DOI:
10.1039/D1RA08009A
(Paper)
RSC Adv., 2021,
11, 39270-39277
Hydrazone connected stable luminescent covalent–organic polymer for ultrafast detection of nitro-explosives†
Received
1st November 2021
, Accepted 24th November 2021
First published on 9th December 2021
Abstract
Developing promising luminescent probes for the selective sensing of nitro-explosives remains a challenging issue. Porous luminescent covalent–organic polymers are one of the excellent sensing probes for trace hazardous materials. Herein, fluorescent monomers 1,1,2,2-tetrakis(4-formyl-(1,1′-biphenyl))ethane (TFBE) and 1,3,5-benzenetricarboxylic acid trihydrazide (BTCH) were selected to build a novel hydrazone connected stable luminescent covalent–organic polymer (H-COP) of high stability by typical Schiff-base reaction. The N2 sorption study, BET surface area analysis, and TGA profile indicate the porosity and stability of this H-COP material. Such properties of the H-COP material enable a unique sensing platform for nitro-explosives with great sensitivity (Ksv ∼ 106 M) and selectivity up to μM. This polymer material shows attractive selectivity and sensitivity towards phenolic nitro-explosives and other common explosives among earlier reported COP-based sensors.
Introduction
Explosives detection through fluorescence quenching is a frequently used powerful tool for national security and ecological protection applications.1–3 Hazardous materials sensing at low concentration has gained significant interest to date.4–6 Nitro-explosives, such as dinitrotoluene (DNT), dinitrobenzene (DNB), 4-nitrophenol (4-NP), and picric acid (PA) are common industrial explosives in unexploded land mines and ordnance bases.7,8 Nitro-explosives are relatively rare in nature and have been introduced into the environment mainly by human activities.9–12 Some nitro-explosives are plasma and liver contaminants that could be easily taken up by human skin, lungs, and many other parts of the body.13–15 Considerably, such compounds' presence has been proven toxic for our environment. In order to minimize their chronic exposure, favorable sensing tools are highly desirable.16 Therefore, rapid and selective detection of explosive materials has become a major ongoing challenge.17 In the past, the detection study of explosives was sticky on instrumental based techniques.18–20 The instruments used in the past were large, costly, non-movable, and time-consuming, which limited their use.21 Currently, the nitro-explosives fluorescence quenching has become powerful sensing tool due to simplicity, high selectivity, sensitivity and strong sensing process, over other techniques including ion-mobility spectrometry,22 gas chromatography technique coupling with mass spectrometry (GC-MS),23 surface enhanced Raman spectroscopy (SERS)24 plasma desorption-mass spectrometry (PDMS),25 energy dispersive X-ray diffraction (EDXRD),26 and several techniques of spectral imaging.27 In the last few decades, nitro-explosive detection via fluorescence quenching technique has offered a smart and favorable alternative tool since it contains more advantages over other conventional methods.27–30 From the first case study of nitro-explosives via luminescent porous material till now, a lot of efforts have been made in this field.31–34 So far, various luminescent materials have been widely used for explosive compounds detection, include metal–organic frameworks (MOFs), porous–organic frameworks (POFs) and numerous kinds of polymer hybrid materials.7,35–39
For promising sensing setups, there is a need of cost-effective, highly sensitive, and advanced luminescent probes which can reveal rapid response even at very low concentrations.40 The covalent–organic polymer (COP) based luminescent porous materials containing low weight components and all essential characteristics including high surface area, pre-designed pore parameters, well-ordered channel structure and high stability shows effective attraction in sensing field.41 The effective way for optimizing the targeted property of covalent polymers is the incorporation of individual functional groups.
Herein, we have established a novel hydrazone connected stable luminescent covalent–organic polymer (H-COP) via condensation reaction of 1,1,2,2-tetrakis(4-formyl-(1,1′-biphenyl))ethane (TFBE) and 1,3,5-benzenetricarboxylic acid trihydrazide (BTCH) units. Such binding components give potential to π-electrons, connecting sites, chemical stability, and good luminescence capabilities for promising nitro-aromatic explosives recognition. The aldehyde based ligands with strong conjugation typically used for the sensing directions and developing luminescent porous materials.42 Covalent–organic polymers with electron-rich interiors and connection sites have been proved efficient candidates for attaining excellent consequences and sensing of electron-deficient explosive materials sensing.43–45 This sagacity has been reasoned for the incorporation of hydrazone and aldehyde based units as stable luminescent groups into the polymer walls. This hydrazone linked stable luminescent covalent–organic polymer H-COP based novel sensing platform shows fascinating sensitivity and selectivity towards nitro-explosives over reported covalent–organic polymers (COPs) to date.
