Open Access Article
Xichang Liu†
a,
Yimin Jiang†a,
Wei Chen
a,
Jixiang Wua,
Yongmin He
a,
Yu-Cheng Huangb,
Ying-Rui Luc,
Yansong Zhou
*a and
Shuangyin Wang
*a
aState Key Laboratory of Chemo and Biosensing, College of Chemistry and Chemical Engineering, Advanced Catalytic Engineering Research Center of the Ministry of Education, Hunan University, Changsha, China
bCurtin Centre for Advanced Energy Materials and Technologies, WA School of Mines: Minerals, Energy and Chemical Engineering (WASM-MECE), Curtin University, Perth WA 6102, Australia
cNational Synchrotron Radiation Research Center, Hsinchu 300092, Taiwan
First published on 28th November 2025
The direct electrosynthesis of value-added esters from carbon monoxide (CO) represents a promising strategy for sustainable carbon utilization. In this study, we report the synthesis of propyl acetate with a faradaic efficiency of 16.5% and a partial current density reaching up to 24.7 mA cm−2 via CO electrolysis on a polarized Cu/Cu3N interface. Comprehensive mechanistic investigations elucidate a dual-pathway mechanism: ketene undergoes nucleophilic addition with n-propanol; and C2–C3 coupling occurs between nucleophilic *CH2CO and electrophilic intermediates such as *COHCOCO. Charge redistribution and interfacial polarization induced by the Cu/Cu3N interface reduce the activation barrier for the electrophilic addition between C2–C3 intermediates. These findings offer an alternative and sustainable pathway for the synthesis of esters through direct CO electroreduction.
Among the products of electrocatalytic CO reduction reaction (CORR), esters are particularly attractive due to their wide applications in fragrances, solvents, etc. Of these, propyl acetate, valued for its low toxicity, excellent solvency, and biocompatible characteristics, has been widely utilized in coatings, pharmaceuticals and biomedical fields.4 Given these diverse applications, global demand for propyl acetate is growing. Market research estimates its value at USD 1.56 billion in 2024, projected to reach USD 2.54 billion by 2034 with a compound annual growth rate of 4.98%, reflecting its expanding role across multiple sectors.5
Traditionally, propyl acetate is synthesized through the esterification of acetic acid with n-propanol, requiring harsh reaction conditions (363–403 K, >1 atm), corrosive acid catalysts, and energy-intensive purification procedures.6 CORR offers a sustainable alternative under ambient conditions, utilizing electricity as the driving force. This approach reduces carbon emissions and simplifies synthesis by integrating CO conversion and ester formation into a single step (Fig. 1). The realization of the electrosynthesis of esters in our previous work via CORR encourages us to develop an alternative sustainable pathway for propyl acetate production.7 However, selective production of propyl acetate via CORR remains a significant challenge, primarily due to the difficulty and complexity involved in the formation of C2/C3 intermediates.8,9 Efficient catalysts and mechanistic insights are essential to improve propyl acetate selectivity and yield.
Propyl acetate production via CORR involves the sequential formation of three C–C bonds and one C–O bond. Copper-based catalysts can achieve this goal by optimally adsorbing key intermediates, thus promoting C–C bond formation.7 A Cu/Cuδ+ mixed valence system has been shown to effectively promote the C–C coupling process.10–12 However, Cuδ+ species derived from oxides are prone to reduction to metallic Cu under cathodic potentials.13 To address this challenge, strategies including introducing heteroatoms to form compounds such as copper oxides, borides, and nitrides have been developed to stabilize Cuδ+ during CO(2)RR.14–16 Among these, copper nitride (Cu3N) stands out due to its Cu–N bond maintained at the reductive potentials, thereby providing stable Cuδ+ sites during CO(2)RR.17,18 Moreover, recent studies indicate that Cu–N-based catalysts can enhance the stabilization of C3 intermediates, which may promote propyl acetate formation pathways.19
Herein, we report the electrosynthesis of a substantial amount of propyl acetate via CORR on a Cu/Cu3N electrocatalyst. The integration of Cu3N onto metallic Cu generates coherent interfaces that modulate the electronic structure and stabilize key intermediates, thereby promoting C–C and C–O bond coupling for propyl acetate production. The Cu/Cu3N catalyst achieves a considerable production of propyl acetate with a faradaic efficiency (FE) of 16.5% and a partial current density reaching up to 24.7 mA cm−2—approximately an order of magnitude higher than the previously reported value.7 A dual-pathway mechanism for propyl acetate formation is proposed. Beyond the n-propanol–ketene (CH2
C
O) addition reaction, we identify parallel C2–C3 intermediate coupling pathways involving *CH2CO and active C3 intermediates (e.g., *COHCOCO). These findings are supported by both experimental and theoretical results.
