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PAPER www.rsc.org/analyst | Analyst
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View Article Online / Journal Homepage / Table of Contents for this issue
Sensitive and selective localized surface plasmon resonance light-scatteringsensor for Ag+ with unmodified gold nanoparticles
Chengke Wu, Cen Xiong, Linjing Wang, Chongchong Lan and Liansheng Ling*
Received 3rd April 2010, Accepted 8th July 2010
DOI: 10.1039/c0an00201a
A novel localized surface plasmon resonance (LSPR) light-scattering sensor for Ag+ was developed
with unmodified gold nanoparticles (AuNPs), based upon the specific recognition property of Ag+ with
a cytosine–cytosine mismatched base pair. The addition of Ag+ induced the oligonucleotide 50-TAC
ATA CAT ACT ATC TAT CTA-30 to be desorbed from the surface of the AuNPs, resulting in the
aggregation of AuNPs, accompanied by a dramatic enhancement of the LSPR light-scattering
intensity. The enhancement of LSPR light-scattering intensity was proportional to the concentration of
Ag+ in the range of 0.13–1.12 mM, with a limit of detection of 62.0 nM. The results were also proved by
a colorimetric method. Furthermore, this method can provide satisfactory results for the determination
of Ag+ in water samples and industrial products.
Introduction
Silver ions play a significant role in the photography, pharmacy
and imaging industries. With the increase in the application of
Ag+, much more attention has been paid to its potential toxicity.1
Silver ions exist in water in the form of inorganic or organic
compounds, which could be bioaccumulated by aquatic
creatures.2,3 The accumulation of Ag+ can restrain the activity of
protein, influence the reproduction of aquatic creatures and
terrestrial organisms. Thus, a rapid and sensitive analysis of Ag+
in environmental or industrial samples is of vital importance. For
these reasons, several methods for Ag+ analysis have been
developed, such as fluorescence spectrometry,4,5 neutron activa-
tion analysis,6 electrochemistry,7–9 atomic absorption spectrom-
etry,10,11 inductively coupled plasma mass spectrometry,12
spectrophotometry13,14 and scanning electrochemical micros-
copy.15 Some of these can achieve a detection limit at the ppm
level.
Au nanoparticles (AuNPs) have specific photonic properties
and exhibit various surface plasmon resonance and surface
plasmon absorption with different sizes. The color of AuNPs is
red when they are dispersed in water, but it changes into purple,
even blue, when aggregation of the AuNPs occurs.16–20 The
assembly and disassembly of AuNPs can be controlled by DNA
hybridization and other recognition processes. Colorimetric
sensors such as those involving the detection of DNA,16,19–22
RNA,23 protein,24–26 small molecules,27,28 and metal ions29–38 have
been reported based upon each recognition process. Recently,
a sensitive and selective colorimetric sensor for Ag+ was devel-
oped by Li et al.39 and Zhou et al.40 using G-quadruplex DNA.
The detection limit of most of these assays was in the mM range,
only a few reached the nM range.
Localized surface plasmon resonance (LSPR) is a photon-
driven coherent oscillation of the surface conduction electrons,
which are excited by electromagnetic radiation. The light
School of Chemistry and Chemical Engineering, Sun Yat-Sen University,Guangzhou, 510275, People’s Republic of China. E-mail: [email protected].; Tel: 0086-20-84110156
2682 | Analyst, 2010, 135, 2682–2687
interacts with particles much smaller than the incident wave-
length and the electrons in the nanoparticles oscillate locally
around the nanoparticles. Moreover, LSPR light-scattering
happens when the electromagnetic wave frequency is the same as
that of the oscillating electron.41 Because of its good sensitivity
and convenient apparatus manipulation, the LSPR light-scat-
tering method based on AuNPs has been used for the determi-
nation of amino acids,42,43 biomolecules44–46 and other samples.47
Here we report a new Ag+ sensor with unmodified AuNPs based
upon its specific C–C mismatch recognition property, which
demonstrates a new strategy to investigate other types of metal–
DNA interaction in the future.
Experimental
Chemicals and materials
HAuCl4$3H2O was purchased from Sigma-Aldrich Co., and
oligonucleotides were synthesized by Shanghai Sangon Biolog-
ical Engineering Technology & Services Co., Ltd. (Shanghai,
China). All reagents were AR unless mentioned otherwise, and
the water was double distilled water.
