Libin
Zeng
ab,
Xinyue
Wang
a,
Dashuai
Wang
b,
Xianyun
Peng
b,
Zhibin
Liu
b,
Na
Wu
b,
Kexin
Wang
ae,
Zhongjian
Li
ab,
Bin
Yang
ab,
Qinghua
Zhang
ab,
Lecheng
Lei
ab,
Paolo
Samorì
e and
Yang
Hou
*acd
aKey Laboratory of Biomass Chemical Engineering of Ministry of Education, College of Chemical and Biological Engineering, Zhejiang University, Hangzhou, China. E-mail: yhou@zju.edu.cn
bInstitute of Zhejiang University-Quzhou, Quzhou, China
cHydrogen Energy Institute, Zhejiang University, Hangzhou 310027, China
dSchool of Biological and Chemical Engineering, NingboTech University, Ningbo 315100, China
eUniversité de Strasbourg, CNRS, ISIS, 8 allée Gaspard Monge, Strasbourg, 67000, France
First published on 28th November 2025
Electrochemical conversion of methane (CH4) is a sustainable route for converting greenhouse gases into valuable liquid fuels and chemicals. However, achieving high-yield products at industrially relevant current densities remains a formidable challenge. Here, we report a machine learning-guided Mo–Cu dual-site cascade catalytic strategy, enabling selective modulation of key *CH3O and achieving ethanol (EtOH) electrosynthesis. This system delivers a current density of 103 mA cm−2 with an EtOH faradaic efficiency of 55.8% ± 0.2%, establishing new performance benchmarks. Mechanistic and DFT analyses reveal that CH4 is activated by a three-electron *O2−-mediated oxidation pathway, while *CH3 spillover from Mo to Mo–Cu active sites facilitates exothermic C–C coupling, leading to high-efficiency EtOH production. Techno-economic analysis suggests that integrating renewable electricity can lower the CH4-to-EtOH production cost from $2.12 per kg to $1.50 per kg within a decade, offering a 53% energy return. This work establishes a cascade-regulated, dual-site framework for efficient CH4-to-EtOH conversion and offers a framework for machine learning-assisted catalyst design, contributing to cleaner energy technologies and substantial reductions in greenhouse gas emissions.
Broader contextMethane electro-upgrading is a sustainable strategy to valorize the most abundant hydrocarbon while mitigating greenhouse gas emissions. However, the direct and selective conversion of CH4 to ethanol (EtOH) remains a great scientific challenge. Two central scientific questions have hindered progress: (i) how to efficiently activate the strong C–H bond of CH4 (439 kJ mol−1) under mild electrochemical conditions and (ii) how to stabilize reactive C1 intermediates (e.g., *CH3 and *CH3O) to enable controlled C–C coupling rather than side reactions such as methanol formation and complete oxidation. Here, we report a machine learning-guided Mo–Cu dual-site cascade strategy that selectively modulates the key *CH3O intermediate, achieving EtOH electrosynthesis with a faradaic efficiency of 55.8% ± 0.2% at a current density of 103 mA cm−2—establishing a new benchmark in CH4 electroconversion. Mechanistic investigations supported by DFT calculations reveal that CH4 is activated via a three-electron *O2−-mediated pathway, while *CH3 spillover from Mo to Cu sites facilitates exothermic C–C coupling toward EtOH. Techno-economic analysis further suggests that integrating renewable electricity can reduce the production cost from $2.12 per kg to $1.50 per kg within a decade, delivering a 53% energy return. |
The electrochemical direct partial oxidation of CH4-to-EtOH (CH4OR) under ambient conditions is a sustainable and promising alternative to traditional syngas refining and biomass fermentation processes (Fig. 1a and b). However, the dominance of competitive oxidation pathways leading to CO2 or side reactions presents challenges in electrochemical CH4-to-EtOH conversion.8,9 Recent efforts have explored direct CH4 electrooxidation as a potential route to oxygenates, but achieving high EtOH selectivity via efficient C–C bond coupling remains elusive, largely due to uncontrolled radical pathways and catalyst limitations.10,11
A critical bottleneck in electrochemical CH4-to-EtOH conversion is the modulation of the *CH3O intermediate,12–16 which is central to optimizing product selectivity and overall energy efficiency. While transition metal-based catalysts have shown potential in selectively electro-synthesizing EtOH via CH4OR, advanced modification strategies, such as the strong metal–support interaction (SMSI),17,18 morphology engineering,19,20 electronic structure regulation,21,22 and electrode/electrolyte interface optimization,23,24 have significantly improved the faradaic efficiency (FE) up to 68%. However, currently reported design methods often rely on empirical strategies, which lack the precision needed to optimize multiple interconnected catalytic properties simultaneously. Moreover, they are constrained by low production rates (<4.67 mmol gcat−1 h−1) and small operational current densities (<20 mA cm−2) in flow cell devices,16 largely hindering their industrial scalability.
