Xianggang
Huang‡
a,
Xin
Wang‡
b,
Mengling
Zhang
a,
Qilei
Jiang
a,
Zheng
Qin
a,
Yingxin
Liu
a,
Yan
Hou
a,
Xueqin
Cao
*a and
Hongwei
Gu
*a
aKey Laboratory of Organic Synthesis of Jiangsu Province, College of Chemistry, Chemical Engineering and Materials Science and Collaborative Innovation Center of Suzhou Nano Science and Technology, Soochow University, Suzhou 215123, P. R. China. E-mail: hongwei@suda.edu.cn; xqcao@suda.edu.cn
bKey Laboratory of Rare Mineral of hubei Province, Ministry of Natural Resources, Hubei Geological Experimental Testing Center, Wuhan 430034, P. R. China
First published on 11th January 2023
As one of the semi-reactions of water splitting, electrocatalytic oxygen evolution reactions (OERs) are key process to generate sustainable energy. Co-based spinel oxides are deemed as promising OER electrocatalysts, but the low intrinsic activity limits their further practical applications. Herein, we report an effective strategy to synthesize CoCeMn coordination-driven self-assembled aggregates (CDSAAs) by a one-pot multi-step method. It is different from the common mixed addition method to synthesize trimetallic nanomaterials. Subsequently, CoCeMn-CDSAAs served as self-templates, and Mn and Se co-doped CeO2@Co3O4 porous core–shell nanospheres (MnSe–CeO2@Co3O4) were obtained after calcination and selenization treatments. It is worth mentioning that CeO2 and the doping Mn/Se elements increase the oxygen vacancy content and the ratio of Co3+/Co2+ on the surface respectively and can effectively accelerate the four-electron transfer process of OERs. Moreover, the special porous core–shell structure exposes more active sites and is also useful for boosting OER performance. When explored as an anode electrocatalyst for OERs, MnSe–CeO2@Co3O4 exhibits excellent OER performance (284 mV@10 mA cm−2) and a long-time stability of 40 h in an alkaline medium. This work provides a feasible idea for the construction of multi-component porous core–shell nanoelectrocatalysts with non-noble metals.
In recent years, spinel transition-metal oxides have received extensive attention from researchers around the world due to their low price, easy availability and abundant storage.7,8 Furthermore, Co3O4, as a cobalt-based spinel oxide, has been regarded as a potential OER electrocatalyst because of its excellent performance in an alkaline medium.9,10 However, the practical application of pure Co3O4 is limited because of its poor intrinsic conductivity and insufficient active sites.11 Developing efficient OER electrocatalysts with competitive price, low overpotential and long-time stability is challenging, and researchers have made considerable efforts to boost the OER performance of Co3O4 through these years.
On the one hand, the intrinsic activity of the materials can be improved obviously by increasing oxygen vacancies or doping other elements.12–14 CeO2, as a rare earth oxide, has been considered as an effective synergist for OERs due to its excellent redox ability and abundant oxygen vacancies.15,16 After introducing CeO2, the valence state conversion between Ce3+ and Ce4+ can accelerate electron transfer and increase the oxygen vacancies of materials, thus promoting the catalytic activity for OERs.17 Qiu et al. constructed a special CeO2/Co3O4 heterojunction interface with enhanced OER performance, which is attributed to the abundant oxygen vacancies and interfacial coupling effect between the components.18 Moreover, doping other elements such as manganese (Mn),19 iron (Fe),20 selenium (Se),21 and sulfur (S)22 can regulate the electronic structure of catalysts, resulting in faster four-electron transfer progress and is regarded as a promising method to enhance their intrinsic activity. Moreover, a higher content of Co3+ in nanomaterials also contributes to better OER performance.23,24 Qi et al. designed a Mn and S dual-doped Co3O4 electrode array for efficient OERs. The excellent OER performance is attributed to their improved electrical conductivity and increasing ratio of Co3+/Co2+ after doping with Mn and S elements.25 On the other hand, appropriate morphology designs such as core–shell structure can expose more active sites and facilitate charge transfer in materials.26,27 Currently, numerous strategies have been developed to construct core–shell structures such as the Kirkendall effect,28 Ostwald ripening,29 and template method.30 Zhang et al. synthesized pure CeO2 core–shell nanospheres by a simple self-template and calcination method.31 However, the preparation of multielement core–shell hybrid nanomaterials is still a great challenge and has rarely been reported.
