ARTICLE
Received 15 Jul 2015 | Accepted 8 Jan 2016 | Published 10 Feb 2016
Lili Fan1,2,*, Peng Fei Liu3,*, Xuecheng Yan1, Lin Gu4, Zhen Zhong Yang4, Hua Gui Yang3, Shilun Qiu2 & Xiangdong Yao1
Hydrogen production through electrochemical process is at the heart of key renewable energy technologies including water splitting and hydrogen fuel cells. Despite tremendous efforts, exploring cheap, efcient and durable electrocatalysts for hydrogen evolution still remains as a great challenge. Here we synthesize a nickelcarbon-based catalyst, from carbonization of metal-organic frameworks, to replace currently best-known platinum-based materials for electrocatalytic hydrogen evolution. This nickel-carbon-based catalyst can be activated to obtain isolated nickel atoms on the graphitic carbon support when applying electrochemical potential, exhibiting highly efcient hydrogen evolution performance with high exchange current density of 1.2 mA cm 2 and impressive durability. This work may enable new opportunities for designing and tuning properties of electrocatalysts at atomic scale for large-scale water electrolysis.
DOI: 10.1038/ncomms10667 OPEN
Atomically isolated nickel species anchored on graphitized carbon for efcient hydrogen evolution electrocatalysis
1 School of Natural Sciences, Queensland Micro- and Nanotechnology Centre, Grifth University, Brisbane, QLD 4111, Australia. 2 State Key Laboratory of Inorganic Synthesis and Preparative Chemistry, College of Chemistry, Jilin University, Changchun 130012, China. 3 Key Laboratory for Ultrane Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai 200237, China. 4 Institute of Physics, Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China. * These authors contributed equally to this work. Correspondence and requests for materials should be addressed to H.G.Y. (email: mailto:[email protected]
Web End [email protected] ) or to S.Q. (email: mailto:[email protected]
Web End [email protected] ) or toX.Y. (email: mailto:[email protected]
Web End [email protected] ).
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ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/ncomms10667
Ni-MOF
Ni@C
A-NiC
Molecular hydrogen (H2), when generated from carbon-neutral processes, plays a vital role in the sustainable energy systems and chemical industry13. Electrolysis
has stood out among various hydrogen production technologies because of high energy-conversion efciency and environmentally benign process, especially coupled with energy sources such as solar and wind46. In this rapidly developed eld, nding active catalysts for hydrogen evolution reaction (HER) to lower large potentials is of paramount importance to promote water electrolysis application. It has been conrmed that platinum (Pt) is the most active and stable electrocatalyst for HER, with only small overpotentials for high reaction rate. However, its low abundance and consequently high cost limit its large-scale commercial applications. Hence, exploring cheap, efcient and durable alternatives of Pt is crucial to facilitate the global scalability of such potential clean-energy technology7. Therefore, a series of Pt-free electrocatalysts have been identied for HER in strong acids, such as metal compounds817 (suldes, nitrides, carbides, borides and phosphides) and carbon-based materials1820. Moreover, remarkable advances in nanostruc-turing or stabilizing these electrocatalysts on carbon substrates have further exposed more active sites simultaneously with enhanced electrical conductivity2127. Recently, design strategies like encapsulating 3d transition metals into carbon nanotubes and graphene nanoshells have been reported to improve the long-term activity2830. Even so, compared with Pt, these reported materials show dwarfed in activity and durability.
Isolated metal atoms, owing to their low-coordination and unsaturated atoms functioned as active sites, have been demonstrated more catalytic active than nanometer-sized metal particles3135. Supported isolated noble metals, such as palladium, Pt and gold, have been reported as highly active catalysts for hydrogenation reactions, CO oxidation reactions and watergas shift reactions3335. However, earth-abundant 3d transition metals, which have been investigated as promising alternatives in alkaline electrolytes36,37, have not been downsized to single atoms to improve their activity for HER so far.
