DOI:
10.1039/C6RA27844B
(Paper)
RSC Adv., 2017,
7, 10875-10880
Ratiometric luminescence detection of hydrazine with a carbon dots–hemicyanine nanohybrid system†
Received
6th December 2016
, Accepted 4th February 2017
First published on 10th February 2017
Abstract
It is significant to develop probes for rapid, selective, and sensitive detection of highly toxic hydrazine in both environmental and biological science. In this work, under mild conditions, through the electrostatic attraction between negatively charged CDs and positively charged hemicyanine molecules, a novel ratiometric fluorescent probe containing CDs and a hemicyanine derivative was fabricated for reliable, selective, and sensitive sensing of hydrazine. This nanohybrid system possesses dual emission peaks at 550 and 610 nm under a single excitation wavelength of 530 nm. The addition of hydrazine to CDs–hemicyanine nanohybrid solution results in complete fluorescence quenching of the hemicyanine derivative, while the orange fluorescence of CDs remains constant. Furthermore, the CDs–hemicyanine nanohybrid system shows high selectivity toward hydrazine over other various species, including some nucleophilic species, metal ions and anions. The limit of quantification (LOQ) was 0–1 mM and the detection limit was as low as 8.0 μM.
Introduction
As a highly reactive base and reducing agent, hydrazine plays crucial roles in the chemical, pharmaceutical and agricultural industries.1–3 Due to its detonable characteristics, hydrazine is also a high-energy fuel for rocket-propulsion systems and missile systems.4 However, hydrazine is classed as a highly toxic and pollutant compound, which can potentially lead to serious environmental contamination during its manufacture, use, transport and disposal. In addition, as a neurotoxin, hydrazine has several mutagenic effects, which can cause damage to the liver, lungs, kidneys and central nervous system of humans.5–7 Besides, hydrazine is readily absorbed through oral, dermal or inhalation routes of exposure and it can cause harm to live cells. Due to its widespread application, easy absorbance, and high toxicity, hydrazine has been classified as a probable human carcinogen by the U.S. Environmental Protection Agency and has a low threshold limit value of 10 ppb.8 Thus, an efficient and simple method for determining hydrazine levels is urgently needed in both environmental and biological science.
Approaches such as chromatography-mass spectrometry, titration and electrochemical methods are available to measure hydrazine, but they often require complicated equipment and sample handling and professional operating personnel. Therefore, it is difficult to detect trace hydrazine in situ, fast and low cost in room temperature. On the other hand, fluorescence-based method has been widely used to detect various analytes such as metal ions, anions and biomolecules due to its simplicity, high sensitivity, rapid response, capacity of real-time and in situ monitoring of the dynamic biological processes in living cells.9–13 However, available fluorescent probes for hydrazine are still very limited and most of them are turn-on types.14–24
As we all know, the emission intensity may be influenced by many factors, such as optical path length and the illumination intensity, which are prone to disturbance in quantitative detection. In addition, when turn-on mode fluorescent probes are used in complicated biosystems, the detection is influenced by the probe concentration, autofluorescence, and instrumental factors. A ratiometric approach can eliminate the effects of these factors and realize more effective quantitative detection through measuring the ratio of fluorescence intensities at two different wavelengths.25 On the other hand, fluorescent probes could be significantly influenced by excitation power and detector sensitivity. By comparison, colorimetric probes are more suitable for direct observation with the naked eye because they are based on absorption properties of the ground state.26–28 Up to now, very few ratiometric fluorescent and colorimetric probes toward hydrazine have been reported.29–35 Therefore, it is of great interest to design ratiometric fluorescent and colorimetric probes for hydrazine.
As an ideal ratiometric fluorescent sensing mode, fluorescence resonance energy transfer (FRET) has been widely adopted in ratiometric detection because of its facile control and basis on established theory.36 For a FRET system, the use of the ratio of two interconnected fluorescence signals as the detection index could effectively eliminate the background interference and the fluctuation of detection conditions.37,38
On the other hand, due to their small size, tunable surface functionalities and good photostability, carbon nanodots (CDs) have many excellent properties such as good water solubility, biocompatibility, excellent cell membrane permeability and low cost.39–43 Such features make CDs especially useful for fluorescent biosensing or imaging.44–48 However, exploration of CDs as fluorescent probes still remains at an early stage and no reports about CDs fluorescent probe toward hydrazine has been reported.
