Yue
Chen
a,
Yu
Ma
a,
Chen
Liao
a,
Jiacheng
You
a,
Huihuang
Fang
*ab,
Chongqi
Chen
*ab,
Yu
Luo
ab and
Lilong
Jiang
*ab
aNational Engineering Research Center of Chemical Fertilizer Catalyst (NERC-CFC), School of Chemical Engineering, Fuzhou University, Fujian 350002, China. E-mail: hhfang@fzu.edu.cn; c.q.chen@fzu.edu.cn; jll@fzu.edu.cn
bQingyuan Innovation Laboratory, Quanzhou, Fujian 362801, China
First published on 25th July 2025
The construction and stabilization of Cu–O–Si interfaces in copper-based catalysts remain critical yet challenging for the water–gas shift reaction (WGSR), as conventional strategies fail to mitigate copper nanoparticle (NP) aggregation and interfacial instability. This study innovatively proposes a spatial confinement strategy by anchoring Cu NPs inside (Cuin/SBA-15) or outside (Cuout/SBA-15) the mesoporous channels of SBA-15, leveraging nanoscale confinement to optimize Cu–O–Si interfaces. The confined Cuin/SBA-15 catalyst demonstrated exceptional WGSR performance, achieving a reaction rate of 5.4 μmolCO gcat−1 s−1, significantly surpassing conventional Cu/SBA-15 (3.6 μmolCO gcat−1 s−1) and surface-loaded Cuout/SBA-15 (3.1 μmolCO gcat−1 s−1), along with remarkable stability. This enhancement originates from the SBA-15 channels enabling the in situ formation of stable Cu–O–Si interfaces, which regulate the dynamic equilibrium between Cu0 (active for H2O dissociation) and Cu+ (critical for CO adsorption) species. In situ studies revealed their synergistic dynamic interconversion during the WGSR, while domain confinement effects suppressed sintering by maintaining interfacial integrity. Kinetic and mechanistic analyses further identified the associative pathway, with HCOO* intermediate dissociation as the rate-determining step, facilitated by the stabilized Cu–O–Si interfaces. By resolving interfacial instability through confinement engineering, this work provides a paradigm for designing robust Cu-based catalysts, advancing both fundamental understanding and practical applications in the WGSR and related heterogeneous catalysis.
Typically, the deactivation of copper-based catalysts manifests as a disturbance in the balance between Cu+ and Cu0 in the catalyst. As a result, the copper particles aggregate and grow by migrating across the silica surface. Two forms of migratory sintering of copper species have been identified in the literature;12–14 one mechanism involves the migration of entire particles across the support, resulting in aggregation. The other mechanism involves the detachment of metal species from one particle, followed by their transport through the support or in the gas phase, and subsequent attachment to another particle, and this process is commonly referred to as Ostwald ripening. These phenomena have limited the widespread application of copper-based catalysts. To spatially restrict the migration of copper nanoparticles, some researchers have stabilized copper-based catalysts using spatial immobilization techniques involving oxides,15,16 carbon materials,17 and molecular sieve encapsulation.18–20 Li et al.21 prepared Cu@SiO2 catalysts with high Cu dispersion that effectively prevented particle growth and aggregation during the reaction. Ma et al.22 reported a carbon nanotube-alumina strip (CAS)-loaded Co–Cu catalyst for the CO2 methanation reaction, where CAS exhibited a limiting effect, prolonging the residence time of the reactants within the mesoporous pores compared to single carbon nanotubes. Cui et al.23 used an HKUST-1 encapsulated Cu precursor and successfully avoided sintering of homogeneous substances. Despite these advances, maintaining the dynamic Cu+/Cu0 balance under WGSR conditions remains unresolved. Conventional approaches often fail to stabilize multivalent Cu species while ensuring reactant accessibility, limiting their long-term catalytic robustness.
