Combined catalyst–pathway design for efficient and green urea synthesis

Zhuohang Li , Xuezi Xing , Ruichao Zhang , Xue Zeng * and Ke Chu *
School of Materials Science and Engineering, Lanzhou Jiaotong University, Lanzhou 730070, China. E-mail: zengxue@lzjtu.edu.cn; chuk630@mail.lzjtu.cn

Received 2nd September 2025 , Accepted 22nd October 2025

First published on 22nd October 2025


Abstract

Urea electrosynthesis from CO2 + NO3 co-electrolysis (UECN) offers a promising pathway for sustainable urea synthesis, while necessitating rational catalyst/pathway design to boost CO2/NO3 co-activation and C–N coupling. Herein, we demonstrate an atomically dispersed Ag on oxygen vacancy (OV)-rich TiO2 (Ag1/TiO2−x) catalyst for efficient UECN. Theoretical calculations and in situ spectroscopic analyses reveal the synergy of OV-induced Ag1-OV and TiOV dual-sites in promoting the selective C–N coupling of *CO and *NO2 for target urea generation. Notably, with the integration of plasma-assisted air-to-NOx conversion and CO2 + NOx co-electrolysis, Ag1/TiO2−x achieves an exceptional urea faradaic efficiency of 75.7% and a urea yield rate of 74.6 mmol h−1 g−1 along with excellent catalytic stability.



Green foundation

1. We pioneer a plasma-electrocatalytic pathway for efficient and green urea synthesis using atmospheric air (N2/O2) and CO2 as feedstocks, eliminating fossil fuel-derived NH3 required in conventional processes. The Ag1/TiO2−x catalyst enables selective C–N coupling of *CO/*NO2 intermediates via dual-site synergy for target urea generation.

2. Quantitatively, our strategy achieves a record-high urea faradaic efficiency of 75.7% and urea yield rate of 74.6 mmol h−1 g−1 along with excellent catalytic stability. Qualitatively, it bypasses the energy-intensive Haber–Bosch process and enables much lower energy consumption versus industrial urea synthesis under mild conditions.

3. Future work should optimize plasma energy efficiency using renewable electricity and scale catalyst loading and membrane-electrode assemblies for industrial deployment.


Urea (CO(NH2)2) plays a vital role in agricultural and industrial development.1 The industrial urea synthesis remains tethered to the energy-intensive Bosch–Meiser process under harsh conditions, giving rise to enormous global energy consumption and huge CO2 emissions.2 Electrocatalytic C–N coupling of CO2 and nitrogenous species (i.e., N2/NO3) offers a promising alternative pathway for sustainable urea synthesis by repurposing waste carbon/nitrogen sources while leveraging renewable energy.3–6 Recent studies have demonstrated the feasibility of urea electrosynthesis from CO2 + NO3 co-electrolysis (UECN), simultaneously realizing environmental remediation and value-added urea production.7 Nevertheless, UECN faces sluggish reaction kinetics due to the inefficient C–N coupling and low selectivity from competing reaction pathways (NO3-to-NH3 reduction reaction (NO3RR) and hydrogen evolution reaction (HER)).8–11 These challenges necessitate innovative UECN catalyst/pathway design to enhance activity, selectivity and stability for efficient and durable urea electrosynthesis.

Recent advances highlight single-atom catalysts (SACs) and oxygen vacancy (OV) engineering as promising strategies, in which SACs maximize atom utilization and tailor active sites, while OVs modulate the catalyst electronic structure to enhance intermediate stabilization and accelerate charge transfer.12–14 For instance, integrating metal single atoms into OV-rich oxides can effectively boost CO2 activation and concurrently leverage metal–support interactions to promote C–N coupling.14–18 Despite these merits, simultaneously achieving high urea yield rate and faradaic efficiency (FEurea) remains challenging due to the competitive adsorption of various C/N reactants, inherent scaling relations in multi-step reactions, and insufficient stabilization of key C/N intermediates.10 In addition, the NO3 feedstocks still indirectly depend on fossil fuels, which undermines the process sustainability, thus underscoring the need for nitrogen sources that require facile activation with sustainable production.19

