Open Access Article
Fuzhen Lia,
Huan Lin
c,
Chunying Chenc,
Li-Lin Tanb,
Dawei Wang
c,
Cunyuan Zhaoc,
Li Zhang
*c and
Cheng-Yong Su
c
aSchool of Chemical Engineering and Technology, Sun Yat-sen University, Zhuhai 519082, China
bShantou Engineering Technology Research Center for Green and Precise Manufacturing of High-value Chemicals, Chemistry and Chemical Engineering Guangdong Laboratory, Shantou 515031, China
cLehn Institute of Functional Materials, School of Chemistry, Sun Yat-Sen University, Guangzhou 510006, China. E-mail: zhli99@mail.sysu.edu.cn
First published on 29th April 2026
The development of efficient electrocatalysts for the nitrate reduction reaction (NO3RR) to ammonia is crucial for sustainable nitrogen management, but remains challenging due to its intricate multi-step mechanism and competing side reactions. A key bottleneck is the severe imbalance between the generation and consumption of H*, which critically constrains ammonia selectivity and yield. Herein, a molecular engineering strategy was developed through the incorporation of Pd-porphyrin to promote the generation of H*, while grafting ethoxyphenyl groups to create a hydrophobic microenvironment and inhibit the hydrogen evolution reaction. The covalent organic framework of Pd-PCOF-2(Cu3), which was prepared from the reaction of Pd(II) diaminoporphyrin and trinuclear copper cluster aldehyde, achieved a high NH3 faradaic efficiency of 94.7% and a production rate of 15.09 mg h−1 cm−2. A rechargeable Zn–NO3− battery with Pd-PCOF-2(Cu3) as the cathode was further constructed, which served as a dual-function system for both power output and ammonia production.
N triple bond (941 kJ mol−1) and the low solubility of N2 in aqueous solutions (∼0.6 mM), resulting in poor reaction kinetics and negligible yield.4,5
Inspired by the comparatively lower dissociation energy of NO3− (204 kJ mol−1) and its high solubility, the formation of NH3 from the electrocatalytic nitrate reduction reaction (NO3RR) has emerged as a compelling alternative strategy.6–8 Nevertheless, the NO3RR process involves a complex multi-step mechanism encompassing an eight-electron, nine-proton transfer pathway (NO3− + 9H+ + 8e− → NH3 + 3H2O), with the sequential hydrogenation/deoxygenation step of NO3− and critical intermediates such as nitrite (NO2−) driven by active hydrogen (H*) from H2O decomposition/reduction.9,10 Hence, the supply and utilization of H* play a pivotal role.11,12 An inadequate supply of H* can kinetically limit the hydrogenation steps, leading to the accumulation of reaction intermediates and reduced efficiency. Conversely, an over-abundance of H* readily promotes H–H coupling, triggers the competing hydrogen evolution reaction (HER) and lowers the faradaic efficiency for NH3. Therefore, the precise regulation of the H* supply to couple with the specific hydrogenation steps of the nitrate reduction pathway is crucial for achieving optimal performance.13,14 Some strategies to address this issue have been reported, including single-atom alloys, dual-atom catalysts and heterojunction engineering.15–20 Given that hydrophobicity can limit the accumulation of water molecules at the catalyst surface and thus suppress the HER, the rational construction of a hydrophobic microenvironment to precisely regulate the supply of H* represents a feasible strategy.21 So far, its application in the field of electrocatalytic NO3RR has been underdeveloped.
Owing to the precise structural tunability and robust covalent architectures, covalent organic frameworks (COFs) display advantages in electrocatalytic reactions, especially under alkaline conditions.22–28 Porphyrins possess conjugated structures and excellent electrical properties, and are thus employed as pivotal building blocks and active sites in the construction of porphyrin-based COFs (PCOFs) for electrocatalytic applications.29–35 Furthermore, the single-metal site within the metalloporphyrin is pivotal for the formation of M−H (metal−hydride) active species, which could assist in the electrocatalytic reduction of NO3− to NH3.36,37 Nevertheless, the vast majority of reported PCOFs are structurally limited to sql topology derived from C4-symmetric tetraphenylporphyrin building blocks. Consequently, not only the promising strategy of porphyrin side-chain engineering for PCOFs remains largely unexplored, but also the design and construction of new PCOF topologies merit further investigation.
