposed that circumventing the scale relationship is a breakthrough in catalytic activity. They designed FeCoNiCuMo HEA system with high catalytic activity based on DFT calculations. The Vienna ab initio simulation package (VASP) was applied to perform spin-polarized DFT calculations. The core electrons were described by the projectoraugmented wave pseudopotential and the generalized gradient approximation (GGA) with the Perdew–Burke–Ernzerhof functional (PBE) was considered for all DFT calculations. The high entropy alloy structures were built by a neural evolution structure (NES) generation methodology. Based on 1280 adsorption sites, a machine learning model was established to predict the adsorption energies of COOH*, CO* and CHO*. The rotation of COOH*, CO* and CHO* on the surface of the designed HEA avoids the scaling relationship of the adsorption energies of COOH*, CO* and CHO*, and CO2RR has excellent catalytic activity with a limit potential of 0.29–0.51 V (Fig. 6b). This work not only accelerates the development of HEA catalyst, but also provides an effective strategy to avoid scaling relationship.
With a theoretical basis, Nellaiappan et al.106 used a nanocrystalline HEA (AuAgPtPdCu) to convert CO2 into gaseous hydrocarbons. They prepared HEAs by forming a solid solution at high temperature. At low application potential (−0.3 V vs. reversible hydrogen electrode), the faradaic efficiency for gaseous products is about 100% (Fig. 6c). Li et al.107 reported the preparation of a series of high-entropy alloy aerogels (HEAAs) by freeze–thaw method as highly active and durable electrocatalysts for CO2RR (Fig. 6d). PdCuAuAgBiIn HEAAs can achieve almost 100% faradaic efficiency (FE) for C1 products between −0.7 and −1.1 V, and 98.1% FE for formic acid at −1.1 V. It is better than PdCuAuAgBiIn HEAs and Pd metallic aerogel (MAs) reported. As shown in Fig. 6d, compared with the reported HEA, HEAAs have more pore structure, which means it has more effective active sites, adsorption capacity of reactants and desorption capacity of products. This work not only provides a simple synthesis strategy for the preparation of HEAAs, but also opens the way for the development of efficient catalysts.
Li et al.110 reported a dealloying process for a nanoporous multi-component anode and cathode catalyst for high performance ethanol fuel cells. As shown in Fig. 7a, on the anode side, the porous AlPdNiCuMo alloy showed electrochemical activity of 88.53 m2 gPd−1 and mass activity of 2.67 A mgPd−1 during the ethanol oxidation reaction. At the cathode side, dealloying spinel (AlMnCo)3O4 nanocrystalline sheets without noble metals showed comparable catalytic performance to standard Pt/C in oxygen reduction reaction, and showed tolerance to high concentration of ethanol. Flexible solid ethanol fuel cells, equipped with such anode and cathode catalysts, provide an ultra-high energy density of 13.63 mW h cm−2 with just 3 mL ethanol, which is outstanding compared to other similar solid energy devices.
Fig. 7 Examples of HEMs in alcohol oxidation: (a) schematic and catalytic performance characterization of flexible solid-state AlPdNiCuMo. Reprinted with permission.110 Copyright 2020, Wiley-VCH. (b) Schematic illustration and catalytic performance characterization of PdPtCuAgAu HEA NWs. Reprinted with permission.111 Copyright 2022, Elsevier Ltd. (c) TEM image, XRD pattern and catalytic performance of the PtRhBiSnSb HEI nanoplates. Reprinted with permission.112 Copyright 2022, Wiley-VCH. (d) TEM, HRTEM images and elemental mappings of Co0.2Ni0.2Cu0.2Mg0.2Zn0.2O. Reprinted with permission.113 Copyright 2020, Wiley-VCH. |
Similarly, this catalytic reaction is focused on practical applications, so HEMs catalysts need to be supported on certain substrates or self-supported. Fan et al.111 reported a simple method to prepare high entropy PdPtCuAgAu nanowire networks using carboxyl functionalized surfactants as soft templates (Fig. 7b). The PdPtCuAgAu alloy electrocatalyst has high mass activity (7.7 A mgPd+Pt−1), good stability/durability, anti-poisoning ability and good electrocatalytic kinetics, which significantly improves the electrocatalytic performance of ethanol oxidation reaction. This method for the synthesis of HEAs will provide a new approach for the rational design of other high entropy nanocatalysts with ideal morphology/structure and function for a wide range of catalytic applications.
On the other hand, the control of catalyst composition needs to be more precise and variable in practical application. The elements in most reported HEMs are basically located in the same group or have similar atomic radius, so it is relatively easy to achieve synthesis. However, it is difficult to synthesize and regulate HEMs with large differences in atomic radius. Chen et al.112 recently reported a one-pot synthesis of hexagonal tightly packed (hcp) PtRhBiSnSb high entropy intermetallic compound (HEI) nanoplates with intrinsically isolated Pt, Rh, Bi, Sn, and Sb atoms to facilitate the electrochemical oxidation of liquid fuels (Fig. 7c). Using the combination of these five metals, the PtRhBiSnSb HEI nanoplates show significant mass activity of 19.529, 15.558 and 7.535 A mgPt+Rh−1 for the electrooxidation of methanol, ethanol and glycerol in alkaline electrolyte, respectively. They found that PtRhBiSnSb HEI achieves record methanol oxidation reaction (MOR) activity in an alkaline environment. This work provides an important research advance for the development of HEMs with fine control of composition and properties, further expanding the membership of the HEMs family. In addition, HEMs also play an important role in catalytic oxidation of organic alcohols. Feng et al.113 prepared a porous layered HEO (Co0.2Ni0.2Cu0.2Mg0.2Zn0.2O) material with a mesoporous structure using an anchoring consolidation process (Fig. 7d). The HEO catalyst has high catalytic activity for solvent-free aerobic oxidation of benzyl alcohol and can achieve 98% conversion within 2 hours, which is the highest conversion rate of benzyl alcohol oxidation to date. By adjusting the catalytic reaction parameters, benzoic acid or benzaldehyde can be selectively optimized as the main products. This study is of great significance for the utilization of HEO materials with unique structure and provides a prospect for the development of multiphase catalysts in industrial catalysis field.