Herein, we demonstrate an atomically dispersed Ag on OV-rich TiO2 (Ag1/TiO2−x) catalyst for efficient UECN. By combining extensive experimental and theoretical calculations, we elucidate how Ag single atoms and OV-rich TiO2−x synergistically promote C–N coupling while suppressing the competing side reactions towards efficient and selective urea generation. Notably, with integration of plasma-assisted air-to-NOx conversion and CO2 + NOx co-electrolysis, Ag1/TiO2−x exhibits outstanding UECN performance, achieving an FEurea of 75.7% and a urea yield rate of 74.6 mmol h−1 g−1 along with excellent catalytic stability.

Ag1/TiO2−x was synthesized through a combined hydrothermal/annealing method. The XRD pattern (Fig. S1) of Ag1/TiO2−x reveals the characteristic TiO2 diffraction peaks (PDF#86-1157) with no Ag-related species observed, indicating that the introduced Ag species are ultrasmall and highly dispersed on TiO2−x. A typical nanosheet morphology is observed in the TEM images of Ag1/TiO2−x (Fig. 1a and Fig. S2a). The HRTEM (Fig. S2b) image of Ag1/TiO2−x displays clear lattice fringes with an interplanar distance of 0.352 nm, assigned to the (101) plane of Ag1/TiO2−x. The AC-STEM (Fig. 1b) image of Ag1/TiO2−x displays numerous atomically dispersed bright spots, assigned to isolated Ag atoms. The atomic-level isolation of Ag species can be further confirmed by the corresponding atomic intensity line scanning and 3D surface intensity profile (Fig. 1c). Elemental mapping images of Ag1/TiO2−x (Fig. 1d) reveal a homogeneous dispersion of Ag atoms on the TiO2−x substrate. Inductively coupled plasma analysis shows that the Ag content is 3.37 wt%. The EPR spectra (Fig. S3) display much stronger g-signals of TiO2−x and Ag1/TiO2−x relative to bulk TiO2, indicating the existence of rich oxygen vacancies (OVs) on both TiO2−x and Ag1/TiO2−x. Meanwhile, Ag1/TiO2−x exhibits a similar g-signal intensity to TiO2−x, implying that the introduced Ag species have little impact on the OV concentration of TiO2−x.


image file: d5gc04601g-f1.tif
Fig. 1 (a–d) Characterization of Ag1/TiO2−x: (a) TEM image, (b) AC-STEM image and the corresponding (c) intensity line scanning profile and 3D intensity profile, and (d) elemental mapping images. (e–h) Ag K-edge XAS analyses: (e) XANES spectra, (f) EXAFS spectra, (g) EXAFS fitting curve of Ag1/TiO2−x and (h) wavelet transform analyses of Ag foil, Ag2O and Ag1/TiO2−x.

XAS is used to study the coordination and valence environment of Ag1/TiO2−x. The XANES (Fig. 1e) spectra reveal that the Ag K-edge of Ag1/TiO2−x is located between Ag foil (0) and Ag2O (+1), and linear fitting analysis reveals an average Ag valence state of +0.65 for Ag1/TiO2−x (Fig. S4). The EXAFS spectra (Fig. 1f) of Ag1/TiO2−x exhibit prominent Ag–O coordination with no Ag–Ag coordination (2.75 Å) observed, suggesting that the loaded Ag species are atomically dispersed on the TiO2−x substrate,20–22 thus ruling out the formation of Ag nanoparticles or clusters. Quantitative EXAFS fitting analysis (Fig. 1g) shows that the isolated Ag atoms are coordinated with two surrounding O atoms, forming an Ag–O2 geometric unit (Fig. 1g, inset, Table S1). The corresponding wavelet transform contour plots (Fig. 1h) reveal a sole intensity maximum of Ag–O at 3.9 Å−1 for Ag1/TiO2−x, further confirming that isolated Ag atoms are highly dispersed on the TiO2−x substrate.

