Chen Liu,
Han Zhu*,
Shuanglong Lu,
Fangping Xu,
Fang Duan and
Mingliang Du*
Key Laboratory of Synthetic and Biological Colloids, Ministry of Education, School of Chemical and Material Engineering, Jiangnan University, Wuxi 214122, P. R. China. E-mail: zhysw@jiangnan.edu.cn; du@jiangnan.edu.cn
First published on 1st June 2021
Developing advanced electrocatalysts with low cost for electrocatalytic water splitting are highly desirable. Herein, we report the design of two-dimension on two-dimension growth of hierarchical Ni0.2Mo0.8N nanosheets on Fe-doped Ni3N nanosheets supported on Ni foam (Ni0.2Mo0.8N/Fe–Ni3N/NF) via hydrothermal reaction and nitridation treatment. In the hierarchical structures, small Ni0.2Mo0.8N nanosheets were uniformly anchored on Fe–Ni3N nanosheets. Due to enhanced electron transfer between Ni0.2Mo0.8N and Fe–Ni3N, Ni0.2Mo0.8N/Fe–Ni3N/NF exhibits superior electrocatalytic activity for the oxygen evolution reaction (OER) and the hydrogen evolution reaction (HER). After stability tests for 50 h, Ni0.2Mo0.8N/Fe–Ni3N/NF exhibits negligible degradation of the current density for the OER (91% remain) and HER (95% remain), suggesting excellent stability. Owing to the outstanding performance, Ni0.2Mo0.8N/Fe–Ni3N/NF display a cell voltage of 1.54 V (10 mA cm−2) for electrocatalytic overall water splitting.
Nowadays, transition metal-based materials19–21 including the chalcogenides,22–24 phosphides,25–27 nitrides,28–30 carbides31–33 and selenides34–36 have been extensively applied for electrocatalysis. Among of these electrocatalysts, transition metal nitrides (TMNs) are the new emerging alternative electrocatalyst for water splitting due to the high electrical conductivity and corrosion-resistance.37–39 However, amounts of electrocatalysts with highly performance are only suitable for OER or HER. Therefore, developing outstanding bifunctional electrocatalysts with excellent activity for OER and HER is crucial. Integrating multiple metal into one integrated material provide a powerful way to turn the electronic structure, further improving the OER and HER activity.40–43
Herein, we reported the design of two-dimension on two-dimension growth of hierarchical Ni0.2Mo0.8N nanosheets on Fe-doped Ni3N nanosheets supported on Ni foam (Ni0.2Mo0.8N/Fe–Ni3N/NF). In the hierarchical structures, small Ni0.2Mo0.8N nanosheets were homogenously distributed on Fe–Ni3N nanosheets. The Ni0.2Mo0.8N/Fe–Ni3N/NF exhibits lowest OER overpotential of 266 mV (20 mA cm−2), compared with the Fe–Ni3N/NF (292 mV), Ni0.2Mo0.8N/NF (320 mV) and commercial RuO2 (328 mV). The Ni0.2Mo0.8N/Fe–Ni3N/NF shows negligible degradation of the current density (91%) after OER stability test for 50 h. In addition, the Ni0.2Mo0.8N/Fe–Ni3N/NF also displays the lower overpotential (40 mV, 20 mA cm−2) and excellent durability (50 h, 95% current density remain). The Ni0.2Mo0.8N/Fe–Ni3N/NF shows a quite low cell voltage of 1.54 V (10 mA cm−2) for overall water splitting.
The dry NiMoO4/NF was placed at furnace and treated in a flow of 20 standard cubic centimeters (sccm) NH3 and 130 sccm Ar. The NiMoO4/NF kept at 500 °C for 1 h (5 °C min−1). Ni0.2Mo0.8N/NF was obtained after the treatment.
