Sharanya
Kannan Anbarasu‡
a,
Raja Arumugam
Senthil‡
a,
Sieon
Jung
a,
Anuj
Kumar
b,
Mohd
Ubaidullah
c and
Myong Yong
Choi
*ad
aDepartment of Chemistry (BK21 FOUR), Research Institute of Advanced Chemistry, Gyeongsang National University, Jinju 52828, Republic of Korea. E-mail: mychoi@gnu.ac.kr
bNano-Technology Research Laboratory, Department of Chemistry, GLA University, Mathura, Uttar Pradesh 281406, India
cDepartment of Chemistry, College of Science, King Saud University, Riyadh 11451, Saudi Arabia
dCore-Facility Center for Photochemistry & Nanomaterials, Gyeongsang National University, Jinju 52828, Republic of Korea
First published on 9th May 2025
Electrocatalytic overall water splitting (OWS) is a promising technology for sustainable hydrogen (H2) production. However, its practical application is hindered by the sluggish kinetics of the anodic oxygen evolution reaction (OER). To address this challenge, high-entropy oxides have emerged as promising OER electrocatalysts owing to their tunable composition and synergistic effects among constituent elements. In this study, we present the fabrication of a spinel-structured high-entropy Cr(NiFeCoV)2O4 (HE-Cr(NiFeCoV)2O4) catalyst using a rapid continuous-wave CO2 laser thermal-shock method. The resulting HE-Cr(NiFeCoV)2O4 catalyst demonstrated excellent electrochemical OER performance in 1 M KOH electrolyte, achieving a low overpotential of 284 mV at 10 mA cm−2 and maintaining long-term stability over 100 h at 50 mA cm−2. Furthermore, an OWS electrolyzer assembled with HE-Cr(NiFeCoV)2O4 as the anode and Pt/C as the cathode operated at a low cell voltage of 1.57 V at 10 mA cm−2 for efficient H2 production. In situ Raman spectroscopy confirmed the surface formation of active FeOOH species during OER, while density functional theory calculations revealed how the multi-metal synergy within a single lattice modulated the electronic structure, thereby enhancing the OER activity of Cr(NiFeCoV)2O4. This study establishes a cost-effective and energy-efficient pathway for developing advanced multicomponent electrocatalysts for clean energy applications.
Transition metals and their compounds, including oxides, sulfides, phosphides, carbides, and hydroxides, have been extensively studied as potential OER electrocatalysts.11–13 Among these, transition metal oxides-particularly those with rock-salt, perovskite, and spinel crystalline structures-have demonstrated exceptional electrocatalytic performance owing to their strong OH− adsorption and surface-active *OOH intermediate generation capabilities via metal–oxygen (M–O) bonding, which enhances OER kinetics.14,15 Spinel-structured metal oxides particularly stand out owing to their straightforward synthesis, structural and compositional versatility, mixed metal valence states (+2 and +3), excellent catalytic redox properties, and stability in strongly alkaline environments.16,17 Recently, high-entropy oxides (HEOs), comprising five or more equimolar cations alongside oxygen anions, have emerged as a transformative class of electrocatalysts, offering viable alternatives to noble metal catalysts in energy conversion and storage applications.18–20 The incorporation of multiple metal cations in a single HEO structure facilitates extensive electron transfer between metal cations, resulting in strong electron redistribution and abundant active sites for electrochemical reactions.21,22 Additionally, the lattice distortion induced by multiple metal species generates efficient surface-oxygen vacancies, enhancing electron redistribution and creating unsaturated coordination environments in the HEOs.23–25 Remarkably, the high-entropy effect in HEOs, induced by multiple metal components, increases configurational entropy and reduces Gibbs free energy (ΔG↓ = ΔH − TΔS↑), thereby improving catalytic activity, structural stability, and synergistic interactions among constituent metals.26–28 These unique features endow HEO-based OER electrocatalysts with exceptional electrochemical performance and long-term stability, making them promising candidates for advancing OWS efficiency.
