High-performance hydrogen evolution electrocatalysis by layer-controlled MoS2 nanosheets

Jiao Denga, Wentao Yuanb, Pengju Rena, Yong Wangb, Dehui Deng*a, Ze Zhangb and Xinhe Baoa
aState Key Laboratory of Catalysis, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Zhongshan Road 457, Dalian, 116023, China. E-mail: dhdeng@dicp.ac.cn; Fax: +86-411-8469 4447; Tel: +86-411-8246 3003
bDepartment of Materials Science and Engineering, Zhejiang University, Zheda Road 38, Hangzhou, ZheJiang 310027, China

Received 11th June 2014 , Accepted 23rd July 2014

First published on 23rd July 2014


Abstract

Hydrogen is considered as an important clean energy carrier for the future, and electrocatalytic splitting of water is one of the most efficient technologies for hydrogen production. As a potential alternative to Pt-based catalysts in hydrogen evolution reaction (HER), two-dimensional (2D) molybdenum sulfide (MoS2) nanomaterials have attracted enormous research interest, while the structure control for high-performance HER electrocatalysis remains a considerable challenge due to the lack of efficient preparation techniques. Herein, we reported a one-pot chemical method to directly synthesize 2D MoS2 with controllable layers. Multiple-layer MoS2 (ML-MoS2), few-layer MoS2 (FL-MoS2) and single-layer MoS2 coating on carbon nanotubes (SL-MoS2-CNTs) can be efficiently prepared through the modulation of experimental conditions. The enhanced catalytic activity in HER is demonstrated by reducing the layer number of MoS2 nanosheets. Remarkably, the optimized SL-MoS2-CNTs sample showed long-term durability with an accelerated degradation experiment even after more than 10[thin space (1/6-em)]000 recycles, and high HER activity with an onset overpotential of only ∼40 mV vs. RHE. This study introduces a novel, cheap and facile strategy to prepare layer-controlled 2D MoS2 nanosheets in a large quantity, and is expected to broaden the already wide range energy applications of 2D MoS2 nanosheets.


Context

Two-dimensional (2D) molybdenum sulfide (MoS2) nanomaterials have attracted significant research interest because of their intriguing structural and electronic properties as well as numerous potential applications in many energy fields, such as electronic devices,1–3 lithium batteries4–6 and electrocatalytic hydrogen evolution from water.7–10 Bulk MoS2 consists of several single-layer MoS2 nanosheets, which are linked by van der Waals force, and each sheet is made up of a hexagonal layer of molybdenum atoms between two hexagonal layers of sulfur atoms. Previous studies indicate that few-layer, especially single-layer, MoS2 possesses distinctively different physical and chemical properties compared with their bulk counterparts, viz. stronger photoluminescence,11 greater luminescence quantum efficiency12 and higher on–off ratio of transistors.2,13 Therefore, extensive efforts have been devoted for the preparation of few-layer and single-layer MoS2 nanosheets. Presently, there are mainly two strategies: top-down methods, including mechanical exfoliation,14,15 chemical exfoliation,16,17 electrochemical lithium intercalation,18,19 laser thinning20 and ball milling,21 and bottom-up methods, including chemical vapor deposition on substrates22,23 and chemical synthesis.18,24,25 Although significant progress has been made by several research groups, controlling the layer numbers of these materials still remains a considerable challenge. In particular, for the chemical synthesis methods in the liquid phase, reaction-intermediates are usually unstable and tend to form quasi-0D nanoparticles or 3D bulk materials during the preparation process.26,27

Herein, we report a facile and scalable strategy for the production of MoS2 nanosheets with controllable layers via the direct chemical reaction of hexaammonium heptamolybdate ((NH4)6Mo7O24) and carbon disulfide (CS2) under mild conditions. The layer number of MoS2 nanosheets can be efficiently controlled by modulating the experimental conditions, i.e. synthesis under H2O-free environment for multiple-layer MoS2 (ML-MoS2), and synthesis process under H2O-assisted environment for few-layer MoS2 (FL-MoS2). On the basis of this method, we can further prepare single-layer (SL) MoS2 coating on carbon nanotubes (SL-MoS2-CNTs) by adding CNTs in the precursors. This method can easily scale up because the throughput is only limited by the size of the autoclave (for more details, see the Experimental section in ESI). The significantly enhanced catalytic activity is demonstrated in a hydrogen evolution reaction (HER) by reducing the layer number of MoS2 nanosheets. Remarkably, the optimized SL-MoS2-CNTs samples showed long-term durability and high HER activity with an onset overpotential of only ∼40 mV vs. RHE.

