ABSTRACT
Conventional olefin epoxidation suffers from poor atomic economy and significant environmental/economic burdens due to the reliance on harsh oxidants. While electrochemical epoxidation using water as an oxygen source presents a sustainable alternative, existing systems remain hampered by noble‐metal dependence or inefficiency. To address this, we design a core‐shell nanostructure integrating titanium silicalite‐1 (TS‐1) nanozeolite with Mn‐N‐C (TS‐1@Mn‐N‐C). Critically, the interfacial synergy drives a tandem catalytic process: Mn‐N‐C sites electrosynthesize H2O2 via 2e− water oxidation, which directly migrates to adjacent TS‐1 active centers for selective epoxidation. Such spatial coupling ensures maximized H2O2 utilization and enhanced catalytic efficiency. As expected, TS‐1@Mn‐N‐C achieves exceptional performance for the epoxidation of cyclooctene to 1,2‐epoxycyclooctane in neutral electrolytes, outperforming both individual components and recently reported benchmarks. In situ characterizations combined with theoretical calculations reveal that the TS‐1@Mn‐N‐C interface lowers the energy barrier for H2O2 activation toward reactive η‐Ti‐OOH intermediates, enabling efficient and sustained epoxidation. The catalyst also shows broad substrate applicability, highlighting its potential as a sustainable and cost‐effective solution for electrochemical olefin epoxidation. This work pioneers a dual‐site interface strategy to optimize reaction kinetics and advance green chemical synthesis.
Keywords: electrochemical epoxidation, interfaces, Mn‐N‐C, tandem reactions, Ti‐Si zeolites
Core–shell interface of TS‐1@Mn‐N‐C enables in situ generation of high‐concentration H2O2 and its spatially confined activation toward epoxidation‐active η‐Ti‐OOH species, leading to highly efficient and continuous electrochemical epoxidation. The work successfully addresses the key challenge of inefficient mass transfer and slow kinetics caused by spatial separation in electrochemical‐chemical tandem catalysis.

1. Introduction
Olefin epoxidation is a fundamental process in chemical industries, as the resulting epoxides serve as essential intermediates for the production of epoxy resins, coatings, surfactants, pharmaceuticals, food additives, fragrances, etc. [1, 2, 3]. Currently, the industrial synthesis of epoxides primarily relies on the chlorohydrin process and catalytic aerobic or peroxide‐based oxidation [4, 5, 6], which suffer from several critical drawbacks, including harsh reaction conditions, high energy consumption, complex operational procedures, and significant safety risks. Meanwhile, they contribute substantially to carbon emissions due to the reliance on fossil fuel‐derived reagents and energy sources [7, 8]. There is an urgent need to develop cost‐effective and eco‐friendly alternatives that adhere to green chemistry principles and support carbon neutrality [9, 10].
Electrocatalysis powered by sustainable electricity offers a compelling alternative to the traditional olefin epoxidation approaches, featuring mild reaction conditions, high energy efficiency, and the use of water as a green oxygen source [11, 12]. Direct electrooxidation of olefins typically employs noble‐metal catalysts such as Pt, Pd, Ag, and their oxides [13, 14, 15, 16], which often yield not only epoxides but also aldehydes or carboxylic acids as byproducts [17, 18]. To circumvent the use of precious metals, manganese oxides have been explored as cost‐efficient alternatives; however, their application is severely limited by the low Faradaic efficiency (F.E. < 40%) for epoxidation [19], even after doping with a precious metal like Ir [20]. Strategies combining mediated reactions can significantly enhance epoxidation by generating reactive intermediates, such as HOX (X = Cl and Br) from halides, which react with olefins to produce target products and subsequently revert to their original states [21, 22, 23, 24]. Compared to environmentally hazardous halide mediators, the in situ generation of peroxides would enable more benign oxidation under the assistance of epoxidation‐efficient components like titanium silicalite‐1 (TS‐1). TS‐1, with a MFI zeolite topology, is highly effective for H2O2‐mediated epoxidation, producing high‐purity epoxides with minimal side reactions [25]. Recent studies have highlighted its application in electrochemical epoxidation, such as coupling the 2‐electron oxygen reduction reaction (2e− ORR) at the cathode with dispersed TS‐1 in electrolytes [26, 27, 28]. However, these systems struggle to fully utilize high‐concentration intermediates at electrode/electrolyte interfaces due to the spatial separation of H2O2 synthesis and organic oxidation, unfortunately leading to greater limitation from sluggish mass transfer and inevitable H2O2 dilution [29]. Moreover, the low solubility of gaseous O2 in electrolytes significantly restricts H2O2 generation at gas‐liquid‐solid triple‐phase interfaces [30], adversely affecting the overall reaction performance. In contrast, H2O2 production via the 2‐electron water oxidation reaction (2e− WOR) could offer a more efficient pathway for coupling with TS‐1 [31], which, however, remains unexplored. Designing dual‐site interfaces that synergistically integrate H2O2 electrosynthesis via 2e− WOR and subsequent H2O2 activation for epoxidation, while maximizing interfacial concentrations, is critical for advancing electrochemical olefin epoxidation.
