Spiky/hollow metal nanoparticles have applications across a broad range of fields. However, the current bottom-up methods for producing spiky/hollow metal nanoparticles rely heavily on the use of strongly adsorbing surfactant molecules, which is undesirable because these passivate the product particles' surfaces. Here we report a high-yield surfactant-free synthesis of spiky hollow Au-Ag nanostars (SHAANs). Each SHAAN is composed of >50 spikes attached to a hollow ca. 150 nm diameter cubic core, which makes SHAANs highly plasmonically and catalytically active. Moreover, the surfaces of SHAANs are chemically exposed, which gives them significantly enhanced functionality compared with their surfactant-capped counterparts, as demonstrated in surface-enhanced Raman spectroscopy (SERS) and catalysis. The chemical accessibility of the pristine SHAANs also allows the use of hydroxyethyl cellulose as a weakly bound stabilizing agent. This produces colloidal SHAANs that remain stable for >1 month while retaining the functionalities of the pristine particles and allows even single-particle SERS to be realized.
Spiky/hollow metal nanoparticles have applications across a broad range of fields. However, the current bottom-up methods for producing spiky/hollow metal nanoparticles rely heavily on the use of strongly adsorbing surfactant molecules, which is undesirable because these passivate the product particles' surfaces. Here we report a high-yield surfactant-free synthesis of spiky hollow Au-Ag nanostars (SHAANs). Each SHAAN is composed of >50 spikes attached to a hollow ca. 150 nm diameter cubic core, which makes SHAANs highly plasmonically and catalytically active. Moreover, the surfaces of SHAANs are chemically exposed, which gives them significantly enhanced functionality compared with their surfactant-capped counterparts, as demonstrated in surface-enhanced Raman spectroscopy (SERS) and catalysis. The chemical accessibility of the pristine SHAANs also allows the use of hydroxyethyl cellulose as a weakly bound stabilizing agent. This produces colloidal SHAANs that remain stable for >1 month while retaining the functionalities of the pristine particles and allows even single-particle SERS to be realized.
Ag and Au nanoparticles
have been extensively studied in the past
few decades due to their unique catalytic and plasmonic properties.[1−6] Up to now, the most popular route to produce Ag and Au nanomaterials
has been through bottom-up colloidal synthesis, which typically employs
a strongly adsorbing surfactant to direct particle growth and provide
colloidal stability.[7−11] A variety of anisotropic metal nanoparticles with distinct properties
can now be synthesized with the aid of surfactants, for instance,
the polyvinylpyrrolidone (PVP)-assisted synthesis of nanocubes,[12−14] the cetyltrimethylammonium bromide (CTAB)-assisted synthesis of
nanorods,[15−17] the Triton-X-assisted synthesis of nanostars, and
so on.[18−20] Whereas the use of surfactant capping molecules offers
easy manipulation of the morphology of the synthesized nanoparticles,
their existence is also problematic for nearly every type of application,
for example, in plasmonic sensing and catalysis, where the surface-bound
surfactant molecules act as both physical and chemical barriers that
restrict the free access of analytes/reactants to the nanosurface,[9,21−23] or in bioapplications where the free surfactants
induce cytotoxicity.[24,25] As a result, methods for the
postsynthesis removal of surfactant molecules or surfactant-free synthesis
have become important areas of research.[26−30] For example, Gao et al. showed that diethylamine
can be used as a general and highly effective intermediate ligand
to facilitate the replacement of strongly adsorbed capping agents
with weakly adsorbed capping agents.[29] Odom
et al. demonstrated that it was possible to use weakly adsorbing and
biocompatible Good’s buffers, such as 4-(2-hydroxyethyl)-1-piperazineethanesulfonic
acid, to synthesize Au nanostars.[30]Among the anisotropic metal nanoparticles reported to date, spiky
or hollow nanoparticles have drawn particular interest as catalysts
due to their large surface-to-volume ratio and the presence of high-index
crystal planes that are composed of highly active low-coordinated
atoms.[31,32] If they are composed of plasmonic materials,
such as Au and Ag, then spiky or hollow nanoparticles have also been
shown to possess significantly enhanced plasmonic properties compared
with their isotropic counterparts.[33−36] To take full advantage of the
plasmonic and catalytic properties of hollow and spiky nanoparticles,
a few research groups have reported methods for synthesizing Au/Ag
nanostars that are both spiky and hollow.[20,37−41] However, in general, bottom-up methods that allow the production
of spiky Au/Ag nanostars that contain a hollow interior remain extremely
rare. More importantly, the current methods for producing Ag/Au nanostars
with hollow interiors are either complex or require the extensive
use of surfactants, which has significantly limited the application
of these particles, despite their promising properties. For example,
Rodríguez-Fernández et al. showed that spiky and hollow
Au nanoparticles with tailored near-infrared plasmonic properties
could be produced using Triton X-100 as the growth-directing agent.[20] Evans et al. showed that spiky and hollow Au
nanoparticles with excellent catalytic and surface-enhanced Raman
spectroscopy (SERS) activity could be produced using methyl-orange-FeCl3 templates.[38]In this work,
we demonstrate a mild and surfactant-free synthesis,
which can be completed at room temperature within minutes to produce
spiky hollow Au–Ag nanoparticles (SHAANs) with ca. 100% morphological
yield. The unique morphology of the SHAANs combined with their highly
accessible surfaces allows them to exhibit outstanding catalytic and
single-particle SERS activities, which were significantly enhanced
compared with those of their conventional surfactant-capped counterparts.
