FeNi LDH/V2CTx/NF as Self-Supported Bifunctional Electrocatalyst for Highly Effective Overall Water Splitting

The development of bifunctional electrocatalysts with efficient oxygen evolution reaction (OER) and hydrogen evolution reaction (HER) is still a key challenge at the current stage. Herein, FeNi LDH/V2CTx/nickel foam (NF) self-supported bifunctional electrode was prepared via deposition of FeNi LDH on V2CTx/NF substrate by hydrothermal method. Strong interfacial interaction between V2CTx/NF and FeNi LDH effectively prevented the aggregation of FeNi LDH, thus exposing more catalytic active sites, which improved electrical conductivity of the nanohybrids and structural stability. The results indicated that the prepared FeNi LDH/V2CTx/NF required 222 mV and 151 mV overpotential for OER and HER in 1 M KOH to provide 10 mA cm−2, respectively. Besides, the FeNi LDH/V2CTx/NF electrocatalysts were applied to overall water splitting, which achieved a current density of 10 mA cm−2 at 1.74 V. This work provides ideas for improving the electrocatalytic performance of electrocatalysts through simple synthesis strategies, structural adjustment, use of conductive substrates and formation of hierarchical structures.


Introduction
Electrocatalytic water splitting to produce H 2 and O 2 as a green and efficient energy carrier has gained wide recognition and attention in the past decades [1][2][3][4]. Electrocatalytic water splitting consists of the process of HER and OER at the cathode and anode, respectively. In both cases, it is greatly significant to explore efficient and low-cost electrocatalysts to reduce the excessive overpotential [5,6]. To date, the commonly used OER and HER electrocatalysts are the commercially IrO 2 , RuO 2 materials and Pt/C materials [7,8]; however, the high cost, limited reserves and poor multifunctional properties greatly limit their applications in water splitting [9,10].

Sample Preparation 2.2.1. Preparation of V 2 CT x
Firstly, 1.0g V 2 AlC powder was gradually added to 20mL HF solution under stirring for 0.5 h and the suspension was kept stirring for 48 h at 55 • C. Secondly, the reaction mixture was rinsed with argon deoxygenated water and centrifuged. After that, the precipitate was re-dispersed to 20 mL TPAOH and stirred for 24 h. Next, the synthesized multilayer V 2 CT x was centrifuged and washed twice, freeze-dried and weighed for V 2 CT x MXene. V 2 CT x nanosheets suspension concentration is 8 mg mL −1 .

Preparation of V 2 CT x /NF
NFs (1 × 3 × 0.1 cm 3 ) were pretreated with concentrated HCl (3 M) for 0.5 h, and subsequently washed with acetone absolute ethanol and DI water. After that, NFs (1 × 3 × 0.1 cm 3 ) were placed in 20 mL MXene suspension for 1 h. MXene is firmly adsorbed on the surface of NF by electrostatic adsorption, and V 2 CT x /NF is prepared. After repeated washing with Ar de-aerated DI water, vacuum drying for later use.

Preparation of FeNi LDH/V 2 CT x /NF
FeNi LDH/V 2 CT x /NF was synthesized by the hydrothermal method. 100 mM urea, 5 mM Fe(NO 3 ) 3 ·9H 2 O and 15 mM Ni(NO 3 ) 2 ·6H 2 O were dissolved in 5 mL of DI water, stirring for 0.5 h to form a mixed solution (named solution A). 25 mL NMP was added to solution A and continued to stir for 0.5 h (named solution B). Then, V 2 CT x /NFs (1 × 3 × 0.1 cm 3 ) were placed in solution B and heated for 12 h at 120 • C. For comparison, FeNi LDH/NF, V 2 CT x /NF and Ni(OH) 2 V 2 CT x /NF was synthesized with the same process. The load of electrocatalyst was measured by weighing the NF electrode before and after electrocatalyst growth. In this report, for FeNi LDH/V 2 CT x /NF, the electrocatalyst load was about 5 mg cm −2 .

Preparation of RuO 2 /NF and Pt/C/NF
The RuO 2 (10 mg) was dispersed ultrasonically in a mixture of isopropanol (750 µL), Nafion (16 µL, 5.0 wt%) and deionized water (250 µL). The suspension was ultrasonic for 30min to obtain an evenly dispersed ink solution. Then, 500 µL of electrocatalyst ink was loaded on 1 × 1 cm 2 NF and the electrocatalyst load is about 5 mg cm −2 . The process for preparing Pt/C/NF is the same, except that commercial Pt/C (20 wt%) is used instead of commercial RuO 2 .

