green synthesis of pt/ceo2/graphene hybrid nanomaterials with remarkably enhanced electrocatalytic...
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This journal is c The Royal Society of Chemistry 2012 Chem. Commun., 2012, 48, 2885–2887 2885
Cite this: Chem. Commun., 2012, 48, 2885–2887
Green synthesis of Pt/CeO2/graphene hybrid nanomaterials with
remarkably enhanced electrocatalytic propertiesw
Xiao Wang,ab
Xiyan Li,ab
Dapeng Liu,aShuyan Song
aand Hongjie Zhang*
a
Received 28th November 2011, Accepted 17th January 2012
DOI: 10.1039/c2cc17409j
We developed a facile strategy for clean synthesis of Pt/CeO2/
graphene nanomaterials with remarkably enhanced catalytic
properties. The graphene oxide (GO) could be used as an
oxidant to oxidize Ce3+
into CeO2 NPs, and L-lysine was used
as a linker to realize the in situ growth of Pt NPs around CeO2
NPs dispersed on graphene.
Owing to its merits like low cost, less environmental pollution,
and quick start at low temperature, etc., the direct methanol
fuel cell (DMFC) has been considered the most potential
energy carrier to meet the continuously increasing demand
for portable electronic devices.1,2 However, problems such as
the low methanol electro-oxidation kinetics and methanol
permeation across the proton exchange membrane obstruct
its commercialization.3 To prevent the noble metal catalysts
from being poisoned by CO that is an intermediate product of
anodic methanol oxidation, efforts have been devoted to
developing Pt-based alloys such as Pt–Ru, Pt–Ni, etc.4,5 On
the other hand, the recently developed strategy is to load Pt
nanoparticles (NPs) on high-surface-area metal oxides as
supporting materials. Research on the metal oxides-based
composites such as Pt/CeO2, Pt/TiO2 and Pt/SnO2, etc.6–8
has confirmed that such a kind of hybrid nanomaterials could
exhibit higher catalytic activities and stabilities during the
methanol oxidation. Especially, rare earth oxide CeO2 is of
particular interest due to the high oxygen transfer ability, high
efficiency for gaseous CO oxidation and much lower price,
which might significantly promote methanol oxidation and
reduce the preparation cost of the catalyst.9 However, due to
the low electron conductivity of CeO2 at the cost of catalytic
performance, it still necessarily deserves the investigation of
the structural design of Pt/CeO2 based catalysts to weaken the
side effects resulting from the low electron conductivity and
the lack of attachment of Pt and CeO2 NPs.
In recent years, the emergence of graphene with its unique
properties, such as high surface area and high electrical
conductivity, has opened a new avenue for utilizing two-
dimensional carbon material as a support in DMFCs.10–12
Actually, graphene supported Pt catalysts have been extensively
investigated and commonly employed as electrocatalysts for
methanol electro-oxidation.11,12 However, some serious problems
including stability and poisoning of Pt/graphene catalysts by
intermediate species were observed during the electrocatalytic
processes, which limited their further applications. In addition,
irreversible agglomeration of graphene was inevitable, which
made it difficult to provide large surface areas for good
adherence and homogeneous distribution of Pt NPs. In this
case, the combination of CeO2, Pt, and graphene may lead to
the materials with enhanced electrocatalytic activity for
methanol oxidization as well as stability and dispersibility in
the catalytic process.
Herein, we design a green and facile method to synthesize the
novel Pt/CeO2/graphene composite, which could present several
important benefits: (a) CeO2 added in the composites has high
efficiency for CO oxidation derived from its own oxygen defects
in the methanol oxidation.13 (b) Graphene could improve the
conductivity required for electrochemical reactions and also
provide a large scaffold for anchoring Pt and CeO2 NPs owing
to its large specific surface area and two-dimensional planar
conjugation structure. (c) Pt NPs grown around CeO2 NPs in situ
on the graphene nanosheet surface with the exposed clean active
surface will enhance the utilization efficiency of Pt catalysts and
the electrocatalytic activity for methanol oxidization.
