Shuai
Sun
ab,
Chao-Qin
Han
*b,
Jia-Xin
Guo
ab,
Lei
Wang
b,
Ze-Yang
Wang
a,
Gonghao
Lu
*a and
Xiao-Yuan
Liu
*b
aSchool of Chemical Engineering, University of Science and Technology Liaoning, 185 Qianshan Zhong Road, Anshan, 114051, P. R. China. E-mail: ghlu@ustl.edu.cn
bHoffmann Institute of Advanced Materials, Shenzhen Polytechnic University, 7098 Liuxian Blvd, Nanshan District, Shenzhen, 518055, P. R. China. E-mail: hancq_lv@szpu.edu.cn; liuxiaoyuan1989@szpu.edu.cn
First published on 3rd December 2024
The development of covalent organic frameworks (COFs) with efficient photocatalytic H2O2 generation and building the structure–performance relationships are essential to rationally design and construct COFs for photocatalysis. Herein, COFs with kgm and fes underlying nets were successfully prepared via tuning the side-chain length of organic building units to investigate topological effects on H2O2 photosynthesis. We found that an ethoxy group-based fes COF, HIAM-0023 (HIAM = Hoffmann Institute of Advanced Materials), exhibits a much higher H2O2 generation rate (149.5 μmol g−1 h−1) than a non-substituted kgm type COF (68.9 μmol g−1 h−1). Furthermore, an enhanced photocatalytic efficiency of 391.7 μmol g−1 h−1 is obtained using mixed-linker HIAM-0023 with 37.5% hydroxyl substitution. This work sheds light on the rational construction of COFs with controllable topologies and compositions to realize efficient H2O2 photosynthesis.
It has been reported that locations and numbers of nitrogen atoms in COFs, lengths of building units, and linkage microenvironments have shown significant effects on H2O2 generation rates of resultant COFs.21–24 For example, Jiang et al. prepared three donor–acceptor COFs using non-conjugated hydrazine linkages, partially π-conjugated imine linkages and fully π-conjugated vinylene linkages, in which the COF possessing hydrazine linkages exhibits the best photocatalytic H2O2 generation performance with a rate of 5.7 mmol g−1 h−1 and an apparent quantum efficiency of 17.5% at 420 nm.18 It has also been proven that molecular junctions in COFs can be utilized as a useful strategy to enhance the photocatalytic H2O2 production.12,25 For example, Lan et al. constructed a COF with an oxidation–reduction molecular junction, which presents a record-high yield of 276 mmol g−1 h−1 for photocatalytic H2O2 generation without sacrificial agents.12 Although great efforts have been made to investigate the structure–property relationships between COFs and their H2O2 production performances, no work has been done to investigate topological effects on the photocatalytic H2O2 generation performances of COFs. COFs with different topologies can be obtained via varying reaction conditions, such as solvents,26–28 the aging process,29 and monomer concentrations.28,30 As an alternative approach, the side-chain on the skeleton of monomers has also been considered as a useful strategy to regulate the topologies of resultant COFs.31–33
Herein, to investigate the topological influence on the activity of H2O2 photosynthesis, COFs possessing kgm and fes underlying nets were constructed using N1,N1′-(benzo[c][1,2,5]thiadiazole-4,7-diyl)bis(N1-(4-aminophenyl) benzene-1,4-diamine) (BTAPA) and terephthalaldehydes with different lengths of side chains, such as terephthalaldehyde (TPA), 2,5-diethoxyterephthalaldehyde (DETA), 2,5-dipropoxyterephthalaldehyde (DPTA) and 2,5-dibutoxyterephthalaldehyde (DBTA). The experimental results reveal that the condensation of BTAPA and TA led to the formation of a COF, HIAM-0022, with a dual-pore kgm structure, while the reactions of BTAPA with DETA or DPTA or DBTA resulted in generation of COFs with a single-pore fes structure, namely HIAM-0023, HIAM-0024 and HIAM-0025, respectively. HIAM-0023 exhibits a significantly higher H2O2 generation rate of 149.5 μmol g−1 h−1 compared to 68.9 μmol g−1 h−1 for HIAM-0022. In addition, an enhanced photocatalytic H2O2 generation performance of 391.7 μmol g−1 h−1 was realized via partial hydroxylation of HIAM-0023. This work sheds light on the rational design and synthesis of COFs with specific underlying nets and compositions to achieve enhanced photocatalytic activity.