Design of the oligonucleotide
Oligodeoxyribonucleotide with the sequence of 50-TAC ATA
CAT ACT ATC TAT CTA-30 (oligo-1) was designed for our
research. As shown in Fig. 1, it can adsorb on the surface of
AuNPs and prevent the aggregation of AuNPs in the presence
of a sodium salt. The addition of Ag+ leads to the formation of
dsDNA and desorption of the oligonucleotide from the gold
nanoparticles. Oligodeoxyribonucleotide 50-ACA ACA ACA
ACA TCT TTT TTT-30 (oligo-2), which contains the same base
contents but a different sequence to that of oligo-1, was selected
as a control sequence.
Instruments
Intensity and LSPR light-scattering spectra were measured with
an RF-5301PC spectrofluorimeter (Shimadzu, Japan) with an IR
This journal is ª The Royal Society of Chemistry 2010
Fig. 1 Scheme of recognizing a Ag+ ion with unmodified AuNPs, based
upon its specific binding to a C–C mismatched base pair.
Fig. 2 LSPR light-scattering spectra of AuNPs–oligonucleotide with
and without Ag+. a) 0.78 nM AuNPs + 0.5 mM oligo-1 + 0.02 M NaNO3;
b) a + 0.5 mM Ag+; c) 0.78 nM AuNPs + 0.5 mM oligo-2 + 0.02 M
NaNO3; d) c + 0.5 mM Ag+.
Fig. 3 Solution color and absorption spectra of the AuNPs–oligonu-
cleotide with and without Ag+. a) 3.87 nM AuNPs + 3.23 mM oligo-1 +
0.096 M NaNO3; b) a + 6.45 mM Ag+; c) 3.87 nM AuNPs + 3.23 mM
oligo-2 + 0.096 M NaNO3; d) c + 6.45 mM Ag+.
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sensitive detector. All absorbance measurements were made with
a TU-1901 double-beam spectrophotometer (Beijing Purkingje
General Instrument Co., Ltd., China). Transmission electron
microscopy (TEM) images were recorded with a JEM-2010HR
transmission electron microscope (JEOL Ltd., Japan).
Preparation of Au nanoparticles
AuNPs with an average diameter of 13 nm were prepared using
the method of the reaction of HAuCl4 with citrate. Sodium
citrate solution (3.0 mL, 38.8 mM) was added to a stirred boiling
solution of HAuCl4 (30 mL, 1.0 mM), after the color turned to
red, keeping the solution boiling for another 20 min, then it was
cooled down to room temperature, and the AuNPs were
collected after filtering through a 0.45 mm filter membrane.
Preparation of samples for LSPR light-scattering detection
Oligo-1 (100 mM, 10 mL) with different concentrations of Ag+
ions was added to the gold nanoparticles (10.44 nM, 150 mL),
then 150 mL buffer (PBS, 10 mM) was injected into the solution
to control the pH value, and 15 mL NaNO3 (2.0 M) was added to
control the ion strength. Finally, the mixture was diluted to
2.0 mL with distilled water for LSPR light-scattering determi-
nation. All of the LSPR light-scattering spectra were obtained by
simultaneously scanning the excitation and the emission wave-
length (namely Dl ¼ 0 nm) from 300 to 800 nm, by keeping the
slit width for excitation and emission at 3.0 nm.
Preparation of samples for colorimetric detection
Oligo-1 (100 mM, 10 mL) with a quantity of Ag+ (100 mM, 20 mL)
was added to the AuNPs (10.44 nM, 115 mL), then 150 mL buffer
solution (PBS, 10 mM) was injected into the solution to control
the pH, and 15 mL NaNO3 (2.0 M) was added subsequently.
Results and discussions
Spectra characteristics
The LSPR light-scattering spectra of AuNPs–oligonucleotides
with and without Ag+ were studied. As demonstrated in Fig. 2,
the LSPR light-scattering spectrum of AuNPs–oligo-1 changed
noticeably after the addition of Ag+. When AuNPs–oligo-1 was
observed in the absence of Ag+ ions, the LSPR light-scattering
spectrum was weak within the range of 300–800 nm (curve a),
This journal is ª The Royal Society of Chemistry 2010
while the intensity was enhanced dramatically after the addition
of Ag+ ions, and the light scattering intensity reached a maximum
peak at 665 nm (curve b). This phenomenon suggests the
aggregation of AuNPs.41 Comparatively, the AuNPs with
a control sequence of oligo-2 showed no change in the LSPR
light-scattering spectrum before and after the addition of Ag+
(curve c, d).