Materials Characterization
The morphology was studied by field emission scanning electron microscopy (FESEM, FEI Zeiss Sigma 300). Transmission electron microscopy (TEM) was recorded using an FEI TalosF200x. Powder XRD pattern was obtained by Cu-Kα (λ = 0.1540 nm) on a SMARTLAB (9) X-ray photoelectron spectroscopy (XPS); the signal was captured using Axis Ultra DLD Kratos AXIS SUPRA.

Electrochemical Measurements
The electrocatalytic property was determined using a standard three-electrode system in 1.0 M KOH solution on a CHI 760E electrochemical workstation. FeNi LDH/V 2 CT x /NF served as the working electrode, carbon rod (OER) or platinum plate (HER) and Hg/HgO electrode (1 M KOH solution) were served as the counter electrode and reference electrode, respectively. According to the Nernst Equation (E RHE = E Hg/HgO + 0.059 pH + 0.098 V), all potentials measured at the Hg/HgO electrode in this study were converted to potentials with the reversible hydrogen electrode (RHE). OER and HER were measured under the condition of O 2 and Ar saturation, respectively. Until the electrochemical data were tested, the working electrode was electrochemically activated for cyclic voltammetry 50 times. All the linear sweep voltammetry (LSV) curves are tested at 5 mV s −1 with 100% iR-compensation. The linear part of the Tafel curve was fitted according to the Tafel equation, and the Tafel slope was obtained to estimate the kinetic performance of the prepared electrocatalyst. Electrochemical impedance spectroscopy (EIS) was measured in the frequency range of 10 −2 to 10 6 Hz. The double layer capacitance (C dl ) of the electrocatalysts was obtained by cyclic voltammetry at different scanning rates at non-Faraday potentials, and the ECSA of the catalysts was calculated. At room temperature, the prepared electrodes acted directly for overall water splitting in a two-electrode cell.

DFT Calculation Details
Vienna AB-Initio Simulation Package using the projector augmented wave (PAW) method was applied for all DFT calculations [37,38]. The local d-electrons of Ni and Fe in hydroxides were described by the DFT+U method. The value of U-J was 3.3 eV for V, 6.4 eV for Ni and 4.3 eV for Fe [9,[39][40][41]. In order to simulate FeNi LDH/MXene nanohybrid, Fe doped NiOOH monolayer adsorption on O end V 2 CT x was considered to simulate the electrocatalyst [42]. Since it is difficult to measure the crystal orientation of Fe-doped NiOOH intermediates, a surface exposed (001) Fe-doped NiOOH layer was coupled with V 2 CT x to obtain the model with the most favorable energy structure and the lowest lattice mismatch for subsequent calculation. A 2 × 2 supercell of FeNi LDH and V 2 CT x monolayer was constructed to become an 11.69 Å × 11.69 Å cell with a 16 Å vacuum space. Every four Ni atoms are replaced by one Fe atom. The whole calculation process uses the K-point grid with dimensions of 3 × 3 × 1. During the structure optimization, the tolerance of residual force for each atom is 0.05 eV/Å. When two consecutive self-consistent calculations are performed, the energy difference does not exceed 10 −4 eV.

