A novel fluorescent functional monomer as the recognition element in core-shell imprinted sensors responding to concentration of 2,4,6-trichlorophenol.

We have demonstrated a fluorescent functional monomer instead of the traditional functional monomers for molecularly imprinted sensors. The sensors were firstly used to selectively detect 2,4,6-trichlorophenol (2,4,6-TCP) by solid fluorescence detection without a dispersion solution. Moreover, the selectivity and anti-interference ability of the SiO2@dye-FMIPs sensor meet the requirements of a fluorescent sensor. The novel fluorescent monomer introduced into MIP is no longer just a fluorophore without recognizing ability. The fluorescence intensity of SiO2@dye-FMIPs showed a linear response to 2,4,6-TCP concentration in the range of 0-100 nM with a detection limit of 0.0534 nM. We could also demonstrate that such a system can not only get rid of the confines of traditional functional monomers and detection manner, but also improved the applications of MIPs sensors in sensing systems. This journal is © The Royal Society of Chemistry.

Introduction

Molecularly imprinted polymers (MIPs) with functional groups are an indispensable and powerful medium for selectively enriching and separating chemical species, in particular for small organic molecules. They are generally assembled by polymerizing functionalized monomers interacting with template molecules that are representative of the target or a similar molecule in size and chemical functionality. Once the templates are removed, cavities that are complimentary in terms of appropriate size and chemical functional demand remain in the cross-linked polymer matrix, compared to molecular non-imprinted polymers (NIPs), prepared for selectively recognizing and binding the target molecule.[1-3] MIPs have been used as chromatographic stationary phases or solid-phase extraction materials for their numerous advantages, such as excellent recognition properties, easy preparation, low cost, durability to heat and pressure, storage stability and applicability in harsh chemical media. Recently, MIPs have been applied for rather advanced analytical tasks, such as chemical sensing,[4-9] but the key step for their future success in a broader range of applications is introducing additional functional features.

The central part of a chemical sensor is the recognition element in order to assess the binding events directly with a sensitive analytical procedure, for example fluorescence detection technique.[10-15] Fluorescence detection based on fluorescent sensors is the most valuable method utilized in sensing thanks to its high sensitivity and simplicity. Fluorescence detection is the superior detection method in the field of sensing technology owing to several well-established advantages. Such signaling MIPs would be a sensor material and would expand the application of MIPs in fluorometric analysis instead of fluorescence label and displacement assays.[16-21] MIPs are usually used to separate analytes as a selective sorbent. A further analysis will then be carried out by other apparatus, which is not ideal for sensor applications.

MIPs in which fluorescent moieties are directly incorporated in the polymer are scarce. Moreover, the covalently embedded dye can only be employed as a fluorophore without recognition ability.[22,23] Perhaps the most feasible method, the covalent integration of a fluorescent probe monomer into an MIP, cannot however form the recognition sites with a functional monomer like methacrylic acid.[24-27] As the most appealing type, if we can find a fluorescent functional monomer that catches an analyte by hydrogen bonds, hydrophobic interactions, and/or π–π stacking interactions, the application of MIPs as a fluorescence sensor would provide satisfactory fluorometric analysis. To develop MIPs that show a reduction of fluorescence upon analyte binding and perform well in molecular recognition, we chose 7-allyloxycoumarin as the fluorescent functional monomer. It is constructed from a coumarin fluorophore and an allyloxy moiety, which can recognize templates via hydrogen bonds and π–π interactions. In addition, most fluorogenic MIPs are simply dispersed in solution at the presence of analytes in an analytical process. So, the unsteady dispersion solution may bring about an inaccurate result. Maybe solid fluorescence detection can solve the problem.

2,4,6-Trichlorophenol (2,4,6-TCP), widely employed in the manufacturing of fungicides, herbicides, pesticides, insecticides, antiseptics, pharmaceuticals, dyes and plastics, has been listed as a priority pollutant by the US Environmental Protection Agency and the European Union,[28] together with some other chlorophenol congeners. Adverse effects on human health caused by TCP, such as respiratory effects from coughs to serious pulmonary defects, gastrointestinal effects, and cardiovascular effects, have been reported.[26] Even low levels of 2,4,6-TCP in drinking water may be a serious threat to human health and natural ecosystems. Therefore, it is important to monitor the concentration of 2,4,6-TCP for human health, safety and environmental protection purposes.

