Open Access Article
Lijun Luo,
Libo Li,
Xixi Xu,
Dong Liu,
Jinyang Li,
Kun Wang
* and
Tianyan You*
School of Agricultural Equipment Engineering, Institute of Agricultural Engineering, Jiangsu University, Zhenjiang, Jiangsu 212013, China. E-mail: youty@ujs.edu.cn; Fax: +86-511-88982992; Tel: +86-511-88982992
First published on 30th October 2017
Sensitive and quantitative analysis of pentachlorophenol (PCP) is especially important in the field of ecology and agriculture. Herein, a highly sensitive and stable Ru(bpy)32+-based anodic electrochemiluminescence (ECL) system utilizing nitrogen-doped graphene quantum dots (NGQDs) as a novel co-reactant was firstly constructed to detect PCP. In this system, Ru(bpy)32+ was used as luminophor, while NGQDs were applied as co-reactant in place of the toxic and volatile tripropylamine. The novel co-reactant not only promoted the luminous efficiency of Ru(bpy)32+, but also improved the stability of the ECL system. In addition, the enhancement mechanism of NGQDs on Ru(bpy)32+ and quenching mechanism of PCP on Ru(bpy)32+/NGQDs were investigated in detail. Under the optimum conditions, the as-fabricated sensor for ultrasensitive PCP determination expressed a wider linear range of 1 × 10−15 to 1 × 10−5 g mL−1 and a lower detection limit of 2 × 10−17 g mL−1 with good stability and repeatability. Furthermore, based on the distinctive advantages of the novel ECL sensor, it was successfully used to detect PCP in tap water and river water, and satisfactory recoveries were obtained.
In recent years, the development of an electrochemiluminescent (ECL) sensor for the detection of PCP has attracted more and more attention owing to its miniaturization, inexpensive detection instrument, high sensitivity and rapid response. Using Au nanoclusters as luminophor with S2O82− as co-reactant, Luo et al.12 constructed a cathodic ECL sensor to detect PCP with an unprecedented sensitivity. In order to further improve the sensitivity of the developed ECL sensor based on novel ZnO-nanocrystal composites, Jiang et al.13 introduced graphene into the ECL system as a substrate and signal amplification reagent, resulting in ECL intensity enhancement by about 4.3-fold. Currently, with the development of carbon material science, many ECL systems based on carbon nanomaterials, such as graphene,14 g-C3N4,15 and graphene quantum dots (GQDs)16 have been widely used for detection. Among them, the ECL of GQDs, especially the heteroatom-doped GQDs, have attracted wide attention owing to their unique features, including good water solubility, low toxicity and better edge effect.17 For example, Li et al.18 built a novel ECL sensor based on carbon quantum dots with S2O82− as co-reactant to detect PCP, achieving a low limit of detection. Similarly, utilizing nitrogen-doped GQDs (NGQDs) as luminophor, Du et al.19 constructed a cathodic ECL sensor for the detection of PCP. The introduction of N atoms significantly enhanced the stability and reproducibility in comparison with GQDs. However, most of the above-mentioned ECL systems for PCP detection are mainly based on the cathodic ECL system. To the best of our knowledge, the use of anodic ECL system for the detection of PCP is rarely reported.20
Ru(bpy)32+ is a typical anodic ECL luminophor possessing many distinguishing features, such as recyclability, high luminous efficiency, chemical stability and excellent biocompatibility.21 Therefore, the Ru(bpy)32+-based anodic ECL system is widely applied in many fields.22–26 However, tripropylamine (TPA), as the traditional co-reactant of Ru(bpy)32+, has undesirable volatility and toxicity, as well as low sensitivity at low concentrations. Hence, it is extremely imperative to develop alternative co-reactants to TPA. Recently, it has been reported that carbon quantum dots (CQDs) can be innovatively utilized as co-reactant of Ru(bpy)32+ to fabricate the anodic ECL system.27,28 We also carried out some preliminary work on a Ru(bpy)32+/CQDs ECL system,29,30 which showed that using carbon dots or related composites as the co-reactant of Ru(bpy)32+ resulted in good analytical performance for bisphenol A or dopamine detection. Nevertheless, it is well known that the exploration of anodic ECL systems based on Ru(bpy)32+/GQDs is still in its infancy.
