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Molybdenum Carbide Nanoparticles Coated into the Graphene Wrapping N-Doped Porous Carbon Microspheres for Highly Efficient Electrocatalytic Hydrogen Evolution Both in Acidic and Alkaline Media
Huifang Wei, Qiaoya Xi, Xi'an Chen,* Daying Guo, Feng Ding, Zhi Yang, Shun Wang, Juan Li, and Shaoming Huang*
Molybdenum carbide (Mo2C) is recognized as an alternative electrocatalyst to noble metal for the hydrogen evolution reaction (HER). Herein, a facile, low cost, and scalable method is provided for the fabrication of Mo2C-based eletrocatalyst (Mo2C/G-NCS) by a spray-drying, and followed by annealing. As-prepared Mo2C/G-NCS electrocatalyst displays that ultrafine Mo2C nano-partilces are uniformly embedded into graphene wrapping N-doped porous carbon microspheres derived from chitosan. Such designed structure offer several favorable features for hydrogen evolution application: 1) the ultrasmall size of Mo2C affords a large exposed active sites; 2) graphene-wrapping ensures great electrical conductivity; 3) porous structure increases the electrolyte-electrode contact points and lowers the charge transfer resistance; 4) N-dopant interacts with H+ better than C atoms and favorably modifies the electronic structures of adjacent Mo and C atoms. As a result, the Mo2C/G-NCS demonstrates superior HER activity with a very low overpotential of 70 or 66 mV to achieve current density of 10 mA cm-2, small Tafel slope of 39 or 37 mV dec-1, respectively, in acidic and alkaline media, and high stability, indicating that it is a great potential candidate as HER electrocatalyst.
As a clean and sustainable energy source, hydrogen has been considered as one of the most alternatives to fossil fuels.'1' The evolution of hydrogen through electrocatalytic splitting water is one of the important strategies for hydrogen production.'2' Although the Pt-based materials have been proven to be the
H. F. Wei, Q. Y. Xi, Dr. X. Chen, D. Y. Guo, F. Ding, Prof. Z. Yang, Prof. S. Wang, J. Li, Prof. S. M. Huang Key Laboratory of Carbon Materials of Zhejiang Province College of Chemistry and Materials Engineering Wenzhou University Wenzhou 325035, P. R. China
E-mail: xianchen@wzu.edu.cn; smhuang@wzu.edu.cn
Prof. S. M. Huang
School of Materials and Energy
Guangdong University of Technology
Guangzhou, Guangdong 510006, P. R. China
© 2018 The Authors. Published by WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim. This is an open access article under the terms of the Creative Commons Attribution License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
DOI: 10.1002/advs.201700733
most efficient electrocatalysts for hydrogen evolution reaction (HER), the high cost, limited supply, and poor durability hinder their global-scale application.'3,4' Therefore, much effort has been dedicated to develop robust nonnoble-metal HER catalysts,'5-22' such as cobalt-, nickel-, iron-, tungsten-, and molybdenum-based materials.
In recent years, Mo2C has been exploited as one of the promising HER electrocatalysts due to its Pt-like features and low-cost. However, Mo2C obtained at high temperature usually suffers the inevitable aggregation,'23' which leads to the less exposure active sites, thus compromising the HER performance. To tackle the drawback, various conductive carbon materials, such as graphene, carbon nanotube, porous carbon, etc., were introduced as framework for supporting Mo2C to reduce its aggregation and improve conductivity.'24-30' Recently, the electrochemically active N-doped nanocarbon matrix for Mo2C has been proved to be effective for improving its electro-catalytic activity, mainly due to that the N-dopant could interact with H+ better than C atoms for enhanced H+ adsorption and favorably modify the electronic structures of adjacent Mo and C atoms for improved H desorption from Mo—H.'31-44' Despite these progresses, exploring the suitable precursors to uniformly hybridize Mo and carbon source to perform the controllable preparation of well-defined Mo2C nanostructure with an N-doped nanocarbon framework is still great demand.
