Electrochemically exfoliated Ni-doped MoS2 nanosheets for highly efficient hydrogen evolution and Zn-H2O battery

Hao Wei Jincheng Si Libin Zeng Siliu Lyu Zhiguo Zhang Yange Suo Yang Hou

Citation:  Hao Wei, Jincheng Si, Libin Zeng, Siliu Lyu, Zhiguo Zhang, Yange Suo, Yang Hou. Electrochemically exfoliated Ni-doped MoS2 nanosheets for highly efficient hydrogen evolution and Zn-H2O battery[J]. Chinese Chemical Letters, 2023, 34(1): 107144. doi: 10.1016/j.cclet.2022.01.037 shu

Electrochemically exfoliated Ni-doped MoS2 nanosheets for highly efficient hydrogen evolution and Zn-H2O battery

English

  • With ever-increasing global energy needs and the intensification of environmental pollution, new renewable energy conversion technologies have been inevitably attracting much attention [1-5]. Electrochemical water splitting to generate green H2 is a sustainable and environmentally friendly strategy. As one of two half-cell reactions of water splitting, hydrogen evolution reaction (HER) is a key step and has been extensively studied in the last decades [6-10]. Noble metal catalysts, especially Pt-based materials, are still the most efficient electrocatalysts for HER [2, 11]. However, the high cost and scarcity of noble Pt catalyst greatly hinder their large-scale commercial applications. Thereupon, the development of low-cost and efficient catalysts for electrochemical water splitting is of great importance [12, 13].

    Recently, transition metal dichalcogenides (TMDs) materials have been regarded as promising alternatives for Pt-based catalysts due to their abundant exposed edge sites and excellent electron mobility along the nanosheets [13, 14]. Among them, molybdenum sulfide (MoS2) is one of the most promising TMDs candidates for HER because of its favorable electronic structure, good corrosion resistance, and high stability [14, 15]. Nevertheless, local exposed active sites and inherent poor conductivity largely suppress the HER performance of bulk-phase MoS2 [15-18]. Therefore, several strategies have been proposed to improve their catalytic performances. For up-to-down strategy, exfoliating bulk MoS2 into two-dimensional (2D) layer-like MoS2 nanosheets is an encouraging approach, which can obtain monolayer/few-layer MoS2 with large surface area as well as rich exposed active sites [18-20]. Unfortunately, due to the multistep synthesis reactions, the conventional exfoliation methods, such as mechanical exfoliation [21], liquid sonication exfoliation [22], and lithium-ion intercalation [23] are usually hard to control the number of layers and thickness of 2D nanosheets. Compared with these reported methods, electrochemical exfoliation route has attracted great interest owing to its simple procedure, high efficiency as well as good controllability, and it has been successfully applied to the exfoliation of most 2D materials, such as phosphorene, graphene, and WS2 [24]. Besides, transition metals doped TMDs materials can efficiently modulate hydrogen adsorption/desorption energy to enhance whole electrocatalytic activity [24-26]. Especially, the doping of Ni atoms could optimize the electronic structure of MoS2, regulate the electron density of Mo atom [26], which would reduce the free energy of hydrogen adsorption and boost catalytic performance. Therefore, it is desirable to develop an effective method for rapid exfoliation production of TMDs and in situ doping of transition metal to improve their HER performance. In this work, a usual 2D Ni-doped MoS2 (Ni-EX-MoS2) nanosheets was prepared through a one-step electrochemical exfoliation treatment of bulk MoS2 in a mixture electrolyte of N, N-dimethylformamide (DMF) and tetrabutylammonium bromide (TBAB). The obtained Ni-EX-MoS2 catalyst with a thickness of ~3.5 nm and a lateral dimension of ~500 nm, exhibited an excellent HER activity, featured by a low overpotential of 145 mV at 10 mA/cm2 and a small Tafel slope of 89 mV/dec in 1.0 mol/L KOH, which was ascribed to the formation of 2D 1T/2H-MoS2 heterojunction and doping of Ni species during the exfoliation process. Intriguingly, the Ni-EX-MoS2 could also be employed as a cathode electrode for alkaline Zn-H2O battery with a power density up to 3.3 mW/cm2 and good stability of ~6.0 h.

