Open Access Article
Jin Jia‡
acd,
Gui-Juan Cheng‡b,
Aihua Wu
*c and
Shengji Luana
aCollege of Environmental Science and Engineering, Peking University, Beijing 100871, China
bKey Laboratory of Computational Chemistry and Drug Design, College of School of Chemical Biology and Biotechnology, Peking University Shenzhen Graduate School, Shenzhen 518055, China
cKey Laboratory of Environment Simulation and Pollution Control, PKU-HKUST Shenzhen-Hongkong Institution, Shenzhen 518057, China. E-mail: phenix_wah@aliyun.com
dShenzhen Graduate School of Harbin Institute of Technology, Shenzhen 518055, China
First published on 20th July 2017
Novel ion imprinted nano-fluorescent probes (IIP–fluorescein) based on polyethyleneimine (PEI) were obtained via simple imprinting and grafting with fluorescein, and used for high recognition, detection and adsorption of Cu2+, Zn2+ and Cr3+ in aqueous solution. The selectivity of PEI is adjustable through an imprinting process for Cu2+, Zn2+or Cr3+, which have a strong affinity for the amino group. Each probe reveals specific selectivity to and recognition of the relevant template metal ion over seven other common metal ions. The three probes exhibit a large linear detection range, high accuracy and strong adsorption capacity for Cu2+, Zn2+ and Cr3+. The sensitive and selective detection, as well as the removal of Cu2+, Zn2+ and Cr3+ by using IIP–fluorescein was further demonstrated in polluted tap and river water, indicating their potential application in environmental monitoring and treatment. Additionally, the sensing mechanism of IIP–fluorescein for metal ions was investigated through Gaussian 09. The synergistic effect of photo-induced electron transfer (PET) and intramolecular charge transfer (ICT) was demonstrated in the sensing process for metal ions. The design concept might propose a method for developing and studying other fluorescent probes with similar systems (containing amino groups, mercapto groups or cyano groups).
Up to now, extensive research has been conducted on fluorescent probes with aminoquinoline,8 porphyrin,9 coumarin,10 rhodamine derivatives11 and polycyclic aromatic hydrocarbon,12 etc. However, most of those small-molecule fluorescent probes display the disadvantage of anti-jamming, stability, reusability and causing secondary pollution. To overcome these weaknesses, researchers made great efforts to develop various novel probes and methods, including quantum dots,13–15 biosensors16–18 and nano-fluorescent probes.19–21 The nano-fluorescent probes are extremely attractive and arouse the interest of researchers. It shows more stable, easy recovery and higher sensitivity due to the huge surface area per unit mass (S/M ratio).22,23 The nano-fluorescent probes could be easily designed by various receptor and fluorophore. However the reversal design of fluorescent probes according to different target metal ions is still a big problem. Thus it is very necessary but also challenging to develop method for fabricating probes and sensing target metal ions.
Ion imprinting could be a promising solution to that problem since its controllable selectivity. The ion imprinted polymer (IIP) can be conveniently synthesized according to the target metal ions, and shows advantage of anti-interference and stability.24–26 Recently, many studies focus on the applications of fluorescent probes grafting with IIP.27–29 However, little attempt was done on selectivity control mechanism.
Polyethyleneimine (PEI) is a cationic polymer with large amount of amine groups. Thus, it can form chelation complexes with heavy metal ions possessing good hydrophilicity, high adsorption capacity and rapid chelating rate.30–32 In our previous work, PEI revealed strong affinity towards Cu2+, Zn2+, Cr3+, and also showed great potential of specific selectivity.33 To further investigate the control mechanism of selectivity, ion imprinted nano-fluorescent probes based on PEI were achieved via simple imprinting by Cu2+, Zn2+ or Cr3+ and grafting with fluorescein. The selectivity could be further enhanced and specialized by imprinting effect and fluorescence signal transmission. The probe imprinted by Cu2+, Zn2+ or Cr3+ respectively reveals specific selectivity and recognition to the relevant template metal ion over seven other common metal ions. Additionally, the sensing mechanism for metal ions was investigated through Frontier molecular orbital and electron density distribution. The novel probes were applied as sensor and absorbent for metal ions in aqueous solution. The three probes exhibit large linear detection range, high accuracy and strong adsorption capacity for Cu2+, Zn2+ and Cr3+. The sensitive and selective detection, as well as the removal of Cu2+, Zn2+ and Cr3+ by using IIP–fluorescein was further demonstrated in polluted tap and river water, indicating their potential application in environmental monitoring and treatment. The design concept might propose a method for developing and studying other fluorescent probes with similar systems.