In this paper, we describe the first example of a FRET-based CDs–hemicyanine nanohybrid ratiometric probe toward hydrazine. In this probe, the CDs not only serve as the energy donor, but also as the anchoring site for the probe, a hemicyanine derivative. The schematic illustration for the selective detection of hydrazine by the CDs–hemicyanine probe is shown in Fig. 1. The probe based on this CDs–hemicyanine architecture demonstrates several advantages: it is a FRET-based ratiometric probe toward hydrazine which can ensure more accurate detection with a detection limit of 8 μM, and it also has a large shift (80 nm) between donor excitation and acceptor emission, which rules out any influence of excitation backscattering effects on fluorescence detection. Moreover, due to the λex-dependent PL emission of the CDs, we can readily control the emission wavelength of the donor (CDs) and allow for precise energy matching between the donor and the acceptor of the FRET system, which is beneficial to detection accuracy.
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| Fig. 1 Dual-emission fluorescence sensing of hydrazine based on a CDs–hemicyanine nanohybrid system. | |
Results and discussions
Synthesis of probe 1 and preparation of CDs
For the fabrication of the sensing system, first we synthesized amino and carboxyl coated CDs by a simple hydrothermal method using citric acid and ethylenediamine as the precursors. Fig. 2a indicates the TEM image of as-prepared CDs. Well-resolved lattice fringes are observed in high-resolution TEM (HRTEM, Fig. 2b) image. The diameter distribution of the CDs is about 2.72 nm and the zeta potential is −30.4 mV (Fig. 2c), which is ascribed to the surface negative electricity of the CDs. FT-IR spectra (Fig. S1 in ESI†) reveal that the CDs mainly contain carbon, nitrogen, oxygen, and the surfaces of the CDs are functionalized with amino, hydroxyl, and carboxylic/carbonyl moieties.
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| Fig. 2 (a) TEM image of the as-prepared CDs, (b) HRTEM image of the as-prepared CDs, (c) diameter distribution of the as-prepared CDs. | |
Hemicyanine derivative 1 was selected as the sensing unit and energy accepter, which was synthesized in a high yield starting from p-hydrazinobenzoic acid hydrochloride through three steps. The reaction of p-hydrazinobenzoic acid hydrochloride and dimethylacetone gives product 3. Compound 2 was obtained with a yield of 44.7% by the reaction of compound 3 and CH3I. The reaction of 2 and 4-diethylaminobenzaldehyde gives product 1 in a yield of 31.6%. Probe 1 was characterized by 1H NMR, 13C NMR and HRMS.
Hydrazine sensing properties
Fig. 3a and b and present the absorption and fluorescence spectra of probe 1 upon addition of hydrazine. It was clear that the absorbance at about 577 nm and emission at 610 nm decreased dramatically in the presence of hydrazine and completely disappeared when the concentration of hydrazine was up to 1 mM. The absorption and fluorescence spectra change of probe 1 by hydrazine is presumably due to the reaction of probe 1 and hydrazine. However, the emission spectrum of the CDs hardly changes upon addition of hydrazine, and the slight change was presumably due to electron/hole annihilation through effective electron or energy transfer process, which resulted from the strong electrostatic interaction between CDs and hydrazine (Fig. 3c). Prior to probe preparation, the interaction between CDs and probe 1 in the hybrid system was first investigated by monitoring their absorption and fluorescence spectra changes. As shown in Fig. 3d, the maximum absorption peak of probe 1 is at about 577 nm and the emission peak of CDs is at about 550 nm upon excitation at 530 nm. That is to say, there is a good overlap between the absorption spectrum of probe 1 and the PL spectrum of CDs, indicating that the energy transfer efficiency from CDs to probe 1 may be high. Therefore, it is possible to select a 530 nm wavelength laser to excite CDs in the hybrid probe. Upon 530 nm excitation, the emission of CDs was absorbed by probe 1 and the nanohybrid system exhibits one very strong emission peak at 610 nm and a very weak emission peak at 550 nm. To obtain a ratiometric fluorescence probe with an appropriate color variation during sensing, we prepared a mixture solution containing CDs (0.01 mg mL−1) and probe 1 (10 μM) as the probe solution for hydrazine detection.