The linear sweep voltammogram (LSV) for OER was measured in a potential range of 1.0 to 1.6 V versus RHE (vs. RHE). For HER measurements, the LSV was measured in a potential range of and 0 to −0.5 V vs. RHE. The scan rate is 1 mV s−1. OER and HER curves of were treated by iR correction. According to the equation: Ecorrected = Euncorrected − iRs, the curve of iR correction would be finished. Rs (solution resistance) was able to observed by the electrochemical impedance spectroscopy (EIS) tests. The EIS for OER and HER was tested at 1.47 V and −0.03 V vs. RHE from 10 kHz to 0.01 Hz with a 10 mV AC amplitude. The stability test for OER was operated at 1.515 V vs. RHE for 50 h. The stability test for HER was finished at −74 mV vs. RHE for 50 h. The double-layer capacitance (Cdl) was obtained by the CVs cycling tests from 0.1 to 0.2 V vs. RHE with scan rates ranged from 10–60 mV s−1. Cdl can be used to calculate the electrochemically active surface area (ECSA). Overall water splitting was measured in a two-electrode electrolyzer. The LSV was measured in a potential range of 1.0 to 1.9 V voltage. The stability test of overall water-splitting was operated at 1.59 V voltage for 20 h.
Fig. 1 FE-SEM images of (a–c) Fe–Ni(OH)2/NF, (d–f) Fe–Ni3N/NF, (g–i) Ni0.2Mo0.8N/NF and (j–l) Ni0.2Mo0.8N/Fe–Ni3N/NF at different magnifications. |
The diameters of the Ni0.2Mo0.8N nanowires ranged from 80 to 200 nm (Fig. S1†). When NiMoO4 meets Fe–Ni(OH)2 (Fig. S2d–f†), the as-synthesized NiMoO4/Fe–Ni(OH)2/NF exhibited a hierarchical structure consist of Fe–Ni(OH)2 as substrates and NiMoO4 vertically grown on Fe–Ni(OH)2 nanosheets. Through the NH3 treatment at 500 °C, the NiMoO4/Fe–Ni(OH)2/NF were converted into Ni0.2Mo0.8N/Fe–Ni3N/NF (Fig. 1j–l) with two unique phases. The Fe–Ni3N nanosheets were coated by small Ni0.2Mo0.8N nanosheets. It is interesting that with the Ni0.2Mo0.8N, the Fe–Ni3N substrates still remain the morphology of NiMoO4/Fe–Ni(OH)2. The thickness of Ni0.2Mo0.8N/Fe–Ni3N/NF ranged from 210–350 nm (Fig. S3a and b†), while the thickness range of small nanosheet is 7–15 nm (Fig. S3c and d†). Different from the individual Fe–Ni3N (Fig. 1d–f), Fe–Ni3N substrates were not also transformed into the similar structure. The small Ni0.2Mo0.8N nanosheets could hinder the collapse of Fe–Ni3N from nanosheets to interconnected nanospheres. The unique structure of Ni0.2Mo0.8N/Fe–Ni3N/NF may be provide more active sites for electrocatalysis.
The crystal structures of materials were investigated by the XRD characterization. Fig. 2a and S4† show the sharp peaks near the 44.5°, 51.8° and 76.4°, corresponding to the metal Ni in the NF. The peaks of Fe–Ni(OH)2/NF were observed at 33.5°, 34.4° and 38.8° (Fig. S4†), indicating the formation of Ni(OH)2 phase (JCPDS 38-0715). The peaks at 38.9°, 42.1°, 58.5°, 70.6° and 78.4° of Fe–Ni3N/NF (Fig. 2a) were assigned to Ni3N phases (JCPDS 10-0280), indicating that the Ni(OH)2/NF were transformed to Fe–Ni3N phases after NH3 treatment. The visible diffraction peaks of Ni0.2Mo0.8N/NF at 32.2°, 36.5° and 49.4° belong to the crystal planes of Ni0.2Mo0.8N (JCPDS 29-0931). For the Ni0.2Mo0.8N/Fe–Ni3N/NF, the peaks for Ni3N phases were very weak due to the low crystallinity, while the peaks for Ni0.2Mo0.8N phases are strong. The HRTEM image of Fe–Ni3N/NF reveals a lattice fringe (0.20 nm) (Fig. S5a and b†), corresponding to the (100) plane of Ni3N. The TEM image of Ni0.2Mo0.8N/Fe–Ni3N/NF (Fig. S5c†) indicates that small Ni0.2Mo0.8N nanosheets were uniformly dispersed on Fe–Ni3N/NF nanosheets. Fig. 2b shows the HRTEM image of Ni0.2Mo0.8N/Fe–Ni3N/NF. The (100) and (101) planes of Ni0.2Mo0.8N was observed. Furthermore, the (002) plane (the interplanar distance of 0.21 nm) of Ni3N was observed in Fig. 2b. There were no peaks of metal Fe or Fe oxides and nitrides in the measured XRD patterns and HRTEM images, indicating that the Fe elements were doped into the Ni(OH)2 and the Ni3N crystal matrix.44–46 The STEM-EDS mapping images of Ni0.2Mo0.8N/Fe–Ni3N/NF were represented in Fig. 2c. As shown in new Fig. 2c, the Ni, Mo, Fe and N were uniformly distributed throughout the randomly examined Ni0.2Mo0.8N/Fe–Ni3N nanosheets. The Fe, Ni and N elements can be visible observed as substrates while the Ni, Mo and N elements also distributed as spots. The results confirmed the formation of hierarchical structures of Ni0.2Mo0.8N/Fe–Ni3N/NF using Fe–Ni3N as support.