Herein, we utilize nitrogen-doped graphene quantum dots (NGQDs) as the co-reactant of Ru(bpy)32+ to establish an anodic ECL sensor for PCP detection and to solve the problem of low sensitivity and poor stability. Effects of some experimental conditions on the ECL system were optimized, and the detection of PCP in real samples was analyzed under the optimum conditions. Furthermore, the enhancement mechanism of NGQDs and quenching mechanism of PCP on ECL signals were studied in detail.
The tap water and river water samples were obtained from the tap used in the experiment and Yudai River (Jiangsu University), respectively. The water samples were filtered with a 0.22 μm cellulose membrane, and a certain volume of the solution was added to the background solution for PCP assay.
The functional groups on the surface of NGQDs were characterized by FT-IR measurement. As can be seen from Fig. 1B, the broad peaks at 3460 and 3173 cm−1 indicate the presence of O–H and N–H bonds, respectively. The band around 1640 cm−1 is assigned to the C
O stretching vibrations of the carbonyl and carboxyl groups. The appearance of C–N stretching vibration at 1400 cm−1 illustrates the successful doping of N31 into GQDs. In addition, the absorption band at 1116 cm−1 is attributed to the stretching vibration of C–O. These results demonstrate that NGQDs are well prepared, and the nitrogen atoms have been successfully doped into GQDs.
The optical performance of NGQDs was investigated by UV-vis and FL spectroscopy. From the UV-vis spectrum (Fig. 1C), it can be observed that NGQDs exhibit one remarkable peak centered at 334 nm, which is ascribed to the π–π* conjugate structures of aromatic sp2 domains in the NGQDs. The inset of Fig. 1C shows that the bright yellow aqueous solution of NGQDs can emit bright blue fluorescence under UV light of 365 nm. The maximum excitation and emission wavelength of NGQDs are located at 350 nm and 436 nm, respectively. In order to deeply investigate the optical properties of NGQDs, detailed photoluminescence studies were carried out under different excitation wavelengths. In general, the photoluminescence spectra of most carbon nanoparticles are dependent on the excitation wavelength. In other words, the emission wavelength and peak intensity change obviously with the excitation wavelength, attributed to quantum confinement of emission energy traps on the particle surface.32 In contrast, as shown in Fig. 1D, the as-prepared NGQDs exhibit photoluminescent properties independent of the excitation wavelength. When the excitation wavelength increases from 300 to 390 nm, the emission peak location changes slightly (Fig. 1D), indicating that the surface state of NGQDs is relatively uniform.33
Corresponding ECL-potential curves illustrate that the ECL signal (Fig. 2B, a) of Ru(bpy)32+ is observed at 1.15 V (ca. 400 a.u.), while the signal of NGQDs (Fig. 2B, b) is fairly weak. In contrast, upon the addition of NGQDs to the Ru(bpy)32+ system, the ECL intensity (ca. 12
800 a.u.) of Ru(bpy)32+ is enhanced by about 30-fold (Fig. 2B, c). The obvious improvement of ECL intensity illustrates that NGQDs indeed can be used as a novel co-reactant of Ru(bpy)32+. However, with the existence of PCP, the ECL signal is significantly quenched by 50% (Fig. 2B, d), which further proves that PCP has quenching effect on the anodic ECL system and that it is feasible to detect PCP using the Ru(bpy)32+/NGQDs system.