Experimental
Materials and methods
All the reagents were purchased of analytical grade from certified sellers and used without any further refinement. FT-IR spectra were recorded with wavelength range 4000–400 cm−1 using Bruker Alpha II spectrophotometer. The PXRD spectra obtained with Rigaku Miniflex diffractometer. Solid 13C (CP/MAS-NMR) analysis applied via Bruker Ultrashield 400wb Plus. TGA analysis was conducted via TA Q50 thermal analyzer using sample 5 mg with range of 50–800 °C at the constant heating rate of 10 °C min−1 under ambient environment. Nitrogen sorption isotherms were calculated at 77 K via BELSORP Max II equipment using relative pressure (0–1 bar), while pore size is determined via NLDFT model. Scanning electron microscopic (SEM) study was investigated with Zeiss Sigma 500 microscope. Transmission electron microscopy (TEM) was explored via Tecnai G2 F20 S-TWIN equipment functioning at an acceleration voltage of 200 kV. UV-visible spectroscopy was performed via Hitachi UH4150 spectrophotometer. Photoluminescence emission and excitation spectra were recorded at ambient temperature with a HORIBA FluoroLog-3 fluorescence spectrometer, while time-resolved decay measurements were carried on HORIBA FluoroLog-3 fluorescence spectrometer equipped with a laser of 355 nm working in time-correlated single-photon counting mode (TCSPC) with a time resolution of 100 ns.
Preparation
Synthesis of H-COP. 1,1,2,2-Tetrakis(4-formyl-(1,1′-biphenyl))ethane (TFBE) (30 mg, 0.04 mmol), 1,3,5-benzenetricarboxylic acid trihydrazide (BTCH) (13.4 mg, 0.05 mmol) anhydrous mesitylene (1.5 mL), 1,4-dioxane (1.5 mL) were charged in 10 mL vial. The vial was sonicated for several minutes to get a homogeneous solution. Then 0.2 mL of 6 M acetic acid was added. Simultaneously stirring and Ar gas bubbling were maintained for a few minutes then at once closed the vial. The vial was then kept in monitored oven at 120 °C for 72 hours. After that material was removed and left undisturbed at ambient temperature for cooling. The final resulting solid was washed with anhydrous THF, acetone, CH3OH, and 1,4-dioxane then put in a vacuum dry oven at 60 °C for one day to attain as yellow color powder.The elemental analysis was used to determine the H-COP carbon (C), hydrogen (H) and nitrogen (N) contents. The observed values of C (69.61%), N (7.88%) and H (5.10%) were comparable with corresponding theoretical values (70.15%, 13.36% and 5.05%).
Nitro-explosives sensing. In this sensing arrangement, 96 μg of H-COP was added into 3 mL quartz cuvette containing DMF then sonication was applied for achieving homo disperse suspension (32 μg mL−1). Dispersing property of the H-COP will smooth vicinal interaction among polymer and explosives. The fluorescence intensity measurement was performed at 500 nm upon excitation at 378 nm, while the sensing phenomenon was observed via explosives sequential addition (70 μL each time) from the stock solution (5.0 × 10−6 M). All sensing experiments were repeated thrice and steady results were stated.
Results and discussion
The synthesis assembly has been described in Scheme 1. The porous luminescent (H-COP) successfully synthesized via condensation reaction of 1,1,2,2-tetrakis(4-formyl-(1,1′-biphenyl))ethane (TFBE) and 1,3,5-benzenetricarboxylic acid trihydrazide (BTCH).