Hydroxyl groups (–OH) on the surface of SiO2 can form Cu–O–Si bonds with copper species, and their formation mainly depends on the interaction between the metal and the support. It has been shown that the Cu–O–Si interface can significantly enhance catalytic activity, as it not only provides more active sites but also stabilizes reaction intermediates. For example, in the selective hydrogenation of dimethyl oxalate (DMO) to ethylene glycol (EG), the presence of the Cu–O–Si interface facilitates ester hydrogenation because Cu–H+ and Si–OH+ can stabilize the hydrogenation transition state, thus lowering the reaction energy barrier.24 The ordered mesoporous structure of SBA-15 has been identified as a promising approach for enhancing the catalytic performance of Cu-based catalysts due to its distinctive pore structure. A large number of isolated silanol (Si–OH) groups on the surface undergo dehydration and condensation with Cu species after heat treatment or reduction, resulting in the formation of a stable Cu–O–Si bonding structure at the interface. In addition, the unique pore structure promotes the dispersion of active centers and facilitates the transfer of reactants and products within the confined space, without leading to unwanted side reactions.25–27 The confined nanospace thus provides a novel platform for promoting catalytic reactions.
Although the metal confinement by mesoporous or zeolitic frameworks has been widely studied, pure-silica SBA-15 with uniform mesopores to form highly dispersed and redox-stable Cu species is still attractive. Unlike aluminosilicates such as HZSM-5 or HUSY, SBA-15 allows the formation of stable Cu–O–Si interfaces and offers sufficient pore space for both molecular transport and in situ characterization. These features make SBA-15 an ideal platform for understanding the dynamic evolution of Cu+/Cu0 during the WGSR. Therefore, a detailed mechanistic understanding of confined Cu species and their redox dynamics under reaction conditions is both timely and crucial. Meanwhile, the multivalent state of Cu implies that the catalytically active sites, Cu0 and Cu+, undergo stochastic and dynamic changes in the reaction environment. In recent years, studies on the synergistic effect of Cu+ and Cu0 in copper-based catalysts for the WGSR have intensified.28–30 It has been well documented that synergy between Cu+ species, which play a key role in CO adsorption and activation, and Cu0, which promotes H2O dissociation and OH* species generation, is essential for achieving high activity and selectivity. Although these studies have made progress in material design, most studies are limited to static valence characterization and fail to reveal the in-depth reaction mechanism, particularly the dynamic valence transformation of Cu species under reaction conditions and its direct correlation with catalytic performance. In addition, there is still a lack of systematic approaches to observe how the Cu+/Cu0 ratio is stabilized by the microstructure during the actual WGSR process and how its evolution affects the intermediate conversion and the rate-determining steps. As a result, identifying the active Cu species and further elucidating the catalytic mechanism of Cu-based catalysts remain challenging.
Herein, we address these challenges by anchoring Cu nanoclusters within SBA-15 mesochannels to construct a stable Cu–O–Si interface. Systematic characterization reveals that the confined environment enhances Cu dispersion and interfacial integrity, and the catalyst with stable and balanced Cu+ and Cu0 species exhibits excellent activity and stability in the low-temperature WGSR. Microstructural characterisation confirms that the mesoporous material provides spatial confinement effects, resulting in uniform dispersion of copper nanoparticles within the SBA-15 pores. This structure stabilizes the Cu+ and Cu0 species through the formation of a large number of Cu–O–Si interfaces. In addition, in situ and transient isotope-switching experiments reveal the rate-determining steps of the WGSR process over the domain-confined Cu-based catalysts and provide insight into the state of the active Cu species and the dynamic evolution of the catalytic process.