Herein, three new A2B2-type diaminoporphyrin monomers were designed and synthesized, which subsequently reacted with a trinuclear copper cluster (Cu3) aldehyde ligand via Schiff-base condensation, giving rise to three two-dimensional imine-linked PCOFs with ABC stacking and a hcb topology, denoted as Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3), and PCOF-2(Cu3), respectively. On one hand, the precise integration of hydrophobic phenyl or ethoxyphenyl side groups of porphyrins engineered a pore-confined hydrophobic microenvironment. On the other hand, the introduction of Pd centers within the porphyrin macrocycles, alongside the Cu3, established well-defined bimetallic active sites. This deliberate architectural design facilitated exceptional electrocatalytic performance for the NO3RR under alkaline conditions. Catalytic results showed that Pd-PCOF-2(Cu3) achieved a remarkable faradaic efficiency up to 94.7% and a high NH3 generation rate of 15.09 mg h−1 cm−2 at applied potentials of −1.0 V and −1.1 V vs. RHE, respectively. It also maintained stable performances over 10 consecutive catalytic cycles, ranking among the top reported COF/MOF-based electrocatalysts (Table S1). Mechanistic investigations revealed that the hydrophobic microenvironment played a critical role in precisely regulating the supply of H*, which could effectively suppress the competing HER. Concurrently, the Cu3 and Pd centers served as the catalytic sites for the adsorption/activation of NO3− and the hydrogenation of the NO2− intermediate, respectively, forming an efficient bimetallic synergistic catalytic mechanism, which minimized the accumulation of NO2−, enhanced the overall reaction rate, and optimized NO3− to NH3 conversion (Fig. 1).
:
1) to afford DNPP as a purple solid (0.78 g, 11% yield).
:
1) to afford EDAPP as a purple solid (0.264 g, 90% yield). 1H NMR (400 MHz, DMSO-d6, Fig. S3) δ 8.92 (d, J = 4.8 Hz, 4H), 8.82 (d, J = 4.8 Hz, 4H), 8.11 (d, J = 8.4 Hz, 4H), 7.85 (d, J = 8.1 Hz, 4H), 7.37 (d, J = 8.5 Hz, 4H), 7.01 (d, J = 8.3 Hz, 4H), 5.57 (s, 4H), 4.35 (q, J = 6.9 Hz, 4H), 1.54 (t, J = 6.9 Hz, 6H), −2.79 (s, 2H).
:
1) to afford Pd-DNPP as a reddish purple solid (0.364 g, 90% yield).
000
000 to 0.1 Hz at 0 V.
The power density (P) of the Zn–NO3− battery was calculated using the following formula:
| P = I × V |
The crystalline architectures of Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3) were determined via powder X-ray diffraction (PXRD) measurement and theoretical structural simulations via Materials Studio (Fig. 3a–c). Pd-PCOF-1(Cu3) exhibited two distinct peaks at 2θ = 3.40° and 6.80°, corresponding to the (110) and (220) planes, respectively (Fig. 3d). Pawley refinement gave the optimized unit cell parameters of a = b = 54.020 Å, c = 6.739 Å, α = β = 90.00°, γ = 120.00°, with good agreement parameters of Rp = 3.70% and Rwp = 3.20% for Pd-PCOF-1(Cu3) (Tables S2–S4). According to theoretical structure simulations, the experimental PXRD patterns of Pd-PCOF-1(Cu3) well agreed with the simulated ABC stacking (staggered) model in the R-3 space group rather than the AA or AB stacking model (Fig. S12 and S13). It is noted that the PXRD patterns of the three PCOFs were different from those of Pd-DAPP, Pd-EDAPP, EDAPP and Cu3(PyCA)3, demonstrating the formation of the new crystal structures (Fig. S14–S16).