Herein, we designed a core‐shell nanostructure composed of TS‐1 zeolite encapsulated by Mn‐N‐C (TS‐1@Mn‐N‐C), which orchestrated a tandem process at the interfaces: the H2O2 generated on Mn‐N‐C sites via 2e− WOR undergoes spatially confined transfer to TS‐1 centers for the selective epoxidation of olefins. TS‐1@Mn‐N‐C demonstrated exceptional performance for cyclooctene epoxidation in 0.1 m LiClO4 (pH 6.8), where pH‐neutral conditions effectively suppressed undesired side‐reactions (e.g., epoxide hydration and oxygen evolution) [32, 33]. At 2.0 V vs. Ag/AgCl, it achieved superior 1,2‐epoxycyclooctane selectivity (83.0%) and yield (64.7%), significantly outperforming both TS‐1 alone (70.8% selectivity, 17.7% yield) and Mn‐N‐C (64.2% selectivity, 45.0% yield). Combined experimental and theoretical investigations confirmed the synergistic interplay between H2O2 production and cyclooctene epoxidation at the TS‐1@Mn‐N‐C interfaces. Consequently, the Mn‐N‐C sites facilitated 2e− WOR to H2O2, while the TS‐1@Mn‐N‐C interface significantly reduced the energy barrier for H2O2 activation and promoted the formation of reactive η‐Ti‐OOH intermediates essential for the epoxidation. This synergy minimizes the need for long‐range H2O2 diffusion and bulk accumulation by promoting its rapid utilization at the adjacent Ti site. Moreover, TS‐1@Mn‐N‐C exhibited broad applicability for the epoxidation of cyclic and chain olefins, underscoring its potential for practical electrosynthesis.
2. Results and Discussion
2.1. Materials Synthesis and Characterization
Initial screening of M‐N‐C electrocatalysts (M = Pd, Ag, Mn, Zn, Ni, and Co) for H2O2 electrosynthesis revealed Mn‐N‐C as the top performer (Figure S1). Afterward, the composite of TS‐1@Mn‐N‐C was fabricated via pyrolyzing polydopamine (PDA) coated TS‐1 (TS‐1@PDA) with a manganese acetylacetonate (Mn(acac)2) precursor under an inert atmosphere (Figure 1a). PDA coating was achieved on nanosized TS‐1 zeolites (∼ 100 nm) via the polymerization of dopamine monomers in a Tris‐HCl buffer, resulting in core‐shell TS‐1@PDA that was then dispersed into Mn(acac)2 solution. After the pyrolysis at 800°C, TS‐1@Mn‐N‐C nanocomposites were obtained. Fourier transform infrared (FT‐IR) spectroscopy and thermogravimetric analysis (TGA) were conducted to explore the above coating and pyrolysis process. In FT‐IR (Figure S2), the band at 1620 cm−1 on TS‐1@PDA was attributed to the vibration of a benzene ring, indicative of the encapsulation by PDA. Accordingly, the TGA showed the gradual weight loss of TS‐1@PDA from 100 to 800°C (Figure S3), associated with the carbonization of the external PDA layer [34].
FIGURE 1.

(a) Schematic illustration for the fabrication of TS‐1@Mn‐N‐C nanocomposites. (b) TEM, (c) HR‐TEM, (d) HAADF‐STEM, (e) linear‐EDS images, and (f) EDS‐mapping of TS‐1@Mn‐N‐C.
Scanning electron microscopy (SEM) showed negligible morphological differences among TS‐1, TS‐1@PDA, and TS‐1@Mn–N–C (Figure S4). As further identified by transmission electron microscopy (TEM, Figure 1b), there was a clear boundary (the white dashed line) between the TS‐1 core and the Mn–N–C coating. The d‐spacing of 1.11 nm observed on the core corresponded to the (200) lattice of TS‐1, while no lattice fringes could be discriminated in the Mn–N–C layer (Figure 1c). The aberration‐corrected high‐angle annular dark field scanning transmission electron microscopy (AC‐HAADF‐STEM) revealed predominantly atomically dispersed Mn with bright spots in both TS‐1@Mn‐N‐C and Mn‐N‐C samples (Figure 1d and Figure S5), indicating that isolated Mn sites constitute the major population of Mn species. This atomic‐level dispersion of Mn is critical for enhancing catalytic activity and stability, as it allows for more active sites exposed for reactions. The energy dispersive x‐ray spectroscopy (EDS) linescan (Figure 1e) and the corresponding mapping (Figure 1f) confirmed a core‐shell structure, with distinct elemental distribution patterns highlighting the core (Si, Ti, and O) and shell (C, N, and Mn) regions.