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Kinetic evaluations were performed in the same continuous flow fixed bed with a quartz reactor as previously described. In order to eliminate internal and external diffusion limitations, measurements were carried out at a temperature of 175 °C, where the CO conversion was kept below 20% by adjusting the weight of the catalyst or the flow rate of the mixed gas. The reaction rate and the turnover frequency (TOF) were calculated as follows:32
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A similar trend was observed in dissociative N2O adsorption. The dispersion of Cu over the three catalysts was investigated utilizing N2O as a probe, with the results of the N2O chemisorption measurements summarized in Table 1. The data revealed superior Cu dispersion in Cuin/SBA-15 (27.8%) versus counterparts, confirming the enhanced distribution of active sites due to spatial confinement. Nitrogen physisorption analysis (ESI Fig. S3†) maintained type IV isotherms with H1 hysteresis for all materials, characteristic of mesoporous systems. Comparative textural properties (Table 1) showed sequential reductions in the BET surface area and pore volume relative to pristine SBA-15. This trend suggested gradual pore occupation by Cu species and indicated that the apparent decrease in the surface area for Cuout/SBA-15 may be attributed to pore blockage by larger, externally located particles.
Sample | Cu contenta (wt%) | A BET (m2‧g−1) | V Pore (cm3‧g−1) | d Pore (nm) | D Cu (%) | d Cu (nm) | Ratioe of Cu+/Cu0 (%) |
---|---|---|---|---|---|---|---|
a Determined by ICP-OES analysis. b BET specific surface area. c Cu metallic surface area per gram of catalyst determined by the N2O titration method. d Calculated on the basis of TEM images. e Quantitative by Auger. | |||||||
SBA-15 | — | 762.7 | 1.02 | 6.48 | — | — | — |
Cu/SBA-15 | 4.35 | 503.6 | 0.76 | 6.63 | 25.1 | 2.71 | 41 |
Cuin/SBA-15 | 5.51 | 492.7 | 0.75 | 6.69 | 27.8 | 1.87 | 35 |
Cuout/SBA-15 | 5.45 | 440.7 | 0.74 | 7.14 | 19.1 | 4.41 | 52 |
The morphology and details of the reduced state of the Cuin/SBA-15 catalyst are shown in Fig. 1(e and f). The high-resolution TEM image of Cuin/SBA-15 revealed lattice fringes with a spacing of 0.209 nm, corresponding to the Cu(111) planes.38 This observation indicated that the predominant exposed facet of the confined Cu nanoparticles was Cu(111), which was well-recognized for its balanced activity in both CO adsorption and H2O dissociation.39 The prevalence of Cu(111) planes, stabilized by SBA-15 confinement, may thus synergistically contribute to enhanced catalytic performance.
The co-existence of fcc Cu and cubic Cu2O phases was confirmed by XRD (Fig. S2†), with no evidence of amorphous or mixed-phase transformations. This crystalline dual-phase structure remains stable under reaction conditions, particularly in the Cuin/SBA-15 catalyst, where spatial confinement helps prevent Cu nanoparticle agglomeration and surface oxidation. In contrast, the external Cu in Cuout/SBA-15 undergoes partial structural degradation, as evidenced by broadened diffraction peaks and reduced crystallinity. The ability to retain a well-defined Cu0/Cu+ crystalline interface is considered a key factor in maintaining redox activity and catalytic efficiency in the WGSR process. The dark-field TEM image (Fig. 1(f)) showed numerous high-density bright spots corresponding to Cu clusters uniformly dispersed within the inner wall of the mesopores, indicating small and well-dispersed Cu particles. Furthermore, elemental mapping (Fig. 1(g)) confirmed the uniform distribution of Si, O, and Cu elements, further supporting the role of SBA-15 mesopores in facilitating the anchoring and dispersion of Cu species through a confinement effect.