Fig. 2 (a) XRD patterns of Ni0.2Mo0.8N/Fe–Ni3N/NF, Ni0.2Mo0.8N/NF and Fe–Ni3N/NF. (b) HRTEM image of Ni0.2Mo0.8N/Fe–Ni3N/NF. (c) STEM-EDS mapping images of Ni0.2Mo0.8N/Fe–Ni3N/NF. |
XPS spectra were shown in Fig. S6† and 3 to research the chemical compositions and surface chemical states of materials. Fig. S6† is the XPS survey of Ni0.2Mo0.8N/Fe–Ni3N/NF, indicating that the Ni, Fe, Mo and N were observed. In Fig. 3a, the two peaks of the Ni0.2Mo0.8N/Fe–Ni3N/NF at 852.6 and 870.2 eV belong to the Ni species in Ni–N bonds.47–49 Furthermore, the peaks located at 855.6, 873.5 eV and 857.1, 876.3 eV correspond to the oxidized Ni2+ and Ni3+ species, while the remaining two peaks (880.1 and 861.8 eV) belong to satellite peaks.50,51 Compared with the BE of Ni0.2Mo0.8N/NF, the binding energy (BE) values of Ni–N bond of Ni0.2Mo0.8N/Fe–Ni3N/NF shifts negatively by about 0.2 eV (Fig. 3a). The difference in BEs of the Ni–N bond between the Ni0.2Mo0.8N/Fe–Ni3N/NF and Fe–Ni3N/NF might be attributed to the electron interaction between the Fe–Ni3N nanosheets and Ni0.2Mo0.8N nanosheets or the interaction with underlying NF substrates.
The BEs shift in Mo 3d suggests the strong electron transfer from the Ni0.2Mo0.8N to Fe–N3N, leading to the strong interaction between the two phases. Fig. 3d shows the N 1s XPS spectra Ni0.2Mo0.8N/Fe–Ni3N/NF, the peak at about 397.1 eV corresponds to the N species of transition metal–N bonds, while the peak at about 395.2 eV was attributed to Mo–N bonds.53 The peak at 398.2 eV belongs to the N–H species on the surface of materials.54 Fig. 3e and f represented the N 1s XPS spectra of Ni0.2Mo0.8N/NF and Fe–Ni3N/NF. By analyzing the peak in Fig. 3d and f, the negative shift in BEs of the Ni0.2Mo0.8N/Fe–Ni3N/NF was observed. The changes in BEs of N 1s of Ni0.2Mo0.8N/Fe–Ni3N/NF suggests that the Fe–Ni3N integrated with Ni0.2Mo0.8N can lead to the enhanced charge transfers and electron interactions.
The OER performance of samples was examined. As shown in Fig. 4a and b, the Ni0.2Mo0.8N/Fe–Ni3N/NF displays the overpotential of 266 mV to acquire 20 mA cm−2. The overpotentials of Ni0.2Mo0.8N/NF (320 mV), Fe–Ni3N/NF (292 mV) and commercial RuO2 (328 mV) are higher than those of the Ni0.2Mo0.8N/Fe–Ni3N/NF. Fig. 4c shows the Tafel slopes of electrocatalysts. The Ni0.2Mo0.8N/Fe–Ni3N/NF had the lowest Tafel slopes (54 mV dec−1), indicating the best OER performance than those of the Fe–Ni3N/NF, Ni0.2Mo0.8N/NF and commercial RuO2, respectively. In addition, the performances of Ni0.2Mo0.8N/Fe–Ni3N/NF was superior to those of recently reported OER catalysts (Table S1†).