    A schematic diagram of the synthetic route for Ni-EX-MoS2 was presented in Fig. 1. Bulk MoS2 was firstly synthesized by a solid phase reaction in a sealed quartz tube by annealing a mixture of Mo and S powders. Then, as-prepared bulk MoS2 was used as cathode and underwent an electrochemical exfoliation at 5.0 V for 10 min with TBA+ (6 mg/mL) in NiCl2 6H2O (5 mg/mL)/DMF electrolyte to obtain Ni-EX-MoS2 nanosheets. The cathodic bulk MoS2 was polarized by the specific electric field and a negative charge was generated on the surface. The TBA+ and Ni2+ ions in the electrolyte could migrate to the bulk MoS2, and then the TBA+ ions intercalates into the interlayer of bulk MoS2, which causes the expansion of MoS2 interlayers. Meanwhile, the Ni2+ ions was intercalated into MoS2 interlayer, which was further trapped by the negatively charged exfoliated MoS2. A final product of Ni-EX-MoS2 nanosheets was subsequently collected by ultrasonic shaking, centrifugation, and freeze-drying steps. The operation details refer to the section of experimental synthesis and the main products are synthesized under these conditions, except for special markings.

    Figure 1

    Figure 1.  Schematic diagram of the electrochemical exfoliation and synthetic procedure.

    As shown in Fig. S1 (Supporting information), X-ray diffraction (XRD) patterns of bulk MoS2 and Ni-EX-MoS2 showed the main peak located at 14.2°, which was attributed to the (002) crystal plane of MoS2 crystal [27]. After the electrochemical exfoliation, the peak intensity on the (002) plane of Ni-EX-MoS2 was much weaker than that of bulk MoS2, which can be attributed to the thinner layered structure formed in the Ni-EX-MoS2 [20, 28]. No signal peaks of Ni-related species were detected. The morphologies of bulk MoS2 and Ni-EX-MoS2 were explored by field emission scanning electron microscopy (FESEM) images. As shown in Figs. 2a and b, few-layer Ni-EX-MoS2 nanosheets was successfully synthesized by the electrochemical exfoliation from original multilayered stacked bulk MoS2. Transmission electron microscopy (TEM) (Fig. 2c) and atomic force microscopy (AFM) images (Fig. 2d) showed that the Ni-EX-MoS2 nanosheets processed a lateral size of ~500 nm and a thickness of ~3.5 nm, corresponding to five layers stacked together (single-layer thickness of 0.62 nm for MoS2) [29, 30]. Atomic-resolution high-angle annular dark-field scanning TEM (HAADF-STEM) image in Fig. 2e revealed the flat surface of Ni-EX-MoS2 without obvious particles formed. Moreover, energy dispersive X-ray spectroscopy (EDX) mapping images displayed the homogenous distribution of Ni, Mo and S elements throughout the whole Ni-EX-MoS2 nanosheet structure (Fig. 2f), respectively. The content of Ni species in the Ni-EX-MoS2 catalyst was determined to be 4.8% by inductively coupled with plasma atomic emission spectroscopy (ICP-AES) analysis (Table S1 in Supporting information).

    Figure 2

    Figure 2.  SEM images of (a) bulk MoS2 and (b) Ni-EX-MoS2. (c) TEM image of Ni-EX-MoS2. (d) AFM image of Ni-EX-MoS2. (e) HAADF-STEM image of Ni-EX-MoS2. (f) EDX elemental mapping images of O, S, Ni and Mo in the corresponding region.

    Considering that the magnitude of voltage plays a key role in the electrochemical exfoliation process, the exfoliation quality and particle size of MoS2 nanosheets were furtherly explored at other applied voltages (3.0 and 10 V). At a voltage of 3.0 V, the MoS2 surface produced little negative electrical attraction to TBA+ ions, which made it difficult to intercalate into the interlayer of bulk MoS2, thus leading to poor exfoliation. As a result, the large-sized multilayer MoS2 sheets was obtained (Fig. S2a in Supporting information). In contrast, when the applied voltage was increased to 10 V, it resulted in a higher intercalation rate and the faster disruption of the van der Waals forces between bulk MoS2 layers, thus leading to the smaller crystal sizes for few-layer MoS2 nanosheets (Fig. S2b in Supporting information). Due to the moderate intercalation rate and amount of TBA+ ions into the MoS2 interlayer, the Ni-EX-MoS2 with high quality was obtained at the voltage of 5.0 V.