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Fig. 2 (a) CO conversion (T = 240 °C) and WGSR rate (T = 175 °C) of the Cu/SBA-15 series catalysts; (b) TOF values (T = 175 °C), dispersion of Cu, and Cu+/Cu0 ratios of the Cu/SBA-15 series catalysts; (c) CO conversion of Cu/SBA-15 series catalysts and some typical WGSR catalysts: 1–5 wt.%Cu/SBA-16,40 2–9 wt.%Cu/SiO2,41 3–5 wt.%Cu/SiO2, 4–5 wt.%Cu/Silicalite-1, 5-Cu/SBA-15, 6-Cuin/SBA-15, and 7-Cuout/SBA-15; (d) stability test and (e) process of associative and regeneration and (f) start–stop cycle tests of Cuin/SBA-15; reaction conditions: WHSV = 4500 mL‧gcat−1‧h−1, steam![]() ![]() ![]() ![]() |
Among all the prepared catalysts, even at a relatively low temperature of 240 °C, the Cuin/SBA-15 catalyst with 5% Cu loading achieved a CO conversion of 75%, whereas the Cuout/SBA-15 catalyst exhibited only 30% to 40% conversion under the same conditions. This activity disparity aligned with structural characteristics, as the Cuin/SBA-15 catalyst exhibited a superior reaction rate of 5.4 μmolCO‧gcat−1‧s−1, approximately 1.7 times higher than that of the Cuout/SBA-15 catalyst. To further rationalize the structure and performance relationship among the three catalyst configurations, a simplified quantitative model was introduced to evaluate the additive behavior of copper distribution, as illustrated in Fig. S5.† Based on structural and catalytic data, the performance of the three catalysts can be described using a semi-quantitative expression, suggesting that the activity of the randomly distributed Cu/SBA-15 catalyst arises from a weighted combination of confined and non-confined copper contributions. In the absence of spatial control, the Cu species cannot fully benefit from either confinement-induced stabilization or external accessibility, leading to diluted and suboptimal catalytic performance. These results clearly indicated that the internal confinement of copper species within the mesopores of SBA-15 (Cuin/SBA-15) provides a more favorable structural environment compared to external deposition (Cuout/SBA-15) or random distribution (Cu/SBA-15). The enhanced performance arose from higher copper dispersion, an optimized Cu+/Cu0 ratio, and enhanced accessibility of dual active sites. Collectively, these factors synergistically contribute to enhanced catalytic activity. These results conclusively demonstrated that spatial confinement enhanced catalytic activity by stabilizing highly dispersed active species and optimizing pore architecture, thereby maximizing active site accessibility.
Kinetic analysis (Fig. 2(b)) further elucidated performance drivers through turnover frequency (TOF) correlations. TOF exhibited an inverse dependence on Cu+/Cu0 ratios but scaled positively with Cu dispersion, establishing low oxidation states and high metal dispersion as critical for catalytic efficiency. The nanoconfined Cuin/SBA-15 system achieved a TOF 1.16 times greater than its non-confined counterpart, highlighting interfacial synergy between Cu nanoparticles and the SiO2 framework. This synergistic interaction likely stabilizes metastable Cu species while facilitating electron transfer at Cu–O–Si interfaces, thereby enhancing reaction dynamics under confinement conditions.
To more comprehensively evaluate the catalytic performance of the Cuin/SBA-15 catalyst developed in this study, we have summarized and compared its CO conversion and TOF values with those of representative Cu-based WGSR catalysts reported in the literature, as shown in Fig. 2(c) and Table S1.† Catalysts supported on conventional SiO2 or silica zeolite frameworks (e.g., Cu/Silicalite-1 and Cu/SBA-16) typically exhibit lower CO conversions in the range of 16–45% at 240 °C, even when the copper loading is comparable.
In contrast, the Cuin/SBA-15 catalyst achieved a significantly higher CO conversion of 75.8% under similar reaction conditions and metal content, outperforming both the randomly dispersed Cu/SBA-15 (55.6%) and the externally deposited Cuout/SBA-15 (38.5%) catalysts. Notably, Cuin/SBA-15 also exhibited a markedly higher TOF compared with several benchmark systems, including 10Cu/CeO2, 5Cu5Ni/CeO2, Cu/ZnO, and Cu/ZnO/La, despite the use of reducible oxide supports in those systems. These results clearly demonstrate that the superior catalytic performance of Cuin/SBA-15 is not solely attributable to copper loading or support type, but rather to the precise spatial confinement of Cu nanoclusters within the mesoporous SBA-15 channels.