Herein, we report a facile approach to fabricate CoCeMn coordination-driven self-assembled aggregates (CDSAAs) by a simple one-pot multi-step method, in which the Ce element is enriched at the core of the solid nanosphere. Subsequently, CoCeMn-CDSAAs as self-temples were calcined in air to form Mn-doped CeO2@Co3O4 porous core–shell nanospheres (Mn–CeO2@Co3O4). Finally, Mn–CeO2@Co3O4 was selenized in an Ar atmosphere and Se/Mn co-doped CeO2@Co3O4 porous core–shell nanospheres (MnSe–CeO2@Co3O4) were obtained (Fig. S1, ESI†). CeO2 can effectively increase the oxygen vacancy content on the surface, which is helpful for promoting the OER performance. After doping of Se and Mn elements, the alteration of Co electronic structure can not only increase the electrical conductivity, but also improve the ratio of Co3+/Co2+ of the nanomaterial, which both contribute to enhancing the OER kinetic properties. In an alkaline medium of 1.0 M KOH, MnSe–CeO2@Co3O4 exhibits a low overpotential of 284 mV@10 mA cm−2, which is much lower than that of Co-oxides (419 mV@10 mA cm−2). In addition, they also exhibit the lowest Tafel slope of 94 mV dec11 and excellent stability of 40 h.
From the perspective of morphology, CoCeMn-CDSAAs are smooth solid nanospheres with a diameter of about 1 μm (Fig. 1(a) and (b)). Moreover, the larger magnification TEM image reveals that there is a darker shadow inside the nanospheres (Fig. 1(c)). A series of CoCeMn-CDSAAs with different metal ratios can be easily obtained when adjusting the amount of different metal salts added in the one-pot multi-step method. Meanwhile, it can be illustrated by inductively coupled plasma-atomic emission spectroscopy (ICP-AES) that the elemental ratios of Co and Ce roughly match the feeding ratios and the Mn element is mainly doped by small amounts (Table S1, ESI†). When adjusting metal ratios or synthesizing by a one-step method, the obtained nanospheres show different sizes or inhomogeneity (Fig. S2–S6, ESI†). When illustrated from a structural perspective, X-ray diffraction (XRD) and selected area electron diffraction (SAED) results both indicate that CoCeMn-CDSAA nanospheres are amorphous (Fig. 1(d) and (e)). Similarly, monometallic and bimetallic nanospheres can also be easily synthesized, and XRD patterns demonstrate that Co-CDSAAs, CoCe-CDSAAs and CoMn-CDSAAs are also amorphous (Fig. S7, ESI†). Moreover, the Fourier transform infrared (FT-IR) spectroscopy characterizations (Fig. S8, ESI†) reveal that Co-CDSAAs, CoMn-CDSAAs, CoCe-CDSAAs and CoCeMn-CDSAAs show the same IR absorption peaks, which suggest that they have the same coordination mode, and thus, they have similar morphological characteristics.32,33 EDX elemental mapping results indicate that the Ce element enriches at the core of the sphere, while C, N, O, Co and Mn elements are uniformly distributed in the solid nanospheres (Fig. 1(f)), which is the basis for the formation of porous core–shell structures after calcination.
