Yuwei
Zhang
a,
Ce
Xing
a,
Zhibin
Tian
b,
Wanyi
Zhao
a,
Yongfeng
Zhi
*b,
Lina
Zhao
*a and
He
Li
*c
aLaboratory of Preparation and Applications of Environmental Friendly Materials (Jilin Normal University), Ministry of Education, Changchun, 130103, China. E-mail: zhaolina1975@163.com
bSchool of Chemistry and Chemical Engineering, Hainan University, Haikou, 570228, China. E-mail: zhiyf@hainanu.edu.cn
cDivision of Energy Materials, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, China. E-mail: lihe@dicp.ac.cn
First published on 18th September 2024
Covalent organic frameworks (COFs) possess versatile advantages, including their lightweight nature, exceptional stability, and having a well-defined π structure, rending them highly promising for fluorescence sensors. One of the most important factors for sensing is the presence of interaction sites, which previous research has not considered extensively. In this study, we present the synthesis of two emissive hydrazone-linked COFs (EH-COFs) under solvothermal conditions. The hydrazone linkages, which contain –NH single bond groups on the walls, reduce aggregation-caused fluorescence quenching, resulting in enhanced emission activity. Furthermore, the abundance of interaction sites (nitrogen and oxygen atoms) on the walls enables efficient interaction with guest molecules. Owing to these advantages, EH-COFs exhibited elevated sensitivity and selectivity, with low detection limits, for hydrazine sensing, ranking them among the top-performing fluorescence probes reported to date.
Compared with traditional fluorescent probes, covalent organic frameworks (COFs) have garnered significant attention due to their distinctive characteristics.8–13 COFs represent a novel class of porous organic materials renowned for their exceptional crystalline structure and uniform nano-pore architecture.14–16 These inherent advantages have propelled COFs to the forefront of materials research, attracting considerable interest across diverse applications such as substance adsorption, catalysis, and energy devices.17–38
COFs have exhibited significant advancements as fluorescent chemical sensors. In contrast to conventional chemical sensors, COFs possess a permanent pore structure, which offers abundant space for the capturing of guest molecules.8,9 Moreover, the precise pore structure and active sites in the channel facilitate targeted interactions with complex analytes.10–14 Additionally, COFs featuring π-linked structures contribute to signal amplification, which is a critical factor in trace target detection.9,29–31 Given these advantages, COFs exhibit high specificity and sensitivity, garnering widespread acclaim.32–36 Numerous studies have emphasized the effectiveness of luminescent COFs in detecting hazardous explosive molecules, metal ions, anions, and pH levels.37–49 However, conventional COFs often lack adequate detection sites, which may lead to overlooking certain analytes.
In this study, we synthesized two emissive hydrazone-linked COFs (EH-COFs, chemical structure as shown in Fig. 1) under solvothermal conditions. The design of EH-COFs was guided by several considerations. Firstly, we introduced hydrazone linkages with –NH groups on the walls, characterized by single bonds, which weaken aggregation-caused fluorescence quenching.38–42 Additionally, the incorporation of –OH groups adjacent to the Schiff-base centers facilitates intramolecular hydrogen bonding, enhancing the chemical stability of EH-COF-2.43–46 Furthermore, the abundance of nitrogen atoms and oxygen on the walls allows for interaction with guest molecules. Consequently, EH-COFs have emerged as attractive candidates for the development of novel molecular sensors. As anticipated, the EH-COFs exhibited strong crystallinity, excellent stability, high luminescence efficiency, and abundant active sites. Most notably, EH-COFs demonstrated high sensitivity and selectivity as a fluorescent probe for hydrazine sensing, attributable to their synergistic structural features.
Fig. 2 (a and b) FT-IR spectra of EH-COFs and building units. 13C NMR spectra of (c) EH-COF-1 and (d) EH-COF-2. |
We examined the porous properties of the EH-COFs using nitrogen adsorption–desorption measurements. According to the IUPAC classification, EH-COFs exhibited a combination of type-I and type-IV nitrogen sorption isotherm features (Fig. S4a and S5a†). The microporous nature was evident in the P/P0 range of 0 to 0.1, attributable to the steep increase in nitrogen uptake within this range. The Brunauer–Emmett–Teller (BET) specific surface area of EH-COF-1 and EH-COF-2 was found to be 316 and 187 m2 g−1, respectively. Both EH-COFs exhibit microporous characteristics, with pore diameters mainly distributed at 1.8 nm (Fig. S4b and S5b†).
The powder X-ray diffraction (PXRD) analysis results indicated their highly crystalline structure. EH-COF-1 exhibited PXRD peaks at 4.60°, 8.04°, 9.42°, 12.42°, and 25.86°, assigned to the (100), (110), (200), (210), and (001) facets, respectively (Fig. 3a, red). EH-COF-2 displayed PXRD peaks at 4.64°, 8.22°, 9.33°, 12.34°, and 26.05°, corresponding to the (100), (110), (200), (210), and (001) facets, respectively (Fig. 3b, red). After Pawley refinement of unit cells, the AA stacking model for EH-COFs aligned with experimental results, while the AB model failed to match. The unit crystal structures of both COFs with AA stacking model are depicted in Fig. 3c and d (a = b = 21.7401 Å, c = 3.7230 Å, α = β = 90.00°, γ = 120.00° for EH-COF-1; a = 22.9190 Å, b = 22.5673 Å, c = 3.5273 Å, α = β = 90.43°, γ = 122.13° for EH-COF-2).