Moreover, the high accessibility of the SHAAN surface also meant that
they could be stabilized in the colloidal state using extremely weakly
bound capping ligands, such as hydroxyethyl cellulose (HEC). This
allowed the product colloid to remain stable for >1 month while
fully
retaining the surface accessibility of the particles. This is significant
because good colloidal stability is crucial for a variety of important
applications, such as catalysis, kinetic monitoring, and slow drug
release,[1,42,43] but has typically
been overlooked in previous studies regarding the surfactant-free
synthesis of colloidal nanoparticles. More generally, the ability
to access enhanced nanoproperties with anisotropic nanoparticles prepared
using an easy and reliable room-temperature process not only offers
a powerful tool for fundamental research but also paves the way for
a broad range of important real-life applications, such as trace molecule
detection, biomedical diagnostics, or the construction of functional
devices.
Results and Discussion
The synthesis of the SHAANs
is a simple and rapid one-step process.
In brief, NaCl and AgNO3 solutions are first added in sequence
to a HAuCl4 solution under constant stirring. The mixture
is then incubated, after which l-ascorbic acid solution is
quickly injected. (See details in the Materials and Methods section
of the Supporting Information.) This causes
the color of the solution to change immediately (typically within
ca. 15s), indicating the formation of the product nanoparticles. The
critical step in the process is the incubation of the mixed HAuCl4, NaCl, and AgNO3 solution before the addition
of l-ascorbic acid. As shown in Figure a–e, the morphology of the nanoparticles
obtained changed dramatically with different incubation times. The
addition of ascorbic acid without incubation produced small spiky
nanoparticles with an average diameter of ca. 40 nm. The resulting
colloid had a light-blue color with λmax measured
via UV–vis at ca. 782 nm (Figure f,g). Further scanning transmission electron
microscopy (STEM) characterization and energy-dispersive X-ray (EDX)
spectroscopy of this colloid sample revealed that some of the nanoparticles
that appeared to have a hollow interior when observed with scanning
electron microscopy (SEM) actually had a Ag/AgCl core (Figure S1). As shown in Figure b, when the incubation time was extended
to 5 min, approximately half of the nanoparticles became larger SHAANs
with a particle diameter of ca. 150 nm. These SHAANs had a larger
number of spikes on the surface compared with smaller nanoparticles
obtained with less incubation, and the spikes were notably narrower
and longer. Additionally, the interiors of particles were found to
be hollow, which will be discussed in detail in the following section.
The change in morphology with incubation was also reflected in the
color of the colloids and their UV–vis extinction spectra.
As shown in Figure f,g, the color of the colloids with incubation was clearly different,
and their extinction peaks were broadened and red-shifted significantly
compared with the nonincubated sample. The optimal incubation time,
which led to the highest yield (ca. 100% morphological yield) of SHAANs,
was found to be 10 min, as shown in Figure c. The resulting colloid was gray, with its
UV–vis extinction peak centered around 805 nm (Figure f,g). Extending the incubation
time beyond 10 min led to the population of SHAANs decreasing and
eventually nearly completely disappearing. As shown in Figure d, the population of the product
colloid with 15 min of incubation was similar to those obtained with
5 min of incubation, which is reflected by their identical colors
and UV–vis extinctions (Figure f,g). If the incubation time was increased to 60 min,
then very few SHAANs were formed, and the product colloid mainly consisted
of small (ca. 30 nm) spheres (Figure e). Unsurprisingly, this colloid was purple, with a
UV–vis extinction centered at ca. 527 nm (Figure f,g), which is characteristic
of small spherical Au nanoparticles.[44]
Figure 1
(a–e)
Scanning electron microscopy (SEM) images of Au/Ag
alloy nanoparticles synthesized by incubating the mixture solution
of HAuCl4, NaCl, and AgNO3 for (a) 0, (b) 5,
(c) 10, (d) 15, and (e) 60 min and then adding ascorbic acid. Scale
bars in all images correspond to 500 nm. (f) Corresponding optical
images of colloids prepared with different incubation times. (g) UV–vis
spectra of colloids prepared with different incubation times.
