Ying
Cui‡
ab,
Shanji
Fan‡
c,
Yunran
Zhai
a,
Yingjie
Liu
c,
Junhua
Li
b,
Jiawen
Hu
*a and
Lijia
Wang
*d
aHunan Key Laboratory of Two-Dimensional Materials, Advanced Catalytic Engineering Research Center of the Ministry of Education, College of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, China. E-mail: jwhu@hnu.edu.cn
bKey Laboratory of Functional Metal-Organic Compounds of Hunan Province, College of Chemistry and Materials Science, Hengyang Normal University, Hengyang, 421001, PR China
cDepartment of Breast and Thyroid Surgery, The First Affiliated Hospital, Hengyang Medical School, University of South China, Hengyang 421000, China
dChildren's Hospital, Zhejiang University School of Medicine, National Clinical Research Center for Child Health, National Children's Regional Medical Center, Hangzhou, Zhejiang 310052, China. E-mail: wanglijia@zju.edu.cn
First published on 2nd April 2024
This study reports a metal-enhanced fluorescence chemodosimeter for highly sensitive detection of Hg2+ ions. Silica-coated Au nanoparticles (Au@SiO2 NPs) with a pinhole-free 4–5 nm shell were synthesized and functionalized with a monolayer of turn-on fluorescent probes. Compared to other organic fluorescent probes suffering from poor biocompatibility and detection limits, this design of a monolayer of turn-on fluorescent probes immobilized on the Au@SiO2 NPs with a pinhole-free 4–5 nm shell avoids fluorescence quenching and allows the fluorescent probe within the field of the inner Au NPs to experience metal-enhanced fluorescence. With this design, the chemodosimeter permits fluorescence emission in the presence of Hg2+ ions, because they trigger the ring-opening reaction of the fluorescent probe immobilized on the Au@SiO2 NPs. Additionally, the fluorescent probe is distanced by the thin SiO2 shell from directly attaching to the metallic Au NPs, which not only avoids fluorescence quenching but allows the fluorescent probe within the long-ranged field of the inner Au NPs to experience metal-enhanced fluorescence. As a result, the detection limit for the chemodosimeter can reach up to 5.0 × 10−11 M, nearly two orders of magnitude higher than that achieved for the free fluorescent probe. We also demonstrate the acquisition of images of Hg2+ in HTC116 cells and zebrafish using a simple fluorescence confocal imaging technique. The fluorescence response results for HTC116 cells and zebrafish show that the probes can permeate into cells and organisms. Considering the availability of the many organic fluorescent probes that have been designed, the current designed metal-enhanced fluorescence chemodosimeter holds great potential for fluorescence detection of diverse species and fluorescence imaging.
In recent years, fluorescence-based colorimetric chemodosimeters for the detection of Hg2+ ions have attracted increasing attention because of their high selectivity, sensitivity, irreversible binding ability, mild reaction conditions (e.g., room temperature), and water solubility.14,15 In 1992, Chae et al. first introduced the term chemodosimeter, which refers to an abiotic molecule that recognizes the analyte and at the same time irreversibly transduces an observable signal.16 Generally, mechanisms for chemodosimeters can be divided into two main modes: the analyte can react with the chemodosimeter or act as a catalyst.17 For example, one fluorescence chemodosimeter relies on the binding of Hg2+ for the desulfurization of a thioamide to amide to produce fluorescence signals.18–20