Such confinement effectively suppresses particle migration and sintering, while simultaneously enabling the formation of stable Cu–O–Si interfacial structures within the pores. These interfaces help to dynamically stabilize the Cu+/Cu0 redox pair and promote a balanced interplay between H2O dissociation and CO adsorption, which are two essential steps in the WGSR pathway.
In summary, although a wide variety of Cu-based WGSR catalysts have been reported (Table S1†), most studies lack precise control and in situ monitoring of the copper valence state and interfacial dynamics during the reaction. The domain-confinement strategy proposed in this work effectively stabilizes both the reactive redox state and interfacial structure, while maintaining a high dispersion of active species.
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Fig. 3 (a) H2-TPR profile and (b) CO2-TPD profile and (c) in situ Cu 2p XPS spectra and (d) in situ Cu LMM Auger spectra of Cu/SBA-15, Cuin/SBA-15 and Cuout/SBA-15 catalysts. |
CO2-TPD profiles (Fig. 3(b)) elucidated surface basicity variations critical for WGSR equilibrium management. All catalysts exhibited three desorption regimes: α-peak (bidentate carbonate decomposition), β-peak (monodentate carbonate on moderately basic sites), and γ-peak (monodentate carbonate on strongly basic sites),45 respectively. The Cu/SBA-15 catalyst exhibited a greater number of weakly basic sites, while the Cuout/SBA-15 catalyst displayed a greater number of moderately basic sites. The presence of weakly basic sites on the Cuout/SBA-15 catalyst may result in the formation of carbonate-based reaction products that were challenging to desorb within the specified temperature range. This could potentially cover the active sites of the catalysts,46 leading to a reduction in their overall activity. This was consistent with the results shown in Fig. 2(a) above, indicating that the limiting effect of SBA-15 can effectively avoid the coverage of some active sites.
To further investigate the existence state of copper species in copper based catalysts, XPS characterization was performed on the Cu/SBA-15, Cuin/SBA-15 and Cuout/SBA-15 catalysts. The XPS energy level spectra of the Cu 2p orbitals for each catalyst are shown in Fig. 3(c), with two primary peaks centered at binding energies of 932.4 eV corresponding to Cu 2p3/2 and 952.3 eV corresponding to Cu 2p1/2, attributed to copper species in the reduced state (Cu0 or Cu+).47 Notably, Cuin/SBA-15 exhibited positive binding energy shifts versus counterparts, signaling enhanced Cu-support electronic interactions. As previously reported, the Cu oxidation state played a crucial role in WGSR performance,48,49 but since Cu0 and Cu+ had very similar binding energies, further distinction was made using X-ray excited Auger electron spectroscopy (XAES). The Cu LMM Auger spectra (Fig. 3(d) and Table 1) identified two components, located at 918.12 eV (Cu+) and 914.37 eV (Cu0). The relative proportions of Cu species for the three samples were also listed and the Cuin/SBA-15 catalyst had the highest molar ratio of Cu0/(Cu0+Cu+) (74.0%) compared with the other three samples, which was responsible for the shift of the core energy level binding energy of the Cu 2p orbitals of the catalyst towards a higher binding energy, contrasting sharply with the Cu+-dominant profile (52% Cu+) of Cuout/SBA-15. The critical Cu+/Cu0 ratio emerged as a performance-determining parameter. While Cu+ facilitates CO adsorption and Cu0 promotes H2O dissociation,48,50 the synergistic balance governs the overall activity. The Cu+/Cu0 ratio of Cuin/SBA-15 optimally reconciles these complementary functions, and sufficient Cu+ ensures CO activation without overstabilizing intermediates, while abundant Cu0 accelerates water splitting. Based on these results, it is reasonable to believe that on catalysts in this study, a suitable Cu+/Cu0 ratio is the predominant factor to control the reaction performance.
