The HN liquid used in this work was prepared by slowly adding FeSO4 solution (in H2O) into Ni(NO3)2 solution (in isopropanol) (Fig. 1a), and the insoluble nanoparticles were formed due to the poor solubility of metal salts (e.g., sulfates) in organic solvents. High-angle annular dark-field imaging scanning transmission electron microscopy (HAADF-STEM) images demonstrate that the insoluble nanoparticles were widely and evenly distributed, with an average diameter of 1.57 ± 0.49 nm (Fig. 1b and Supplementary Fig. 1). Energy-dispersive X-ray (EDX) results showed the uniform distribution of Fe, Ni, O, and S in the nanoparticles (Supplementary Fig. 2), with a Ni/Fe atomic ratio of 3.96 characterized by inductively coupled plasma mass spectrometry (ICP-MS). Then, a one-step soaking of NF in the above HN liquid at 25°C for 24 h was conducted to obtain the CAPist-L1 catalyst (Fig. 1a and Supplementary Fig. 3). The nanoparticles adsorb on the surface of NF to reduce the interfacial energy and act as the crystal nucleus (i.e., seeds), without the fundamental nucleation process (e.g., common LDH catalysts generated in homogeneous solution), to facilitate the formation of the catalyst structure. The seed-assisted HN process could easily prepare the CAPist-L1 catalyst with a large size of 20 cm × 20 cm over nickel-based substrates, such as NF (Fig. 1c) or nickel mesh (Supplementary Fig. 4).
X-ray diffraction (XRD) patterns for prepared CAPist-L1 were consistent with the refined Ni2Fe(SO4)0.5(OH)6(H2O)3.85 (Fig. 1d and Supplementary Fig. 5). The large SO42− ions in the interlayer resulted in a small diffraction peak corresponding to (001) at 8.1°. The Raman peak at 980 cm− 1 also confirmed the presence of SO42− in CAPist-L1 (Supplementary Fig. 6). Both X-ray absorption near-edge structure (XANES) spectra of the Fe K-edge and X-ray photoelectron spectra of Fe 2p confirmed that the oxidation state of Fe in CAPist-L1 was similar to that in a typical NiFe-LDH catalyst (Supplementary Fig. 7a and Fig. 8). Fourier transform extended X-ray absorption fine structure (FT-EXAFS) data showed a larger Fe-O scattering path for CAPist-L1 (1.56 Å) than that for NiFe-LDH (1.51 Å), while their Fe-O-Fe/Ni scattering paths were similar to each other (2.75 Å) (Supplementary Fig. 7b). Scanning electron microscopic images (SEM) of CAPist-L1 showed micron-scale hydrangea-shaped structures grew vertically and evenly distributed on a honeycomb-like catalyst base (Fig. 1e), different from the stacked nanosheets of NiFe-LDH (Supplementary Fig. 9). As demonstrated below, this hierarchical structure of CAPist-L1 can effectively increase the electrochemically active area and facilitate the release of oxygen bubbles from inter-channels to the surface before ultimate detachment. ICP-MS results indicated a Ni/Fe atomic ratio of 2.21 in CAPist-L1. Energy-dispersive X-ray (EDX) transmission electron microscopy (TEM) images indicated that Ni, Fe, O, and S were uniformly distributed in the catalyst structure (Supplementary Fig. 10).
The OER performance of CAPist-L1 was evaluated in 1 M KOH at 25°C in a three-electrode system, compared with those of typical NiFe-LDH (self-synthesized, one of the best LDH-type OER catalysts as shown in Supplementary Fig. 11), commercial IrO2, and blank NF catalysts. The iR-corrected polarization curves at an ampere-scaled current density of 1000 mA cm− 2 show that the overpotential of CAPist-L1 was only 220 ± 4.5 mV, much lower than those of NiFe-LDH (337 ± 4.8 mV) and IrO2 (594 ± 4.2 mV) (Fig. 2a). Furthermore, CAPist-L1 exhibited an overpotential of only 283 ± 12.7 mV even at a higher current density of 5000 mA cm− 2. These results indicated that CAPist-L1 had a high OER activity. Noticeably, we also found that the activity of CAPist-L1 had high repeatability and uniformity (Supplementary Fig. 12). The OER Faradaic efficiency of CAPist-L1 was nearly 100% (Supplementary Table 1), which together with facile synthesis temperature and ultra-low material cost (Fig. 2b) makes it a great promise for industrial applications.
