Open Access Article
Donghui Wang,
Jin-Gang-Lu Tao,
Haiyang Zhang,
Po Zhang and
Feng Chen
*
Key Laboratory for Advanced Materials and Institute of Fine Chemicals, School of Chemistry and Molecular Engineering, East China University of Science and Technology, Shanghai, P. R. China. E-mail: fengchen@ecust.edu.cn
First published on 20th April 2026
Photocatalytic production of hydrogen peroxide (H2O2) from water and oxygen under sunlight offers a safe and sustainable alternative to traditional processes. However, the sluggish water oxidation reaction (WOR) often imposes kinetic limitations on the accompanying oxygen reduction reaction (ORR) in pure water systems. This research developed a series of tailored covalent organic frameworks (COFs) with localized polarization features to boost the reaction rates of the WOR. By incorporating varying numbers of sp2-hybridized nitrogen atoms into a single benzene ring, a locally polarized electronic environment was established. In particular, the dual sp2-hybridized nitrogen atoms in pyrimidine units induce strong local polarization, which facilitates charge separation and activates adjacent C
C bonds as more favorable sites for the WOR. Together with the highly efficient ORR activity enabled by the two nitrogen atoms, the pyrimidine-functionalized TpDa demonstrates outstanding performance in a sacrificial-agent-free system, achieving an H2O2 production rate of 6.94 mmol g−1 h−1 and an apparent quantum yield (AQY) of 25.2%. This work establishes local polarization engineering as an effective strategy for optimizing COF photocatalysts and highlights its potential for solar-driven chemical transformations.
In recent years, metal-free organic polymers such as graphitic carbon nitride (g-C3N4) derivatives,7,8 resorcinol–formaldehydes (RFs)9,10 and COFs11–13 have emerged as promising photocatalysts owing to their low cost, high efficiency, and structural tunability. Among them, COFs are particularly attractive due to their well-defined molecular structures that allow rational active site design, extended π-conjugation for improved light harvesting, and intrinsic porosity that facilitates mass transport.14,15 Despite these advantages, the photocatalytic efficiency of COF-based systems for sacrificial-agent-free H2O2 production remains unsatisfactory. One limitation arises from the kinetically sluggish water WOR, which provides the protons required for H2O2 formation via the ORR. However, the catalytic sites responsible for the WOR in COF systems are often poorly defined, hindering rational catalyst design.16
Several recent studies have attempted to enhance H2O2 production in COF photocatalysts through structural modulation. For example, BTT–PhPD and TTDN–COF systems demonstrated improved catalytic performance through heteroatom engineering that enhances the oxygen reduction reaction (ORR) pathway.13,17 Nevertheless, these studies primarily focused on promoting ORR activity, while the identification and regulation of WOR active sites were rarely addressed. More recently, COF–N32 suggested that nitrogen atoms may serve as potential catalytic centers for the WOR.18 However, the precise nature of WOR active sites in organic photocatalysts remains controversial. Various structural motifs, including benzene rings, C
C bonds, and C
C bonds, have been proposed as possible WOR centers, yet these assignments are often speculative and lack systematic verification.19,20 Therefore, developing strategies that can precisely define and regulate catalytic active sites for the WOR in COF photocatalysts is of great importance.
In parallel, dipole-field engineering has recently emerged as an effective approach for regulating charge separation and transport in conjugated frameworks. By constructing donor–acceptor architecture or introducing asymmetric electronic structures, internal dipole moments can promote charge redistribution and improve photocatalytic performance. For instance, BT-COF achieves accelerated charge transfer through the ordered arrangement of donor–acceptor units, generating both in-plane and intermolecular polarization.21 Similarly, BTT-TAA-COF, composed of terthiophene donors and triazine acceptors, exhibits enhanced π-electron delocalization and improved charge mobility.22 Although these approaches effectively enhance charge separation, they mainly rely on long-range intermolecular polarization or framework-level electronic modulation. In contrast, the influence of localized intramolecular polarization on charge redistribution and catalytic site activation has rarely been explored in COF photocatalysts.