Furthermore, x‐ray diffraction (XRD) analysis presented the well‐preserved MFI topology of TS‐1 after pyrolysis (Figure S6), with the characteristic diffractions at 2θ = 7.8°, 8.8°, 23.2°, 23.8°, and 24.3° [35, 36]. X‐ray photoelectron spectroscopy (XPS) was then performed to analyze the chemical states of elements. The Mn 2p spectra confirmed the co‐presence of Mn2+, Mn3+, and Mn4+ in both TS‐1@Mn‐N‐C and Mn‐N‐C (Figure S7) [37]. Meanwhile, the N 1s spectra revealed characteristic pyridinic‐N, pyrrolic‐N, and Mn‐N species (Figure S8), while the O 1s profile showed Mn(VI)‐O features attributed to surface oxidation (Figure S9) [38, 39]. Compared to zeolite materials with poor conductivity, TS‐1@Mn‐N‐C exhibited greatly improved conductivity after carbon coating (Figure S10), conducive to the following electrochemical epoxidation. Argon adsorption‐desorption isothermals were carried out to characterize the pore structure of the different samples (Figure S11). TS‐1@Mn–N–C exhibited a typical type I‐B isotherm with a high surface area and large pore volume, suggesting that the porous Mn–N–C layers would not hinder substrate molecules from reaching the internal active sites of the TS‐1 core. Moreover, the pore distribution of TS‐1 remained unchanged in TS‐1@Mn‐N‐C associated with the well‐maintained framework.
To further understand the coordination environment and valence state of Mn in TS‐1@Mn‐N‐C and Mn‐N‐C, x‐ray absorption near‐edge structure (XANES) and extended x‐ray absorption fine structure (EXAFS) were analyzed, along with three references of Mn foil, MnO2, and Mn phthalocyanine (MnPc). The Mn K‐edge XANES results (Figure 2a and Table S1) showed that the absorption edge energies of Mn‐N‐C and TS‐1@Mn‐N‐C samples fell between those of Mn foil and MnO2, suggesting an average oxidation state between 0 and +4. Compared to Mn‐N‐C, TS‐1@Mn‐N‐C exhibited a distinct blue shift in the Mn K‐edge absorption, with its position closer to the MnPc reference. The results indicated that the spatial confinement by TS‐1 promotes a more ordered Mn‐N coordination environment, consistent with the Mn‐N coordination observed in MnPc, whereas free Mn‐N‐C likely adopts non‐planar disordered configurations. Notably, the slightly higher absorption edge energy of TS‐1@Mn‐N‐C compared to MnPc suggested strong interfacial interactions with the TS‐1 framework. To further clarify the local coordination environment of Mn, the Mn K‐edge EXAFS spectra were re‐fitted using a Mn‐N first‐shell contribution together with an additional Mn‐related second‐shell scattering path. To illustrate the local coordination environment, the prominent Fourier‐transformed k3‐weighted EXAFS (FT‐EXAFS) was primarily assigned to the Mn‐N first coordination shell (Figure 2b and Figure S12). TS‐1@Mn‐N‐C and Mn‐N‐C presented a prominent peak at 1.55 and 1.60 Å, respectively, corresponding to Mn‐N bonds, and a weaker second‐shell Mn‐related contribution (∼2.30 Å). These results indicate that Mn‐N coordination constitutes the dominant local environment, while a minor fraction of Mn species may experience secondary Mn‐related interactions. Although the weak Mn‐related second‐shell contribution suggests the presence of minor Mn–Mn interactions, this feature is shared by the compared Mn‐containing catalysts. The Mn‐N scattering path in TS‐1@Mn‐N‐C closely matched that of the MnPc reference, consistent with the XANES results. Therefore, the Mn sites in TS‐1@Mn‐N‐C are more appropriately described as predominantly atomically dispersed rather than exclusively isolated. Such secondary Mn‐related interactions may further modulate the electronic structure of the Mn sites and thus influence H2O activation and H2O2 generation. Accordingly, we performed a wavelet transform (WT) analysis to achieve higher resolution in R‐space (Figure 2c). The Mn‐N (1.55 Å) scattering path of TS‐1@Mn‐N‐C observed in R space was shorter than that of Mn‐N‐C (1.60 Å), indicating again the strong interfacial interactions. This is conducive to the tandem electrochemical‐chemical processes on the adjacent Mn and Ti sites.