Herein, we provide a simple protocol for synthesis of ultrafine Mo2C nanoparticles uniformly anchored into gra-phene wrapping N-doped porous carbon microspheres (Mo2C/G-NCS) using low cost chitosan and ammonium molyb-date tetrahydrate (AM) as carbon and Mo source, respectively (Scheme 1, see in the Experimental Section for detail). By virtue of the electrostatic interaction of Mo7O24- and the —NH3+ group derived from the long chain chitosan molecular in acetic acid medium (Figure S1, Supporting Information), the uniform hybrid Mo and carbon source can be achieved, thus ensuring the well-regulated Mo2C-embedded into N-doped carbon
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Scheme 1. Schematic illustration of the procedure for preparing Mo2C/G-NCS.
nanostructure. The particle average size increases when the AM is added into chitosan solution, which indirectly verifies the existence of electrostatic interaction (Figure S2, Supporting Information). Due to the such designed structure with N-doped carbon microsphere as carbon matrix and graphene wrapping for fast electron transfer, ultrafine Mo2C nanoparticles for sufficient catalytic sites, and porous structure for easy mass transfer, the resulting material acts as highly active and stable nonplat-inum HER electrocatalyst with a very low overpotential of 70 or 66 mV to achieve current density of 10 mA cm-2, small Tafel slope of 39 or 37 mV dec-1, respectively, in acidic and alkaline media, which is one of most active Mo-based HER electrocata-lysts and comparable to the commercial 20 wt% Pt/C catalyst.
The morphology and micro structure of as-prepared Mo2C-based composites were first observed by field emission scanning electron microscopy (FESEM) and transmission electron microscopy (TEM). As can been seen from Figure 1a, the product Mo2C/G3-NCS750 is composed of uniform microspheres with rough surface and porous texture. On the contrast, the corresponding products Mo2C/NCS750 without the addition of graphene oxide and Mo2C/NC750 without the spray-drying show relatively smooth and compact surface (Figure S3, Supporting Information). This indicates that the spray drying and addition of graphene oxide could cause into a loose, porous texture, thus not only increasing the electrolyte-electrode contact points and exposing the more active sites but also providing efficient electron transport and mass transfer. This is also verified by nitrogen adsorption/desorption isotherms (Figure S4, Supporting Information). The sample Mo2C/NC750 has little adsorption of nitrogen gas, indicating its extremely small specific surface area and the absence of pores. By contrast, the adsorption amount of nitrogen gas obviously increases for Mo2C/G3-NCS750, indicating that it possesses a larger Brunner-Emmet-Teller (BET) surface area than that of Mo2C/NC750. From the TEM image, the graphene wrapping the microspheres to form the rugged surface is also observed clearly. The high-resolution TEM (HRTEM) image shows that ultrafine nanoparticles with a size ~4 nm are embedded into carbon matrix (Figure 1c; Figure S5, Supporting Information),
which is consistent with the observation from the bright and dark field TEM image (Figure S6, Supporting Information). The apparent lattice fringes with a distance of 0.23 and 0.34 nm are assigned to crystallographic planes (101) of hexagonal Mo2C and (002) of graphene, respectively. X-ray energy-dispersive spectroscopy (EDS) elemental mapping (Figure 1d-g) indicates the C, Mo, N, and O atoms are uniformly distributed into the hybrids, which verifies that there is a homogeneous coating of Mo2C nanoparticles. N atoms are originated from the amino group of chitosan and NH4+ of (NH4)6Mo7O24.