Herein, we report a COF photocatalyst that integrates efficient WOR and ORR sites through an intramolecular local polarization strategy. By incorporating pyrimidine units into the COF framework, the higher electronegativity of nitrogen relative to carbon induces a strongly polarized electronic environment within the molecular unit. Both experimental results and theoretical calculations reveal that the two sp2-hybridized nitrogen atoms in the pyrimidine ring serve as highly selective ORR active sites, while the C
C bond polarized by dual nitrogen atoms may serve as a more favorable site for the WOR. This localized electronic polarization enables precise regulation of catalytic functionality within a single structural motif. As a result, the resulting TpDa-pyrimidine COF exhibits outstanding photocatalytic performance for sacrificial-agent-free H2O2 production, achieving a rate of 6.94 mmol g−1 h−1 and an apparent quantum yield (AQY) of 25.2%, outperforming most reported COF-based photocatalysts.
Structural characterization studies were conducted on four as-synthesized COFs. Powder X-ray diffraction (PXRD) analyses (Fig. 2a–d) show that all COFs exhibit diffraction peaks for the (100) plane, confirming long-range in-plane order. Intense diffraction peaks at 26°–28° correspond to the (001) plane, indicating the layer-by-layer stacking of 2D structures. Two-dimensional COFs can adopt either eclipsed (AA) or staggered (AB) stacking configurations. Combined structural simulations (Fig. S1 and S2) and pore size distribution (Fig. S3) analyses indicate that the four COFs adopt the AA stacking mode with pore widths of 1.3–1.6 nm which provides the open channels for mass transport.23 In addition, Pawley refinement of the experimental PXRD data showed good agreement with AA stacking (TpTz: Rwp = 8.26%, Rp = 4.25%; TpDa: Rwp = 8.61%, Rp = 7.57%; TpPy: Rwp = 2.27%, Rp = 1.79%; TpMa: Rwp = 1.76%, Rp = 1.58%). N2 adsorption–desorption isotherms yielded Brunauer–Emmett–Teller (BET) surface areas of 8.6, 61, 35.1, and 48.2 m2 g−1 for TpTz, TpDa, TpPy and TpMa, respectively.
The FTIR spectra of the COFs and their corresponding monomers are shown in Fig. 2f and S4. –NH2 (3300–3460 cm−1) and –CHO (2894 cm−1) peaks24 in diamines and Tp vanished in COFs. Peaks for C
O (1630–1670 cm−1), C
C (1530–1580 cm−1), and C–N (1240–1280 cm−1) emerged,25 confirming β-ketoenamine linkage formation. Additional peaks at 1311, 1467, and 1361 cm−1 for TpTz, TpDa, and TpPy are assignable to C
N vibrations in triazine, pyrimidine, and pyridine units.26,27 The solid-state 13C NMR spectra of the four COFs display distinct peaks labeled a, b, and c at characteristic chemical shifts assigned to C
O (∼180 ppm), C
C (103–105 ppm), and C–N (144 ppm), respectively.28 This observation correlates well with FTIR data, providing evidence for the formation of the β-ketoenamine linkage. Carbon signals from the phenyl rings primarily appear in the lower chemical shift region (112–135 ppm). In contrast, the 13C signals associated with the nitrogen-containing heterocyclic rings exhibit shifts towards higher chemical shifts (143–160 ppm). This phenomenon arises from the influence of the highly electronegative nitrogen atoms and reflects the intramolecular polarization effect inherent to these asymmetric heterocyclic units.
The XPS survey spectra (Fig. S5a) confirm the presence of C, N, and O in all COFs. Notably, the C 1s peak intensity progressively increases across the series TpTz < TpDa < TpPy < TpMa, while the N 1s intensity decreases accordingly. This inverse correlation directly corresponds to the carbon/nitrogen content ratio in the diamine monomers. Deconvolution of the high-resolution N 1s XPS spectra (Fig. 2h) reveals two peaks at 398.9 eV and 400.3 eV, assigned to C
N and C–N species, respectively.29 The relative area of the C
N peak sequentially decreases from TpTz to TpMa, with quantified proportions of 61.6%, 44.4%, 29.0%, and 4.5%, respectively. The minor C
N component in TpMa originates from ketoenamine-to-enolimine tautomerization. Elemental analysis (EA, Table S1) further corroborates the compositional trend observed by XPS (Table S2), with both techniques reflecting the monomeric C/N ratios. The high-resolution O 1s spectra (Fig. S5b) exhibit two components at ∼531 eV and ∼533 eV, attributed to C
O and C–O groups.30 Collectively, FT-IR, 13C NMR, and XPS results confirm the successful synthesis of four COFs featuring the β-ketoenamine linkage.
