G Model
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Y. Lai et al. / Chinese Chemical Letters xxx (2019) xxx–xxx
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X-ray photoelectron spectroscopy (XPS) was adopted to analyze
the surface composition and state of Au@AgPd NFs within 2 nm,
and results showed that both Ag and Pd existed in the surface of
Au@AgPd NFs (Fig. S4 in Supporting information). The binding
energy of Pd 3d is evidently shifted to 335.7 and 340.9 eV
compared to the standard Pd 3d peaks (335.2 and 340.4 eV), which
suggests that there is electron transfer from Pd to Ag due to the
alloying of Ag and Pd. To directly observe the spatial distributions
of Ag, Pd and Au in Au@AgPd NFs, high-angle annular darkfield
TEM (HAADF-TEM) equipped with energy-dispersive X-ray (EDX)
elemental mapping was employed, and results are shown in Fig. 1.
By overlaying these elemental maps, it can be seen that Au element
clearly separated from Ag and Pd elements, confirming the core/
shell structure; while the well overlapped flower-like Ag and Pd
maps indicated the alloy structure of AgPd branch. The cross-
sectional composition line profiles also suggest the homogeneity of
the AgPd shell. Taken together, the highly-branched shell are
demonstrated alloy structure in full-scale. The stability of this
alloyed shell was demonstrated by unchanged morphology of
Au@AgPd NFs after reaction with H2O2 (2 wt%) for 20 min (Fig. S5
in Supporting information). This result also implied that the alloy
structure can protect Ag from etching. In addition, the Au@AgPd
NFs showed excellent SERS activity in comparison with Au@Pd NCs
(Fig. S6 in Supporting information). It should note that the Au@Pd
NCs tightly coated with Pd shell also showed slight SERS activity,
which suggest the core/shell structure endowed Pd shell with SERS
activity. The result of finite difference time domain (FDTD)
simulation in Fig. S7 (Supporting information) further confirmed
this conclusion. The reason for markedly enhanced SERS activity of
Au@AgPd NFs may be multiple. Highly-branched shell, addition of
Ag, core/alloy-shell structure may endow the small-sized
Au@AgPd NFs with SERS activity together. However, reliable and
accurately quantitative statements on the SERS enhancement
factor of this complex nanostructure are difficult to be achieved
due to the unknown parameters of molar extinction coefficient and
exact surface area of the Au@AgPd NFs [4].
nanotwins (Figs. 2b and c), which could act as highly efficient
catalytic sites.
To elucidate the mechanism involved in the formation of
highly-branched Au@AgPd NFs,
a set of experiments were
conducted. The role of CTAB was firstly investigated because it
has been widely used in morphological regulation [14–16]. With no
addition of CTAB, the synthesized Au@AgPd NFs showed rough
surface and wide branches (Fig. S8 in Supporting information). This
result suggests that CTAB may not be the key factor governing the
branch formation, but can assist AgPd bloom on Au seeds forming a
highly-branched shell. The possible explanation is that the Ag and/
or Pd nucleated on AuNPs surface and formed Ag and/or Pd islands,
then CTAB capped on the surface of the islands [17] with lower
density on the island top than that on the sides due to their
difference in curvature [18]. This resulted in the deposition of Ag
and Pd atoms on the island top rather than its sides, therefore, the
formation of narrowed AgPd branches. In the absence of CTAB,
however, the difference of AgPd deposition rate between island top
and sides is not that large, and hence broad branches formed.
The molar ratio of Pd to Ag was found to markedly affect the
shell growth. As illustrated in Fig. 3, core/shell structured Au@Pd or
Au@Ag NCs with smooth and rather highly-branched shell was
formed when H2PdCl4 or AgNO3 was used as precursor alone.
However, distinct branches appeared when co-reducing both Pd
and Ag precursors with various Pd/Ag ratios, which imply the
critical role of the coexistence of Ag and Pd metals in the branch
formation. Specifically, the branches changed from sparse to
compact and then to sparse again with increasing of Pd/Ag ratio,
and the Pd/Ag ratio of 1:1 is the optimal point at which closely
spaced, and uniform branches were obtained. This was attributed
to the large lattice mismatch (6.3%), as metals tend to deposit on
substrate in the manner of island growth (Volmer-Weber mode)
when lattice mismatch larger than 5% [19].
The formation of highly-branched shell is also dependent on the
size of Au seed. Citrate-coated AuNCs with different sizes were at
first prepared (Table S1 and Fig. S1 in Supporting information) to
study the branch shell. As shown in Fig. 4, large sized Au core
inhibited the formation of closely compact branch shell. When the
diameter of Au seeds increased to 60 nm, branches can hardly be
observed. Furthermore, the branches tend to grow at the corner of
Au seeds (Fig. 4c), by which the high surface energies of corner can
To further investigate the structure of AgPd branches down to
the atomic level, aberration-corrected HAADF-STEM imaging was
conducted. The lattice fringes were clearly observed when the
Au@AgPd nanoparticle is viewed along the [110] zone axis,
indicating the good crystallization (Fig. 2a). Although discrimina-
tion of Ag and Pd atoms through Z-contrast difference is impossible
due to their adjacent atomic number, AgPd alloy can be confirmed
in atomic level by measuring their lattice spacings. As shown in
Fig. 2a, the average lattice spacing of AgPd branch is determined as
0.2323 nm, which is between that of the (111) plane of Ag
(0.2370 nm) and Pd (0.2230 nm), confirming the AgPd alloy
structure. It is noteworthy that in the AgPd alloy branch there
are abundant lattice defects including steps, atomic corners and
be released and thus
a more stable structure is adopted.
Consistently, smaller sized Au seeds have more twin boundary
sites facilitating the AgPd nucleation, and thus densely branches
tend to grow on small sized AuNPs. Additionally, it should be noted
that the sodium citrate (SC) concentration in all growth solutions
with different AuNCs sizes were kept closely in the range of 0.13–
0.14 mmol/L (Fig. S9 in Supporting information), which suggested
the impact of SC on branches growth is not remarkable.
Fig. 2. (a) Aberration-corrected HAADF-STEM image of branches in Au@AgPd NCs. Step (b) and nanotwins (c) in branches. The inset image in (a) shows the fast Fourier
transform (FFT) pattern.
Please cite this article in press as: Y. Lai, et al., Synthesis of highly-branched Au@AgPd core/shell nanoflowers for in situ SERS monitoring of