According to thermogravimetric (TGA) curves (Fig. S9, ESI†), CoCeMn-CDSAAs are able to form corresponding oxides after annealing at over 400 °C. Based on energy-dispersive X-ray spectroscopy (EDX) data (Table S2, ESI†), the metal ratios in the corresponding metal oxides remain consistent with the precursors. Interestingly, the high content of Ce elements can effectively strengthen their structural stability under high temperature conditions. The intensity of the diffraction peaks belonging to CeO2 in the XRD pattern gradually decreases (Fig. S10, ESI†), which also indicates that the content of CeO2 gradually decreases from CoCeMn-oxides-1 to CoCeMn-oxides-5. With the decrease in the content of Ce elements, the solid structure of the nanospheres starts to disappear and forms a porous core–shell structure (Fig. S11 and S12, ESI†). When the atomic ratio of Co/Ce is 8.54 in CoCeMn-CDSAAs, Mn-CeO2@Co3O4 exhibits a complete porous core–shell structure after calcination (Fig. 2(a) and (b)). When the content of Ce elements continues to be reduced, the structure of CoCeMn-oxides-5 collapses (Fig. S11g and S12g, ESI†). Follow-up electrochemical active surface area (ESCA) results (Fig. S17d, ESI†) also reveal that Mn–CeO2@Co3O4 possesses the most abundant electrochemical active sites among CoCeMn-oxides-x (x = 1–5), which may be due to their well-defined porous core–shell structure. Fig. 2 shows the successful formation of Mn–CeO2@Co3O4 after calcination. Evidently, the diameter of Mn–CeO2@Co3O4 shrinks to about 600 nm, and a porous core–shell structure is formed (Fig. 2(a)–(c)). The XRD pattern, high-resolution TEM (HRTEM) image and SAED pattern all show that there is a two-component heterogeneous structure in Mn–CeO2@Co3O4 (Fig. 2(d)–(f)), which corresponds to CeO2 (PDF#34-0394) and Co3O4 (PDF#43-1003), respectively. Compared with CoCe-oxides, there is a significant negative shift of Co3O4 (311) in Mn–CeO2@Co3O4 (Fig. S13b, ESI†), which proves the successful doping of Mn elements in Co3O4.34,35 In addition, the EDX elemental mapping (Fig. 2(g)) also reveals the formation of CeO2 and Co3O4 heterostructures and uniform distribution of C, N, O, and Mn elements in Mn–CeO2@Co3O4. When other factors are adjusted to synthesize the comparison material, the spherical morphology of CoCeMn-oxides-x (x = 6–10) are largely preserved though most of nanospheres showed unsatisfactory core–shell morphology (Fig. S4–S6, ESI†). However, the spherical morphology of Co-oxides, CoMn-oxides and CoCe-oxides was severely fragmented after calcination (Fig. S10 and S11, ESI†). All these results indicate that coexistence of Co, Ce and Mn elements is important for maintaining the spherical morphology. Moreover, a suitable metal ratio in precursors and a unique one-pot multi-step method both contribute to favorable porous core shell structures after calcination.
Modulating the electronic structure of metal atoms by heteroatom doping can effectively optimize the kinetic process of OERs.36 Therefore, Mn–CeO2@Co3O4 is selenized to further enhance its OER performance. The SEM and TEM images of the obtained MnSe–CeO2@Co3O4 are shown in Fig. 3, and the porous core–shell structure of Mn–CeO2@Co3O4 is preserved. As exhibited in Fig. S14 (ESI†), the surface area is about 298.67 m2 g−1 and the corresponding pore size is about 4.26 nm for MnSe–CeO2@Co3O4. Fig. 3(a)–(c) show that the morphology of MnSe–CeO2@Co3O4 is almost unchanged after selenization, whose diameter is about 500 nm. The XRD, HRTEM and SAED results (Fig. 3(d)–(f)) all correspond to CeO2 (PDF#34-0394) and Co3O4 (PDF#43-1003), revealing the presence of CeO2 and Co3O4 heterostructures. In addition, there is no new diffraction peak of CoSe2, which proves the successful doping of Se elements in Co3O4. The magnified XRD spectra show that there is almost no obvious movement for the diffraction peak belonging to Co3O4 (311) in MnSe–CeO2@Co3O4 compared with Mn–CeO2@Co3O4 (Fig. S13b, ESI†), implying that suitable elemental doping of Se elements can hardly alter the crystal structure of Mn–CeO2@Co3O4.37 EDX elemental mapping results (Fig. 3(g)) also show the presence of CeO2 and Co3O4 heterostructures and the uniform distribution of C, N, O, Mn, Se elements in MnSe–CeO2@Co3O4.
