Open Access Article
Christian
Ehinger‡
a,
Stephan
Pollitt‡
b,
Jordan
De Jesus Silva
a,
Xiaoyu
Zhou
a,
Kazutaka
Sakamoto
a,
Maarten
Nachtegaal
ab,
Olga
Safonova
*b and
Christophe
Copéret
*a
aD-CHAB, ETH Zürich, Vladimir–Prelog-Weg 2, 8093 Zürich, Switzerland. E-mail: ccoperet@ethz.ch
bCenter for Energy and Environmental Sciences, PSI, Forschungsstrasse 111, 5232 Villigen, Switzerland. E-mail: olga.safonova@psi.ch
First published on 5th March 2025
Bimetallic heterogeneous catalysts combining group 9 metals (Rh, Ir) or group 10 metals (Ni, Pd, Pt) with Mo on a silica-based support have been synthesized via surface organometallic chemistry and assessed in their catalytic activity for the hydrodeoxygenation (HDO) of alcohols with particular emphasis on the structural evolution of the catalysts and the role of Mo. The investigation was conducted with an air-free approach to isolate any sample alterations exclusively to those caused by the reaction. Structural analysis was performed using a combination of (S)TEM, IR, and XAS. It was found that Ir–Mo/SiO2, Rh–Mo/SiO2, and Pt–Mo/SiO2 display high activity for primary, secondary, and tertiary alcohol deoxygenation, while Pd–Mo/SiO2 selectively catalyses tertiary alcohol deoxygenation. Other combinations as well as the corresponding monometallic materials do not display the same activity. X-ray absorption spectroscopy confirmed metallic states for M (M = Ni, Rh, Pd, Ir, or Pt), while Mo K-edge XANES showed varying amounts of Mo(0), Mo(IV) and Mo(VI) depending on the metal counterpart in fresh materials, and indicated complete conversion of Mo(VI) to lower oxidation states (IV and 0) during the reaction. For Rh, Pd, Ir, and Pt, alloy formation (M–Mo) was identified via M–Mo paths in EXAFS and supported by CO-IR spectroscopy. In contrast to Ir, Rh, and Pt, where some Mo(0) is present at the nanoparticle surface, Pd–Mo forms an alloy but likely retains Mo in the nanoparticle core, as suggested by CO-IR spectroscopy and CO-chemisorption. Reactivity studies suggest that tertiary alcohols primarily undergo dehydration–hydrogenation, evidenced by olefin formation with MoOx/SiO2, as well as Ir/SiO2 and Ir–Mo/SiO2 under inert conditions. In contrast, primary and secondary alcohols follow a different mechanism, correlated with the presence of metallic Mo species on the nanoparticle surface, highlighting their role in C–O bond activation. These findings provide new insights into the structure–activity relationships of Mo-based bimetallic catalysts, underscoring the influence of Mo in different oxidation states and strong substrate dependence on mechanistic pathways.