FIGURE 2.

(a) Mn K‐edge XANES, (b) FT‐EXAFS, and (c) the corresponding WT of TS‐1@Mn‐N‐C, Mn‐N‐C, and Mn foil, MnO2 and MnPc references.
2.2. Electrochemical Epoxidation Performance and Mechanism
Before conducting electrochemical epoxidation, we characterized the cyclic voltammetry (CV) profiles of TS‐1, TS‐1@Mn‐N‐C, and Mn‐N‐C in 0.1 m LiClO4 (pH 6.8). The TS‐1 modified electrode exhibited a small current regardless of the presence or absence of cyclooctene (Figure 3a), indicating negligible electrocatalytic activity. By contrast, TS‐1@Mn‐N‐C and Mn‐N‐C showed obvious redox peaks in the CVs (Figure 3b,c). In the absence of cyclooctene, TS‐1@Mn‐N‐C displayed the reduction of Mn4+→Mn3+ and Mn3+→Mn2+ at more positive potentials than Mn‐N‐C [40, 41], indicating the higher activity of Mn sites strongly interacted with TS‐1. Upon the addition of cyclooctene, the redox peaks were obviously weakened, as cyclooctene epoxidation on the catalyst surface consumed the reactive oxygen species (ROS) that were originally responsible for the Mn‐related redox process.
FIGURE 3.

CV curves of (a) TS‐1, (b) TS‐1@Mn‐N‐C, and (c) Mn‐N‐C in 0.1 m LiClO4 (pH 6.8) with/without 10 mm cyclooctene.
Afterward, the epoxidation performance was evaluated at 1.4 ∼ 2.0 V vs. Ag/AgCl in a 0.1 m LiClO4 aqueous mixed solution with 10 mm cyclooctene (Figure 4a). The conversion and epoxide yield followed the order of TS‐1@Mn‐N‐C > Mn‐N‐C > TS‐1. In contrast to bare TS‐1 with negligible activity, TS‐1@Mn‐N‐C and Mn‐N‐C presented obvious cyclooctene conversion and 1,2‐epoxycyclooctane yield, suggesting the key contribution to electrochemical epoxidation by Mn‐N‐C sites. Although TS‐1@Mn‐N‐C only exhibited a slightly higher cyclooctene conversion than Mn‐N‐C, the yield of the target 1,2‐epoxycyclooctane was 2–3 fold higher at low potentials (1.4 and 1.6 V) and 30%–40% higher at high potentials (1.8 and 2.0 V), associated with the selective epoxidation enabled by the core‐shell interfaces. At 2.0 V vs. Ag/AgCl, it achieved superior selectivity of 83.0% and yield of 64.7%, significantly outperforming both TS‐1 alone (70.8% selectivity, 17.7% yield) and Mn‐N‐C (64.2% selectivity, 45.0% yield). Notably, under these conditions, the TS‐1@Mn‐N‐C and Mn‐N‐C electrodes show comparable impedance behavior (Figures S13 and S14), which indicates that the higher epoxide yield of TS‐1@Mn‐N‐C cannot be attributed solely to enhanced conductivity. The time‐dependent conversion of cyclooctene to 1,2‐epoxycyclooctane on TS‐1@Mn‐N‐C was in accordance with the visible decrease of cyclooctene (Figure S15), while the by‐product cyclooctanone, derived from the electrooxidation, was limited to a low level. Moreover, TS‐1@Mn‐N‐C afforded good recyclability for epoxidation with well‐retained conversion (> 70%), product selectivity (> 80%), and yield (> 55%) over 15 consecutive cycles (Figure 4b and Figure S16). The structural stability of TS‐1@Mn‐N‐C was further corroborated by the post‐reaction characterizations (XRD, TEM, and x‐ray absorption spectroscopy), which clearly identified the well‐preserved core‐shell structure with the consistent electronic/coordination environment (Figures S17–S19). In further comparison with recently reported catalysts for the (photo)electrochemical epoxidation of cyclic olefins [19, 20, 21, 42, 43, 44], TS‐1@Mn‐N‐C presented an outstanding overall performance with excellent selectivity and yield (Figure 4c and Table S2).
FIGURE 4.