EIS measurements were performed to analyze the OER electrode kinetics. In the Nyquist plots (Fig. 4d), the Ni0.2Mo0.8N/Fe–Ni3N/NF reveals a small charge transfer resistance (Rct) of 4.4 Ω. The Rct of Fe–Ni3N/NF and Ni0.2Mo0.8N/NF is 10.6 Ω and 26.9 Ω, respectively. The relatively lower Tafel slope and Rct suggests the fast kinetics process of Ni0.2Mo0.8N/Fe–Ni3N/NF. The combination of Fe–Ni3N and Ni0.2Mo0.8N nanosheets lead to the superior OER activity.
The stability test was carried out by chronopotentiometry measurement to investigate the changes of the Ni0.2Mo0.8N/Fe–Ni3N/NF catalyst after prolonged water electrolysis. Fig. 4e shows the current–time curves of OER chronopotentiometry test. The current density of Ni0.2Mo0.8N/Fe–Ni3N/NF still retain 91% after continuous electrolysis for 50 h, and FE-SEM image of Ni0.2Mo0.8N/Fe–Ni3N/NF demonstrates that the hierarchical and two-dimensional features of the Ni0.2Mo0.8N/Fe–Ni3N/NF remain unchanged after the stability test. As displayed in Fig. 4f, the LSV curves before and after cycle tests also exhibit negligible decrease in current density, suggesting the excellent stability in alkaline condition.
The XRD patterns, XPS survey and XPS spectra of the Ni0.2Mo0.8N/Fe–Ni3N/NF after OER and HER stability test was shown in Fig. S6–S10† and 5. As shown in Fig. S7 and S9,† the diffraction peaks for Ni0.2Mo0.8N (JCPDS 29-0931) both become weaker after the HER and OER stability test, respectively. The XPS survey and XPS spectra of Ni0.2Mo0.8N/Fe–Ni3N/NF after OER and HER all indicate the existences of Ni, Mo, Fe and N elements. The chemical states display small changes, suggesting the superior stability of main structures. The N 1s XPS changes after the HER and OER suggests the surface oxidation of Ni0.2Mo0.8N and the formation of metal-oxyhydroxide or metal-hydroxide. In Fig. 5a, the Ni 2p XPS spectra after stability tests show the BEs of Ni3+ (874.5 and 856.8 eV) and Ni2+ (872.9 and 855.4 eV).50 In the Fe 2p XPS spectra (Fig. 5b), the peaks of Fe3+ (725.5 and 713.0 eV), Fe2+ (722.3 and 709.7 eV) and satellite can be observed.55 Fig. 5c and d represent the Mo 3d and N 1s spectra after OER test. The peaks of Mo6+ 235.0 and Mo4+ (233.8 and 230.1 eV), Mo3+ (233.0 and 229.0 eV) and N–H bond (399.4 eV), metal–N bond (397.9 eV), Mo–N bond (394.3 eV) can still be observed.38,49 The chemical states of elements exhibit changes after the OER stability tests, suggesting that the surface of electrocatalyst might be transformed into the metal-oxyhydroxide or metal-hydroxide.48
Fig. 5 (a) Ni 2p, (b) Fe 2p, (c) Mo 3d and (d) N 1s XPS spectra of Ni0.2Mo0.8N/Fe–Ni3N/NF after OER stability test for 50 h. |
The electrochemical performance of as-synthesized materials toward HER has also been performed. As shown in Fig. 6a and b, the Ni0.2Mo0.8N/Fe–Ni3N/NF displays the best HER activity (40 mV, 20 mA cm−2), which is lower than other electrocatalysts. In addition, the Ni0.2Mo0.8N/Fe–Ni3N/NF also obtains the lowest Tafel slope of 51 mV dec−1 (Fig. 6c). The Nyquist plots under HER condition were shown in Fig. 6d. The Ni0.2Mo0.8N/Fe–Ni3N/NF displays a smaller charge-transfer resistance (Rct), indicating that the Ni0.2Mo0.8N/Fe–Ni3N/NF exhibits enhanced charge-transfer ability. The outstanding charge-transfer ability of electrocatalysts for HER lead to favorable electrocatalytic kinetics. Some recently reported HER electrocatalyst was summarized in Table S2,† the overpotential of Ni0.2Mo0.8N/Fe–Ni3N/NF can be comparable. It is noted that the outstanding HER performance of Ni0.2Mo0.8N/Fe–Ni3N/NF could be ascribed to the strong interactions between Fe–Ni3N and Ni0.2Mo0.8N/NF phases.