The morphology and structure of MoS2 nanosheets were examined by scanning electron microscopy (SEM) and transmission electron microscopy (TEM). One can see that FL-MoS2 exhibits a typical 3D flower-like morphology, which consists of MoS2 nanosheets (Fig. 1a and b). Further, the high resolution (HR) TEM image shows that these nanosheets mainly contain 1–5 layers (L) (Fig. S1d) with a layer distance of 0.62 nm, corresponding to the (002) plane of MoS2 (Fig. 1c). The sub-angstrom resolution high angle annular dark field-scanning transmission electron microscopy (HAADF-STEM) images (Fig. 1d and S2a) reveal that the honeycomb arrangement of the atoms extend over the entire nanosheet of FL-MoS2, and the corresponding energy dispersive X-ray (EDX) mapping images reveal that the distribution of molybdenum atoms and sulfur atoms in the entire nanosheet is very homogeneous (Fig. 1e and f and S2b and S2c), further confirming the structural feature of MoS2 nanosheets. In comparison, the ML-MoS2 presents an irregular aggregation (Fig. S3a) with an obvious thicker nanosheet structure compared with FL-MoS2, i.e. the average layer number is ca. 6 L for ML-MoS2 and 3 L for FL-MoS2, as obtained from the statistical analysis of the HRTEM images in Fig. 2b and S1d and S3d. In addition, when CNTs are added during synthesis, it is interesting to find that MoS2 nanosheets tend to continuously coat on CNTs (Fig. 1g–i), and most of the layer numbers (more than 70%) are 1 L (Fig. 2b and S4d).


image file: c4ra05614k-f1.tif
Fig. 1 (a) SEM image of FL-MoS2. (b) TEM image of FL-MoS2. (c) HRTEM image of FL-MoS2 with inset showing a layer distance of 0.62 nm. (d) HAADF-STEM image of FL-MoS2 with the inset showing a honeycomb arrangement of MoS2; blue and yellow dots represent Mo and S, respectively. The scale bar in the inset is 0.5 nm. The area with the dashed circles shows the defects in the nanosheets. (e) and (f) EDX mapping images of Mo and S for FL-MoS2 corresponding to figure (d). (g)–(i) HRTEM images of SL-MoS2-CNTs.

image file: c4ra05614k-f2.tif
Fig. 2 (a) XRD patterns of SL-MoS2-CNTs, FL-MoS2 and ML-MoS2 in comparison to bulk MoS2. (b) Intensity ratio of the MoS2 (002) peak and MoS2 (110) peak (I(002)/(100)) for bulk MoS2, ML-MoS2, FL-MoS2 and SL-MoS2-CNTs in XRD, and the average layer number of ML-MoS2, FL-MoS2 and SL-MoS2-CNTs obtained from the statistical analysis by HRTEM in Fig. S1, S3 and S4, respectively. (c) Raman spectra of SL-MoS2-CNTs, FL-MoS2 and ML-MoS2 in comparison to bulk MoS2.

X-ray diffraction (XRD) and Raman spectroscopy were used to further analyze the layer structure of these MoS2 samples. As observed in the XRD patterns in Fig. 2a, all the samples exhibited the typical (002), (100), (103) and (110) planes of hexagonal 2H-MoS2. Because the (002) reflection of MoS2 is the characteristic peak for the c axis and (100) for the ab plane, we can take the intensity ratio between (002) and (100) peaks (I(002)/(100)) of MoS2 to assess the layer number variation in the series of these samples. One can see the ratio I(002)/(100) of bulk MoS2 (22.67), ML-MoS2 (1.69), FL-MoS2 (0.85) and SL-MoS2-CNTs (0.28) decrease gradually (Fig. 2b), indicating that the layer number of these MoS2 samples also decreases. In addition, all the Raman spectra (Fig. 2c) of these MoS2 samples showed two characteristic peaks at 390 and 415 cm−1 corresponding to the E2g1 and A1g modes of the hexagonal MoS2 crystal, respectively. It is reported that the frequency of A1g mode will have a red-shift as the layer number of MoS2 decreases.28–30 As expected, an obvious red-shift of A1g modes was observed from bulk MoS2 to FL-MoS2, indicating that the layer number decreases gradually in these samples, which is in good agreement with the XRD and HRTEM analysis. Note that there was a slight blue-shift of the A1g modes from FL-MoS2 to SL-MoS2-CNTs, which was probably due to the presence of a strain introduced by the increase in curvature of MoS2 nanosheets when coating onto the CNTs.31,32