As described in Scheme 1, the composites were firstly
prepared by dispersing the CeO2 NPs on graphene, and then
Scheme 1 Schematic representation of the synthesis of Pt/CeO2/
graphene composites.
a State Key Laboratory of Rare Earth Resource Utilization,Changchun Institute of Applied Chemistry, Chinese Academy ofSciences, Changchun 130022, P. R. China.E-mail: [email protected]; Fax: +86-431-85698041;Tel: +86-431-85262127
bGraduate University of the Chinese Academy of Sciences,Beijing 100049, P. R. China
w Electronic supplementary information (ESI) available. See DOI:10.1039/c2cc17409j
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2886 Chem. Commun., 2012, 48, 2885–2887 This journal is c The Royal Society of Chemistry 2012
Pt NPs were selectively grown around CeO2 NPs supported on
graphene. Since there is no reducer such as ethylene glycol,14
hydrazine15 or NaBH4,16 etc. employed in the process of
preparation of CeO2/graphene, graphite oxide with a large
amount of oxygen-containing groups (e.g., carboxyl, hydroxyl,
and epoxy groups) could serve as a strong oxidant to oxidize
Ce3+ into CeO2.17–19 The obtained graphene plays the role of
stabilizer for its surface anchored CeO2 NPs and at the same
time CeO2 NPs serve as spacers to prevent the graphene from
aggregating and restacking after removal of solvents, finally
leading to the separated manolayer CeO2/graphene hybrid
materials. This has been firmly proved by atomic force micro-
scopy (AFM) analysis (Fig. S3, ESIw). The powder X-ray
diffraction (XRD) patterns of GO and the synthesized CeO2/
graphene are shown in Fig. 1a and b. Compared with the
characteristic diffraction peak at 2y = 10.61 in the XRD
pattern of disordered GO, the XRD pattern of the CeO2/
graphene shows a broad, low intensity peak at 2y = 22.51,
indicating the reduction of GO, and all the other peaks can be
indexed to the fluorite structured CeO2 in good consistence
with the standard data of CeO2 (JCPDS No. 34-0394). Raman
spectra also proved directly the reduction of GO (Fig. 1c and
d). As shown in Fig. 1c, GO displays two prominent peaks at
B1585 andB1351 cm�1 corresponding to the G and D bands,
respectively. After redox process, the D/G intensity ratio
increased slightly from GO to graphene, suggesting a decrease
of sp2-domain induced by the Ce3+ reduction.
The morphology of the CeO2/graphene hybrid was investi-
gated by transmission electron microscopy (TEM) and AFM
analysis. As shown in Fig. 2a and b, the as-obtained CeO2/
graphene hybrid was well dispersed on graphene nanosheets
with a uniform size of about 3 nm. The AFM analysis (Fig. S3,
ESIw) reveals that the average thickness of CeO2/graphene
hybrids obtained in this work was ca. 5 nm. When compared
with well exfoliated GO sheets, with a spacing of ca. 0.7 nm
(Fig. S1, ESIw), the greater thickness of CeO2/graphene hybrids
further suggested that the CeO2 was completely covered on
surfaces of the graphene. The energy-dispersive X-ray spectrum
(EDX) of CeO2/graphene showed the peaks of C, O, Ce and
Cu elements (from the Cu grid, Fig. S2a, ESIw).After the formation of CeO2/graphene nanocomposites,
bio-molecular L-lysine was introduced to further modify the
surface of the CeO2/graphene. Then Pt NPs were introduced
which are supposed to be preferably adsorbed on the hydro-
philic surface of CeO2, rather than on the hydrophobic surface
of graphene sheets. Fig. 2c and d show that the majority of the
Pt NPs are formed around CeO2 NPs, which can be seen from
the adjacent NPs with different lattice spacing, B0.2295 and
B0.3143 nm, corresponding to Pt (111) and CeO2 (111)
planes,20 respectively. The EDX spectrum showed the peaks
of Pt, C, O, Ce and Cu elements, further confirming the
formation of Pt/CeO2/graphene composites (Fig. S2b, ESIw).It is surmised that the L-lysine was preferred to adsorb on the
hydrophilic surface of CeO2 NPs which were full of –NH2
groups to induce the in situ growth of Pt NPs around CeO2
NPs.21 Controlled experiments were conducted without the
modification of L-lysine on CeO2/graphene, and the result
showed that the Pt NPs were aggregated together with a bad
dispersivity on the graphene (Fig. S5, ESIw). It may be due to
the presence of residual oxygenate groups on the reduced
graphene (Fig. 2b) which could bind with the Pt NPs.
However, the Pt NPs showed significant mobility on graphene
surfaces and hence tend to agglomerate,22,23 which also
indicated the important role of L-lysine in the formation of
Pt/CeO2/graphene composites.
Fig. S4 (ESIw) shows the survey of XPS spectra of CeO2/
graphene and Pt/CeO2/graphene composites. After reduction
of GO (Fig. S4a and b, ESIw), the peaks associated with C–C
(284.6 eV) became predominant, while the peaks related to
the oxidized carbon species such as C–OH (285.2 eV), C–O
(286.7 eV) and O–CQO (288.4 eV) were greatly weakened.24
These results indicate that GO has been well deoxygenated to
form graphene, which is very important for improving its
conductivity. The XPS patterns of the resulting CeO2/graphene
composite show significant Ce 3d signals corresponding to the
binding energy of CeO2 (Fig. S4c, ESIw). The Ce 3d binding
energy peaks, such as those at 883.7, 889.6, 899.6 and 918.3 eV,
for the graphene composite are consistent with a previous
report on Ce4+.25 As for the Pt/CeO2/graphene composites,
besides the Ce 3d and C signals, the major peaks at 70.6 eV
and 73.9 eV can be assigned to the 4f7/2 and 4f5/2 states of Pt
metals (Fig. S4d, ESIw), which means that the Pt metals have
been dispersed on the CeO2/graphene nanocomposites.