In order to investigate the enhancement mechanism of NGQDs on Ru(bpy)32+, UV-vis, FL and ECL spectra are measured in detail. Fig. 2C shows the UV-vis absorption spectra of NGQDs, Ru(bpy)32+ and their mixture. NGQDs display one characteristic band at 334 nm (Fig. 2C, a), while individual Ru(bpy)32+ (Fig. 2C, b) exhibits two adsorption peaks at 281 and 455 nm, which are ascribed to the π–π* transition and metal-to-ligand charge transfer, respectively. Meanwhile, it can be observed that the NGQDs/Ru(bpy)32+ mixture has three absorption peaks (Fig. 2C, c) at 334, 283 and 455 nm, corresponding to the adsorption peaks of NGQDs and Ru(bpy)32+, respectively, indicating that no direct chemical reaction occurs between them. The FL spectra (Fig. 2D) of the mixture also exhibits the approximate emission features of both NGQDs (417 nm) and Ru(bpy)32+ (610 nm), which illustrates that NGQDs and Ru(bpy)32+ maintain their original FL characteristics, further confirming the conclusion that they do not react with each other. Fig. 2E shows that the ECL spectrum of the Ru(bpy)32+ and NGQD mixture agrees well with the FL spectrum of Ru(bpy)32+, but is totally different from that of NGQDs. The results clearly prove that the ECL signal is caused by Ru(bpy)32+ rather than NGQDs, illustrating that Ru(bpy)32+ is the luminophor rather than NGQDs, which is consistent with the previous report.34 More importantly, the NGQDs acted as a novel co-reactant to significantly increase the ECL signal.
Based on the above studies and previous reports,29,34 we can speculate that the role of NGQDs is similar to that of TPA as co-reactant, which could promote the luminous efficiency of Ru(bpy)32+. The specific mechanism involved in the presence of NGQDs is described as follows (Scheme 1): first, Ru(bpy)32+ is oxidized to Ru(bpy)33+ on the surface of the working electrode; then, Ru(bpy)33+ reacts with the NGQD intermediate to form an excited Ru(bpy)32+*. Finally, the return of Ru(bpy)32+* to its ground state is accompanied by the emission of light at 620 nm.
![]() | ||
| Scheme 1 The possible enhancement mechanism by NGQDs and quenching mechanism by PCP of the ECL system. | ||
Cyclic voltammetry was carried out to understand the possible quenching mechanism of PCP on the novel anodic ECL system. Fig. 2F shows that PCP exhibits irreversible electrochemical oxidation at about 0.78 V (vs. Ag/AgCl) under the scan rate of 100 mV s−1. The oxidation potential of PCP is more negative than that of Ru(bpy)32+/3+ (1.15 V). Therefore, it can be deduced that the oxidation products of PCP may play an important role in the quenching process. To examine this, the oxidation process of PCP was studied by changing the scan rate from 25 to 500 mV s−1. It can be seen (Fig. 2F) that with the increase of the scan rate, the oxidation peak potential of PCP gradually shows a positive shift. The inset of Fig. 2F expresses the relationship of peak potential (Epa) and ln
ν with the linear regression equation: Epa (V) = 0.6894 + 0.02245 ln
ν (V s−1) (R2 = 0.993). According to Laviron's theory,35 the Epa can be described by the following equation,
The concentration of NGQDs is a very key factor that affects ECL intensity (IECL). Thus, the influence of NGQDs on IECL was investigated in the range of 1–10 mg mL−1. As indicated in Fig. 3A, IECL increases with increasing NGQD concentration from 1 mg mL−1 to 5 mg mL−1, while it begins to decrease when the concentration exceeds 5 mg mL−1. As described earlier, NGQDs could promote the luminous efficiency of Ru(bpy)32+; thus, IECL increases with higher NGQD amounts. However, the inner filter effect from a high concentration of NGQDs could cause a secondary reaction,27 which could decrease the IECL. Therefore, the optimum NGQD concentration is chosen as 5 mg mL−1.
![]() | ||
| Fig. 3 Optimization of experimental parameters: (A) NGQD concentration, (B) Ru(bpy)32+ concentration, (C) pH value, and (D) concentration of buffer solution. | ||
Concentration of Ru(bpy)32+ is another important factor that influences ECL intensity. Fig. 3B shows that the ECL signal increases correspondingly when the concentration of Ru(bpy)32+ increases from 0.1 mM to 0.5 mM; then, IECL begins to drop off thereafter. This is due to the increase of Ru(bpy)32+, which results in more luminophors dispersed in the solution, resulting in a higher ECL response. When the concentration is too high, the ECL emission may be absorbed or scattered.39 Thus, 0.5 mM Ru(bpy)32+ is selected for sensor preparation.
