Abstract

Herein, by using the green and cheap L-cysteine as the precursor, nitrogen and sulfur codoped carbon dots (NS-CDs) were synthesized via a facile one-step hydrothermal method. The obtained NS-CDs showed the relatively narrow size distributions (2.1~3.9 nm) with the lattice spacing of 0.29 nm, as well as the excitation-dependent photoluminescence (PL) emission activity with the quantum yield (QY) of 18%. More interestingly, the PL intensity of NS-CDs was quenched by the addition of copper or lead ions (Cu2+ or Pb2+), which was shown in the tradition detection method by PL spectra. The NS-CDs exhibited ultrasensitive colorimetric sensing capability for both Cu2+ and Pb2+ by the color variance using naked eyes without any further treating. Two different coupling ways for detecting Pb2+ and Cu2+ were induced by the analysis of the Fourier transform infrared spectroscopy (FT-IR) and X-ray photoelectron spectroscopy (XPS). And the as-prepared NS-CDs showed their potential application in the heavy metal ions detection for the wastewater determination.

1. Introduction

Aside from the essential contribution in industry and electrochemistry, the pollutants of heavy metal ions such as copper (Cu2+) and lead (Pb2+) are still an unresolved issue in the industrial wastewater. Trace Cu2+ and Pb2+ would contaminate the drinking water as well as the bare soil, which would severely have long-term damage effects on human being’s brain, heart, kidney, lungs, and other organs. It is reported too much Cu2+ would affect the enzyme activity, and the cell metabolism would also be inhibited by excessive Cu2+ in the human body. And according to the United States Environmental Protection Agency (EPA), the maximum allowable level of Pb2+ in the blood is 0.1 mg/L (483 nM) [1, 2].

To protect human health and the environment, instrument-based assays including the atomic absorption spectrometry (AAS), electrochemical method, and inductively coupled plasma mass spectrometry (ICPMS) have been developed for the analysis detection of heavy metal ions. However, they have inevitable disadvantages such as the expensive equipment, sophisticated instrumentation, and tedious preparation processes [3, 4]. Nowadays, fluorescent sensors (including quantum dots, organic dyes, metal clusters, and rare-earth nanocrystals) have been widely explored for the detection of the heavy metal ions. Among these fluorescent sensors, carbon dots (CDs) have attracted considerable attentions, owing to their low cytotoxicity, robust chemical inertness, excellent biocompatibility, low photo-bleaching, and stable photoluminescence (PL) properties [58]. Plentiful preparation methods including “bottom-up” and “top-down” approaches made great efforts to synthesize the doped-CDs and significantly enhanced their properties to broaden their novel applications [9]. Nitrogen (N) and sulfur (S) are the most commonly doping elements for CDs. With the comparable atomic size (the radius of C: 0.77 Å, N: 0.75 Å), strong valence bonds, and similar electronegativity (electronegativity of C:2.55, S:2.58), the presence of the N and S atoms could produce additional electron pairs, new defects sites and the active sites, which would significantly modify the local chemical activities of the carbon nanostructures. In addition, these active sites can induce the electron transfer between the heavy metal ions and the doped-CDs. As it is reported, the doped-CDs have been successfully used in detection of Pb2+and Cu2+, respectively [1012].