    Fig. 3a showed the enlarged HRTEM image of Ni-EX-MoS2 nanosheets. Unambiguously, it is observed the coexistence of 1T and 2H phases MoS2 in the plane (marked with red and yellow circles). The interplanar spacings of 0.27 and 0.27 nm in the yellow region can be attributed to the (010) and (100) crystal faces of 2H phase MoS2, respectively [19]. While the interplanar spacing of 0.27 nm in the red region could be assigned to the (101) crystal face of 1T phase MoS2 [31], which indicates that the original 2H-phase MoS2 was partially transformed into 1T-phase MoS2 after electrochemical exfoliation [29, 32]. Obviously, it can be identified the doped Ni atoms (marked with orange circles) and continuous lattice streaks of the 1T-2H phase within the section. As displayed in Fig. 3b, the diffraction rings in the selected area electron diffraction (SAED) for Ni-EX-MoS2 can be indexed to the (100), (110) and (103) facets of MoS2. Raman spectra was used to characterize the bulk MoS2 and Ni-EX-MoS2 catalysts (Fig. 3c), where the characteristic peaks located at 379.3 and 405.9 cm−1 are attributed to the in-plane (E2g1) and out-of-plane (A1g) modes of 2H phase MoS2 [33, 34]. In addition, several additional peaks appeared at 147.6 and 226.1 cm−1, corresponding to J1 and J2 vibrational modes of S-Mo-S bonds in 1T-phase MoS2 [19, 35]. These results demonstrated that the partial phase transformation occurred from the 2H-phase MoS2 to 1T-phase MoS2 after the electrochemical exfoliation.

    Figure 3

    Figure 3.  (a) HRTEM images Ni-EX-MoS2 nanosheets. Inset: red and yellow dots in the atomic arrangement of 1T and 2H phases represent for Mo and S atoms. (b) Corresponding SAED pattern. (c) Raman spectra of Ni-EX-MoS2 and bulk MoS2. High-resolution XPS spectra of (d) Mo 3d, (e) S 2p and (f) Ni 2p, respectively.

    To further explore the electronic structures of Ni-EX-MoS2, the measurements of X-ray photoelectron spectroscopy (XPS) were conducted. The full-survey XPS spectrum presented Ni, Mo, and S elements in the Ni-EX-MoS2 (Fig. S3 in Supporting information). In high-resolution Mo 3d XPS spectra (Fig. 3d), bulk MoS2 showed two peaks located at 232.4 and 229.3 eV, which corresponds to the characteristic Mo 3d5/2 and Mo 3d3/2 peaks of 2H phase MoS2, respectively [27, 36]. For the Ni-EX-MoS2, it showed three peaks centered at 235.1, 232.1, and 228.9 eV corresponding to the characteristic peaks of Mo6+, Mo 3d5/2, and Mo 3d3/2, respectively [36, 37]. The decrease in the binding energy was probably due to the shift of Fermi energy level, as additional electrons populated the d orbitals caused by the partial phase transition, as verified by the coexistence of 1T and 2H phases MoS2 heterojunction [38, 39]. In Fig. 3e, the high-resolution S 2p XPS spectra of the Ni-EX-MoS2 displayed two peaks located at 162.9 and 161.8 eV, which are assigned to the characteristic peaks of S 2p1/2 and S 2p3/2, respectively. Compared with the S 2p1/2 (163.3 eV) and S 2p3/2 (162.2 eV) peaks of bulk MoS2 with 2H phase, the corresponding peaks of Ni-EX-MoS2 decreased a 0.4 eV in binding energy, further demonstrating the formation of 1T phase MoS2 in the Ni-EX-MoS2 [38, 39]. A new characteristic peak in the sulfur oxidation state was found in Fig. 3e, which might be due to the oxidation of the Ni-EX-MoS2 when exposed to air during the XPS test [20]. The peaks located at 873.2 and 855.6 eV in Fig. 3f can be assigned to Ni 2p1/2 and Ni 2p3/2, respectively, in consistent well with the previous report [40]. Based on HRTEM, Raman, and XPS results, one can conclude that the rapid electrochemical exfoliation enables synchronous exfoliation of bulk MoS2 and incorporation of Ni species into Ni-EX-MoS2 nanosheets.