The powder X-ray diffraction (PXRD) analysis and theoretical simulations were conducted to determine the structures and crystallinity of the four as-synthesized COFs. As shown in Fig. 1c, HIAM-0022 exhibits great PXRD patterns with peak positions at about 2.39° and 4.78°, which are very different from those for HIAM-0023 to HIAM-0025. The main peak positions for these three COFs are approximately at 4.60°, 6.51° and 9.19° (Fig. 1d–f). These results indicate that HIAM-0022 and the other three COFs possess different underlying nets. According to the PXRD patterns of these four COFs, simulations were carried out to obtain their exact structures. It should be noted that dual-pore (DP) or single-pore (SP) structures might be generated with eclipsed packing (AA) and staggered packing (AB) using such organic building units. For HIAM-0022, as depicted in Fig. 1c and g, the simulated PXRD patterns based on the DP-AA structure show excellent agreement with the experimental patterns. Meanwhile, for HIAM-0023 to HIAM-0025, the simulated PXRD patterns according to the SP-AA structures well-matched with the experimental patterns (Fig. 1d–h, e–i and f–g). Furthermore, negligible differences were observed between the profile of Rietveld refinement and experimental diffractions. As a result, HIAM-0022 possesses a kgm topology, in which the lattice parameters are a = c = 43.6752 Å, b = 3.4977 Å, α = β = 90° and γ = 59.2° with final Rwp and Rp values of 3.77% and 4.39%. HIAM-0023, HIAM-0024 and HIAM-0025 possess a fes underlying net. The unit cell parameters are: a = 32.2745 Å, b = 29.3605 Å, c = 4.7628 Å, α = γ = 90°, and β = 91° with final Rwp and Rp values of 3.28% and 4.39% for HIAM-0023; a = 30.7571 Å, b = 32.7385 Å, c = 4.6603 Å, α = γ = 90°, and β = 90° with final Rwp and Rp values of 3.56% and 4.80% for HIAM-0024; a = 31.7806 Å, b = 32.2379 Å, c = 4.4875 Å, α = γ = 90°, and β = 90° with final Rwp and Rp values of 4.46% and 6.09% for HIAM-0025.
Fourier-transform infrared (FTIR) spectra were used to confirm the formation of the C
N band. As depicted in Fig. 2a and Fig. S7 (ESI†), these four COFs show a characteristic C
N stretching band around 1631 cm−1. The vibration of the NH2 group (∼3450 cm−1) in BTAPA and the aldehyde stretching (∼1695 cm−1 for TPA, ∼1680 cm−1 for DETA, ∼1683 cm−1 for DPTA and ∼1678 cm−1 for DBTA) were largely attenuated after condensation reactions. These results indicated a high degree of polymerization and the generation of imine bonds. The solid-state 13C NMR spectra of these four COFs were also measured. The signals are around 153 and 155 ppm (Fig. S8, ESI†), which correspond to the C atom in the C
N bonds, further indicating the formation of HIAM-0022 to HIAM-0025. The morphologies and compositions of the four COFs were analysed using scanning electron microscopy (SEM) and energy dispersive X-ray spectroscopy (Fig. S9–S13, ESI†). The CO2 adsorption–desorption analysis was performed to evaluate the porosity of HIAM-0022 and HIAM-0025. As depicted in Fig. S14 (ESI†), HIAM-0022 and HIAM-0025 show Type I isotherms with surface areas of 129.25, 556.82, 430.26 and 260.69 m2 g−1 using the Brunauer–Emmett–Teller (BET) model. The corresponding pore size distributions are around 0.53 and 0.70 nm for HIAM-0022 and 0.83 nm for the other three COFs. These results further demonstrate the DP-AA structure for HIAM-0022 and the SP-AA structures for HIAM-0023 to HIAM-0025.