The crystalline phase composition of as-prepared Mo2C-based materials yielded at different condition was determined by powder X-ray diffraction (Figure 2). When the precursor is pyrolyzed, the corresponding product Mo2C/G3-NCS750 clearly shows the characteristic diffraction peaks at 34.5°, 38.0°, 39.6°, 52.3°, 61.9°, 69.8°, 72.8°, 75.0°, and 76.0°, attributing to the (100), (002), (101), (102), (110), (103), (200), (112), and (201) planes of a hexagonal ^-Mo2C (JCPDS 65-8766), respectively. No addition peak is observed except for a weak diffraction peaks at 42.6° corresponding to (100) plane of graphite. The particle size was evaluated by Scherrer equation, and the average size of Mo2C particles is around 4.5 nm (see the calculation details in the Supporting Information). These results agree well the HRTEM observation. A similar X-ray diffraction (XRD) pattern is observed for the Mo2C/G3-NCS850, suggesting the similar crystalline structure. The average size of Mo2C particles increases to 6.5 nm calculated according the Scherrer equation (see the calculation details in the Supporting Information) when the pyrolysis temperature is elevated to 850 °C, which is consistent with the size of ~6 nm judged by the observation on the HRTEM image (Figure S7, Supporting Information). When the annealing temperature decreases to the 650 °C, no characteristic diffraction peak of the Mo2C is observed for Mo2C/ G3-NCS650. These results offer strong evidence of a solid-state reaction between (NH4)6Mo7O24 and chitosan at about 750 °C. Other than the characteristic diffraction peaks of the Mo2C, the (002) diffraction peak of MoO2 is observed for the product Mo2C/G5-NCS750, where the amount of graphene oxide increases (Figure S8, Supporting Information). The materials
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Figure 1. a) SEM images at different magnifications, b,c) TEM images at different magnifications and d-g) the corresponding EDS elemental mapping of Mo2C/G3-NCS750.
Mo2C/NC750 and Mo2C/NCS750 also show the similar crystalline structure (Figure S8, Supporting Information).
Since the HER performance of transition-metal-based materials is closely corrected with the chemical environment of the metal, the surface electronic state and composition of Mo2C/G3-NCS750 were further characterized by X-ray photo-electron spectroscopy (XPS). The survey spectrum (Figure 3a) displays the obvious signals of the atom Mo and C, as well
Figure 2. XRD patterns of all the as-prepared composites.
as the atom N, indicating that N has been successfully introduced into Mo2C/G3-NCS750 as expected. The high resolution Mo 3d spectrum (Figure 3b) can be well-fitted into four pairs of peaks, indicating that four oxidation states for Mo species (+2, +3, +4, and +6) exist on the surface of Mo2C nanoparticles. The peaks at binding energies of230.4/234.2 and 232.2/235.9 eV are ascribed to Mo4+ and Mo6+ species, which is attributed that the surface of Mo2C NPs can be readily oxidized to molybdenum oxides when exposed to air.[24,25,30] Mo2+ with the binding energies of 228.3/231.4 eV is assigned as carbides, which is known to be served as active sites for HER.[23-25] From the thermal gravimetric analysis of Mo2C/G3-NCS750 composite, the content of Mo2C is about 69.7% (Figure S9, Supporting Information). The peaks at binding energies of 229.1/232.8 eV corresponding to Mo3+ for nitrides suggest N occupying part of C sites in Mo2C nanoparticles.[37,39,41,42] The deconvolution analysis of the detailed N1s spectrum (Figure 3c) displays the presence of pyridinic N (398.4 eV), graphitic N (401.7 eV), and N-Mo (396.4 eV).[3742] Among these type of N-doping, the pyridinic N is the main nitrogen species in Mo2C/G3-NCS750, which is beneficial to the HER.[32 34 37 39] The presence of low level (less than 4%) of N-Mo species further confirms that N is doped into molybdenum carbide, which is in good agreement with the analysis of Mo 3d spectrum. This
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Figure 3. a) The wide, b) Mo 3d, c) N1s, and d) C1s XPS spectra of Mo2C/G3-NCS750.
part of N-doping as an electron-rich dopant could downshift the density of empty d-band in Mo2C, and thus weaken Mo—H strength.!37,39,41,42] No diffraction signals of nitride are identified by XRD analyzer, indicating that few N occupy part of C sites in Mo2C, which agrees well the above analysis of N1s XPS spectrum. The deconvolution analysis of the high-resolution C1s spectrum is also consistent with the expected structure of Mo2C/G3-NCS750 (Figure 3d).