Encouraged by the superior advantages of HEO catalysts in OER, we aimed to develop a spinel-structured high-entropy Cr(NiFeCoV)2O4 (denoted as HE-Cr(NiFeCoV)2O4) electrocatalyst. The integration of Cr, Ni, Fe, Co, and V cations within a single oxide matrix is anticipated to enhance electrocatalytic activity for OER. Additionally, the synthesis method plays a decisive role in determining the production cost, purity, and catalytic performance of nanomaterials. Conventional furnace-based heating methods are frequently utilized for the synthesis of metal oxides, including HEO nanomaterials.29,30 However, these conventional approaches often require extended heating durations, substantial energy input, and may generate impurities as byproducts, thereby constraining their practical applicability. To mitigate these challenges, thermal-shock synthesis employing a continuous-wave CO2 laser has been introduced, facilitating rapid, localized heating that allows for precise control over phase formation, crystallinity, and defect engineering.31–33 Furthermore, this innovative technique reduces thermal gradients, prevents undesired phase transitions, and drastically reduces synthesis time and energy consumption. These benefits position thermal-shock synthesis as a versatile and efficient method for the fabrication of advanced nanomaterials, offering a viable alternative to traditional synthesis techniques.
Herein, we successfully synthesized a spinel-structured HE-Cr(NiFeCoV)2O4 catalyst for the first time via a rapid thermal-shock approach using continuous-wave CO2 laser technology and evaluated its OER performance. The HE-Cr(NiFeCoV)2O4 catalyst demonstrated outstanding OER performance, achieving a low overpotential of 284 mV at 10 mA cm−2 and long-term stability over 100 h at 50 mA cm−2 in 1 M KOH electrolyte. Furthermore, when integrated as the anode in an OWS electrolyzer with Pt/C as the cathode, the system required a low cell voltage of only 1.57 V at 10 mA cm−2 for H2 production and maintained long-term operational stability over 100 h at 50 mA cm−2, highlighting its practical applicability. To elucidate the origins of the superior performance of the HE-Cr(NiFeCoV)2O4 catalyst, advanced in situ Raman spectroscopy and theoretical density functional theory (DFT) simulations were employed. In situ Raman spectroscopy revealed the formation of surface-active FeOOH species on HE-Cr(NiFeCoV)2O4 during OER, providing real-time insights into catalyst surface transformations. Concurrently, DFT simulations showed strong electronic modulations within the HE-Cr(NiFeCoV)2O4 structure and lower energy barriers for reaction intermediates, contributing to its exceptional OER performance. Overall, this study integrates advanced synthesis techniques and in-depth structural analyses to pave the way for the development of efficient, cost-effective, and durable multicomponent electrocatalysts for renewable energy applications.
Details on material characterization techniques, electrochemical assessments, in situ Raman spectroscopy, and computational methods are provided in the ESI.†
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Fig. 1 (a) Schematic of the synthesis process, (b–d) HR-TEM images, (e) SAED pattern, and (f) TEM-EDS mapping images of the HE-Cr(NiFeCoV)2O4 catalyst. |
The surface morphologies and elemental compositions of the synthesized HE-Cr(NiFeCoV)2O4 were analyzed using field-emission scanning electron microscopy (FE-SEM), high-resolution transmission electron microscopy (HR-TEM), and energy-dispersive X-ray spectroscopy (EDS). FE-SEM (Fig. S1a and b†) images revealed agglomerated nanoparticles in both CrCo2O4 and HE-Cr(NiFeCoV)2O4 catalysts. SEM-EDS mapping confirmed the uniform distribution of Cr, Ni, Co, Fe, V, and O in the HE-Cr(NiFeCoV)2O4 structure. The SEM-EDS spectra (Fig. S2†) showed the elemental composition of CrCo2O4: 18.93 wt% Cr, 43.48 wt% Co, and 37.59 wt% O. In contrast, HE-Cr(NiFeCoV)2O4 catalyst showed elemental compositions of 19.75 wt% Cr, 12.53 wt% Ni, 11.85 wt% Fe, 12.92 wt% Co, 7.30 wt% V, and 35.65 wt% O, confirming the successful incorporation of multiple metals and its high-entropy nature. HR-TEM images of the HE-Cr(NiFeCoV)2O4 catalyst (Fig. 1b–d) further demonstrated agglomerated nanoparticles with well-defined lattice fringes, showing an interplanar spacing of 0.18 nm corresponding to the (311) crystalline plane of spinel CrCo2O4 structure. The selected-area electron diffraction (SAED) pattern (Fig. 1e) confirmed the polycrystalline nature of HE-Cr(NiFeCoV)2O4, with distinct crystal planes matching the spinel CrCo2O4 framework. Furthermore, TEM-EDS spectra (Fig. S3†) and mapping (Fig. 1f) validated the uniform distribution of Cr, Ni, Fe, Co, V, and O with compositions of 21.45 wt%, 12.75 wt%, 11.33 wt%, 13.04 wt%, 7.06 wt%, and 34.37 wt%, respectively, closely aligning with SEM-EDS results. Based on these compositions, the total mixing entropy (ΔSmix) was calculated using the equation: , where R is the gas constant, Ci represents the mole fraction of the ith element, and n denotes the total number of components. The calculated ΔSmix value for HE-Cr(NiFeCoV)2O4 was 1.65R, further emphasizing its high-entropy characteristics.