The above mentioned results demonstrate that MoS2 nanosheets with controllable layers have been successfully synthesized via a one-step reaction between (NH4)6Mo7O24 and CS2 with appropriately chosen conditions, and we propose a possible mechanism for this method. As depicted in Scheme 1, the direct reaction of (NH4)6Mo7O24 and CS2 will form the small 2D domains of MoS2 and then assemble into multiple-layer MoS2 nanosheets due to the interaction via the van der Waals force between the layers. When the reaction was assisted with H2O, the layer-assembling was partly hindered due to the adsorbed H2O molecules around them, hence leading to thinner nanosheets. When CNTs are introduced in the H2O-assisted reaction, the CNTs can serve as templates to immobilize the small MoS2 domains during the reaction, which further hinders the layer-assembling and finally leads to the formation of a single-layer MoS2 nanosheets coating on the surface of the CNTs. The mechanism of MoS2 nanosheets growing on CNTs here should be similar with that on the other templates, e.g. graphene.33,34


image file: c4ra05614k-s1.tif
Scheme 1 Schematic illustration for the direct chemical synthesis of multiple-layer MoS2 (ML-MoS2), few-layer MoS2 (FL-MoS2) and single-layer MoS2 coating on carbon nanotubes (SL-MoS2-CNTs) by modulating the experimental conditions.

2D MoS2 based nanomaterials have been regarded as a promising non-precious catalysts for hydrogen evolution reaction (HER), and have stimulated great research interest in the past few years.35–41 Previous experimental and computational studies indicated that the activity of hydrogen evolution reaction (HER) originates from the edges and defects of MoS2 nanosheets.8,35,36,42,43 It implies that increasing the edges and defects in MoS2 nanosheets will efficiently promote the HER activity. In this study, we find that reducing the layer number of MoS2 nanosheets will introduce mass defects in these nanosheets, as observed in Fig. 1d and S4, implying that the HER activity could be enhanced by reducing the layer number of MoS2 nanosheets. Therefore, we investigate the effect of layer numbers of MoS2 nanosheets on the HER activity and expect that the optimization of MoS2 catalysts can enhance the HER performance. The HER electrochemical measurements were performed by a typical three-electrode setup in 0.1 M H2SO4. As shown in Fig. 3a, all the prepared MoS2 samples exhibited high activity compared with bulk MoS2 and blank glassy carbon (GC) electrode. Moreover, the HER activity increases significantly as the layer number of MoS2 nanosheets reduces, i.e. the HER onset overpotential is ∼200 mV for bulk MoS2, ∼110 mV for ML-MoS2 and ∼50 mV for FL-MoS2 (see Table S1). Remarkably, the polarization curve of SL-MoS2-CNTs shows an onset overpotential of only ∼40 mV vs. RHE, beyond which the cathodic current increased rapidly under more negative potentials. Further, the overpotential at a current density of 10 mA cm−2 is 236 mV, showing that SL-MoS2-CNTs is amongst the most active non-precious HER catalysts in an acidic medium.37,43–47 In addition, the HER exchange current density (j0), normalized by the mass loading of these catalysts can be favorably compared to that of some reported outstanding MoS2-based catalysts (Table S2). The high HER activity of SL-MoS2-CNTs may arise from the increasing defects in the single layer, as well as the enhanced electrical conductivity of CNTs that promotes electron transfer during the reaction. The Tafel slope is often used to reveal the inherent property of HER electrocatalysts: a smaller Tafel slope will lead to a faster increment of the HER rate with increasing overpotential.8 As shown in Fig. 3b, the Tafel slope of SL-MoS2-CNTs is 63 mV dec−1, much smaller compared with FL-MoS2 (87 mV dec−1) and ML-MoS2 (110 mV dec−1), further confirming that SL-MoS2-CNTs possess higher HER activity.


image file: c4ra05614k-f3.tif
Fig. 3 (a) Polarization curves of SL-MoS2-CNTs, FL-MoS2, and ML-MoS2 in comparison with bulk MoS2, CNTs, 40% Pt/C and blank GC electrode. (b) Tafel plots of ML-MoS2, FL-MoS2, SL-MoS2-CNTs and 40% Pt/C. (c) Durability measurements of SL-MoS2-CNTs and FL-MoS2. The polarization curves recorded initially and after 10[thin space (1/6-em)]000 CV sweeps between +0.57 and −0.13 V (vs. RHE). (d) Potential values recorded initially and after every 1000 CV sweeps for SL-MoS2-CNTs and FL-MoS2 at 1 mA cm−2 and 10 mA cm−2.