To address these challenges, the machine learning method has emerged as a transformative tool in catalyst design, enabling the prediction of structure–activity relationships and accelerating the discovery of high-performance catalysts.25 By employing data-driven algorithms to explore compositional spaces and identify key catalytic descriptors, machine learning offers a systematic approach to unravel the complexity of multi-site catalysis. It is particularly effective in dual-site-driven systems, where it predicts optimal active site configurations and fine-tunes cooperative interactions to enhance intermediate generation, migration, and conversion pathways.25,26 Recently, Chen et al. demonstrated that dual-site cooperative strategies effectively activated CH4 and initiated reaction cascades. However, uncontrolled intermediate migration often leads to unforeseeable mixed products,19,20,27 underscoring the need for precise control over the catalytic behavior of *CH3O in cascade systems. Specifically, the generation, migration, and transfer of key *CH3O remain major bottlenecks, which largely limit EtOH selectivity and yield.
Herein, we report a machine learning-assisted dual-site-driven cascade strategy for CH4-to-EtOH conversion under ambient conditions. Guided by structure–activity relationship predictions, a Mo-doped Cu2Se catalyst stabilized by cetyltrimethylammonium chloride (Mo–Cu-CTAC) was identified as the optimal candidate. It achieves an optimal balance between *CH3O stabilization and migration through its dual-site interface. This cascade system achieved an EtOH FE of 55.8% ± 0.2% at a high current density of 103 mA cm−2 and a formation rate of 529.1 µmol h−1 cm−2, exhibiting record-breaking nearly 100% carbon selectivity toward the alcohol product in a gas-fed flow cell (100% alcohol product selectivity refers to all detectable carbon-containing products in the liquid phase, e.g., EtOH, with no detectable gas-phase carbon products). Mechanistic investigations combining density functional theory (DFT) calculations, in situ spectroscopy, isotope labeling, and kinetic isotope effect analysis revealed that CH4 activation occurs via a three-electron *O2−-mediated oxidation pathway, followed by *CH3O migration from Mo to Mo–Cu, enabling favorable C–C coupling. The CTAC-induced microenvironment enhanced CH4 enrichment and suppressed O2 accumulation, promoting EtOH selectivity. Techno-economic analysis forecasted that integrating renewable energy reduces the cost of CH4-to-EtOH conversion to $1.50 per kg within a decade, highlighting the dual advantages of economic feasibility and environmental sustainability.
As depicted in Fig. 2, the proposed framework employs a two-step machine learning assisted screening strategy to identify the optimal dual-site configuration for CH4-to-EtOH conversion. A computational database was established correlating *CH3O diffusion barriers and C–C coupling energies across over 300 M-Cu bimetallic catalysts (M = transition metals), as shown in Fig. 2a, revealing quantitative relationships between the local structure and catalytic behaviour. In Fig. 2b, the sure independence screening and sparsifying operator (SISSO) algorithm was applied to extract key descriptors, including d-orbital occupancy, electronegativity differences, and coordination environment, that govern CH4 activation and *CH3O generation. These interpretable descriptors retain the physical essence of catalytic mechanisms while reducing computational complexity. The electronic structure analysis (Fig. 2c) shows that the Mo–Cu pair optimally balances oxophilicity and electronic coupling, a configuration critical for highly selective EtOH production: Mo activates CH4, while Cu promotes *CH3O transfer and C–C coupling.
Among the screened catalysts, the overall structure–activity relationship exhibits a Mo–Cu dual-site cascade system which emerged as the most promising candidate owing to its balanced electronic coupling, enabling energetically favorable *CH3O migration (−0.93 eV) from Mo to Cu sites, as well as its optimal C–C coupling energetics. This approach underscores the critical role of electronic and structural tuning in achieving high efficiency, with the Mo–Cu dual-site system identified as optimal for CH4-to-EtOH conversion. Therefore, subsequent work mainly focuses on the synthesis of the selected Mo–Cu dual-site catalyst and the experimental validation of its electrocatalytic performance in CH4-to-EtOH conversion.