Preparation and Characterization of FeNi LDH/V 2 CT x /NF
The synthesis scheme of FeNi LDH/V 2 CT x /NF is shown in Figure 1a. First, the Al layer of massive V 2 AlC powder was removed by 40 wt% HF selective etching to prepare multilayer V 2 CT x . After TPAOH intercalation and ultrasonic dissection, V 2 CT x nanosheets with fewer layers and higher surface functional groups (−F, −OH) were obtained, which was beneficial to electrostatic adsorption on nickel foam and the nucleation and anchoring of FeNi LDH on V 2 CT x surface. Then, NF was immersed in V 2 CT x nanosheet suspension to obtain a V 2 CT x /NF electrode. After that, FeNi LDH nanosheets were hydrothermally deposited on V 2 CT x /NF substrate to obtain FeNi LDH/V 2 CT x /NF self-supported electrode. The XRD patterns of V 2 AlC and few-layer V 2 CT x are illustrated in Figure 1b. The peaks of 41.3 • and 13.5 • correspond with the (103) and (002) crystal planes of V 2 AlC, respectively (PDF#29−0101). The peaks at 41.3 • and 13.5 • disappear completely for the exfoliated few-layer V 2 CT x , and the characteristic peak (002) is reduced to 6.74 • , indicating that the Al atoms of few-layer V 2 CT x are completely removed, and the C-lattice parameters increase [33,43,44]. In addition, the full and magnification XRD of the FeNi LDH/V 2 CT x /NF peeled off the nickel foam are shown in Figure S1 and Figure 1c. The peaks of 2θ = 44.5 • , 51.9 • and 76.37 • correspond to the (111), (200), and (220) planes of Ni (PDF#04-0850). As shown in Figure 1c, the peaks at 2θ = 7.28 • coincided very well with (002) crystal planes of V 2 CT x , while the peaks at 2θ = 11.41 • , 22.974 • , 34.425 • , and 61.254 • were in good agreement with the (003), (006), (012) and (113) of the FeNi LDH (PDF#40-0215), respectively; these results showed that FeNi LDH/V 2 CT x /NF had been successfully prepared.
The pristine V 2 AlC powders present bulk-like shapes ( Figure S2) and unintercalated V 2 CT x exhibits an accordion-like morphology (Figure 1d and Figure S3). V 2 CT x nanosheets with a size of 200-300 nm and many edge defects were obtained by further intercalation and ultrasonic exfoliation of TPAOH ( Figure 1e). As shown in Figure S4, the clear Tyndall effect in the supernatant illustrates the uniformly dispersed layers of V 2 CT x . Because of the electrostatic interaction between the positively charged NF substrate and the negatively charged V 2 CT x surface, V 2 CT x is able to anchor to the 3D NF structure, with silver NF turning into black NF ( Figure S5). The low magnification SEM image of the FeNi LDH/V 2 CT x /NF sample can be seen in Figure 1g and the corresponding high magnification SEM image is shown in Figure 1h. The thickness of FeNi LDH nanosheets is about 8.03 nm ( Figure S6). FeNi LDH is evenly distributed over the surface of the V 2 CT x /NF substrate. As a comparison, FeNi LDH was grown directly on NF without V 2 CT x attached. It can be seen that FeNi LDH are clustered together (Figure 1f). The elemental mapping displays the welldistributed Fe, Ni, C and V elements in the FeNi LDH/V 2 CT x /NF ( Figure S7); moreover, the TEM image of peeling FeNi LDH/V 2 CT x from nickel foam ( Figure 1i) indicates loose flake texture grows on the surface of V 2 CT x with fewer layers and Figure 1j shows the interplanar spacing of 0.23 nm and 0.25 nm corresponding to (015) of FeNi LDH and the (100) of V 2 CT x , respectively. There are multiple diffraction rings on the (110) and (100) planes of V 2 CT x and the (015) plane of FeNi LDH in the regional electron diffraction image selected in Figure 1j. The even distribution of V, Ni, Fe, O and C in the FeNi LDH/V 2 CTx nanohybrid is observed in Figure 1k.   [45]. Similarly, in Fe 2p spectra (Figure 2c), peaks at 725.98 eV and 712.75 eV are due to 2p 1/2 and 2p 3/2 orbits of Fe 3+ , respectively [46]. In contrast, for FeNi LDH/V 2 CT x /NF samples, the positive displacement of the Ni 2p peak is 0.6-0.65 eV and the Fe 2p peak is 0.43 eV. The higher the binding energy is, the higher the oxidation state of Fe and Ni iron after V 2 CT x binding is. Specifically, the electron transfer from V 2 CT x to LDHs increased the valence states of Fe and Ni, suggesting that there is a strong chemical interaction between FeNi LDH and V 2 CT x . Figure 2d shows the V 2p spectra, the V 4+ of V 2 CT x corresponds to the V 2p 1/2 at 524.25 and V 2p 3/2 at 516.91 eV [47]. are due to 2p1/2 and 2p3/2 orbits of Fe 3+ , respectively [46]. In contrast, for FeNi LDH/V2CTx/NF samples, the positive displacement of the Ni 2p peak is 0.6-0.65 eV and the Fe 2p peak is 0.43 eV. The higher the binding energy is, the higher the oxidation state of Fe and Ni iron after V2CTx binding is. Specifically, the electron transfer from V2CTx to LDHs increased the valence states of Fe and Ni, suggesting that there is a strong chemical interaction between FeNi LDH and V2CTx. Figure 2d shows the V 2p spectra, the V 4+ of V2CTx corresponds to the V 2p1/2 at 524.25 and V 2p3/2 at 516.91 eV [47].