DFT calculations were carried out to elucidate the electronic structure of Ag1/TiO2−x (Fig. S5). Differential charge density maps (Fig. S6) show more enriched electron density of Ag1/TiO2−x compared to TiO2, TiO2−x and Ag1/TiO2, suggesting that OV and Ag1 are both favorable for boosting the electronic interaction and this is further verified by the remarkable Ag/O/Ti orbital hybridization shown by the partial density of states (PDOS, Fig. S7). In addition, Ag1/TiO2−x reveals the equilibrium energy and temperature states below 698 K (Fig. S8) during the simulation, verifying the excellent thermodynamic stability of Ag1/TiO2−x. Furthermore, the Ag1 introduction modulates the electronic structure of TiO2−x to cause a decreased work function of Ag1/TiO2−x (Fig. S9), thereby facilitating efficient proton-coupled electron transfer to promote the electrocatalytic UECN kinetics.23–25

The electrochemical UECN performance of Ag1/TiO2−x was first evaluated in an H-cell containing a CO2-saturated electrolyte (0.1 M KNO3 and 0.1 M KHCO3).26 Liquid and gas products were detected using colorimetric and gas chromatographic methods (Fig. S10), respectively. Linear sweep voltammetry (LSV, Fig. S11a) curves show that compared to the Ar-saturated electrolyte, the CO2-saturated electrolyte presents a relatively higher current density (j), suggesting the pronounced catalytic UECN activity of Ag1/TiO2−x. A chronoamperometric test for 1 h of electrolysis at various potentials (Fig. S11b) was then performed to quantitatively determine the produced urea on Ag1/TiO2−x. As shown in Fig. 2a, Ag1/TiO2−x exhibits the highest FEurea of 40.1% with a corresponding urea yield rate of 25.9 mmol h−1 g−1 at −0.7 V, which are higher than those of most reported catalysts (Table S2). The FEs of other by-products were also tested with NH3 being the primary by-product (Fig. 2b).


image file: d5gc04601g-f2.tif
Fig. 2 (a) UECN performances of Ag1/TiO2−x at different potentials. (b) FEs of different products on Ag1/TiO2−x. (c) 13C NMR spectra of the 13CO(NH2)2 standard sample and those fed with 13CO2 after electrolysis at −0.7 V. (d) Schematic diagram of the flow cell. (e) LSV curves of Ag1/TiO2−x in an H-cell and flow cell. (f) UECN performances of Ag1/TiO2−x at different potentials in the flow cell. (g) Comparison of urea yield rates and FEurea in the H-cell and flow cell. (h) Comparison of the catalytic performance between Ag1/TiO2−x and recently reported catalysts.

Several tests were carried out to verify the N/C sources of the produced urea. 1H nuclear magnetic resonance (NMR) experiments show that using 15NO3 as the N-source results in a characteristic doublet chemical shift of CO (15NH2)2 (Fig. S12), while employing 13CO2 leads to a typical singlet chemical shift of 13CO(NH2)2 (Fig. 2c), evidencing that urea is exclusively produced through combined CO2 and NOx. Fig. S13 shows negligible urea detection without the CO2 feeding gas, in an NOx-free electrolyte or at the open circuit potential (OCP), suggesting that the generated urea originates from the UECN process. We further studied the long-term electrolysis of Ag1/TiO2−x, which showed a rather stable current density (Fig. S14), indicating the good long-term stability of Ag1/TiO2−x. In addition, as shown in Fig. S15 during the eight consecutive electrolysis cycles, FEurea and urea yield rate show no obvious changes, indicating the outstanding cycling stability of Ag1/TiO2−x.27–29 After the stability test, Ag1/TiO2−x retains the atomic Ag dispersion and Ag content (Fig. S16), confirming the robust structure of Ag1/TiO2−x.30,31

