Guang-Bo
Wang‡
a,
Hai-Peng
Xu‡
a,
Ke-Hui
Xie
a,
Jing-Lan
Kan
a,
Jianzhong
Fan
b,
Yan-Jing
Wang
a,
Yan
Geng
*a and
Yu-Bin
Dong
*a
aCollege of Chemistry, Chemical Engineering and Materials Science, Collaborative Innovation Center of Functionalized Probes for Chemical Imaging in Universities of Shandong, Key Laboratory of Molecular and Nano Probes, Ministry of Education, Shandong Normal University, Jinan 250014, P. R. China. E-mail: gengyan@sdnu.edu.cn; yubindong@sdnu.edu.cn
bSchool of Physics and Electronics, Shandong Normal University, Jinan 250014, P. R. China
First published on 6th January 2023
Covalent organic frameworks (COFs), featuring semiconductor-like behavior, have recently garnered widespread interest for applications in photocatalysis by virtue of their well-defined and tailorable porous structures, high surface areas and excellent chemical stability. A facile strategy for designing COFs exerting efficient charge transfer and separation as well as suppressing charge carrier recombination is the precise integration of electron-donating and electron-withdrawing moieties to form long-range ordered donor–acceptor (D–A) type structures. In this work, we rationally designed and synthesized a novel imine-linked COF (DABT-Py-COF) by the condensation of a newly designed D–A–D type monomer of 4,4′,4′′,4′′′-(benzo[c][1,2,5]thiadiazole-4,7-diylbis(9,9-dimethyl-9,10-dihydroacridine-10,2,7-triyl))tetrabenzaldehyde and 1,3,6,8-tetrakis(4-aminophenyl)pyrene under solvothermal conditions. Remarkably, the obtained DABT-Py-COF exhibited outstanding and steady hydrogen production with a maximum hydrogen evolution rate (HER) of 5458 μmol g−1 h−1 under visible-light irradiation (AM 1.5). This work has paved the way for the rational design and preparation of more efficient D–A type COFs for photocatalysis.
Covalent organic frameworks (COFs), as a burgeoning family of advanced crystalline porous materials that allow the atomically precise assembly of different building units into extended two-dimensional (2D) or three-dimensional (3D) frameworks with periodically ordered skeletons,7 have received increasing interest and become a rapidly growing research field for a wide range of applications in recent years.8–13 In particular, COFs have recently exhibited promising potential application in hydrogen production by virtue of their multiple merits including π–π stacking structures, excellent visible-light response ability, tunable band gaps and remarkable physiochemical stability, which are rather challenging to be simultaneously realized within previously reported inorganic and organic amorphous photocatalysts.14,15 In 2014, Lotsch and co-workers pioneered the employment of a hydrazone-linked COF as the photocatalyst loaded with a Pt co-catalyst in the presence of a certain sacrificial electron donor (SED) for photocatalytic H2 evolution under visible-light irradiation;16 subsequently, a variety of COFs with different linkages or topologies were designed and reported for efficient hydrogen evolution17–22 and the hydrogen evolution rate (HER) could even reach up to 100 mmol g−1 h−1 under visible-light irradiation (λ ≥ 420 nm).17 Among all the reported COF materials, the combination of electron-rich and electron-deficient moieties within a COF backbone to form a periodically ordered donor (D)–acceptor (A) structure has proven to be an effective approach to achieve more efficient charge transport and separation, leading to enhanced photocatalytic performance.18,23,24 For example, we have designed and reported a benzodifuran-based D–A type COF material (BDF-TAPT-COF) by the condensation of electron-donating 4,4′-(benzo[1,2-b:4,5-b′]difuran-4,8-diyl)dibenzaldehyde and electron-withdrawing tris-(4-aminophenyl)triazine, which exhibited an excellent and steady HER of 1390 μmol g−1 h−1 and an outstanding apparent quantum yield of 7.8% at 420 nm.18 The advantages of the introduction of the donor–acceptor–donor type monomer mainly include the enhanced visible-light absorption ability, higher charge transfer and separation efficiency together with a lower charge recombination rate. In this regard, the polycondensation of a D–A–D type of monomer consisting of two electron-donating groups and one electron-withdrawing group within one building unit with another building unit to construct D–A type COFs is expected to facilitate stronger intramolecular charge transfer (ICT) and therefore realizing enhanced charge separation and transport,25,26 while it is still rarely explored thus far.27 In this context, we herein report a novel D–A type imine-linked COF material, termed DABT-Py-COF, by condensation of a newly designed D–A–D type monomer of 4,4′,4′′,4′′′-(benzo[c][1,2,5]thiadiazole-4,7-diylbis(9,9-dimethyl-9,10-dihydroacridine-10,2,7-triyl))tetrabenzaldehyde (DABT-4CHO), and 1,3,6,8-tetrakis(4-aminophenyl)pyrene (PyTA) under conventional solvothermal conditions. The obtained DABT-Py-COF features high crystallinity, permanent porosity, broad light absorption range and excellent chemical stability. More importantly, the DABT-Py-COF exhibited remarkable sunlight-driven hydrogen evolution with a maximum HER of 5458 μmol g−1 h−1 under visible-light irradiation (AM 1.5) and it can be reused for at least 5 consecutive cycles over 20 h with negligible loss of its photoactivity and stability.