Durability is another important criterion to evaluate a HER electrocatalyst. Herein, accelerated degradation experiments were adopted to conduct the evaluation. After every 1000 cyclic voltammetric (CV) sweeps between −0.13 and +0.57 V (vs. RHE), a polarization curve was recorded. From Fig. 3c, one can see that the SL-MoS2-CNTs retains almost the same activity as the initial, even after 10[thin space (1/6-em)]000 recycles. In contrast, FL-MoS2 exhibits an obvious degradation in the activity. Moreover, from the potential values recorded at the same current density of 1 mA cm−2 and 10 mA cm−2 with different CV sweeps in Fig. 3d, one can see that SL-MoS2-CNTs shows higher durability with negligible increase in overpotential compared with FL-MoS2. Considering that more edges and defects will be introduced in MoS2 nanosheets as the layer number are reduced, the structural stability of MoS2 will reduce and usually lead to a decrease in the catalytic durability. However, in this study, the single-layer MoS2 on CNTs shows even higher durability than free-standing few-layer nanosheets. We deduce that the introduction of CNTs may enhance the interaction of CNTs and MoS2 nanosheets, which can efficiently hinder the degradation of HER durability.

In summary, we introduce a facile and efficient chemical method to directly synthesize 2D MoS2 nanosheets with controllable layers. Within the method, both free-standing MoS2 nanosheets and single-layer MoS2 coating on CNTs can be efficiently prepared via the modulation of experimental conditions. These MoS2 nanosheets exhibit a significant layer number effect on the hydrogen evolution reaction (HER), i.e. the HER activity will be enhanced by reducing the layer number. Remarkably, the optimized SL-MoS2-CNTs samples showed long-term durability with more than 10[thin space (1/6-em)]000 recycles and high HER activity with an onset overpotential of only ∼40 mV vs. RHE. These resulting layer-controlled MoS2 nanosheets are expected to find potential applications as non-precious HER catalysts as well as in other fields such as electronics and lithium batteries.

Acknowledgements

We gratefully acknowledge the financial support from the National Natural Science Foundation of China (no. 21303191 and 51390474) and the strategic Priority Research Program of the Chinese Academy of Sciences (no. XDA09030100), and thank Prof. Ting Yu at Nanyang Technological University for fruitful discussions on Raman analysis.