    The electrocatalytic HER activities of the Ni-EX-MoS2 were evaluated using a three-electrode cell in 1.0 mol/L KOH. All polarization curves were recorded with iR compensation. For comparison, the reference samples including bulk MoS2 and EX-MoS2 were also tested. As shown in Fig. 4a, commercial Pt/C exhibited the highest HER activity. In addition, the Ni-EX-MoS2 displayed the excellent HER performance with an overpotential as low as 145 mV at 10 mA/cm2, much lower than those of MoS2 (> 600 mV at 10 mA/cm2) and EX-MoS2 (425 mV at 10 mA/cm2), respectively. Furthermore, the Tafel slope of Ni-EX-MoS2 was measured to be 89 mV/dec, which was lower than those of EX-MoS2 (96 mV/dec) and MoS2 (121 mV/dec) (Fig. 4b), demonstrating excellent HER kinetic property [41].

    Figure 4

    Figure 4.  (a) Polarization curves of bulk MoS2, EX-MoS2, Ni-EX-MoS2, and Pt/C after iR-correction and (b) Tafel plots of bulk MoS2, EX-MoS2, Ni-EX-MoS2 and Pt/C in 1 mol/L KOH solution. (c) Nyquist plots of bulk MoS2, EX-MoS2, Ni-EX-MoS2. Inset: An equivalent circuit for fitting impedance data. (d) Comparison of overpotentials at 10 mA/cm2 and Tafel slopes with recently reported MoS2-based electrocatalysts. (e) Chronopotentiometry curve of Ni-EX-MoS2 without iR-correction. Inset: photograph for electrochemical stability at 10 mA/cm2. Inset: polarization curves of Ni-EX-MoS2 for the first and 1000th CV cycles.

    To further clarify the intrinsic activity of Ni-EX-MoS2, the electrochemically active surface areas (ECSA) of the catalysts were estimated by the electrochemical double-layer capacitance (Cdl, Figs. S4a–c in Supporting information). The Ni-EX-MoS2 showed the largest Cdl value of 3.78 mF/cm2 as compared to the EX-MoS2 (2.21 mF/cm2) and bulk MoS2 (1.11 mF/cm2), suggesting more exposed active sites in the Ni-EX-MoS2 (Fig. S4d in Supporting information). In addition, the tests of electrochemical impedance spectroscopy (EIS) showed that the charge-transfer resistance (Rct) value of Ni-EX-MoS2 was 101 Ω, which was smaller than that of EX-MoS2 (196 Ω) and bulk MoS2 (1022 Ω), respectively, indicating that the Ni-EX-MoS2 possessed a faster electron transfer capability (Fig. 4c and Table S2 in Supporting information). Notably, the as-prepared Ni-EX-MoS2 exhibited an outstanding HER catalytic activity with low Tafel slope and small overpotential, which was superior to most of previously reported MoS2-based HER electrocatalysts under alkaline conditions (Fig. 4d and Table S3 in Supporting information).

    Fig. S5a (Supporting information) showed a multicurrent step curve for the Ni-EX-MoS2 with the current densities being cumulative from 5.0 mA/cm2 to 25 mA/cm2. Likewise, the corresponding multipotential step curve of Ni-EX-MoS2 was also displayed in Fig. S5b in Supporting information. All other steps showed the same trends, which presented the outstanding mass transport property and superior mechanical robustness of Ni-EX-MoS2 [42]. Further durability tests showed that Ni-EX-MoS2 had excellent stability in alkaline media, with negligible potential drop after 8 h of continuous HER process (Fig. 4e). This conclusion was further supported by inset of Fig. 4e, no obvious change in the polarization curves of Ni-EX-MoS2 before and after 1000 cycles was observed.