The electro catalytic HER performance of the as-prepared Mo2C-based materials was first investigated using three-electrode electrochemical configuration in 0.5 m H2SO4 solution, as well as the commercial catalyst 20% Pt/C. Figure 4 displays the corresponding linear sweep voltammetry (LSV) curves. As expected, the Pt/C catalyst is highly active toward HER in acidic electrolyte with a near-zero onset overpotential. It is exciting that Mo2C/G3-NCS750 exhibits a very small overpotential of 70 mV to drive a current density of 10 mA cm-2. Furthermore, the current density can reach to 75 mA cm-2 at an overpotential of 150 mV, which is even larger than the value obtained at n = 200 mV for many Mo2C-based electro catalysts reported. These results represent that as-prepared Mo2C/G3-NCS750 is one of the currently most efficient Mo2C-based HER electrocat-alysts in acidic electrolyte (Table S1, Supporting Information). On the contrary, Mo2C/NC750 and Mo2C/NCS750 need the overpotential of 97 and 82 mV, respectively, to achieve a current density of 10 mA cm-2. The enhancement on the HER performance is believed to be attributed that graphene-wrapping improves electrical conductivity, and porous structure increases the electrolyte-electrode contact points and lower the charge
transfer resistance, thus exposes more active sites, which is evidenced by the electrochemically active surface area (ECSA). To evaluate the ECSA of these as-prepared electro catalysts, the cyclic voltammetry (CV) was measured in the region from 0.2 to 0.4 V at scan rate varying from 20-180 mV s-1. The calculated electrochemical double-layer capacitance (Cdl) of Mo2C/ G3-NCS750 (46.3 mF cm-2) is ~3 times larger than Mo2C/ NC750 (11.9 mF cm-2) and Mo2C/NCS750 (13.3 mF cm-2) (Figure S10, Supporting Information). If we suppose a standard value of 40 ||F cm-2,[37] the ECSA of Mo2C/G3-NCS750 is estimated to ~91.3 cm3 g-1 (see the calculation details in the Supporting Information). ESCA of Pt/C electrocatalyst is also calculated (~71.0 cm3 g-1), and the polarization curves of Mo2C/ G3-NCS750 and Pt/C are normalized by ESCA (Figures S11 and S12, Supporting Information). From the Figure S12 (Supporting Information), the Mo2C/G3-NCS750 still exhibits excellent HER performance, which is comparable to the Pt/C electrocatalyst.
In control experiments, we first investigate the influence on the performance of the mass ratio between AM and chitosan (Figure S13, Supporting Information). When a mass ratio of AM and chitosan is 1:1, the corresponding product Mo2C/NC750 displays best HER activity. The effect of the carbonization temperature and amount of graphene oxide on the electrocatalytic properties were further evaluated (Figure S14, Supporting Information). Further increasing the annealing temperature to 850 °C, the corresponding electrocatalyst Mo2C/G3-NCS850 shows a slightly larger onset overpotential. The decline in performance is believed to be ascribed to the increase of Mo2C
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the desorption step, or the Tafel reaction (H*ads + H*ads ^ H2) is a recombination step at the Tafel slope of 40 mV dec-1 or 30 mV dec-1, respectively. In the case, the tafel slope of 39 mV dec-1 demonstrates that Mo2C/G3-NCS750 catalyzed HER proceeds by a Volmer-Heyrovsky mechanism, where the electrochemical desorption of hydrogen is the rate-limiting step. The j0 value of Mo2C/G3-NCS750 was determined to be 0.33 mA cm-2, outperforming many Mo2C-based HER electrocatalysts reported in the literature, such as MoDCA-5 (0.179 mA cm-2),'39' P-Mo2C@C NWs (0.18 mA cm-2),'24' etc. Electron impedance spectroscopy (EIS) was conducted to further probe the catalytic behavior of these as-prepared electro-catalysts, and the corresponding Nyquist plots are shown in Figure 4c. Since the semicircle in the low-frequency region typically means the charge transfer resistance, the smaller value implies that a faster electrode kinetic is occurred for the Mo2C/G3-NCS750 catalyst. Mo2C/NC750 and Mo2C/NCS750 display the higher impedance, which is well in agreement with the analysis result of the Tafel slopes. In addition, the only one semicircle also indicates that HER proceeds by a Volmer-Heyrovsky mechanism for these presented electrocatalysts.