The effect of Ag+ on the solution color and the absorption
spectrum was investigated as well. It is demonstrated in Fig. 3
that the solution of AuNPs–oligo-1 was red with a maximum
absorption peak at 520 nm in the presence of 0.096 M NaNO3,
while it changed from red to purple after Ag+ was added,
accompanied by a dramatic decrease in absorption intensity at
520 nm and the appearance of a new absorption band at a longer
wavelength. These phenomena may be due to the aggregation of
AuNPs,19 which is in good accordance with the results of the
LSPR light-scattering spectra. However, the addition of Ag+ had
little effect on the solution color and the absorption spectrum of
AuNPs–oligo-2, which revealed that the Ag+ ions could not
induce the aggregation of AuNPs with the oligo-2.
To elucidate the phenomena of the Ag+-triggered LSPR light-
scattering spectra enhancement, the dispersion and aggregated
states of AuNPs induced by silver ions were studied using TEM
images. As displayed in Fig. 4, only a little aggregation of AuNPs
existed in AuNPs–oligo-1 (image a) and AuNPs–oligo-2
(image c) in the presence of NaNO3. However, when Ag+ was
added, a manifest aggregation was observed for AuNPs–oligo-1
Analyst, 2010, 135, 2682–2687 | 2683
Fig. 4 TEM images of the AuNPs–oligo-1 and AuNPs–oligo-2 with and
without Ag+. Experimental conditions: a) 0.78 nM AuNPs + 0.5 mM
oligo-1 + 0.02 M NaNO3; b) a + 0.5 mM Ag+; c) 0.78 nM AuNPs +
0.5 mM oligo-2 + 0.02 M NaNO3; d) c + 0.5 mM Ag+.
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(image b), while there was almost no change for AuNPs–oligo-2
(image d). This difference between AuNPs–oligo-1 and AuNPs–
oligo-2 induced by Ag+ was in quite good accordance with the
results of the LSPR light-scattering spectra, absorption spectra
and color change.
The addition of Ag+ induced different changes for AuNPs–
oligo-1 and AuNPs–oligo-2, when examined separately, which
might result from the different interaction between the oligonu-
cleotide and Ag+. The melting temperature (Tm) was used to
interpret the virtue of the interaction between the oligonucleotide
and Ag+. As shown in Fig. 5, the melting temperature of oligo-1
was about 21 �C, and it increased to 33 �C with the addition of
Ag+. However the addition of Ag+ had no effect on the melting
temperature of oligo-2; it remained at 21 �C with Ag+. This
difference was attributed to the different sequence of oligo-1 and
oligo-2. Oligo-1 is a self-complementary oligonucleotide except
that it has five cytosine–cytosine (C–C) mismatch-base pairs,
which can specifically bind with the Ag+ ions to form a C–Ag–C
Fig. 5 Melting curves of oligo-1 and oligo-2 without and with Ag+.
A ¼ [(At�C � A6�C)/(A60�C � A6�C)] at 260 nm,49 a) --- 3.0 mM oligo-1;
b) -C- 3.0 mM oligo-1 in the presence of 9.0 mM Ag+; c) -:- 3.0 mM
oligo-2; d) -+- 3.0 mM oligo-2 in the presence of 9.0 mM Ag+.
2684 | Analyst, 2010, 135, 2682–2687
base pair. So, with the help of Ag+ ions, the oligo-1 can overcome
the negative effect of the C–C mismatched base pairs, and form
a stable duplex structure.48,49
Optimization of the experimental conditions
The effect of pH on the LSPR light-scattering intensity was
studied within the range of pH 4.0–10.0 (Fig. 6). It was demon-
strated that the DI increased when the pH increased from 4.0 to
5.0, this could be attributed to two factors: firstly, the AuNPs
may aggregate in a strong acidic or alkaline medium; secondly,
the double helix structure of DNA is unstable at lower pH
environment. The DI reached a maximum when the solution
pH increased from 6.0 to 8.0. However the DI decreased when the
pH was changed from 8.0 to 10.0, this may be attributed to
the formation of silver hydroxide, which is unfavorable for the
formation of a C–Ag–C base pair, and further blocks the duplex
structure formation. Therefore, a pH 7.0 buffer was employed.