Generally, the low CO2 solubility and mass transfer limitation of an H-cell give rise to compromised UECN performance. To further improve the UECN activity of Ag1/TiO2−x, we employed a flow cell (Fig. 2d) that can enhance the CO2 mass transfer during UECN electrolysis. As shown in the LSV curves (Fig. 2e), Ag1/TiO2−x exhibits a much larger current density in the flow cell than in the H-cell, suggesting that the enhanced UECN activity of Ag1/TiO2−x is enabled by the flow cell. Quantitative measurement at various potentials (Fig. 2f and Fig. S17) shows that Ag1/TiO2−x in the flow cell reaches the maximum FEurea of 66.1% with the corresponding urea yield rate of 61.6 mmol h−1 g−1, significantly outperforming its H-cell counterpart (Fig. 2g) and most reported catalysts (Fig. 2h and Fig. S18). Moreover, the current density remains virtually constant during 36 h of continuous electrolysis (Fig. S19) and there are no significant changes in the UECN performances for eight consecutive electrolysis cycles (Fig. S20),32,33 highlighting the excellent UECN performance of the Ag1/TiO2−x/flow cell toward efficient and durable urea electrosynthesis.

To elucidate the underlying reasons for the enhanced UECN performance of Ag1/TiO2−x, operando FTIR spectroscopy was first employed to detect the key intermediates generated during the UECN electrolysis at various potentials. As displayed in Fig. 3a and b, Ag1/TiO2−x exhibits a pronounced infrared band of *NO2 at 1430 cm−1.34 The infrared bands probed at 2050 cm−1 and 1330 cm−1 are assigned to *CO and *COOH, respectively.35 The infrared band at 1400 cm−1 corresponds to the stretching mode of the C–N bond, while the bands at 1580 cm−1 and 1690 cm−1 are assigned to the generated *CONO2 and *CONH2 intermediates, respectively.36,37 The pronounced bands of C–N bonds and *CONO2 and *CONH2 intermediates alongside the urea-related band (∼1170 cm−1)26 collectively confirm that Ag1/TiO2−x can effectively drive the UECN process and promote C–N coupling towards urea generation. Furthermore, online DEMS measurements (Fig. S21) show the distinct signals of *CONO2 (m/z = 74), *CONH2 (m/z = 44), *NO2 (m/z = 46), *CO (m/z = 28) and *COOH (m/z = 45), while no signals of *NO2H (m/z = 47) can be found. The absence of the *NO2H intermediate and the presence of *CONO2 and *CONH2 intermediates disclose that Ag1/TiO2−x preferentially proceeds through the *CO + *NO2 coupling pathway (*NO3 → *NO2 → *CONO2 → *CONOOH → *CONO → *CONHO → *CONH → *CONH2 → *CO NO2NH2 → urea) to drive the UECN process towards urea formation.


image file: d5gc04601g-f3.tif
Fig. 3 Operando FTIR spectra of (a and b) Ag1/TiO2−x and (c) TiO2−x during UECN electrolysis at various potentials. (d and e) Operando Raman spectra of (d) Ag1/TiO2−x and (e) TiO2−x during UECN electrolysis at various potentials.

In stark contrast, pristine TiO2−x (Fig. 3c) exhibits the dominant *CO band at 2050 cm−1 but negligible C–N (1400 cm−1), *CONO2 (1580 cm−1) and CONH2 (1690 cm−1) signals, highlighting its limited C–N coupling capability despite efficient CO2 → *CO conversion. This is further supported by the operando Raman spectra, where pristine TiO2−x displays a weak N–C–N stretching band (Fig. 3e), in contrast to the much stronger N–C–N band observed in Ag1/TiO2−x (Fig. 3d). These operando FTIR/Raman results underscore the synergistic roles of Ag1 and TiO2−x in enhancing the UECN process, where TiO2−x facilitates the reduction of CO2 to *CO while Ag1 promotes the conversion of NOx to *NO2 and drives the C–N coupling of generated *NO2 and *CO for urea formation.