Fig. 3 PXRD patterns of (a) EH-COF-1 and (b) EH-COF-2. Top views of the AA stacking structure for (c) EH-COF-1 and (d) EH-COF-2. |
The stability of COFs is a crucial factor in their functional exploration. We assessed the chemical stability of EH-COF samples by exposing them into various solvents, including water, N,N-dimethylformamide, ethanol, 1 M HCl, and 1 M NaOH, for 24 hours at room temperature. Remarkably, EH-COF-1 and EH-COF-2 samples maintained strong PXRD patterns at their original positions after treatment, indicating that the excellent crystallinity of these two COFs is well-preserved under harsh conditions (Fig. S6†). Additionally, the FT-IR spectra of the COFs after treatment showed consistent vibration information across all samples (Fig. S7†). These results suggest that EH-COFs exhibit good chemical stability, which is essential for their functionalization and practical application. The ability to retain crystallinity and structural integrity under various chemical conditions underscores the robustness of EH-COFs, making them suitable for diverse environments and enhancing their potential applications.
The EH-COF-1 powder exhibited an electronic absorption band around 375 nm (Fig. 4a, black), which showed a red-shift compared to its building units. Similar results were found for EH-COF-2 with an absorption band at 390 nm (Fig. 4b, black). Additionally, the EH-COF-2 exhibited a highly conjugated skeleton owing to the presence of hydroxyl groups and nitrogen atoms, which resulted in hydrogen-bonding interactions. The EH-COF-1 displayed blue emission at 460 nm (Fig. 4c) when excited at 383 nm (Fig. S8a†) in the solid state. In contrast, the EH-COF-2 exhibited yellow fluorescence with an emission peak at 590 nm (Fig. 4d) when excited at 392 nm (Fig. S8b†).
Fig. 4 Solid spectra of (a and b) EH-COFs and building units in the solid state. Fluorescence spectra of (c) EH-COF-1 and (d) EH-COF-2 in the solid state (inside their images under 365 nm). |
EH-COF-1 and EH-COF-2 samples were dispersed in Phosphate Buffer Saline (PBS) buffer, which was applied to detect hydrazine (N2H4, 20 mM, pH = 7.4). In addition, EH-COFs kept stable in PBS buffer solutions under different conditions confirmed via the FT-IR and PXRD analysis in Fig. S9.†Fig. 5a and b show the fluorescence emission spectra of EH-COFs sample suspensions after adding different concentrations of hydrazine solution (0–10 μM). Surprisingly, when hydrazine was mixed with the EH-COFs in PBS buffer suspension, the fluorescence intensity of the original material was significantly quenched. For example, the fluorescence quenching degrees of EH-COF-1 and EH-COF-2 decreased by 73% and 67%, respectively. A good linear relationship was observed between the fluorescence intensity of EH-COFs and lower hydrazine concentration in Fig. 5c and d. The detection limit was estimated from the lower hydrazine concentration, which was down to 51 nM and 28 nM for EH-COFs, respectively, ranking as the best performance among reported COFs and metal–organic frameworks (Table S1†).50–55 Additionally, the fluorescence quenching efficiency of the EH-COFs sensor can be nearly fitted to the Stern–Volmer equation, I0/I = Ksv × [Q] + 1, which relates the fluorescence intensity, where I0 and I are the fluorescence intensities in the absence and presence of a quencher, respectively. [Q] represents the hydrazine concentration and Ksv is the quenching constant. According to the fluorescence titration of EH-COFs with hydrazine, a near curvier Stern–Volmer plot was obtained with a Ksv value of 2.3 × 105 M−1 (Fig. S10†). The results indicate an excellent sensitivity towards hydrazine detection owing to the active sites on the walls of EH-COFs.
To gain a deeper understanding of the quenching mechanism, we investigated the fluorescence lifetime of EH-COF with and without hydrazine (Fig. 5e and f). The fluorescence lifetime of EH-COF-1, which was initially 1.4 ns, was reduced to 1.3 ns in the presence of hydrazine. Similarly, the fluorescence lifetime changed from 1.5 to 1.3 ns of EH-COF-2 with the addition of hydrazine. These results suggest that a photoinduced electron transfer (PET) process is responsible for the fluorescence quenching of EH-COFs.
Selectivity is crucial for sensors. To evaluate the sensing performance of EH-COFs under different acidic and alkaline conditions, we investigated the effect of pH on the fluorescence intensity of EH-COFs. As illustrated in Fig. 6a and b, within the pH range of 4 to 10, the fluorescence intensity of EH-COFs remained almost unchanged, indicating excellent pH stability. Upon the addition of hydrazine, the fluorescence intensity of the EH-COFs exhibited only slight fluctuations within this pH range, with a minimal decrease observed under strong acidic and alkaline conditions. This suggests that EH-COFs demonstrate robust stability and can be effectively utilized for hydrazine detection across a wide range of acidic and alkaline environments.
Fig. 6 Quenching efficiency of (a) EH-COF-1 and (b) EH-COF-2 under different pH values. Quenching efficiency of (c) EH-COF-1 and (d) EH-COF-2 with hydrazine and different ions. |
We further considered the potential interference from metal ions and anions. To explore the anti-interference and specific recognition properties of EH-COFs for hydrazine sensing, we selected common metal cations and anions as interference components. After adding these various interference components (as depicted by the orange bars in Fig. 6c, d and Fig. S9, S10†), the fluorescence emission intensity of EH-COFs remained almost unchanged, indicating minimal response to these common interference components. However, upon the addition of hydrazine (depicted by the green bars in Fig. 6c and d), there was a significant decrease in fluorescence intensity. This demonstrates the high sensitivity and specific recognition capability of EH-COFs for hydrazine detection. These results suggest that EH-COFs exhibit excellent selectivity for detecting hydrazine, maintain stability across a wide pH range and demonstrate minimal interference from common metal ions and anions.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4py00815d |
This journal is © The Royal Society of Chemistry 2024 |