We further employed synchrotron-based X-ray absorption spectroscopy (XAS) to precisely characterize the local coordination environment of the Mo–Cu dual-site catalyst. The Mo K-edge X-ray absorption near-edge structure (XANES) spectrum of Mo–Cu2Se, positioned between Mo foil and the MoS2 reference (Fig. S11), in conjunction with Mo 3d XPS results, revealed that doped Mo existed in a state intermediate between Mo(III) and Mo(IV) states.31,32 The Fourier-transformed extended X-ray absorption fine structure (FT-EXAFS) spectra displayed a prominent peak at 2.16 Å (Fig. S11b), also corroborated by Raman vibrational features at ∼350 and ∼600 cm−1 (Fig. S12), both indicative of Mo–Cu bond formation.16 Artemis fitting results revealed that one Mo atom is coordinated with three Cu atoms and one Se atom, as shown in Fig. S13, forming a Mo–Cu3–Se coordination configuration, supported by an R-space fitting factor of 0.004 (Fig. S14). Wavelet transform (WT) analysis of the Mo–Cu dual-site catalyst showed a maximum intensity of approximately 8.5 Å−1 (Fig. S15), a distinctive feature absent in Mo foil, MoS2 and MoO3. These results demonstrated that the introduced Mo atoms acted as dopants, establishing a distinctive Mo–Cu3–Se coordination.
The Mo–Cu-CTAC system exhibits superior local reactant availability, as evidenced by a higher OH− ion concentration of 0.09 mol L−1 (Fig. S17), compared to the Mo–Cu dual-site (∼0.07 mol L−1) and the Cu only site (∼0.06 mol L−1). Charge distribution analysis also reveals a significantly enhanced surface charge density (20 mC m−2), surpassing the Mo–Cu dual-site (∼15 mC m−2) and the Cu only site (∼12 mC m−2), indicating improved charge transfer dynamics. Moreover, a stable and uniform local pH of 13–14 was maintained, contributing to stabilizing the catalytic microenvironment. COMSOL simulations (Fig. S17 and S18) further demonstrate that the increased local OH− concentration not only promotes the formation of reactive oxygen species (ROS), particularly *O2− radicals, but also correlates strongly with higher surface EtOH coverage. While the OER is not entirely suppressed under these alkaline anodic conditions, the interfacial environment in Mo–Cu-CTAC kinetically favors the three-electron ROS pathway over the four-electron O2 evolution route, effectively diverting oxidative equivalents toward CH4 activation and *CH3O formation. These optimized local conditions result in a high EtOH production of 0.10 mol L−1, as shown in Fig. S18, outperforming the Mo–Cu dual-site (∼0.07 mol L−1) and the Cu only site (∼0.05 mol L−1). In parallel, the incorporation of CTAC introduces long-chain quaternary ammonium cations that increase surface hydrophobicity, as confirmed by contact angle test results (Fig. S19 and S20a), promoting CH4 enrichment and limiting O2 accumulation near active sites16 (Fig. S21), thereby reinforcing the kinetic selectivity for CH4 oxidation. Post-electrolysis 1H nuclear magnetic resonance (1H NMR) analyses of both the anolyte and the catholyte detected no CTAC, and both the contact angle (Fig. S20b) and XPS N 1s binding energy (Fig. S20c) remained unchanged, indicating that the CTAC layer remains stably anchored to the catalyst surface. Based on the above results, the synergistic combination of Mo–Cu dual-site design and the optimized local microenvironment caused by CTAC enhances the performance of CH4-to-EtOH conversion.
Further optimization of doped Mo contents in CTAC-modified samples revealed that the CTAC-modified catalyst with the Mo–Cu dual site achieved the highest EtOH FE of 54.5% ± 0.3% with an optimal EtOH/O2 production ratio of 1.23 (Fig. 3b). Potential-dependent experiments demonstrated that maintaining a nearly 1
:
1 EtOH/O2 production ratio is critical for maximizing CH4-to-EtOH conversion efficiency (Fig. S30). This observation suggests a synergistic relationship between the OER and CH4OR, where the controlled release of oxygen facilitates a balanced reaction microenvironment, paving the way for the efficient formation of key intermediates in the CH4-to-EtOH conversion pathway.