Theoretical computation was utilized to clarify the UECN mechanism of Ag1/TiO2−x. According to the previous XAS (Fig. 1e–h) and DFT results (Fig. S5–S7), four active sites on Ag1/TiO2−x are considered: the pristine Ti site, the Ag single-atom site (Ag1), the OV-adjacent Ti site (TiOV), and the OV-adjacent Ag single-atom site (Ag1-OV). Fig. 4a shows that among all four sites, NO3 is mostly preferentially adsorbed on the Ag1-OV site while *CO2 is mostly preferentially adsorbed on the TiOV site. Accordingly, in the UECN process, the Ag1-OV site mainly drives NO3 reduction while the TiOV site drives *CO2 reduction. The formed C-intermediates on the TiOV site and N-intermediates on the Ag1-OV site would undergo C–N coupling towards urea formation.


image file: d5gc04601g-f4.tif
Fig. 4 (a) Adsorption free energies of *CO2 and *NO2 on various active sites (Ti site, Ag1 site, TiOV site and Ag1-OV site) on Ag1/TiO2−x. (b and c) Free energy barriers of (b) coupling of *NO2 with various C-intermediates and (c) coupling of *CO with various N-intermediates. (d) Free energy diagrams of CO2 → *CO pathways. (e and f) Calculated TS energy barriers for the migration of (e) *CO from the TiOV site to the Ag1-OV site and (f) migration of *NO2 from the Ag1-OV site to the TiOV site. (g) Free energy diagrams for the electrocatalytic C–N coupling of the CO2 + NO3 pathway on Ag1/TiO2−x.

Previous operando FTIR results (Fig. 3a–c) indicate that *NO2 is the critical N-intermediate in the UECN process. After analyzing the free energy barriers for the C–N coupling of *NO2 with various C-intermediates (Fig. 4b and Fig. S22, S23), it is found that *NO2 coupling with *CO shows the lowest energy barrier, suggesting that *CO/*NO2 coupling is mostly energetically favored for urea formation. Likewise, for the C–N coupling of *CO with various N-intermediates, *CO coupling with *NO2 shows the lowest energy barrier (Fig. 4c and Fig. S24). Thus, the UECN process on Ag1/TiO2−x involves two key steps, namely, the initial CO2 → *CO and *NO3 → *NO2 and the subsequent C–N coupling of *NO2 and *CO to generate urea (*NO2 + *CO → *CONO2 → *CONOOH → *CONO → *CONHO → *CONH → *CONH2 → *CO NO2NH2 → urea). For the CO2 → *CO process, compared to the Ti site (0.73 eV), the TiOV site shows a much lower rate-determining step (RDS) energy barrier of 0.50 eV (Fig. 4d and Fig. S25–S27), indicating that TiOV serves as the primary site for CO2 → *CO reduction, thus ensuring a steady supply of the *CO intermediate necessary for the subsequent C–N coupling with *NO2 on the Ag1 site. For the NO3 → *NO2 process (Fig. S28), the Ag1-OV site (0.55 eV) exhibits a larger downhill energy change than the Ag1 site (0.83 eV), suggesting that the Ag1-OV site is more energetically effective in facilitating NO3 activation for *NO2 formation. These results demonstrate that OVs play a crucial role in enhancing the capabilities of both Ag1 and Ti sites for CO2/NO2 activation and reduction.