(a) Epoxidation performance over TS‐1@Mn‐N‐C, Mn‐N‐C, and TS‐1 at 1.4 ∼ 2.0 V vs. Ag/AgCl in 0.1 m LiClO4 with 10 mm cyclooctene, and (b) cycling stability of TS‐1@Mn‐N‐C over 15 consecutive cycles at 2.0 V vs. Ag/AgCl. (c) Comparison between TS‐1@Mn‐N‐C with recent reports (Table S2) for the electrochemical epoxidation of cyclooctene. (d) In situ Raman spectra of TS‐1@Mn‐N‐C collected during cyclooctene epoxidation at 2.0 V vs. Ag/AgCl and (e) in situ EPR spectra of the analyte collected with DMPO as the trapping agent at 2.0 V vs. Ag/AgCl. (f) Charge‐yield curves of epoxidation yield on TS‐1@Mn‐N‐C with different quenchers.
In situ Raman spectroscopy monitoring of the epoxidation reaction revealed characteristic Mn‐O bending (Eg) and stretching (A1g) vibrations at ∼474.4 and ∼645.1 cm−1 (Figure 4d) [45], respectively. The progressive intensification of these bands with reaction time indicated continuous accumulation of Mn‐O species. Accordingly, EPR trapping experiments with 5,5‐dimethyl‐1‐pyrroline N‐oxide (DMPO) showed the presence of •OH and •OOH radicals (Figure 4e), which were derived from the initial step of 2e− WOR and the H2O2 activation at Ti sites, respectively. Upon adding cyclooctene, the •OOH signal decreased sharply, indicating consumption by Ti‐OOH mediated epoxidation. Concurrently, •OH signals slightly intensified, suggesting accelerated H2O2 generation and thus •OH formation due to the •OOH depletion. Quenching experiments with scavengers further supported this assumption (Figure 4f). The addition of catalase, which decomposes H2O2 caused a pronounced activity drop, as it directly reduced the key epoxidizing species of Ti‐OOH. In contrast, mannitol, as a •OH scavenger, had a weaker inhibitory effect, suggesting the activation of H2O2 as the rate‐determining step of epoxidation [46].
Accordingly, the time‐dependent measurements of H2O2 concentration using Mn‐N‐C and TS‐1@Mn‐N‐C, both in the absence and presence of cyclooctene, support a tandem process in which H2O2 is electrochemically generated at Mn‐N‐C and subsequently consumed at the TS‐1 component for cyclooctene epoxidation (Figure S20). The pronounced suppression of the steady‐state H2O2 concentration in the presence of cyclooctene indicates that electrogenerated H2O2 is rapidly consumed in the subsequent epoxidation reaction. Notably, this effect is much more significant for TS‐1@Mn‐N‐C than for Mn‐N‐C, supporting the role of TS‐1 in promoting efficient H2O2 utilization. Meanwhile, the low epoxidation activity of pristine M‐N‐C catalysts (M = Pd, Mn, Zn, Ni, Co, and Ag) further identified the active sites of TS‐1 for cyclooctene epoxidation (Figure S21). We next examined the influence of electrolyte composition (i.e., 0.1 m LiClO4, 0.05 m Na2SO4, and 0.1 m NaHCO3) to determine whether the conditions favoring H2O2 production are also optimal for epoxide formation (Figure S22). Although the H2O2 production rate increased in the order LiClO4 < Na2SO4 < NaHCO3, the corresponding epoxide yields did not follow the same trend. Notably, LiClO4 afforded the highest epoxide yield, despite exhibiting the lowest H2O2 production rate among the three electrolytes. These results indicate that bulk H2O2 generation alone does not determine the overall epoxidation efficiency. Instead, rapid interfacial utilization of electrogenerated H2O2 by the adjacent TS‐1 sites plays a critical role in directing the reaction toward epoxidation. These results collectively demonstrate that H2O2 is the crucial ROS for the epoxidation, generated electrochemically via Mn‐N‐C and subsequently activated by TS‐1 to form Ti‐OOH, the active species for epoxidation [47].