In this work, we chose 2,4,6-TCP as our template, 7-allyloxycoumarin as the fluorescent functional monomer, ethylene glycol dimethacrylate (EGDMA) as the crosslinker, and 3-(methacryloxyl)propyltrimethoxysilane (MPS)-modified SiO2 spheres as the solid carrier to prepare an ideal fluorescent MIP sensor SiO2@dye-MIPs.

Experimental section

Materials and instruments

Tetraethyl orthosilicate (TEOS), 3-(methacryloxyl)propyltrimethoxysilane (MPS), 2,4-dichlorophenol (2,4-DCP), 2,5-dichlorophenol (2,5-DCP), 2,6-dichlorophenol (2,6-DCP), 2,4,6-trichlorophenol (TCP), N,N-dimethylformamide (DMF, 99.5%), allyl bromide, 7-hydroxycoumarin, ethylene glycol dimethacrylate (EGDMA), and 2,2′-azobis(2-methylpropionitrile) (AIBN) were obtained from Aladdin Reagent Co., Ltd. (Shanghai, China). Allyl bromide, acetonitrile, acetone, methanol, acetic acid and ammonia solution were all purchased from Sinopharm Chemical Reagent Co., Ltd. (Shanghai, China). Double distilled water was prepared in our laboratory and used for cleaning processes. All other chemicals used were of analytical grade and were obtained commercially.

1H-NMR spectroscopy was recorded on a Bruker AVANCE III HD400 NMR spectrometer. The morphologies of the samples were observed by an S-5500 scanning probe microscope and a transmission electron microscope (TEM, JEM-2100). Fluorescence intensity was measured using an F-4600 FL spectrophotometer.

Synthesis of 7-allyloxycoumarin

7-Allyloxycoumarin was prepared by Williamson reaction. A mixture of 7-hydroxycoumarin (1.62 g, 10.0 mmol), allyl bromide (2.42 g, 20.0 mmol), K2CO3 (4.97 g, 36.0 mmol) and acetone (60 mL) was heated and stirred at 57 °C in the dark under N2 for 10 h. The solvent was evaporated under reduced pressure. The crude product was recrystallized from chloroform, and the resulting product was separated by column chromatography on silica to obtain the product as a white powder. 1H NMR (400 MHz, CDCl3) δ 7.63 (d, J = 9.5 Hz, 1H), 7.37 (d, J = 8.6 Hz, 1H), 6.92–6.77 (m, 2H), 6.25 (d, J = 9.5 Hz, 1H), 6.04 (ddt, J = 17.2, 10.6, 5.3 Hz, 1H), 5.39 (ddq, J = 36.3, 10.5, 1.4 Hz, 2H), 4.60 (dt, J = 5.3, 1.5 Hz, 2H), in Fig. S1.†

Preparation of SiO2 beads modified by MPS

2 mL of ammonium hydroxide and 25 mL of double distilled water were added to 25 mL of ethanol and stirred for 15 min. The mixture was poured into a 100 mL flask. Then, 2.0 mL of TEOS was added into the flask sequentially and stirred at 300 rpm continuously at room temperature. After 6 hours, SiO2 spheres were separated by centrifuge and washed by ethanol and double distilled water.

The SiO2 spheres were redispersed in 40 mL of ethanol inside a round-bottomed flask and 1 mL of MPS was added into the flask. The round-bottomed flask was submerged in a thermostatically controlled oil bath at 40 °C and stirred at 300 rpm for 24 hours. The resulting SiO2–MPS spheres were separated by centrifuge from the solvent and washed five times sequentially in ultrasonic baths containing ethanol. Finally, the SiO2–MPS beads obtained were dried under vacuum for 12 hours at 40 °C.