Scanning electron microscopy (SEM) images (Fig. S6) reveal the morphology of the synthesized COFs. A distinct morphological evolution from nanorods to webbed networks is observed with decreasing nitrogen content. TpTz and TpDa comprise stacked nanorods several hundred nanometers in length and 60–80 nm in diameter. In contrast, TpPy and TpMa exhibit an interconnected webbed structure formed by numerous fibrils approximately 30 nm in diameter. High-resolution transmission electron microscopy (HRTEM) of TpDa (Fig. 2i) clearly shows lattice fringes with a measured interplanar spacing of 1.32 nm. These fringes are assigned to the (100) crystallographic plane, providing more definitive evidence for the crystalline structure of TpDa.
To elucidate the structure–activity relationships in photocatalytic H2O2 production, we systematically evaluated the optical and charge separation properties of the four COFs. Ultraviolet-visible diffuse reflectance spectroscopy (UV-vis DRS, Fig. 3a) reveals absorption edges extending to ∼600 nm for all COFs, attributed to their highly conjugated frameworks. Tauc plot analysis (Fig. 3b) yields optical band gaps (Eg) of 2.49 eV (TpTz), 2.46 eV (TpDa), 2.34 eV (TpPy), and 2.43 eV (TpMa). XPS valence band (VB) spectra (Fig. S7) determine valence band maxima (VBM) at 2.26 V (TpTz), 1.89 V (TpDa), 1.95 V (TpPy), and 1.87 V (TpMa) relative to the NHE. The conduction band minimum (CBM) was subsequently calculated from Eg and VBM. The resultant energy band structures (Fig. 3c) demonstrate that for all COFs, the CBM is strictly more negative than the O2/H2O2 redox potential (0.695 V vs. NHE), while the VBM is more positive than the O2/H2O redox potential (1.23 V vs. NHE). These thermodynamic relationships suggest that photogenerated electrons can drive the reduction of O2 to H2O2, while the holes possess sufficient driving force to promote the WOR. Notably, the four COFs exhibit no significant differences in their band structures, suggesting that their photocatalytic performance is predominantly governed by the nature of the active sites.
Photoelectrochemical measurements reveal that TpDa generates a higher photocurrent density compared to TpTz, TpPy, and TpMa (Fig. 3d), indicating superior charge separation efficiency, which facilitates interfacial redox reactions. Electrochemical impedance spectroscopy (EIS) analysis demonstrates a significantly lower charge transfer resistance for TpDa and TpTz relative to TpMa and TpPy (Fig. 3e), confirming that interfacial charge mobility markedly improves with increased intramolecular polarization. Time-resolved photoluminescence studies show average fluorescence lifetimes of 6.02 ns (TpTz), 7.57 ns (TpDa), 1.93 ns (TpPy), and 1.43 ns (TpMa) (Fig. 3f and Table S3). Notably, TpDa and TpTz exhibit considerably prolonged lifetimes, ascribed to polarization of nitrogen-containing heterocycles enhancing charge carrier separation. Intriguingly, although TpTz exhibits stronger calculated polarization, its photocurrent response, EIS behavior, and average fluorescence lifetime are slightly inferior to those of TpDa. A quantitative analysis of the (100) diffraction peaks in the PXRD patterns shows that the full width at half maximum (FWHM) of TpTz (0.363) is larger than that of TpDa (0.278) (Fig. 2a and b), indicating a lower degree of in-plane ordering. The higher in-plane ordering of TpDa may facilitate more efficient charge carrier separation, which could contribute to its improved photoelectrochemical performance.