(a–e)
Scanning electron microscopy (SEM) images of Au/Ag
alloy nanoparticles synthesized by incubating the mixture solution
of HAuCl4, NaCl, and AgNO3 for (a) 0, (b) 5,
(c) 10, (d) 15, and (e) 60 min and then adding ascorbic acid. Scale
bars in all images correspond to 500 nm. (f) Corresponding optical
images of colloids prepared with different incubation times. (g) UV–vis
spectra of colloids prepared with different incubation times.Further characterization of the nanoparticles was
performed by
scanning transmission electron microscopy–high-angle annular
dark field (STEM-HAADF) imaging. This was used in combination with
energy-dispersive X-ray spectroscopy (EDX) to investigate the internal
morphology, local elemental distribution, and composition of the SHAANs.
Images from the 10 min incubated specimen revealed that the homogeneous
population of nanoparticles has cubic hollow cores in addition to
the spiky surface morphology observed by SEM (Figure a). The average diameter of the cubic core
was found to be 150 ± 16 nm, as measured from 100 individual
SHAANs. Figure b shows
the high-magnification STEM-HAADF image of a typical SHAAN. The hollow
cavity of the SHAAN was measured to be ca. 100 nm in diameter, and
the length of spikes ranged between 30 and 45 nm. Elemental mapping
revealed a fairly evenly dispersed mixture of Ag and Au, which resembled
bimetallic Au–Ag alloys, with a mean composition of 90 at %
Au and 10 at % Ag (Figure c,d). Interestingly, as shown in Figure e,f, the high-magnification elemental line
scan also revealed that the at % ratio between Ag and Au was clearly
higher at the surface of the SHAANs, which suggested the existence
of a ∼1 nm thick Ag-rich surface layer that could have been
formed due to the lower surface energy of Ag compared with Au.[45] STEM-HAADF analysis for a nonincubated specimen
(see Figure S2) also revealed some hollow
particles but with a smaller and less regular size and shorter spikes,
consistent with the SEM data. These particles also had a composition
of 90 at % Au and 10 at % Ag and a few nanometers thick Ag-rich surface
layer (Figures S3 and S4).
Figure 2
(a) Low- and (b) high-magnification
scanning transmission electron
microscopy–high-angle annular dark field (STEM-HAADF) images
of SHAANs. Energy-dispersive X-ray (EDX) elemental mapping of SHAANs:
(c) Au mapping image and (d) Ag mapping image. (e) EDX elemental mapping
of a tip on the SHAAN shown in panel b. (f) Plot showing the material
composition obtained with a high-magnification elemental line scan
across the line labeled in panel e. Scale bars in panel a, panels
b–d, and panel e correspond to 200, 60, and 10 nm, respectively.
