2
Y.-S. Feng et al. / Tetrahedron xxx (2014) 1e5
3
2
shown in Fig. 1. The XRD patterns of Pd/G and Co/G that included in
lamellae sp hybridized carbon atoms re-converted to sp hybrid-
2
the figure were used as a comparison. The first diffraction peak at
ized carbon atoms, but the average of sp carbon ribbons’ area
became smaller, making the D peak and G peak ratio increase.
These results indicated that GO had been reduced and subsequently
gave rise to the restoration of sp network with small and isolated
domains of aromatics within the sheets.
Fig. 3 shows the morphology and structure of PdeCo (1:1)/G
catalyst determined by TEM and HRTEM. It can be seen that
nanoparticles are well-dispersed on graphene. From Fig. 3b, it is
clearly that the size distribution of PdeCo (1:1)/G catalyst was
3e16 nm, with an average size of 8.96 ꢂ0.4 nm, which is con-
sistent with X-ray diffraction pattern. The elemental mapping
images (Fig. 3d, e) reveal that a single alloy nanoparticle was built
up by Pd (Fig. 3d) and Co (Fig. 3e). Furthermore, to confirm the
PdeCo alloy structure, the energy dispersive spectrometer (EDS)
was texted (as shown in Fig. 3f), which reveals the presence of C,
Pd, and Co on the surfaces of the G sheets (Si and Cu peaks from
the TEM grid).
ꢀ
about 26 in all the XRD patterns was originated from the G sup-
ꢀ ꢀ ꢀ ꢀ
port. The peaks at 2q values of 40.1 , 46.80 , 68.20 , and 82.16 are
2
due to the (111), (200), (220), and (311) diffraction peaks of face
centered cubic Pd (JCPD-46-1043). The XRD pattern of the pure Co
21
ꢀ
ꢀ
sample exhibited two diffraction peaks around 2
q
¼44.5 , 47.3 ,
which increased the lattice structure of the Co (JCPD-15-0806)
species. As the cobalt content increases, the diffraction peak posi-
tion was shifted to a higher angle. This confirms the alloy formation
between Pd and Co, and which indicates a lattice contraction,
which was caused by the incorporation of Co into the Pd face
centered cubic structure. But no significant diffraction peak
characteristic was found when the content of Co decreased, which
was likely due to their poor crystallinity.
16
Fig. 1. XRD patterns of PdeCo/G with different Pd/Co atomic ratios (a) Co/G; (b)
PdeCo (1:3)/G; (c) PdeCo(1:1)/G; (d) Pd eCo (3:1)/G; (e) Pd/G.
3 3
Fig. 3. (a, b) TEM image and the particle size distribution of PdeCo (1:1)/G catalyst, (c)
TEM image of a single PdeCo (1:1)/G nanoparticle, (d) Pd and (e) EDS mapping pro-
files, (f) EDS of PdeCo (1:1)/G catalyst.
Raman spectra of GO and PdeCo (1:1)/G were shown in Fig. 2.
ꢁ
1
The band at about w1355 cm
corresponded to the disorder-
induced D band may be due to disorder-induced features caused
by lattice defect.17 While the in-phase vibration of the G lattice (G
ꢁ
1
band) at about w1605 cm represented the first-order scattering
As shown in Fig. 4, the surface composition of GO and PdeCo/G
was further analyzed by X-ray photoelectron spectroscopy (XPS).
The binding energies obtained in the XPS analysis were corrected
18
of the E2g vibrational mode within aromatic carbon rings. The
GO
I(D)/I(G) intensity ratio of GO (I(D)/I(G) ¼0.92) was slightly lower
G
19,20
than that of PdeCo (1:1)/G (I(D)/I(G) ¼1.41).
Such an en-
for specimen charging by referencing the
C
1s signal to
2
5
hancement therefore suggested after restored large number of
284.70 eV. The survey spectra of GO and PdeCo/G were shown in
Fig. 4a. Compared to that of GO, the XPS spectrum of PdeCo/G not
only exhibits O 1s and C 1s but also exhibits two additional peaks,
which correspond to the Pd 3d and Co 2p states. The higher res-
olution XPS data of C 1s peaks of GO and PdeCo/G are shown in the
Fig 4b and c, respectively. From the C 1s XPS spectrum of GO
(
Fig. 4b), the most resolved peak, located at 284.7 eV, corresponds
17,25,27
to CeC bonds of the G such as CeC, C]C, CeH bonds.
The
weak peak centered at 285.08 eV was attributed to CeO, and the
other two peaks at 286.8 eV and 288.2 eV were attributed to epoxy
carbon and carbonyl carbon. The C 1s XPS spectrum of the PdeCo/
G also exhibits the same functionalities, and their peak intensities
are a litter smaller than those in GO, revealing that most of the
epoxide and hydroxy functional groups were successfully re-
moved. In addition, the O 1s XPS spectra of GO and PdeCo/G are
presented in Fig. 4d, which exhibit different peak shape. The O 1s
peak of GO at 532.38 eV is closely related to the significant hy-
droxyl groups on the surface of GO, whereas, the O 1s peak of
PdeCo/G is at around 530.5 eV. All these results further confirm
GO reduction to G, the successful integration between PdeCo
Fig. 2. The Raman spectra of (a) GO, (b) PdeCo (1:1)/G.