To further investigate the coupled H2O2 electrosynthesis and epoxidation processes at TS‐1@Mn‐N‐C interfaces, we conducted a series of control experiments (Figure 5a). Neither TS‐1 powder alone in O2‐saturated electrolyte (without bias, Case I) nor blank carbon cloth at 2.0 V vs. Ag/AgCl (Case II) exhibited notable activity (conversion < 10%), confirming the negligible background interference. Importantly, a physically mixed TS‐1/Mn‐N‐C electrode (Case III) afforded only 39% conversion and 35% epoxide yield. When Mn‐N‐C was coated on the electrode while TS‐1 was dispersed in the electrolyte (Case IV), the electrogenerated H2O2 at anode diffused randomly through the bulk electrolyte to reach TS‐1, resulting in the markedly lower conversion (44.0%) and yield (38.1%) compared to TS‐1@Mn‐N‐C (77.0% and 64.7%) deposited on the electrode (Case V). Since this electrochemical process primarily occurs at the electrode surface, dispersing TS‐1@Mn‐N‐C in the anolyte inevitably reduced activity (Case VI). The above comparison highlights the critical synergy between Mn‐N‐C and TS‐1: Mn‐N‐C electrogenerates H2O2 and rapidly transfers it to adjacent TS‐1, where the Ti sites confine and activate H2O2 for epoxidation. TS‐1 is indispensable because direct olefin epoxidation without H2O2 activation faces high energy barriers and ill‐defined pathways [48]. Increasing the size of the TS‐1 core led to a slight decrease in the 1,2‐epoxycyclooctane yield (Figure S23), suggesting that the epoxidation occurs predominantly at the TS‐1/Mn‐N‐C interface. Replacing TS‐1 with zeolites lacking Ti sites, such as S‐1 or ZSM‐5, resulted in a significant decline in reaction activity (Figure S24), confirming again the indispensable Ti sites for epoxidation. Moreover, the efficiency of electrochemical epoxidation was governed by the kinetic matching between the electrocatalytic H2O2 generation on the Mn‐N‐C shell and the chemical epoxidation on the TS‐1 core, with notable dependence on the relative concentrations of water and cyclooctene [16, 19, 20]. As the water concentration increased, the rate of H2O2 production and the corresponding epoxidation current both increased (Figure S25a), likely attributable to the enhanced electrolyte conductivity. Meanwhile, increasing the substrate concentration led to a decrease in the epoxidation current, which can be explained by excessive adsorption of the substrate at the Mn‐N‐C shell, inhibiting the 2e− WOR pathway (Figure S25b).
FIGURE 5.

(a) Scheme of controlled reaction conditions (I: TS‐1@Mn‐N‐C in electrolyte, 0.1 MPa O2; II: carbon cloth, 2.0 V vs. Ag/AgCl; III: TS‐1 mixed with Mn‐N‐C physically; IV: TS‐1 in electrolyte, Mn‐N‐C on electrode, 2.0 V vs. Ag/AgCl; V: TS‐1@Mn‐N‐C on electrode, 2.0 V vs. Ag/AgCl; VI: TS‐1@Mn‐N‐C in electrolyte, 2.0 V vs. Ag/AgCl, the Ti and Mn content was controlled as the same in Cases III‐VI. DFT calculated Gibbs free energy diagram for (b) 2e− WOR and (c) H2O2 activation.
As a direct comparison, the thermal catalytic system using either TS‐1 or TS‐1@Mn‐N‐C required as high as 7.5 wt.% H2O2 concentration, a staggering 75‐fold higher than that produced in the electrocatalytic system with TS‐1@Mn‐N‐C, to achieve the same product yield under identical reaction conditions (Figure S26). This striking contrast vividly demonstrates the superior efficiency enabled by the interfacial synergism for the epoxidation. Notably, the electrocatalytic system with TS‐1@Mn‐N‐C offers additional advantages, including facile catalyst recovery and continuous operation capability through successive substrate additions to the electrolyte, enabled by the in situ H2O2 generation via 2e− WOR. In cycling tests (Figure S27), the electrocatalytic system exhibited progressively enhanced activity, ultimately surpassing the performance of conventional TS‐1‐H2O2 thermo‐catalysis after five consecutive runs without electrolyte replacement. These findings confirm that the electrochemical epoxidation maintains stable efficiency despite the consumption of ROSs, attributable to the continuous electrosynthesis and efficient utilization of H2O2.
Density functional theory (DFT) calculations were further conducted to acquire deeper mechanistic insights into the tandem H2O2 electrosynthesis‐chemical epoxidation occurring at the TS‐1@Mn‐N‐C interfaces (Figure 5b,c). The calculations mapped the Gibbs free energy landscape for the reaction pathway leading to the formation of the key epoxidation species, η‐Ti‐OOH [25].