Preparation of SiO2@dye-FMIP and SiO2@dye-FNIP

SiO2@dye-FMIP and SiO2@dye-FNIP were prepared by surface molecular imprinting technique (SMIT). 1.0 g of MPS-modified SiO2 beads was added to a 100 mL round-bottomed flask and dispersed in 60 mL of acetonitrile by sonication for 30 min. Then, 2,4,6-TCP (0.394 g, 2.0 mmol), 7-allyloxycoumarin (0.404 g, 2.0 mmol) and EGDMA (1.88 mL, 10.0 mmol) were dissolved in the round-bottomed flask in a glove box with N2. The reaction system was sparged with oxygen-free nitrogen for 15 min to expel the oxygen present inside the reaction flask. The flask was then submerged in a thermostatically controlled oil bath at 70 °C. After 3 hours, the SiO2@dye-FMIPs particles were collected from the reaction medium by centrifuge and then cleaned successively with methanol/acetic acid (100 mL, 95/5 v/v) to remove the templates by Soxhlet extractor. Finally, the product was dried in vacuo overnight at 40 °C. Fluorescent SiO2@dye-NIPs were prepared under nominally duplicate conditions to those used for the SiO2@dye-FMIPs in the absence of the 2,4,6-TCP template. By gravimetric analysis, the yields of SiO2@dye-FMIPs and SiO2@dye-FNIPs were found to be 87% and 83%, respectively.

The solid fluorescence detection experiments

The samples of SiO2@dye-FMIPs (100.0 mg) were dispersed in 100.0 mL of alcohol solution for spectrum measurement. After that, 2,4,6-TCP solutions in ethanol were prepared at various concentrations in the range of 0–1000 nmol. For the fluorescent measurements, 5 mL of the sample solution was mixed with 5 mL of the 2,4,6-TCP solutions of different concentrations. After 1.0 hour of dipping, the solids were separated by centrifuge and dried in vacuo overnight at 40 °C. Then a fluorescence spectrophotometer was used to detect the fluorescence intensity of the SiO2@dye-FMIPs sensors. Fluorescence spectra were measured under a 332 nm excitation light source. The fluorescence quenching efficiency of the SiO2@dye-FMIPs sensors with 2,4,6-TCP was calculated by Stern–Volmer equation (I0/I) − 1 = KSVC (I0 is the initial fluorescence intensity without analyte, I is the fluorescence intensity of the SiO2@dye-FMIPs with different standard 2,4,6-TCP concentrations, and KSV is the quenching constant with 2,4,6-TCP).

Selectivity experiments

To estimate the selectivity of the SiO2@dye-FMIPs sensor, we made a comparison between three structurally related compounds and 2,4,6-TCP. The 100 mg SiO2@dye-FMIP sensors were added to 100 mL of ethanol solutions containing 20.0 nmol of 2,4,6-TCP, 2,4-TCP, 2,5-TCP or 2,6-TCP. The mixtures were stirred for 1 hour at room temperature and solids were separated by centrifuge. The fluorescence intensity of the solids was detected by fluorescence spectrophotometer and the [(I0/I) − 1] was calculated with the fluorescence data. For comparison, the same procedure was applied using SiO2@dye-FNIPs instead of SiO2@dye-FMIPs.

Interference experiments

The capacity to resist interferents is one key fact to evaluate whether a sensor would be used in practical samples. To evaluate the SiO2@dye-FMIPs sensor's capacity of resisting interferents, 100 mg of SiO2@dye-FMIP was added into 100 mL of ethanol solutions containing 20.0 nmol of 2,4,6-TCP, 2,4-TCP, 2,5-TCP or 2,6-TCP. After stirring for 1 hour at room temperature, solids were separated by centrifuge. The fluorescence intensity of the solids was detected by fluorescence spectrophotometer.