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| Fig. 3 Absorption (a) and fluorescence (b) titration spectra of probe 1 (1.0 × 10−5 M, VDMSO/Vwater = 9/1) upon gradual addition of hydrazine from 0 to 1 mM. (c) Fluorescence spectra change of CDs (water, 0.01 mg mL−1) with excitation at 530 nm. (d) Absorption of probe 1 (1.0 × 10−5 M, VDMSO/Vwater = 9/1) (black line) and fluorescence spectrum of CDs (water, 0.01 mg mL−1) with excitation at 530 nm (red line). | |
To study the sensing properties of the CDs–hemicyanine nanohybrid system toward hydrazine, UV-Vis and fluorescence titration experiments (Fig. 4) were conducted with 0–1 mM hydrazine water solution in aqueous solution of CDs–hemicyanine nanohybrid system (Vwater/VDMSO = 1/9). Upon addition of hydrazine, the absorbance at 561 nm in the UV-Vis spectra decreased gradually with the original peak at 317 nm changing a little, and then, the peak at 561 nm reached the minimum at 100 equiv. of hydrazine (Fig. 4a). Accordingly, upon excitation at 530 nm, the emission intensity at 610 nm decreased and that at 550 nm increased with increasing hydrazine concentration (Fig. 4b). The decrease of the absorption peak at 561 nm and that at 610 nm in emission spectrum is ascribed to the reaction of hydrazine and probe 1. The increase of the emission peak at 550 nm can be explained as below: upon excitation at 530 nm and with no hydrazine, the emission at 550 nm of the CDs was mostly absorbed by probe 1 and gave a strong emission at 610 nm; with the addition of hydrazine, a new compound was obtained, which cannot absorb energy at 550 nm and no emission at 610 nm was given, thus, the emission at 550 nm increased and that at 610 nm decreased. Moreover, the solution color of 1 changed by degrees from pink to colorless in the presence of different concentrations of hydrazine (Fig. 4c). The Commission Internationale de L'Eclairage (CIE) 1931 (x, y) chromaticity diagram of the solutions after addition of different concentrations of hydrazine for 30 minutes are shown in Fig. 4d. When the hydrazine concentration was increased, the fluorescence color of the solution changed from red to orange. All of the above spectra, solution and fluorescence color change implied that probe 1 can serve as not only a highly sensitive ‘naked-eye’ probe but also a ratiometric fluorescence probe for hydrazine.
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| Fig. 4 (a) Absorption and (b) emission spectra of the CDs–hemicyanine nanohybrid system [Vwater/VDMSO = 1/9] upon titration of hydrazine water solution (0–100 equiv. to 1) with excitation at 530 nm. The reaction time is 60 min hydrazine concentration from left to right: 0 M, 1.0 × 10−4 M, 2.0 × 10−4 M, 3.0 × 10−4 M, 4.0 × 10−4 M, 5.0 × 10−4 M, 6.0 × 10−4 M, 7.0 × 10−4 M, 8.0 × 10−4 M, 9.0 × 10−4 M, 1.0 × 10−3 M. Photographs of the CDs–hemicyanine nanohybrid system [Vwater/VDMSO = 1/9] upon addition of hydrazine at various concentrations (0 M, 1.0 × 10−4 M, 2.0 × 10−4 M, 3.0 × 10−4 M, 4.0 × 10−4 M, 5.0 × 10−4 M, 6.0 × 10−4 M, 7.0 × 10−4 M, 8.0 × 10−4 M, 9.0 × 10−4 M, 1.0 × 10−3 M, from left to right) in water in daylight (c). The reaction time is 20 min. (d) CIE 1931 (x, y) chromaticity diagram of the solutions for the detection of hydrazine at different concentrations. | |
Fig. 5a suggested a good linear relationship between the ratio of I550/I610 with hydrazine concentration in the range of 0 and 1 mM, implying that hydrazine can be quantitatively detected in a wide concentration range in ratiometric fluorescence mode. From the linear calibration graph with the fluorescence titration experiment (Fig. 5a), the detection limit of probe CDs–hemicyanine for hydrazine was figured out to be about 8.0 μM based on signal-to-noise ratio (S/N) = 3.49,50 These results led us to conclude that CDs–hemicyanine nanohybrid system could be an effective ratiometric fluorescent probe for hydrazine.
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| Fig. 5 The linearity of emission intensity of the CDs–hemicyanine nanohybrid system (Vwater/VDMSO = 1/9) with respect to hydrazine concentrations. The excitation wavelength was 530 nm and the reaction time is 60 min (a). Kinetics of fluorescence change rate by the reaction of the CDs–hemicyanine nanohybrid system [Vwater/VDMSO = 1/9] and hydrazine (the concentration of hydrazine is 1.0 × 10−3 M) (b). I550 and I610 represent the emission intensity at 550 nm and 610 nm. | |
Time-dependent fluorescence experiments on the CDs–hemicyanine nanohybrid system toward hydrazine the CDs–hemicyanine nanohybrid system hydrazine is completely accomplished within 190 min and hydrazine can be detected within 60 min when the concentration of hydrazine is higher or equal to 1.0 × 10−3 M.