The durability of Ni0.2Mo0.8N/Fe–Ni3N/NF toward HER was tested at a potential of 74 mV vs. RHE. After HER chronopotentiometry test for 50 h, FE-SEM image (Fig. 6e) shows that the hierarchical and two-dimensional features of the Ni0.2Mo0.8N/Fe–Ni3N/NF remain the same after the HER stability test. The current density of Ni0.2Mo0.8N/Fe–Ni3N/NF retain 95% (Fig. 6e). The LSV curves (Fig. 6f) of Ni0.2Mo0.8N/Fe–Ni3N/NF after HER stability tests both show slight difference, suggesting the excellent stability for HER in alkaline condition.
The peak for Ni0.2Mo0.8N phases can be observed from the Fig. S9.† In XPS survey, the signal of N was observed (Fig. S10†). By analyzing the Fig. 7a, the peaks of Ni3+ (875.5 and 856.4 eV), Ni2+ (873.1 and 855.4 eV) and Ni–N bonds (870.0 and 852.6 eV) can be observed.45 For the Fe 2p XPS spectra (Fig. 7b), the peaks of Fe3+ (723.9 and 711.8 eV) and Fe0 (720.6 and 706.6 eV) still exist.52 Furthermore, Mo 3d (Fig. 7c) and N 1s (Fig. 7d) XPS spectra still show the existence of Mo6+, Mo4+, Mo3+ and N–H, metal–N, Mo–N.49 XRD pattern and XPS spectra indicated that the chemical compositions of sample were almost unchanged, revealing the superior stability of Ni0.2Mo0.8N/Fe–Ni3N/NF in HER process.
Fig. 7 (a) Ni 2p, (b) Fe 2p, (c) Mo 3d and (d) N 1s XPS spectra of Ni0.2Mo0.8N/Fe–Ni3N/NF after HER stability test for 50 h. |
The ECSA of various electrocatalysts were roughly obtained by the Cdl. The Cdl were measured through CVs (Fig. S11†). In Fig. 8a, the Cdl of the Ni0.2Mo0.8N/Fe–Ni3N/NF, Fe–Ni3N/NF and Ni0.2Mo0.8N/NF were 129, 11 and 70 mF cm−2, respectively. The ECSA of the Ni0.2Mo0.8N/Fe–Ni3N/NF, Fe–Ni3N/NF and Ni0.2Mo0.8N/NF was 1612.5 cm2, 137.5 cm2 and 875.0 cm2, respectively. The bigger Cdl and ECSA of Ni0.2Mo0.8N/Fe–Ni3N/NF demonstrates that the integration of the small Ni0.2Mo0.8N nanosheets on Fe–Ni3N nanosheets can expose abundant catalytically active site.
Considering the excellent performance of OER and HER and practical applications of the material, Ni0.2Mo0.8N/Fe–Ni3N/NF was used as the bifunctional electrocatalysts for overall waters splitting. Fig. 8b shows the overall water splitting polarization curves of electrocatalysts. The Ni0.2Mo0.8N/Fe–Ni3N/NF only requires a potential of 1.54 V to achieve a current density of 10 mA cm−2, which is much smaller than that of Fe–Ni3N/NF (1.67 V) and Ni0.2Mo0.8N/NF (1.59 V). Furthermore, the Ni0.2Mo0.8N/Fe–Ni3N/NF bifunctional electrocatalyst shows strong stability, which displayed small degradation after stability test for 20 h (Fig. 8c). The Ni0.2Mo0.8N/Fe–Ni3N/NF electrode after stability test only need 1.55 V (10 mA cm−2) (Fig. 8d), which further demonstrate its excellent durability.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra01299a |
This journal is © The Royal Society of Chemistry 2021 |