Results and discussion

One of the factors that limits the application of fluorescent molecular imprinting is the complexity of the fluorescent functional monomer. Herein, we adopted the Williamson reaction to synthesize 7-allyloxycoumarin, which greatly simplified the process of the preparation of fluorescent functional monomers. As-synthesized 7-allyloxycoumarin not only had a recognition group but could also polymerize with other monomers (Scheme 1). To our knowledge, there are no reports about 7-allyloxycoumarin being used for MIPs, probes or sensors. The crucial interaction between 7-allyloxycoumarin and 2,4,6-TCP is hydrogen bonding because the absorption peak position of 2,4,6-TCP has a blue shift of 12 nm after adding 7-allyloxycoumarin in dichloromethane (in Fig. S2†). This blue shift in the absorption spectra might be attributed to the hydrogen bond between 2,4,6-TCP and 7-allyloxycoumarin. Versus covalent methods, non-covalent formation of MIPs is most often employed for introducing functionality into MIPs because of easier methodology and faster elution as a consequence of the rapid and reversible nature of the non-covalent interaction between the polymer and the template.

Scheme 1

Schematic illustration of the synthesis of 7-allyloxycoumarin.

As an alternative to molecular imprinting technique, surface molecular imprinting technique has emerged as an attractive, simple, and seemingly general method for facilitating the production process of imprinted products. The reason that we chose SiO2 microspheres as the solid support is because they possess a vast surface area, physical robustness and thermal stability, and can also be integrated in MIPs membranes.[29,30] Silica particles of about 255 nm were used as the support, as measured from the SEM image (Fig. S3†). The pure SiO2@dye-FMIPs was highly spherical and monodisperse with an average size of about 275 nm, as shown in Fig. S4.† A representative TEM image of the pure SiO2@dye-FMIPs is shown in Fig. S5;† when MPS-modified SiO2 spheres were coupled with the dye-FMIP layer, the grain size was increased by about 20 nm. In order to make 7-allyloxycoumarin copolymerise with other monomers in the MIP system, allyl groups were attached to the hydroxyl by reacting with allyl bromide. The structural properties of the synthesised SiO2@dye-FMIPs microspheres were analysed by FT-IR spectra. As shown in Fig. S6,† the characteristic peaks at 1730, 1258 and 1151 cm−1 are attributed to the stretching of the CO and C–O of EGDMA. The typical peaks of 2986 and 2956 cm−1 proved that 7-allyloxycoumarin had copolymerised with other monomers in the MIP system. The strong and broad peak around 1103 cm−1 indicated the Si–O–Si asymmetric stretching. These FT-IR spectra suggest that the SiO2@dye-FMIPs have been successfully prepared.

The performances of the SiO2@dye-FMIPs and SiO2@dye-FNIPs sensors were assessed by solid fluorescence with 2,4,6-TCP. Structural analogues 2,4-dichlorophenol (2,4-DCP), 2,5-dichlorophenol (2,5-DCP), and 2,6-dichlorophenol (2,6-DCP) were chosen as potential competitors. Solid fluorescence spectra were measured under a 332 nm excitation light source at room temperature. To study the fluorescence quenching mechanism of SiO2@dye-FMIPs sensors with 2,4,6-TCP, the quenching efficiency of SiO2@dye-FMIPs was evaluated by the Stern–Volmer equation (I0/I) − 1 = KSVC (I0 is the initial fluorescence intensity of SiO2@dye-FMIPs, I is the peak of the SiO2@dye-MIPs with different standard 2,4,6-TCP, and KSV is the quenching constant with 2,4,6-TCP).

As shown in Fig. 1, a significant inverse relation was found between fluorescence intensity and 2,4,6-TCP concentration. The more 2,4,6-TCP that is added, the weaker the fluorescence intensity is. It means that the fluorescence intensity of SiO2@dye-FMIPs (Fig. 1a) decreases with increasing 2,4,6-TCP concentration, and the reduced degree of fluorescent SiO2@dye-FMIPs was notably higher than that of the fluorescent SiO2@dye-FNIPs (Fig. 1b). It is illustrated that the spatial adsorption sites could be incorporated into the SiO2@dye-FMIPs matrix, but not in SiO2@dye-FNIPs. Therefore, it is also confirmed that SiO2@dye-FMIPs particles are more sensitive than SiO2@dye-FNIPs particles.

Fig. 1

Response of SiO2@dye-MIPs (a) and SiO2@dye-NIPs (b) to 2,4,6-TCP in the concentration range from 0 to 1000.0 nM.