Considering that the long-term stability is another key factor of the catalytic performance of a HER electrocatalyst, the durability of Mo2C/G3-NCS750 catalyst was evaluated by 2000 cycles of CV scanning from 0.05 to -0.4 V at a scan rate of 100 mV s-1 in acidic electrolyte. As can be seen from Figure 4d, the almost same polarization curves of Mo2C/G3-NCS750 before and after 2000 CV cycles are observed, suggesting its excellent stability. Meanwhile, the chronoamperometry test of Mo2C/G3-NCS750 for 20 h at n = 70 mV in acidic electrolyte was also performed. Only =10% catalytic current decay of Mo2C/G3-NCS750 demonstrates its high stability under corrosive acidic medium. As mentioned, the crystalline phase composition of Mo2C/ G3-NCS750 after continuously producing hydrogen for 20 h remains unchanged, which is evidenced by the XRD analysis (Figure S15, Supporting Information).
Since water splitting is often occurred in alkaline solution for practical applications, the HER performance of as-prepared molybdenum-based catalyst is further evaluated in 1 m KOH. The HER activity of as-prepared the Mo2C-based catalysts (Mo2C/G3-NCS750, Mo2C/NCS750, and Mo2C/NC750) is slightly enhanced in alkaline solution instead of acidic medium, and their overpotential to achieve 10 mA cm-2 is reduced to 66, 75, 81 from 70, 82, 97 mV, respectively (Figure 5a). Interestingly, their Tafel slopes are further decreased to 37, 43, 56 mV dec-1 (Figure 5b). This change trend on the performance is consistent with some previous reports.'32,44-46' As we know, such a low overpotential (66 mV) to drive the 10 mA cm-2 and small Tafel slope means that Mo2C/G3-NCS750 is one of Mo2C-based electrocatalysts reported with best catalytic activity in alkaline electrolyte (Table S1, Supporting Information). From the Figure S16 (Supporting Information), the Rct value of Mo2C/ G3-NCS750 is much smaller than that of Mo2C/NC750 and Mo2C/NCS750 under the same conditions, implying the faster electron transfer rate and higher catalytic activity of Mo2C/ G3-NCS750 electrocatalyst for HER, which agrees well with the analysis results of HER performance above-mentioned. In addition, the polarization curves for Mo2C/G3-NCS750 before and after 2000 CV cycles is almost overlap, indicating its long-term
durability in alkaline electrolyte (Figure S17, Supporting Information).
We demonstrate a simple, low cost, and scalable strategy for the fabrication of Mo2C-based eletrocatalyst by a spray-drying, and followed by annealing. As-prepared Mo2C/G3-NCS750 catalyst under the optimized synthetic condition exhibits excellent HER performance both in acidic and alkaline media, with a small overpotential, low Tafel slope, and long-term durability, which is superior to most of the Mo2C-based electrocatalysts reported previously (Table S1, Supporting Information) and close to the commercial Pt/C (20 wt%). The enhanced HER property is believed to attribute that the well-defined porous microspherical structure, graphene wrapping, ultrasmall Mo2C nanocrystallinity, and nitrogen-dopant offer many appealing features, such as a large exposed activity sites, improved electron transfer, fast charge transport, the enhanced interaction with H+ and low desorption energy of Mo—H bond. The facile preparation and excellent properties for G-Mo2C/CS make this material very promising for practical application in hydrogen production. Futhermore, this method is expected to be generalized to prepare other metal carbides for electrocatalysis or energy storage and conversion devices, where exposed more active sites, and efficient ionic and electronic transport are critical.
