Peiyao
Lv
,
Ying
Cao
,
Zi
Liu
,
Rong
Wang
,
Baoxian
Ye
and
Gaiping
Li
*
College of Chemistry, Zhengzhou University, Zhengzhou, 450001, PR China. E-mail: lgpingzy@zzu.edu.cn; Fax: +86 0371 67763654; Tel: +86 0371 67781757
First published on 26th November 2019
In this work, we report a new fluorescence ratiometric method for Hg2+ assay based on the dual-ligand fluorescent probe GMP–Tb–luminol coordination polymers (CPs), which can be excited at the same wavelength and reveal characteristic luminescence of Tb3+ and luminol with spectrally distinguishable emission peaks. The addition of Hg2+ leads to the decrease of Tb3+ luminescence due to the higher coordination between Hg2+ and GMP, which inhibits energy transfer from GMP to Tb3+. Meanwhile, the fluorescence of luminol increases because of the aggregation-induced emission phenomenon. Therefore, a ratiometric fluorescent sensor for Hg2+ assay can be constructed by measuring the ratio of fluorescence intensity of luminol at 430 nm (I430) to that of Tb3+ at 548 nm (I548). Under the optimal conditions, the fluorescence intensity ratio I430/I548 exhibits a good linear relationship versus the concentration of Hg2+ in the range from 5 nM to 130 μM with a low detection limit of 1.3 nM. Additionally, the probe can also adsorb Hg2+ in water with high efficiency, which makes Hg2+ removal in water possible. The proposed method has been successfully used for the determination of Hg2+ in tap water, indicating its potential applications in the detection of Hg2+ pollution in environmental water.
Fluorescence is a desired technique for Hg2+ assay owing to its unique properties, such as multiparametric nature, high sensitivity, easy operation, rapid response, diversity of emerging novel probes, and so on.7–9 However, the sometimes complicated synthesis procedure, which is time consuming, and consumption of toxic organic reagents, as well as the poor water-solubility of the probes, have often hindered its practical applications.10–13 Recently, lanthanide coordination polymer (Ln-CP) based fluorescent sensors have gained increasing attention because of their appealing advantages, including excellent optical properties, facile preparation, tailorability of the structure and components, and the adaptive inclusion ability for enwrapping guest materials.14–17 Particularly, the lattermost is conveniently used for encapsulation of quantum dots or fluorescent dyes as an internal calibration to prepare dual-emission probes for ratiometric assay.18,19 These ratiometric sensors give response signals by self-calibration of two different emission intensities, and this can largely eliminate the fluctuations arising from the instrument and environment in the luminescence intensity measurement.20,21 Therefore, they can provide more accurate results than traditional turn-on or turn-off type sensors with the change in single-wavelength-intensity, and thus are more desirable for practical applications.
Although it is easy to incorporate fluorophores into Ln CPs through the self-assembly process to prepare dual-emission probes, the doped materials are often not covalently linked with the central metal ions, and this may lead to instability of the probe, particularly for long-duration or complicated sample measurements.22,23 Hence, the quest to prepare a stable Ln CP-based dual-emission probe for ratiometric assay is of significant importance. A convenient strategy is to introduce a suitable cofactor ligand with appropriate luminescence and coordination properties to construct a stable dual-emission probe, and luminol was recently proven to be a suitable candidate.24,25
In this work, we chose GMP and luminol as two bridging ligands to coordinate with Tb3+ to form GMP–Tb–luminol CPs through self-assembly, where GMP served as the antenna ligand to switch on the Tb3+ luminescence via energy transfer. Under single wavelength irradiation, the obtained GMP–Tb–luminol emitted characteristic fluorescence of luminol and Tb3+ with good separate peaks. In the presence of Hg2+, the fluorescence of Tb3+ was quenched, while that of luminol increased. This phenomenon makes ratiometric assay for Hg2+ feasible, and the possible sensing mechanism was speculated. Very interestingly, we found that the proposed probe could also efficiently remove Hg2+ from water simultaneously.
000 rpm, 5 min) and washed three times with ultrapure water. Then, GMP–Tb was re-dispersed in 1 mL HEPES buffer. GMP–Tb–luminol was prepared by adding luminol (10 mM, 10 μL) and stirring for 10 min. Finally, the obtained GMP–Tb–luminol mixture was stored at 4 °C prior to use.