The sensing mechanism
The sensing mechanism was studied by mass spectra. For pure probe 1, a characteristic peak at m/z = 3777.2227 was obtained which corresponds to the species [M − I], whilst on reaction of hydrazine, the peak at 3777.2224 disappeared and one new peak appeared at m/z = 192.1499 corresponding to the species [4 + H]. Such mass spectra data confirm that compound 4 was formed through the reaction of hydrazine with probe 1 (Scheme 1).
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| Scheme 1 Synthesis of the probe 1 and the proposed mechanism of the response of 1 to hydrazine. | |
The selectivity study of the CDs–hemicyanine nanohybrid system for hydrazine
To evaluate the selectivity of the CDs–hemicyanine nanohybrid system for hydrazine, various species including some biological species (His, lle, Val, Asn, Thr, Ser, Trp, Glc, Pro, Tyr, Leu, Lys, GSH, Glu, Gly, Met, Ala, Phe, Cys), various metal ions (Na+, Mg2+, Al3+, K+, Ca2+, Cr3+, Mn2+, Fe3+, Co2+, Ni2+, Cu2+, Zn2+, Cd2+, Hg2+, Pb2+) and anions (CH3COO−, SO42−, SO32−, HS−, S2O32−, S2−, P2O74−, NO3−, N3−, I−, HSO4−, HSO3−, HPO42−, HCO3−, H2PO4−, F−, ClO4−, ClO3−, Cl−, C2O42−, and Br−) were tested. As shown in the red bars of Fig. 6, S3 and S4 in the ESI,† only the introduction of hydrazine to the CDs–hemicyanine nanohybrid system solution induced a significant fluorescence change. In the same condition, other tested species mentioned above did not induce any obvious fluorescence change to the CDs–hemicyanine nanohybrid system solution.
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| Fig. 6 Fluorescence response (red bars) of the CDs–hemicyanine nanohybrid system (Vwater/VDMSO = 1/9) upon addition of different species (100 equiv. of species relative to 1), and fluorescence changes (green bars) of the mixture of the CDs–hemicyanine nanohybrid system (Vwater/VDMSO = 1/9) and hydrazine hydrate (1 mM in water) after addition of an excess of the indicated species (100 equiv. relative to 1) (green bars). The excitation wavelength was 530 nm and the reaction time was 60 min. I550 and I610 represent the emission intensity at 550 nm and 610 nm. The species used were His, lle, Val, Asn, Thr, Ser, Trp, Glc, Pro, Tyr, Leu, Lys, GSH, Glu, Gly, Met, Ala, Phe, Cys. | |
The anti-disturbance effect study of the CDs–hemicyanine nanohybrid system for hydrazine detection
To further assess its utility as a hydrazine-selective ratiometric fluorescent probe, its fluorescence spectral response to hydrazine in the presence of other species mentioned above (green bars of Fig. 6, S3 and S4†) was also tested. The results demonstrated that all of the selected species have no interference in the detection of hydrazine except some metal ions such as Mg2+, Al3+, Ca2+, Cr3+, Fe3+, Co2+, Cu2+, Zn2+, Cd2+, Hg2+ and Pb2+. This result strongly indicates that the CDs–hemicyanine nanohybrid system could be an excellent ratiometric fluorescent probe towards hydrazine with strong anti-interference ability.
Experimental section
Materials and methods
p-Hydrazinobenzoic acid hydrochloride, dimethylacetone, CH3I, AcOH, AcONa, 4-diethylaminobenzaldehyde, His, lle, Val, Asn, Thr, Ser, Trp, Glc, Pro, Tyr, Leu, Lys, GSH, Glu, Gly, Met, Ala, Phe, Cys, NaCl, MgCl2, AlCl3, KNO3, CaCl2, CrCl3, MnCl2, FeCl3, CoCl2, NiCl2, CuCl2, ZnCl2, CdCl2, HgCl2, Pb(NO3)2, CH3COONa, Na2SO3, NaHS, Na2S2O3, NaS2, Na4P2O7, NaN3, KI, NaHSO4, NaHSO3, Na2HPO4, NaHCO3, NaH2PO4, NaF, NaClO4, NaClO3, Na2C2O4, and KBr. All commercial grade chemicals and solvents were purchased and were used without further purification. Mass spectra were obtained on high resolution mass spectrometer (IonSpec4.7 Tesla FTMS-MALDI/DHB). 1H and 13C NMR spectra were recorded on a Bruker 400 NMR spectrometer. Chemical shifts are reported in parts per million using tetramethylsilane (TMS) as the internal standard. All spectral characterizations were carried out in HPLC-grade solvents at 20 °C within a 10 mm quartz cell. UV-Vis absorption spectra were measured with a TU-1901 double-beam UV-Vis spectrophotometer. Fluorescence spectroscopy was determined on a Hitachi F-4600 spectrometer. Fourier transform infrared spectroscopy (FTIR) was performed on a NEXUS-470 spectrometer at frequencies ranging from 400 to 4000 cm−1. Samples for transmission electron microscopy (TEM) analysis were prepared by drying a colloidal solution of nanoparticles on amorphous carbon-coated copper grids. Low-resolution TEM were operated on a JEOL-JEM 2100 transmission electron microscopy operated at 200 kV. High resolution TEM (HRTEM) were carried out on a JEOL-JEM 2100F field emission transmission electron microscope operated at 200 kV. The particle size and zeta potential of the CDs (0.5 mg mL−1) were recorded on a zetasizer (Nanoplus-3, Micromeritics, the United States).