To verify the high-entropy formation and phase purity of the HE-Cr(NiFeCoV)2O4 catalyst, X-ray diffraction (XRD) analysis was performed. The XRD patterns (Fig. 2a) of both CrCo2O4 and HE-Cr(NiFeCoV)2O4 catalysts exhibited similar diffraction peaks, consistent with cubic spinel oxide structure (PDF#22-1084).34,35 Notably, HE-Cr(NiFeCoV)2O4 showed peak shifts toward higher 2θ values compared to CrCo2O4, indicating lattice distortion caused by the incorporation of additional Ni, Fe, and V cations into the CrCo2O4 structure. This lattice distortion likely modulates the electronic properties of the HE-Cr(NiFeCoV)2O4 catalyst, enhancing its OER catalytic activity. These findings confirm the successful synthesis of a single-phase HE-Cr(NiFeCoV)2O4 catalyst with multiple metal cations and no additional phases, highlighting its excellent phase purity. Further structural characterization was performed using Raman spectroscopy, which revealed characteristic peaks for the CrCo2O4 catalyst (Fig. 2b) at 188, 459, 539, 592, and 660 cm−1 corresponding to the typical F2g, Eg, F2g, F2g, and A1g vibrational modes of cubic spinel oxides, respectively.17,36 These characteristic peaks shifted to higher wavenumbers in the HE-Cr(NiFeCoV)2O4 catalyst, attributable to modified vibrational modes resulting from enhanced M–O interactions and lattice distortions induced by the integration of multiple metals into a single spinel oxide structure. In addition, Fourier transform infrared spectra (Fig. S4†) revealed distinct vibrational peaks at 487 and 632 cm−1 in CrCo2O4, corresponding to M–O stretching vibrations at octahedral and tetrahedral sites, respectively. These peaks were noticeably reduced in intensity for the HE-Cr(NiFeCoV)2O4 catalyst, likely owing to lattice distortions from Ni, Fe, and V cation incorporation into the CrCo2O4 framework. Brunauer–Emmett–Teller (BET) surface area analysis was performed to assess the influence of multiple metal components on the surface area of the HE-Cr(NiFeCoV)2O4 catalyst (Fig. 2c), exhibiting considerably higher nitrogen adsorption and desorption capacities, resulting in a higher BET surface area of 116.11 m2 g−1 compared to CrCo2O4 (85.37 m2 g−1). This increased surface area provides abundant surface-active sites and enhances surface adsorption of reaction intermediates, contributing to improved catalyst's OER performance.
Advanced X-ray photoelectron spectroscopy (XPS) was employed to analyze the chemical composition and oxidation states of the CrCo2O4 and HE-Cr(NiFeCoV)2O4 catalysts. The core-level XPS plots of the HE-Cr(NiFeCoV)2O4 catalyst are shown in Fig. S5† and 2d–i, while those of the CrCo2O4 catalyst are shown in Fig. S6a–d.† The wide-range XPS plots confirmed the presence of Cr, Ni, Co, Fe, V, and O in HE-Cr(NiFeCoV)2O4 (Fig. S5†), whereas only Cr, Co, and O were detected in CrCo2O4 (Fig. S6a†), verifying the successful incorporation of multiple metal components into the HE-Cr(NiFeCoV)2O4 structure. The Cr 2p XPS plots of both catalysts revealed two doublet peaks at ∼575.8/585.5 and 578.1/587.3 eV (Fig. 2d and S6b†), corresponding to Cr 2p3/2/2p1/2 spins associated with Cr3+ and Cr4+, respectively.37 The Ni 2p XPS plots of HE-Cr(NiFeCoV)2O4 splits into two doublet peaks at ∼854.8/872.4 and 857.6/875.1 eV (Fig. 2e), along with satellite peaks, corresponding to Ni 2p3/2/2p1/2 spins of Ni2+ and Ni3+, respectively.35 Similarly, the Fe 2p XPS plots of HE-Cr(NiFeCoV)2O4 (Fig. 2f) exhibited two doublet peaks at ∼709.9/712.3 and 723.2/725.9 eV along with satellite peaks, ascribed to Fe 2p3/2/2p1/2 spins of Fe2+ and Fe3+, respectively.38 The Co 2p XPS plots of both catalysts (Fig. 2g and S6c†) showed two doublet peaks at ∼780.0/795.6 and 782.6/797.5 eV, with satellite peaks, corresponding to the Co 2p3/2/2p1/2 spins of Co3+ and Co2+, respectively. The V 2p XPS plots of HE-Cr(NiFeCoV)2O4 (Fig. 2h) showed two peaks at 516.2 and 523.6 eV, corresponding to the V 2p3/2 and V 2p1/2 spins of V3+, respectively.39,40 The O 1s XPS plots of both catalysts (Fig. 2i and S6d†) exhibited a peak at ∼529.4 eV, corresponding