References

  1. M. S. Xu, T. Liang, M. M. Shi and H. Z. Chen, Chem. Rev., 2013, 113, 3766–3798 CrossRef CAS PubMed.
  2. B. Radisavljevic, A. Radenovic, J. Brivio, V. Giacometti and A. Kis, Nat. Nanotechnol., 2011, 6, 147–150 CrossRef CAS PubMed.
  3. Q. H. Wang, K. Kalantar-Zadeh, A. Kis, J. N. Coleman and M. S. Strano, Nat. Nanotechnol., 2012, 7, 699–712 CrossRef CAS PubMed.
  4. T. Stephenson, Z. Li, B. Olsen and D. Mitlin, Energy Environ. Sci., 2014, 7, 209–231 CAS.
  5. M. Chhowalla, H. S. Shin, G. Eda, L. J. Li, K. P. Loh and H. Zhang, Nat. Chem., 2013, 5, 263–275 CrossRef PubMed.
  6. Z. Wang, T. Chen, W. X. Chen, K. Chang, L. Ma, G. C. Huang, D. Y. Chen and J. Y. Lee, J. Mater. Chem. A, 2013, 1, 2202–2210 CAS.
  7. M. R. Gao, Y. F. Xu, J. Jiang and S. H. Yu, Chem. Soc. Rev., 2013, 42, 2986–3017 RSC.
  8. D. Merki and X. L. Hu, Energy Environ. Sci., 2011, 4, 3878–3888 CAS.
  9. J. Yang and H. S. Shin, J. Mater. Chem. A, 2014, 2, 5979–5985 CAS.
  10. A. B. Laursen, S. Kegnaes, S. Dahl and I. Chorkendorff, Energy Environ. Sci., 2012, 5, 5577–5591 CAS.
  11. G. Eda, H. Yamaguchi, D. Voiry, T. Fujita, M. W. Chen and M. Chhowalla, Nano Lett., 2011, 11, 5111–5116 CrossRef CAS PubMed.
  12. K. F. Mak, C. Lee, J. Hone, J. Shan and T. F. Heinz, Phys. Rev. Lett., 2010, 105, 136805–136808 CrossRef.
  13. Y. J. Zhang, J. T. Ye, Y. Matsuhashi and Y. Iwasa, Nano Lett., 2012, 12, 1136–1140 CrossRef CAS PubMed.
  14. K. S. Novoselov, D. Jiang, F. Schedin, T. J. Booth, V. V. Khotkevich, S. V. Morozov and A. K. Geim, Proc. Natl. Acad. Sci. U. S. A., 2005, 102, 10451–10453 CrossRef CAS PubMed.
  15. H. Li, Z. Y. Yin, Q. Y. He, H. Li, X. Huang, G. Lu, D. W. H. Fam, A. I. Y. Tok, Q. Zhang and H. Zhang, Small, 2012, 8, 63–67 CrossRef CAS PubMed.
  16. J. N. Coleman, M. Lotya, A. O'Neill, S. D. Bergin, P. J. King, U. Khan, K. Young, A. Gaucher, S. De, R. J. Smith, I. V. Shvets, S. K. Arora, G. Stanton, H. Y. Kim, K. Lee, G. T. Kim, G. S. Duesberg, T. Hallam, J. J. Boland, J. J. Wang, J. F. Donegan, J. C. Grunlan, G. Moriarty, A. Shmeliov, R. J. Nicholls, J. M. Perkins, E. M. Grieveson, K. Theuwissen, D. W. McComb, P. D. Nellist and V. Nicolosi, Science, 2011, 331, 568–571 CrossRef CAS PubMed.
  17. K. G. Zhou, N. N. Mao, H. X. Wang, Y. Peng and H. L. Zhang, Angew. Chem., Int. Ed., 2011, 50, 10839–10842 CrossRef CAS PubMed.
  18. H. S. S. R. Matte, A. Gomathi, A. K. Manna, D. J. Late, R. Datta, S. K. Pati and C. N. R. Rao, Angew. Chem., Int. Ed., 2010, 49, 4059–4062 CrossRef CAS PubMed.
  19. Z. Y. Zeng, Z. Y. Yin, X. Huang, H. Li, Q. Y. He, G. Lu, F. Boey and H. Zhang, Angew. Chem., Int. Ed., 2011, 50, 11093–11097 CrossRef CAS PubMed.
  20. A. Castellanos-Gomez, M. Barkelid, A. M. Goossens, V. E. Calado, H. S. J. van der Zant and G. A. Steele, Nano Lett., 2012, 12, 3187–3192 CrossRef CAS PubMed.
  21. Y. G. Yao, Z. Y. Lin, Z. Li, X. J. Song, K. S. Moon and C. P. Wong, J. Mater. Chem., 2012, 22, 13494–13499 RSC.
  22. X. S. Wang, H. B. Feng, Y. M. Wu and L. Y. Jiao, J. Am. Chem. Soc., 2013, 135, 5304–5307 CrossRef CAS PubMed.
  23. W. J. Zhang, J. K. Huang, C. H. Chen, Y. H. Chang, Y. J. Cheng and L. J. Li, Adv. Mater., 2013, 25, 3456–3461 CrossRef CAS PubMed.