Herein, we show a nickelcarbon (NiC)-based catalyst, which can be tuned by electrochemical methods to obtain atomically isolated Ni species anchored on graphitized carbon, consequently displaying high activity and durability for HER. The activated-NiCarbon (A-NiC) catalyst exhibts overpotential for the current density of 10 mA cm 2, 20 mA cm 2 and 100 mA cm 2 at 34 mV, 48 mV and 112 mV, respectively, a low Tafel
slope of 41 mV per decade and a large exchange current density of1.2 mA cm 2. More importantly, A-NiC could maintain high activity for 425 h in the chronoamperometric test. A variety of analytical techniques illustrate that Ni single atoms formed during the activation process, which could contribute greatly to HER performance. Compared with Pt and other Pt alternatives, A-NiC is composed of more abundant elements in the earths crust. These ndings in our work may help accelerate the large-scale application of proton exchange membrane (PEM) electro-lysers and solar photoelectrochemical (PEC) water electrolysers.
ResultsSythesis and characteration of A-NiC catalyst. A-NiC catalyst was obtained from well-dispersed Ni metal in the graphitized carbon matrix. The synthesized Ni-based metal-organic framework (Ni-MOF) was used as the precursor (Fig. 1). Followed by carbonization at 700 C in nitrogen (N2) atmosphere, Ni nano-particles encapsulated in graphene layers (Ni@C) were prepared. Hydrochloric acid (HCl) leaching treatment was used to remove the redundant Ni metal (HCl-Ni@C). After HCl treatment, hollow onion-like carbon nanoshells along with little Ni
nanoparticles protected by graphene layers remained. We then applied electrochemical cyclic-potential on the HCl-Ni@C catalysts-decorated electrode, unexpected activation process was observed. Similar activation processes were also reported in the literature13,20. To our surprise, direct constant potential on Ni@C can also activate the electrocatalyst, which was conducted until the electrocatalyst reached the optimized and stable activity. We found Ni single atoms formed during all these activation process, which is veried as discussed later.
The nanostructure of Ni@C was characterized by a transmission electron microscope (TEM). Low-magnication TEM image of Ni@C displays Ni metal inside carbon nanospheres (Supplementary Fig. 1a). The size distribution image (Supplementary Fig. 1b) suggests that the nanospheres have an average size around 10 nm. After HCl leaching, the high-resolution TEM image of HCl-Ni@C shows hollow onion-like nanoshells along with little Ni metal aggregates encapsulated in the graphene layers (Fig. 2a). To further study the structure changes of the catalyst before and after activation, a JEM-ARM200F scanning TEM (STEM) tted with a double aberration-corrector for both probe-forming and the imaging lenses was used. In the STEM image of HCl-Ni@C, the measured Ni (111) d-spacing (0.204 nm) and Ni (200) d-spacing (0.176 nm) again conrm the existence of well crystalline Ni metal in the graphitic carbon nanoshells (inset of Fig. 2a). The thickness of graphene layer is uneven with exposure of Ni nanoparticles, which would provide possibilities for slow dissolution of Ni metal during the activation process in the acidic solution. The bright-eld STEM image of A-NiC (Supplementary Fig. 2) illustrates that the measured (002) d-spacing of the graphitic carbon ranges from about 0.33 to0.36 nm, indicating the carbon structure is somewhat disordered, rather than ideally graphitic, which was also evidenced by the X-ray diffraction (XRD) and Raman analysis. Individual metal atoms in practical catalysts can be discerned in the atomic resolution high-angle annular dark-eld (HAADF) images3335. For the sample A-NiC, the atomically isolated Ni species (marked by white circles) are dispersed on the partially graphitized carbon matrix (Fig. 2b). Examination of different regions (Supplementary Fig. 2) conrms abundance of Ni single atoms present in A-NiC. Considering that the elements of N, F and S have a smaller atomic number than Ni, these impuries can hardly exsit as bright tiny spots in the metal-carbon system. HAADF images of controled samples have also ruled out this possiblity (Supplementary Fig. 3). About 78% of the Ni species counted in the images were present as single atoms away from each other (inset of Fig. 2b). A minority of subnanometer Ni clusters present in the same sample did not have the packed Ni atom structure of Ni nanoparticles.
Carbonization
HCl leaching
& activation
Figure 1 | Schematic diagram of synthesis and activation processof the NiC catalysts. The Ni-MOF used as a precursor consists of an orthorhombic crystal. Atoms are shown as follows: C, black; H, white;
O, red; N, blue; Ni, royal blue. Carbonization of the synthesized Ni-MOF was at 700 C in N2 atmosphere to obtain Ni@C. HCl leaching treatment was repeated three times to sufciently dissolve exposed Ni metal. Constant potential and CV treatments were performed to activate the catalysts until they reached the optimal performance and remained stable. During the activation process, Ni single atoms formed in situ anchored on the graphitized carbon.