Pd-PCOF-2(Cu3) and PCOF-2(Cu3) displayed similar PXRD patterns and sharper diffraction peaks than Pd-PCOF-1(Cu3), indicating that the introduction of the ethyl group significantly improved crystallinity but did not fundamentally alter the structure of the ABC stacking model in the R-3 space group (Fig. 3e, f, S17–S20 and Tables S5–S10). Taking Pd-PCOF-2(Cu3) as an example, the PXRD pattern of Pd-PCOF-2(Cu3) displayed two dominant peaks at 2θ = 3.30° and 6.60° and three weaker peaks at 2θ = 5.76°, 11.44° and 13.20°, which were assigned to the (110), (220), (300), (600), and (440) facet diffractions in the calculated ABC stacking mode, respectively (Fig. 3e, S17 and S18). The simulated PXRD curve of the ABC stacking model matched well with the experimental one with small fitting parameters of Rp = 2.37% and Rwp = 1.47% and the optimized unit cell parameters were determined to be a = b = 53.903 Å, c = 6.953 Å, α = β = 90.00° and γ = 120.00° on the basis of the Pawley refinement (Table S7).
A scanning electron microscope (SEM) and high-resolution transmission electron microscope (HR-TEM) were used to investigate the morphology and crystal structure of these three PCOFs. In the SEM images, the three PCOFs exhibited irregular nanoparticles with sizes ranging from 100 to 200 nm (Fig. S21–S23). Their HR-TEM images displayed distinct lattice fringes with a spacing of approximately 2.52, 2.62 and 2.58 nm for Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3), respectively, corresponding to their (110) facets, which were in good agreement with the theoretical values of 27.02, 26.95 and 27.06 Å based on the ABC stacking model, further proving their high crystallinity (Fig. 3g–i).
Fourier transform infrared (FT-IR) spectrometry was employed to analyze the chemical structure of the three PCOFs (Fig. 4a). The peak of the C
O stretching vibration of Cu3(PyCA)3 appeared at 1670 cm−1, and meanwhile, the N–H and C
N stretching vibrations of the porphyrin rings were located at 3300–3500
and 1620 cm−1, respectively (Fig. S24–S26).
N2 adsorption–desorption isotherms at 77 K were employed to characterize the porosity of Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3) (Fig. 4b). All three COFs exhibited typical type-II reversible isotherms with Brunauer–Emmett–Teller (BET) surface areas of 37.36, 97.17 and 78.15 m2 g−1 for Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3), respectively. The reduced BET surface area of Pd-PCOF-1(Cu3) may be attributed to its lower crystallinity than Pd-PCOF-2(Cu3) and PCOF-2(Cu3). According to the nonlocal density functional theory (NLDFT) method, the pore sizes were predominantly distributed at approximately 0.93, 0.80, and 0.88 nm for Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3), respectively (Fig. S27).
According to the static water contact angle measurement, obvious hydrophobicity was visualized in the three PCOFs, in which the water contact angles were measured to be 130.8°, 144.3° and 139.8° for Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3), respectively (Fig. 4c). Compared with Pd-PCOF-1(Cu3), the increased water contact angles of Pd-PCOF-2(Cu3) and PCOF-2(Cu3) might be attributed to the presence of ethoxyphenyl groups within the channels.
The solid-state 13C cross-polarization magic angle spinning nuclear magnetic resonance (13C CP-MAS NMR) spectrum of Pd-PCOF-2(Cu3) was examined. The characteristic C signal of the ethoxy group was observed at 61.5 and 12.5 ppm, while the porphyrin ring and pyrazole carbons exhibited resonance at 139.5, 129.5, 118.5 and 113.0 ppm and 139.5 and 118.5 ppm, respectively, in Pd-PCOF-2(Cu3) (Fig. 4d). The characteristic resonance peak of the imine carbon appeared at ∼156.5 ppm in the 13C CP-MAS NMR spectrum, which further confirmed the successful formation of imine bonds.
