Open Access Article
This Open Access Article is licensed under a
Creative Commons Attribution 3.0 Unported Licence

In situ growth of NiO nanoparticles on carbon paper as a cathode for rechargeable Li–O2 batteries

Hong-qiang Wangac, Xiao-ping Fana, Xiao-hui Zhanga, You-guo Huanga, Qiang Wub, Qi-chang Pana and Qing-yu Li*ab
aSchool of Chemistry and Pharmaceutical Sciences, Guangxi Normal University, Guilin 541004, China. E-mail: liqingyu62@126.com
bGuangxi Key Laboratory of Low Carbon Energy Materials, School of Chemical and Pharmaceutical Sciences, Guangxi Normal University, Guilin 541004, China
cCollege of Chemical Engineering, Huanggang Normal University, Huanggang 438000, China

Received 10th March 2017 , Accepted 24th April 2017

First published on 27th April 2017


Abstract

Novel NiO nanoparticles have been successfully designed and directly grown on carbon paper (CP) as a cathode for rechargeable Li–O2 batteries via a facile two-step in situ synthesis strategy, including a simple electro-deposition technique, following by high temperature oxidation. Using in situ synthesis methods means that the porous structure of CP is effectively inherited and the use of a binder avoided, which eliminates possible side reactions and over-potential from the binder and enhances the electrochemical performance. SEM and TEM show that the NiO nanoparticles homogenously cover the exposed surface of CPs and the size of the NiO particles is around 10 nm. Benefiting from these structural advantages, the binder-free cathode of NiO/CP exhibits a high discharge capacity of 8934 mA h g−1 under the current density of 100 mA g−1 and could cycle more than 112 times within a capacity limitation of 500 mA h g−1.


Introduction

In recent years, the global energy crisis and environmental destruction situation are getting worse, and the development of efficient and clean energy sources has become imperative.1 Owing to their significantly high theoretical specific energy density (5200 W h kg−1), rechargeable Li–O2 batteries (LOBs) are a kind of energy storage and conversion device that is a promising candidate for next-generation electric power sources.2–5 The theoretical energy density of Li–O2 batteries is about eight times higher than the conventional Li-ion batteries because of the fact that the cathode active material (oxygen) is obtained directly from the atmosphere without being stored in the batteries.6,7 A typical nonaqueous Li–O2 battery is composed of a Li metal anode in contact with a Li-ion containing organic electrolyte and a porous cathode.8 During discharging, oxygen from the atmosphere combines with Li+ to yield discharge products (e.g. Li2O2), which is defined as the oxygen reduction reaction (ORR). During charging, the discharge products decompose to Li+ and oxygen, which is defined as the as the oxygen evolution reaction (OER).7,9–11 Many efforts have been devoted to develop high performance Li–O2 batteries. However, the development of Li–O2 batteries is still in the initial stage, there are still many problems (such as low round-trip efficiency, instability of the batteries and especially poor cycle life) restricting the practical application of Li–O2 batteries.12–16

In order to solve the above problems, developing a suitable catalyst is the critical link to achieve the application of Li–O2 batteries. On the one hand, high performance catalyst can accelerate the ORR and OER as well as reducing the overpotential for Li–O2 batteries, on the other hand, an active catalyst can effectively catalyze the decomposition of solid discharge products, which would improve cycle life and round-trip efficiency of Li–O2 batteries.17,18 In recent years, many efforts have been devoted to study transition metal oxide due to their advantages of low cost, excellent catalytic activity and natural abundance.19–22 NiO has been studied in Li–O2 battery due to its good catalytic performance,23–26 Swapna Ganapathy also confirmed that Li2O2 was more easily formed on the surface of NiO owing to its potential nucleation site for the formation of Li2O2, and this is supported by first principle calculations, which predict a low interfacial energy for the formation of NiO–Li2O2 interfaces.27

However, the poor conductivity of NiO limits its electrochemical performance. To overcome this problem, one effective way to improve the conductivity of electrons is to add an electron-conductive material as a support for the catalyst. Meanwhile, such support should contain a lot of mesoporous to provide more void spaces for storing Li2O2. Carbon paper has been widely used as the collector of Li–O2 batteries because of its unique porous structure and excellent electrical conductivity.28–30