To further validate the superior CH4-to-EtOH performance, a series of transition metal-doped Cu2Se samples were examined, among which the Mo–Cu-CTAC system achieved the highest EtOH FE of 54.5% ± 0.3% (Fig. 3c). Control experiments using MoSex-CTAC catalysts yielded methanol, formate and only a trace of EtOH (Fig. S31), confirming that only Mo facilitates ROS generation but lacks the ability to drive C–C coupling without Cu. Furthermore, the industrial applicability of Mo–Cu-CTAC at high current density was assessed in a flow cell equipped with a gas diffusion layer (Fig. S32 and S33). The integration of the gas diffusion layer in the flow cell ensured optimized mass transport and reaction kinetics, enabling the cascade system to achieve an impressive EtOH yield of 529.1 µmol h−1 cm−2 with a FE of 55.8% ± 0.2% at 1.9 V, corresponding to a high current density of 103 mA cm−2, with stable operation maintained over 20 h (Fig. 3d and e). Compared to other reported transition metal-based CH4OR catalysts, the Mo–Cu-CTAC system demonstrated an unparalleled activity and selectivity for EtOH production at high current densities (Fig. 3f).10,16,18,24,35–45 Although a-KB24 and CoNi2Ox38 exhibit excellent activity, the Mo–Cu dual-site system operates under oxidant-free, halide-free, and near-neutral conditions to achieve direct C–C coupling and EtOH production. Also, the cascade electrocatalytic system surpassed traditional thermal or photo catalytic processes, which suffer from low selectivity and elevated energy demands.
The detailed CH4-to-EtOH conversion process was further investigated at varying potentials and time intervals (Fig. 4a and b). A steady increase in positive peaks within the region of 3200–3600 cm−1, accompanied by broad band signals indicative of O–H stretching vibrations in alcohols, as well as bending vibrations of –OH at 1670 cm−1, signified EtOH formation. Simultaneously, a negative-going peak at 1620 cm−1 reflected continuous water consumption during the reaction.25 In Fig. 4c, positive peaks at 1420, 1390, 1258, 1210, and 1110 cm−1 were attributed to C–H bending vibrations of EtOH, *CH3O, and *CH3CH2O, O–O stretching vibrations of *CH3OO, and C–O stretching vibrations of *CH3CH2O, respectively.46–48 These intermediates exhibited a sequential trend of *CH3CH2O > *CH3O > *CH3OO, highlighting a stepwise transformation where *CH3OO is reduced to *CH3O and subsequently to *CH3CH2O. Time-resolved in situ Raman spectroscopy further revealed the dynamic formation of *CH3O at ∼1058 cm−1 and its subsequent conversion to EtOH, evidenced by the emergence of a broad band around 1350–1400 cm−1 (Fig. S35). These observations provide direct support for *CH3O as a key intermediate in the cascade CH4-to-EtOH pathway.