The electronic valence state of the PCOFs was investigated by X-ray photoelectron spectroscopy (XPS) measurements. The full XPS spectra of both Pd-PCOF-1(Cu3) and Pd-PCOF-2(Cu3) displayed C 1s, N 1s, O1s, Cu 2p and Pd 3d elemental signal peaks, while the full XPS spectrum of PCOF-2(Cu3) only showed C 1s, N 1s, O1s and Cu 2p elemental signal peaks (Fig. S28). Furthermore, the high-resolution Cu 2p XPS spectrum of Pd-PCOF-2(Cu3) showed two major peaks belonging to Cu 2p1/2 and Cu 2p3/2, which were mainly composed of peaks assigned to the binding energy of CuI centered at 953.2 and 933.4 eV (Fig. 4e). Similar values were observed for Pd-PCOF-1(Cu3) (953.2 and 933.4 eV), PCOF-2(Cu3) (953.1 and 933.2 eV) and Cu3(PyCA)3 (952.8 and 933.0 eV), revealing the main CuI state nature of the Cu3 moiety (Fig. S29). The high-resolution Pd 3d XPS spectrum of Pd-EDAPP, Pd-PCOF-1(Cu3) and Pd-PCOF-2(Cu3) all exhibited two peaks centered at 343.6 and 338.4 eV, corresponding to Pd 3d3/2 and Pd 3d5/2, respectively, indicating a +2 oxidation state of the coordinated palladium centers in porphyrin (Fig. 4f and S30). The results of XPS spectra demonstrated that the formation of PCOFs did not alter the oxidation states of copper and palladium of the starting materials.
Energy-dispersive X-ray (EDS) spectroscopy was employed to investigate elemental distribution, revealing the homogeneous dispersion of C, Cu and Pd in both Pd-PCOF-1(Cu3) and Pd-PCOF-2(Cu3), whilst only C and Cu were observed in PCOF-2(Cu3) (Fig. 4g–i).
The chemical structural stability of the PCOFs was first studied by thermogravimetric analysis (TGA), which disclosed only 5% mass loss at 265, 244 and 235 °C under a N2 atmosphere for Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3), respectively (Fig. S31). Furthermore, the PXRD patterns of Pd-PCOF-2(Cu3) and PCOF-2(Cu3) remained almost unchanged after being soaked in a range of solvents such as tetrahydrofuran (THF), acetonitrile (CH3CN), methanol (CH3OH), 1 M NaOH and 0.1 M HCl for 24 h (Fig. S32 and S33). Pd-PCOF-1(Cu3) was also stable in these solvents with the exception of 0.1 M HCl (Fig. S34). These studies revealed the high chemical structural stability of these PCOFs and the importance of hydrophobicity in their acid-base resistance.
The linear sweep voltammetry (LSV) curves revealed a dramatic enhancement in the current density upon the addition of NO3− for the three PCOFs, manifesting their remarkable electrocatalytic NO3RR activity (Fig. 5a). Pd-PCOF-1(Cu3) and Pd-PCOF-2(Cu3) displayed stronger current density responses than PCOF-2(Cu3), suggesting that the incorporation of Pd centers in porphyrin could improve the NO3RR activity.
Chronoamperometry electrolysis with applied potentials from −0.6 to −1.1 V vs. RHE was employed to investigate the differences in electrocatalytic efficiency among Pd-PCOF-1(Cu3), Pd-PCOF-2(Cu3) and PCOF-2(Cu3) (Fig. S40–S42). The NH3 generation rate exhibited a nearly linear enhance with increasingly negative applied potential and reached the maximum values of 14.34 and 15.09 mg h−1 cm−2 at −1.1 V vs. RHE for Pd-PCOF-1(Cu3) and Pd-PCOF-2(Cu3), respectively, which were superior to that of PCOF-2(Cu3) (9.52 mg h−1 cm−2), further demonstrating the contribution of the Pd center in porphyrin to enhance the overall electrocatalytic activity (Fig. 5b). The faradaic efficiencies (FEs) of NH3 exhibited a typical volcano-shaped trend (Fig. 5c). Pd-PCOF-2(Cu3) maintained the highest NH3 FEs (over 80%) among the three PCOFs at almost all applied potentials and reached the maximum value of 94.70% at −1.0 V vs. RHE, which was significantly higher than those of Pd-PCOF-1(Cu3) (87.69% at −0.9 V vs. RHE) and PCOF-2(Cu3) (86.96% at −0.8 V vs. RHE).
The NO2− FEs of all the PCOFs gradually decreased with increasingly negative potentials, under which conditions more active hydrogen (H*) could be generated, which subsequently promoted the hydrogenation of NO2− to NH3, thereby reducing the accumulation of NO2− (Fig. 5d). For comparison, the H2 FEs increased sharply with increasingly negative potentials (Fig. 5e). Compared to Pd-PCOF-1(Cu3) and PCOF-2(Cu3), Pd-PCOF-2(Cu3) exhibited much lower H2 FEs at all potentials. This demonstrated that the hydrophobic microenvironment suppressed the HER, while the generation of H* at Pd-porphyrin promoted the NO3RR process .