Because the fluorescence intensity determines the sensitivity of a fluorescent probe, metal-enhanced fluorescence (MEF) has been widely used to enhance the intensity of the fluorescence.21,22 Surface plasmon resonance is the light-induced of collective oscillation of free electrons in a metal, and thus generates a very strong electromagnetic field that can improve the fluorescence intensity.23,24 This phenomenon is called metal-enhanced fluorescence (MEF) and has been reported for various organic fluorophores25,26 and quantum dots27,28 in proximity to gold or silver substrates or other metal nanostructures. It has also been found that metal nanoparticles (NPs) can affect fluorescence intensity. This effect mostly depends on the distance between the metal nanostructures and fluorophores; too-great proximity results in quenching, while separation by several nanometers produces enhancement.29 However, when the distance is too large, the fluorophore will be far from the magnetic field generated by the plasma resonance of the metal nanoparticles, and the fluorescence intensity of the fluorophore will not be affected. Therefore, optimization of fluorophore-metal NP distance is critical for fluorescence enhancement.30 To date, a great deal of work has been performed using metal NPs deposited on glass,31 plastics,32,33 paper34 or other non-metallic plate substrate surfaces via self-assembly,35 to study the MEF effect on photoluminescent materials. Therefore, it is desirable to fabricate uniform and disperse nanocomposite systems to realize the MEF effect in biological,36 nanophase electronic,37 single nanoparticle sensing38,39 and fluorescence imaging.40
Fluorescent chemosensors for Hg2+ have been extensively explored, including cyclen,41 hydroxyquinoline,42 azine,43,44 diazatetrathia crown ethers36 and calixarene.45 However, many of these sensors suffer from limitations in terms of synthetic difficulty, high cost of starting materials, high detection limits or lack of selectivity towards potential competitors such as copper (Cu2+) and silver (Ag+) due to the similarity of their chemical behavior to that of Hg2+.46 In addition, two different modes, namely, the “turn-off” mode47 and “turn-on” mode,48 have been proposed for optical sensors based on fluorescence. Most of the reported fluorescent sensors have been based on the “turn-off” mode, in which false positive results occur due to other quenchers in real samples.49 Compared to the traditional “turn-off” mode, the latter approach based on the “turn-on” fluorescence change (quenching recovery) can not only expand the detection range but also increase stability and reduce environmental interferences.50
In this study, we developed a facile, highly sensitive and selective chemodosimeter for the detection of Hg2+ ions based on MEF. This was accomplished by immobilizing a fluorescent probe on ultrathin SiO2-shell-coated Au NPs51 (Au@SiO2 NPs, where the diameter of the SiO2 shell was 4–5 nm). With this core–shell type configuration, the plasmon of the inner Au NPs produces long-range electromagnetic fields to enhance the fluorescence emission. Additionally, the ultrathin SiO2 shell can avoid fluorescence quenching through separating the fluorophore probe from the metal. Furthermore, the fluorescence can be further enhanced via optimizing the core size. To demonstrate the feasibility of the MEF-based fluorescence platform, we demonstrated its application for the detection of Hg2+ ions. The optimized detection limit achieved was 5.0 × 10−11 M, which was about two orders of magnitude lower than that achieved using the free fluorescent probe (8.5 × 10−9 M) and far lower than the permissible EPA limit for Hg2+ ions in drinkable water (<1.0 × 10−9 M). Additionally, this MEF-based fluorescence platform has high selectivity for Hg2+ over other metal ions. The proposed strategy opens new avenues to fabricate a sustainable chemodosimeter that affords superior performance in the detection of Hg2+ in real environments, such as food samples and even whole cells.