For the detection of heavy metal ions, many researchers focused on the synthesizing luminescent CDs capable of sensitively and selectively detecting the metal ions, including choosing the green materials as the precursor, doping different elements into the CDs, and optimizing the surface functionalities for chelating with the metal ions [1316]. The photoluminescence (PL) spectra were commonly utilized for the detection of different heavy metal ions. Based on this method, the previous reports indicated that trace Cu2+ or Pb2+ ions (as low as to nanomole or micromole) would be detected by the various CDs in the aqueous solution [17, 18]. However, for the practical applications, visual one-site detection methods would be recommended for their convenience without any expensive equipment or complex processes. Few groups reported for this method. For example, Liu et al. developed a novel fluorescence test paper for the detection of Cu2+ ions. Under the 365 nm light, the fluorescence color of the test paper would change from blue to purple with the increasing concentration of Cu2+ ions. This method would be used as the semiquantification of the trace Cu2+ ions (~25 nM) [19]. Ansi and Renuka proposed the colorimetric analysis for Pb2+ ions in water. They prepared the CDs from the table sugar and applied them for the detection of Pb2+ ions. Due to the aggregation of CDs, the precipitated solution of CDs+Pb2+ ions could easily detected by the naked eye 9 (the detection limit of 67 nM) [20]. Therefore, the novel visual sensor systems should be developed in the field of water pollution detection.

Herein, a facile hydrothermal method was explored to prepare the N,S codoped CDs (NS-CDs) by using the green and nontoxic L-cysteine as the precursor. The obtained NS-CDs exhibited ultrasensitive detection characteristics for Cu2+ and Pb2+ through the PL emission quenching. Apart from the traditional PL detection method, it is also found that the NS-CDs could detect the Cu2+ and Pb2+ ions in aqueous solution directly and sensitively by the colorimetric method without further treatment. And unlike the complicated colorimetric detection process reported previously (for example, the gold nanoparticles functionalized by L-cysteine could detect the metal ions and the whole reaction should be induced by the ultraviolet light) [21], the newly synthesized NS-CDs have the advantages of simple and visual one-site detection for Pb2+ and Cu2+ with potential applications in the heavy ion detection of wastewater.

2. Experimental

All the reagents were purchased from Aladdin (Shanghai, China). All chemicals were used as received, without further purification. The ultrapure water used in the whole experiment holds the resistivity no lower than 18.1 MΩ cm. The Ca(NO3)2•4H2O, FeCl3, Pb(NO3)2, MgCl2•6H2O, Zn(NO3)2•6H2O, KNO3, Cu(NO3)2•3H2O, FeCl2•4H2O, Na2CO3, and Al(NO3)3•9H2O were selected as the sources of heavy metal ions, and each solution was confected to the concentration of 20 mmol/L.

3. Preparation of Samples

The NS-CDs are synthesized as follows. The mixture of 0.015 g L-cysteine and 30 ml ultrapure water became a homogeneous solution after a stirring drastically for 10 minutes and was transferred into the Teflon-lined autoclave. After maintained at 190°C for 6 hours, the obtained slight green solution was further dialyzed for 8 h in the dialysis bag with the molecular weight cutoff (MWCO) of 1000 Da against the ultrapure water for purification. And finally, the product was dried through a freezing dryer. A series of metallic salt (including Ca2+, Fe2+, Al3+, Pb2+, Mg2+, Zn2+, Fe3+, K+, Cu2+, and Na+) solutions were prepared separately and added into the NS-CDs solution for determining the detection properties.

4. Sample Characterization

The transmission electron microscopy (TEM) was performed using an F-30 S-TWIN electron microscope (Tecnai G2, FEI Company). A Rigaku D/Max-2400 X-ray diffractometer (XRD) was employed to check the phases of the obtained samples. Deionized water was gained by a Millipore Elix 5 UV and Milli-Q Gradient Ultra-Pure Water System. X-ray photoelectron spectroscopy (XPS, PHI-5702, Physical Electronics) was performed using a monochromated Al Ka irradiation. The Fourier transform infrared spectra (FT-IR) of the samples were recorded between 500 and 4000 cm-1 on a FT-IR spectrometer (Nicolet NEXUS 670) using KBr pellets. The photoluminescence (PL) spectra and fluorescence emission spectra were recorded using an FLS-920T fluorescence spectrophotometer and a HORIBA JOBIN YVON Fluorolog-3 Spectrofluorometer system at 16°C, respectively. Without a particular statement, all the measurements were performed at room temperature.