Probe 1 was synthesized according to Scheme 1. Compounds 3 and 2 were obtained following the recently reported method.51
Synthesis of compound 2. Compound 3 (1.0 g, 4.93 mmol) and CH3I (700 mg, 4.93 mmol) were dissolved in 10 mL acetonitrile. The mixture was refluxed for 12 hours and then allowed to cool to room temperature. By filtration of the above mixture, the solid was obtained as product 2 (0.76 g, 44.7%): 1H NMR (400 MHz, DMSO-d6, TMS): δH 8.38 (s, 1H), 8.19 (d, 1H), 8.03 (d, 21H), 4.00 (s, 3H), 2.82 (s, 3H), 1.57 (sd, 6H). 13C NMR (100 MHz, DMSO-d6): δC 199.48, 166.95, 142.42, 141.72, 132.04, 130.83, 124.68, 115.85, 54.72, 35.52, 21.96, and 15.12.
Synthesis of probe 1 (ref. 52). Compound 2 (690 mg, 2.0 mmol), and 4-diethylaminobenzaldehyde (354 mg, 2.0 mmol) were dissolved in 10 mL ethanol. The mixture was refluxed for 3 h at 80 °C and cooled to room temperature. The final product (probe 1, 318.6 mg, 31.6%) was obtained by filtration and being washed with ethanol for three times. Characterization of 1: HRMS (EI) m/z: calcd for C24H30IN2O2 [M − I], 3777.2224; found, 377.2227. 1H NMR (400 MHz, DMSO-d6, TMS): δH 13.09 (s, 1H), 8.37 (d, 1H), 8.29 (s, 1H), 8.10 (d, 3H), 7.74 (d, 1H), 7.22 (d, 1H), 6.91 (d, 2H), 3.94 (s, 3H), 3.59 (q, 4H), 1.78 (s, 6H), 1.20 (t, 6H). 13C NMR (100 MHz, DMSO-d6): δC 180.75, 167.25, 155.57, 153.64, 146.07, 142.94, 130.86, 129.71, 123.97, 122.82, 113.55, 112.77, 104.86, 50.97, 45.09, 33.51, 26.78, and 13.08.
Preparation and characterizations of the fluorescent CDs
CDs were prepared by hydrothermal treatment of citric acid and ethylenediamine following the reported method.53–55
Absorption and fluorescence assay of hydrazine
The detection of hydrazine was performed in the mixture of DMSO and water solution (VDMSO/Vwater = 9/1) at room temperature. In a typical run, 30 μL of CDs dispersion solution (1 mg mL−1) was added into 3 mL mixed solution mentioned above in the presence of 10 μM probe 1, followed by the addition of calculated amount of hydrazine. The sensitivity and selectivity measurements were conducted in triplicate.
Conclusions
A novel ratiometric fluorescent probe containing CDs and a hemicyanine derivative was fabricated for reliable, selective, and sensitive sensing of hydrazine. The probe was built through the electrostatic attraction between negatively charged CDs and positively charged hemicyanine molecule. This nanohybrid system possesses dual emission peaks at 550 and 610 nm under a single excitation wavelength of 530 nm. The addition of hydrazine to CDs–hemicyanine nanohybrid solution results in complete fluorescence quenching of the hemicyanine derivative 1, while the orange fluorescence of CDs keeps constant. Furthermore, the CDs–hemicyanine nanohybrid system shows high selectivity toward hydrazine over other various species including some biological species, metal ions and anions.
Acknowledgements
We are grateful for the financial supports from National Natural Science Foundation of China (21601158 and U1504203), Key Laboratory of Photochemical Conversion and Optoelectronic Materials and Zhengzhou University.
Notes and references
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Footnote |
† Electronic supplementary information (ESI) available: Synthesis procedure and spectral data. See DOI: 10.1039/c6ra27844b |
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