To understand the intrinsic reasons that dominate the OER activity of CAPist-L1, the in-situ Raman measurements were conducted in 1 M KOH to explore the active sites of the catalyst. With increasing anodic potentials, especially over 1.35 V (vs. RHE, same as below unless otherwise mentioned), two new peaks at 475 cm− 1 and 556 cm− 1 corresponding to NiIII-O 35 appeared (Supplementary Fig. 13). The result showed that OER processes were mainly related to the NiIII-O for both CAPist-L1 and NiFe-LDH. Besides, because of the strong hierarchy of CAPist-L1 catalyst layers, abundant interspaces existed in the hierarchical sheet array, which was capable of contributing to the decrease of ions diffusion distance and thus the increase of OER activity 36.
Note that mass transfer becomes a key factor determining electrochemical performance when the current density is increased. At an ampere-scaled current density, sluggish detachment of the oxygen bubbles (i.e., bubble clogging) from the catalyst surface inevitably contributes to a decrease in the surface area, inhibition of electrolyte ion diffusion, an increase in the local pressure, and thus shedding and stripping of the catalyst. Therefore, the OER activity is significantly limited at high current densities, as indicated by crooking of the polarization curve for NiFe-LDH at approximately 1500 mA cm− 2 (relative to the dashed line in Fig. 2a). In contrast, CAPist-L1 exhibited good mass transfer, and no obvious OER suppression was observed even up to 5000 mA cm− 2. The good mass transfer of CAPist-L1 was further evidenced by the statical analysis of the formed bubbles at the electrode surface at 1000 mA cm− 2, which demonstrated an average bubble diameter of ~ 39 µm much smaller than that of NiFe-LDH (~ 66 µm) (Supplementary Fig. 14). Interestingly, the size of the bubbles generated by CAPist-L1 decreased as the current density increased, which is the opposite of the trend seen for NiFe-LDH (Supplementary Fig. 15). It is plausible that the difference in mass transfer rates resulted mainly from the different material morphologies; that is, the hierarchical structure of the CAPist-L1 catalyst favored the bubble detachment because of the increase in the interlayer spaces from the inner catalyst layer to the outer layer 37. In addition, O2 bubble rupture may result in fluctuating OER performance 38, especially for large bubbles generated at high current densities.
Apart from the OER activity, the operation lifetime is a key parameter for the industrial utilization of catalysts. The durability of the CAPist-L1 catalyst was measured in a three-electrode system employing chronopotentiometry at a current density of 1000 mA cm− 2 in 1 M KOH at 25°C, comparing with those of NiFe-LDH and IrO2 (Fig. 2c). The anodic potential of CAPist-L1 was stable for over 14000 h (> 20 months). In contrast, the NiFe-LDH showed an obvious increase in the potential of approximately 400 mV after 1500 h, and the degradation of IrO2 was more severe as the potential increased from ~ 1.80 to ~ 2.50 V within 510 h. Considering the different synthesis technologies of these electrocatalysts, the CAPist-L1 (H2O) catalyst was further synthesized via soaking NF in a homogeneous metal solution (i.e., nickel and iron ions in water) for comparison. It also showed an obvious potential increase within 1700 h at 1000 mA cm− 2, similar to that of NiFe-LDH (Fig. 2c). The results confirmed that the unique seed-assisted HN process contributed to constructing a CAPist-L1 catalyst with enhanced stability.