The chemical and thermal stabilities of HIAM-0022 to HIAM-0025 were analysed, which is essential for their practical applications. For HIAM-0022, the excellent agreement of the PXRD patterns of HIAM-0022 before and after treatment under various conditions (including in water at room temperature, pH = 4, 10 and 12 aqueous solutions for 24 hours) indicated its high chemical stability (Fig. S15a, ESI†). Meanwhile, under much harsher conditions, such as boiling water and pH = 2 aqueous solution, the long-range order of HIAM-0022 could be gradually broken. However, almost no changes were recorded for the PXRD patterns of HIAM-0023 to HIAM-0025 under all these tested conditions (Fig. S15b–d, ESI†), which demonstrate that the long-range orders of HIAM-0023 to HIAM-0025 were maintained very well. The well-matched FT-IR spectra before and after various treatments also indicate the high chemical stability of HIAM-0022 to HIAM-0025 (Fig. S16, ESI†). Thermogravimetric analysis (TGA) reveals that these four COFs exhibit excellent thermal stability up to about 460 °C for HIAM-0022 and about 400 °C for the other three COFs (Fig. S17, ESI†).
Encouraged by the excellent chemical stability and suitable electronic structures for O2 reduction and H2O oxidation of HIAM-0022 to HIAM-0025 (Fig. 2d), their photocatalytic activities toward H2O2 generation were explored without adding any sacrificial reagents in water and air under Xe lamp irradiation (λ > 420 nm). As depicted in Fig. 3a, among these four COFs, HIAM-0023 exhibits the best catalytic efficiency for H2O2 photosynthesis compared with the other three COFs with H2O2 generated rates of 68.9, 149.5, 86.1 and 70.1 μmol g−1 h−1 for HIAM-0022, HIAM-0023, HIAM-0024 and HIAM-0025, respectively. To gain a deep understanding about the H2O2 generation mechanism, a series of control experiments were carried out using HIAM-0023. The photocatalytic H2O2 generation rates in the O2 and N2 atmospheres were 182.7 and 44.1 μmol g−1 h−1 (Fig. 3b), respectively, suggesting that photocatalytic H2O2 evolution governed by the 2e− O2 reduction reaction and water oxidation reaction hardly contributes to H2O2 generation. As shown in Fig. 3c, H2O2 generation rates obviously decreased to 59.3 and 65.0 μmol g−1 h−1 when benzoquinone (BQ, trapping agent of ˙O2−) and NaBrO3 (trapping agent of electrons) were added into the photocatalytic system, respectively. When tert-butanol (TBA, trapping agent of ˙OH) was added, an increased rate of 226.5 μmol g−1 h−1 was obtained, which illustrates that ˙OH did not participate in the photocatalytic reaction system. Similarly, an enhanced performance was recorded when methanol was added as a sacrificial reagent like TBA. The 2e− O2 reduction reaction was further confirmed by the electron paramagnetic resonance (EPR) experiment, where the typical characteristic signals for ˙O2− are observed under visible-light irradiation for HIAM-0023 (Fig. 3d).
The amount of generated H2O2 gradually increased with continuous irradiation and reached up to 2.94 mmol after 8 hours (Fig. 3e). The resultant H2O2 solution can be directly used to degrade rhodamine. The color of rhodamine solution became faint in a few seconds and eventually turned colorless (Fig. S20a, ESI†), which was confirmed by the significant decrease in the UV-vis absorption spectra of rhodamine solution (Fig. S20b, ESI†). The generation efficiency of H2O2 was gradually reduced after three cycles, which might be ascribed to the loss of COFs during recovery (Fig. 3f). After the photocatalytic reaction, no significant change was recorded for the PXRD patterns and FT-IR spectra of HIAM-0022 to HIAM-0025 (Fig. S21 and S22, ESI†), which further indicated their high stability for practical applications.