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| Scheme 1 The H-COP synthesis assembly. | |
In polymer skeleton, monomers condensation reaction confirmation and imine linkage primarily determined through Fourier transform-infrared spectroscopy (FT-IR). There is a solid band around 1695 cm−1 endorsed to the aldehyde (CO) stretching vibrations (Fig. 1a), while an adjacent strong band around 3400–3300 cm−1 correspond to the vibration band of amines (Fig. 1b).46 In this H-COP framework, the absence of NH2 group and CO well stretching bands, while imine (CN) vibrational stretching band presence at 1610 cm−1, shows the reaction completion indication among both monomers. Condensation of monomers happens effectively, but still a very small band around 1650 cm−1 is observable, attributed to the certain unreacted aldehydes in the COP setup (Fig. 1c). According to literature studies, the H-COP also possess a one wide diffraction peak in PXRD spectrum at 20°, shows the low crystallinity of the framework (Fig. S1†).36,47,48
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| Fig. 1 FT-IR spectra (a) 1,1,2,2-tetrakis(4-formyl-(1,1′-biphenyl))ethane (TFBE) (b) 1,3,5-benzenetricarboxylic acid trihydrazide (BTCH) and (c) H-COP. | |
The H-COP synthesis further validation was carried through 13C CP/MAS solid-state NMR spectroscopy. The 13C NMR spectrum shows imine carbon typical resonance signal around 156 ppm, which also confirms the bond formation among both monomers. Correspondingly, CO bond minor chemical shift can be observed around 192 ppm (Fig. S2†). This validates unreacted groups in the polymer setup, which may cause defects in the chemical structure. For AIE property investigation, fluorescence and UV-visible experiments were carried out in DMF with increased fractions of water.49–52 There is no obvious change in absorption and emission spectra of H-COP after addition of different fractions of water (Fig. S3†). The pH of H-COP was measured before and after the addition of water in the DMF solution, which changed from 6 to 7. The photo-physical features study shows that H-COP has no AIE effect. The luminogenic status of H-COP was also investigated after exposure to different solvents for one week. There is a slight difference in fluorescence peak heights even after one week of treatment in different chemical environments (Fig. S4†). The H-COP permanent porosity was observed through N2 sorption analysis at 77 K. The pore size distribution analysis of H-COP was measured through non-local density functional theory (NLDFT).53–55 The H-COP experimental pore sizes were centered at 0.755 nm and 1.919 nm, correspond to micro-pores (Fig. 2b). Afterwards, the method of Barrett, Joyner and Halenda (BJH) applied to endorse the micro-pores existence and displays worthy consent with pore size calculation via NLDFT method. The H-COP surface area was determined via BET model. The H-COP experimentally calculated surface area is 164 m2 g−1, indicates the porous framework (Fig. 2a).
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| Fig. 2 The H-COP (a) N2 sorption isotherms and (b) pore size distribution calculation. | |
The common characterization techniques scanning electron microscopy (SEM) and transmission electron microscopy (TEM) were used to expose H-COP surface morphology. Different magnification images were used to explain the morphology of the H-COP. The H-COP lower and higher magnification images of SEM and TEM display identical porous nano-scale structure with average size of 15–25 nm (Fig. 3a–d).
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| Fig. 3 (a–d) The H-COP Different magnification SEM, TEM images. | |
Stability
In order to investigate the H-COP chemical stability, the H-COP material was exposed to different chemical environments for more than one week including open-air, different solvents (acetonitrile, ethanol, HCl (3 M), HNO3 (3 M) and tetrahydrofuran), different temperatures and pH, then run for FT-IR analysis. The FT-IR chemical studies show that all the peaks possess unaltered positions and imine bond (CN) except for higher basic pH and HNO3 acid which shows slight imine bond peaks. The H-COP is chemically stable and retains its unique porous structure even after treatment with different environments (Fig. S5a–c†). The H-COP possesses a low crystalline structure; hence, PXRD measurements were not performed for these different environments. To examine the H-COP thermal stability, thermo-gravimetric (TGA) analysis and heating at different temperatures was conducted. The TGA profile of H-COP shows the thermal stability up to 300 °C, and loss of weight mainly occurs around 400 °C because of framework decay or carbonization (Fig. S6†), while spectra measured at different heating temperatures also shows that H-COP starts losing some peaks at elevated temperatures and endows that high temperature analysis destroy this framework.
Nitro-explosives sensing study
The hydrazone and aldehyde units based luminescent H-COP provides fluorescent channels enrich with π-electrons and act as an exceptional fluorescent sensor. The hydrazone unit possesses favorable complementary hydrogen-bonding active sites for guest probe molecules. These kind of binding interactions can aid in fluorescence-quenching phenomenon and contribute to host guest probes selective sensing.46,56 Similarly aldehyde and hydrazone units provide platform for different interactions like π–π, electron transfer and energy transfer. Such important features of H-COP encourage us to investigate the sensing properties of explosives. Picric acid (PA), 4-nitrophenol (4-NP), 1,3-dinitrobenzene (DNB), and 2,4-dinitrotoluene (DNT) were chosen to examine H-COP sensing capability towards common explosives. Due to the well dispersion of polymer and selected explosives good solubility, all the sensing experiments were carried out in the DMF media. A suitable excitation wavelength 378 nm was selected for the H-COP through spectrophotometer. At ambient conditions, the H-COP luminescence spectra show intense emission centered at 500 nm when excited by 378 nm UV-light. The H-COP detection behavior was investigated via luminescence-quenching titration phenomenon with explosives addition each time (70 μL) to the H-COP suspension Fig. 4a–d, S9 & S10.† Hence proves that H-COP fluorescence intensity depends mainly on the concentration of the analyte; the H-COP fluorescence intensity decreases as the nitro explosives concentration increases.