    To clarify the HER mechanism of Ni-EX-MoS2, a series of experiments and analyses were carried out. Firstly, we used the thiocyanate ions (SCN), which is considered as a toxic effect on Ni species, to reveal the real active site of Ni-EX-MoS2. It is evident that after the addition of SCN ions, the current density of Ni-EX-MoS2 suddenly decreased and the potential dropped from 0.18 V to 0.35 V (Fig. S6 in Supporting information), demonstrating the effective blocking of active Ni sites. Besides, the high-resolution XPS spectra of Ni 2p, Mo 3d and S 2p on the Ni-EX-MoS2 before and after HER tests were compared (Fig. S7 in Supporting information). In the high-resolution XPS spectrum of Ni 2p, the binding energy of Ni 2p was significantly increased after HER catalysis, indicating a higher valence state of Ni species in the Ni-EX-MoS2 [43, 44]. Further, the Ni-EX-MoS2 showed a positive shift of 0.5 eV of Ni 2p peak during the HER process, which can be attributed to the electrons transferred from the Ni center to the adjacent H2 molecules [45, 46]. These results revealed that the Ni species in the Ni-EX-MoS2 was acted as the main active center for HER. The post-TEM and post-HRTEM characterizations demonstrated that the lamellar structures and lattice stripes were almost unchanged after the HER reaction (Figs. S8a–c in Supporting information). The presence of uniformly distributed Ni species (Fig. S8d in Supporting information) and the coexistence of 1T and 2H phases of MoS2 (Fig. S8b) on the base of Ni-EX-MoS2 demonstrated its strong durability.

    Moreover, in order to verify the general applicability of this electrochemical exfoliation strategy, the different kinds of TMDs materials induced by doping of other metals (Fe, Co, Ni and Mn) were also explored, and this synthetic strategy of the electrochemical exfoliation with simultaneous metal doping was experimentally demonstrated to enhance HER activity (Fig. S9 in Supporting information). Especially, the Co-EX-MoSe2 and Co-EX-WSe2 catalysts displayed a greater improvement in HER activity than those of the corresponding bulk phases.

    To further realize the efficient application of simultaneous H2 and electricity production, the Ni-EX-MoS2 based Zn-H2O fuel battery in 1.0 mol/L KOH was constructed (Fig. 5a). When the battery started to discharge, an oxidation reaction occurred at anode Zn plate, while the HER happened at the cathode [47-50]. The commercial Pt/C-based Zn-H2O battery displayed the best electrochemical performance. Fig. 5b showed the discharge polarization curves of the Zn-H2O battery with different cathode materials. The Ni-EX-MoS2 exhibited a higher current density than that of the control EX-MoS2 during the discharge process. Moreover, the Ni-EX-MoS2-based Zn-H2O battery reached a high power density of 3.3 mW/cm2 (Fig. 5c), exceeding the EX-MoS2-based battery (1.5 mW/cm2). In Fig. 5d, no significant loss of voltage at different current densities of 5, 10, 15 and 20 mA/cm2 was observed for the Ni-EX-MoS2 based Zn-H2O battery, indicating the excellent stability of Ni-EX-MoS2-based Zn-H2O battery. During the discharge process, the specific capacities of the Zn-H2O battery at 5 mA/cm2 was calculated to be 826 mAh/g (Fig. S10 in Supporting information). In addition, the Ni-EX-MoS2-based Zn-H2O battery exceeded the chronopotentiometry curve for 6 h at 10 mA/cm2 with insignificant voltage change, which indicates outstanding durability of this Zn-H2O battery (Fig. 5e). Significantly, Fig. 5f illustrated that three Zn-H2O batteries connected in series light up a blue light-emitting diode, which indicates that the proposed Zn-H2O battery shows a great perspective in terms of energy supply.

    Figure 5

    Figure 5.  (a) Schematic illustration of Zn-H2O battery. (b) Discharge polarization curves of EX-MoS2, Ni-EX-MoS2 and Pt/C. (c) Corresponding power density curves. (d) Chronopotentiometric responses of EX-MoS2, Ni-EX-MoS2, and Pt/C-based Zn-H2O battery at current densities ranging from 5 mA/cm2 to 20 mA/cm2 during discharging process. (e) Galvanostatic discharge curves at 10 mA/cm2. (f) Actual photograph of a blue light-emitting diode lit by three series-connected Ni-EX-MoS2-based Zn-H2O batteries.