Breaking C–O bonds is associated with a significant energy barrier due to their high kinetic and thermodynamic stability, requiring the use of catalysts.12,13 Heterogeneous catalysts for HDO often comprise late transition metals – to activate dihydrogen – combined with a group V–VII transition metal, in particular Mo, that are thought to facilitate the activation of the C–O bond because of their oxygen affinity and their ability to introduce Brønsted and/or Lewis acidity.14–20 These bifunctional-bimetallic catalysts can lead to enhanced activity compared to the corresponding monometallic materials, suggesting a synergy that is crucial for the desired reactivity.21–25 However, the exact role and interplay of the components in these catalysts are still poorly understood and often remain speculative, mainly due to the complexity of these materials.13,26
In classical synthetic approaches, metallic nanoparticles of late transition metals (M) are commonly prepared via impregnation techniques, often relying on metal chloride (or nitrate) precursors, possibly leading to contamination or uneven particle formation.27,28 While cost and time efficient, these approaches generally afford rather ill-defined materials, with non-uniform distribution of surface sites and particle sizes. This complexity arises from the synthetic process as it involves uncontrolled dissolution and precipitation processes in water. This, in turn, makes it challenging to achieve molecular-level understanding of catalytic processes and to develop informative structure–property relationships. In that context, surface organometallic chemistry (SOMC) has emerged as a synthetic strategy to generate better-defined catalyst structures using tailored (traceless) molecular precursors that are evenly dispersed on the surface by anchoring onto hydroxy groups (grafting), followed by a post treatment to remove the organic ligands; this approach typically generates smaller nanoparticles and a narrower size distribution.29 In addition, these materials provide tailored interfaces and compositions, while avoiding the incorporation of undesired elements.30
In the presented work, we investigate a series of HDO catalysts prepared via SOMC based on the combinations of a transition-metal, known for their hydrogenation properties (M = Rh, Ir, Ni, Pd, and Pt) and Mo, dispersed on a silica support. Among M–Mo/SiO2, we show that the promotional effect of Mo for HDO of alcohols as prototypical oxygenate substrates is highly efficient with Pt, Rh, and particularly so for Ir, while negligible for Ni, and only observed for tertiary alcohols in the case of Pd. Characterization based on the adsorption of CO and pyridine probe molecules, High-Angle Annular Dark Field Scanning Transmission Electron Microscopy (HAADF-STEM), and X-ray absorption spectroscopy (XAS), performed on the catalysts before and after the HDO reaction and preserved under inert atmosphere, show that Mo is reduced from Mo(VI) to Mo(IV) and Mo(0) in the presence of the primary metal (M) and incorporated in narrowly dispersed 2–3 nm alloyed nanoparticles (for M = Rh, Ir, Pd, Pt), without significant changes in Brønsted or Lewis acidity. Overall, the data point to the importance of a metallic state of Mo and alloy formation, indicating M–Mo phases play a critical role in efficient HDO processes.
:
M ratio (ca. 1
:
8, vide infra) was chosen because small amounts of Mo have been shown to significantly enhance deoxygenation activity,17 and it also ensures that Mo predominantly contributes to the active phase while minimizing spectroscopic interference from inactive species. The second metal (ca. 1 M atom per nm2) is next introduced using SOMC (Fig. 1a). We select amidinate-based precursors, because they provide a structurally unified platform for all five investigated metals M (Ni, Pd, Pt, Rh, and Ir) and afford supported nanoparticles with relatively narrow size distribution upon treatment under H2.33–35 In short, after grafting the amidinate-based precursors on isolated surface OH groups, as evidenced by IR spectroscopy (Fig. 1c, middle spectrum), the obtained materials are treated under a flow of H2 at 500 °C. The resulting IR spectrum (Fig. 1c, top spectrum) confirms the removal of all organic ligand fragments while the isolated OH groups are restored. The respective monometallic materials are prepared from the same precursors, using SiO2–700 (SiO2 subjected to a temperature treatment at 700 °C at 10−6 mbar) in place of the Mo-doped support.
HAADF-STEM micrographs of all as-prepared materials are recorded and analysed without prior exposure to air (Table 1, Fig. 1b, and S20–S24†). All materials contain narrowly dispersed nanoparticles of 2–3 nm. With the exception of PtMo, all bimetallic materials exhibit smaller and more narrowly dispersed nanoparticles compared to their monometallic counterparts.36 For NiMo, the sub-nanometre particles are not resolved. For PdMo, the particles are considerably better dispersed, than in the monometallic case; this effect had been previously observed for alloyed bimetallic Pd–Ga/SiO2 derived from the same precursor.33,37 Both IrMo and RhMo also display nanoparticles that are ca. 1 nm smaller than the respective monometallic materials. The strong influence of Mo is particularly remarkable considering that the M
:
Mo ratio is ca. 8
:
1, suggesting a strong interaction between the two metals.