Guided by these insights, we synthesized the Cu/Cu3N electrocatalyst by electrochemically deriving it from N2 plasma-treated basic copper nitrate (Cu2(OH)3NO3, BCN). Both the as-prepared BCN and the N2 plasma-treated BCN (p-BCN) samples exhibit the monoclinic Cu2(OH)3NO3 phase (JCPDS no. 75-1779, Fig. 2a).21 Compared to the X-ray diffraction (XRD) pattern of BCN, the shifts of the characteristic (001) and (002) planes observed for p-BCN may be attributed to the formation of surface/interfacial heterostructures during N2 plasma treatment (Fig. S2). The scanning electron microscopy (SEM) analysis reveals the formation of dense nanoparticles with a size of approximately 10 nm on the surface of bulk BCN particles in the p-BCN sample, confirming the formation of a new surface phase with N2 plasma treatment (Fig. S3). X-ray photoelectron spectroscopy (XPS) reveals the coexistence of reduced Cu2+ species (Cu+ and/or Cu0) with Cu2+ (Fig. S4), suggesting the partial reduction of Cu2+ induced by N2 plasma treatment. The Cu LMM Auger spectrum further confirms that the reduced Cu2+ species are predominantly Cu+ species (Fig. 2b).22 In the N 1s spectrum of p-BCN (Fig. 2c), peaks attributed to nitrogen vacancies and the Cu–N bond in copper nitrides are observed, suggesting the formation of a N2 plasma treatment induced copper nitride phase on the BCN surface.19,23 In the transmission electron microscopy (TEM) image of p-BCN, lattice spacings of 0.220 nm and 0.269 nm, assigned to the (111) and (110) planes of Cu3N, were observed, confirming that the surface copper nitride phase is Cu3N.24,25 This is further supported by the results of Raman spectroscopy analysis in which the characteristic band of Cu3N at 660 cm−1 was observed (Fig. 2d and S5).26 High-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) and energy-dispersive X-ray (EDX) spectroscopy mapping further confirm the homogeneous distribution of Cu, N, and O throughout the p-BCN sample (Fig. 2e and f). In summary, these results demonstrate the successful introduction of Cu3N onto the Cu2(OH)3NO3 surface for the subsequent electrochemical derivation of Cu/Cu3N electrocatalysts. Moreover, the relative amount of Cu3N present on the catalyst surface was quantitatively estimated from the XPS N 1s spectra (Table S1). X-ray absorption spectroscopy was used to investigate the local atomic structure and valence electronic structure of the catalysts. The Cu K-edge X-ray absorption near-edge structure (XANES) spectra indicate that the oxidation state of Cu in p-BCN is slightly lower than that in BCN (Fig. 2g). This trend is consistent with the XPS results, indicating that N2 plasma treatment leads to the formation of reduced Cu species.27 The further pronounced shift of the absorption edge in the Cu K-edge spectrum of p-BCN after post-electrolysis indicates the reduction of the Cu2(OH)3NO3 phase under CORR conditions (Fig. 2g). The Fourier-transformed (FT) k3-weighted extended X-ray absorption fine structure (EXAFS) spectra of Cu reveal changes in the local coordination environment (Fig. 2h). Specifically, in BCN, the first-shell coordination bond length is 1.53 Å, corresponding to the Cu–O bond. In p-BCN, this bond length shortens to 1.46 Å due to the co-existence of the Cu–N bond and Cu–O bond. Notably, after electrolysis, the bond length shifts to 1.41 Å, which is attributed to the disappearance of Cu–O coordination and the dominance of the Cu–N bond.25,28 This result is further supported by wavelet-transformed (WT) k3-weighted EXAFS analysis (Fig. 2i), indicating the stable presence of Cu3N alongside the reduction of BCN under CORR conditions. Together with the results from XPS, Raman, and TEM analyses of the post-reacted samples, it is clearly indicated that the Cu–N bond associated with Cu3N can be stably retained, in contrast to the complete reduction of Cu2(OH)3NO3 to metallic Cu (Fig. S6 and S7). Collectively, these findings confirm the successful formation and structural stability of the Cu/Cu3N interface derived from p-BCN during CO2RR.