(a) Low- and (b) high-magnification
scanning transmission electron
microscopy–high-angle annular dark field (STEM-HAADF) images
of SHAANs. Energy-dispersive X-ray (EDX) elemental mapping of SHAANs:
(c) Au mapping image and (d) Ag mapping image. (e) EDX elemental mapping
of a tip on the SHAAN shown in panel b. (f) Plot showing the material
composition obtained with a high-magnification elemental line scan
across the line labeled in panel e. Scale bars in panel a, panels
b–d, and panel e correspond to 200, 60, and 10 nm, respectively.The proposed mechanism for the formation of SHAANs
is shown in Scheme . The synthesis is
initiated by the addition of AgNO3 to a mixed NaCl/HAuCl4 solution, which leads to the formation of small AgCl seed
nanoparticles. This is consistent with the observation that the mixture
solution gradually changes from transparent to slightly cloudy after
the addition of AgNO3. Subsequent incubation leads to the
growth of the AgCl seeds to form larger cubic AgCl nanoparticles;
however, this process can be interrupted by the addition of ascorbic
acid, which triggers a series of redox reactions (Table S1) that ultimately lead to the formation of SHAANs
if the optimized incubation time of 10 min is used. More specifically,
the addition of ascorbic acid to the incubated solution leads to the
reduction of the AgCl nanoparticles to Ag0 nanoparticles,
as has been previously observed.[46−48] However, these are not
stable in the presence of Au3+ cations, which can galvanically
reduce them, leading to the replacement of the Ag0 by Au0 in the nanocrystal structure, a process that would be expected
to yield cubic hollow Au shells.[46,47] Simultaneously,
the presence of ascorbic acid and Au3+ cations along with
residual Ag+ and Cl– leads to growth
of spikes on the surface of the particles.[34]
Scheme 1
Schematic Illustration of the Formation of SHAANs with 10 min of
Incubation Time Compared with When a 0 min of Incubation Is Used
Without incubation, the reaction
goes through three simultaneous pathways, which leads to the formation
of a mixture of nanoparticles including solid Au stars, Au hollow
spheres, hollow Ag–Au stars, and solid Au stars with spherical/cubic
AgCl cores. With 10 min of incubation, the reaction goes through a
single pathway, leading to the formation of SHAANs.
Schematic Illustration of the Formation of SHAANs with 10 min of
Incubation Time Compared with When a 0 min of Incubation Is Used
Without incubation, the reaction
goes through three simultaneous pathways, which leads to the formation
of a mixture of nanoparticles including solid Au stars, Au hollow
spheres, hollow Ag–Au stars, and solid Au stars with spherical/cubic
AgCl cores. With 10 min of incubation, the reaction goes through a
single pathway, leading to the formation of SHAANs.This mechanism accounts for the importance of the duration
of the
incubation step and the nature of the products that are formed when
it is changed from the optimum value. If the initial mixture was over-incubated
(60 min), then the majority of Ag+ and Cl– ions were consumed in the growth of AgCl nanoparticles, and not
enough were left to assist the formation of Au spikes. Therefore,
the nanoparticles formed by the subsequent addition of ascorbic acid
were mostly quasi-spherical (Figure e). In contrast, if the initial mixture was under-incubated
(0 min), then there were not sufficient AgCl seeds to template the
growth of SHAANs, and the AgCl seeds that were available were under-grown,
which resulted in the formation of polydisperse spiky/hollow nanoparticles
(Figure a and Figure S2). Although it is important to use the
correct incubation time to achieve an appropriate balance between
AgCl seeds, Ag+ and Cl– necessary for
the formation of SHAANs (Figure c), it is useful to stress that provided that this
time is used, the process is very robust, and it reliably generates
SHAANs, as shown by SEM and SERS measurements in Figures S5 and S6. Although AgCl nanoparticles act as intermediates
during the synthesis, a significant amount of residual AgCl is not
expected to be present in the product SHAANs because it is reduced
by the excess ascorbic acid in the solution. This was confirmed by
the observation that washing SHAANs with ammonia–water, which
would dissolve any residual AgCl, gave no detectable change in the
morphology of the SHAANs (Figure S7).X-ray photoelectron spectroscopy (XPS) was used to further study
the surface composition of the SHAANs, in particular, to identify
the oxidation state of the metals and the number of species present.
Surprisingly, the XPS revealed that Ag was present in just one oxidation
state, Ag+, indicated by the photoelectron peak at 367.5
eV (Ag 3d5/2) (Figure a).[49,50] Because, as previously discussed,
it is unlikely that a significant amount of AgCl is present in the
product SHAANs, the Ag+ observed by XPS is most likely
in the form of Ag2O, which is formed postsynthesis due
to the high reactivity of colloidal Ag toward oxygen.[51] As shown in Figure b, the XPS also showed a photoelectron peak at 83.4 eV, corresponding
to metallic Au 4f7/2. Interestingly, the binding energy
observed for Au was lower than the conventional values reported in
literature (84.0 eV). This could be due to charge-transfer effects
that arise from the formation of Ag–Au alloys in the SHAANs.[52,53]Table S2 and Figure S8 show the XPS data
and at % of the relevant elements in the SHAAN sample from XPS. Importantly,
as a surface-specific technique, the XPS results were consistent with
the Ag surface enrichment observed in the STEM-elemental mapping and
showed that the at % ratio between Ag and Au (1:1.6) on the surface
of the SHAANs was much higher than the overall ratio between Ag and
Au in the whole particle (1:9).
Figure 3
XPS analysis of SHAANs showing the characteristic
peaks of (a)
Ag and (b) Au.