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NATURE COMMUNICATIONS | DOI: 10.1038/ncomms10667 ARTICLE
a
a
Ni (111)
0.176 nm
0.204 nm Ni (200)
Ni (111)
Ni (200)
Intensity (a.u.)
Intensity (a.u.)
400 800 1,200 1,600 2,000 Raman shift (cm1)
Ni (220)
Ni@C
HCl-Ni@C
A-NiC
10 20 30 40 50 60 70 80
2[afii9835] (degree)
b
b
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Ni@C
2D
100
Percentage (%)
Single atoms
ID/IG = 0.63
D
80
60
Nano clusters
40
2,400 2,800 3,200
20
Figure 3 | Structure characterization of the NiC catalysts. (a) XRD patterns of Ni@C, HCl-Ni@C and A-NiC, respectively. The diffraction peaks of Ni in Ni@C and HCl-Ni@C conrm the existence of well crystalline Ni metal. The red line corresponding to A-NiC illustrates that no NiContaining crystal phase was detected after activation process.(b) Raman spectrum of Ni@C with ID/IG 0.63, indicating the partial
graphitization at 700 C.
0
0.10.3nm
Figure 2 | Micrographs of samples HCl-Ni@C and A-NiC. (a) HRTEM image of HCl-Ni@C. Scale bar, 10 nm. Inset of a, BF STEM image of Ni metal encapsulated in graphene layers. Scale bar, 5 nm. The area of graphene with exposure of Ni nanoparticle provides the opportunity that Ni metal would slowly resolve during the activation process. (b) Subngstrm resolution HAADF STEM image of A-NiC. The circles are drawn around isolated Ni atoms. Scale bar, 3 nm. Inset of b, the size distribution gure, which is based on 4120 observed Ni species counted from high-magnication images (recorded at 4 original magnication).
0.30.5nm
0.51.0nm
The multiple peaks on the XRD pattern of the synthesized Ni-MOF (Supplementary Fig. 4a) well match those of the typical crystalline structure of [Ni2(L-asp)2(bpy)] CH3OH H2O. Ni@C
exhibits the cubic phase of Ni metal (JSPDS NO. 04-0850) with a broad shoulder peak in the range 2030 (2y), which originates from the partially graphitized carbon specie (Fig. 3a). The diffraction peaks of graphitic carbon become higher and sharper with the increased temperature (Supplementary Fig. 4b). Raman spectrum of Ni@C (Fig. 3b) further conrms that the Ni-MOF is partially graphitized at 700 C. Among carbon-based catalysts, these graphitic carbon structures formed during the carbonization treatment may signicantly enhance the electronic conductivity
and corrosion resistance, which would improve the electro-catalytic efciency29. After sufciently washed by HCl, little Ni nanoparticles encapsulated in the multi graphene layers remained. The XRD pattern of HCl-Ni@C proves the existence of the Ni metal. However, no NiContaining signal was detected in the sample A-NiC, primarily attributed to insensitivity of XRD to single atoms or small clusters.
The binding state was investigated by X-ray photoelectron spectroscopy (XPS). As shown in Supplementary Fig. 5, NC bonds in the samples of Ni@C, HCl-Ni@C and A-NiC are in the form of pyridine (398.9 eV), pyrrole (400.4 eV) and graphite (401.3 eV) (refs 28,38). The quantitative analysis of the XPS results reveals that the atomic ratios of N/C in Ni@C, HCl-Ni@C and A-NiC are 4.62:100, 3.80:100 and 2.21:100, respectively. The existence of N dopants in the A-NiC would inherently increase the ability of interacting with reactants and render high positive charge density on their adjacent carbon atoms, which could also
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ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/ncomms10667
contribute to the high activity of A-NiC samples28,29. The Ni 2p XPS spectrum of Ni@C reveals the coexistence of Ni0 (852.8 eV) and Ni2 (853.7 eV), which can be ascribed to Ni-Ni and Ni-O bonding39,40 (Fig. 4a). After HCl leaching, the Ni 2p XPS spectrum of HCl-Ni@C nearly remains the same as that of Ni@C, suggesting the residue of Ni metal. The existence of Ni-O bonding can be attributed to the slow oxidation of the exposed Ni metal41
43. We further collected samples of A-NiC for analysis. The XPS analysis of A-NiC (Supplementary Fig. 6, Supplementary Table 1) illustrates it contains Ni, C, N, F, S and O elements without any Pt impurity, eliminating the inuence of Pt for HER performance. We should point out that F, S and O elements mainly resulted from the Naon solution. To conrm that trace amount of Ni in the A-NiC sample contributes to the HER activity, we determined the Ni contents by indicatively coupled plasma atomic emission spectroscopy. As shown in Supplementary Table 2, the weight ratios of Ni in the Ni@C, HCl-Ni@C and A-NiC were 85.0%, 5.3% and 1.5%, respectively. We found that the Ni content decreased during the CV activation process. What is more, no detectable Pt impurities were found in all these samples. In addition, the Ni 2p XPS spectrum of A-NiC (Fig. 4b) has a sharp peak B860.7 eV, which can be associated with the strong NiF binding. Specically, the peak at 852.8 eV is assigned to Ni0, reecting NiNi binding of the Ni clusters.