Fluorescence spectrum was recorded using Hitachi fluorescence spectrophotometer (F-4600). Flame atomic absorption spectrophotometer (FAAS) was purchased from Thermo (Solaar-S4). Scanning electron microscope (SEM) was from Phenom (Pro). Fourier transform infrared spectrometer (FTIR) was from Thermo (Nicolet IS50). Laser particle size analyzer was form Malvern (Nano ZS90). Filtering centrifuge tube from Millipore (50 mL, MWCO 3k) and dialysis tube from Yuanye Bio-Technology Corporation (MWCO 8000–14
000, 100k) were utilized in this study.
The nano-fluorescent probes were prepared by grafting fluorescein onto surface of IIP. 0.166 g fluorescein was dissolved in 50 mL DMF, following by adding of HOBT, HBTU and DIEA (mole ratio of 1
:
1
:
2) with stirring for 3 h. Then the solution was mixed with previously obtained IIP with stirring at room temperature. After standing for 12 h, the mixed solution was extracted by diethyl ether and washed repeatedly with ethyl acetate. To remove unreacted fluorescein, the products were dialyzed (MWCO 8000–14
000) with ethanol/water solution and confirmed by fluorescence spectrophotometer, then dialyzed with distilled water for 3 days. Finally, IIP grafted fluorescein nano-fluorescent probes (M–IIP–fluorescein) were obtained and stored at 4 °C for future usage.
To characterize chemical composition of fluorescent probes, infrared spectra of PEI, Cu–IIP, fluorescein and Cu–IIP–fluorescein are performed (Fig. S1†). The characteristic peaks of PEI (NH4+ at 2948 cm−1 and 2840 cm−1), IIP (C–O at 1033 cm−1) and fluorescein (phenols C–O at 1213 cm−1) appearing in M–IIP–fluorescein demonstrate that fluorescein has been successfully grafted onto surface of M–IIP.
:
1
:
1). All the calculations were carried out with the Gaussian 09 package.34 The ground state structures were optimized using density functional theory (DFT) with the M06 hybrid functional. The LANL2DZ basis set with ECP was used for metal atoms and the 6-31G(d) basis set was used for other atoms. Frequency analysis was conducted at the same level of theory to verify the stationary points to be real minima and to obtain the thermodynamic energy corrections. Single point energies were calculated at the M06/SDD-6-311++G (d, p) level in water by using the SMD solvation model. The excited state related calculations were performed with the time dependent DFT (TD-DFT) at the M06/SDD-6-311++G (d, p) level in water with the optimized structure of the ground state. The energies are presented in kcal mol−1.
The specific sensing mechanism was demonstrated with Frontier molecular orbital and electron density distribution by Gaussian 09. The Frontier molecular orbital distributions and energy of Cu–IIP–fluorescein were presented in Fig. S4.† The orbital energy of IIP (HOMO−1) is lower than fluorescein (HOMO and LUMO) when absence of copper ions, which means PET process will not occur. When Cu–IIP–fluorescein coordinates with copper ions, two types of electron transition (α electron and β electron) will exist due to an unpaired electron in copper ions (II). The orbital and energy distributions of α electron are similar with absence of copper ions. On the contrary, LUMO lies on IIP for β electron. The transition type on fluorescein is HOMO → LUMO+1. This means orbital energy of IIP lies between transition energy of fluorescein. Therefore the PET process from fluorescein (LUMO+1) to IIP (LUMO) will occur.
To further verify the PET process, we calculated the vertical excitation results of Cu–IIP–fluorescein in Table 1. The evaluation of the electronic excited states and the photophysical properties of the probes are based on the selection rule for electronic transitions.35–37 The parameter to evaluate the possibility of a transition is the oscillator strength (f). Usually transitions with f > 0.01 are allowed; conversely, a small f < 0.01 infers a forbidden transition. The same rules are applicable to the emission processes.38,39 In absence of copper ions, the value of f (0.4023) indicates effective transition and fluorescence emission. After coordinating with copper ions, the transition is mainly composed by β electron transition, however, the small f (0.0014) reveals fluorescence quenching by PET process.