Subsequently, the addition of CO led to the formation of metallic Cu0 during the WGSR process. It was worth noting that this process involved both CO-induced reduction of Cu+ to Cu0 and the participation of H2 produced during the WGSR process in reducing Cu+, thereby inhibiting CO conversion. As observed in Fig. 4(b), after 1 hour of the WGSR, the Cu+/Cu0 of the Cuout/SBA-15 catalyst decreased the most. This was because H2 molecules directly participated in the reduction of Cu+ to Cu0 on the surface of SBA-15, competing with the main WGSR pathway and resulting in a decreased CO conversion. Therefore, the Cuout/SBA-15 catalyst exhibited the worst catalytic activity for the WGSR. In contrast, the confined architecture of Cuin/SBA-15 moderated excessive Cu+ depletion, maintaining optimal redox equilibrium through spatial regulation of metal–support interactions.
In situ DRIFTS investigations (Fig. 4(c)) elucidated site-specific behaviours and the Cuin/SBA-15 catalysts were pre-treated with CO at 280 °C, followed by in situ DRIFTS experiments. Fig. 4(c) shows the co-adsorption process through H2O after the pre-adsorption of CO. The peaks at 2111 cm−1 and 2130 cm−1 corresponded to the vibrations of Cu0–CO and Cu+–CO,53,54 respectively. The intensity of the CO absorption band on the Cu0 surface at 2111 cm−1 decreased rapidly and finally disappeared after the introduction of water vapor to simulate the feed gas of the reactants. In contrast, the intensity of the CO absorption band at 2130 cm−1 on the Cu+ surface decreases slowly, and the spectral band generated between 3000 and 3500 cm−1, attributed to the stretching vibrations of the O–H bond, gradually increased.55 This suggested that H2O can dissociate more easily on the Cu0 surface and form CO2 by the WGSR with adsorbed CO molecules on the Cu0 surface, whereas the slowly decreasing intensity of the CO–Cu+ band suggested that H2O can also dissociate on the Cu+ site, but the dissociation process was slower. Fig. 4(d) shows the desorption process after co-adsorption at the same temperature. The spectral bands near 2090, 2111, 2130, and 2170 cm−1 were detected corresponding to the vibrations of Cu0–CO, Cu+–CO, and gaseous CO, respectively, confirming the co-existence of the Cu0 and Cu+ sites, but the adsorption of CO at the Cu0 site was unstable. The Cu0–CO and gaseous CO peaks disappear rapidly within the first 4 minutes but the Cu+–CO peak decreased much more slowly and reached stability after 12 minutes. Thus, Cu+ species may be the main active site for adsorption and activation of CO molecules. Based on these findings, a dual-site mechanistic framework can be shown in Fig. 4(e). The H2O molecule was adsorbed and activated at the Cu0 site and then produced *OH and *H, while the CO molecule was adsorbed and activated mainly at the Cu+ site and then gradually converted to become CO2, which was the representative intermediate of the mechanism of the reaction, and a number of other intermediate products. The confined architecture in Cuin/SBA-15 enabled spatial orchestration of these complementary processes, with Cu0 sites driving rapid hydroxyl generation while Cu+ sites sustain CO activation, and their synergy was moderated through controlled electron transfer at Cu–O–Si interfaces.