5. Results and Discussion

Just as it revealed in the TEM image NS-CDs (Figure 1(a)), the as-prepared NS-CDs showed an ellipsoid morphology and well-dispersed with a relatively narrow size distribution of 2.1-3.9 nm (Figure 1(b)). The high-resolution TEM (HRTEM) image inset of Figure 1(a) indicated the high crystallinity of the NS-CDs with the lattice spacing of 0.29 nm, corresponding to the (002) spacing of graphitic carbon lattice parameters. For further exploring the statue of elements, XPS use used to probe the NS-CDs. In the high-resolution XPS carbon (C) spectrum (Figure S1), the five peaks at 284.4, 284.9, 285.5, 286.5, and 288.7 eV should be attributed to C=C, C-S, C-N, C-O, and C=O groups. The S 2p band could be deconvoluted into two peaks, corresponding to C-S-C 2p 2/3 (163.8 eV) and C-S-C 2p 1/2 (164.9 eV), and the N band could be divided into two peaks, corresponding to pyrrolic N (400.1 eV) and N-H (401.5 eV), as shown in Figure S2. Clearly, the N and S atoms were successfully doped and should constitute the main surface functional groups on the NS-CDs.

The UV-vis absorption spectrum (Figure 1(c)) displayed several small absorption bands in the range of 250-400 nm, the band at 270 nm should be corresponding to the π-π transition of the aromatic sp2 domains [22], and the bands at 340 nm and 400 nm should be ascribed to the trapping of the excited state energy of the surface states. Various surface states were original from the multiple N-, S-, C-, and O-containing functional groups on the surface of the NS-CDs. The decay curve was recorded for the NS-CDs at 360 nm by a time-correlated single-photon counting technique, as shown in Figure 1(d). The lifetimes were , , and [23].

The PL emission spectra of NS-CDs were shown in Figure 2(a), and the maximum emission peak positions were dependent of the excitation wavelength. The emission peaks slightly shifted to longer wavelengths (from 407 nm to 450 nm) when the excitation wavelength increased from 310 nm to 390 nm, accompanying with the decreasing PL emission intensity. The maximum emission wavelength is located at 440 nm with the excitation wavelength of 360 nm. The Commission International de L’Eclairage (CIE) under different excitation wavelength (310-390 nm) was shown in Figure 2(b), and the CIE coordinate was calculated as (0.1746, 0.1551), displaying the area of maximum emission (440 nm) under the excitation at a wavelength of 360 nm. With the excitation wavelength increasing, the emission position ranged from the blue to blue-green area. The PL behavior might be attributed to the different size distribution and various surface state emissive traps on the surface of NS-CDs [24]. The quantum yield (QY) of the NS-CDs was measured according to the method of quinine sulfate [25]. Quinine sulfate diluted by 0.1 M H2SO4 solution was chosen as the reference standard substance, and the QY was 0.55. The calculation equation of QY is as follows.

The NS-CDs was represented as the subscript “,” and the standard substance was represented as the subscript. The “,” “,” “,” “,” and “” are the absorbance, integrated fluorescent emission intensity, refractive index, and the QY. Based on the calculation with quinine sulfate as the standard substance, the QY value of the NS-CDs is 18%.

The stability of CDs is very important for their practical application. Then, the fluorescent stability of NS-CDs was examined for a wide range of postheat treatment temperature (30~90°C) at fixed temperature for 2 h. The PL emission spectra were shown in the supporting information (Figure S3). The maximum emission intensity at 440 nm slightly increased upon raising the heat treatment temperature from 30 to 90°C, and the phenomena would be attributed to the recovery of partial surface defects. The result is similar to the reported N-doped CDs prepared by using ammonium citrate and urea as the precursors [26]. The as-prepared CDs exhibited excellent thermal stability.