Herein, we report a facile two-step procedure successfully load uniformly NiO nanoparticles on the carbon paper (NiO/CP). It is worth mentioning that this method was first proposed to prepare NiO nanoparticles catalyst for Li–O2 batteries. As shown in Fig. 1, firstly, we use an effective and simple electro-deposition method to prepare a free-standing material that Ni nano-flowers directly grown from carbon paper and then calcined oxidized to NiO at 550 °C in an air atmosphere. Using in situ synthesis methods synthesized NiO directly on the CPs to avoid the use of the binder, it eliminates the problem of great polarization and poor electrochemical performance due to the addition of the binder and inherits the porous structure of CPs that promotes rapid transmission of oxygen and Li ion and infiltration of electrolyte. In addition, using electro-deposition method can effectively control the morphology and size of the catalyst particles, increasing the active surface area of the catalyst to improve the utilization of the catalyst,20 so that the electrochemical performance is improved greatly.


image file: c7ra02932b-f1.tif
Fig. 1 Synthetic process of NiO/CP and structure of the rechargeable Li–O2 batteries.

Experimental

Preparation of NiO/CP

The positive electrodes were prepared via in situ fabricate NiO nanoparticles anchored on carbon paper (NiO/CP). Firstly, we electrodeposited nickel metal particles on carbon paper (Ni/CP) under a current of 40 mA cm−2 deposition for 30 s wherein titanium plate as the anode, carbon paper as the cathode. The electro-deposition solutions consists of 100 g L−1 NiSO4·6H2O, 60 g L−1 NiCl2·6H2O, 40 g L−1 H3BO3, 0.1 g L−1 CN2H4S and 0.1 g L−1 C12H25SO3Na. Then the samples were washed with deionized water and dried at 80 °C for 1 h. Finally, we put Ni/CP composite into the Branch Crystal tube furnace to calcine in air atmosphere, and kept at 550 °C for 2 h. As a result, the metal nickel oxidized to NiO.

Characterization of the electrodes

The morphology and structure of the NiO/CP are investigated by scanning electron microscopy (SEM, Philips, FEI Quanta 200 FEG) and transmission electron microscopy (TEM, JEOL 2011). The content of various components of NiO/CP composite was determined from thermogravimetric analysis (TGA) (Nitzsch STA 449C) at a heating rate of 5 °C min−1. The phases present in the electrode were checked by X-ray diffraction (XRD-Rigaku D/Max-2550pc) with Cu Kα radiation (λ = 0.1541 nm). X-ray photoelectron spectroscopy (XPS) experiments were carried out using an AXIS ULTRA DLD instrument, using aluminum Kα X-ray radiation during the XPS analysis.

Electrode preparation and electrochemical measurements

Electrochemical characterizations of Li–O2 cells were carried out using 2032-type coin cells which were assembled in an argon-filled glovebox. Li foil was used as the anode, 1 mol L−1 LiTFSi in mixed solution of tetraethylene glycol dimethyl ether (TEGDME) was used as the electrolyte, Celgard 2400 and a glass fiber were used as the separator and the NiO/CP composites as the cathode. The cells were sealed except holes of the cathode shell exposed to 1 atm O2 environment. The electrochemical properties were studied with a Land batteries measurement system (LAND BT2013A, Wuhan, China). Galvanostatic charge–discharge cycling was performed over a voltage window of 2.2–4.3 V. The working electrode was measured at room temperature during the whole process.

Results and discussion

CPs, owning porous skeleton and stability, are popular current collectors for Li–O2 batteries. The porous and interconnected morphology of CPs is shown in Fig. 2a. Because of its interconnected 3D scaffold structure which are benefit to the rapid transmission of oxygen and the contact with the electrolyte and the surface of catalyst, so it is used as a template for the growth of NiO. High magnification SEM of CPs indicates that CPs are consist of carbon fibers and the surface of CPs are smooth. From the Fig. 2c and d we can clearly see that the flower metal nickel were successfully coated on the surface of the CPs by electro-deposition method and the size of nickel particle is around 50 nm. The SEM images of the NiO/CP are shown in Fig. 2e–g. In contrast to Fig. 2a and e, we can clearly see that nickel oxide homogenously cover the exposed surface of CPs. From high-magnification SEM of NiO/CP we can clearly see the uniform and dense surface structure of NiO/CP and the diameter of the NiO particles sizes which is only about 10 nm in Fig. 2f and g. Nanoscale NiO particles improved the specific surface area of cathode materials and more active sites were exposed, thereby effectively improve the catalytic performance. The corresponding elemental mapping spectrum of the NiO/CP as shown in Fig. 2h, it can be seen that the carbon, oxygen and nickel elements are homogeneously distributed in the whole detected area and suggest that NiO nanoparticles were uniformly loaded on the carbon paper.
image file: c7ra02932b-f2.tif
Fig. 2 (a and b) SEM image of pristine CP; (c and d) SEM of the Ni/CP composite; (e–g) SEM of the NiO/CP composite; (h) EDS of the C, O, Ni.