Scheme 1 Schematic illustration of the preparation flow for the fluorophore-labeled Au@SiO2 NP probe and its detection mechanism for Hg2+ ions. |
Silica coating was performed according to the method established by Li et al.51 By carefully controlling reaction parameters such as pH, reaction time, temperature, and the amount of silica source, this method allows coating of the Au NPs with a controlled-thickness SiO2 shell. Fig. 1 shows the TEM images of the 80 nm Au NPs (a) and the corresponding Au@SiO2 NPs with a 4–5 nm SiO2 shell (b). Upon silica coating, a thin and uniform SiO2 shell of ∼4–5 nm is clearly seen coating each isolated Au NP. Moreover, the Au NPs supported on the GC electrode show typical electrochemical responses of a polycrystalline Au surface (Fig. 1c), with a wide Au oxide peak initiating at about 1.2 V and a corresponding stripping peak for the Au oxide at 0.9 V. On the contrary, the thin SiO2 shell completely restrains the formation of the Au oxide peak during the cationic scan and accordingly strips the peak of the Au oxide in the cyclic voltammetry (CV) curve of the Au@SiO2 NPs (Fig. 1c). Therefore, the SiO2 shell coating is “pinhole-free”, as further confirmed by the lack of any discernable SERS peaks for pyridine molecules when immersing the Au@SiO2 NPs in pyridine solution (for details, see Fig. 1d). The naked pure Au NPs show strong SERS peaks because of their easily available surface, which allows the adsorption of the pyridine molecules to experience SERS enhancement. In contrast, the Au@SiO2 NPs do not show any SERS peaks from pyridine, because the SiO2 shell effectively blocks the pyridine molecules from approaching and adsorbing on the inner Au NPs. This “pinhole-free” SiO2 shell can thus effectively separate the fluorophore from direct contact with the Au metal underneath, thereby avoiding fluorescence quenching. Conversely, the SiO2 shell is very thin, so that the field created by the Au NPs underneath can sufficiently penetrate the shell and enhance the fluorescence of the fluorophore immobilized therein. Moreover, a comparison material, 50 nm Au NPs, and the corresponding Au55 nm@SiO2 NPs were synthesized (for details, see ESI, Fig. S1 and S2†).
Fig. 2a shows the UV-vis spectrum of the free fluorescent molecule, which exhibits a strong adsorption peak with a maximum wavelength (λmax) of 563 nm. Upon the addition of Hg2+ ions, the λmax red-shifts to 570 nm. At the same time, as shown in the corresponding fluorescence spectrum in Fig. 2b, the fluorescence intensity of the free fluorescent probe was enhanced after the addition of Hg2+, indicating that the ring-opening reaction occurred in the fluorescent molecule. Interestingly, the fluorescence intensity was dramatically enhanced when Hg2+ was added to the solution of the probe-labeled-Au@SiO2, which is because the excitation region of the probe is consistent with the plasmon of Au@SiO2 (Fig. 2b). The enhancement factor therefore results from the mercury-induced ring-opening reaction. More importantly, MEF, as a leading effect, causes a significant fluorescence enhancement. Because of the much wider resonance, the enhancement effect of the probe-labeled Au@SiO2 NPs is more remarkable than that of the free fluorescent probe. A comparison was made using 55 nm gold NPs, and it was found that the 80 nm NPs have better MEF performance (for details, see ESI, Fig. S3†). The time profile of the fluorescence response of the probes (0.5 μM) in the presence of Hg2+ (1.0 equiv.) in pH 7.4 PBS buffer is displayed in Fig. S4,† showing that the response of probes to sulfite was very quick. In addition, to study the stability of the probes at different pH values, the fluorescence spectra of the response of the probes toward Hg2+ under different pH conditions were evaluated (Fig. S5, see ESI†). These results clearly show that this probe can be used in a broad pH range of 6.0–9.0. This result shows that the probes can be applied to biological systems.