The enhancement of the LSPR light-scattering intensity was
mainly due to the aggregation of AuNPs, thereby the concen-
tration of AuNPs played a crucial role in the research. The effect
of the AuNPs concentration was studied within the range of
0.45–0.95 nM (Fig. 7). DI increased with the increase in the
concentration of AuNPs within the range of 0.45–0.75 nM, and
reached a plateau at a concentration range of 0.75–0.90 nM.
Therefore, a AuNPs concentraton of 0.78 nM was used for the
research.
The effect of oligo-1 concentration on the enhancement of the
LSPR light-scattering intensity was also investigated. In Fig. 8,
the DI increases with the increase of the concentration of oligo-1
within the range of 0.20–0.45 mM, and reaches a maximum and
remains at a plateau when the concentration of the oligo-1 is
higher than 0.45 mM. This suggests that the physisorption of
oligo-1 could protect the AuNPs from aggregation, and reaches
saturation when oligo-1 is higher than 0.45 mM, excessive oligo-1
does not further affect the DI. So 0.5 mM oligo-1 was used
throughout the research.
Naked AuNPs and ssDNA adsorbed AuNPs have different
abilities for NaNO3 resistance;20 whether the AuNPs aggregate
or not is controlled by the concentration of NaNO3. Fig. 9
demonstrates the effect of the concentration of NaNO3. DI
increases dramatically with the increase of the concentration of
Fig. 6 Effect of pH value on the enhancement of the LSPR light-scat-
tering intensity. AuNPs: 0.78 nM; oligo-1: 0.5 mM; Ag+: 0.5 mM; NaNO3:
0.02 M; absorbed time: 10.0 min; desorbed time: 5.0 min.
This journal is ª The Royal Society of Chemistry 2010
Fig. 7 Effect of the concentration of AuNPs on the enhancement of the
LSPR light-scattering intensity. Oligo-1: 0.5 mM; Ag+: 0.5 mM; NaNO3:
0.02 M; pH: 7.0; adsorption time: 10.0 min; desorption time: 5.0 min.
Fig. 8 Effect of the concentration of oligo-1 on the enhancement of the
LSPR light-scattering intensity. AuNPs: 0.78 nM; Ag+: 0.5 mM; NaNO3:
0.02 M; pH: 7.0; adsorption time: 10.0 min; desorption time: 5.0 min.
Fig. 9 Effect of the concentration of NaNO3 on the enhancement of the
LSPR light-scattering intensity. AuNPs: 0.78 nM; oligo-1: 0.5 mM; Ag+:
0.5 mM; pH: 7.0; adsorption time: 10 min; desorption time: 5 min.
Fig. 10 Effect of the adsorption and desorption time on the enhance-
ment of the LSPR light-scattering intensity. AuNPs: 0.78 nM; oligo-1:
0.5 mM; Ag+: 0.5 mM; NaNO3: 0.02 M.
Fig. 11 Selectivity of the assay for the determination of Ag+ ions.
DI ¼ IM�I0. The concentration of all the metal ions was 0.5 mM. AuNPs:
0.78 nM; oligo-1: 0.5 mM; oligo-2: 0.5 mM; NaNO3: 0.02 M; pH: 7.0.
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NaNO3 in the range of 0.005–0.015 M, and it reaches a plateau
when the concentration of NaNO3 varies within the range of
0.015–0.025 M. Excessive NaNO3 concentration induces the
decrease of DI. These results indicate that the AuNPs–oligo-1
could not aggregate completely when the NaNO3 was lower than
the threshold of 0.015 M in the presence of Ag+. But excessive
NaNO3 might lead to the aggregation of AuNPs–oligo-1 in the
absence of Ag+, which results in the decrease of DI at concen-
trations of NaNO3 higher than 0.025 M. Thereby 0.020 M
NaNO3 was applied in the research.