Transmission electron microscope (TEM) analysis was performed to further characterize the detailed morphology and microstructure of the NiO/CP electrode. As shown in Fig. 3a and b, TEM image indicates that NiO nanoparticles uniformly distributed on the carbon paper with an average size of 10 nm. High magnification TEM image of Fig. 3c reveals the spacing of the adjacent lattice planes is 0.24 nm corresponding to the (111) planes of NiO phase, which is further confirmed by X-ray diffraction (XRD) (space group: Fm[3 with combining macron]m (225), JCPDS no. 47-1049).


image file: c7ra02932b-f3.tif
Fig. 3 (a–c) TEM images of NiO/CP.

The content of NiO in the NiO/CP composite was confirmed by the thermo-gravimetric analysis (TGA) in O2. The TGA curves of the NiO/CP composite is shown in Fig. 4. The one continuous weight loss in the range of approximately 570–800 °C for the NiO/CP composite is attributed to the oxidation of C of carbon paper to CO2, when the temperature is higher than 800 °C, the TGA curves tends to be gentle, indicating that the C element has all become CO2. The mass fraction of NiO and CP in the NiO/CP composite can be calculated to be around 7.75% and 92.25%, respectively.


image file: c7ra02932b-f4.tif
Fig. 4 TGA analysis for the NiO/CP composite.

The XRD patterns of CP and the NiO/CP composites of with the electro-deposition time of 30 s and 300 s are shown in Fig. 5. The pure carbon paper shows one intense diffraction peaks located at 26.3° and one weak diffraction peaks at 54.2°. Compared with the pure carbon paper, when the electro-deposition time which is consistent with experimental conditions is 30 s, the NiO/CP composites with shows there was no significant change, which may be attributed to that the content of NiO is too little to detect and the disturbance of high intensity of the C peak. When increasing the deposition time to 300 s, the deposited quantity of NiO on carbon paper increases, which is obvious in the XRD pattern. The NiO/CP composites exhibits the typical characteristic peaks of NiO at 37.24°, 43.27° and 62.86°, according to JCPDS card no. 71-1179, these peaks can be assigned to the (111), (200) and (311) plane reflections of the NiO, respectively. Highlighted X-ray diffraction patterns related to the 2θ range of 19–23° are shown in Fig. 5, there are two low-intensity peaks at 75.39° and 79.38°, which can be attributed to the (311) and (222) plane reflections of the NiO, respectively. In addition, there are some Ni peaks in the XRD pattern due to incomplete oxidation of Ni.


image file: c7ra02932b-f5.tif
Fig. 5 The XRD patterns of CP and the NiO/CP composites of with the electro-deposition time of 30 s and 300 s.

The chemical states of NiO/CP is also confirmed by X-ray photoelectron spectroscopy (XPS) measurements. Fig. 6a shows the XPS survey scan of the NiO/CP, which indicates the presence of Ni, O, and C elements and shows a 2.76 at% percentage composition of Ni and this content is obviously lower than the detection range of XRD. Fig. 6b–d show the Ni 2p, O 1s and C 1s peaks, which were analyzed by using the software of XPS peak version 4.1. In the Ni 2p spectra of Fig. 6b, the main Ni 2p3/2 peak located at 861.4 eV, 855.2 eV and 851.1 eV (ref. 31 and 32) which all are characteristic peaks of the NiO and located at 861.7 eV which is characteristic peak of the Ni(OH)2.33 As shown in Fig. 6c, three peaks for the O 1s are observed at 529.5 eV, 531.2 eV and 532.4 eV, which are associated with O 1s binding energy in O–Ni, Ni–O–H and O–C,34,35 respectively. In the C 1s spectra of Fig. 6d indicates that NiO/CP has three peaks at 284.6 eV, 284.7 eV and 285.6 eV, which correspond to the binding energies of C 1s in C–C, C[double bond, length as m-dash]C and C–O, respectively.20


image file: c7ra02932b-f6.tif
Fig. 6 XPS spectra of the NiO/CP composite. (a) Survey scan; (b) Ni 2p spectrum; (c) O 1s spectrum; (d) C 1s spectrum.