Fig. 3a and b show the fluorescence spectrum of the free fluorescent probe and fluorophore-labeled Au@SiO2 probe, respectively, in the presence of different amounts of Hg2+ ions. For reliable comparison, the number of fluorescent probes immobilized on the Au@SiO2 NPs was adjusted to the same amount (all achieved 0.5 μM). After that, Hg2+ ions were introduced with increasing molar ratio to the probe-labeled Au@SiO2 NP solutions. With increasing amount of Hg2+ ions, the intensity of the fluorescence initially quickly increased. The fluorescence intensities then became saturated at a molar ratio of 1.8 for the probe-labeled Au@SiO2 NPs and 1.4 for the free fluorescent probe, as shown in Fig. 3b and d, because the mercury-induced ring-opening reactions reached equilibrium. The addition of Hg2+ to the probe-labeled Au@SiO2 solutions causes strong yellow fluorescence, as shown in the inset of Fig. 3c. Consistent with its large fluorescence enhancement ability (Fig. 3a and c), the fluorescence enhancement achieved on the Au@SiO2 probe is more prominent than that achieved for the free fluorescent probes. The number of fluorescent molecules immobilized on the surface of the Au@SiO2 NPs can be estimated, as described in the ESI Fig. S6† section;52 the fluorescence enhancement achieved on the Au@SiO2 NPs was 8.2-fold. With this core–shell type configuration, the fluorescence enhancement arises because the plasmon of the inner Au NPs is resonant with maximum UV-vis absorption peaks for the fluorescent probe. This large fluorescence enhancement makes the Au@SiO2 NPs very attractive for the practical detection of Hg2+ ions, which relies on fluorescence as the signaling pathway. The plots shown in Fig. 3b and d reveal that the fluorescence intensities changed as a function of the Hg2+ concentration, and the insets show the linear plot ranges of fluorescence intensity versus Hg2+ ionic concentration that were extracted from Fig. 3b and d. For the free fluorescent probe (Fig. 3b), the detection limit achieved is 8.5 × 10−9 M, while that achieved for the Au@SiO2 NPs is 5.0 × 10−11 M. The capability of our MEF probe to detect Hg2+ was comparable to that of other materials (Table 1). Apparently, owing to the large fluorescence enhancement, the fluorophore-labeled Au@SiO2 probes show much improved sensitivity toward Hg2+ ions. To study the stability of the probe RS (Rhodamine spirocyclic type fluorescent molecular probe) at different pH values, the fluorescence spectra of the RS response toward Hg2+ under different pH conditions were evaluated (Fig. S5, see ESI†). These results clearly show that this probe can be used in a broad range pH of 6.0–9.0.
Material | LOD/mol L−1 | Year | Ref. |
---|---|---|---|
SBA-15 | 0.6 × 10−6 | 2008 | 53 |
NaYF4:Yb3+ | 0.6 × 10−10 | 2010 | 54 |
CdTe QDs | 0.7 × 10−7 | 2012 | 55 |
Rhodamine derivative | 2.9 × 10−8 | 2013 | 56 |
Au NP | 5.0 × 10−9 | 2016 | 57 |
Aptamer-Ag@SiO2 | 3.3 × 10−10 | 2015 | 58 |
Unsymmetrical quinoline type tolans | 2.0 × 10−10 | 2016 | 59 |
G-quadruplex DNA | 1.3 × 10−10 | 2017 | 60 |
Au/N-CQDs | 1.2 × 10−5 | 2018 | 61 |
Ag@SiO2 NPs | 2.0 × 10−19 | 2022 | 62 |
Au@SiO2-probe | 5.0 × 10−11 | Now | This work |
To further reveal their resistance against interferent ions, Fig. 4a and b shows fluorescence spectra for the Au@SiO2 probes in the presence of other metal ions, namely, Co2+, Fe3+, Cd2+, Fe2+, K+, Cr2+, Cu2+, Pb2+, Mg2+, Ag+, Ba2+, and Ni2+ ions. Clearly, only the presence of Hg2+ ions can trigger the high fluorescence intensity of the probe, thereby indicating the excellent selectivity of the Au@SiO2 fluorescent probes. In addition, we further examined the fluorescence response of the probe toward Hg2+ ions in the presence of other potentially competing species. These other species only displayed minimum interference (Fig. S7†). This suggests that the Au@SiO2 probe is potentially useful for sensing Hg2+ ions in the presence of other related species in pH 7.4 PBS buffer.
Because of the desirable sensitivity and selectivity of this fluorophore-labeled Au@SiO2 probe toward Hg2+ ions, it shows potential application in real water sample analysis. For demonstration, the proposed fluorescent probe was applied to detect Hg2+ ions in many different kinds of water collected from local places (Xiangjiang River, Peach Lake, and Yuelu Mountain Spring, in Changsha, China). The fluorescence intensity of the solutions was recorded after adding the fluorophore-labeled Au@SiO2 and a spiking concentration of Hg2+ ions to the water samples. To prove the reliability of our sensor, the same detection was carried out using ICP (inductive coupled plasma emission spectrometry), and the results are summarized in Table 2. The results of the two methods show good agreement between expected and found values, which proved that the Au@SiO2 NP fluorescent probes exhibit satisfactory performances in real environmental water samples.