Isotope-labeling experiments using 13CH4 (99 atom%) unambiguously verified that both carbon atoms in the EtOH product originated from CH4, as evidenced by the dominant GC–MS molecular ion at m/z = 48 and characteristic fragment at m/z = 33 (Fig. S36). Control experiments with Na213CO3 as the electrolyte and unlabeled CH4 showed only unlabeled EtOH (m/z = 46 and 31), excluding carbonate as a carbon source under the applied conditions (Fig. S37). To deeply corroborate the proposed CH4-to-EtOH conversion pathway, isotope-labeling in situ ATR-FTIR experiments were subsequently conducted at 1.9 V using 13CH4 as the feeding gas. As shown in Fig. 4d, the characteristic peaks of 13C-labeled intermediates shifted to the lower wavenumbers due to the isotope effect.49 The formation of the 13EtOH product was confirmed and quantified by 13C-NMR spectroscopy (Fig. S38), demonstrating that the carbon in the EtOH product originated from CH4 oxidation. Combining these findings with free radical trapping results presented in Fig. 4e, we concluded that the *O2− radical acted as the active species generated during the CH4OR. This elucidates the catalytic pathway, wherein activated *CH3 underwent the transformation to *CH3OO, facilitated by the generation of *O2−, potentially involving a three-electron *O2−-mediated oxidation process. As shown in Fig. S39, the traditional four-electron OER process generates O2 through a concerted transfer of four-electron pathways. In contrast, the three-electron *O2−mediated oxidation pathway produces ROS such as *O2−, particularly under alkaline and dual-site catalytic conditions. These partially oxidized intermediates exhibit moderate oxidation potential for *CH3 radicals without overoxidation. On the Cu–Mo dual-site catalyst, this radical-mediated catalytic route is more compatible with cascade coupling pathways, allowing for stabilization and stepwise conversion of *CH3 to EtOH. Computational calculations of kinetic analysis in Table S2 support that the Mo–Cu-CTAC exhibits the highest formation rates for *CH3O (7.80 × 10−3 s−1), *CH3CH2O (6.40 × 10−3 s−1), and EtOH (4.20 × 10−3 s−1), highlighting the enhanced efficiency enabled by the synergistic interaction between the Mo–Cu dual-site and CTAC. Based on these experimental and kinetic insights, a detailed CH4-to-EtOH conversion mechanism was proposed (Fig. 4f). The Mo–Cu-CTAC system activated CH4, enabling its stepwise oxidation via *CH3, *CH3OO, and *CH3O to produce EtOH. Based on these findings, they collectively substantiate that reactive *O2− generated through a three-electron *O2−-mediated oxidation pathway played a pivotal role in driving CH4 oxidation and stabilizing key *CH3O intermediates, where *O2− radicals initiate C–H activation and enable subsequent C–C coupling, ensuring high selectivity and yield of EtOH production.
Theoretical exploration of CH4OR identifies two potential mechanisms: non-radical and free-radical pathways, on both Mo–Cu and Mo sites (Fig. S41–S43). Both sites show comparable activity for CH4 activation, with low activation energies of +0.22 eV (Mo–Cu) and +0.24 eV (Mo). The intermediate *OO plays a central role, reacting with *CH3 to produce *CH3OO, which subsequently transforms into *CH3O. These steps are exothermic on Mo sites, with energy changes of −4.97 and −4.88 eV. In contrast, the critical C–C coupling step to form *CH3CH2O is exothermic on Mo–Cu sites (−0.93 eV) but endothermic on Mo sites (+0.42 eV), highlighting the superior role of Mo–Cu sites in enabling efficient *CH3O transfer and final C–C bond formation.50 These insights collectively emphasize the importance of the synergistic interactions between Mo and Mo–Cu sites in optimizing the CH4OR processes, particularly in the formation and transfer of *CH3O.
To deeply elucidate the dynamic behavior of the *CH3O during the CH4OR, molecular dynamics (MD) simulations were conducted. For comparative analysis, the Zn-doped system was included as a benchmark due to its previously reported high mobility for *CH3O (Fig. S44). Mean square displacement (MSD) analysis (Fig. 5a) shows that the Mo–Cu dual-site exhibits a remarkable *CH3O mobility, achieving a favorable diffusion coefficient of 0.017 Å2 ps−1, surpassing those of other dopants such as Co, Ni, and Fe, and nearly matching the performance of the Zn-doped system. However, for driving force (Fdrive) of *CH3O transfer, the Mo dopant offers additional advantages in catalytic efficiency and energy favorability, as evidenced by minimal energy requirement of −0.70 eV, among all other metal doped models in Table S3. This enhanced *CH3O migration facilitates subsequent C–C coupling steps, underscoring the critical role of Mo as the preferred dopant in optimizing CH4-to-EtOH conversion.
Based on DFT and MD simulations, the Mo–Cu dual-site exhibits enhanced *CH3O migration and C–C coupling efficiency during the CH4OR, due to distinct electronic complementarity. The Mo center, with stronger oxophilicity, stabilizes *CH3O via enhanced electron withdrawal, while the adjacent Cu site offers moderate adsorption strength that facilitates *CH3O desorption and subsequent C–C coupling. This dual-site configuration enables interfacial charge redistribution and orbital interactions between Mo d-states and Cu conduction bands, collectively lowering the energy barriers for intermediate migration and favoring cascade conversion toward EtOH (Fig. 5b). Notably, the unique role of the Mo dopant, vividly depicted as a fast-running athlete, ensures rapid *CH3O migration to the Cu sites with precisely matched speed and efficiency, outperforming other metal dopants such as Zn, Fe, and Co. This synergy between Mo and Cu not only accelerates the transfer process but also enhances the selectivity and yield of EtOH production.
