Wanyi
Zhao
a,
Ce
Xing
a,
Yuwei
Zhang
*a,
Juntao
Ren
*b and
He
Li
*b
aLaboratory of Preparation and Applications of Environmental Friendly Materials (Jilin Normal University), Ministry of Education, Changchun, 130103, China. E-mail: yw_zhang@jlnu.edu.cn
bDivision of Energy Materials, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian 116023, China. E-mail: jtren@dicp.ac.cn; lihe@dicp.ac.cn
First published on 8th August 2024
Covalent organic frameworks (COFs) are a novel type of nanoporous and crystalline polymers with a precise and highly conjugated skeleton, making them promising candidates for constructing emissive materials. However, the strong high conjugation structures between adjacent layers easily lead to aggregation-caused quenching (ACQ) of emission properties. In this study, we have designed COFs with a flexible skeleton to suppress ACQ effects, enhancing their luminescence activity. In addition, the high density of nitrogen and oxygen atoms on these flexible walls serves as binding sites for hydrogen bonding interactions, indicating sensitivity and selectivity towards nitro-explosives. This strategy establishes a new approach for creating luminescent materials for chemical sensors.
Recently, many researchers have shown a deep interest in emissive materials due to their practical applications, such as hazardous substance detection, bioimaging, illumination, and many more.7–9 COFs maintained precise and highly conjugated skeletons, making them promising candidates for designing and producing emissive materials. However, the strong high-conjugate structures between adjacent layers can easily lead to aggregation-caused quenching (ACQ) of emissive properties.18–25 With these considerations in mind, various approaches have been employed to enhance the luminescence of COFs. Using fluorescent monomer construction materials seems to be a very simple and effective way. However, in most cases, this strategy has little to no effect, resulting in either no fluorescence or very weak fluorescence.7–9 More recently, Banerjee et al. achieved uniform nanosheets through a simple mechanical peeling method, resulting in a fluorescent chemosensor.27 Liu et al. designed a monomer with tert-butyl units to synthesize highly emissive COFs for a copper sensor with good selectivity and sensitivity.28 Another effective approach involves introducing long alkyl chains into COF channels, resulting in emissive COFs.29,30 Furthermore, utilizing multi-component building units with different alkyl chains have led to broad emission spectra, with some emission close to near-white light.31 Recently, flexible linkers have been incorporated into the COF structure, significantly influencing the luminescence properties of COFs.32 Although substantial progress has been made in all of the aforementioned areas, exploration of light-emitting COFs is also a worthwhile endeavour.
In this study, we designed flexible walls to light up COFs, significantly improving their emissive properties. The flexible unit, denoted as 4,4′,4′′-((1,3,5-triazine-2,4,6-triyl)tris(oxy))trianiline (TTTTA), serves as the vertex, while other units, such as 3-hydroxy-[1,1′-biphenyl]-4,4′-dicarbaldehyde (BP-OH-1) and 3,3′-dihydroxy-[1,1′-biphenyl]-4,4′-dicarbaldehyde (BP-OH-2), act as linkers. These components are used to construct TTTT-COF-1 and TTTT-COF-2 as illustrated in Fig. 1. In this design, the flexible channels effectively mitigate aggregation effects caused by strong conjugation between layers, leading to enhanced luminescence. Furthermore, the presence of hydroxyl groups and nitrogen atoms in the linkage results in hydrogen-bonding interactions, referred to as excited-state intramolecular proton transfer (ESIPT).33 These features contribute to the outstanding emission capability of the COFs. Notably, the high-density nitrogen and oxygen atoms within the flexible channels serve as sites for hydrogen-bonding interactions with nitro-explosives. This imparts remarkable sensitivity and selectivity towards nitro-explosives in TTTT-COFs, surpassing the capabilities of reported detectors.
The permanent porosities of TTTT-COFs were assessed through nitrogen sorption experiments conducted at 77 K. The nitrogen adsorption curves for TTTT-COF-1 and TTTT-COF-2 revealed a type-IV sorption isotherm, indicative of their mesoporous nature (Fig. S6a and S7a†). The Brunauer–Emmett–Teller (BET) surface areas were calculated to be 560 m2 g−1 for TTTT-COF-1 and 175 m2 g−1 for TTTT-COF-2, respectively. The primary pore size was predominantly centered at about 3.7 nm for both TTTT-COFs (Fig. S6b and S7b†). Mesopores could facilitate the diffusion and transport of adsorbates within the pore channels.
The crystalline nature of TTTT-COFs was confirmed through powder X-ray diffraction (PXRD) analysis. TTTT-COF-1 exhibited a strong peak at 2.16° and relatively weaker peaks at 3.82°, 5.94°, 7.84°, and 9.76° (Fig. 2a, red), corresponding to the (110), (200), (210), (220), and (220) facets, respectively. Similar results were observed for TTTT-COF-2, with distinct signals at 2.20°, 3.96°, 6.08°, 8.12°, and 10.16° (Fig. 2c, red), corresponding to the (110), (200), (210), (220), and (220) facets, respectively. After the Pawley refinement of unit cells, the AA stacking model for TTTT-COFs closely matched the observed patterns, while the AB model was not suitable. The unit cells of the AA model of both COFs are illustrated in Fig. 2b and d. The optimized simulation parameters for TTTT-COF-1 were α = β = 90°, γ = 120°, a = b = 46.5468 Å, and c = 3.5068 Å (Rwp: 5.10% and Rp: 3.85%). For TTTT-COF-2, the optimized simulation parameters were α = β = 90°, γ = 120°, a = b = 46.5355 Å, and c = 3.5045 Å (Rwp: 5.59% and Rp: 3.64%). PXRD analysis demonstrated that TTTT-COFs form a highly crystalline network.