Subsequently, we conducted density functional theory (DFT) calculations utilizing full periodic models rather than repeated monomeric fragments, enabling more accurate representation of the highest occupied crystalline orbital (HOCO) and lowest unoccupied crystalline orbital (LUCO) distributions31 in the synthesized crystalline porous materials. As illustrated in Fig. 3g, no discernible separation between HOCO and LUCO occurs in the keto-enamine region of TpDa. However, periodic separation emerges within the polarized pyrimidine ring. Specifically, LUCO is predominantly localized on the two nitrogen heteroatoms, while HOCO is chiefly distributed across C
C bonds. Consequently, upon photoexcitation, electrons and holes are spatially separated at N sites and C
C bonds within the pyrimidine ring, which is consistent with the possibility that N sites participate in the ORR while C
C bonds may be involved in the WOR. For TpTz, pronounced in-plane periodic separation of HOCO and LUCO is evident: LUCO concentrates on N atoms within the triazine ring, and HOCO resides within the keto-enamine moiety (Fig. S8a). Given the absence of C
C bonds in the triazine ring, the WOR predominantly occurs at the keto-enamine C
C sites. Compared to TpDa and TpTz, TpPy and TpMa exhibit negligible HOCO–LUCO periodic separation due to insufficient intramolecular polarization in their pyridine and benzene rings (Fig. S8b and S8c). Additionally, we computed electron localization function (ELF) maps for all four COFs (Fig. 3h and S9). Notably, relative to the fully localized electrons at carbon atoms in benzene rings, nitrogen atoms in N-heterocycles display enhanced electron delocalization, which may contribute to improved catalytic activity. Furthermore, time-dependent density functional theory (TDDFT) calculations mapped the distributions of excited-state electrons and holes32,33 in molecular fragments of the COFs (Fig. 3i and S10). TDDFT reveals that in N-heterocyclic units of TpTz, TpDa, and TpPy, electrons localize on N atoms while holes remain at C
C bonds. Conversely, in TpMa, which lacks this heterocyclic cycle, electrons and holes are partially delocalized in ketoamine and benzene sections, respectively. This suggests that polarized N-heterocycles may enhance spatial carrier separation21,34 and potentially provide favorable sites for the ORR and WOR.
The photocatalytic H2O2 synthesis performances of the four COFs were evaluated under xenon lamp irradiation. TpDa exhibited a H2O2 production rate of 6.94 mmol g−1 h−1 in pure water under an O2 atmosphere (Fig. 4a), far exceeding those of TpPy (2.18 mmol g−1 h−1), TpTz (1.28 mmol g−1 h−1), and TpMa (0.22 mmol g−1 h−1). A distinct parabolic trend is observed in the H2O2 photosynthetic efficiency as a function of nitrogen content, which initially increases and subsequently decreases with increasing nitrogen incorporation. In contrast, the non-heterocyclic COF TpMa exhibits negligible photocatalytic activity. This indicates that H2O2 photosynthesis performance is not solely determined by the number of nitrogen atoms, but also by the structural nature of the heteroaromatic units. H2O2 decomposition capabilities under an Ar atmosphere were subsequently tested (Fig. 4b). Without sacrificial agents, COF decomposition activity directly correlates with their H2O2 production rates. No noticeable H2O2 decomposition was observed under dark conditions (Fig. S11a). This confirms that the H2O2 decomposition observed in Fig. 4b mainly originates from photocatalytic processes. However, adding the electron scavenger NaIO3 completely suppressed H2O2 decomposition for all COFs (Fig. S11b), confirming that photogenerated electrons drive decomposition. The enhanced decomposition kinetics of TpDa, which have similar reduction sites and potentials to other COFs, further corroborates its superior charge separation capability. During prolonged operation, TpDa steadily produced H2O2 at the fastest speed, but as the concentration of H2O2 increased, the rate of H2O2 production gradually decreased, which was attributed to the high concentration of H2O2 competing for oxygen reduction active sites (Fig. 4c). Subsequently, we evaluated the effect of TpDa dosage on the production rate of H2O2. Catalyst dosage optimization revealed increasing H2O2 production rates with TpDa concentration, plateauing at 0.33 g L−1 with negligible further increase (Fig. S12). This optimal dosage was selected for subsequent apparent quantum yield (AQY) and solar-to-chemical conversion (SCC) efficiency measurements. TpDa achieved an AQY of 25.2% at 400 nm (Fig. 4d), exhibiting strong spectral dependency, along with a remarkable SCC efficiency of 0.54%. These values surpass most state-of-the-art COF photocatalysts (Fig. 4e and Table S4). After five catalytic cycles, all COFs retained >90% initial activity (Fig. 4f). Post-cycling characterization revealed decreased TpDa crystallinity (Fig. S13) while maintaining the chemical composition (FTIR: Fig. S14; XPS: Fig. S15), demonstrating robust chemical stability. Furthermore, decomposition temperatures exceeding 300 °C indicate substantial thermal resilience (Fig. S16).