  24. C. Altavilla, M. Sarno and P. Ciambelli, Chem. Mater., 2011, 23, 3879–3885 CrossRef CAS.
  25. Y. Y. Peng, Z. Y. Meng, C. Zhong, J. Lu, W. C. Yu, Y. B. Jia and Y. T. Qian, Chem. Lett., 2001, 30, 772–773 CrossRef.
  26. M. M. Mdleleni, T. Hyeon and K. S. Suslick, J. Am. Chem. Soc., 1998, 120, 6189–6190 CrossRef CAS.
  27. R. Tenne, Nat. Nanotechnol., 2006, 1, 103–111 CrossRef CAS PubMed.
  28. H. Li, Q. Zhang, C. C. R. Yap, B. K. Tay, T. H. T. Edwin, A. Olivier and D. Baillargeat, Adv. Funct. Mater., 2012, 22, 1385–1390 CrossRef CAS PubMed.
  29. C. Lee, H. Yan, L. E. Brus, T. F. Heinz, J. Hone and S. Ryu, ACS Nano, 2010, 4, 2695–2700 CrossRef CAS PubMed.
  30. G. Plechinger, S. Heydrich, J. Eroms, D. Weiss, C. Schuller and T. Korn, Appl. Phys. Lett., 2012, 101, 101906 CrossRef PubMed.
  31. M. Virsek, A. Jesih, I. Milosevic, M. Damnjanovic and M. Remskar, Surf. Sci., 2007, 601, 2868–2872 CrossRef CAS PubMed.
  32. E. Scalise, M. Houssa, G. Pourtois, V. V. Afanasev and A. Stesmans, Phys. E, 2014, 56, 416–421 CrossRef CAS PubMed.
  33. K. Chang and W. X. Chen, Chem. Commun., 2011, 47, 4252–4254 RSC.
  34. X. S. Zhou, L. J. Wan and Y. G. Guo, Chem. Commun., 2013, 49, 1838–1840 RSC.
  35. B. Hinnemann, P. G. Moses, J. Bonde, K. P. Jorgensen, J. H. Nielsen, S. Horch, I. Chorkendorff and J. K. Nørskov, J. Am. Chem. Soc., 2005, 127, 5308–5309 CrossRef CAS PubMed.
  36. T. F. Jaramillo, K. P. Jorgensen, J. Bonde, J. H. Nielsen, S. Horch and I. Chorkendorff, Science, 2007, 317, 100–102 CrossRef CAS PubMed.
  37. Y. G. Li, H. L. Wang, L. M. Xie, Y. Y. Liang, G. S. Hong and H. J. Dai, J. Am. Chem. Soc., 2011, 133, 7296–7299 CrossRef CAS PubMed.
  38. J. F. Xie, H. Zhang, S. Li, R. X. Wang, X. Sun, M. Zhou, J. F. Zhou, X. W. Lou and Y. Xie, Adv. Mater., 2013, 25, 5807 CrossRef CAS PubMed.
  39. H. T. Wang, Z. Y. Lu, S. C. Xu, D. S. Kong, J. J. Cha, G. Y. Zheng, P. C. Hsu, K. Yan, D. Bradshaw, F. B. Prinz and Y. Cui, Proc. Natl. Acad. Sci. U. S. A., 2013, 110, 19701–19706 CrossRef CAS PubMed.
  40. T. Y. Wang, L. Liu, Z. W. Zhu, P. Papakonstantinou, J. B. Hu, H. Y. Liu and M. X. Li, Energy Environ. Sci., 2013, 6, 625–633 CAS.
  41. Y. F. Yu, S. Y. Huang, Y. P. Li, S. N. Steinmann, W. T. Yang and L. Y. Cao, Nano Lett., 2014, 14, 553–558 CrossRef CAS PubMed.
  42. H. I. Karunadasa, E. Montalvo, Y. J. Sun, M. Majda, J. R. Long and C. J. Chang, Science, 2012, 335, 698–702 CrossRef CAS PubMed.
  43. J. Kibsgaard, Z. B. Chen, B. N. Reinecke and T. F. Jaramillo, Nat. Mater., 2012, 11, 963–969 CrossRef CAS PubMed.
  44. J. F. Xie, J. J. Zhang, S. Li, F. Grote, X. D. Zhang, H. Zhang, R. X. Wang, Y. Lei, B. C. Pan and Y. Xie, J. Am. Chem. Soc., 2013, 135, 17881–17888 CrossRef CAS PubMed.
  45. J. Deng, P. J. Ren, D. H. Deng, L. Yu, F. Yang and X. H. Bao, Energy Environ. Sci., 2014, 7, 1919–1923 CAS.
  46. Z. B. Chen, D. Cummins, B. N. Reinecke, E. Clark, M. K. Sunkara and T. F. Jaramillo, Nano Lett., 2011, 11, 4168–4175 CrossRef CAS PubMed.
  47. T. F. Jaramillo, J. Bonde, J. D. Zhang, B. L. Ooi, K. Andersson, J. Ulstrup and I. Chorkendorff, J. Phys. Chem. C, 2008, 112, 17492–17498 CAS.

Footnote

Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra05614k

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