Sample | Added (equiv.) | Measured | ICP (mol L−1) |
---|---|---|---|
a N = no Hg2+ was detected. | |||
River water | 0 | N | N |
1.00 | 1.13 | 5.27 × 10−7 | |
1.60 | 1.75 | 8.18 × 10−7 | |
Lake water | 0 | N | N |
1.00 | 1.32 | 5.41 × 10−7 | |
1.60 | 1.94 | 8.33 × 10−7 | |
Spring water | 0 | N | N |
1.00 | 0.92 | 4.66 × 10−7 | |
1.60 | 1.43 | 7.72 × 10−7 |
To demonstrate the potential use of the probe and Au@SiO2 probe in bioimaging applications, we tested the cytotoxicity of the Au@SiO2 probe toward HCT116 colorectal cancer cells using the reduction activity of the methylthiazolyltetrazolium (MTT) assay (Fig. S8, see ESI†). The viability of untreated cells was assumed to be 100%. Upon the incubation with 0.5 μM of the probe or Au@SiO2 probe for 24 h, no significant difference in the proliferation of the cells was observed. Specifically, a cell viability of about 80% was observed after 24 h even at a high-dose concentration of 1.8 equiv. Hg2+. These data indicated the satisfactory biocompatibility of the Hg2+ fluorescent probe at all dosages, enabling the probe and Au@SiO2 probe to serve as a potential probe for fluorescence bioimaging.
To extend the application of the probes to more complex metrics, we examined the imaging characteristics of the probes in cultured living cells in vitro (HCT116, human colorectal cancer cells) using fluorescence microscopy (Fig. 5). The cells were incubated with 0.5 μM of the probe and Au@SiO2 probe for 1 h and 6 h at 37 °C, respectively. The cells were then washed with PBS three times and mounted on a microscope stage. As shown in Fig. 5a, the cells display modest intracellular staining after incubation with the probe and subsequent addition of 1.8 equiv. Hg2+. Upon incubation for 1 h, striking turn-on fluorescence is observed inside the HCT116 cells, indicating the formation of the probe + Hg2+ complex, which was in agreement with studies performed in solution. Under same conditions, the Au@SiO2 probe (0.5 μM) was incubated for 6 h and 1.8 equiv. Hg2+ was added and incubated for 1 h, and a notable enhancement was observed (Fig. 5b). In contrast, the Au@SiO2 probe produces a stronger fluorescence imaging effect than the free probe. The fluorescence microscopy analysis strongly suggested that the Au@SiO2 probe could cross the membrane barrier, permeate into the HCT116 cells, and rapidly sense intracellular Hg2+. It is significant to mention that bright field imaging of treated cells did not reveal any gross morphological perturbations, which suggested that the HCT116 cells were viable. These preliminary experimental results demonstrated that the Au@SiO2 probe could be applied for the fluorescence imaging of Hg2+ in biological samples with high resolution.
Whole-organism experiments were also carried out to examine whether the probe could be used to image Hg2+ in living organisms. A 3 day-old zebrafish was incubated with 1 μM of probe and Au@SiO2 probe in E3 embryo media for 4 h and 24 h at 28 °C and later incubated in a solution containing 1.8 equiv. Hg2+ for 2 h. Subsequently, the samples were washed with PBS to remove remaining probes. The treated zebrafish is shown in Fig. 6. The zebrafish remained alive throughout imaging experiments. The results of fluorescence microscopy analysis of these specimens showed that Hg2+ in the zebrafish was fluorescently detected by the probes (Table 1). In this case, the Au@SiO2 probe has stronger fluorescence intensity than the free probe. These results indicate that the probes are useful for the study of the toxicity or bioactivity of Hg2+ in living organisms.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3na00746d |
‡ Co-first authors. |
This journal is © The Royal Society of Chemistry 2024 |