To better understand the cascade mechanism in facilitating *CH3O transfer and subsequent C–C coupling during CH4-to-EtOH conversion, Fig. 5c shows the critical synergy between Mo and Cu sites in driving selective CH4-to-EtOH conversion. At 1.9 V, the free energy for *CH3O migration from Mo to the Mo–Cu interface is minimized, enabling an efficient cascade process. The stepwise energy profile reveals that the subsequent C–C coupling step is highly exothermic, releasing −1.01 eV upon formation of *CH3CH2O. To assess the competing C1 pathways, the thermodynamics of *CH3 evolution toward CH3OH and HCOOH were evaluated. Both routes exhibit higher relative free energy, indicating that these by-products are thermodynamically disfavored under the electrochemical CH4-to-EtOH conversion conditions. Besides, in situ ATR-FTIR spectra reveal *CH3O formation on Mo-based catalysts and EtOH on Cu2Se, while both signals are observed on the Mo–Cu2Se (Fig. S45). This spectral evolution supports an intermediate spillover process,51 in which *CH3O is generated on Mo sites and migrates to adjacent Cu domains for subsequent C–C coupling. Fig. 5d further illustrates the energy profile for *CH3O migration within the Mo–Cu interface, identifying key intermediates and a transition state corresponding to a migration barrier of +0.86 eV. This step represents the rate-determining step of the cascade mechanism and highlights the importance of spatially separated sites.
As shown in Fig. 5e, the subsequent *CH3 and *CH3O coupling is highly exergonic (−1.01 eV), reflecting the strong thermodynamic driving force toward EtOH formation. A comprehensive cascade mechanism is summarized in Fig. 5f and Fig. S46, where CH4 activation initiates at Mo sites through a three-electron *O2−-mediated oxidation pathway, generating *O2− that abstracts H from CH4 to form *CH3. This is followed by *CH3O spillover from Mo to Cu, where it undergoes C–C coupling with *CH3 to yield *CH3CH2O. This mechanistic sequence is supported by kinetic isotope effect (KIE) experiments. In Fig. S47, a significant primary KIE with CD4 (kCH4/kCD4 of ∼2.88) confirms that C–H bond cleavage is rate-determining, while the minor effect with D2O (kH2O/kD2O of ∼1.15) suggests that protonation steps are not involved in the kinetic bottleneck. To confirm the robustness of the dual-site system under CH4OR conditions, DFT calculations (Fig. S48) revealed the thermodynamic stability of the Mo–Cu interface during *CH3O binding and migration, while the post-reaction XPS analysis (Fig. S49 and Table S4) showed negligible changes in Mo and Cu oxidation states, demonstrating excellent structural and chemical durability.
The economic feasibility of the electrochemical process was evaluated against conventional thermal catalytic methods, including steam reforming methanol (SRM) and chemical looping. Based on the economic and technological assumptions outlined in Table S5 and the SI, the analysis reveals that the electrochemical approach is more cost-competitive for EtOH production capacities below 500 tonnes per day (Fig. 6b).52–54 At a scale of 400 tonnes per day, the electrocatalysis system achieves a competitive production cost of ∼$2.12 per kg, compared to $2.59 per kg for SRM and $1.71 per kg for chemical looping. Although the electrochemical process currently involves a slightly higher cost than chemical looping, it benefits from ambient-condition operation, modular scalability, and low CO2 emissions. Importantly, techno-economic projections further suggest that integrating renewable electricity could lower the CH4-to-EtOH cost to ∼$1.50 per kg within a decade, achieving a 53% energy return. Besides, the modest improvements in FE, cell voltage, CAPEX, or OPEX, etc., in Table S6, could yield economic parity, underscoring the route's promising scalability and technological headroom.
Moreover, process-level performance metrics, including single-pass CH4 conversion, energy efficiency, specific energy consumption, and electron economy, are summarized in Table S7, further substantiating the strong scalability and energy return potential of this electrocatalytic platform. Looking ahead, the integration of renewable natural gas and electricity is expected to further transform the economics of CH4 electro-upgrading, offering a sustainable and flexible platform for future energy and carbon utilization infrastructures.
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