Electrocatalytic HER activity evaluation. The HER electro-catalytic activity was evaluated in 0.5 M H2SO4 using a typical three-electrode set-up. All tests were performed without iR compensation. The lineal sweep voltammetry (LSV) curves showing the normalized current density (j) versus voltage (j versus V) for A-NiC and HCl-Ni@C along with commercial Pt/C (5 wt% Pt on Vulcan carbon black), for comparison, are show in Fig. 5a. As expected, Pt/C catalyst exhibits excellent HER performance. HCl-Ni@C requires overpotential (Z) of about
440 mV to reach j of 10 mA cm 2. In sharp contrast, A-NiC produces j of 10 mA cm 2, 20 mA cm 2 and 100 mA cm 2 at Z of 34 mV, 48 mV and 112 mV, respectively. These over-
potentials are the lowest among the reported acid-stable and earth-abundant HER electrocatalysts, including recently reported Ni2P14,
MoP | S16, FeP17, MoS2 (refs 8,22,24), WS2 (refs 21,23,25), Mo2C (refs 12,13) and chemically doped grapheme-based materials1820 (more details in Supplementary Table 3).
To understand the detailed underlying mechanism of HER activity, Tafel plots based on LSV curves were acquired (Fig. 5b). The linear regions of Tafel plots were t to the Tafel equation (Z b log j a, where b is the Tafel slope), yielding
Tafel slopes of B34, 41, 194 mV per decade for Pt/C, A-NiC and HCl-Ni@C, respectively. The value for A-NiC does not correspond to one of the standard HER Tafel slopes (29, 38, 116 mV per decade), indicating the HER occurs through a VolmerHeyrovsky mechanism and electrochemical recombination with an additional proton is the rate-limiting step28. Moreover, the exchange current density (j0) was obtained by extrapolation of Tafel plots (Supplementary Fig. 7). The j0 of
A-NiC is about 1.2 mA cm 2 (the same magnitude as the value of 2.5 mA cm 2 for Pt/C), also highlighting the exceptional H2 evolving efciency of A-NiC catalyst.
The optimal activity of A-NiC catalyst would also be attributed to strong chemical and electronic coupling between graphitized carbon and Ni single atoms, permitting highly efcient electrical communication between the catalytic active sites and the underlying electrode substrate. Electrochemical impedance spectroscopy measurements were performed to conrm the hypothesis (Fig. 5c). The charge transfer resistance of A-NiC is similar to that of Pt/C, which is much lower than that of HCl-Ni@C. Thus, much faster electron transfer between the catalytic active sites of A-NiC and the electrode substrate is one of the key factors contributing to the superior HER kinetics.
Durability of A-NiC catalyst. The durability is a key concern of all catalysts. In this study, accelerated degradation measurements were adopted to evaluate the durability. Cyclic voltammetric (CV) sweeps between 905 mV and 95 mV versus the reversible
hydrogen electrode potential (versus RHE) at 100 mV s 1 were applied to HCl-Ni@C-decorated glassy carbon (GC) electrode.