XPS analysis of SHAANs showing the characteristic
peaks of (a)
Ag and (b) Au.The plasmonic properties of SHAANs
were investigated using a finite
element method, with the particle structure and material composition
modeled according to the microscopy measurements. (See the Materials
and Methods section of the Supporting Information.) The volume-averaged near-field enhancement factor was calculated
aswhere the volume V was made
by a 2 nm thick shell covering the nanoparticle surface (Figure a). Figure b compares the calculated electromagnetic
field distribution of individual SHAANs (x corresponds to the approximated length of the
spikes within a SHAAN) and a hollow cube core excited by 785 nm laser.
Regardless of the exact spike length, the near-field enhancement factor
maps showed that the distribution of the excited surface plasmon resonance
was mainly localized around the sharp tips rather than within the
hollow cavity. Essentially, the electromagnetic-field distribution
around the SHAANs was much more similar to that of solid nanostars
rather than hollow/porous nanoparticles or nanocubes.[54−56] The profile and strength of the volume-averaged near-field enhancement
were found to be highly dependent on the length of the spikes. For
example, Figure c
shows a plot comparing the volume-averaged near-field enhancement
of individual hollow cubes and SHAANs at different wavelengths, which shows that the optimal excitation
wavelength shifted by >200 nm when the spike length increased from
20 to 40 nm. Figure d compares the maximum and average near-field enhancement of hollow
nanocubes and SHAANs at the same excitation
wavelength as our Raman measurements (see as follows). As shown in
the plot, the SHAANs were significantly
more plasmonically active compared with hollow nanocubes. Interestingly,
the simulations also revealed that the maximum near-field enhancement
increased with the increasing spike length of the SHAANs, whereas
the volume-averaged enhancement decreased.
Figure 4
Finite element method
simulation of the electrodynamic of SHAANs and hollow cube nanostructures. (a) 3D renderings
of a SHAAN, in red (30 nm spike length), and of the volume, in light
blue, which define the volume-averaged near-field enhancement factor.
(b) Near-field enhancement factor maps for SHAANs with three different spike lengths x (x = 20, 30, or 40 nm) and the hollow nanocube core. (c)
Volume-averaged near-field enhancement factors for the structures
in panel b. (d) Comparison between the volume-averaged near-field
enhancement factors and maximum punctual enhancement factor of the
structures in panel b calculated at 785 nm excitation wavelength.
Finite element method
simulation of the electrodynamic of SHAANs and hollow cube nanostructures. (a) 3D renderings
of a SHAAN, in red (30 nm spike length), and of the volume, in light
blue, which define the volume-averaged near-field enhancement factor.
(b) Near-field enhancement factor maps for SHAANs with three different spike lengths x (x = 20, 30, or 40 nm) and the hollow nanocube core. (c)
Volume-averaged near-field enhancement factors for the structures
in panel b. (d) Comparison between the volume-averaged near-field
enhancement factors and maximum punctual enhancement factor of the
structures in panel b calculated at 785 nm excitation wavelength.The SERS performance of SHAANs was first investigated
using 4-mercaptobenzoic
acid (MBA) as the model analyte. Strong SERS signals of MBA were observed
using freshly prepared, well-dispersed pristine SHAANs colloids as
the enhancing substrate, and the limit of detection was measured to
be ca. 10–8 M, as shown in Figure S9. The analytical enhancement factor (AEF), which is calculated
differently from the enhancement factor (EF), is widely regarded as
the gold standard for quantifying the enhancing ability of colloidal
SERS substrates because the complex geometry makes the direct calculation
of EF difficult.[57] Using MBA as the probe
analyte, the AEF of SHAANs was determined to be ca. 4.9 × 105 under nonresonant conditions for the pristine SHAAN colloid
(Figure S9). This value is notably stronger
than the enhancement predicted in Figure , which is likely due to the presence of
additional far-field electromagnetic enhancement and chemical enhancement
that are not considered in the simulations. It is worth noting that
this experimentally recorded value is comparable to the AEF value
reported for state-of-the-art plasmonic particles, such as Au nanotriangles
(ca. 1.2 × 105), and to aggregated silver nanoparticles
(ca. 5 × 105), which have been used for single-molecule