The computational model was constructed to represent the predominant Mn–N‐coordinated environment identified experimentally. Thus, we used the MFI structure with some Ti replacing Si as the calculation model for TS‐1, and placed a single‐layer Mn‐N‐C structure near the Ti site to simulate the TS‐1@Mn‐N‐C interface. The reaction pathway involves sequential steps of H2O adsorption/oxidation to H2O2 formation (Figure 5b), and subsequent η‐Ti‐OOH generation (Figure 5c). As revealed, the H2O2 generation is thermodynamically favorable on the Mn‐N‐C site, in comparison with the apparent energy barriers of TS‐1 (2.56 eV) and TS‐1@Mn‐N‐C sites (1.48 eV). This pronounced energetic advantage aligns with prior DFT studies highlighting the superior activity of well‐defined M‐N‐C sites for the initial 2e− WOR step to H2O2 [49], and quantitatively explains why the Mn‐N‐C site is the preferred location for H2O activation and H2O2 generation. Following H2O2 formation, its transfer and activation at the Ti site to form η‐Ti‐OOH is critical [50], in which the Lewis acidity of Ti4+ significantly weakens the O─O bond in H2O2, lowering the activation energy for oxygen transfer compared to free H2O2 [51]. The differential charge density analysis of H2O2 adsorption (Figure S28) visually demonstrated the cooperative interactions facilitated by the intimate TS‐1 and Mn‐N‐C interface in the TS‐1@Mn‐N‐C model. Importantly, DFT calculations showed a lower energy barrier for η‐Ti‐OOH formation at the TS‐1@Mn‐N‐C interface (0.17 eV) compared to that on pristine TS‐1 (0.48 eV) (Figure 5c), where the adjacent Mn‐N‐C site promotes the direct generation of the η‐Ti‐OOH structure from H2O2 on the Ti site, minimizing energy loss through intermediate states or inefficient H2O2 diffusion. These results are strongly supported by our experimental observations, where the TS‐1@Mn‐N‐C catalyst showed a visible increase of epoxide yield (∼20%) compared to separating TS‐1 in electrolyte under identical conditions (Figure 5a). Under operational (anodic) conditions, the Mn site is predominantly occupied by oxygen or hydroxyl groups (e.g., as Mn‐OH or Mn‐O), rendering it less active toward H2O2 decomposition [52], as evidenced by in situ Raman analysis (Figure 4d). The proximity and electronic coupling at the intimate TS‐1/Mn‐N‐C interface, combined with the oxidized Mn site (Mn‐OH), likely facilitate a more direct pathway toward η‐Ti‐OOH. Specifically, the Mn‐OH group could act as a proton acceptor or participate in hydrogen bonding, lowering the energy barrier for H2O2 adsorption and activation directly on the adjacent Ti site. This interfacial synergy facilitates efficient H2O2 activation at adjacent Ti sites and minimizes the need for long‐range diffusion of H2O2 through the bulk electrolyte.
It is worth noting that the EXAFS analysis also reveals a weak Mn‐related second‐shell contribution, suggesting that a minor fraction of Mn species may experience secondary Mn–Mn interactions or form small Mn ensembles. Such local structural perturbations may modulate the electronic structure and intrinsic reactivity of the single‐atom Mn sites and thus potentially influence H2O activation and H2O2 generation. Nevertheless, the present study primarily focuses on the synergistic coupling between the Mn‐containing shell and Ti sites at the TS‐1/Mn‐N‐C interface. In the Mn‐containing comparison systems used to establish the interface effect, the Mn‐related secondary structural contribution is not the distinguishing variable; therefore, it does not change our conclusion that the enhanced epoxidation mainly originates from the spatially confined coupling of H2O2 generation and Ti‐mediated H2O2 activation. A systematic investigation of the individual roles of Mn nuclearity and coordination environment in H2O2 generation will be pursued in future studies.
2.3. Substrate Scope of Electrochemical Epoxidation
In a further set of experiments, we examined the efficacy of TS‐1@Mn‐N‐C for the electrosynthesis of value‐added epoxides from various cyclic and chain olefins. It showed good compatibility for cyclic olefin substrates, including 1‐hexene, 1‐octene, cyclohexene, cyclopentene, cycloheptene, cyclooctene and styrene, with high selectivity and yield (Figure 6a and Table S2). For chain olefins (e.g., 1‐hexene and 1‐octene), TS‐1@Mn‐N‐C exhibited relatively lower activity, likely due to the absence of ring strain, a factor that typically distorts and activates the C═C bond. We further targeted propylene, a fundamental C3 chain olefin feedstock of paramount industrial importance, for further investigation. Its epoxidation product, propylene oxide (PO), is a multi‐million‐ton commodity chemical crucial for producing polyurethanes, propylene glycol, and other derivatives [53]. The electrochemical oxidation of propylene was carried out on TS‐1@Mn‐N‐C in a flow cell (Figure 6b). As schematically shown, the flow paths of propylene and electrolyte are on respective sides of the gas diffusion electrode, so that propylene and electrolyte are well mixed at the gas–liquid interface. Therefore, the overall reaction current is greatly improved compared with the H‐type electrolytic cell. The current with propylene was higher than that with N2, associated with the favorable epoxidation compared to the oxygen evolution reaction (OER). More importantly, the catalytic performance was quantitatively evaluated in terms of F.E. and yield (Figure 6c). The F.E. of PO increased steadily from 1.8 V to a maximum at 2.2 V vs. Ag/AgCl, before slightly decreasing owing to the extensive OER at 2.4 V vs. Ag/AgCl. In parallel, the PO yield showed a continuous increase with applied potential, reaching 680 µmol gMn −1 h−1 at 2.4 V vs. Ag/AgCl. To further clarify whether the superior performance in the gas‐diffusion configuration originates from the core‐shell architecture rather than simply from the presence of both catalytic components, additional control electrodes with sequentially coated TS‐1 and Mn‐N‐C layers were evaluated under otherwise identical conditions (Figure S29). The sequentially coated configurations exhibited lower propylene oxidation activity than the TS‐1@Mn‐N‐C core‐shell electrode, demonstrating that intimate nanoscale integration of the two components is also critical under gas‐diffusion conditions.