Post-potential-cycling LSV curves were recorded (Supplementary Fig. 8). HER performance after 8,000 cycles retained almost the same to the test after 4,000 cycles. To further probe the durability of A-NiC in the acidic environment, continuous HER at a static overpotential was conducted (Fig. 5d). When operating a constant overpotential of 45 mV, a continuous HER process
occurred to generate molecular H2 (different overpotentials were applied to generate H2 shown in Supplementary Movie 1). During the rst 11 h, the current density of B10 mA cm 2 was observed, and then gradually increased to B14 mA cm 2, which might be caused by adequate activation of the catalyst. In addition, the current density levelled out at B12 mA cm 2. It should be mentioned that the high activity was maintained for 425 h in the chronoamperometric electrolysis (after CV activation, Z4,000
a
Main peak
Ni0
Ni0
Ni 2p3/2
Intensity (a.u.)
Intensity (a.u.)
Ni@C
HCl-Ni@C
Satellite peak
845 850 855
Binding energy (eV)
860 865
b
NiF
Main peak
Ni 2p3/2
Ni2+
Ni2+
A-NiC
845 850 855
Binding energy (eV)
860 870
865
Figure 4 | XPS spectra of the NiC catalysts. (a) XPS spectra of Ni 2p peaks of Ni@C and HCl-Ni@C. (b) XPS spectrum of Ni 2p peaks of A-NiC. The peaks at 852.8 eV and 853.7 eV are assigned to Ni0 and Ni2 , respectively. The sharp peak at 860.7 eV can be correlated with NiF binding, and the element F comes from Naon solution.
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a
b
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HCl-Ni@C
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(mA cm2 )
Overpotential (V)
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Pt/C 194 mV per decade
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Current density
(mA cm2 )
8
4
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6 8 10 12 14 16 18
0 0 400
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Z ()
Time (h)
Figure 5 | HER electrocatalytic properties of the NiC catalysts. (a) LSV curves of HCl-Ni@C, A-NiC and Pt/C. (b) Tafel plots obtained from LSV curves in a, indicating signicant improvement in activity for HER after activation. (c) EIS spectra of HCl-Ni@C, A-NiC and Pt/C at the overpotential of 100 mV.
Inset of c represents a close-up view of the spectra at high frequencies. A-NiC-modied GC electrode displays much lower impedance than HCl-Ni@C-modied GC electrode, similar to that of Pt/C-modied GC electrode. (d) Chronoamperometric curve of A-NiC at Z 45 mV, revealing nearly no
apparent deactivation after 25 h. Note: all the electrochemical data of A-NiC catalysts were obtained after electrochemical cyclic-potential activation.
a
Constant-potential activation at [afii9834] = 200mV
0 min
5 min
30 min
60 min
120 min
b
c
d
Ni@C
4
Oxidation peak intensity trend
Under constant-potential activation
0
Current density (mA cm2 )
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Current density (mA cm2 )
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HCl-Ni@C
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Scan atfer 4 h
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Under cyclic-potential activation
Activity trend
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0.5
0.4
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Potential (V vs RHE) Potential (V vs RHE) Potential (V vs RHE)
Figure 6 | Activation processes of the NiC catalysts. (a) Hydrogen bubbles driven at Z 100 mV at GC electrodes with different degrees of activation
(constant-potential activation at Z 200 mV for different time). All the digital photos were taken when the cell turned on for 20 s. The diameter of
glassy carbon electrode is 5 mm. (b) Initial and post-constant-potential activation LSV curves of Ni@C. The applied constant potential would activate Ni@C catalyst. (c) Cyclic voltammograms of HCl-Ni@C (cycle 1, cycle 1,000, cycle 2,000, cycle 2,500, cycle 3,000 and cycle 4,000 were selected). Catalytic activity trend corresponds to the improving current density. (d) Oxidation peaks of the catalyst in different cycles. The oxidation peak intensity increased and the peak potentials shifted in the negative direction in the anodic-going scan.
cycles). Furthermore, we did the galvanostatic electrolysis test to collect the evolved hydrogen gas to evaluate the Faradaic efciency of the A-NiC catalyst. In Supplementary Fig. 9, the result
demonstrates that A-NiC gives about 100% Faradaic yield during the electrolysis process. Overall, the high catalytic activity and outstanding durability illustrate the potential of A-NiC for
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ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/ncomms10667
cost-effective electrocatalytic hydrogen evolution in water electrolysis system and solar-driven hydrogen system.