We investigated the CORR performance of the catalysts in a membrane electrode assembly (MEA) system (Fig. 3a). p-BCN derived Cu/Cu3N exhibited significantly enhanced CORR selectivity (Fig. 3b and Tables S2 and S3). At a current density of 150 mA cm−2, the FE for C2+ products increased from 71.5% to 80.6%. Notably, the BCN-derived catalyst demonstrated its outstanding advantages in the electrosynthesis of propyl acetate from CORR with a maximum FE of propyl acetate (FEpropyl acetate) of 8.0%, approximately four times higher than previously reported values.7 On the p-BCN-derived catalyst, this value was further enhanced to a maximum FEpropyl acetate of 16.5%, with the corresponding propyl acetate partial current density (jpropyl acetate) reaching up to 24.7 mA cm−2, both of which are record values to date (Fig. 3c and S10–S13). To further identify the origin of the enhanced catalytic performance, two control samples—pristine Cu2O and Ar-plasma-treated BCN (Ar-BCN)—were prepared and evaluated under identical CORR conditions (Fig. S14–S16). The results show that (i) the isolated Cu2O phase exhibits negligible selectivity toward propyl acetate, and (ii) depositing Cu2O onto the BCN surface does not improve propyl acetate selectivity. These findings indicate that the marked increase in propyl acetate selectivity cannot be attributed to residual Cu2O species on the p-BCN surface. This confirms that the Cu/Cu3N interface derived from p-BCN plays a decisive role in enhancing the faradaic efficiency for propyl acetate (FEpropyl acetate).
We further assessed the practical potential of electrosynthesis of propyl acetate via CORR. Productivity was evaluated at a current density of 150 mA cm−2. The p-BCN-derived catalyst achieved a propyl acetate yield of 227 µmol h−1 in a MEA with a working area of 4 cm2. Furthermore, co-feeding of CO and n-propanol—identified as a key intermediate in propyl acetate formation from CORR in a MEA7—into the MEA cell can significantly enhance the production rate of propyl acetate up to 682 µmol h−1. Further optimization of the gas–liquid mixture ratio can increase the n-propanol concentration, resulting in an elevated production rate of 779 µmol h−1 (Fig. 3d). Based on these remarkable performance metrics, we evaluated the scalability and industrial feasibility of propyl acetate production via the CORR process. A preliminary techno-economic analysis was conducted, incorporating both electrolyzer capital costs and the costs associated with the downstream separation of liquid products (Fig. S17a).32 The calculation results indicate that the production cost of one ton of propyl acetate via the proposed CORR route is $1084.3, which is significantly lower than the reference price for the liquid product ($1542.1), indicating a favourable plant-gate levelized cost and promising economic viability. Sensitivity analyses show that at electricity prices of $0.01–0.02 kWh−1 and cell voltages of 2.0–3.0 V, most operating conditions allow economically viable electrosynthesis of propyl acetate (Fig. S17b). These findings underscore the substantial economic potential of CORR-based electrocatalytic production of propyl acetate.
Other ester products, including methyl acetate, ethyl acetate, and butyl acetate, were also detected in the product stream. For the p-BCN-derived catalyst, the total ester FE reached 26.8% with a partial current density of 40.2 mA cm−2 (Fig. 3e), among which propyl acetate accounted for 72.5% of ester FE and up to 20.3% of all CORR products (Fig. 3f). These results further highlight the significant potential of the p-BCN-derived catalyst for selective propyl acetate production.
We then sought to investigate the underlying factors contributing to the enhanced CORR performance of p-BCN derived catalysts. Double-layer capacitance measurements indicated comparable electrochemical active surface area (ECSA) values of BCN (139 µF) and p-BCN (156 µF), implying that the enhanced selectivity of p-BCN toward propyl acetate arises from its improved intrinsic catalytic activity (Fig. S18a–e). Besides, p-BCN exhibited a 1.8-fold higher ECSA-normalized propyl acetate partial current density (Fig. S15f), demonstrating the superior catalytic capability of the Cu/Cu3N heterojunction for selective propyl acetate production.
The reaction microenvironment critically dictates product selectivity in a MEA. The anion exchange membrane (AEM) thickness is found to play a pivotal role by modulating ion transport and water permeation. Experimental results revealed that reducing the AEM thickness led to a pronounced decline in ester production: at equivalent current densities, the FEpropyl acetate decreased from 16.5% to 1.5% when the membrane thickness decreased from 100 to 40 µm (Fig. S19). Notably, no ester products were detected when employing the X37-50 Grade RT (50-micro-thick) AEM, despite its previously reported effectiveness for CORR.33 This is attributed to increased water permeation through the thinner AEM, which promotes competitive hydrolysis of ketene.34 Moreover, even at comparable thicknesses, substantial variations in FEpropyl acetate were observed among different AEMs, which might be attributed to differences in interfacial properties between the membrane and the catalyst (Fig. S19).