Fig. 1 XRD patterns of (a) GO and (b) CeO2/graphene composites.
Raman spectra of (c) GO and (d) CeO2/graphene composites.
Fig. 2 (a, b) TEM images of CeO2/graphene. (c, d) TEM images of
Pt/CeO2/graphene composites. The scale bar in (d) is 1 nm.
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This journal is c The Royal Society of Chemistry 2012 Chem. Commun., 2012, 48, 2885–2887 2887
The electrocatalytic oxidation of methanol using Pt/CeO2/
graphene composites as catalysts was investigated. The
Pt/graphene hybrids and commercial Pt/C catalysts were also
investigated for comparison. Fig. 3a shows the cyclic voltam-
metry (CV) curves in 0.5 M H2SO4 containing 1 M CH3OH
solution. The onset potential, peak potential, current density
and the tolerance (If/Ib) are listed in Table S1 (ESIw). It is
interesting to observe that the onset potential of Pt/CeO2/
graphene for methanol oxidation starts at 0.15 V, which is
lower than that of CeO2/graphene (0.23 V) and Pt/C (0.20 V)
catalysts, and is also much lower than the ones reported for
carbon materials supported catalysts,10,26 demonstrating the
excellent electrochemical catalytic activity of the present
Pt/CeO2/graphene nanocomposites toward the oxidation of
methanol. In addition, considering the electrochemical active
surface area (ECSA) of the Pt/CeO2/graphene did not change
much compared to Pt/graphene (Fig. S6, ESIw), it was furtherproved that the Pt NPs are selectively deposited on CeO2/
graphene and methanol is much more easily electro-oxidized
on Pt/CeO2/graphene hybrids. As listed in Table S1 (ESIw),the Pt/CeO2/graphene catalyst exhibits especially higher peak
current densities of 366 A g�1Pt at about 0.69 V (versusAg/AgCl)
in the forward potential scan (If) and 230 A g�1Pt at 0.50 V
(versus Ag/AgCl) in the backward potential scan (Ib), respec-
tively. Correspondingly, the higher If/Ib ratio of Pt/CeO2/
graphene indicates that methanol molecules are more effec-
tively oxidized on Pt/CeO2/graphene during the forward
potential scan, and also it is speculated that the added ceria
may assist the removal of the carbonaceous intermediate.
Chronoamperometric (CA) measurement was also used to
appraise the durability of catalysts. The CA technique is an
effective method to evaluate the electrocatalytic activity and
stability of catalyst material. Fig. 3b demonstrates CA curves
of Pt/CeO2/graphene, Pt/graphene and Pt/C for methanol
oxidation at a fixed potential of 0.742 V/Ag/AgCl. As
expected, the methanol oxidation current of Pt/CeO2/graphene
was evidently higher than Pt/graphene and Pt/C systems.
These results indicate that the Pt/CeO2/graphene has a durable
higher catalytic activity than Pt/graphene and Pt/C systems for
the electro-oxidation of methanol.
In conclusion, we demonstrated a facile and green method
to synthesize the Pt/CeO2/graphene nanocomposites. The GO
could be used as a green and efficient oxidant to oxidize Ce3+
cations into CeO2 NPs, leading to the in situ formation of
CeO2/graphene hybrids. L-Lysine serves as linkers to connect
Pt and CeO2 NPs together on graphene. As used for the electro-
catalytic oxidation of methanol, the obtained Pt/CeO2/graphene
composites exhibited a remarkably enhanced catalytic performance
such as the higher catalytic activity compared with simple
Pt/graphene and commercial Pt/C catalysts. Additionally, our
approach is expected to be a viable and low-cost strategy to
fabricate graphene-based complexes multi-functional nano-
materials. It is believed that this kind of nanocatalysts will
have a great potential for industrial applications in future.
The authors are grateful for the financial aid from the
National Natural Science Foundation of China Major Project
(Grant No. 91122030), ‘863’-National High Technology
Research and Development Program of China (Grant No.
2011AA03A407) and National Natural Science Foundation
for Creative Research Group (Grant No. 20921002).