Experimental Section
Preparation of the Catalyst: Chitosan (1 g) was first dissolved deionized water (200 mL) containing acetate acid (2 mL). Second, AM (1 g) was dissolved into deionized water (10 mL), and then added into the 60 mL (5.0 mg mL-1) graphene oxide (GO) solution prepared according to the method reported previously by us.l47l Subsequently, the above solution was sprayed into the chitosan solution and further stirred 12 h at room temperature to generate a mixture. Then, the powder was collected after spray-drying the mixture, and further annealed under Ar at 750 °C for 3 h with a temperature ramping rate of 2 °C min-1 to yield the product (Mo2C/G3-NCS750). Similarly, when the mass of GO is 0, 0.1, 0.5 g, Mo2C/NCS-750, Mo2C/G1-NCS750, and Mo2C/G5-NCS750 can be readily obtained. For comparison, the Mo2C/G3-NCS samples were carbonized at different carbonization temperatures such as 650, 850 °C, which were denoted as Mo2C/G3-NCS650, Mo2C/G3-NCS850, respectively. The Mo2C/NC750 is prepared using a similar procedure to Mo2C/NCS750, except that the solids were collected by centrifugation instead of spray-drying. The mass ratio of AM and Chitosan is 2:1, 1:1, and 1:2, the corresponding products are denoted as Mo2C/0.5NC750, Mo2C/NC750, and Mo2C/2NC750, respectively.
Electrochemical Measurements: The electrochemical experiments for HER were carried out in a conventional three-electrode cell using a CHI 660E at room temperature. Ag/AgCl (3 m KCl) and graphite rod were used as reference and counter electrodes, respectively in N2-saturated 0.5 m H2SO4. Pt wire is used as reference electrode instead of graphite rod when the electrochemical experiments conducted in 1 m KOH solution. All potentials were corrected versus reversible hydrogen electrode (RHE) according to Erhe = EAg/AgCl + EAg/AgCl + 0.059 x pH. 2 mg of the catalyst powder and 1 mg of black carbon were dispersed in a mixture of 400 |L of water, 100 |L of ethanol, and formed a catalyst ink after 1 h of sonication. Then, 10 |L of catalyst ink was pipetted onto the glassy carbon surface with a diameter of 3 mm (catalyst loading =0.57 mg cm-2). Then, 5 |L of 0.05 wt % Nafion solution was coated onto the electrodes and was dried at room temperature before measurement. The mass loading of referred Pt/C is same with the catalysts. The LSV was tested at a rate of 30 mV s-1 from 0.05 to -0.4 V versus RHE. The stability tests were carried out by repeating the potential scan from 0.05 to -0.4 V versus RHE for 2000 cycles. EIS
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measurements were carried out from 105 to 0.01 Hz at -80 mV in acidic medium or -77 mV in alkaline medium versus RHE. The double-layer capacitances (Cdl) were obtained through cyclic voltammograms (CV) curves which were performed at scan rates varying from 20 to 180 mV s-1 in the potential region from 0.2 to 0.4 V versus RHE.
Supporting Information
Supporting Information is available from the Wiley Online Library or from the author.
Acknowledgements
The work was supported by grants from the National Natural Science Foundation of China (Grant Nos. 51402217 and 51672193) and the National Science Fund for Distinguished Young Scholars (Grant No. 51420105002).
Conflict of Interest
The authors declare no conflict of interest.
Keywords
electrocatalytic hydrogen evolution, graphene wrapping N-doped porous carbon microspheres, molybdenum carbide, spray-drying
Received: October 12, 2017 Revised: November 19, 2017 Published online:
[1] L. Schlapbach, A. Zuttel, Nature 2001, 414, 353.
[2] J. A. Turner, Science 2004, 305, 972.
[3] J. Greeley, T. F. Jaramillo, J. Bonde, I. B. Chorkendorff, J. K. Norskov, Nat. Mater. 2006, 5, 909.
[4] M. G. Walter, E. L. Warren, J. R. McKone, S. W. Boettcher, Q. Mi,
E. A. Santori, N. S. Lewis, Chem. Rev. 2010, 110, 6446.
[5] X. Zou, Y. Zhang, Chem. Soc. Rev. 2015, 44, 5148.
[6] H. Yang, Y. Zhang, F. Hu, Q. Yang, Nano Lett. 2015, 15, 7616.
[7] S. Peng, L. Li, X. Han, W. Sun, M. Srinivasan, S. G. Mhaisalkar,
F. Cheng, Q. Yan, J. Chen, S. Ramakrishna, Angew. Chem., Int. Ed. 2014, 53, 12594.
[8] X. Fan, Z. Peng, R. Ye, H. Zhou, X. Guo, ACS Nano 2015, 9, 7407.