The photocatalytic H2O2 formation mechanism comprises two half-reactions: two-electron oxygen reduction (2e− ORR) and two-electron water oxidation (2e− WOR).35,36 In most photocatalytic systems, the 2e− ORR pathway (eqn (1)) is favored over the 2e− WOR route (eqn (2)).37 Water oxidation predominantly follows the thermodynamically preferred four-electron pathway (4e− WOR, eqn (3)).38 However, its sluggish four-electron transfer kinetics frequently renders the 4e− WOR the rate-limiting step in the overall H2O2 synthesis process.39
| O2 + 2H+ + 2e− → H2O2 | (1) |
| 2H2O + 2h+ → H2O2 + 2H+ | (2) |
| 2H2O + 4h+ → O2 + 4H+ | (3) |
To elucidate the mechanism of the cathodic ORR in the COFs, linear sweep voltammetry (LSV) curves were acquired using a rotating ring-disk electrode (RRDE) (Fig. S17). The RRDE measurements were performed in an O2-saturated phosphate buffer electrolyte under neutral pH conditions in order to approximate the photocatalytic reaction environment as closely as possible. The electron transfer numbers (n) calculated for TpTz, TpDa, TpPy, and TpMa were 2.45, 2.54, 2.55, and 2.63, respectively, approaching a value of 2. These values suggest that the ORR proceeds predominantly through a two-electron pathway, although minor contributions from other pathways cannot be excluded. The corresponding H2O2 selectivities are 77.6%, 72.8%, 72.6%, and 68.5%, respectively (Fig. S18). These results suggest that the ORR over the COFs mainly follows a 2e− pathway, providing favorable selectivity toward H2O2 formation. The RRDE results mainly serve as supporting evidence for the feasibility of the 2e− ORR pathway, while the photocatalytic mechanism is primarily inferred from photocatalytic control experiments and radical trapping studies. To validate this mechanism, a series of control experiments were designed by modulating the photocatalytic reaction environment. As shown in Fig. 5a, introduction of the electron scavenger NaIO3 drastically suppressed H2O2 yield. Subsequent Ar purging (in the presence of NaIO3) prevented detectable H2O2 formation, demonstrating that H2O2 originates exclusively from photogenerated electron-mediated O2 reduction rather than the WOR. Addition of nitroblue tetrazolium (NBT), a superoxide (˙O2−) scavenger, to the reaction system resulted in a sharp decline in H2O2 content. This observation substantiates a stepwise 2e− ORR mechanism, where O2 undergoes initial single-electron reduction to superoxide/hydroperoxyl radicals (˙O2−/HOO˙), followed by further reduction to H2O2.
Correspondingly, to validate the impact of the WOR on H2O2 generation, EDTA-2Na was employed as a valence band hole scavenger. This intervention enhanced the H2O2 production performance of TpTz, TpDa, and TpPy by factors of 2.82, 1.30, and 1.90, respectively (TpMa was excluded from comparison due to its poor performance resulting from the lack of high-activity ORR sites). Scavenging holes accelerated the oxidation half-reaction kinetics, thereby promoting the H2O2 generation rate via the ORR. Notably, TpTz exhibited the most significant performance enhancement, while TpDa showed the smallest improvement. It indicates that the H2O2 production efficiency of TpTz is more strongly influenced by WOR kinetics, followed by TpPy, and least affected for TpDa. This trend may arise because the polarized pyrimidine and pyridine rings in TpDa and TpPy offer additional potential sites (C
C) for the WOR. In contrast, while the triazine ring in TpTz offers abundant ORR sites (pyridine nitrogen), it lacks activated sites conducive to an efficient WOR. Furthermore, using tert-butanol (tBA) as a hydroxyl radical (˙OH) scavenger led to increased H2O2 production for TpTz and TpPy but yielded a paradoxical decrease for TpDa. This divergence suggests that TpDa possesses a strong inherent capability for oxidizing ˙OH intermediates. Consequently, adding tBA competes for catalytic surface sites, hindering further anodic oxidation processes. Conversely, TpTz and TpPy exhibit weaker ˙OH oxidation capacity; thus, tBA addition scavenges ˙OH radicals, allowing the catalytic cycle to bypass energetically unfavorable sequential oxidation steps. To verify this hypothesis, electron paramagnetic resonance (EPR) spectroscopy was employed using NaIO3 as an electron scavenger to detect ˙OH radicals. (note: DMPO–˙O2− adducts readily convert to DMPO–˙OH in aqueous environments40). As shown in Fig. 5b, TpDa generated the lowest detectable ˙OH signal during photocatalysis, indicating its high efficiency in rapidly converting ˙OH intermediates formed on its surface. This observation aligns perfectly with the inferences drawn from the tBA scavenger experiments in Fig. 5a. Additionally, EPR revealed similar DMPO–˙O2− signal intensities for TpTz, TpDa, and TpPy but a substantially higher signal for TpMa (Fig. S19). This apparent discrepancy with the performance metrics (where TpMa performs poorly) will be addressed in the subsequent theoretical calculation section on reaction pathways.