SERS.[57,58] To clearly demonstrate the advantages of
the SHAANs, we compared the SERS of MBA on SHAANs with solid nanostars
synthesized following a well-recognized surfactant-free approach from
the literature and with surfactant-free hollow Ag–Au nanocubes
produced via an in-house procedure derived from literature.[56,59] As shown in Figure S10, the hollow nanocubes
were ca. 250 nm in diameter, which was similar to the diameter of
the cubic hollow core of the SHAANs, whereas the solid nanostars were
ca. 50 nm in diameter. As shown in Figure S11, the SERS signals of MBA were clearly the strongest on SHAANs. More
specifically, under the same unaggregated experimental conditions,
no signals of MBA were observed from the hollow nanocubes, whereas
the SERS signals of MBA obtained from the conventional solid nanostars
were more than two times weaker than the signals of MBA obtained from
SHAANs.It is important to note that the strong AEF of SHAANs
arises not
only from their excellent plasmonic properties but also from their
chemically exposed surfaces. More specifically, the surfactant-free
synthesis means that the only chemical species adsorbed on the surface
of the SHAANs were Cl– ions originating from HAuCl4 and NaCl. It is known that charged ligands, such as Cl–, occupy only ca. 20% of the surface of Ag/Au nanoparticles.[60] As a result, the blank SERS signals of the pristine
SHAANs colloids showed only a single weak Au–Cl vibration band
(Figure S12). This means the surface of
SHAANs is much more accessible to analyte molecules than conventional
spiky nanostars, which are covered in strongly adsorbed ligands, such
as Triton-X, PVP, or poly(ethylene glycol) methyl ether thiol. The
lack of capping agents in surfactant-free syntheses does lead to issues
in the long-term stability of the product nanoparticle colloids because
there are no capping ligands to protect the nanoparticles from aggregation.
Indeed, it was found that the pristine SHAANs colloids were very unstable
against aggregation and typically precipitated as aggregates from
solution within 1 h. The challenge is to be able to stabilize the
SHAAN colloid without compromising the surface accessibility of the
particles. This was not a problem because another advantage of the
surfactant-free environment is that it allowed us to use weakly adsorbed
polymeric molecules, such as HEC polymer, as stabilizing agents.[61−63] This allowed the SHAANs to remain highly stable for >1 month,
as
characterized by UV–vis spectroscopy (Figure S13), while retaining their surface accessibility for further
applications. Interestingly, SERS monitoring of the same batch of
SHAANs revealed that their SERS activity slightly decreased, by approximately
two-fold, during the first day of storage (Figure S14). This is most likely due to oxidation of the thin Ag surface
layer rather than aggregation or Ostwald ripening of the SHAANs because
the extinction spectrum of the colloid remained unchanged.[17,64] More importantly, the long-term SERS kinetics showed that the slight
decrease in SERS activity was observed only during the first day of
storage, after which the SHAANs remained highly plasmonically stable
for >1 month. The high chemical stability of SHAANs against further
oxidation is likely due to SHAANs being mainly composed of a Ag–Au
alloy, which is consistent with previous plasmonic studies comparing
Ag and Ag–Au nanocubes.[64]Figure a compares
the SERS activity of three batches of pristine, HEC-stabilized, and
PVP-stabilized SHAAN colloids for the detection of a model SERS analyte,
crystal violet (CV). As shown in spectra sets i and ii, the intensity
of the SERS signals of CV was fully retained on the HEC-SHAANs. In
contrast, because the Cl–, which must adsorb onto
the enhancing surface to facilitate the adsorption of the cationic
CV dye, cannot displace PVP, a significant drop in SERS intensity,
by approximately ten-fold, was observed when PVP-SHAANs (Figure a, spectrum iii)
were used as the enhancing substrate. It is worth noting that CV is
not a special case. The exposed surface of SHAANs also provides significant
advantages in the SERS detection of important real-life targets. For
example, Figure b,c
compares the SERS signals of two anticancer drugs, Niraparib and Doxorubicin,
obtained using pristine SHAANS, HEC-SHAANs, and PVP-SHAANs at a final
drug concentration of 10–5 M. For both anticancer
drugs, the SERS signals were intense on pristine SHAANS and HEC-SHAANs
but barely visible on PVP-SHAANs, which emphasizes the importance
of surface accessibility in the SERS monitoring of real-life analytes.