To unravel the dominant pathway in Cu/SBA-15 systems, we focused on the high-performance Cuin/SBA-15 catalyst. Fig. 5(a) shows the in situ DRIFTS profiles of CO and H2O co-adsorption over the Cuin/SBA-15 catalyst at different temperature points, simulating the process of the WGSR. It can be observed that the bands in the range of 1000–1700 cm−1 correspond to both symmetric and asymmetric stretching vibrations of OCO, but both carbonates and formates contain OCO stretching vibrations.60,61 In addition, peaks in the region of 1550–1650 cm−1 were detected, indicating the formation of a single bidentate formate species,62 while the peaks at 2700–3000 cm−1 were associated with the C–H stretching vibration of the formate species.63–65 The intensity of all the peaks increased with decreasing temperature, which may be due to the fact that formate species with COO vibrations increased the stability of the active metal with the support at lower temperatures, and strongly and irreversibly adsorbed carbonate species are retained on the metal surface, leading to a decrease in the catalytic activity, a result consistent with the activity results. Therefore, it can be tentatively concluded that the catalyst followed the associative mechanism.
On the other hand, as the temperature increases, the carbonate species decomposes more readily into CO2. The results showed that at higher temperatures, there were two distinct absorption bands at 2322 and 2369 cm−1 indicating the presence of asymmetric stretching of the CO2 molecule and that the intensity of these absorption bands decreased with decreasing temperature.66,67 Thus, it can be described that the WGSR of formic acid species as intermediates and the decomposition of formic acid were considered as rate-determining steps. Briefly, the WGSR process over the Cuin/SBA-15 catalyst can be outlined as the production of reactive surface OH groups on silica sites and the formation of formate species (HCOO–) following a reduction process, followed by the decomposition of the bicarbonate formate species into bidentate formate species, which were finally decomposed to produce H2 and CO2, resulting in a decrease in the intensities of the bands associated with formate species and a significant increase in the bands associated with CO2. Complementary TPSR experiments (Fig. 5(b)) employing mass spectrometry provided mechanistic validation.68 The Cuin/SBA-15 catalyst was reduced and then treated with CO and H2O for 2 hours to obtain the real catalytic reaction interface structure. After purging with helium, the catalyst was exposed to H₂O for 2 hours by exchanging helium with water vapour at 280 °C (H2O dissociation experiment). It was then treated at 280 °C for 1 hour under a helium atmosphere to remove excess adsorbed water from the surface. After cooling to room temperature, the helium was converted to CO and reacted at 280 °C for 2 hours (CO-TPSR experiment). The output gas was analysed with m/z = 44 (CO2) and 2 (H2).
In the redox mechanism, CO reacts with reactive oxygen species at the catalytic interface to form CO2 and O vacancies, and H2O dissociates at the oxygen vacancies to form hydrogen. The process of the associative mechanism is shown in Fig. 5(c), including the dissociation of H2O molecules directly at the O vacancies to form hydroxyl groups and the reaction of CO with the hydroxyl groups to produce CO2 and H2 in a yield of approximately 2:
1. There was no direct appearance of the H2 signal, suggesting that the reaction process did not involve the redox mechanism. In the following CO-TSPR experiments, the concentration ratio of CO2 to H2 remained close to 2, further demonstrating that the reaction followed the associative mechanism.
Isotopic substitution experiments employing D2O as a probe molecule (Fig. 6(a)) yielded critical kinetic insights. By comparing the reaction in the presence of H2O or D2O, the difference in the reaction rates (kH/kD), known as the kinetic isotope effect (KIE), reveals whether protons are involved in the rate-determining step (RDS) of the reaction.69 As shown in Fig. 6(b), by comparing the rate constants of water oxidation under H2O and D2O, a KIE (kH/kD) value of 1.46 was obtained for Cuin/SBA-15, indicating a first-order kinetic isotope effect.1 This significant KIE value suggested that the HCOO* breakage was involved in the rate-determining step of the WGSR.70 The microscopic reaction pathway of the WGSR is shown in Fig. 6(c), where the HCOO* intermediate was formed at the Cu–O–Si interface, followed by slow decomposition to form carbon dioxide and hydrogen gas.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5ta03435c |
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