Activation processes. Activation processes (constant-potential activation and cyclic-potential activation) were also recorded to investigate changes after activation. Hydrogen bubbles generated at Z 100 mV on Ni@C-decorated GC electrodes with differ
ent degrees of activation (Fig. 6a). Constant potential at Z of
200 mV (Supplementary Fig. 10) was used to stabilize the catalyst to reach the best performance, simultaneously ruling out the possibility that the high j would result from the reaction between the unsecure Ni metal and the strongly acidic solution. The j gradually improved in the rst 2 h and levelled out in the next 2 h. These activation treatments also ensured stable and reproducible results. LSV curves of Ni@C after different periods of constant-potential activation prove the activation process of Ni@C (Fig. 6b). During CV activation process, the catalytic j of HCl-Ni@C gradually increased with the consecutive CV scans and reached the maximum efciency after about 4,000 cycles (Fig. 6c). Notably, the anodic peaks around 0 V (versus RHE) shifted to lower potentials during the process, indicating a more easily occurring oxidation reaction. Interestingly, the oxidation peak intensities were also enhanced during the CV treatment (Fig. 6d). These signs during CV activation reveal that A-NiC could lose electrons more easily in the anodic-going scan. The oxidation peak intensity gradually levelled out when the cathodic catalytic j nearly remained stable (Supplementary Fig. 11). These changes of the oxidation peak corresponding to valance changes of Ni coincide with the trend of the catalytic activity. In addition, we also collected the activated samples after different CV cycles for STEM analysis (Supplementary Figs 12 and 13). The down-sizing of the Ni nanoparticles and the formation of single Ni atoms can be evident to be observed during the activation process. Throughout the detailed CV activation process, we summarize that active Ni single atoms would form during the activation process, leading to these changes of the oxidation peak and simultaneously contributing greatly to the improved activity. Furthermore, the HCl-Ni@C samples can also be activated on the uorine-doped SnO2 (FTO) glass substrate (Supplementary
Figs 14 and 15).
DiscussionIn summary, we have used carbonization of MOFs to synthesize NiC-based catalyst and applied electrochemical potential to activate NiC catalyst, which can reach outstanding performance during HER processes. The discovery of this A-NiC catalyst highlights a new area of tuning structure and functionality of metal-carbon-based catalyst at atomic scale by electrochemical methods, which would hold the promise for large-scale real-world water splitting electrolysers.
Methods
Chemicals. Nickel (II) carbonate basic hydrate (4850% Ni, Fluka), L-aspartic acid (98%, Sigma-Aldrich), 4,40-bipyridyl (98%, Alfa Aesar), Naon-117 solution (5 wt. % in a mixture of lower aliphatic alcohols and water) (Sigma-Aldrich), sulphuric acid (98%, Merck) and HCl (32%, RCI labscan) were used as received without any further purication.
Synthesis of Ni(L-asp)(H2O)2 . H2O. Measured amount of NiCO3 2Ni(OH)2
H2O (2.450 g) and L-aspartic acid (2.630 g) were dissolved in water (200 ml) under stirring and heating for 3 h. After ltering out all the remaining solid particles, the clear turquoise solution was then evaporated at 80 C oven overnightto obtain the pale blue Ni(Asp) powder.
Synthesis of [Ni2(L-asp)2(bpy)] . CH3OH . H2O (Ni-MOF). Ni(L-asp)(H2O)2
H2O (0.219 g) and 4,40-bipyridyl (0.312 g) were dispersed in a mixture containing water (6 mL) and methanol (4.742 g) under ultrasonic vibration. The nal solution
was sealed into an autoclave and heated at 150 C for 48 h. The product, [Ni2(L-asp)2(bpy)] CH3OH H2O, was ltered, washed with copious amounts of water
and methanol and dried at 60 C for 24 h.
Carbonization of Ni-MOF. Carbonization processes were carried out in N2 atmosphere. The dried Ni-MOF powder was pretreated at 150 C for 2 h and then carbonized at different temperatures for 5 h with a heating rate of 5 C min 1.
HCl leaching treatment. Excess concentrated HCl was slowly added into Ni@C hybrids and then the suspension was put under ultrasonic condition to dissolve Ni metal. The suspension was separated when being left to stand for 6 h. The entire process was repeated two additional times. Then the product was washed with copious amount of water until the pH of the solution was B7 and then dried at 60 C for 24 h.