The electrochemical performance of the as-prepared NiO/CP was investigated by the galvanostatic discharge/charge method. Fig. 7a and b shows the charge and discharge curves obtained by limiting the capacity of 1000 mA h g−1 at various current density. It can be observed from Fig. 7a that there is a very small overpotential of 0.55 V in the middle of the charge–discharge plateaus at the current density of 100 mA g−1. As the current densities increasing, the overpotential increases appropriately, when the current density increased to 300 mA g−1, the overpotential increases to 1.3 V, but is still smaller than the overpotential of the general Li–O2 batteries. Besides, Fig. 7b shows the discharge curves of the Li–O2 batteries with the NiO/CP electrode at different current densities. At 100 mA g−1, the batteries deliveres extremely high discharge specific capacity of 8934.0 mA h g−1, when the current density were increased to 200 mA g−1 and 300 mA g−1, the batteries still show higher discharge specific capacity of 5000.4 mA h g−1 and 4361.4 mA h g−1, respectively, exhibiting good rate capability of the Li–O2 batteries with the NiO/CP electrode. The full discharge–charge curves of the first ten cycles of the Li–O2 batteries with the NiO/CP electrode at the current density of 100 mA g−1 as shown in Fig. 7c. The first discharge specific capacity of the Li–O2 batteries is up to 8934.0 mA h g−1 with a discharge platform of 2.73 V. Comparing with other Li–O2 batteries systems which using NiO as catalyst, it exhibits the highest discharge specific capacity, which may be due to its unique spherical nanoparticles and allowing more active sites to be exposed.23–26 After 5 cycles, the discharge specific capacity is still higher 4000 mA h g−1, while after 10 cycles, the discharge specific capacity decreased to 1327 mA h g−1. In fact, the stable full discharge/charge Li–O2 batteries system still can't be achieved due to the accumulation of the discharge product and instability of the electrolyte, which is still a serious challenge to be solved for Li–O2 batteries. The excellent electrochemical performance NiO/CP electrode is due to unique three dimensional structure, high catalytic activity of NiO nanoparticles. As shown in Fig. 7d and e, the cycle stability of NiO/CP cathode is investigated with a an upper-limit capacity to 500 mA h g−1 at a current density of 100 mA g−1 based on mass of NiO in the range of 2.0–5.0 V versus Li/Li+. Fig. 7d displays the superior cycle performance and excellent stability of the LOBs with NiO/CP electrode which can be cycled for 112 cycles and most of the discharge capacities are delivered above 2.6 V. The 1st, 5th, 20th, 50th, 100th and 112th cycles of discharge/charge voltage profiles are selected to display in Fig. 7e, which further validated the excellent catalytic performance of NiO/CP composites.


image file: c7ra02932b-f7.tif
Fig. 7 Electrochemical properties of NiO/CP catalyzed Li–O2 batteries. (a) Discharge/charge curves of Li–O2 batteries with NiO/CP electrodes at the current density of 100 mA g−1, 200 mA g−1 and 300 mA g−1 with a limited of 1000 mA h g−1 based on mass of NiO; (b) the rate capacities of Li–O2 batteries using NiO/CP electrode at the current density of 100 mA g−1, 200 mA g−1 and 300 mA g−1; (c) full discharge/charge curves between 2.2–4.3 V at 100 mA g−1; (d) cycling performance of NiO/CP electrodes at 100 mA g−1 with limited capacity of 500 mA h g−1; (e) capacity and terminal voltage of discharge vs. cycle numbers.

In order to further demonstrate the catalytic properties of NiO, we made a comparison with pristine CP. NiO/CP and CP were used as cathode and were assembled into the LOBs to compare their electrochemical performance, which the specific capacity was calculated based on the total mass of the whole cathode electrode. As shown in Fig. 8, the Li–O2 batteries with the NiO/CP cathode and pristine CP electrode without NiO were cycled at the current density of 0.05 mA cm−2. The initial discharge capacity of the NiO/CP cathode is 12.4 mA h g−1, after 5th cycles, the capacity reduced to 8.0 mA h g−1 and has been remained around 8.0 mA h g−1 until to 20th cycles. As a comparison, the initial discharge capacity of the pristine CP cathode is only 3.6 mA h g−1, after 5th cycles, the capacity reduced to 1.2 mA h g−1 and after 20th cycles, the capacity is only 0.5 mA h g−1. Compared with the pure CP without NiO, the NiO/CP composite has greatly improved the specific capacity of Li–O2 batteries.


image file: c7ra02932b-f8.tif
Fig. 8 Discharge/charge cycling of Li–O2 cell with the NiO/CP cathode and pure CP electrode without NiO, based on total electrode mass at a current density of 0.05 mA cm−2.