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| Fig. 4 H-COP luminescence-quenching titrations spectra while sequential addition (a) PA and (b) 4-NP. Stern–Volmer (S–V) plot calculations for H-COP with (c) PA and (d) 4-NP. | |
Moreover, for various nitro explosive analytes, the quenching response also varies.
The quenching mechanism for this COP was explained via Stern–Volmer equation (I0/I) = 1 + Ksv[Q], while Ksv = Kq τ0.57 Here I0 and I indicate probe luminescence intensities, before and after addition of quenching analyte, Ksv indicates Stern–Volmer constant (M−1) while [Q] stands for molar concentration of quenching analyte, Kq denotes quenching constant (M−1 s−1) and τ0 is the lifetime of excited state fluorescence without quenching probe. For Stern–Volmer graph, if the relationship between I0/I and [Q] comes linear, then the value of Ksv is calculated from the slope value. Most of the cases, the relationship between I0/I and [Q] possess linear deviation. The linear S–V plot suggests quenching mechanism is dynamic while deviation from linearity suggests that either its static quenching or simultaneously combination of the static and dynamic quenching.58 During static mechanism of quenching, complex formation arises among quenching analyte and sensor probes in ground state, while the transfer of electron takes place between quenching probes and sensors in the excited state during dynamic quenching.59 As presented above, at different concentration attained S–V graph shows very slight non-linear behavior and suggests involvement of either energy or electron transfer.
As shown above in Fig. 4a–d, S9 & S10,† the Ksv values were calculated by general Stern–Volmer equation. The calculated Ksv values for PA, P-NP, 1,3-DNB, and 2,4-DNT are 2.5 × 106, 3.8 × 106, 2.1 × 106 and 1.5 × 106, respectively. The sensitivity has direct relationship with Ksv and Kq values. If the Ksv value is larger, then it shows greater sensitivity and more interactions among the H-COP and nitro-explosive analytes. The calculated Kq values for PA, 4-NP, DNB, and DNT are given 0.94 × 1015, 1.43 × 1015, 0.79 × 1015 and 0.56 × 1015, respectively. The obtained higher Kq value assures higher quenching rate for COP sensor.60 The attained Ksv and Kq values for all tested common explosives are greater than reported COP based chemo-sensors till now (Tables S1 & S2†). Both cases followed the same order for Ksv and Kq (4-NP > PA > DNB > DNT).
The H-COP structure is more selective towards nitro-phenolic compounds than other common explosives and non-explosives. The reason is the existence of hydrogen-bonding among guest explosive analytes hydroxyl group, and imine bond of H-COP. This kind of ground state complex formation also aids in quenching.61 Remarkably, our luminescent material shows fascinating and comparable sensitivity values for PA and 4-NP among previously reported polymer sensors. Furthermore, the detection limit was obtained via IUPAC recommended method (3σ/slope). Here (σ) represents standard deviation and assessed through blank sample H-COP/DMF suspension fluorescence intensity, while slope (m) value was determined via fluorescence intensity calibration curve against nitro explosive different concentrations (Fig. S7–S10†). Extraordinarily, the H-COP detection limit in DMF solution for PA, P-NP, DNB, and DNT is able to reach 0.17, 0.13, 0.18, and 0.25 μM, respectively.
In order to explain the H-COP sensing selectivity, the quenching efficiency against common nitro-explosives and non-explosives were also tested at different concentrations 2.27 × 10−6 M to 2.27 × 10−4 M, wherein the quenching % calculations were done through
Quenching% = (I0 − I)/I0 × 100 |
given equation.
23
As discussed above I0 and I represent probe luminescent intensities, calculated before and after quencher analytes addition. The non-explosive aromatic compounds concentration was adjusted 100 times greater than explosive aromatic compounds. As demonstrated above nitro explosives sequential addition to the H-COP/DMF suspension causes obvious reduction in the luminescence intensities of H-COP. Therefore, quenching percentage increases with the increasing nitro-explosive compounds concentration PA (92.50%), 4-NP (93.07%), DNB (89.84%), and DNT (85.0%) (Fig. 5a and b).