Figure 5
(a) SERS
spectra of 10–6 M crystal violet (CV),
(b) 10–5 M doxorubicin (DOX), and (c) 10–5 M niraparib (NI) recorded on pristine SHAAN colloid (i), hydroxyethyl-cellulose
(HEC)-stabilized SHAAN colloid (ii), and PVP-stabilized SHAAN colloid
(iii). (d) Time-dependent SERS spectra showing single SHAANs moving
into and out of the probed laser volume. Spectra with detectable SERS
signals of the MBA analyte at 1045 cm–1 are highlighted
in red. The plot below shows the change in the SERS signal for an
extended period of 20 s, with red dots representing the appearance
of the MBA signal and black dots representing the disappearance of
the MBA signal. (e,f) Plots showing the decrease in the concentration
of 4-nitrophenol with time in the NaBH4 reduction of 4-nitrophenol
catalyzed by (e) HEC- and (f) PVP-stabilized SHAANs. Insets show the
rates of the reactions.
(a) SERS
spectra of 10–6 M crystal violet (CV),
(b) 10–5 M doxorubicin (DOX), and (c) 10–5 M niraparib (NI) recorded on pristine SHAAN colloid (i), hydroxyethyl-cellulose
(HEC)-stabilized SHAAN colloid (ii), and PVP-stabilized SHAAN colloid
(iii). (d) Time-dependent SERS spectra showing single SHAANs moving
into and out of the probed laser volume. Spectra with detectable SERS
signals of the MBA analyte at 1045 cm–1 are highlighted
in red. The plot below shows the change in the SERS signal for an
extended period of 20 s, with red dots representing the appearance
of the MBA signal and black dots representing the disappearance of
the MBA signal. (e,f) Plots showing the decrease in the concentration
of 4-nitrophenol with time in the NaBH4 reduction of 4-nitrophenol
catalyzed by (e) HEC- and (f) PVP-stabilized SHAANs. Insets show the
rates of the reactions.The outstanding AEF of
SHAANs also suggests that they might be
suitable for single-particle SERS measurements, which is an important
property in both fundamental and applied studies, such as SERS sensing
and imaging in biological samples.[65,66] The HEC-SHAAN
colloid was diluted, labeled with MBA, which is commonly used as a
Raman tag molecule for biological studies, and Raman-probed using
a confocal Raman microscope with a diffraction-limited probe diameter
of 1.04 μm to test this. Figure d shows a subset of the SERS spectra from a total of
20 spectra series continuously recorded at 1 s intervals. Even though
MBA is a nonresonant analyte and the accumulation time was short,
the signal of MBA was still intense and was measured to be 38 ±
11 counts using the characteristic peak at 1045 cm–1. More importantly, the MBA signals showed an on/off pattern, which
is associated with the movement of the enhancing particle–substrate
moving into and out of the probed volume due to Brownian motion. Because
within this diluted SHAAN colloid there is only a single particle
every 2000 μm3 (see the Supporting Information for details), which is more than 2000 times larger
than the probe volume (0.7 μm3) of the confocal microscope,
this meant that the consistently observed on/off signals of MBA most
likely arose from a single SHAAN in the probe laser acting as a single-particle
SERS probe. To validate that the SHAANs were active as single particles,
we studied the effect of colloidal aggregation on the plasmonic properties
of SHAANs by performing contrast SERS kinetic experiments using pristine
and HEC-SHAANs. As shown in Figure S15,
the SERS signals obtained from the pristine SHAANs decreased almost
linearly as they aggregated naturally without any visible precipitation,
whereas the SERS signals of the unaggregated HEC-SHAANs remained constant
over the same period of time. This shows that aggregation has a negative
impact on the SERS activity of the SHAANs, which is consistent with
previous reports regarding star-type Au particles,[67,68] and more importantly, argues against attributing the intermittent
signals in Figure d to aggregates. The SERS properties of the SHAANs functionalized
with MBA Raman tags were also studied in artificial serum, which contained
3.3 wt % albumin, to mimic a real-life environment. SERS analysis
in the presence of albumin is challenging because albumin is known
to compete with analyte molecules for the enhancing surface and prevent
particle aggregation, which is often crucial for the formation of
plasmonic hot spots.[69,70] As shown in Figure S16, because the MBA Raman tag molecules were strongly
adsorbed on the single-particle SERS-active SHAANs, this allowed the
strong SERS signals of MBA from the SHAANs to be fully retained, even
in the presence of albumin, which demonstrates their potential in
biochemical applications, for example, as pH reporters.The
HEC-SHAANs also showed superior catalytic properties to PVP-SHAANs.