Conclusions

In summary, we have designed a novel NiO nanoparticles directly grown on carbon paper via an in situ method as the cathode for Li–O2 batteries. Compared with other methods, the size of NiO nanoparticle obtained by this method is far less than hexagonal plate NiO, so the specific surface area of NiO were greatly improved and more active site were exposed. In addition, this strategy can make NiO only deposit on surface of CPs, thus the NiO/CP electrode inheriting the porous structure of CPs that promotes rapid transmission of oxygen and infiltration of electrolyte. SEM and TEM show that the NiO nanoparticles homogenously cover the surface of CPs and the size of the NiO particles is around 10 nm. Benefiting from the structural advantages, the binder-free cathode of NiO/CP exhibits excellent catalytic performance and delivers high discharge capacity of 8934 mA h g−1 under the current density of 100 mA g−1 and could cycle more than 112 times within a capacity limitation of 500 mA h g−1. These results suggest that NiO/CP composite as binder-free and freestanding cathode electrocatalyst, which exhibits good electrochemical performance would promote the practical application of LOBs.

Acknowledgements

This research was supported by National Science Foundation of China (U1401246, 51364004, 51474077, 21473042 and 51474110), Guangxi Natural Science Foundation (2012GXNSFAA053214).

Notes and references

  1. B. Dunn, H. Kamath and J. M. Tarascon, Science, 2011, 334, 928–935 CrossRef CAS PubMed.
  2. P. G. Bruce, S. A. Freunberger, L. J. Hardwick and J. M. Tarascon, Nat. Mater., 2012, 11, 19–29 CrossRef CAS PubMed.
  3. L. Grande, E. Paillard, J. Hassoun, J. B. Park, Y. J. Lee, Y. K. Sun, S. Passerini and B. Scrosati, Adv. Mater., 2015, 27, 784–800 CrossRef CAS PubMed.
  4. R. Black, B. Adams and L. F. Nazar, Adv. Energy Mater., 2012, 2, 801–815 CrossRef CAS.
  5. Y. Shao, F. Ding, J. Xiao, J. Zhang, W. Xu, S. Park, J.-G. Zhang, Y. Wang and J. Liu, Adv. Funct. Mater., 2013, 23, 987–1004 CrossRef CAS.
  6. G. A. Elia, J. Hassoun, W. J. Kwak, Y. K. Sun, B. Scrosati, F. Mueller, D. Bresser, S. Passerini, P. Oberhumer, N. Tsiouvaras and J. Reiter, Nano Lett., 2014, 14, 6572–6577 CrossRef CAS PubMed.
  7. Z. Peng, S. A. Freunberger, Y. Chen and P. G. Bruce, Science, 2012, 337, 563–566 CrossRef CAS PubMed.
  8. Z. Ma, X. Yuan, L. Li, Z.-F. Ma, D. P. Wilkinson, L. Zhang and J. Zhang, Energy Environ. Sci., 2015, 8, 2144–2198 CAS.
  9. K. Abraham and Z. Jiang, J. Electrochem. Soc., 1996, 143, 1–5 CrossRef CAS.
  10. Y. Yang, T. Zhang, X. Wang, L. Chen, N. Wu, W. Liu, H. Lu, L. Xiao, L. Fu and L. Zhuang, ACS Appl. Mater. Interfaces, 2016, 8, 21350–21357 CAS.
  11. T. Ogasawara, A. Débart, M. Holzapfel, P. Novák and P. G. Bruce, J. Am. Chem. Soc., 2016, 128, 1390–1393 CrossRef PubMed.
  12. Y. Jing and Z. Zhou, ACS Catal., 2015, 5, 4309–4317 CrossRef CAS.