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| Fig. 5 The H-COP (a) quenching efficiency (%) against various concentrations of nitro explosive analytes. (b) Luminescence-quenching efficiency towards common explosives and non-explosives. | |
However, similar conditions non-explosive aromatic compounds addition (1.14 × 10−5 M to 2.27 × 10−4 M) to the suspension of H-COP/DMF, very slight change occurs (Fig. S11†). The calculated quenching % for dibromo-benzene (DBB) and methyl benzene (MB) was 10% and 12.2%, respectively (Fig. 5b), which demonstrates H-COP shows more attractive quenching efficiency towards explosive analytes over non-explosive analytes.
The H-COP effective quenching response may be due to electron enrich core ability to transfer electrons, the ability of nitro explosives to absorb energy and host–guest attraction forces. In particular, the well conjugated structure of aldehyde units facilitates nitro explosives quenching via π–π stacking interactions in a well-ordered system.62 The attained results showed that H-COP provides a unique chemo-sensor platform, where aldehyde units and imine binding sites work synergistically to achieve greater selectivity and sensitivity towards dangerous nitro explosives.
To validate the quenching phenomenon, the H-COP fluorescence decay was investigated at room temperature with and without quenching probe at 500 nm while using excitation wavelength 378 nm (Fig. S12†). The calculated decay time of the H-COP was 2.65 ns. Moreover, the average lifespan decay of H-COP after addition of different quenchers PA, 4-NP, 1,3-DNB, and 2,4-DNT (5.22 × 10−7 M, 350 μL from stock solution) reduces to 2.02, 1.81, 1.72, and 1.73 ns, respectively, which indicates typical dynamic quenching for H-COP (Table S3†).
The theoretical calculations for H-COP and selected nitro-explosives were also explored to validate the mechanism through Gaussian 09W (Fig. 6b).63 The effective quenching happens, when the framework conduction band is at a higher energy level than the LUMOs of the quenching analytes (Table S4†).64–67 DFT calculations for H-COP show that excited electrons transferred from the conduction band of H-COP to the LUMOs of the nitro-explosives.
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| Fig. 6 (a) The H-COP HOMO–LUMO structures. (b) HOMO–LUMO calculations for H-COP and nitro-explosives. | |
On the other hand, the fluorescence resonance energy transfer (FRET) hardly contributes towards quenching because of the less overlap between nitro-explosives absorption spectrums and the emission spectrum of the H-COP (Fig. 7),68 while the electron transfer enhances the quenching rate due to association of the quencher and the H-COP. In addition, very slight non-linear quenching graphs also depict a little existence of fluorescence resonance energy transfer (FRET) (Fig. 4c, d, S9b & S10b†). Hence, from the above investigations, it is clear that the PET process is more dominant in the quenching mechanism.69–71
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| Fig. 7 The UV-vis spectra of PA, 4-NP, DNT and 4-NP and excitation & emission spectra of H-COP. | |
Conclusions
In this contribution, 1,1,2,2-tetrakis(4-formyl-(1,1′-biphenyl))ethane (TFBE) and 1,3,5-benzenetricarboxylic acid trihydrazide (BTCH) monomers were chosen to build a novel luminescent polymer (H-COP) via typical Schiff-base condensation reaction. The H-COP material shows greater sensitivity for PA, 4-NP, 1,3-DNB, and 2,4-DNT with detection limit 0.17, 0.13, 0.18, and 0.25 μM, respectively. In addition, the H-COP displays exceptionally great selectivity for common nitro explosive compounds over non-explosive compounds. The quenching mechanism shows that the PET process is more dominant over the RET. Under similar conditions, the H-COP till now is superior to the formerly reported polymer luminescent based sensors. This investigation provides capable strategy for developing luminescent porous polymers with excellent potential for nitro-explosives detection.
Conflicts of interest
The authors declare no conflict of interest.
Acknowledgements
This work was supported by the National Natural Science Foundation of China (No. 92061201, 21825106, 21901234, 21905254), NSFC-Henan Joint Foundation (U12004190), the Program for Innovative Research Team (in Science and Technology) in Universities of Henan Province (19IRTSTHN022), the Central Plains Academician Fund of Henan Province (No. 22180017), the Key Scientific and Technological Project of Henan Province (202102210027) and Zhengzhou University.
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Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra08009a |
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