The high crystallinity and structure of DABT-Py-COF were confirmed by powder X-ray diffraction (PXRD) together with corresponding structural simulations and Pawley refinements using Materials Studio. As shown in Fig. S6,† no diffraction peaks related to the starting materials were detected. The diffraction peaks at 2.64°, 4.54° and 5.27° could be assigned to the (100), (010) and (200) facets, respectively (Fig. 1a). The experimental PXRD pattern of DABT-Py-COF matched well with the simulated slipped AA stacking model (Fig. 1b and S7, ESI†) and the Pawley refinement showed negligible differences between the simulated and experimental PXRD patterns (Rwp = 5.05% and RP = 3.95%). And the two-dimensional layers in the crystalline state were nonplanar with a large dihedral angle of 54.4° between benzothiadiazole and acridine moieties, which could be applied to explain the tendency for the slipped AA stacking model in DABT-Py-COF (Fig. S8, ESI†). DABT-Py-COF was assigned to the space group of P1 with the unit cell parameters of a = 33.4252 Å, b = 28.0981 Å, and c = 7.0436 Å; α = 44.9959°, β = 90.0502°, and γ = 90.0440° (Table S1, ESI†).
As indicated by the FT-IR spectra (Fig. S9, ESI†), the characteristic peak at 1624 cm−1 clearly confirmed the formation of the imine linkages,29 while the weak peak at 1695 cm−1 is assigned to the free aldehyde groups, indicating the existence of bonding defects.30 As for the solid-state 13C CP-MAS NMR spectrum of DABT-Py-COF (Fig. S10, ESI†), the chemical shifts at approximately 23 and 35 ppm are related to the acridine carbons, while the typical signal at 152 ppm corresponds to the formed imine-linkages31 and other signals from 112 to 150 ppm can be attributed to the aromatic carbons of DABT-Py-COF.32,33 In addition, the X-ray photoelectron spectroscopy (XPS) data further disclosed the structural information of DABT-Py-COF. For example, in the N 1s spectrum, the peaks at 399.0 ± 0.1 and 400.1 ± 0.1 eV are attributed to CN and C–N, respectively. The S 2p spectrum shows a doublet characteristic (at 165.7 ± 0.1 and 166.8 ± 0.1 eV) for the sulfur of the benzothiadiazole groups (Fig. S11, ESI†).19 These results confirmedly verified the successful condensation of the building units. The scanning electron microscopy (SEM) image shows that DABT-Py-COF possesses a sheet-like morphology up to micrometres (Fig. S12, ESI†) and the layered structure of the framework could be obviously observed from its corresponding high-resolution transmission electron microscopy (TEM) image (Fig. S13, ESI†).
The permanent porosity of DABT-Py-COF was investigated by N2 adsorption and desorption measurements performed at 77 K (Fig. 2a). The Brunauer–Emmett–Teller (BET) surface area was estimated to be 549 m2 g−1 with a total pore volume of 0.50 cm3 g−1 at P/P0 = 0.99. The pore size distribution of DABT-Py-COF was centered at 1.18 and 2.16 nm (Fig. 2a, inset) by the nonlocal density functional theory (NLDFT), which is consistent with its theoretical value. To evaluate the chemical stability of the obtained DABT-Py-COF, the DABT-Py-COF samples (10 mg) were respectively immersed in various solvents, including ascorbic acid/water, DMSO, DMF, 3 M HCl and 3 M NaOH, for 1 week. Remarkably, the crystallinity and chemical structures of DABT-Py-COF were well preserved as confirmed by using corresponding PXRD patterns and FT-IR spectra (Fig. 2b and S14, ESI†). Thermogravimetric analysis (TGA) indicated that DABT-Py-COF can be stable up to 260 °C under nitrogen (Fig. S15, ESI†).