  13. P. Zhang, R. Wang, M. He, J. Lang, S. Xu and X. Yan, Adv. Funct. Mater., 2016, 26, 1354–1364 CrossRef CAS.
  14. S.-M. Xu, Q.-C. Zhu, J. Long, H.-H. Wang, X.-F. Xie, K.-X. Wang and J.-S. Chen, Adv. Funct. Mater., 2016, 26, 1365–1374 CrossRef CAS.
  15. Q. C. Liu, J. J. Xu, D. Xu and X. B. Zhang, Nat. Commun., 2015, 6, 7892 CrossRef CAS PubMed.
  16. C. Zhao, C. Yu, S. Liu, J. Yang, X. Fan, H. Huang and J. Qiu, Adv. Funct. Mater., 2015, 25, 6913–6920 CrossRef CAS.
  17. D. Geng, N. Ding, T. S. A. Hor, S. W. Chien, Z. Liu, D. Wuu, X. Sun and Y. Zong, Adv. Energy Mater., 2016, 6, 1502164 CrossRef.
  18. Z. Huang, B. Chi, L. Jian, S. Youyi and Y. Liu, J. Alloys Compd., 2017, 695, 3435–3444 CrossRef CAS.
  19. W. H. Ryu, T. H. Yoon, S. H. Song, S. Jeon, Y. J. Park and I. D. Kim, Nano Lett., 2013, 13, 4190–4197 CrossRef CAS PubMed.
  20. H.-Q. Wang, J. Chen, S.-J. Hu, X.-H. Zhang, X.-P. Fan, J. Du, Y.-G. Huang and Q.-Y. Li, RSC Adv., 2015, 5, 72495–72499 RSC.
  21. J. Liu, R. Younesi, T. Gustafsson, K. Edström and J. Zhu, Nano Energy, 2014, 10, 19–27 CrossRef CAS.
  22. L. Jin, L. Xu, C. Morein, C.-h. Chen, M. Lai, S. Dharmarathna, A. Dobley and S. L. Suib, Adv. Funct. Mater., 2010, 20, 3373–3382 CrossRef CAS.
  23. D. Qiu, G. Bu, B. Zhao, Z. Lin, L. Pu, L. Pan and Y. Shi, Mater. Lett., 2015, 141, 43–46 CrossRef CAS.
  24. S. Tong, M. Zheng, Y. Lu, Z. Lin, J. Li, X. Zhang, Y. Shi, P. He and H. Zhou, J. Mater. Chem. A, 2015, 3, 16177–16182 CAS.
  25. M. Hong, H. C. Choi and H. R. Byon, Chem. Mater., 2015, 27, 2234–2241 CrossRef CAS.
  26. C. Wang, Y. Zhao, J. Liu, P. Gong, X. Li, Y. Zhao, G. Yue and Z. Zhou, Chem. Commun., 2016, 52, 11772–11774 RSC.
  27. S. Ganapathy, Z. Li, M. S. Anastasaki, S. Basak, X. F. Miao, K. Goubitz, H. W. Zandbergen, F. M. Mulder and M. Wagemaker, J. Phys. Chem. C, 2016, 120, 18421–18427 CAS.
  28. Z. Guo, G. Zhu, Z. Qiu, Y. Wang and Y. Xia, Electrochem. Commun., 2012, 25, 26–29 CrossRef CAS.
  29. J. Yi, K. Liao, C. Zhang, T. Zhang, F. Li and H. Zhou, ACS Appl. Mater. Interfaces, 2015, 7, 10823–10827 CAS.
  30. Y.-g. Huang, J. Chen, X.-h. Zhang, Y.-h. Zan, X.-m. Wu, Z.-q. He, H.-q. Wang and Q.-y. Li, Chem. Eng. J., 2016, 296, 28–34 CrossRef CAS.
  31. A. N. Mansour, Surf. Sci. Spectra, 1994, 3, 239–246 CrossRef CAS.
  32. S. Uhlenbrock, C. Scharfschwerdt, M. Neumann, G. Illing and H. Freund, J. Phys.: Condens. Matter, 1992, 4, 7973 CrossRef CAS.
  33. A. N. Mansour and C. A. Melendres, Surf. Sci. Spectra, 1996, 3, 247–254 CrossRef.
  34. L. C. Lopez, D. W. Dwight and M. B. Polk, Surf. Interface Anal., 1986, 9, 405–409 CAS.
  35. J. Haber, J. Stoch, L. Ungier, J. Haber, J. Stoch and L. Ungier, J. Electron Spectrosc. Relat. Phenom., 1976, 9, 459–467 CrossRef CAS.

This journal is © The Royal Society of Chemistry 2017
Click here to see how this site uses Cookies. View our privacy policy here.