The excellent linearity of the technique was investigated though the relationship of the fluorescence intensity with the concentration of 2,4,6-TCP in a working range from 0 to 100 nM, as shown in Fig. 2. The linear equation of the SiO2@dye-FMIPs sensor was (I0/I) − 1 = 0.01051Cc + 0.00582 (where Cc is the concentration of 2,4,6-TCP in nM, and (I0/I) − 1 is the relative fluorescence intensity), and the corresponding correlation coefficient (R2) was 0.99947. The limit of detection was evaluated using 3s/S, and was found to be 0.0534 nM (s is the standard deviation of the blank signal and S is the slope of the linear calibration plot). From the figure, we can see that the linear concentration range of SiO2@dye-FMIPs is much larger than that of SiO2@dye-FNIPs. This is because the quenching only took place between 7-allyloxycoumarin and 2,4,6-TCP at the surface of the SiO2@dye-FNIPs particles with no recognition sites, and did not happen both inside and outside like with the SiO2@dye-FMIPs particles.

Fig. 2

Linear response of the SiO2@dye-MIPs (a) and SiO2@dye-NIPs (b) to 2,4,6-TCP in the concentration range from 0 to 1000 nM.

It is well known that fluorescence quenching processes includes dynamic quenching and static quenching. In a dynamic quenching process, excited state molecules and quencher molecules collide with each other, leading to transition of the excited state molecule back to the ground state. At the same time, the lifetime of the fluorescent material reduces with the variety of fluorescence intensity. Static quenching happens between the quenching agent and the fluorescent molecule in the ground state, but the fluorescence lifetime is not changed. Both dynamic quenching and static quenching processes can be described by the Stern–Volmer equation:I0 is the initial fluorescence intensity without analyte. I is the fluorescence intensity in the presence of analyte. KSV is the Stern–Volmer quenching constant in units of L mol−1. C is the concentration of the molecular target. Kq is the rate constant of the bimolecular quenching process in units of L mol−1 s−1. τ0 is the lifetime without quenching agent.

Time-resolved fluorescence curves of SiO2@dye-FMIPs before and after adsorbing 2,4,6-TCP are shown in Fig. 3. The two decay curves were fitted by exponential function. The nonlinear equations of SiO2@dye-FMIPs before and after adsorbing 2,4,6-TCP are I(t) = 42 065.8 exp(−t/4.01076) + 0.00304 and I(t) = 2.47042 × 1010 exp(−t/1.79746) + 0.00363, and the corresponding correlation coefficients (R2) were R2 = 0.98147 and R2 = 0.98801, respectively. From the equations, we found that the lifetimes were τ0 = 4.01076 ns and τ = 1.79746 ns, respectively. The lifetimes were quite different in the presence and absence of 2,4,6-TCP. We found another kind of representation of the Stern–Volmer equation according to eqn (1):where τ is the lifetime with quenching agent.

Fig. 3

Time-resolved fluorescence curves of SiO2@dye-FMIPs before (a) and after (b) adsorbing 2,4,6-TCP.

According to eqn (2), we found the relationship KSV = Kqτ0. KSV is 0.01051 L mol−1, as shown in Fig. 2. Therefore Kq is 2.6 × 106 L mol−1 s−1. The rate constant (Kq) of maximum diffusion controlled dynamic quenching is 2.0 × 1010. The Kq in here is always <2.0 × 1010 L mol−1 s−1. In addition, the lifetime of fluorescent sensors reduces with the variety of fluorescence intensity. Thus, it is confirmed that dynamic quenching is a dominant process in this work.