To further investigate the role of CeO2 as well as the doping of Mn/Se elements in MnSe–CeO2@Co3O4, the elements and the corresponding chemical statuses of samples were investigated by X-ray photoelectron spectroscopy (XPS). The presence of C, N, O, Co, Ce, Mn and Se elements is observed in both EDX (Fig. 4(a)) and survey spectra (Fig. 4(b)) of MnSe–CeO2@Co3O4. The low content of Se and Mn elements in EDX spectrum can further prove their doping in MnSe–CeO2@Co3O4. The orbital peak of Ce 3d splits into a series of Ce3+ and Ce4+ peaks, indicating that Ce3+ and Ce4+ coexist in MnSe–CeO2@Co3O4 (Fig. 4(c)). The peaks at 885.2 and 903.9 eV are attributed to Ce3+, while the peaks at 882.4, 887.8, 898.3, 901.3, 907.4, and 916.7 eV are attributed to Ce4+.38,39 The XPS spectrum of O 1s can be divided into three peaks (donated as O1, O2, and O3 in Fig. 4(d)). The O1 peak at 530.0 eV is attributed to the metal–oxygen bond in the material, the O2 peak at 531.2 eV is attributed to the oxygen vacancy and the O3 peak at 532.7 eV is attributed to the hydroxyl group adsorbed on the surface.40 It is noteworthy that high oxygen vacancy contents can enhance the intrinsic activity of the material and optimize the kinetic properties of the OER progress.41,42 The introduction of CeO2 effectively increases the content of oxygen vacancies (Table S3, ESI†), which is useful for improving the intrinsic activity of nanomaterials. For Co 2p (Fig. 4(e)), the peaks at 796.7 and 781.5 eV correspond to Co 2p1/2 and Co 2p3/2 of Co2+, while the peaks at 795.0 and 779.9 eV are attributed to Co 2p1/2 and Co 2p3/2 of Co3+ with the presence of two vibrational satellite peaks (787.6 and 803.6 eV).43,44 Compared with Co-oxides, there are positive shifts in the binding energy of Co 2p3/2 after introduction of CeO2 and Mn/Se elements (Fig. 4(e)), which implies the electron transfer among different components. This phenomenon may be due to the rearrangement of electron distribution resulting from the interaction of Co with CeO2 or dopants. The strong interaction in MnSe–CeO2@Co3O4 may modulate the frontier orbital energy of the catalysts, which is useful for improving the kinetic process of OERs.45,46 Moreover, it is worth mentioning that the doping of Mn/Se elements can significantly increase the content of Co3+ (Table S3, ESI†), and high activity of Co3+ can effectively accelerate the kinetic process of OERs.47,48 It is obvious that a high ratio of Co3+/Co2+ and a high oxygen vacancy content in MnSe–CeO2@Co3O4 are important to enhance their electrochemical performance.
At room temperature, the OER performance of the prepared catalysts is explored in an alkaline medium of 1 M KOH. It should be noticed that MnSe–CeO2@Co3O4 is chosen as the main discussion object in the following based on that Mn–CeO2@Co3O4, as the precursor of MnSe–CeO2@Co3O4, is demonstrated to have the most promising performance among CoCeMn-oxides-x (x = 1–10), as observed from Fig. S17 and S19 (ESI†). As shown in Fig. 5(a), the anodic linear scanning voltammetry (LSV) polarization curves of different catalysts exhibit significant differences at a scan rate of 10 mV s−1. MnSe–CeO2@Co3O4 exhibits the optimal overpotential of 284 mV among these comparison materials, which is significantly lower than that of Co-oxides (419 mV), CoMn-oxides (390 mV), CoCe-oxides (365 mV) and Mn–CeO2@Co3O4 (336 mV). The OER performance of trimetallic oxides is better than that of monometallic or bimetallic oxides, indicating that the synergistic effect of multiple components and the special porous core–shell structure contribute to their excellent performance. In addition, the corresponding oxides showed similar OER results after selenization (Fig. S19b, ESI†), which are attributed to the synergy of multiple components and porous core shell structure. Moreover, the OER performance of MnSe–CeO2@Co3O4 is superior to that of commercial RuO2 (362 mV) (Fig. S18, ESI†) and most recently reported Co3O4-based or CeO2-based catalysts (Fig. 5(f) and Table S4, ESI†). The Tafel slope can further explain the OER properties from a kinetic point of view. The smaller value of Tafel slope means the faster kinetic process of OERs.49 Among these tested catalysts, MnSe–CeO2@Co3O4 exhibits the smallest Tafel slope of 94 mV dec−1, revealing their boosting OER kinetic process (Fig. 5(b)). The ESCAs are collected to probe the actual number of active sites involved in the electrochemical reaction. The ESCAs of the catalysts exhibit a positive correlation with double layer capacitance (Cdl) and the Cdl value can be obtained in the non-faradaic region with different scan rates (Fig. S20, ESI†).50 As shown in Fig. 5(c), the Cdl value of MnSe–CeO2@Co3O4 (25.3 mF cm−2) is much higher than that of other catalysts, which suggests that MnSe–CeO2@Co3O4 has more active sites under the same loading condition. Electrochemical impedance spectroscopy (EIS) value can effectively reflect the electron transfer rate and resistance value between the catalyst and the electrolyte.51 The smaller radius of the impedance arc represents its smaller charge transfer resistance (Rct), which results in the improved OER activity of the catalysts. The Nyquist curves (Fig. 5(e)) show that MnSe–CeO2@Co3O4 has the smallest semi-circular diameter among catalysts, which means the smallest charge transfer resistance (Rct) (only 34 Ω). This phenomenon indicates that there is a significant enhancement of the electrical conductivity in materials after the doping of Se elements. A series of OER tests have shown that the doping of CeO2, Mn and Se elements can contribute significantly to the improvement of the OER performance. Compared with Co-oxides and CoMn-oxides, CoCe-oxides and CoCe–Mn-oxides clearly possess a lower overpotential, faster OER kinetic performance, larger electrochemically active surface area and smaller charge transfer resistance, respectively. This is attributed to the increased oxygen vacancy content caused by the introduction of CeO2. Similarly, a series of performance tests can also show that Mn and Se elements provide higher levels of Co3+ to the catalyst in favor of the enhanced OER performance of the catalyst.