    In summary, a novel 2D Ni-EX-MoS2 nanosheets catalyst, with a lateral size of ~500 nm and thickness of ~3.5 nm, was synthesized via a one-step electrochemical exfoliation strategy. During the synthesis processes, the simultaneous electrochemical exfoliation and the doping of Ni species were beneficial to the formation of a stable 1T/2H phase-MoS2 heterojunction, which endowed the Ni-EX-MoS2 with the higher conductivity and more active sites, thus led to the excellent HER activity in base. In addition, the Ni-EX-MoS2 acted as a cathode of the Zn-H2O battery displayed a high power density as well as good stability during the HER process. This work might provide new avenues for the development of other transition metal-doped 2D TMDs for various meaningful applications in electrochemistry, including N2 reduction reactions, CO2 reduction, and O2 reduction reactions.

    The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

    This work is financially supported by the National Natural Science Foundation of China (Nos. 21805244, 51776188). We also greatly acknowledg the financial support from National Natural Science Foundation of China (Nos. 21922811, 21878270, 21961160742), the Zhejiang Provincial Natural Science Foundation of China (No. LR19B060002), the Startup Foundation for Hundred-Talent Program of Zhejiang University, Jiangxi Province "Double Thousand Plan" Project (No. 205201000020).

    Supplementary material associated with this article can be found, in the online version, at doi:10.1016/j.cclet.2022.01.037.


    1. [1]

      Y.N. Xia, C.T. Campbell, B.R. Cuenya, et al., Chem. Rev.121 (2021) 563–566. doi: 10.1021/acs.chemrev.0c01269

    2. [2]

      Y. Hou, M. Qiu, M.G. Kim, et al., Nat. Commun. 10 (2019) 1392. doi: 10.1038/s41467-019-09394-5

    3. [3]

      C.X. Zhao, J.N. Liu, J. Wang, et al., Chem. Soc. Rev. 50 (2021) 7745. doi: 10.1039/d1cs00135c

    4. [4]

      C.X. Zhao, J.N. Liu, J. Wang, et al., Adv. Mater. 33 (2021) 2008606. doi: 10.1002/adma.202008606

    5. [5]

      X.M. Liu, X.Y. Cui, K. Dastafkan, et al., J. Energy Chem. 53 (2021) 290. doi: 10.1016/j.jechem.2020.04.012

    6. [6]

      C.J. Lei, H.Q. Chen, J.H. Cao, et al., Adv. Energy Mater. 8 (2018) 1801912. doi: 10.1002/aenm.201801912

    7. [7]

      I.T. McCrum, M.T.M. Koper, Nat. Energy. 5 (2020) 891–899. doi: 10.1038/s41560-020-00710-8

    8. [8]

      L.K. Zheng, L.N. Hu, Y.C. Hu, et al., Catal. Sci. Technol. 11 (2021) 3706. doi: 10.1039/d1cy00240f

    9. [9]

      H. Yang, S. Gao, C.N. Zhang, et al., Sci. China Chem. 64 (2021) 101–108. doi: 10.1007/s11426-020-9895-2

    10. [10]

      Q. Li, Y.C. Wang, J. Zeng, et al., Chin. Chem. Lett. 32 (2021) 3355–3358. doi: 10.1016/j.cclet.2021.03.063

    11. [11]

      Q.R. Shi, C.Z. Zhu, D. Du, et al., Chem. Soc. Rev. 48 (2019) 3181–3192. doi: 10.1039/c8cs00671g

    12. [12]

      Y. Hou, M. Qiu, T. Zhang, et al., Adv. Mater. 29 (2017) 170158.

    13. [13]

      Q. Fu, X.J. Han, X.J. Wang, et al., Adv. Mater. 33 (2021) 1907818. doi: 10.1002/adma.201907818

    14. [14]

      J.F. Zhang, T.Y. Zhu, Y. Wang, et al., Mater. Today. 36 (2020) 83–90. doi: 10.1016/j.mattod.2020.02.006

    15. [15]

      J.J. Wei, G. Wang, Y.J. Zhang, et al., Chin. Chem. Lett. 32 (2021) 1191–1196. doi: 10.1016/j.cclet.2020.08.005

    16. [16]

      P. Prabhu, V. Jose, J.M. Lee, Matter 2 (2020) 526–553. doi: 10.1016/j.matt.2020.01.001

    17. [17]

      Y.K. Rao, H.D. Wang, Y.J. Zeng, et al., Adv. Sci. 8 (2021) 2002284. doi: 10.1002/advs.202002284

    18. [18]

      X.L. Pan, M.Y. Yan, C.L. Sun, et al., Adv. Funct. Mater. 31 (2021) 2007840. doi: 10.1002/adfm.202007840