to the lattice M–O bonds (where M = Cr/Co in CrCo2O4 or M = Cr/Ni/Fe/Co/V in HE-Cr(NiFeCoV)2O4) while additional peaks at 531.2 and 532.3 eV are ascribed to surface-adsorbed O2 and H2O molecules, respectively.36 These results confirmed the presence of Ni, Fe, and Co in mixed +2 and +3 oxidation states, Cr in mixed +3 and +4 oxidation states, and V in the +3 oxidation state in HE-Cr(NiFeCoV)2O4. The incorporation of multiple cations with mixed oxidation states substantially modulates the electronic structure, enhancing the intrinsic electrocatalytic activity of HE-Cr(NiFeCoV)2O4. In addition, ultraviolet photoelectron spectra of the CrCo2O4 and HE-Cr(NiFeCoV)2O4 (Fig. S7a and b†) revealed Ecut-off values of 7.26 and 8.68 eV, respectively, where Ecut-off represents the kinetic energy cutoff of secondary electrons. The work function for HE-Cr(NiFeCoV)2O4 was calculated as 12.54 eV, compared to 13.96 eV for CrCo2O4, reflecting its modulated electronic structure, enhanced electron transport, and improved electrical conductivity.41 Reflection electron energy loss spectra (Fig. S8†) revealed a prominent decrease in elastic peak intensity for HE-Cr(NiFeCoV)2O4 compared to CrCo2O4, highlighting the enhanced surface and electronic properties of the HE-Cr(NiFeCoV)2O4 catalyst—potentially accelerating its electrocatalytic activity for OER.42
Further examination of the electrochemical surface area (ECSA) and double-layer capacitance (Cdl) provided critical insights into the active surface properties of the HE-Cr(NiFeCoV)2O4 catalyst.45 CV measurements at varying scan rates (Fig. S11a–d†) were used to determine the ECSA and Cdl of the catalysts. As shown in Fig. S12 and S13,† HE-Cr(NiFeCoV)2O4 exhibited a higher Cdl of 18.30 mF cm−2 and ECSA of 1.83 cm2 compared to CrCo2O4 (16.62 mF cm−2 and 1.66 cm2) and commercial IrO2 (14.02 mF cm−2 and 1.40 cm2). These results indicate that HE-Cr(NiFeCoV)2O4 possesses a greater number of accessible active sites, attributed to its high-entropy structure, which enhances both the intrinsic activity and availability of catalytically active regions during OER.30,46 In addition to catalytic activity, long-term stability of electrocatalysts is a critical parameter for real-world applications. Long-term stability testing results of the HE-Cr(NiFeCoV)2O4 catalyst are displayed in Fig. 3g. Notably, during the prolonged stability test conducted at 50 mA cm−2 for over 100 h, HE-Cr(NiFeCoV)2O4 maintained a nearly stable potential throughout continuous OER operation, highlighting its excellent long-term stability. Post-stability analyses, including SEM, EDS, and XPS, further confirmed the robustness of the HE-Cr(NiFeCoV)2O4 electrode before and after OER stability testing at 50 mA cm−2 over 100 h. SEM and EDS images (Fig. S14†) showed that the surface morphology and elemental composition of the HE-Cr(NiFeCoV)2O4 electrode were retained after extended OER operation. Additionally, XPS plots (Fig. S15a–f†) indicated slight increases in Cr4+ intensities and shifts in the Cr 2p, Ni 2p, Fe 2p, Co 2p, V 2p, and O 1s peaks of the HE-Cr(NiFeCoV)2O4 electrode following OER stability testing, suggesting electrochemical modifications to its surface during continuous OER. This surface modification likely contributed to the enhanced OER performance of the HE-Cr(NiFeCoV)2O4 catalyst. Remarkably, Fig. 3h and Table S1† illustrate that the HE-Cr(NiFeCoV)2O4 catalyst exhibited the lowest overpotential among many recently reported OER catalysts. Overall, these comprehensive electrochemical results highlight the exceptional OER performance of the HE-Cr(NiFeCoV)2O4 catalyst, which combines low overpotential with excellent stability. These advantages can be primarily attributed to the synergistic effects of its multicomponent composition, optimized electronic structure, large surface area, enhanced electrical conductivity, increased configurational entropy, and improved surface-active sites. Thus, the CO2 laser-engineered HE-Cr(NiFeCoV)2O4 catalyst is a promising candidate for OER in water electrolysis, advancing sustainable H2 production.