| Material | μ (nm) | σ (nm) | N | M (wt%) |
|---|---|---|---|---|
| Ni/SiO2 | 1.9 | 0.6 | 205 | 1.36 |
| Ni–Mo/SiO2 | <1 | — | — | 1.33 |
| Pd/SiO2 | 3.1 | 1.6 | 210 | 2.59 |
| Pd–Mo/SiO2 | 2.5 | 0.5 | 205 | 2.41 |
| Pt/SiO2 | 1.8 | 0.5 | 213 | 3.98 |
| Pt–Mo/SiO2 | 1.8 | 0.6 | 211 | 3.56 |
| Rh/SiO2 | 3.3 | 0.7 | 134 | 2.38 |
| Rh–Mo/SiO2 | 2.4 | 0.6 | 207 | 2.44 |
| Ir/SiO2 | 2.9 | 0.9 | 230 | 4.32 |
| Ir–Mo/SiO2 | 2.0 | 0.6 | 222 | 4.26 |
:
1 ratio) formed via dehydration (Fig. S32†), potentially indicative that a different mechanism can be at play for the deoxygenation of tertiary alcohols, namely via a sequential dehydration–hydrogenation pathway involving olefins as reaction intermediates.
Considering that Pd–Mo/SiO2 is inactive for 1-nonanol and 2-nonanol, we highlight the possibility of selectively deoxygenating tertiary alcohols over primary and secondary alcohols. Subjecting a mixture of 1-nonanol and 2,6-dimethylheptan-2-ol to HDO conditions with Pd–Mo/SiO2 leads to the selective formation of 2,6-dimethylheptane in 64% yield (76% conversion), while no n-nonane is observed (Fig. S34†). The activity of the Pd–Mo/SiO2 catalyst seems to be partially inhibited by the presence of 1-nonanol, however, the deoxygenation is highly selective. Note that, in the analogous experiment with Ir–Mo/SiO2, both alcohols in the mixture are efficiently deoxygenated affording yields of 88% 2,6-dimethylheptane and 98% n-nonane (Fig. S34†), highlighting the specificity of Pd–Mo/SiO2 in the HDO of tertiary alcohols, suggesting that a dehydration–hydrogenation pathway is dominant with Pd rather than a more direct HDO process.
Since Ir–Mo/SiO2 displays the most promising properties as a general deoxygenation catalyst for aliphatic alcohols, we further investigate the reactivity of this catalyst. First, the reaction profile is examined by monitoring the reaction products at various reaction times (1, 3, and 8 h), which confirms that 24 h reaction time is necessary for achieving full conversion (Fig. S36†). We also check the possibility of recycling the catalyst, which reveals a constant decrease of activity, giving 86%, 60%, and 15% yields after the 1st, 2nd, and 5th cycle, respectively (Fig. S37†). While the catalyst productivity is reduced to 70% after one cycle, with an overall conversion corresponding to ca. 6 h reaction time for the fresh catalyst, the material remains catalytically active, enabling meaningful characterization of the spent catalyst. This allows us to study the structural changes that occur during the reaction, providing insights into the active phase under operating conditions. The treatment of the spent material with H2 or calcination followed by H2 cannot fully restore the high activity observed in the first cycle. Elemental analysis after five cycles reveals a partial loss of metals, with approximately 35% reduction in Mo content and 15% reduction in Ir. While this loss likely contributes to some of the observed decline in activity, it does not account for the entirety of the decrease, suggesting that irreversible structural changes may have occurred under reaction conditions.