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| Scheme 1 Schematic illustration of the principle of the fluorescence sensor for determination of Hg2+ using GMP–Tb–luminol. | ||
For the determination of Hg2+ in tap water, Hg2+ stock solution was spiked with tap water to prepare three samples with different concentrations of Hg2+, and the standard addition method was employed.
In a control experiment, GMP–Tb–luminol was separated by centrifugation and then washed three times with deionized water to remove non-coordinated luminol in the mixture. Then, it was re-dispersed by sonication in HEPES buffer (0.1 M, pH 7.4) to prepare sensor 2.
Luminol, an aromatic amine compound widely used in the chemiluminescence and electrochemiluminescence fields due to its unique luminescent properties, can also coordinate with lanthanide ions to form CPs.24,25,29–31 And more interestingly, the luminescence of luminol increased evidently after coordination with Tb3+ owing to the aggregation induced emission (AIE) phenomenon.24,25,32,33 As presented in Fig. S2,† the fluorescence of luminol increased with increasing the concentration of Tb3+, accompanied by a red shift of the emission peak from 420 nm to 430 nm. As shown in Fig. 1 (black line), when we added luminol to the GMP–Tb suspension, a new broad peak at 430 nm emerged as compared to that of GMP–Tb alone. Similarly, the depurated products obtained by centrifugation and washed three times with ultrapure water revealed the characteristic emission peaks of both luminol (430 nm) and Tb3+ (492, 548 and 590 nm) (Fig. 2, red curve). These phenomena indicated that luminol was converted into GMP–Tb readily as a cofactor ligand by coordination with Tb3+, and thus dual-ligand, dual-emission GMP–Tb–luminol CPs were obtained. The obtained GMP–Tb–luminol (Fig. 1B) showed a similar morphology to that of GMP–Tb (Fig. S1A†). The chemical compositions of GMP–Tb (Fig. S1C†) and GMP–Tb–luminol (Fig. 1C) were analyzed using an energy-dispersive X-ray (EDX) spectrometer. The peaks of C, H, O, N, P and Tb were observed in the spectra of GMP–Tb and GMP–Tb–luminol, which indicated that Tb3+, GMP and luminol were present in GMP–Tb–luminol. Furthermore, the formation of the GMP–Tb–luminol CPs was also confirmed by UV-vis and FT-IR characterizations (Fig. S3A and B†). All of these results demonstrated that dual ligand, dual emission GMP–Tb–luminol CPs were obtained.
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| Fig. 2 Fluorescence spectra (λex = 310 nm) of GMP–Tb–luminol (depurated) and GMP–Tb–luminol (depurated) + Hg2+ (40 μM) in HEPES buffer (0.1 M, pH 7.4). | ||
As proof of this mechanism, we compared the fluorescence spectra of the GMP–Tb–luminol mixture (sensor 1) and depurated GMP–Tb–luminol (sensor 2) in the presence of 40 μM Hg2+. It could be seen that Tb3+ emission in both cases decreased significantly upon exposure to Hg2+ (Fig. 1 and 2). However, the luminescence of luminol in the case of sensor 2 remains unchanged, which is different from that of sensor 1, since there is no residual free luminol in the solution. These results further confirmed the proposed mechanism as noted above about the fluorescence response of GMP–Tb–luminol towards Hg2+. By using the ratio of emission intensity of luminol at a wavelength of 430 nm (I430) to that of Tb3+ at 548 nm (I548) (I430/I548) as the response signal for construction of a ratiometric sensor for Hg2+, it is clear that sensor 1 exhibited better properties for signal amplification with higher sensitivity.
As stated above, the residual free luminol in sensor 1 is beneficial for response signal enhancement via the AIE phenomenon. With this in mind, the effect of luminol concentration on the response signal was investigated. As expected, the response signal I430/I548 became enlarged when we increased the concentration of luminol. The maximum was achieved with the concentration of luminol at 50 μM, and additional luminol was less efficient for response signal enhancement (Fig. S5, ESI†). Subsequently, we also tested the effect of irradiation wavelength on the response signal, as illustrated in Fig. S6 in the ESI.† By comparing the change of the response signal before and after addition of Hg2+, the optimal excitation wavelength was set to 310 nm.