Electrochemical Characterization
The OER electrocatalytic property of the prepared electrocatalyst was evaluated in 1.0 M KOH electrolyte with O2-saturated. The activation process of FeNi LDH/V2CTx/NF electrocatalyst is shown in Figure S9. After 50 cycles of voltammetry, the electrocatalyst is transformed from hydroxide to oxyhydroxides. The redox peaks of the Ni(II)/Ni(III) are located at the potential range of 1.25-1.55 V (vs. RHE) [48], which was the strongest at 1.39 V potential. As seen in Figure 3a, FeNi LDH/V2CTx/NF electrocatalyst with a minimum
EIS was tested at −1.0 V (vs. RHE). The results (Figure 4d and Table S3) showed that FeNi LDH/V2CTx/NF had the lowest Rct (Rct = 10.85 Ω) of all electrocatalysts, indicating good reaction kinetics and faster charge transfer. The CV curves were obtained between 0.123 to 0.223 V (vs RHE) to estimate the ECSA of all electrocatalysts ( Figure S13). FeNi LDH/V2CTx/NF measured much higher Cdl (0.88 mF cm −2 ) than FeNi LDH/NF (0.83 mF  Figure 3d shows the elliptic semicircle of the EIS diagram, in which the sharp reduction of the semicircle diameter in the high-frequency region demonstrates the acceleration of charge transfer. The FeNi LDH/V 2 CT x /NF electrocatalyst has the lowest charge transfer impedance (R ct = 3.614 Ω) than that of Ni(OH) 2 /V 2 CT x /NF (R ct = 42.270 Ω) and FeNi LDH/NF (R ct = 4.275 Ω) electrocatalyst according to Table S2. The electrochemically active surface areas (ECSAs) were estimated from the C dl by cyclic voltammetry at 1.02-1.10 V (vs. RHE), as it is linear with ECSA ( Figure S10). As shown in Figure 3e, the C dl value of FeNi LDH/V 2 CT x /NF is 8.09 mF cm −2 , which is larger than those of FeNi LDH/NF (7.28 mF cm −2 ), Ni(OH) 2 /V 2 CT x /NF (4.8 mF cm −2 ) and V 2 CT x /NF (3.79 mF cm −2 ). Figure 3f shows the stability measurements of FeNi LDH/V 2 CT x /NF for η = 10 mA cm −2 at 0.222 V. The current density of FeNi LDH/V 2 CT x /NF did not decrease significantly after 10 h. After a 10h OER test, the morphology of FeNi LDH/V 2 CT x /NF has not changed significantly ( Figure S11), which further confirms its high stability. In addition, XPS measurements of FeNi LDH/V 2 CT x /NF were performed ( Figure S12). From the high-resolution Ni 2p spectra and Fe 2p spectra ( Figure S11a,b), it can be seen that the characteristic peaks of both Ni 2p and Fe 2p have a slight rise. The former indicates that Ni 2+ is oxidized to Ni 3+ , and the latter indicates that Fe is also partially oxidized, which is beneficial to accelerate the redox activity in the OER process; moreover, the two peaks of the V 2p spectrum ( Figure S11c) are still located at 516.91 eV (V 2p 3/2 ) and 524.25 eV (V 2p 1/2 ), corresponding to the V 4+ state, indicating its good stability during the OER.
To further explore the HER activity, FeNi LDH/V 2 CT x /NF with 1 × 1 cm 2 was served as the working electrode, while Pt plate, Hg/HgO (1 M KOH) and 1 M KOH were used as the counter electrode, reference electrode and electrolyte, respectively. The overpotential of FeNi LDH/V 2 CT x /NF at a current density of 10 mA cm −2 is 151 mV (η 10 = 151 mV), which is smaller than that of FeNi LDH/NF (η 10 = 198 mV), Ni(OH) 2 LDH/V 2 CT x /NF (η 10 = 214 mV), V 2 CT x /NF (η 10 = 252 mV) and NF (η 10 = 305 mV), except for Pt/C/NF (η 10 = 81 mV) (Figure 4a). As seen from Figure 4b, FeNi LDH/V 2 CT x /NF electrocatalyst achieves a current density of 50 mA cm −2 with the lowest overpotential of 274 mV; moreover, the Tafel slope of the FeNi LDH/V 2 CT x /NF was 136 mV/dec, which was lower than that of FeNi LDH/NF (148 mV dec −1 ), Ni(OH) 2 LDH/V 2 CT x /NF (152 mV dec −1 ) and V 2 CT x /NF (173 mV dec −1 ) (Figure 4c), further confirmed the internal reaction kinetics of the prepared FeNi LDH/V 2 CT x /NF significantly accelerated.  Based on the results, the FeNi LDH/V2CTx/NF electrode can be used as a robust and efficient electrocatalyst for OER and HER. Therefore, the FeNi LDH/V2CTx/NF electrode was used as both cathode and anode in 1.0 M KOH for overall water splitting. It can be seen from Figure 5a that when the current density is 50 mA cm −2 , it is easy to achieve a voltage of 1.74 V (η50 = 1.74V), which is small than FeNi LDH/NF (η50 = 1.81 V), Ni(OH)2 LDH/V2CTx/NF (η50 = 1.87 V) and V2CTx/NF (η50 = 1.92 V) ( Figure 5b); moreover, FeNi LDH/V2CTx/NF has a superiority compared with other electrocatalysts prepared by the one-step hydrothermal method in the literature (Table S4), such as NiFe LDH/NiCoP/NF (1.75 V) [14], NiCo2S4@NiFe-LDH/NF (1.83 V) [51] and NiCo-LDH/NF (1.86 V) [52]. As can be seen from the LSV curve before and after 24 h of the overall water splitting test (Figure  5c), the performance of the electrocatalyst is relatively stable and the overpotential changes little at 10 mA cm −2 . Besides, the overall water splitting can be continued for 24 h  Table S3) showed that FeNi LDH/V 2 CT x /NF had the lowest R ct (R ct = 10.85 Ω) of all electrocatalysts, indicating good reaction kinetics and faster charge transfer. The CV curves were obtained between 0.123 to 0.223 V (vs RHE) to estimate the ECSA of all electrocatalysts ( Figure S13). FeNi LDH/V 2 CT x /NF measured much higher C dl (0.88 mF cm −2 ) than FeNi LDH/NF (0.83 mF cm −2 ), Ni(OH) 2 LDH/V 2 CT x /NF (0.84 mF cm −2 ), V 2 CT x /NF (0.77 mF cm −2 ) and NF (0.56 mF cm −2 ) (Figure 4e). As shown in Figure 4f, the FeNi LDH/V 2 CT x /NF electrocatalyst maintained excellent catalytic performance and showed better durability in alkaline solution after a 10 h cycling test at −10 mA cm −2 . As seen in Figure S14, the morphology of the electrocatalyst was well maintained after HER testing, indicating its good mechanical stability. Besides, Figure S15 shows the XPS spectra of Ni 2p, Fe 2p and V 2p in the FeNi LDH/V 2 CT x /NF before and after the durability test. No significant changes were observed, indicating high electrochemical stability.
Based on the results, the FeNi LDH/V 2 CT x /NF electrode can be used as a robust and efficient electrocatalyst for OER and HER. Therefore, the FeNi LDH/V 2 CT x /NF electrode was used as both cathode and anode in 1.0 M KOH for overall water splitting. It can be seen from Figure 5a that when the current density is 50 mA cm −2 , it is easy to achieve a voltage of 1.74 V (η 50 = 1.74V), which is small than FeNi LDH/NF (η 50 = 1.81 V), Ni(OH) 2 LDH/V 2 CT x /NF (η 50 = 1.87 V) and V 2 CT x /NF (η 50 = 1.92 V) ( Figure 5b); moreover, FeNi LDH/V 2 CT x /NF has a superiority compared with other electrocatalysts prepared by the one-step hydrothermal method in the literature (Table S4), such as NiFe LDH/NiCoP/NF (1.75 V) [14], NiCo 2 S 4 @NiFe-LDH/NF (1.83 V) [51] and NiCo-LDH/NF (1.86 V) [52]. As can be seen from the LSV curve before and after 24 h of the overall water splitting test (Figure 5c), the performance of the electrocatalyst is relatively stable and the overpotential changes little at 10 mA cm −2 . Besides, the overall water splitting can be continued for 24 h steadily at 50 mA cm −2 (Figure 5d) and the O 2 and H 2 bubbles can be clearly observed (the inset of Figure 5d).