Selectivity is a very important index for a sensor. To evaluate the selective recognition property of the SiO2@dye-FMIPs sensor, we chose structural analogues 2,4-DCP, 2,5-DCP, and 2,6-DCP as the competitors. Fig. 4 shows the fluorescence quenching efficiency of SiO2@dye-FMIPs for 2,4,6-TCP, 2,4-DCP, 2,5-DCP and 2,6-DCP. The fluorescence quenching efficiencies (I0/I) − 1 are 0.249, 0.024, 0.011 and 0.02, respectively. So, the fluorescence quenching efficiency of 2,4,6-TCP is much higher than other competitors. The results showed that none of the competitors being evaluated led to significant fluorescence quenching and the SiO2@dye-FMIPs sensor had a specific affinitive action owing to its recognition sites. In order to evaluate the selectivity, an imprinted selectivity factor was calculated using the following eqn (3):here, IMIP is the fluorescence intensity of SiO2@dye-FMIPs with 100 nM 2,4,6-TCP, INIP is the fluorescence intensity of SiO2@dye-FNIPs with 100 nM 2,4,6-TCP, and I0 is the background fluorescence intensity without 2,4,6-TCP. If the imprinted selectivity factor is higher than 1.0, it indicates that the MIPs exhibited good selectivity for 2,4,6-TCP. Finally, the imprinted selectivity factor obtained from fluorescence measurements was 2.95, which proved that SiO2@dye-FMIPs possessed high selectivity for 2,4,6-TCP.

Fig. 4

Quenching amount of SiO2@dye-FMIPs and SiO2@dye-FNIPs by different kinds of chlorophenols at 20 nmol L−1.

To further investigate the interference of 2,4-DCP, 2,5-DCP, and 2,6-DCP, the three competitors were mixed with same concentration of 2,4,6-TCP to form a mixture. In Fig. 5, the fluorescence intensity of the SiO2@dye-FMIPs sensor was changed unobviously for the three competitors, and the competitors being evaluated did not give any significant interference. This proves again that the SiO2@dye-FMIPs sensor has high selectivity for 2,4,6-TCP. The higher selectivity for 2,4,6-TCP results from its specific binding affinity of 2,4,6-TCP for an efficient imprinting effect because the same fluorescence quenching does not happen for SiO2@dye-FNIPs particles.

Fig. 5

Test for the interference of different chlorophenols on the fluorescence response toward 2,4,6-TCP of SiO2@dye-FMIPs sensor.

In order to assess the practical efficiency of the SiO2@dye-FMIPs sensor for the analysis of food samples, soda water purchased at Chinese supermarkets was used as a sample material. 5.0 mL of soda water was mixed with 5 mL of 2,4,6-TCP solution (concentration range 0–100 nM) and analyzed using the procedure discussed in Section 2. The results listed in Table 1 clearly demonstrate that SiO2@dye-MIPs sensor is capable of quantitatively measuring 2,4,6-TCP content in the concentration range of 0–100 nM. The results intelligibly established that SiO2@dye-MIPs could attain good recovery and could be effectively applied in the detection of 2,4,6-TCP in soda water samples. Compared to gas chromatography (GC),[31] the method in this work can selectively detect 2,4,6-TCP in complicated samples without interference from analogues. In addition, SiO2@dye-FMIPs could be used to monitor trace 2,4,6-TCP with a lower limit of detection (0.0534 nM), while the limit of detection for the GC method is 0.25 μg kg−1, which is much higher than the present method.

Recovery of 2,4,6-TCP in soda water samples at different concentration levels

Samples	Concentration taken (nM)	Concentration found (nM)	Recovery (%)
2,4,6-TCP	0	—	—
	1	0.98	98
	2	2.19	108
	5	5.13	103
	10	10.22	102
	20	20.87	104
	50	49.13	98
	100	101.45	101

Conclusions

In conclusion, we have demonstrated a fluorescent functional monomer instead of a traditional functional monomer for SMIP sensors. The sensors were firstly used to selectively detect analyte by solid fluorescence detection without a dispersion solution. Moreover, the selectivity and anti-interference ability of the SiO2@dye-MIPs sensor meet the requirements of a fluorescent sensor. The novel fluorescent monomer introduced into MIP is not only as a fluorophore but also as a functional monomer for recognizing the analyte. We could also demonstrate that such a system can not only get rid of the confines of the traditional functional monomers and detection manner, but also improved the applications of MIPs sensors in sensing systems.

Conflicts of interest

The authors declare no conflict of interest.