| Molecule | Electronic transitiona | Energy (eV) | fb | Compositionc | CId |
|---|---|---|---|---|---|
| a Only S1 excited states were considered.b Oscillator strength.c H stands for HOMO and L stands for LUMO. Only the main configurations are presented (CI coefficients >0.1).d CI coefficients are in absolute values. | |||||
| Cu–IIP–fluorescein | S0 → S1 | 2.9391 | 0.4023 | H → L | 0.67601 |
| H−2 → L | 0.10973 | ||||
| Cu–IIP–fluorescein with Cu2+ | S0 → S1 | 0.8598 | 0.0014 | Hbeta−2 → Lbeta | 0.79224 |
| Hbeta−20 → Lbeta | 0.41887 | ||||
To investigate and interpret the ICT process, the electron density distribution of probes was calculated and presented in Fig. S5.† The carbonyl on the fluorescein is electron-acceptor with electron density of −0.13 e. After grafting with IIP, the electron density distribution of probe is more homogeneous due to the electron donating effect and conjugation effect of IIP. The electron negativity of carbonyl is decreased with electron density of −0.118 e. In the meanwhile, the conjugation effect leads to decrease of probe dipole moment, followed by declining of energy gaps between excited state and ground state. As the result, the red shift of fluorescence emission spectrum can be observed. Afterwards, coordination with metal ions will reduce electron donating ability of IIP, as well as the conjugation extent. The electron negativity of carbonyl returned with electron density of −0.14 e. Moreover, the energy gap between HOMO and LUMO is usually proportional to conjugation extent of molecule.40 The energy gap of Cu–IIP–fluorescein is −0.1328 a.u.; after coordinating with copper ions, the energy gap are −0.1293 a.u. (α electron) and −0.1142 a.u. (β electron), which are both declined. On the basis of these results, we conclude that the PET and ICT function together in sensing process of IIP–fluorescein nano probes.
The fluorescence quantum yields of probes were calculated as eqn (1). Fluorescein was chosen as standard substance with fluorescence quantum yield of 95% (in 0.1 M NaOH solution). The results for Cu–IIP–fluorescein, Zn–IIP–fluorescein, Cr–IIP–fluorescein and NIP–fluorescein were 0.861, 0.801, 0.820 and 0.745, respectively. The slight decrease of quantum yields comparing with fluorescein is due to the absorbance of IIP or NIP cannot transform into fluorescence radiation. The quantum yields of M–IIP–fluorescein are overall higher than NIP–fluorescein. It reveals the imprinting effect of metal ions, which increase regularity and rigidity of the molecular chain. The results demonstrate probes still have extremely high fluorescence quantum yields and might be applicable in high sensitive detection of metal ions. The details of absorbance and fluorescent peak area are given in Table S2 in the ESI.†
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| Fig. 3 Emission spectrum of IIP–fluorescein coordinating with each metal ion. (A) Cu–IIP–fluorescein, (B) Zn–IIP–fluorescein and (C) Cr–IIP–fluorescein. | ||
To further check the selectivity and resistance to interference by other metal ions, competition experiments were conducted in the presence of 1 equiv. of each interfering ion, with the subsequent addition of 1 equiv. of template metal ion. As shown in Fig. 4, the emission profile of the Cu–IIP–fluorescein/Cu2+, Zn–IIP–fluorescein/Zn2+ and Cr–IIP–fluorescein/Cr3+ complex are all unperturbed in the presence of these interfering ions, indicating the strongest affinity and selectivity for template metal ion. A reasonable explanation would be that the structure and dimension of imprinted sites in IIP only fit for template metal ion. The selectivities of three probes are independent and show specific affinity to each template metal ion. Thus the controllable selectivity of PEI fluorescent probe could be achieved, which promotes applications in recognition and extraction of certain target metal ions.
According to the above standard procedures and under the optimized assay conditions, different concentrations of Cu2+, Zn2+ or Cr3+ were added to the buffer and fluorescence emission intensity was measured to evaluate the sensitivity of the probes. As shown in Fig. 5, fluorescence emission intensity decreased gradually with the increase of template ion concentration. For further increasing of metal ions, the fluorescence quenching rates gradually stabilized and fluorescence intensity retained 21.5%, 27.0% and 24.9% for Cu–IIP–fluorescein, Zn–IIP–fluorescein, Cr–IIP–fluorescein, respectively. The decrement fluorescence emission intensity was found to be linear with the concentration of Cu2+, Zn2+ or Cr3+in the range of 6.65 × 10−6–1.17 × 10−2 g L−1, 9.17 × 10−6–8.03 × 10−3 g L−1 and 8.39 × 10−6–1.02 × 10−2 g L−1. According to the standard deviation for the blank signal with 15 parallel measurements, limits of detection of 1.99 × 10−6 g L−1, 3.67 × 10−6 g L−1, 2.75 × 10−6 g L−1 for Cu2+, Zn2+ and Cr3+ were estimated by 3 times the standard deviation rule. The World Health Organization (WHO) regulate the maximum allowable levels of Cu2+, Zn2+ and Cr3+ in drinking water to be 1.0 × 10−3 g L−1, 1.0 × 10−3 g L−1 and 5 × 10−5 g L−1, respectively. The nano-fluorescent probes present the wide linearity range in detection. Moreover, the limit of detection is appropriate to monitor the metal ions changes in natural water or contaminated water.