Fig. 2 Experimental, Pawley-refined, simulated PXRD patterns and the difference plots of the PXRD patterns of (a) TTTT-COF-1 and (c) TTTT-COF-2. Unit cells of (b) TTTT-COF-1 and (d) TTTT-COF-2. |
Comparing these constructed monomers, TTTT-COFs exhibited high conjugation, as evidenced by their red-shifts in the solid absorption spectra (Fig. 3a and b). The emission properties of the TTTT-COF powder were initially assessed using fluorescence spectra. Both powders emitted yellow fluorescence with emission peaks at 548 nm (TTTT-COF-1, Fig. 3c) and 561 nm (TTTT-COF-2, Fig. 3d). The absolute fluorescence quantum yields were determined to be 12.3% and 17.63% using the integrating sphere method.
Fig. 3 Solid absorption spectra of (a) TTTT-COF-1, (b) TTTT-COF-2 and the building units. Solid fluorescence spectra of (c) TTTT-COF-1 and (d) TTTT-COF-2 (insets: photos of COFs under 365 nm). |
Explosives are known to pose a significant threat to the environment, as their release can lead to the contamination of soil and aquatic ecosystems.34,42 Nitroaromatic compounds, such as 2,4,6-trinitrophenol (TNP), 2,4-dinitrophenol (DNP), 2-nitrophenol (NP), 2,4-dinitrotoluene (DNT), 2-nitrotoluene (NT), and nitrobenzene (NB) serve as typical examples. The TTTT-COF samples exhibit excellent porosity, a mesoporous structure, and flexible channels, which provide ample space for capturing guest molecules through pore functionality. Furthermore, their strong emission capabilities suggest lower detection limits for molecule detectors. The high-density nitrogen and oxygen atoms within the flexible channels serve as hydrogen bond acceptors for nitroaromatic compounds.33,35,36 The TTTT-COF samples were simply treated with ultrasound to achieve uniform dispersion in tetrahydrofuran. Interestingly, TTTT-COF-1 exhibited a significant emission quenching response towards TNP with high efficiency at 65% (Fig. 4a and b), while the addition of other nitroaromatic compounds had little impact on their emissions (Fig. S8a–S12a†). Similarly, TTTT-COF-2 displayed good selectivity and efficiency with a 76% quenching response towards TNP (Fig. 4c and d). The high quenching efficiency is due to the blockage of the ESIPT process by hydroxyl groups and nitrogen atoms. In the presence of nitroaromatic compounds, the nitrogen and oxygen atoms serve as hydrogen bond acceptors, effectively preventing the ESIPT process and leading to significant fluorescence quenching.23,33,35 The relative lower quenching efficiencies of TTTT-COF-2 towards other compounds were obtained at 19%, 13%, 7%, 5%, and 5% for DNP, DNT, NP, NT, and NB, respectively (Fig. S8b–S12b†).
The detection limit is a crucial parameter for chemical sensors. As the concentration of TNP increased, the fluorescence intensity of both TTTT-COFs gradually decreased (Fig. 4b and d). The emission intensity and TNP concentration exhibited an almost proportional relationship at lower concentrations, resulting in a detection limit of 148 nM for TTTT-COF-1 (Fig. S13a†) and 83 nM for TTTT-COF-2 (Fig. S13b†). These values are excellent and stand out among the reported COFs.32,33,35–41,43,44
The Stern–Volmer constant (KSV) was determined for nitroaromatic compounds based on the fluorescence quenching profiles. For TTTT-COF-1, the KSV was estimated to be as high as 1.26 × 105 M−1 for TNP (Fig. S14a†), decreasing to 2.14 × 104, 1.06 × 104, 8.46 × 103, 5.51 × 103, and 4.27 × 103 M−1 for DNP, DNT, NP, NT, and NB, respectively (Fig. S15a–S19a†). A similar trend was observed for TTTT-COF-2, with a high KSV of 1.53 × 105 M−1 for TNP (Fig. S14b†). For DNP, DNT, NP, NT, and NB, the KSV values decreased to 2.23 × 104, 1.46 × 104, 7.80 × 103, 4.95 × 103, and 4.73 × 103 M−1, respectively (Fig. S15b–S19b†). The high KSV value for TTTT-COF-2 exceeds that of the reported COFs, underscoring its excellent sensing ability.32,33,35–41,43,44 The above interesting results can be attributed to their good porosity, mesoporous structure, and flexible channels. The high-density nitrogen and oxygen atoms within the flexible channels of TTTT-COFs can serve as hydrogen bond acceptors for nitroaromatic compounds.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ce00635f |
This journal is © The Royal Society of Chemistry 2024 |