Sacrificial agent experiments confirm that COF-based photoanodes are incapable of generating H2O2 via the WOR, thus restricting anodic products to O2. We evaluated the O2 evolution capabilities of the four COFs using gas chromatography. As shown in Fig. 5c, TpDa exhibits superior oxygen evolution activity, suggesting that strong local polarization may activate more favorable sites for the WOR. To further probe the relationship between the WOR and ORR, we adopted an alternative quantitative strategy using a low concentration of Ag+ (0.1 mM) as an electron acceptor under O2-free conditions. In this configuration, H2O2 can only be produced via the reduction of O2 generated from water oxidation. As shown in Fig. 5d, negligible H2O2 was detected during the first hour for all four COFs, indicating that photogenerated electrons were primarily consumed by Ag+ reduction. In the second hour, TpDa began to show a clear H2O2 signal, whereas the three comparison samples exhibited much weaker signals. This suggests that TpDa possesses faster WOR kinetics, which accelerates the consumption of Ag+ and allows the system to enter the ORR-driven H2O2 formation stage earlier.
Subsequently, the H2O2 concentration gradually increased for all samples. Notably, the H2O2 concentration for TpDa quickly approached a stable value of approximately 0.046 mM, corresponding to about 92% of the theoretical value (0.05 mM). The remaining ∼8% loss may arise from the reaction equilibrium of H2O2 formation. This behavior indicates that the O2 generated from the WOR in the TpDa system was rapidly consumed by the ORR, whereas the comparison samples continued to generate O2 more slowly.
To gain deeper mechanistic insights into the COF photocatalysts in this study, density functional theory (DFT) calculations were employed to investigate the reaction pathways for both the 2e− ORR and 4e− WOR. In the 2e− ORR, the initial step typically involves adsorption activation of either O2 or H+. The pivotal role of nitrogen atoms in heterocyclic rings was probed by comparing adsorption free energies (ΔGads) for O2 and H+ between TpDa (with N-heterocycles) and TpMa (without N-heterocycles). Results revealed that TpMa exhibited a 0.27 eV lower ΔGads for O2 than for H+, favoring O2 adsorption activation (eqn (4)) (Fig. S20). Conversely, TpDa showed a 0.21 eV lower ΔGads for H+ activation than for O2, indicating preferential H+ adsorption (eqn (5)) (Fig. S21). The preferential O2 activation to form ˙O2− by TpMa likely explains its intensified DMPO–˙O2− EPR signal in Fig. S19. Using proton activation (*H formation) as the initial step, the full 2e− ORR pathway was computed. Optimized structural snapshots (Fig. S22–25) show that in the second step, O2 adsorbs on the β-ketoenamine chain's C
C bond and reacts with *H to form *OOH (eqn (6)). Subsequently, the second H+ adsorbs on C
O and hydrogen-bonds with *OOH to form *HOOH (eqn (7)), which ultimately desorbs as H2O2. Complete free energy diagrams for the 2e− ORR across all four COFs are presented in Fig. 5e. TpTz, TpDa, and TpPy (N-heterocycle-containing) display similar free energy profiles, with substantially lower energy barriers for the *H and *OOH + *H intermediates compared to TpMa, demonstrating the catalytic enhancement from heterocyclic N atoms. Moreover, increased pyridinic-N sites stabilize *H and *OOH intermediates via additional adsorption centers, thereby optimizing 2e− ORR efficiency. Despite possessing the highest pyridinic-N content, TpTz exhibits lower photocatalytic activity, which may be associated with kinetic limitations related to the anodic WOR process.