    19. [19]

      H. Niu, Z. G, Zou, Q. Wang, et al., Chem. Eng. J. 399 (2020) 125675. doi: 10.1016/j.cej.2020.125675

    20. [20]

      J.C. Si, Q. Zheng, H.L. Chen, et al., ACS Appl. Mater. Interfaces 11 (2019) 13205–13213. doi: 10.1021/acsami.8b22052

    21. [21]

      X. Wang, J.J. He, B.Q. Zhou, et al., Angew. Chem. Int. Ed. 57 (2018) 8668–8673. doi: 10.1002/anie.201804886

    22. [22]

      Q. Xu, Y.B. Zhu, T.T. Xie, et al., ChemCatChem 13 (2020) 592–602.

    23. [23]

      Y.T. Luo, X. Li, X.K. Cai, et al., ACS Nano 12 (2018) 4565–4573. doi: 10.1021/acsnano.8b00942

    24. [24]

      D.N. Liu, J.H. Wang, J. Lu, et al., Small Methods 3 (2019) 1900083. doi: 10.1002/smtd.201900083

    25. [25]

      X.P. Li, C. Huang, W.K. Han, et al., Chin. Chem. Lett. 32 (2021) 2597–2616. doi: 10.1016/j.cclet.2021.01.047

    26. [26]

      J.J. Wu, J. Peng, Y. Zhou, et al., J. Am. Chem. Soc. 141 (2019) 592–598. doi: 10.1021/jacs.8b11656

    27. [27]

      X. Wang, Y.W. Zhang, H.N. Si, et al., J. Am. Chem. Soc. 142 (2020) 4298–4308. doi: 10.1021/jacs.9b12113

    28. [28]

      J.C. Si, H.L. Chen, C.J. Lei, et al., Nanoscale 11 (2019) 16200–16207. doi: 10.1039/c9nr04587b

    29. [29]

      X. Hai, W. Zhou, S.Y. Wang, et al., Nano Energy 39 (2017) 409–417. doi: 10.1016/j.nanoen.2017.07.021

    30. [30]

      K. Wu, X. Cao, M.Y. Li, et al., Small 16 (2020) 2004178. doi: 10.1002/smll.202004178

    31. [31]

      B. Pattengale, Y.C. Huang, X.X. Yan, et al., Nat. Commun. 11 (2020) 4114. doi: 10.1038/s41467-020-17904-z

    32. [32]

      D.Z. Wang, X.Y. Zhang, S.Y. Bao, et al., J. Mater. Chem. A5 (2017) 2681–2688. doi: 10.1039/C6TA09409K

    33. [33]

      X.L. Zheng, Z.H. Guo, G.Y. Zhang, et al., J. Mater. Chem. A7 (2019) 19922–19928. doi: 10.1039/c9ta06091j

    34. [34]

      J. Zhang, T. Wang, P. Liu, et al., Energy. Environ. Sci. 9 (2016) 2789–2793. doi: 10.1039/C6EE01786J

    35. [35]

      K. Sun, Y.Q. Liu, Y. Pan, et al., Nano. Res. 11 (2018) 4368–4379. doi: 10.1007/s12274-018-2026-8

    36. [36]

      S.A. Shah, L. Xu, R.N. Sayyar, et al., Chem. Eng. J. 428 (2022) 132126. doi: 10.1016/j.cej.2021.132126

    37. [37]

      X.Y. Meng, C. Ma, L.Z. Jiang, et al., Angew. Chem. Int. Ed. 59 (2020) 10502–10507. doi: 10.1002/anie.202003484

    38. [38]

      W.W. Yang, S.Q. Zhang, Q. Chen, et al., Adv. Mater. 32 (2020) 2001167. doi: 10.1002/adma.202001167

    39. [39]

      H.Q. Jin, Y. Yu, Q.K. Shen, et al., J. Mater. Chem. A9 (2021) 13996–14003. doi: 10.1039/d1ta03513d

    40. [40]

      X.Y. Yu, Y. Feng, Y. Jeon, et al., Adv. Mater. 28 (2016) 9006–9011. doi: 10.1002/adma.201601188

    41. [41]