Pd-PCOF-2(Cu3) maintained excellent electrocatalytic performance stability for NO3RR at −0.9 V vs. RHE over 10 consecutive cycles, without obvious degradation in FE and the generation rate of NH3 (Fig. 5f and S43). The PXRD pattern of Pd-PCOF-2(Cu3) after electrocatalysis over 10 consecutive cycles retained characteristic diffraction peaks at 2θ = 3.30° and 6.60° (Fig. S44).
In short, owing to the suppression of the competitive HER by the hydrophobic microenvironment and the synergistic catalysis of the Cu3 cluster and Pd-porphyrin, Pd-PCOF-2(Cu3) achieved superior electrocatalytic performances for NO3RR in terms of NH3 FE and generation rate in comparison with most reported MOF/COF-based electrocatalysts (Fig. 5g and Table S1).
Pd-PCOF-2(Cu3) (241 mV dec−1) and PCOF-2(Cu3) (239 mV dec−1) manifested higher Tafel slopes than Pd-PCOF-1(Cu3) (217 mV dec−1), revealing an inhibitory effect of the hydrophobic microenvironment on the water dissociation kinetics (Fig. 6b). It is noted that the H* generated from water dissociation (H2O + M + e− → M−H* + OH−) is crucial to the deoxygenation and hydrogenation of NO3− and intermediates. With the addition of NO3−, Tafel slopes of Pd-PCOF-1(Cu3) and Pd-PCOF-2(Cu3) decreased significantly to 149 and 161 mV dec−1, respectively, which were lower than that of PCOF-2(Cu3) (222 mV dec−1), demonstrating that the presence of Pd centers in the porphyrin rings enhanced NO3RR kinetics (Fig. 6c). In addition, Pd-porphyrin-based COFs of Pd-PCOF-1(Cu3) (2.4 Ω) and Pd-PCOF-2(Cu3) (2.8 Ω) exhibited lower charge transfer resistance than PCOF-2(Cu3) (3.1 Ω) (Fig. S46).
According to LSV curves normalized by electrochemical surface area (ECSA, Fig. S47), Pd-PCOF-2(Cu3) presented a higher current density response than Pd-PCOF-1(Cu3) and PCOF-2(Cu3), demonstrating the highest intrinsic NO3RR activity of Pd-PCOF-2(Cu3) (Fig. 6d).
Cyclic voltammogram (CV) curves revealed that the peaks located at 0.52 V vs. RHE in the anodic scan were attributed to adsorbed active hydrogen (*Hads) (Fig. 6e), which could be magnified for precise integration (Fig. S48). The ability to generate *H could be quantitatively compared based on the charge required to oxidize these H* (QH*). Pd-PCOF-1(Cu3) and Pd-PCOF-2(Cu3) exhibited QH* values of 0.0099 and 0.0069 mC, respectively, which were higher than that of PCOF-2(Cu3) (0.0015 mC), indicative of the stronger H* supply ability of Pd-porphyrin-based COFs (Fig. 6f).
To investigate the synergistic effect of the Cu3-cluster and Pd-porphyrin within Pd-PCOF-2(Cu3), electrocatalytic NO3RR performances of Cu3(PyCA)3 and Pd-EDAPP were evaluated under similar conditions. Cu3(PyCA)3 showed much higher current density and NH3 FEs than Pd-EDAPP, suggesting that Cu3(PyCA)3 was the main active center for NO3RR (Fig. S49 and S50). Cu3(PyCA)3 displayed high NH3 FEs (65.0∼84.4%) from −0.6 to 1.1 V (vs. RHE) but negligible H2 FEs at −0.6 V (vs. RHE). With increasingly negative potentials, the H2 FE increased up to 26.6% at −1.1 V (vs. RHE), indicating that it was difficult for Cu3 to achieve precise kinetic matching between the generation of H* and the deoxygenation process of NO3− (Fig. S49d). For comparison, Pd-EDAPP displayed low NH3 FEs but high H2 FEs (56.2∼84.5%) at all potentials, suggesting that the Pd center in porphyrin exhibited slow kinetics for the NO3− activation, giving rise to H2 via the self-coupling of H* as the only rapid outlet (Fig. S50e). Moreover, both Cu3(PyCA)3 and Pd-EDAPP exhibited high performance in the NO2RR process, and the NH3 FEs remained consistently above 60% across the entire applied potential window (Fig. S51 and S52).