Mechanical stability, structural stability, and chemical stability are key factors that substantially affect the lifetime of a catalyst 39–42. As observed in a cross-sectional SEM image (Figs. 3a and 3b), NiFe-LDH showed typically a single stacked nanosheet layer on the NF substrate. The CAPist-L1, however, was composed of two catalytic layers (i.e., hydrangea layer and honeycomb layer) and one dense interlayer on the surface of NF (Figs. 3c and 3d). The size of the catalyst sheet in each layer of CAPist-L1 increased from tens of nanometers for the interlayer to hundreds of nanometers for the honeycomb layer and to micrometers for the hydrangea layer (Supplementary Fig. 16). Accordingly, the interspaces in multilayers of CAPist-L1 catalyst gradually increased from the interlayer to the hydrangea layer as well. This hierarchical structure facilitated ion diffusion and gas release and prevented the decrease in mechanical stability. Besides, the dense interlayer anchored the hydrangea layer and honeycomb layer tightly on the surface of the NF, even covering the irregular surfaces (Supplementary Fig. 17), thus reinforcing the mechanical stability of the catalyst. Nano-scratch measurements were employed to determine the critical binding force of CAPist-L1, and the obtained value of 65.4 ± 6.0 mN was higher than that of NiFe-LDH (35.2 ± 8.2 mN) (Supplementary Fig. 18). The results confirmed a stronger adhesion force between the CAPist-L1 catalyst layer and the NF than that between the NiFe-LDH stacked nanosheet layer and the NF. To prove this, we conducted a short-term OER measurement (at 500 mA cm− 2 for 50 h), observing partial peeling-off of NiFe-LDH catalyst structure from NF substrate after the OER test (Supplementary Fig. 19). In contrast, CAPist-L1 exhibited good maintenance of the catalyst morphology based on the SEM images (Supplementary Fig. 20). Therefore, the interlayer would not participate in the OER process directly, but it mechanically fixed the catalyst layer against the adhesive force of oxygen bubbles and possible catalyst detachment 31.
To investigate the growth process of CAPist-L1, the ex-situ SEM was conducted to observe the catalyst hierarchical structures from the top view (Supplementary Fig. 21) and the cross-sectional view (Fig. 3e and Supplementary Fig. 22). The results showed that the catalyst structure appeared and grew rapidly within the first two hours. The dense interlayer, between the NF and catalytic layers, would hardly be observed until after four hours of soaking probably due to its slow growth kinetics. Then, the thickness of the interlayer gradually increased from hundreds of nanometers (soaking time of 4–8 h) to several micrometers (soaking time of 16–96 h). Based on the grazing incidence X-ray diffraction analysis, the interlayer exhibited the same LDH-type structure as that of the catalytic layer in CAPist-L1 (Supplementary Fig. 23). We anticipated the underlying role of insoluble nanoparticles in HN liquid that contributed to the formation of the interlayer structure. Therefore, it was evaluated by increasing the H2O proportion in the HN liquid to eliminate the nanoparticles (Supplementary Fig. 24). For example, the CAPist-L1 (H2O), synthesized in homogeneous water solution, exhibited typical lamellar catalyst structure but without interlayer structure. Furthermore, interchanging soaking systems between HN liquid and homogeneous solution confirmed that the insoluble nanoparticles played a vital role in inducing the formation of the interlayer especially at the initial soaking stage (Supplementary Fig. 25). The insoluble nanoparticles were thus believed to absorb on the surface of NF substrate and then participate in the formation of interlayer with slow kinetics.
The structural stability of the catalyst was evaluated by exploring the retention of the crystal structure. The in-situ XRD results indicated that the crystallinity of CAPist-L1 was well preserved during electrocatalysis at 1.20–1.60 V, different from that of NiFe-LDH (Supplementary Fig. 26). Moreover, the aforementioned in-situ Raman spectroscopy indicated the formation of oxyhydroxide species during electrocatalysis for CAPist-L1 (Supplementary Fig. 13), which may explain why the interlamellar spacing of the unit cell, obtained from in-situ XRD, decreased from 0.7590 Å (at 1.30 V) to 0.7532 Å (at 1.60 V). Therefore, the presence of an amorphous layer on the surface of the micro-sheet did not damage the main LDH structure even at 1.60 V (Supplementary Fig. 26). Additionally, the aforementioned short-term OER test indicated that the crystal structure of the CAPist-L1 catalyst in KOH persisted after 50 h of the OER at 500 mA cm− 2 (Supplementary Fig. 27a), unlike the amorphization of NiFe-LDH (Supplementary Fig. 27b).