Mechanism Analysis
To further understand the interaction of FeNi LDH and V 2 CT x , the first-principles calculation was performed based on the DFT method ( Figure 6). The side and top view of model structure of FeNi LDH/V 2 CT x composite after structural relaxation are shown in Figure 6a and Figure S16. Figure 6b shows differential charge density in FeNi LDH/V 2 CT x composite study the charge redistribution by subtracting the charge densities of FeNi LDH and V 2 CT x slabs from the total charge density of the structure, which the light blue and yellow colors mean electron loss and electron gain, respectively. After V 2 CT x is introduced, because V 2 CT x has stronger electronegativity than FeNi LDH, electrons are transferred from FeNi LDH to V 2 CT x . The bader quantitative analysis shows that the amount of electron transfer from FeNi LDH to V 2 CT x is 0.44 eper unit cell, which may be due to the high electronegativity of V 2 CT x , which is easy to attract electrons from transition metal.
The project density of states (PDOS) and density of states (DOS) of FeNi LDH and FeNi LDH/V 2 CT x are shown in Figure 6c,d. As exhibited in Figure 6c, compared with FeNi LDH, the electron density of FeNi LDH/V 2 CT x near the Fermi level performs increased DOS and charge transfer, which is conducive to the adsorption-desorption performance of the reaction intermediates. Therefore, the conductivity of the electrocatalyst is improved and the energy barrier of OER is reduced [53,54]. As can be seen from Figure 6d, the PDOS of FeNi LDH/V 2 CT x is further away from the Fermi energy level than that of FeNi LDH, where the D-band centers of FeNi LDH/V 2 CT x and FeNi LDH are −2.96 eV and −2.77 eV, respectively. DFT simulations combined with experiments show that the increased activity is due to a modest downshift in the E d level, which regulates the desorption and adsorption capacities of the intermediates according to D-band center theory [55,56]. Therefore, the balance between intrinsic activity adsorption capacity of electrocatalyst to intermediate should be considered. As illustrated in Figure 6e, FeNi LDH/V 2 CT x shows an excellent electrocatalytic performance because of the increase of active sites and electrical conductivity.