[9] P. Jiang, Q. Liu, Y. Liang, J. Tian, A. M. Asiri, X. Sun, Angew. Chem., Int. Ed. 2014, 53, 12855.
[10] A. B. Laursen, K. R. Patraju, M. J. Whitaker, M. Retuerto, T. Sarkar, N. Yao, K. V. Ramanujachary, M. Greenblatt, G. C. Dismukes, Energy Environ. Sci. 2015, 8, 1027.
[11] R. Wu, J. Zhang, Y. Shi, D. Liu, B. Zhang, J. Am. Chem. Soc. 2015, 137, 6983.
[12] H. Yan, C. Tian, L. Wang, A. Wu, M. Meng, L. Zhao, H. Fu, Angew. Chem., Int. Ed. 2015, 54, 6325.
[13] H. B. Wu, B. Y. Xia, L. Yu, X. Y. Yu, X. W. Lou, Nat. Commun. 2015, 6, 6512.
[14] R. J. Zhang, X. Li, L. Zhang, S. Y. Lin, H. W. Zhu, Adv. Sci. 2016, 3, 1600208.
[15] T. Sun, Q. Wu, Y. F. Jiang, Z. Q. Zhang, L. Y. Du, L. J. Yang, X. Z. Wang, Z. Hu, Chem. - Eur. J 2016, 22, 10326.
[16] K. D. Li, J. F. Zhang, R. W. Wu, Y. F. Yu, B. Zhang, Adv. Sci. 2016, 3, 1500426.
[17] M. Q. Zeng, Y. X. Chen, J. X. Li, H. F. Xue, R. G. Mendes, J. X. Liu, T. Zhang, M. H. Rummeli, L. Fu, Nano Energy 2017, 33, 356.
[18] H. Park, A. Encinas, J. P. Scheifers, Y. M. Zhang, B. P. T. Fokwa, Angew. Chem., Int. Ed. 2017, 56, 5575.
[19] H. L. Lin, W. B. Zhang, Z. P. Shi, M. W. Che, X. Yu, Y. Tang, Q. S. Gao, ChemSusChem 2017, 10, 2597.
[20] P. Li, Z. Yang, J. X. Shen, H. G. Nie, Q. R. Cai, L. H. Li, M. Z. Ge,
C. C. Gu, X. Chen, K. Q. Yang, L. J. Zhang, Y. Chen, S. M. Huang, ACS Appl. Mater. Interfaces 2016, 8, 3543.
[21] M. A. R. Anjum, J. S. Lee, ACS Catal. 2017, 7, 3030.
[22] D. H. Youn, S. Han, J. Y. Kim, J. Y. Kim, H. Park, S. H. Choi, J. S. Lee, ACS Nano 2014, 8, 5164.
[23] W. F. Chen, S. Iyer, S. Iyer, K. Sasaki, C. H. Wang, Y. Zhu, J. T. Muckerman, E. Fujita, Energy Environ. Sci. 2013, 6, 1818.
[24] Z. P. Shi, K. Q. Nie, Z. J. Shao, B. X. Gao, H. L. Lin, H. B. Zhang, B. L. Liu, Y. X. Wang, Y. H. Zhang, X. H. Sun, X. M. Cao, P. Hu, Q. S. Gao, Y. Tang, Energy Environ. Sci. 2017, 10, 1262.
[25] J. S. Li, Y. Wang, C. H. Liu, S. L. Li, Y. G. Wang, L. Z. Dong, Z. H. Dai, Y. F. Li, Y. Q. Lan, Nat. Commun. 2016, 7, 11204.
[26] W. Gao, Y. Q. Shi, Y. F. Zhang, L. Z. Guo, H. Y. Lu, Y. P. Huang, W. Fan, T. X. Liu, ACS Sustainable Chem. Eng. 2016, 4, 6313.
[27] D. H. Youn, S. Han, J. Y. Kim, J. Y. Kim, H. Park, S. H. Choi, J. S. Lee, ACS Nano 2014, 8, 5164.
[28] N. S. Alhajri, D. H. Anjum, K. Takanabe, J. Mater. Chem. A 2014, 2, 10548.