Since the ECL of the Ru(bpy)32+/NGQDs system is a pH-dependent reaction, the effect of buffer solution pH on the ECL response was investigated (Fig. 3C). The IECL increases with pH value in the range of 5.0–7.5, while it begins to gradually decrease at higher pH value. The increase of IECL should be attributed to the comprehensive effect of pH value on Ru(bpy)32+ consumption40 and NGQD deprotonation. However, extremely high pH value would cause decomposition of some species, which further leads to decreased ECL signal and an unstable system. Consequently, the pH value is designated as 7.5 in subsequent experiments.
In addition, the concentration of buffer solution also plays a significant role in constructing the Ru(bpy)32+/NGQDs ECL system (Fig. 3D). The maximum ECL signal can be obtained at a buffer concentration of 30 mM. This could be attributed to the fact that with increasing concentration, the buffering effect becomes better. However, too high ionic strength of the solution caused by higher buffer concentration will result in reduced ECL signal. Hence, 30 mM pH 7.5 buffer solution is used throughout the experiments.
CPCP. The limit of detection (LOD) for PCP analysis using the developed sensor was calculated (using 3σ method) to be 2 × 10−17 g mL−1. Compared with previous ECL sensors for PCP detection, it can be clearly seen from Table 1 that the as-prepared Ru(bpy)32+/NGQDs anodic ECL sensor exhibits a wider linear range, which spans ten orders of magnitude. We also obtain the lowest detection limit for PCP in comparison with other sensors, indicating the highest sensitivity of the proposed sensor.
| Methods | ECL | Linear range (g mL−1) | LOD (g mL−1) | Reference |
|---|---|---|---|---|
| Au NCs-GR/S2O82− | Cathodic | 2.66 × 10−15–2.66 × 10−11 | 2.66 × 10−15 | 12 |
| ZnO/N-GR/GCE/S2O82− | Cathodic | 1.33 × 10−13–1.63 × 10−8 | 4.27 × 10−14 | 13 |
| GQDs-CdS NCs/GCE/H2O2 | Cathodic | 1 × 10−11–5 × 10−7 | 3 × 10−12 | 19 |
| Luminol/GQDs-Cu2O | Anodic | 2 × 10−11–3 × 10−6 | 6.6 × 10−12 | 20 |
| Ru(bpy)32+/NGQDs | Anodic | 1 × 10−15–1×10−5 | 2 × 10−17 | This work |
To investigate the selectivity of the established ECL sensor, 2,3,5-trichlorophenol (TCP), 2,4-dichlorophenol (DCP) and 2,4-dinitrophenol (DNP) were used as interfering substance to evaluate the specificity of the proposed sensor (Fig. 4C). The results indicate that the addition of 0.5 μg mL−1 (5 times of PCP) DCP, DNP and TCP lead to only 2.7%, 3.3% and −4.5% decreases in ECL intensity of the Ru(bpy)32+/NGQDs system, respectively. The addition of 0.1 μg mL−1 PCP results in a 38.3% decrease in ECL intensity, indicating that the sensor has good selectivity for PCP detection. Moreover, there are some other interfering ions in real water samples, such as metal ions (Na+, K+, Ca2+, Mg2+) and inorganic ions (Cl−, NO3−, SO42−). Thus, the effects of these interferences were also examined, and the results show these ions (c.a. 10 times of PCP) have no interference on the ECL system. All of these results prove that the fabricated sensor has a high selectivity for PCP detection.
The stability and repeatability of the anodic ECL sensor were evaluated systematically. Firstly, the operational stability of the sensor was investigated by consecutively scanning for 40 cycles and recording the ECL signals of the Ru(bpy)32+/NGQDs system in the presence of PCP. As seen from Fig. 4D, the ECL response exhibits a desirable consistency with a relative standard deviation (RSD) of only 1.1%, suggesting the high stability of the ECL sensor for PCP detection, which is attributed to the introduction of NGQDs. Secondly, operational and long-term storage repeatability of the sensor were also evaluated. On the one hand, operational repeatability was examined using six different working electrodes. The RSD of six parallel experiments is calculated to be 0.4% (Fig. 4E). On the other hand, the as-prepared sensor is stored at room temperature, and the ECL response of the sensor was continuously recorded every day for one month, with a RSD of 3.5% (Fig. 4F). These results fully demonstrate the ideal repeatability of the Ru(bpy)32+/NGQDs anodic system.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra10247j |
| This journal is © The Royal Society of Chemistry 2017 |