This journal is ª The Royal Society of Chemistry 2010
The LSPR light-scattering enhancement involves the adsorp-
tion of oligo-1 on the surface of AuNPs and the desorption from
it after the addition of Ag+; effects of the adsorption and
desorption time are shown in Fig. 10. The adsorption process
needs 10.0 min so that the enhancement of the LSPR light-
scattering intensity can balance and reach a plateau. After the
addition of Ag+, a duplex structure formed because of the specific
recognition of C–C mismatch between two oligo-1, so that the
oligo-1 desorbed from the surface of AuNPs. This desorption
process needs 5.0 min. Therefore, 10.0 min was used as the
adsorption time and 5.0 min was used as the desorption time.
Calibration curve and accuracy
Using the standard procedure, the relationship between enhanced
LSPR light-scattering intensity and the concentration of Ag+ ions
was investigated. The enhanced intensity was linear with the
concentration of Ag+ within the range of 0.13–1.12 mM, the
regression equation was DI¼ 344.32C + 8.64 (C: mmol L�1), with
a correlation coefficient of 0.9978. The limit of detection was
62.0 nM calculated with the formula CDL¼ 3d/S (where CDL is the
limit of detection, d represents the standard deviation, and S is the
slope of the calibration plot). The relative standard deviation was
1.46% for 1.0 mM Ag+. The linear equation for the colori-
metric method was A ¼ 0.142C + 0.026 (C: mmol L�1,
A¼A700/A520) over the concentration range of 1.29–8.0 mM, with
a correlation coefficient of 0.9912 and a detection limit of 0.87 mM.
Analyst, 2010, 135, 2682–2687 | 2685
Table 1 Results for the determination of of Ag+ in samples
Sample
Found by LSPRlight-scattering(n ¼ 6, mM)
RSD(%, n ¼ 6)
Added/mM
Recovery(%, n ¼ 6)
Found byICP-AES(n ¼ 4, mM)
t-test(t0.95, 5 ¼ 2.57)
Water sample 1 106.8 1.01 0.2 100.2 104.3 1.40Water sample 2 101.0 2.24 0.2 107.7 103.8 0.72Water sample 3 106.7 2.06 0.2 99.4 108.5 0.49Solder sample 1 11.4 5.17 0.2 100.4 11.3 0.01Solder sample 2 10.4 4.51 0.2 98.4 11.2 0.11
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Selectivity of the assay
In addition to sensitivity, we investigated the selectivity of the
assay by comparing the DI intensity in the presence of Ag+ and
other metal ions at a concentration of 5.0 mM. 12 different metal
ions (Cu2+, Co2+, Al3+, Ba2+, Co2+, K+, Zn2+, Ca2+, Cd2+, Fe2+,
Mg2+ and Ni2+) were chosen to study the ion selectivity. Under
the same conditions, only Ag+ showed significant LSPR light-
scattering enhancement (Fig. 11), which proved the high selec-
tivity of the specific binding of Ag+ with the C–C mismatched
base pair between two oligo-1 sequences.18
Determination of Ag+ in samples
Finally, we explored the possibility of using the assay for
detecting Ag+ in synthetic water samples and solder samples
(Table 1). The recovery of this method was 98.4–107.7%, the
determination results of five samples were in accordance with
that of the inductively coupled plasma-atomic emission spec-
troscopy (ICP-AES) method, the t-test showed no salience
difference between these two methods.
Conclusion
A novel localized surface plasmon resonance light-scattering
method for determining Ag+ with unmodified Au nanoparticles
was established. Single strand oligo-1 adsorbs on the surface of
AuNPs and protects them from aggregation with the addition of
NaNO3. Due to the specific binding property of Ag+ with C–C
mismatched base pairs, hybridization occurred with oligo-1, and
it formed a duplex structure with the addition of Ag+, and then
was desorbed from the surface of AuNPs as a result. This process
was accompanied by an enhancement of localized surface plas-
mon resonance light-scattering, a decrease of surface plasmon
absorption band at 520 nm and a color change change of the
solution from red to purple. Under the optimum conditions, the
enhanced intensity of localized surface plasmon resonance light-
scattering was proportional to the concentration of Ag+ ions in
the range of 0.13–1.12 mM, with a limit of detection of 62.0 nM.
Satisfactory results were obtained when the assay was applied to
the determination of Ag+ in the water samples and industrial
products.
Acknowledgements
This work was supported by the Natural Science Foundation of
China (No: 20975116) and SRF for ROCS, SEM.
2686 | Analyst, 2010, 135, 2682–2687
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