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| Fig. 5 Fluorescence spectra and titration curves of the nano-fluorescent probes to template metal ions. (A) Cu–IIP–fluorescein. (B) Zn–IIP–fluorescein and (C) Cr–IIP–fluorescein. | ||
000 rpm. The samples spiked with different concentrations of metal ions were detected according to the general procedure with three replicates. The results were summarized in Table 2 and showed good agreement with the values determined by FAAS. The mean deviation of fluorescent probes and FAAS comparing with truth value are 1.52% and 1.71%, respectively. It is also notable that both methods prove precise selectivity for target ion in the metal mixture. The results reveal the present probes could be excellently applied in environmental detection.
| Sample | Addeda | Cu2+ (mg L−1) | Zn2+ (mg L−1) | Cr3+ (mg L−1) | |||
|---|---|---|---|---|---|---|---|
| Cu–IIP–fluorescein (meanb ± SDc) | FAAS (mean ± SD) | Zn–IIP–fluorescein (mean ± SD) | FAAS (mean ± SD) | Cr–IIP–fluorescein (mean ± SD) | FAAS (mean ± SD) | ||
| a Add of single template ion (Cu2+, Zn2+ or Cr3+) to tap water and river water, add of multi metal ions (Cu2+, Zn2+, Cr3+, Ni2+, Co2+, Pb2+, Cd2+ and Ag+) to distilled water.b Mean of three determinations.c SD = standard deviation. — no concentration could be detected. | |||||||
| Tap water 1 | 0 | — | — | — | — | — | — |
| Tap water 2 | 0.1 | 0.102 ± 0.003 | 0.105 ± 0.002 | 0.114 ± 0.004 | 0.111 ± 0.007 | 0.105 ± 0.006 | 0.103 ± 0.012 |
| Tap water 3 | 1 | 1.014 ± 0.013 | 1.008 ± 0.021 | 1.013 ± 0.031 | 0.997 ± 0.016 | 1.019 ± 0.015 | 1.022 ± 0.033 |
| Tap water 4 | 5 | 5.062 ± 0.023 | 5.058 ± 0.041 | 5.019 ± 0.016 | 5.005 ± 0.031 | 4.982 ± 0.034 | 5.011 ± 0.052 |
| River water 1 | 0 | 0.002 ± 0.000 | 0.002 ± 0.001 | 0.003 ± 0.001 | 0.002 ± 0.001 | — | — |
| River water 2 | 0.1 | 0.106 ± 0.004 | 0.097 ± 0.007 | 0.113 ± 0.003 | 0.115 ± 0.004 | 0.989 ± 0.008 | 0.101 ± 0.002 |
| River water 3 | 1 | 1.011 ± 0.021 | 1.034 ± 0.019 | 1.032 ± 0.013 | 1.026 ± 0.011 | 1.131 ± 0.022 | 1.089 ± 0.021 |
| River water 4 | 5 | 5.063 ± 0.068 | 5.041 ± 0.059 | 5.044 ± 0.036 | 5.084 ± 0.047 | 5.027 ± 0.058 | 5.061 ± 0.107 |
| Distilled water | 1 | 1.006 ± 0.029 | 1.031 ± 0.023 | 1.015 ± 0.034 | 1.027 ± 0.058 | 1.019 ± 0.015 | 1.048 ± 0.044 |
As mentioned above, the probes reveal excellent selectivity and precision for template metal ions. Moreover, the probes also show potential in removing metal ions due to their large adsorption capacity and affinity. To evaluate adsorption and removal ability of the probes, river water samples spiked with mixed metal ions (Cu2+, Zn2+, Cr3+, Ni2+, Co2+, Pb2+, Cd2+ and Ag+ with each of 1 mg L−1) were measured as Fig. S7A.† The template metal ions (Cu2+, Zn2+ or Cr3+) can be selectively removed by relevant probe. After one time of adsorption by each probe, the removal rate could reach 93.4%, 87.9% and 91.7%. The adsorbed metal ion could be eluted with hydrochloric acid or ethylene diamine tetraacetic acid (EDTA), result in recover rate of 84.6%, 79.3% and 80.4% for Cu2+, Zn2+ and Cr3+. The removal rates of probes dependence with concentration of metal ions were also conducted as Fig. S7B.† The concentration of metal ions is proposed to be less than 10 mg L−1 with effective removal by 0.1 μM of probes.
The anti-interference ability of fluorescent probe is an essential target in application. Several common pollutants were added into river water (spiked with Cu2+, Zn2+ and Cr3+ each of 1 mg L−1) to simulate concrete situations of water pollution. The detection and removal rate of probes for template metal ions were measured as Table S3.† The results indicate suspended solids (KAl(SO4)2·12H2O) and colouring agent (KMnO4) will cause severe disturbance for determination. The reasonable explanation would be that light scattering or absorption by the pollutants will influence the intensity of fluorescence emission. The other common organic and inorganic pollutants will cause neglectable influence to determination. However, the removal rates for metal ions remain very high in the presence of those common pollutants, indicating the excellent performance on heavy metal ion treatment in environment water.
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra04712f |
| ‡ These authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2017 |