[29] W. F. Chen, C. H. Wang, K. Sasaki, N. Marinkovic, W. Xu, J. T. Muckerman, Y. Zhu, R. R. Adzic, Energy Environ. Sci. 2013, 6, 943.
[30] X. J. Fan, Y. Y. Liu, Z. W. Peng, Z. H. Zhang, H. Q. Zhou, X. M. Zhang, B. I. Yakobson, W. A. Goddard, X. Guo, R. H. Hauge, J. M. Tour, ACS Nano 2017, 11, 384
[31] J. P. Guo, J. Wang, Z. X. Wu, W. Lei, J. Zhu, K. D. Xia, D. L. Wang. J. Mater. Chem. A 2017, 5, 4879.
[32] Y. Huang, Q. F. Gong, X. N. Song, K. Feng, K. Q. Nie, F. P. Zhao, Y. Y. Wang, M. Zeng, J. Zhong, Y. G. Li, ACS Nano 2016, 10, 11337.
[33] C. B. Lu, D. N. Tranca, J. Zhang, F. R. Hernandez, Y. Z. Su, X. D. Zhuang, F. Zhang, G. Seifert, X. L. Feng, ACS Nano 2017, 11, 3933.
[34] Z. Y. Wu, B. C. Hu, P. Wu, H. W. Liang, Z. L. Yu, Y. Lin, Y. R. Zheng, Z. Y. Li, S. H. Yu, NPG Asia Mater. 2016, 8, e288.
[35] C. C. Du, H. Huang, Y. Wu, S. Y. Wu, W. B. Song, Nanoscale 2016, 8, 16251.
[36] H. Wang, C. Sun, Y. J. Cao, J. T. Zhu, Y. Chen, J. Guo, J. Zhao, Y. H. Sun, G. F. Zou, Carbon 2017, 114, 628.
[37] Y. Y. Chen, Y. Zhang, W. J. Jiang, X. Zhang, Z. H. Dai, L. J. Wan, J. S. Hu, ACS Nano 2016, 10, 8851.
[38] X. J. Yang, X. J. Feng, H. Q. Tan, H. Y. Zang, X. L. Wang, Y. H. Wang, E. B. Wang, Y. G. Li, J. Mater. Chem. A 2016, 4, 3947.
[39] R. G. Ma, Y. Zhou, Y. F. Chen, P. X. Li, Q. Liu, J. C. Wang, Angew. Chem., Int. Ed. 2015, 54, 14723.
[40] K. Zhang, Y. Zhao, D. Y. Fu, Y. J. Chen, J. Mater. Chem. A 2015, 3, 5783.
[41] Z. H. Cheng, J. Gao, Q. Fu, C. X. Li, X. P Wang, Y. K Xiao, Y. Zhao, Z. P. Zhang, L. T. Qu, ACS Appl. Mater. Interfaces 2017, 9, 24608.
[42] J. Gao, Z. H. Cheng, C. X. Shao, Y. Zhao, Z. P. Zhang, L. T. Qu, J. Mater. Chem. A 2017, 5, 12027.
[43] R. Kumar, R. T. Rai, S. Gautam, A. D. Sarkar, N. Tiwari, S. N. Jha,
D. Bhattacharyya, A. K. Ganguli, V. Bagchi, J. Mater. Chem. A 2017, 5, 7764.
[44] M. A. R. Anjum, M. H. Lee, J. S. Lee,J. Mater. Chem. A 2017, 5, 13122.
[45] Y. P. Liu, G. T. Yu, G. D. Li, Y. H. Sun, T. Asefa, W. Chen, X. X. Zou, Angew. Chem., Int. Ed. 2015, 54, 10752.
[46] K. Vezzu, A. B. Delpeuch, E. Negro, S. Polizzi, G. Nawn, F. Bertasi, G. Pagoy, K. Artyushkova, P. Atanassov, V. D. Noto, Electrochim. Acta 2016, 222, 1778.
[47] X. A. Chen, X. H. Chen, F. Q. Zhang, Z. Yang, S. M. Huang,J. Power Sources 2013, 243, 555.