The chemical stability of the catalyst was estimated by measuring the concentrations of dissolved metal ions in the electrolyte. Even though the normalized activity of CAPist-L1 was higher than that of NiFe-LDH, the concentrations of dissolved Fe and Ni ions were much lower (Supplementary Fig. 28a). The stability number of noxygen/nions, proposed by Geiger et al. 43, was used to determine the chemical stability of a catalyst, where noxygen is the number of oxygen molecules, nions is the number of dissolved cations and the high S-number indicates good chemical stability of the catalyst. After 50 h short-term OER catalysis, the S-number of CAPist-L1 (noxygen/nNi+Fe = 24627) was approximated four-fold higher than that of NiFe-LDH (noxygen/nNi+Fe = 5893), indicating that the CAPist-L1 has superior electrochemical stability (Supplementary Fig. 28b). The fitted EXAFS results showed that the coordination numbers (CNs) of the Fe-O and Fe-O-Fe/Ni species in CAPist-L1 are 5.7 and 2.9, respectively, after 50 h of OER, and these values were higher than those of the NiFe-LDH (CN = 5.0 for Fe-O, CN = 2.5 for Fe-O-Fe/Ni) (Supplementary Fig. 29 and Supplementary Table 2), consistent with the aforementioned results of the dissolution experiment. Therefore, the enhanced mechanical, structural, and chemical stabilities of CAPist-L1 enabled long-term measurements for over 14000 h at 1000 mA cm− 2 without an obvious activity decline.
We then explored the practical utilization of CAPist-L1 as an anode catalyst in a 1 cm2 (electrode area: 1 cm × 1 cm) AEM-WE system (Fig. 4a and Supplementary Fig. 30) and compared this anode to the NiFe-LDH and IrO2 anodes. In the AEM-WE electrolyzer, a terphenyl-based poly (aryl piperidinium) polymer (PAP-TP-85, dry thickness of 45.0 ± 0.6 µm) was used as the anion exchange membrane, and noble metal-free Ni4Mo/MoO2 known as a superior HER catalyst (detail information are described in the experimental section of S.I.) was used to catalyze H2O into H2. At 80°C, the current density of the CAPist-L1-catalyzed AEM-WE (CAPist-L1//Ni4Mo/MoO2) system was 7350 mA cm− 2 at a cell voltage of 2.0 V, approximately 1.6-fold and 3.0-fold higher than those of the NiFe-LDH (4450 mA cm− 2) and IrO2 (2410 mA cm− 2) systems, respectively (Fig. 4b and Supplementary Fig. 31). The Faradaic efficiency in the AEM-WE was 99.29 ± 0.59% in a short-term measurement (Supplementary Fig. 32). The CAPist-L1//Ni4Mo/MoO2 system showed one of the best performance levels reported to date for water electrolysis (e.g., AEM-WE and PEM-WE as shown in Supplementary Table 3 and Table 4, respectively) and demonstrated the potential of replacing noble metal-based catalysts with CAPist-L1 to produce hydrogen cost-effectively in alkaline solutions.
The long-term durability of the CAPist-L1//Ni4Mo/MoO2 electrolyzer (1 cm2) was evaluated in 1 M KOH at 1000 mA cm− 2, achieving stable operation for over 1700 h at 25°C and over 1500 h at 80°C (Fig. 4c). In addition, the electrolyzer was also stable at 2000 mA cm− 2 for 1200 h (Supplementary Fig. 33). These results indicated the high stability of CAPist-L1 catalyst at industrial-scale current densities in practical utilization, much better than most reported anode electrocatalysts.
Based on the 1 cm2 electrolyzer measurements, we further tested a 25 cm2 CAPist-L1//Ni4Mo/MoO2 electrolyzer (electrode area: 5 cm × 5 cm) in 1 M KOH. The 25 cm2 electrolyzer exhibited a high current density of 2730 mA cm− 2 (60°C) at a cell voltage of 1.80 V, surpassing the U.S. DOE target for alkaline water electrolysis systems (2000 mA cm− 2 at 1.80 V) 44 (Fig. 4d). Impressively, the water electrolysis performance of the electrolyzers remains similar when increasing the electrode area from 1 cm2 to 25 cm2. For example, at 1000 mA cm− 2, the cell voltage of the 1 cm2 electrolyzer was approximately 1.622 V at 60°C, which was very similar to that of the 25 cm2 electrolyzer (1.623 V). The results demonstrated the good scale-up feasibility of CAPist-L1 as an AEM-WE anode. In addition, the pilot CAPist-L1//Ni4Mo/MoO2 electrolyzer was operated stably at 25000 mA (i.e., 1000 mA cm− 2) for 1500 h at 25°C (Fig. 4e). Overall, the pilot-scale CAPist-L1//Ni4Mo/MoO2 electrolyzer showed the expected durability and strikingly good performance for water electrolysis.