| * + O2 + e− → *˙O2− | (4) |
| * + H+ + e− → *H | (5) |
| *H + O2 → *OOH | (6) |
| *OOH + H+ + e− → *HOOH | (7) |
C bond to generate the hydroxyl radical adsorbate (eqn (8)). In the second step, *OH undergoes dehydrogenation to form the epoxy intermediate *O (eqn (9)). The third step involves dissociation of another H2O molecule, yielding the *O + *OH co-adsorbed state (eqn (10)). This co-adsorbed state subsequently oxidizes in the fourth step to form O2 (eqn (11)). Notably, TpDa, TpPy, and TpMa (but not TpTz) possess two distinct WOR active sites: the C
C bond of the β-ketoenamine chain (site 1) and the C
C bond of the aromatic ring (site 2). Free energy diagrams from DFT indicate that the formation of the *O + *OH intermediate represents the rate-limiting step in the 4e− WOR, with ΔG ≥ 2.99 eV (Fig. 5f, S33 and S34). The 4e− WOR on site 1 of the four COFs showed a close trend (Fig. S35). Across all four COFs, the ΔG for *O + *OH formation is consistently lower on site 2 than on site 1, establishing site 2 as the primary reaction site for the 4e− WOR. ΔG on site 2 of TpDa is markedly lower (1.71 eV), compared to 2.72 eV for TpMa and 2.79 eV for TpPy (Fig. 5g). This suggests that strong polarization from bipyridine nitrogen atoms can lower the thermodynamic barrier for the WOR at site 2. The lowered barrier may accelerate the conversion of *OH to downstream intermediates, which could contribute to improved overall H2O2 synthesis. Concurrently, this mechanistic insight explains the minimal DMPO–˙OH signal observed for TpDa in Fig. 5b, as rapid *OH turnover reduces DMPO trapping efficiency.| * + H2O + h+ → *OH + H+ | (8) |
| *OH + h+ → *O + H+ | (9) |
| *O + H2O + h+ → *O + *OH + H+ | (10) |
| *O + *OH + h+ → O2 + H+ | (11) |
Subsequent in situ diffuse reflectance infrared Fourier transform spectroscopy (DRIFTS) validated the DFT-derived catalytic mechanism. Upon irradiation, peaks assignable to C
NH+ species (∼1692 cm−1)41 emerged in DRIFTS spectra of TpTz (Fig. S36), TpDa (Fig. 5h), and TpPy (Fig. S37), with intensity increasing progressively over illumination time. This feature was absent in pyridine-N-free TpMa (Fig. 5i), confirming proton adsorption activation on pyridinic nitrogen as the initial ORR step in N-heterocyclic COFs, consistent with DFT predictions. Peaks at 1173, 1237, and 1365 cm−1 correspond to O–O stretching modes of adsorbed ˙O2−, OOH, and HOOH* intermediates, respectively.42,43 Crucially, TpDa exhibited substantially stronger intensities for all three oxygen-related species than TpTz, TpPy, and TpMa, indicating accelerated ORR kinetics. This enhancement stems from the reduced thermodynamic barrier in the WOR (previously limiting overall H2O2 synthesis). Furthermore, the 1073 cm−1 peak in DRIFT spectra is attributed to C–OH species.19 As *OH is a critical intermediate in the 4e− WOR, C–OH formation confirms that water oxidation occurs on C
C bonds. The strongest C–OH signal in TpDa suggests more favorable WOR activity, specifically the C
C bonds activated by strong polarization from bipyridinic nitrogen atoms. Collectively, these results are consistent with the reaction pathways suggested by the DFT calculations. The data demonstrate that strong polarization within nitrogen heterocycles plays a crucial promotional role in both the ORR and WOR processes.
C bond while providing highly active ORR sites (pyridine nitrogen). These findings highlight the important role of local polarization in influencing photocatalytic reactions and establish a rational design principle for the development of advanced COF-based materials for solar-driven chemical conversions.
Supplementary information (SI): experimental details, computational details, characterization data, control experiments, and supporting figures and tables related to photocatalytic performance and mechanistic analysis. See DOI: https://doi.org/10.1039/d6sc00783j.
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