The solid-state UV-Vis diffuse reflectance spectrum of DABT-Py-COF exhibits an absorbance tail extending up to 700 nm (Fig. 3a), indicating its wide light harvesting range and the optical band gap (Eg) was evaluated to be 2.00 eV based on the absorption band using the Tauc-plot34 (Fig. 3a, inset). The highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) levels of DABT-Py-COF were respectively calculated to be −6.22 and −4.22 eV by cyclic voltammetry (CV) measurements (Fig. S16 and S17, ESI†). Furthermore, the HOMO and LUMO of the segments of DABT-Py-COF were calculated and visualized by employing density functional theory (DFT) computations. As shown in Fig. 3b, the HOMO and LUMO of the segments are mainly located at the acridine and benzothiadiazole moieties, respectively, indicating sufficient ICT within the framework.
Subsequently, the photocatalytic hydrogen evolution performance of DABT-Py-COF was investigated in an aqueous solution with in situ photogenerated Pt nanoparticles as the co-catalyst and ascorbic acid or TEOA as the sacrificial electron donor (SED) under visible-light irradiation (AM 1.5), as illustrated in Fig. S18.† The control experiments indicated no activity in the absence of light or the photocatalyst, precluding any possible reaction that probably leads to the hydrogen production and only a little amount of hydrogen (299 μmol g−1 h−1) was observed in the absence of the Pt co-catalyst (Fig. S19, ESI†). Furthermore, the photodeposited Pt content and electron donor type also affect the hydrogen production activity. For example, when TEOA was used as the SED, the HER of DABT-Py-COF was only 130 μmol g−1 h−1 and it can reach up to 4726 μmol g−1 h−1 with ascorbic acid as the SED (Fig. S19, ESI†). Moreover, the hydrogen evolution activity of DABT-Py-COF first increased and then decreased with the increase of the photodeposited Pt content (Fig. S20, ESI†). Thus, in a typical photocatalytic reaction, 5 mg of activated DABT-Py-COF was dispersed in 10 mL solution of H2O containing ascorbic acid (0.1 M) and hexachloroplatinic acid (4 μL, 3 wt% aqueous solution) as a platinum precursor. Under the optimized reaction conditions, a remarkable increase of the produced hydrogen amount with the reaction time was observed and a maximum hydrogen evolution rate (HER) of 5458 μmol g−1 h−1 was observed, higher than most of previously reported CMPs and COF materials35,36 (Table S2, ESI†). The photostability of the photocatalyst was further confirmed by multiple H2 evolution tests. Notably, DABT-Py-COF exhibited a steady hydrogen evolution rate under the optimized conditions without significant decay through 5 consecutive cycles of reaction over 20 h (Fig. 3c). Analysis of DABT-Py-COF after photocatalytic reactions by PXRD, FT-IR, SEM and TEM/EDS mapping revealed negligible compositional or morphological changes of the photocatalyst compared with those of the pristine material (Fig. S21–S24, ESI†), and thereby attested to the excellent stability and reusability of DABT-Py-COF. Next, the size of the photodeposited Pt nanoparticles was investigated via TEM and the in situ formed Pt nanoparticles exhibited a similar morphology with an average size of 2.35 nm (Fig. 4a and b).
To further understand the photocatalytic performance of DABT-Py-COF, electrochemical impedance spectroscopy (EIS), photocurrent density (i–t) and time-resolved photoluminescence (TRPL) spectroscopy were performed. First of all, electrochemical impedance spectroscopy was used to evaluate the electrical conductivity of the photocatalysts. As shown in Fig. S25,† the radius of the Nyquist curve of DABT-Py-COF remarkably decreased in the presence of the Pt co-catalyst, suggesting the reduced resistance and enhanced charge migration ability. The significant charge transfer efficiency was further confirmed by the photocurrent response of the photocatalyst (Fig. 4c). The photocurrent response of DABT-Py-COF with Pt was significantly enhanced when the light was switched on in comparison with that of pristine DABT-Py-COF, indicating the low charge recombination rates and high charge transfer efficiency. Furthermore, time-resolved photoluminescence (TRPL) spectroscopy indicated that the average lifetime of DABT-Py-COF was 8.20 ns, beneficial for efficient charge separation and transportation (Fig. 4d).
Footnotes |
† Electronic supplementary information (ESI) available: General methods, and supplementary figures and tables. See DOI: https://doi.org/10.1039/d2ta09625k |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2023 |