:
6.4, 1
:
2.06, 1
:
1.19 and 1
:
0.42 for HIAM-0023-12.5%, HIAM-0023-25.0%, HIAM-0023-37.5% and HIAM-0023-50.0%, respectively. The UV-vis spectra were recorded with a gradual blue-shift with the increased concentration of DHTA (Fig. 4d), with which the Eg values of HIAM-0023-12.5%, HIAM-0023-25.0%, HIAM-0023-37.5% and HIAM-0023-50.0% were calculated to be 1.67, 1.75, 1.88 and 1.97 eV, respectively (Fig. S29, ESI†). According to the Mott–Schottky plots (Fig. S30, ESI†), the corresponding flat band potentials were estimated to be −0.96, −0.90, −0.89 and −0.84 V (vs. Ag/AgCl). Then, the ECB levels were determined to be −0.74, −0.68, −0.67 and −0.62 V (vs. NHE). Consequently, the EVB levels were estimated to be 0.94, 1.07, 1.21 and 1.35 V (vs. NHE) as shown in energy band structure diagrams in Fig. 4e for HIAM-0023-12.5%, HIAM-0023-25.0%, HIAM-0023-37.5% and HIAM-0023-50.0%, respectively. The porosity and pore size distribution of HIAM-0023-X% were evaluated using CO2 adsorption–desorption analysis (Fig. S31, ESI†).
Under the same test conditions as HIAM-0023, the photocatalytic H2O2 generation rates were determined to be 264.0, 307.3, 391.7 and 246.0 μmol g−1 h−1 for HIAM-0023-12.5%, HIAM-0023-25.0%, HIAM-0023-37.5% and HIAM-0023-50.0% (Fig. 5a), respectively, which are much higher than that of HIAM-0023. The highest photocatalytic activity of HIAM-0023-37.5% might be ascribed to its better charge separation ability as confirmed by its higher transient photocurrent response compared with the other three COFs (Fig. S32, ESI†). The H2O2 generation rate was slightly increased to 506.3 μmol g−1 h−1 in pure O2 and remarkably decreased to 40.1 μmol g−1 h−1 in pure N2 for HIAM-0023-37.5% (Fig. 5b), indicating that H2O2 evolution is a 2e− O2 reduction process. The remarkably decreased generation rates were recorded for HIAM-0023-37.5% when BQ and NaBrO3 were added into the photocatalytic system, which increased to 474.9 and 436.6 μmol g−1 h−1 with TBA and methanol as sacrificial reagents (Fig. 5c). The 2e− O2 reduction reaction using ˙O2− as the intermediate was confirmed by the EPR experiment (Fig. 5d). Although the photocatalytic performances of these COFs are lower than those reported in most works (Table S6, ESI†), the main aim of the present work has been achieved to investigate topological effects on the photocatalytic efficiency of resultant COFs.
To have a further understanding about the mechanism for H2O2 generation, the ORR and WOR processes were investigated through rotating disk electrode (RDE) and rotating ring-disk electrode (RRDE) experiments. RDE analysis indicated that the average electron transfer numbers for HIAM-0023-12.5%, HIAM-0023-25.0%, HIAM-0023-37.5% and HIAM-0023-50.0% were determined to be 2.27, 2.01, 2.10 and 2.13 in the oxygen reduction reaction, respectively (Fig. 5e and Fig. S33, S34, ESI†). In the RRDE experiments, weak reduction currents were observed when the Pt ring electrode was set at −0.23 V (Fig. 5f), illustrating that these four COFs can generate O2 in the WOR process. Meanwhile, no oxidation current was recorded when the Pt ring electrode was set at 0.6 V (Fig. S35, ESI†), which demonstrates that no H2O2 can be generated. Based on the aforementioned results, it is clear that the photocatalytic H2O2 generation process is the combination of the 2e− oxygen reduction reaction and one-step 4e− water oxidation.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4tc03991b |
| This journal is © The Royal Society of Chemistry 2025 |