FIGURE 6.

(a) Conversion of various substrates and the corresponding yield and selectivity of epoxides on TS‐1@Mn‐N‐C. (b) Scheme and polarization curve for electrochemical propylene oxidation in a flow cell configuration, and (c) Partial current density and production rate of PO at varying potentials.
3. Conclusion
In summary, the designed TS‐1@Mn‐N‐C core‐shell electrocatalyst successfully integrates H2O2 electrosynthesis via efficient 2e− WOR on atomically dispersed Mn‐N‐C sites with subsequent in situ H2O2 activation for selective epoxidation on Ti sites into a nanostructure. TS‐1@Mn‐N‐C achieved a high yield (∼64.7%) and selectivity (∼83.0%) of cyclooctene to 1,2‐epoxycyclooctane, superior to TS‐1 and Mn‐N‐C, outperforming recent reports. Accordingly, in situ Raman and EPR spectroscopies confirmed the facilitated chemisorption and further epoxidation of cyclooctene on TS‐1@Mn‐N‐C interfaces owing to the synergistic H2O2 generation and TS‐1 epoxidation. Moreover, DFT calculations demonstrated that the TS‐1@Mn‐N‐C interface can adsorb the H2O2 molecules and facilitate the generation of η‐Ti‐OOH, which was conducive to the successive epoxidation. This synergistic coupling, facilitated by the intimate interfaces, enables highly efficient, selective, and stable electrochemical epoxidation of various olefins using water as the green oxygen source under mild conditions. This work provides a promising and sustainable strategy for epoxide production, aligning with green chemistry principles and offering significant advantages over conventional industrial processes. It should be noticed that the single‐atom Mn sites constitute the major local Mn environment, while the weak Mn‐related secondary coordination revealed by EXAFS may further modulate the electronic structure and intrinsic activity of the Mn sites. Elucidating the individual effects of Mn nuclearity and coordination environment on electrosynthesis will be an important direction for future investigation.
Author Contributions
Wenbiao Zhang: funding acquisition, Writing – original draft, Writing – review and editing, conceptualization, software. Guanqiao Zhang: investigation. Wanling Zhang: investigation, validation. Kun Yu: methodology, investigation. Di Pan: investigation, formal analysis. Zhuxin Gui: investigation, data curation. Yi Tang: funding acquisition, writing – original draft, conceptualization, supervision, writing – review and editing. Qingsheng Gao: conceptualization, funding acquisition, writing – original draft, supervision, writing – review and editing.
Funding
This work was supported by the National Natural Science Foundation of China (22501107, 22575099 and 22688201), Science and Technology Project in Guangzhou (202102070001), Fundamental and Interdisciplinary Disciplines Breakthrough Plan of the Ministry of Education of China (JYB2025XDXM802), Guangdong Province International Science and Technology Cooperation Project (2025A0505020057), Guangdong Basic and Applied Basic Research Foundation (2026A1515010789), and Science and Technology Commission of Shanghai Municipality (2024ZDSYS02).
Conflicts of Interest
The authors declare no conflicts of interest.
Supporting information
Supporting File: advs77922‐sup‐0001‐SuppMat.docx.
Acknowledgements
This work was supported by the National Natural Science Foundation of China (22501107, 22575099 and 22688201), Science and Technology Project in Guangzhou (202102070001), Fundamental and Interdisciplinary Disciplines Breakthrough Plan of the Ministry of Education of China (JYB2025XDXM802), Guangdong Province International Science and Technology Cooperation Project (2025A0505020057), Guangdong Basic and Applied Basic Research Foundation (2026A1515010789), and Science and Technology Commission of Shanghai Municipality (2024ZDSYS02).
Contributor Information
Yi Tang, Email: yitang@fudan.edu.cn.
Qingsheng Gao, Email: tqsgao@jnu.edu.cn.
Data Availability Statement
The data that support the findings of this study are available in the supplementary material of this article.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Supporting File: advs77922‐sup‐0001‐SuppMat.docx.
Data Availability Statement
The data that support the findings of this study are available in the supplementary material of this article.