As shown in Figure e, the reduction of 4-nitrophenol by NaBH4 occurred immediately
when catalyzed by HEC-stabilized SHAANs, as measured by UV–vis
spectroscopy (Figure S17). In contrast,
for PVP-stabilized SHAANs, there was a delay of ca. 90 s before any
reaction could be detected (Figure f and Figure S18). In addition,
the average rate constant for the reaction catalyzed by the HEC-SHAANs
(k = 0.0406 ± 0.0015 s–1)
was more than 3.8 times faster than that for their PVP-stabilized
counterparts (k = 0.0105 ± 0.0015 s–1), as shown in the insets of Figure e,f. This can be attributed to the need for surface
reconstruction of PVP-SHAANs when acting as catalysts due to the strongly
adsorbed PVP capping on the particles’ surfaces.[71]The high yield and excellent properties
of the SHAANs also makes
them promising candidates for the construction of multidimensional
nanomaterials with advanced functionalities. For illustration, we
show that HEC-SHAANs can be readily used as the building block for
the construction of surface-exposed nanoparticle sheets (SENSs) via
an interfacial self-assembly technique previously reported by our
group.[72]Figure shows typical SEM
and SERS results obtained from SHAAN SENSs. As shown in Figure a,b, the SHAANs in SENSs are
held as a densely packed 2D monolayer anchored on the surface of the
polystyrene. Importantly, the surface of the HEC-SHAANs in SENSs is
both chemically and physically exposed for interactions in applications. Figure c shows a 5 μm
× 5 μm Raman map of the HEC-SHAAN SENS with MBA adsorbed
on the particle surface. As shown in Figure d, the assembled SHAANs remained highly plasmonically
active, and the relative standard deviation of the SERS intensity
of the MBA peak at 1045 cm–1 across 100 randomly
selected points within this mapped area was very low at just 10.8%,
which demonstrates the potential of HEC-SHAANs as a plasmonic building
block for constructing uniform and active plasmonic devices.
Figure 6
(a) SEM image
of a SHAAN SENS showing a monolayer of densely packed
SHAANs on the surface. (b) Atomic force microscopy (AFM) and (c) Raman
mapping images across a 5 μm × 5 μm area on the SHAAN
SENS labeled with MBA. (d) Raman intensity of the MBA peak at 1045
cm–1 obtained from 100 random spots on the Raman
mapping image.
(a) SEM image
of a SHAAN SENS showing a monolayer of densely packed
SHAANs on the surface. (b) Atomic force microscopy (AFM) and (c) Raman
mapping images across a 5 μm × 5 μm area on the SHAAN
SENS labeled with MBA. (d) Raman intensity of the MBA peak at 1045
cm–1 obtained from 100 random spots on the Raman
mapping image.
Conclusions
We have demonstrated
a rapid, mild, and surfactant-free one-pot
synthesis to prepare spiky Ag–Au nanoparticles (SHAANs) with
near 100% morphological yield. The as-synthesized nanoparticles have
a hollow interior with a dense covering of narrow spikes irradiating
from the surface, which gave rise to distinct catalytic and plasmonic
properties. Moreover, the fact that the synthesis was surfactant-free
meant that the surfaces of the SHAANs were chemically exposed, which
allowed the use of HEC as a weakly bound stabilizing agent to ensure
colloidal stability while retaining surface accessibility for further
applications. As a result, the HEC-SHAANs not only were highly stable
but also exhibited greatly enhanced functionalities as both SERS substrates
and catalysts when compared against their surfactant-capped counterparts.
The combination of easy preparation and outstanding functionality
means that SHAANs have the potential to be exploited in a broad range
of applications as both functional materials in their own right and
as building blocks for functional materials with advanced properties.
Authors: Kallum M Koczkur; Stefanos Mourdikoudis; Lakshminarayana Polavarapu; Sara E Skrabalak Journal: Dalton Trans Date: 2015-10-05 Impact factor: 4.390
Authors: Ming Yang; Ramón Alvarez-Puebla; Hyoung-Sug Kim; Paula Aldeanueva-Potel; Luis M Liz-Marzán; Nicholas A Kotov Journal: Nano Lett Date: 2010-10-13 Impact factor: 11.189
Authors: E Dumont; C De Bleye; J Cailletaud; P-Y Sacré; P-B Van Lerberghe; B Rogister; G A Rance; J W Aylott; Ph Hubert; E Ziemons Journal: Talanta Date: 2018-04-10 Impact factor: 6.057
Authors: Thomas J A Slater; Alexandra Macedo; Sven L M Schroeder; M Grace Burke; Paul O'Brien; Pedro H C Camargo; Sarah J Haigh Journal: Nano Lett Date: 2014-03-07 Impact factor: 11.189