To investigate the sensing specificity of NS-CDs, we measured the PL responses to ten common metal ions such as Na+, Zn2+, Mg2+, K+, Al3+, Ca2+, Fe3+, Fe2+, Pb2+, and Cu2+ (20 mM) for the fixed incubation time of 5 min, as shown in Figure 2(c). It is found that the as-prepared NS-CDs exhibited sensitive detection property for Pb2+ and Cu2+ by the substantial PL emission quenching effect. For the other ions, the existence of the Na+, Zn2+, Mg2+, and K+ ions had almost no influence on the PL intensity of NS-CDs, while the PL was slightly quenched in the presence of Al3+, Ca2+, Fe3+, and Fe2+ ions. Compared with the above metal ions, it was indicated that Cu2+ and Pb2+ ions could effectively quench the PL emission of NS-CDs. The absorption spectra and the decay curves of NS-CDs, dots+Cu2+, and dots+Pb2+ ions are shown in Figure S4. For the Cu2+ ion detection, the quenching process should be related to the static quenching mechanism, which means that a nonfluorescent ground-state complex formed through the interaction between NS-CDs and the quencher (Cu2+ ions). And this quenching is accompanied with the change of the absorption spectrum of the NS-CDs as well as the almost unchanged average fluorescence lifetime ( was 2.98 ns for NS-CDs and 3.04 ns for dots+Cu2+). The quenching mechanism was similar to the previous report of the quenching of Cu2+ ions by the CDs prepared from thiourea and diethylene glycol via microwave irradiation [27]. While for the detection of Pb2+ ions, the change of the absorption spectrum was also observed. After fitting the decay curve, a new and short (0.0567 ns) appeared, and the other values were similar to that of NS-CDs. The calculated average fluorescence lifetime decreased to 2.79 ns. Therefore, static quenching and dynamic quenching process could be coexisted for the Pb2+ quenching mechanism. The new component would be related to the dynamic quenching process, which means that the excited state of NS-CDs would return to the ground state by the collision between the Pb2+ ions and NS-CDs by energy transfer or charge transfer [28].

To further investigate the coordination interactions between NS-CDs with the Cu2+ and Pb2+ ions, the FT-IR spectra of the pristine NS-CDs, dots+Cu2+, and dots+Pb2+ samples were measured to detect the changes of the stretching vibrations of the functional groups, as shown in Figure 3(a). The stretching vibrations of O-H and N-H in the NS-CDs were distinctively observed by the broadband from 3185 cm-1 to 3440 cm-1. Contrarily, after coordinated with Cu2+ or Pb2+ ions, the vibration band of the O-H and N-H shifted to long wavenumbers and narrowed, suggesting the cheating effects of Cu2+ or Pb2+ions with these functional groups on the NS-CDs [29]. The stretching vibrations of C-O-C in the dots+Cu2+ and dots+Pb2+ disappeared (at 1240 cm-1). For dots+Cu2+, the changes of the peaks at 600 cm-1 and 727 cm-1 revealed the combination between the Cu2+ions and C-S groups. For dots+Pb2+, the pyridine-, pyridine-N-O-, and/or pyridine-like peaks at 1125 cm-1 shifted to 1032 cm-1, which was related to bind with Pb2+ ions [30].