We studied the reactivity of n-propanol and ethanol toward ketene to understand the underlying mechanism. Varied amounts of ethanol and n-propanol were co-fed with CO into the MEA, respectively (Fig. 4b and c). There is a linear correlation between both the alcohol feed amounts and the ester yields. However, the slope for ethanol (0.543) was notably steeper than that for n-propanol (0.415), suggesting that ethanol reacts more readily with ketene than n-propanol. This observation aligns with the Gaussian calculations, which indicate a slightly lower activation energy for the ethanol–ketene reaction (0.435 eV) compared to that of the n-propanol–ketene reaction (0.440 eV) (Fig. 4d, e and S22). Therefore, ethyl acetate forms more readily than propyl acetate when more ethanol is available if the ketene–alcohol nucleophilic addition pathway was the sole operative mechanism. However, our experimental results clearly indicate the opposite trend. Accordingly, we propose a C2–C3 intermediate coupling pathway for propyl acetate formation in addition to the ketene–alcohol nucleophilic addition reaction.
We performed DFT calculations to assess the plausibility of the proposed C2–C3 coupling pathway. Specifically, the coupling barriers for various C2 and C3 species on Cu-based surfaces were computed (Fig. 4f, S23–25 and Table S4). Among all combinations, the couplings of *CH2CO to *COCOCO, *COHCOCO, and *COCOHCO to form a C5 intermediate exhibited lower Gibbs free energy change than that of the reaction between ketene and n-propanol as well as ethanol, indicating that these pathways are thermodynamically favourable for propyl acetate formation (Fig. 4g).
We conducted DFT calculations on Cu and Cu/Cu3N surfaces to gain further insight into the higher production of prolyl acetate on the p-BCN-derived catalyst than that on the BCN-derived catalyst (Fig. 5a). We took the C2–C3 coupling between key intermediates *CH2CO and *COHCOCO having the lowest Gibbs energy change as an example. The coupling of *CH2CO and *COHCOCO on Cu/Cu3N is both thermodynamically and kinetically favourable than pure Cu (Fig. 5b and S26). Moreover, charge difference density maps reveal enhanced charge redistribution of the surface adsorbed species at the coupling site on Cu/Cu3N, particularly at the Cu–N boundary (Fig. S27). This conclusion is further supported by Bader charge analysis. Notably, the *CH2CO intermediate exhibits a greater negative charge on the Cu/Cu3N surface (−0.17 e) compared to Cu (−0.12 e), reflecting an enhanced nucleophilic character. At the same time, *COHCOCO shows an increased positive charge (+1.13 e vs. +1.04 e on Cu), which strengthens the nucleophile–electrophile complementarity between *CH2CO and *COHCOCO, facilitating their coupling via an electrophilic addition mechanism (Fig. 5c and d). Notably, this behaviour contrasts with the gas-phase reactivity of ketene, which typically acts as an electrophile in the nucleophilic addition with n-propanol (path I). Consequently, the Cu/Cu3N interface not only stabilizes intermediates but also reverses the intrinsic electrophilic character of ketene, enabling an alternative coupling route (path II). PDOS analysis presents enhanced adsorbate–surface interactions between both *CH2CO and *COHCOCO and the Cu/Cu3N surface, providing more possibility for their further coupling (Fig. 5e, f and S28). Moreover, the Cu3d states exhibit greater localization near the Fermi level in the presence of Cu3N compared to those in pure Cu, resulting in enhanced surface electronic activity of Cu to promote the activation of intermediates and for efficient C–O bond formation. Collectively, these findings demonstrate that the Cu/Cu3N interface creates an electronically optimized environment that promotes C2–C3 electrophilic addition through synergistic charge redistribution and orbital alignment (Fig. 5g). Such interfacial control over product selectivity underscores the critical role of electronic structure engineering in CO electroreduction.
We therefore propose that the predominant formation of propyl acetate in the current system results from both the alcohol–ketene nucleophilic addition reaction and, to a significant extent, electrophilic addition between surface-stabilized C2 (*CH2CO) and C3 intermediates such as *COHCOCO. Specifically, the Cu/Cu3N interface offers a conducive environment for C–C and C–O bond formation through the stabilization of reactive intermediates, enhancement of their spatial proximity, and improved charge transfer across the heterojunction. These synergistic effects reduce the energy barriers for electrophilic addition of C2–C3 intermediates, thereby enabling an efficient and selective catalytic pathway for propyl acetate production. This dual-pathway mechanism rationalizes the observed high selectivity toward propyl acetate.
Supplementary information is available. See DOI: https://doi.org/10.1039/d5sc08178e.
Footnote |
| † These authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2025 |