Catalytic results further showed that Pd-EDAPP could much more effectively activate NO2− than NO3− (Fig. 6g and S53). A comparison of the LSV curves for catalytic NO2RR demonstrated that the current density of Pd-EDAPP became much higher than that of Cu3(PyCA)3 with increasingly negative applied potential (Fig. S54a). Meanwhile, the NH3 yield rate of Pd-EDAPP was much higher than that of Cu3(PyCA)3 in NO2RR (Fig. S54b). Comparison of the consumption rate of H* on NO2RR and NO3RR showed that the H* generated at Pd-porphyrin showed a stronger affinity for NO2− than NO3− (Fig. 6h, i and S55). These results demonstrated that during electrocatalytic nitrate reduction, Cu3 primarily activated NO3− and converted a portion of NO2− to NH3, while Pd-porphyrin played a synergistic role in promoting the conversion of NO2− to NH3.
To uncover the detailed reaction pathway of NO3RR, in situ electrochemical ATR-FTIR spectroscopy was employed under applied potentials ranging from −0.6 to −1.1 V vs. RHE to identify reaction intermediates, which were generated on the surface of the Pd-PCOF-2(Cu3) catalyst. The 3D in situ ATR-FTIR colormap spectra revealed distinct distributions of absorption peaks at various applied potentials (Fig. 7a). The intensity of these peaks gradually increased as the applied potential became more negative. The in situ ATR-FTIR spectra were scrutinized over the wavenumber interval of 4000–1000 cm−1, and the upward and downward bands corresponded to the formation of various nitrogen intermediates and the consumption of the corresponding reactants, respectively (Fig. 7b). The pronounced absorption peaks at around 3400 and 3228 cm−1 were attributed to the O–H stretching of *H2O and the N–H stretching of NH3, respectively.38 The intensity of these peaks augmented as the potential decreased from −0.6 to −1.1 V vs. RHE, indicative of the increase in NH3 production rate and an enhanced H2O molecule adsorption and dissociation process. Within the 2000–1000 cm−1 wavenumber domain, the absorption peak at 1639 cm−1 was attributed to *NO and *H2O.39 The weak but discernible absorption bands at 1357 and 1100 cm−1 were assigned to the N–O asymmetric stretching of *NO3 and *NH2OH, respectively.40 Moreover, the downward band at 1241 cm−1 was ascribed to the N–O antisymmetric stretching of *NO2 and exhibited intensified strengths at more negative potentials.41
Based on the above mechanistic studies and in situ ATR-FTIR spectra analysis, a reaction pathway for the NO3RR over Pd-PCOF-2(Cu3) might be deduced: NO3− → *NO3 → *NO2 → *NO → *NH2OH → *NH3 → NH3. Consequently, NO2− was a critical intermediate and its excessive accumulation could lower the reaction selectivity and efficiency. The H* generated at the catalytic sites could promote the hydrogenation of NO2−, but its oversupply could also facilitate the competitive HER, thereby degrading the selectivity of NO3RR. Therefore, the precise modulation of the conversion rate of NO2− and the supply rate of H* was crucial for enhancing both the reaction rate and the selectivity toward NH3. In Pd-PCOF-2(Cu3)-catalyzed NO3RR, Cu3 served as the primary active sites for the initial deoxygenation of NO3− to the NO2− intermediate. Subsequently, Cu3 partially hydrogenated NO2− to NH3 while the unconverted NO2− migrated to the Pd-porphyrin for subsequent hydrogenation, which could not only effectively mitigate the accumulation of the detrimental NO2− intermediate but also accelerate the overall NO3− to NH3 conversion kinetics. Furthermore, the tailored hydrophobic microenvironment could enable precise modulation of the H* supply for expediting the NO2− hydrogenation rather than the HER. In short, an accelerated catalytic mechanism via synergistic tandem of bimetallic site and modulation of the hydrophobic microenvironment was elucidated (Fig. 8).
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