We also compared the XPS spectra of pristine NS-CDs, dots+Cu2+, and dots+Pb2+ samples, as shown in Figure 3(b). It should be noted that the main state of copper was Cu 2p 3/2 state at 932.0 eV, which were frequently connected to the coordination between Cu and S/O-related groups, and the next-door peak at 954.0 eV corresponded to the Cu 2p1/2 state [31, 32]. There were also observed the small peak at 161.5 eV, which represented the existence of Cu-S bonds. As shown in Figure S5(a), the II peak at 532.2 eV should demonstrate the presence of Cu-O bonds [33]. The full spectrum of dots+Pb2+ displayed that lead mainly existed in the state of Pb 4f in the range of 135-140 eV. The 138.5 eV band was assigned to Pb species adsorbed with the oxygen- and/or nitrogen-containing groups of the NS-CDs, while the 140.0 eV should be related to Pb2+ adsorbed on the NS-CDs surface as the Lewis centers or p-electrons-cation interactions. What is more, the peaks at 412.0 eV, 434.3 eV, and 643.6 eV were assigned to the Pb 4d5, Pb 4d3, and Pb 4p3 states, respectively. As shown in Figure S5(b), the peaks at 529.1 eV and 530.1 eV in the high resolution of O 1 s of dots+Pb2+ revealed that the oxygen was mainly in the state of -C=O (carboxyl). It might be inferred that the coupling of the Pb2+ and NS-CDs was in the following ways of (=C-COO)2Pb, =C-COOPb+, =N-Pb(OH)+, and ≡C-Pb2+ (C -cation interactions) [34]. Figure 4 gave the possible schematic illustration of the NS-CDs and its interaction with Cu2+ or Pb2+ ions.

In addition to the PL detection mentioned above, the fast, portable, and on-site colorimetric method had also been applied in detecting Cu2+ and Pb2+ ions. This method required no equipment and only used the naked eye recognition by the color change. The follow-up experiments were designed to evaluate the detectable concentration of Cu2+ and Pb2+ ions in the solution of NS-CDs by the change of color (Figure 5). It was reasonable to take the high sensitivity and fast response advantages to determine the specific Cu2+ and Pb2+ ions by means of the color variance. Cu2+ and Pb2+ ions produced the visual color response (from colorless to thin yellow for Cu2+ and to brown for Pb2+) after being added into the NS-CDs aqueous solution, while for other metal ions, the solution did not have a noticed color change. For the Cu2+ ions (the concentration range was 0-500 μM, Figure 5(b)), the minimum observable concentration was 50 μM, and the detection degree could reach as high as the result obtained by the reported gold nanoparticles previously [21]. The minimum detection concentration of Pb2+ ions was lower than that of Cu2+ ions (20 μM, Figure 5(a)). And when the concentration of Pb2+ ions was less than 20 μM, no observable change was observed, and it could be considered as the detectable minimum concentration of Pb2+ by the colorimetric method.

6. Conclusion

In summary, NS-CDs were prepared by using the L-cysteine as the precursor via a feasible hydrothermal method. The as-prepared NS-CDs revealed the efficient detectability for Pb2+ and Cu2+ by the PL quenching detection as well as the colorimetric method. The analysis of the FT-IR and XPS spectra of the precipitate revealed that the Cu-O and Cu-S bonds were mainly coordination styles for Cu2+ ions on the NS-CDs, while for Pb2+ ions, they would prefer to connect to the NS-CDs in the forms of =C-(COO)2Pb, =C-COOPb+, =N-Pb(OH)+, and ≡C:Pb2+ (C-cation interactions). With a specific and sensitive detectable property, the NS-CDs exhibited an irreplaceable application in the wastewater determination in the industry and environmental monitoring.

Data Availability

All data generated or analyzed during this study are included in this article.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Authors’ Contributions

Hui Gao and Yuqian Pang contributed equally to this work.

Acknowledgments

This work was financially supported by the National Science Foundation of Gansu Province (18JR3RA269), the National Natural Science Foundation of China (61378037), the National First-class Discipline Program of Food Science and Technology (JUFSTR20180302), and the National Key Research and Development Program of China (2018YFC1604204, 2018YFD0400402).

Supplementary Materials

Figure S1. The high resolution C 1s XPS spectrum for NS-CDs. Figure S2. The high resolution spectra of (a) S 2p XPS and (b) N 1s XPS for NS-CDs. Figure S3. (a) The PL emission spectra and (b) the ratio of I/Io of NS-CDs under different heat treatment temperature for 2 h. Figure S4. (a) The UV-Vis absorption spectra and (b) the luminescence decay spectra of NS-CDs, dots+Cu2+ and dots+Pb2+. (Supplementary Materials)