The stability is an important parameter for evaluating their electrochemical performance, which contributes to the further practical application of the catalysts.52,53 Cyclic voltammetry (CV) and chronopotentiometric (CP) methods are used to test the stability of MnSe–CeO2@Co3O4. The OER polarization curve of MnSe–CeO2@Co3O4 remains almost unchanged after 1000 CV cycles, reflecting their excellent stability (Fig. S21, ESI†). To reduce the effect of sample shedding, MnSe–CeO2@Co3O4 dropped on an inactive carbon paper substrate for testing their OER performance. Reaching the current density of 10 mA cm−2, the overpotential of MnSe–CeO2@Co3O4 on the carbon paper is 310 mV in 1 M KOH solution (Fig. 6(a)) and the OER activity is almost unchanged after the CP test of 40 h (Fig. 6(b)). The TEM image (Fig. 6(c)) shows that the porous core–shell morphology of MnSe–CeO2@Co3O4 is still preserved after the long-time CP test, revealing the superior structural stability of porous core–shell structures. Moreover, the main components of MnSe–CeO2@Co3O4 are still Co3O4 and CeO2 after stability testing (Fig. 6(d), Fig. S22 and S23, ESI†), indicating the stable composition of catalysts. The XPS spectra are employed to further understand the elemental valence changes of MnSe–CeO2@Co3O4 after stability testing. It is worth noting that MnSe–CeO2@Co3O4 still maintains a high ratio of Co3+/Co2+ (Fig. 6(e)) and a high oxygen vacancy content (Fig. 6(f)) after the stability test, which may be the reason for their excellent stability (Table S3, ESI†).
The desirable electrochemical property of MnSe–CeO2@Co3O4 may be attributed to the following reasons. First, BET and ESCA results both reveal that the porous core–shell structure possesses a larger specific surface area and more active sites for OERs. The large area of interfaces in contact with the electrolyte can accelerate the active intermediate transport and diffusion on the surface of catalysts, thus optimizing their catalytic capacity.54,55 Second, high oxygen vacancy contents can strengthen the intrinsic activity of catalysts, which facilitates the reduction of the OER reaction energy barrier and optimizes their OER activity.56 The XPS spectra illustrate that CeO2 can effectively increase the content of oxygen vacancies among the above-mentioned nanomaterials (Table S3, ESI†), which is considered as one of the reasons for their favorable OER activity. Third, element doping can lead to a shift of the metal elements from a lower valence to a more active higher valence state (for instance, Co2+ species are oxidized to Co3+ species) (Table S3, ESI†). The high oxidation state of Co3+ can facilitate the adsorption of OER intermediates and the four-electron transfer process of OERs.57,58 Moreover, the smallest Tafel slope of MnSe–CeO2@Co3O4 also means a faster four-electron transfer process of OERs (Fig. 5(b)). Finally, the EIS value of MnSe–CeO2@Co3O4 is significantly lower than that of other comparison catalysts (Fig. 5(e)). This is mainly because the introduced substances affect the coordination environment and electronic structure of the adjacent Co atoms, leading to lattice distortions and defects, which really enhance the electrical conductivity of the nanomaterials.59 Therefore, MnSe–CeO2@Co3O4 with the unique characteristics of morphology, structure and composition ultimately possess enhanced electrochemical properties.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2ya00315e |
‡ These authors contributed equally. |
This journal is © The Royal Society of Chemistry 2023 |