After the formation of *CO on the TiOV site and *NO2 on the Ag1-OV site, we further investigated the electrocatalytic C–N coupling process required for urea synthesis. Before C–N coupling, *CO must migrate from TiOV to Ag1-OV or *NO2 migration from Ag1-OV to TiOV must occur (Fig. S29 and S30). Transition state (TS) calculations reveal a lower energy barrier for *CO migration (0.63 eV, Fig. 4e) compared to *NO2 migration (1.72 eV, Fig. 4f), indicating a kinetically favored *CO migration from TiOV to Ag1-OV.38,39 This preferential *CO migration facilitates effective C–N coupling with *NO2 on the Ag1-OV site to form *CONO2. After the migration of *CO from the TiOV site to the Ag1-OV site, the first C–N coupling of *CO and *NO2 (*CO + *NO2 → *CONO2) and the second C–N coupling of *CONH2 and *NO2 (*CONH2 + *NO2 → *CONH2NO2) are energetically more favorable on the Ag1-OV site (0.37 eV and 0.21 eV) over the Ag1 site (0.68 eV and 0.53 eV) (Fig. S31–S33). This indicates that C–N coupling for urea formation is more favorable on the Ag1-OV site. All these findings demonstrate the synergistic role of the Ag1-OV and TiOV sites in promoting urea synthesis, where the TiOV site drives CO2 → *CO and the Ag1-OV site drives NO3 → *NO2. The migration of *CO from the TiOV site to the Ag1-OV site promotes selective C–N coupling with *NO2 for urea formation.

In the UECN process, competing side reactions such as the NO3RR and HER can impede selective urea synthesis. For the NO3RR, as shown in Fig. S22, the free energy required for *NO2 coupling with *CO to form *CONO2 is significantly lower than that required for *NO2 hydrogenation to NH3, thereby favoring selective C–N coupling over NH3 formation. Regarding the HER, the free energy calculations (Fig. S34) indicate that Ag1-OV and TiOV sites both preferentially bind NO3/CO2 over H. This selective NO3/CO2 adsorption over H is further supported by molecular dynamics (MD) simulations (Fig. S35), which show stronger catalyst–NO3 and catalyst–CO2 interactions compared to the catalyst–H interaction.40 These results demonstrate that Ag1/TiO2−x can well hamper the competitive NO3RR and HER to result in high UECN selectivity for urea generation.

For CO2 + NO3 co-electrolysis in the UECN process, NO3 feedstock is known to be derived mainly from the Haber–Bosch-derived NH3 that would compromise the sustainability and decarbonization objectives of electrocatalytic processes.19 These challenges underscore the need for nitrogen sources that require facile activation with sustainable production. A breakthrough lies in plasma-assisted nitrogen oxidation, which converts atmospheric air (N2/O2) into nitrogen oxides (NOx) via non-thermal plasma discharge.41 Absorption of NOx in alkaline solution generates NOx ions (NO2/NO3).41,42 Furthermore, plasma-derived NOx leverages air as the sole nitrogen source, bypassing the fossil fuel-dependent NH3 required for industrial urea synthesis and CO2 + NO3 co-electrolysis.43 Accordingly, by integrating plasma-assisted air-to-NOx conversion and CO2 + NOx co-electrolysis (Fig. 5a), we propose a tandem plasma-electrochemical pathway that enables a truly sustainable urea synthesis, offering a viable pathway to mitigate global energy consumption and CO2 emissions associated with the traditional industrial/electrochemical urea production.


image file: d5gc04601g-f5.tif
Fig. 5 (a) Schematic of the plasma-electrocatalytic process for urea synthesis from air and CO2. (b) LSV curves of Ag1/TiO2−x in CO2 + NO3 and CO2 + NOx electrolytes. (c) UECN performances of Ag1/TiO2−x at different potentials. (d) Comparison of urea yield rates and FEurea after 1 h of electrolysis in different electrolytes at optimal potentials. (e) Long-term test of Ag1/TiO2−x at −0.7 V. (f) Urea yield over time.