Electrochemical measurements. All the electrochemical tests were performed in a conventional three-electrode system at an electrochemical station (CHI 660E), using Ag/AgCl (3.5 M KCl solution) electrode as the reference electrode, Pt mesh as the counter electrode and GC electrode as the working electrode. About 4 mg of sample and 80 ml of 5 wt% Naon solution were dispersed in 1 ml of 4:1 v/v water/
ethanol by at least 30-min sonication to form a homogeneous solution. Then 5 ml or 15 ml of the solution was loaded onto the GC electrode of 3 mm or 5 mm in diameter, respectively. The nal loading for all catalysts and commercial Pt/C electrocatalysts on the GC electrodes is about 0.283 mg cm 2. Similar preparation of titanium foil electrode was conducted with the same loading of the HCl-Ni@C samples and corresponding chronoamperometric curves of A-NiC was shown in Supplementary Fig. 16. LSV with scan rate of 5 mV s 1 was conducted in 0.5 M
H2SO4 deaerated with argon at room temperature. The Ag/AgCl/3.5 M KCl reference electrode was calibrated with respect to RHE. The calibration was performed in the high purity hydrogen saturated electrolyte with Pt mesh as the working electrode and counter electrode. CVs were run at a scan rate of 1 mV s 1, and the average of the two potentials at which the current crossed zero was taken to be the thermodynamic potential for the hydrogen electrode reactions (Supplementary Fig. 17). In 0.5 M H2SO4, ERHE E
Ag/AgCl
0.209 V. AC impedance measurements were carried out in the same conguration when the working electrode was biased at the overpotential of 100 mV from 105 Hz to 10 1 Hz with an AC voltage of 5 mV. The CV measurements were performed by use of the scan rate at 100 mV s 1 between 905 mV and 95 mV (versus RHE) without
accounting for uncompensated resistance. Chronoamperometric measurement (Z 45 mV) was performed to evaluate the long-term stability. The faradaic
yield was calculated from the total amount of electrons passed through the cell during the galvanostatic electrolysis and the amount of the evolved H2 gas collected by the water drainage method. The theoretically expected amount of H2 was calculated by applying the Faraday law, which states that the passage of 96485.4 C causes 1 equiv. of reaction. The HER performance mentioned above was well reproducible in our laboratory. More than 10 A-Ni-C-decorated GC electrodes (after CV activation) were evaluated, giving similar activation phenomenon and negligible difference of HER performance.
Characterization. XRD patterns were acquired at room temperature using D/MAX 2550 VB/PC. Raman spectrum was recorded on a Rennishaw InVia spectrometer with a model 100 Ramascope optical bre instrument. XPS data were collected from ESCALAB 250Xi, and the binding energy of the C 1 s peak at 284.8 eV was taken as an internal reference. TEM images were collected from TECNAI F-30 with an acceleration voltage of 300 kV. Subngstrm resolution STEM images were obtained on a JEM-ARM200F STEM tted with a double aberration-corrector for both probe-forming and the imaging lenses.
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Author contributions
X.Y., S.Q. and H.G.Y. conceived the project and contributed to the design of the
experiments and analysis of the data. L.F. and P.F.L. performed the catalyst preparation,
characterizations and wrote the paper. Z.Z.Y. and L.G. conducted the STEM examination
and contributed to writing the STEM section. L.F., P.F.L. and X.Y. collected the
electrochemical data. All the authors discussed the results and commented on the
manuscript.
Additional information
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How to cite this article: Fan, L. et al. Atomically isolated nickel species anchored on
graphitized carbon for efcient hydrogen evolution electrocatalysis. Nat. Commun.
7:10667 doi: 10.1038/ncomms10667 (2016).
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Copyright Nature Publishing Group Feb 2016
Abstract
Hydrogen production through electrochemical process is at the heart of key renewable energy technologies including water splitting and hydrogen fuel cells. Despite tremendous efforts, exploring cheap, efficient and durable electrocatalysts for hydrogen evolution still remains as a great challenge. Here we synthesize a nickel-carbon-based catalyst, from carbonization of metal-organic frameworks, to replace currently best-known platinum-based materials for electrocatalytic hydrogen evolution. This nickel-carbon-based catalyst can be activated to obtain isolated nickel atoms on the graphitic carbon support when applying electrochemical potential, exhibiting highly efficient hydrogen evolution performance with high exchange current density of 1.2 mA cm-2 and impressive durability. This work may enable new opportunities for designing and tuning properties of electrocatalysts at atomic scale for large-scale water electrolysis.
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