Material | Synthesis method | Catalytic reaction | Catalytic performance | Ref. |
---|---|---|---|---|
Pt34Fe5Ni20Cu31Mo9Ru | One-pot of oil bath | ORR | E 1/2 (V vs. RHE) 0.87 V | 80 |
PdCuPtNiCo | Ion exchange | ORR | E 1/2 (V vs. RHE) 0.86 V | 81 |
PtPdAuAgCuIrRu@(AlNiCoFeCrMoTi)3O4 | Alloying–dealloying | ORR | E 1/2 (V vs. RHE) 0.61 V | 25 |
PtRuFeCoNi@Pt | In situ growth | ORR | E 1/2 (V vs. RHE) 0.85 V | 82 |
NiCoFeMnCrP | Sol–gel | OER | Overpotential 270 mV (10 mA cm−2) | 31 |
(FeNiCoCrMnV) HEO | Rapid Joule heating and quenching | OER | Overpotential 247 mV (10 mA cm−2) | 90 |
(CrMnFeCoNi)Sx | Pulse thermal decomposition | OER | Overpotential 247 mV (10 mA cm−2) | 91 |
NiFeCoMnAl oxide | Electrodeposition | OER | Overpotential 190 mV (10 mA cm−2) | 92 |
np-UHEAs (14 elements) | One-step dealloying | HER | Overpotential 32 mV (10 mA cm−2) | 95 |
FeCoNiCuPd | Magnetron sputtering | HER | Overpotential 29 mV (10 mA cm−2) | 96 |
PdMoGaInNi | Oil bath | HER | Overpotential 13 mV (10 mA cm−2) | 97 |
ZnNiCoIrMn | Calcining method | HER | Overpotential 50 mV (50 mA cm−2) | 98 |
AuAgPtPdCu | Melting method | ECR | E (V vs. RHE) −0.3 V | 106 |
FE(CH4) 49.4% | ||||
PdCuAuAgBiIn | Freeze–thaw method | ECR | E (V vs. RHE) −1.1 V | 107 |
FE(HCOOH) 98.1% | ||||
RuRhPdOsIrPt | Wet chemical synthesis | EOR | E onset (V vs. RHE) 0.28 V (50 mV s−1) | 109 |
Precisely controlled synthesis is currently the most explored aspect of HEMs, and more precise and purposeful design is now required. Considering the immiscibility in HEMs due to element differences and composition complexity, synthesis must continue to rely on temperature, force, pressure, energy field and other non-equilibrium methods to achieve uniform mixing and small particle size. But we do not believe that these conditions are necessarily sufficient and necessary. The successful preparation of HEAs single crystal nanosheets by controlled synthesis at room temperature has been reported.34 This breakthrough also means that the synthesis method of HEMs is not limited to extreme environments. We still need to explore how to balance non-equilibrium synthesis with subtle structural or morphological controls in terms of size, phase, shape and surface decoration, which will require considerable effort and knowledge gained from existing chemical synthesis in various fields.
What is lacking in HEMs research at present is a basic understanding of the controllability of surface, intrinsic defects and element distribution in high entropy NPs, which will have great guiding significance for catalytic performance. Most studies do not involve the separation of surface or interfacial elements, the reconstruction of crystal phase, and the reconstruction of electronic structures, especially the dynamic evolution of their components under catalytic conditions, which is particularly important. To overcome these difficulties, it is necessary to introduce more advanced characterization techniques, such as a new transscale imaging method for AFM and scanning microlens associated microscopy,114 Terahertz scanning tunneling microscope system,115 small-molecule serial femtosecond X-ray crystallography,116in situ liquid transmission electron microscopy117 and so on. More information, such as surface atomic structure evolution, lattice strain, atomic diffusion behavior and electronic structure of each atom, can be obtained through more advanced techniques to provide reliable basis for theoretical simulation/theoretical calculation and understanding of the formation mechanism.
HEMs show great promises for high performance catalysis, especially for complex reactions that require different combinations of active sites. However, how to properly design HEMs to best suit these response schemes remains a challenging scientific issue. In addition, it is not clear how to identify the active site and understand the source of performance. Most of the current research on HEMs is based on traditional catalysts, but the active sites of HEMs do not match them, and its four effects may lead to unimaginable new active sites. Among them, high entropy effect and cocktail effect bring the most obvious unpredictability. This is mainly related to the severe lattice distortion of the crystal structure of HEMs and the unpredictable cocktail effect, the existence of which may lead to the creation of unpredictable new active sites in HEMs. At this point, there is no theoretical research to achieve accurate performance prediction of each element combination of HEMs. We believe that a more cohesive effort is needed to link the chemistry, physics, and materials communities to introduce a new frontier in the discovery and design of highly efficient catalytic materials.
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