Notably, Pd is the only system where the normalized intensity of both terminal and bridging CO increases moving from monometallic to the bimetallic material, without a significant shift of the bands. To further investigate this, we again turn to CO-chemisorption (Fig. S29 and S30†). It is known that the Pd
:
CO stoichiometry is highly dependent on particle size (among other variables), ranging from 2
:
1 for large particles to 1
:
1 for small clusters, as the preferential binding mode transitions from bridging to linear.42,43 Again comparing the nanoparticle surface normalized CO uptake, the value obtained for Pd–Mo/SiO2 is 60% higher than for monometallic Pd/SiO2. This is consistent with the smaller particle size but not indicative of any interference of Mo with CO adsorption on the nanoparticle surface, in contrast to Ir–Mo/SiO2. Among the metals investigated by CO adsorption (Rh, Ir, Pd, Pt), Pd has the lowest surface energy for fcc low index surfaces, hence the lowest driving force for exposing Mo on the nanoparticle surface.44,45 This might explain the inactivity in the HDO of primary and secondary alcohols, potentially highlighting the role of Mo in the mechanism for these substrates.
For both fresh and spent Ir–Mo/SiO2, analysis of their X-ray absorption near-edge structure (XANES) spectra at the Ir L3-edge confirm the metallic nature of Ir as analogously observed for the monometallic Ir/SiO2.35 However, the spectroscopic signature in Mo K-edge XANES is more complex: Mo already appears to be present in several oxidation states in the fresh Ir–Mo/SiO2 catalyst. Linear combination fit (LCF) analysis identifies Mo(VI), Mo(IV), and metallic Mo(0) as main components, with the respective reference spectra reproducing the observed spectrum (Fig. 4a and 5a; see ESI† for details). Note that due to the presence of several (at least 3) Mo (oxidation) states, Mo K–edge extended X-ray absorption fine structure (EXAFS) spectra of the fresh Ir–Mo/SiO2 catalyst cannot reliably be fitted. Regarding the spent Ir–Mo/SiO2 catalyst, all remaining Mo(VI) species are converted yielding an increased amount of both Mo(IV) and Mo(0) according to Mo K-edge XANES (Fig. S41†) and LCF analysis (Fig. 5b). Notably, the respective EXAFS spectrum can be fitted with two scattering paths corresponding to Mo–O and Mo–Ir (Fig. 4b and Table 2 column 1, Fig. S59–S61†), indicating the formation of an Ir–Mo alloyed phase. Alternative fits using a Mo–Mo path instead of Mo–Ir resulted in higher R-factors (Table S23†) suggesting a lower probability of Mo–Mo bond formation. In addition, the fitted Mo–Mo bond for Ir–Mo/SiO2 was significantly elongated (ca. 2.91 ± 0.05 Å) in comparison to fitted Mo–Mo bonds in Mo foil (2.700 ± 0.004 Å), and to fitted Ir–Ir (2.697 ± 0.003 Å) and Mo–Ir (2.70 ± 0.05 Å) in the same sample, further supporting the hypothesis of Mo bonding to Ir over forming segregated Mo(0) domains.
![]() | ||
| Fig. 4 (a) LCF of fresh Ir–Mo/SiO2 with Mo(VI), Mo(IV), and Mo(0) references of Mo K-edge XANES spectra. (b) Mo K-edge EXAFS spectrum and fit of spent Ir–Mo/SiO2 after HDO of 1-nonanol. | ||
| Scattering path/Sample | IrMo | PtMo | RhMo | PdMo | NiMo |
|---|---|---|---|---|---|
| M–M fresh | 9.7 ± 0.7 | 10.3 ± 0.4 | 10.2 ± 0.8 | 8.3 ± 0.7 | 8.6 ± 0.9 |
| M–M spent | 9.7 ± 0.6 | 9.7 ± 0.4 | 9.7 ± 0.5 | 10.9 ± 0.5 | 8.3 ± 0.6 |
| Mo–O spent | 3.3 ± 2.0 | 3.5 ± 1.3 | 3.2 ± 1.5 | 3.3 ± 0.8 | 3.5 ± 0.6 |
| Mo–M spent | 2.5 ± 1.4 | 2.8 ± 0.9 | 3.7 ± 0.5 | 4.1 ± 0.4 | 0 |
From the perspective of Ir L3-edge EXAFS, no respective Ir–Mo path can be fitted for both the fresh and spent Ir–Mo/SiO2 catalyst, and only an Ir–Ir path consistent with metallic Ir is found. This is likely due to the low concentration of Mo with respect to Ir (1
:
8). Assuming only two types of Mo species are present (metallic and oxidic), consistent with the XANES spectra, Mo(0) and Mo(IV) are coordinated by Ir and O respectively, where the metallic Mo exhibits a Mo–Ir coordination number of 7.5 (=2.5/33%, from Table 2 and Fig. 5, respectively), which is within error of the respective coordination number for Ir–Ir (9.7), in accordance with Mo being incorporated in the nanoparticles. This is in line with the observations from CO chemisorption and parallels what has been reported for the Rh–Mo/SiO2 syngas conversion catalyst discussed above.39 On the other hand, the coordination number of Mo–O in Mo(IV) is found to be 4.9 (=3.3/67%, from Table 2 and Fig. 5, respectively), well in the range of nanostructured MoO2 with a coordination of 6 in the bulk structure. In this simplified picture, we assume that the oxidized Mo is distributed on the support, while Mo(0) is located in the metallic nanoparticles. Note, that the presence of an intermediate case of partially oxidized Mo on the nanoparticle surface, as proposed to form under syngas conversion conditions with Rh–Mo/SiO2, cannot be excluded. However, consideration of these species would result in the same conclusion of Mo–Ir undercoordination in the nanoparticle, hence a preferential localization of Mo on the nanoparticle surface.39
The monometallic Mo material, MoO3/SiO2, in the absence of Ir, is also reduced under HDO conditions (with 1-nonanol), but only from Mo(VI) to Mo(IV), while no metallic Mo(0) is observed, corroborating the strong interaction between Ir and Mo in Ir–Mo/SiO2 and the necessity of a second metal to achieve a reduction to Mo(0). Overall, these combined results confirm the reduction of Mo by Ir and the alloying of Mo into the Ir nanoparticles, consistent with what is observed by CO IR spectroscopy (vide supra).
Analysis of the XANES and EXAFS spectra of the corresponding Rh and Pt materials show similar trends, and the respective coordination numbers for M–M, M–Mo, and Mo–O after HDO (spent) are in the same range (Table 2 columns 2–4). In these systems, M remains metallic. Regarding the Mo K-edge, Mo(IV) and Mo(0) are present in the fresh materials along with Mo(VI), which is transformed to Mo(IV) and Mo(0) in the spent materials (Fig. 5, S40 and S41†). While EXAFS spectra at the Mo K-edge of fresh materials can again not be fitted reliably due to the coexistence of several species (vide supra), the EXAFS spectra of spent materials can be fitted with Mo–M paths, confirming the presence of M–Mo alloyed phases (Tables S6, S10, S14 and S18† and associated figures). Paralleling the observation with Ir–Mo/SiO2, the inclusion of Mo–Mo paths instead of Mo–M again results in higher R-factors (Table S23†) suggesting alloy formation to be the more likely scenario.
At 50% Mo(0), Pd–Mo/SiO2 exhibits the highest proportion of metallic Mo among the bimetallic materials, and in contrast to the other metals, the Mo(0) content does not evolve significantly during the reaction, paralleling the inactivity of this material in the HDO of 1-nonanol. The Pd–Pd coordination number after the reaction is higher than for the other metals and increases significantly during the reaction, while for the other bimetallic systems it remains constant within error. HAADF-STEM imaging of the spent material reveals the formation of a few large nanoparticles under reaction conditions in addition to smaller nanoparticles, consistent with sintering. EDX mapping shows a spatial correlation of Mo and Pd in larger nanoparticles, in line with alloy formation (Fig. S26†). In contrast to the other metals, this observed sintering behaviour parallels the inactivity in HDO with primary and secondary alcohols as well as the absence of (high concentrations of) Mo on the nanoparticle surface observed by CO-chemisorption, and it is likely that these phenomena are connected. On the other hand, the deoxygenation of tertiary alcohols can occur via a dehydration–hydrogenation pathway which is likely promoted by the tandem reactivity of oxidized Mo located on the support for dehydrogenation coupled to hydrogenation with (alloyed) Pd nanoparticles.