The sensitivity of sensor 1 was demonstrated by detecting changes in the fluorescence intensity ratio I430/I548 upon addition of different concentrations of Hg2+. As presented in Fig. 3A, with increasing concentration of Hg2+, an increase in the emission intensity of luminol at 430 nm occurred, accompanied by a reduction of Tb3+ luminescence. A linear relationship is obtained by plotting the emission intensity ratio I430/I548versus the concentration of Hg2+ in the range from 5 nM to 130 μM. The linear equation is I430/I548 = 0.306C/μM + 0.0281 (R2 = 0.99, Fig. 3B), and the detection limit (LOD) was about 1.3 nM calculated using the equation LOD = 3σ/S, where σ and S are the standard deviation and the slope of the resulting linear relationship, respectively. The sensitivity is better than that of previously reported fluorescence ratiometric sensors.9,36 In a control experiment, we also tested the sensitivity of sensor 2 under the same conditions. As seen in Fig. S7A in the ESI,† Tb3+ emission in sensor 2 was sensitive to Hg2+ and decreased with increasing the concentration of Hg2+, while no fluorescence change was observed for luminol. The unchanged luminescence of luminol in sensor 2 served as an inert reference signal, and then a ratiometric senor was constructed. A linear correlation existed between the emission intensity ratio I430/I548 and the concentration of Hg2+ with a slope of 0.00585 in the range from 50 nM to 80 μM (Fig. S7B, ESI†). Compared with sensor 2, sensor 1 exhibits better performance with a steeper slope and wider linear range, further confirming that the residual luminol in sensor 1 is profitable for enhancing the sensitivity for ratiometric sensing of Hg2+.
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| Fig. 3 (A) Fluorescence spectra of GMP–Tb–luminol with different concentrations of Hg2+ (λex = 310 nm); (B) plot of the I430/I548 ratio versus the concentration of Hg2+. | ||
Subsequently, the selectivity of sensor 1 was evaluated by measuring its performance in the presence of other common metal ions under the same conditions. The results revealed that, with the exception of Cu2+, other metal ions (Na+, K+, Mg2+, Zn2+, Ba2+, Ca2+, Mn2+, Fe2+, Fe3+, Pb2+ and Bi3+) and biological species (Gly, Cys, His, Lys, Glu, Ala, AA and glucose) do not interfere with Hg2+ sensing (black bar in Fig. 4). The considerable interfering effect originating from Cu2+ can be explained by the Cu2+-caused aggregation of GMP–Tb–luminol CPs, which resulted in the dynamic quenching of the Tb3+ luminescence as previously reported.18 Fortunately, the interfering effect of Cu2+ can be eliminated using a masking agent, pyrophosphate (PPi), due to the strong affinity with Cu2+.37,38 Meanwhile, PPi itself shows a negligible influence on Hg2+ assay (Fig. S8, ESI†). Then, a competition experiment of Hg2+ in the presence of these metal ions was performed. As illustrated by the red bar in Fig. 4, the fluorescence intensity ratio I430/I548 is consistent with that when only Hg2+ was added. Therefore, it can be concluded that, with the help of PPi, a superior selectivity and anti-interference could be achieved even in the presence of Cu2+.
| Sample | C 0 | C | C 0 − C/C0 (%) |
|---|---|---|---|
| 1 | 5 nM | 0.085 nM | 98.3% |
| 2 | 10 μM | 0.05 μM | 99.5% |
| 3 | 130 μM | 1.17 μM | 99.1% |
| Sample | Hg2+ added (μM) | Hg2+ found (μM) | Recovery (%) | RSD (%) |
|---|---|---|---|---|
| Tap water | 0 | 0 | — | — |
| 0.005 | 0.0049 | 97.2 | 3.8 | |
| 10 | 10.7 | 107.2 | 1.6 | |
| 25 | 25.7 | 102.7 | 4.9 |
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ay02199j |
| This journal is © The Royal Society of Chemistry 2020 |