      L. Wang, Z.J. Li, K.X. Wang, et al., Nano Energy 74 (2020) 104850. doi: 10.1016/j.nanoen.2020.104850

    42. [42]

      F.P. Cheng, L. Wang, H.Q. Wang, et al., Nano Energy 71 (2020) 104621. doi: 10.1016/j.nanoen.2020.104621

    43. [43]

      H. Wang, Z.J. Li, Y. Li, et al., Nano Energy 81 (2021) 105613. doi: 10.1016/j.nanoen.2020.105613

    44. [44]

      C.J. Lei, Y. Wang, Y. Hou, et al., Energy. Environ. Sci. 12 (2019) 149–156. doi: 10.1039/c8ee01841c

    45. [45]

      H. Wang, J.C. Si, T.Y. Zhang, et al., Appl. Catal. B270 (2020) 118892. doi: 10.1016/j.apcatb.2020.118892

    46. [46]

      Z.Y. Yu, Y. Duan, M.R. Gao, et al., Chem. Sci. 8 (2017) 968–973. doi: 10.1039/C6SC03356C

    47. [47]

      H. Li, M.T. Zhang, L.C. Yi, et al., Appl. Catal. B280 (2021) 119412. doi: 10.1016/j.apcatb.2020.119412

    48. [48]

      P.W. Cai, Y. Li, G.X. Wang, et al., Angew. Chem. Int. Ed. 130 (2018) 3974–3979. doi: 10.1002/ange.201712765

    49. [49]

      Y.C. Ding, P.W. Cai, Z.H. Wen, Chem. Soc. Rev. 50 (2021) 1495–1511. doi: 10.1039/d0cs01239d

    50. [50]

      M.T. Zhang, H. Li, P.W. Cai, et al., Adv. Funct. Mater. 31 (2021) 2103248. doi: 10.1002/adfm.202103248

  • Figure 1  Schematic diagram of the electrochemical exfoliation and synthetic procedure.

    Figure 2  SEM images of (a) bulk MoS2 and (b) Ni-EX-MoS2. (c) TEM image of Ni-EX-MoS2. (d) AFM image of Ni-EX-MoS2. (e) HAADF-STEM image of Ni-EX-MoS2. (f) EDX elemental mapping images of O, S, Ni and Mo in the corresponding region.

    Figure 3  (a) HRTEM images Ni-EX-MoS2 nanosheets. Inset: red and yellow dots in the atomic arrangement of 1T and 2H phases represent for Mo and S atoms. (b) Corresponding SAED pattern. (c) Raman spectra of Ni-EX-MoS2 and bulk MoS2. High-resolution XPS spectra of (d) Mo 3d, (e) S 2p and (f) Ni 2p, respectively.

    Figure 4  (a) Polarization curves of bulk MoS2, EX-MoS2, Ni-EX-MoS2, and Pt/C after iR-correction and (b) Tafel plots of bulk MoS2, EX-MoS2, Ni-EX-MoS2 and Pt/C in 1 mol/L KOH solution. (c) Nyquist plots of bulk MoS2, EX-MoS2, Ni-EX-MoS2. Inset: An equivalent circuit for fitting impedance data. (d) Comparison of overpotentials at 10 mA/cm2 and Tafel slopes with recently reported MoS2-based electrocatalysts. (e) Chronopotentiometry curve of Ni-EX-MoS2 without iR-correction. Inset: photograph for electrochemical stability at 10 mA/cm2. Inset: polarization curves of Ni-EX-MoS2 for the first and 1000th CV cycles.

    Figure 5  (a) Schematic illustration of Zn-H2O battery. (b) Discharge polarization curves of EX-MoS2, Ni-EX-MoS2 and Pt/C. (c) Corresponding power density curves. (d) Chronopotentiometric responses of EX-MoS2, Ni-EX-MoS2, and Pt/C-based Zn-H2O battery at current densities ranging from 5 mA/cm2 to 20 mA/cm2 during discharging process. (e) Galvanostatic discharge curves at 10 mA/cm2. (f) Actual photograph of a blue light-emitting diode lit by three series-connected Ni-EX-MoS2-based Zn-H2O batteries.

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  • 发布日期:  2023-01-15
  • 收稿日期:  2021-12-03
  • 接受日期:  2022-01-13
  • 修回日期:  2022-01-05
  • 网络出版日期:  2022-01-19
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