To gain a deeper understanding of how multiple metal components influence the electronic structure and OER performance of the HE-Cr(NiFeCoV)2O4 catalyst, DFT calculations were performed. The optimized top- and side-view crystal structures of CrCo2O4 (Fig. 5c and S16†) and HE-Cr(NiFeCoV)2O4 (Fig. 5d and S17†) confirmed the successful incorporation of Cr, Ni, Fe, Co, and V into a single spinel oxide structure. The charge density difference plots (Fig. 5e and S18†) revealed considerable redistribution of charge around the metal centers, indicating electronic modulation throughout the HE-Cr(NiFeCoV)2O4 structure. This is ascribed to the incorporation of multiple transition metal cations, which further enhances the electronic properties of the catalyst and is consistent with its superior OER performance.44 Moreover, the partial and total density of states (PDOS and TDOS) plots (Fig. 5f–h) reveal a substantially higher TDOS near the Fermi level for HE-Cr(NiFeCoV)2O4 compared to CrCo2O4. This enhancement primarily arises from the combined contributions of Cr(d), Ni(d), Fe(d), Co(d), and V(d) orbitals, suggesting improved electrical conductivity that facilitates rapid charge transport during OER. These theoretical results further corroborate the experimentally observed enhancement in OER performance of HE-Cr(NiFeCoV)2O4.49
To evaluate the intrinsic OER activity of various metal sites, we calculated the Gibbs free energy changes associated with the adsorption and transformation of key OER intermediates (*OH, O*, and *OOH) on the Cr, Ni, Fe, Co, and V sites of the HE-Cr(NiFeCoV)2O4 surface. The 4e− OER pathway at these active sites, along with the corresponding Gibbs free energy diagrams, is illustrated in Fig. 6a–e. The reaction mechanism proceeds via the adsorption and dissociation of H2O to form the *OH intermediates, followed by the sequential formation of *O and *OOH species. The final step involves the evolution of O2, thereby regenerating the active site. Gibbs free energy diagrams calculated at U = 0 V and U = 1.23 V indicate that the formation of *OOH constitutes the potential-determining step (PDS) across all active sites. Among these, the Fe site exhibits the lowest overpotential of 0.45 V, suggesting it is the most favorable active site for OER. This theoretical finding is consistent with Raman spectroscopy results, which demonstrate the in situ formation of FeOOH during OER, likely due to progressive oxidation at the Fe sites. To further investigate this phenomenon, we constructed a model featuring a surface FeOOH layer on HE-Cr(NiFeCoV)2O4 (Fig. S19†), optimized the adsorption of OER intermediates on the Fe site of this modified structure, and calculated the corresponding Gibbs free energy profile (Fig. 6f). Notably, the presence of FeOOH further decreased the OER overpotential from 0.45 V to 0.41 V, emphasizing the critical role of surface-formed FeOOH in enhancing OER activity. Collectively, these DFT results highlight the synergistic effects of multi-metallic sites in modulating the electronic structure and reducing reaction energy barriers, thereby conferring superior OER performance to the HE-Cr(NiFeCoV)2O4 catalyst.1,50 Consequently, the continuous-wave CO2 laser-synthesized HE-Cr(NiFeCoV)2O4 catalyst emerges as a promising candidate for water electrolysis, facilitating efficient H2 production.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ta01573a |
‡ These authors contributed equally to this work. |
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