Mechanism Analysis
To further understand the interaction of FeNi LDH and V2CTx, the first-principles calculation was performed based on the DFT method ( Figure 6). The side and top view of model structure of FeNi LDH/V2CTx composite after structural relaxation are shown in Figures 6a and S16. Figure 6b shows differential charge density in FeNi LDH/V2CTx composite study the charge redistribution by subtracting the charge densities of FeNi LDH and V2CTx slabs from the total charge density of the structure, which the light blue and yellow colors mean electron loss and electron gain, respectively. After V2CTx is introduced, because V2CTx has stronger electronegativity than FeNi LDH, electrons are transferred from FeNi LDH to V2CTx. The bader quantitative analysis shows that the amount of electron transfer from FeNi LDH to V2CTx is 0.44 eper unit cell, which may be due to the high electronegativity of V2CTx, which is easy to attract electrons from transition metal.
The project density of states (PDOS) and density of states (DOS) of FeNi LDH and FeNi LDH/V2CTx are shown in Figure 6c,d. As exhibited in Figure 6c, compared with FeNi LDH, the electron density of FeNi LDH/V2CTx near the Fermi level performs increased DOS and charge transfer, which is conducive to the adsorption-desorption performance −2.77 eV, respectively. DFT simulations combined with experiments show that the increased activity is due to a modest downshift in the Ed level, which regulates the desorption and adsorption capacities of the intermediates according to D-band center theory [55,56]. Therefore, the balance between intrinsic activity adsorption capacity of electrocatalyst to intermediate should be considered. As illustrated in Figure 6e, FeNi LDH/V2CTx shows an excellent electrocatalytic performance because of the increase of active sites and electrical conductivity.

Conclusions
In summary, through a simple one-step hydrothermal method, a self-supported bifunctional FeNi LDH/V 2 CT x /NF electrode has been successfully prepared. The presence of V 2 CT x promoted the dispersed growth of FeNi LDH nanosheets onto V 2 CT x /NF working electrode and reduced the obstacle of electron transfer. The NF scaffold provides a highly exposed active surface and facilitates the electrolyte infiltration and gas dissipation during OER. As a result, the overpotential of 222 mV and 151 mV of FeNi LDH/V 2 CT x /NF electrode at 10 mA cm −2 for the OER and the HER, respectively, proved an excellent electrocatalytic property. Besides, FeNi LDH/V 2 CT x /NF has a superiority (1.74 V) for overall water splitting at 50 mA cm −2 compared with other electrocatalysts prepared by one-step hydrothermal method in the literature; moreover, the current density of OER, HER and overall water splitting could remain almost the same after 10, 10 and 24 h test, underscoring the fundamentally improved of our bifunctional electrocatalysts.