For the initial plasma-assisted air oxidation, the plasma discharge across the needle electrode arrays generates a bright plasma zone (Fig. S36a) where high-energy electrons powerfully activate N2/O2 molecules into reactive NOx (NO/NO2) gases, as evidenced by the gas stream transition from colorless to reddish-brown after 10 min of plasma discharge (Fig. S36b).42 These generated NOx gases are then absorbed into an alkaline KOH solution, resulting in the generation of NOx (NO2/NO3) ions. Quantitative UV-vis analyses (Fig. S37 and S38) reveal that a prolonged plasma discharge time linearly enhances NOx concentration, with NO2 as the dominant species (Fig. S39). After 60 min of continuous discharge, the total NOx concentration reaches 118.8 mM, comprising 107.3 mM NO2 and 11.5 mM NO3 (Fig. S40, S41 and Table S3). Moreover, our plasma system presents remarkable stability, maintaining >100 mM NOx yield across eight consecutive discharge cycles (Fig. S42), validating its robustness for stable production of NOx feedstocks required for the downstream electrochemical co-reduction of CO2 + NOx to urea.

We then examined the UECN performance of Ag1/TiO2−x in a flow cell using a CO2saturated electrolyte containing plasma-derived NOx (diluted to 0.1 M) and 0.1 M KHCO3. As shown in Fig. 5b, the LSV curves present a marked enhancement in current density for CO2 + NOx (90.2% NO2) co-electrolysis compared to CO2 + NO3 co-electrolysis (Fig. 5b). Such a performance enhancement is attributed to the more efficient 12-electron transfer process of the CO2 + NO2 pathway than the 16-electron pathway required for CO2 + NO3 co-electrolysis. As shown in Fig. 5c, the Ag1/TiO2−x catalyst exhibits outstanding UECN performance, achieving an FEurea of 75.7% and a urea yield of 74.6 mmol h−1 g−1 at −0.7 V, significantly superior to those obtained from CO2 + NO3 co-electrolysis (Fig. 5d). Electrocatalytic stability tests indicate the stable current density and consistent performance of Ag1/TiO2−x over eight electrolysis cycles (Fig. 5e), highlighting the excellent catalytic stability. To produce high-purity urea on a large scale, the electrode area is expanded to 5 × 5 cm2 with the catalyst loading increased to 20 mg. After 8 h of continuous electrolysis (Fig. 5f), 0.93 g of pure urea is obtained through electrolyte evaporation, sediment dissolution in benzene and benzene evaporation. This outcome highlights the technical viability of Ag1/TiO2−x catalysts for potential scalable urea production via a tandem plasma-electrocatalytic pathway.

In summary, Ag1/TiO2−x has been validated to be a highly efficient and durable UECN catalyst. Theoretical calculations and in situ spectroscopic analyses unveil the synergistic roles of Ag1-OV and TiOV sites on Ag1/TiO2−x in promoting urea synthesis, where the TiOV site drives CO2 → *CO and the Ag1-OV site drives NO3 → *NO2. The migration of *CO from a TiOV site to an Ag1-OV site promotes selective C–N coupling of *CO with *NO2 for urea formation. Strikingly, by integrating plasma-assisted air-to-NOx conversion and CO2 + NOx co-electrolysis, Ag1/TiO2−x presents outstanding UECN performance with an FEurea of 75.7% and a urea yield of 74.6 mmol h−1 g−1. The present work opens up new avenues for effective and eco-friendly urea production, highlighting the transformative potential of coupled plasma-electrocatalysis technologies in advancing green chemical synthesis.

Conflicts of interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Data availability

The data supporting this article have been included as part of the supplementary information (SI). Supplementary information is available. See DOI: https://doi.org/10.1039/d5gc04601g.

Acknowledgements

This work was supported by the National Natural Science Foundation of China (52561042), the Gansu Province Joint Research Fund (24JRRA859) and the Industrial Support Plan Project of the Gansu Provincial Education Department (2024CYZC-22).

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