Notes and references
1 S. Celik and M. D. Mat, Int. J. Hydrogen Energy, 2010, 35, 2151.2 A. Lam, D. P. Wilkinson and J. J. Zhang, J. Power Sources, 2009,194, 991.
3 H. Deligoz, S. Yilmazturk, T. Karaca, H. Ozdemir, S. N. Koc,F. Oksuzomer, A. Durmus and M. A. Gurkaynak, J. Membr. Sci.,2009, 326, 643.
4 P. Piela, C. Eickes, E. Brosha, F. Garzon and P. Zelenay,J. Electrochem. Soc., 2004, 151, A2053–A2059.
5 K. W. Park, J. H. Choi, B. K. Kwon, S. A. Lee, Y. E. Sung,H. Y. Ha, S. A. Hong, H. Kim and A. Wieckowski, J. Phys. Chem.B, 2002, 106, 1869.
6 M. A. Scibioh, S.-K. Kim, E. A. Cho, T.-H. Lim, S.-A. Hong andH. Y. Ha, Appl. Catal., B, 2008, 84, 773.
7 S. Y. Huang, P. Ganesan, S. Park and B. N. Popov, J. Am. Chem.Soc., 2009, 131, 13898.
8 L. Jiang, G. Sun, Z. Zhou, S. Sun, Q. Wang, S. Yan, H. Li, J. Tian,J. Guo, B. Zhou and Q. Xin, J. Phys. Chem. B, 2005, 109, 8774.
9 Y.-Y. Chu, Z.-B. Wang, Z.-Z. Jiang, D.-M. Gu and G.-P. Yi, Adv.Mater., 2011, 23, 3100.
10 A. K. Geim and K. S. Novoselov, Nat. Mater., 2007, 6, 183.11 S. Sharma, A. Ganguly, P. Papakonstantinou, X. P. Miao,
M. X. Li, J. L. Hutchison, M. Delichatsios and S. Ukleja,J. Phys. Chem. C, 2010, 114, 19459.
12 P. Kundu, C. Nethravathi, P. A. Deshpande, M. Rajamathi,G. Madras and N. Ravishankar, Chem. Mater., 2011, 23, 2772.
13 H. Yahiro, Y. Bada, K. Eguchi and H. Arai, J. Electrochem. Soc.,1988, 135, 2077.
14 S. J. Guo, D. Wen, Y. M. Zhai, S. J. Dong and E. K. Wang, ACSNano, 2010, 4, 3959.
15 S. Stankovich, D. A. Dikin, R. D. Piner, K. A. Kohlhaas,A. Kleinhammes, Y. Jia, Y. Wu, S. T. Nguyen and R. S. Ruoff,Carbon, 2007, 45, 1558.
16 H.-J. Shin, K. K. Kim, A. Benayad, S.-M. Yoon, H. K. Park,I.-S. Jung, M. H. Jin, H.-K. Jeong, J. M. Kim, J.-Y. Choi andY. H. Lee, Adv. Funct. Mater., 2009, 19, 1987.
17 Y. H. Xue, H. Chen, D. S. Yu, S. Y. Wang, M. Yardeni, Q. B. Dai,M. M. Guo, Y. Liu, F. Lu, J. Qu and L. M. Dai, Chem. Commun.,2011, 47, 11689.
18 G. L. Xiang, J. He, T. Y. Li, J. Zhuang and X. Wang, Nanoscale,2011, 3, 3737.
19 J. T. Zhang, Z. G. Xion and X. S. Zhao, J. Mater. Chem., 2011,21, 3634.
20 D. R. Ou, T. Mori, H. Togasaki, M. Takahashi, F. Ye andJ. Drennan, Langmuir, 2011, 27, 3859.
21 J. Zhang, X. H. Liu, X. Z. Guo, S. H. Wu and S. R. Wang,Chem.–Eur. J., 2010, 16, 8108.
22 J. A. Rodriguez-Manzo, O. Cretu and F. Banhart, ACS Nano,2010, 4, 3422.
23 C. Nethravathi, E. A. Anumol, M. Rajamathi and N. Ravishankar,Nanoscale, 2011, 3, 569.
24 Y. Xu, H. Bai, G. Lu, C. Li and G. Shi, J. Am. Chem. Soc., 2008,130, 5856.
25 L. S. Zhong, J. Q. Hu, A. M. Cao, Q. Liu, W. G. Song andL. J. Wan, Chem. Mater., 2007, 19, 1648.
26 Y. J. Li, W. Gao, L. J. Ci, C. M. Wang and P. M. Ajayan, Carbon,2010, 48, 1124.
Fig. 3 (a) CV and (b) CA curves of (a) Pt/C catalysts, (b) Pt/graphene
hybrids and (c) Pt/CeO2/graphene composites.
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