In the case of Ni-based materials, Ni K-edge XANES indicates a small but detectable amount of oxidized Ni(II) slightly variable (0–12%) across all samples (Fig. S42 and Table S1†). Mo K-edge XANES spectra show that in the fresh sample, there is a significant proportion of metallic Mo(0), while there is no Mo(IV) present. However, for the spent catalyst, all of Mo(VI) and most of Mo(0) are converted to Mo(IV). Moreover, no Mo–Ni path was detected in the Fourier transform of the Mo K-edge (or Ni K-edge) EXAFS of the spent Ni–Mo/SiO2 catalyst. In contrast to the other metals, while Mo(0) is present in the fresh Ni–Mo/SiO2 material, presumably in an alloyed state or the interface, it does not withstand the HDO conditions. This absence of an alloy phase parallels the absence of (or very low) HDO reactivity.
In summary, it can be concluded that across all the investigated bimetallic catalysts based on the motif M–Mo/SiO2, for which HDO activity is observed (M = Ir, Rh, Pt, and Pd for tertiary alcohols), Mo is reduced to a metallic state in significant extent and incorporated in the nanoparticles of M, forming an alloy. In contrast, no significant alloying is observed for Ni exposed to HDO conditions.
In contrast to primary and secondary alcohols (1-nonanol and 2-nonanol), the tertiary alcohol (2,6-dimethylheptan-2-ol) undergoes dehydration to olefins with MoOx/SiO2 under reaction conditions. Similarly, olefinic products are observed for the tertiary alcohol with both monometallic Ir/SiO2 and, to a greater extent, with Ir–Mo/SiO2 under inert atmosphere, while they are absent for 1-nonanol with Ir–Mo/SiO2 under the same conditions. This indicates that Mo increases surface acidity, which selectively impacts tertiary alcohols, and suggests a dehydration–hydrogenation mechanism is operative for these substrates (Fig. 6a). This explains the high activity of Pd-, Rh-, Ir-, and Pt-based bimetallic materials towards tertiary alcohols, and the modest activity of monometallic materials likely following the same mechanism. Ni–Mo/SiO2 shows slightly enhanced activity compared to Ni/SiO2 with tertiary alcohols while overall not exhibiting great compatibility with alcohols under the investigated conditions. For primary and secondary alcohols, a different mechanism is likely dominant and appears to be linked to the presence of reduced Mo species on the nanoparticle surface of Ir-, Rh-, and Pt-based bimetallic materials.
In light of the high Mo–O bond strength, one can propose that Mo sites on the surface of M–Mo alloyed nanoparticles help to activate the C–O bond by strongly binding oxygen functionalities, while the late transition metal activates H2 and helps to (re-)reduce both Mo and the hydrocarbyl part (Fig. 6b).15,23 This parallels what is observed with bimetallic reverse-water–gas-shift (RWGS) catalysts.39,46,47 We propose that the difficulty of maintaining reduced Mo on the surface contributes to the low activity of Ni–Mo, which undergoes dealloying under reaction conditions. Regarding Pd, CO chemisorption suggests Mo not to be present on the nanoparticle surface, which is also reflected by the negligible variation in Mo(0) content before and after the reaction with 1-nonanol. This suggests that reduced Mo is not accessible for alcohol substrates. However, oxidized Mo sites and/or silanols on the support can partake in acid-catalysed dehydration of tertiary alcohols, which is the presumed origin of the excellent chemoselectivity towards HDO of these substrates.
Coming to the role of Mo, with tertiary alcohols, the slight increase of Brønsted (and/or Lewis) acidity (not detected by pyridine as a probe molecule) appears to be sufficient to drive deoxygenation via a dehydration–hydrogenation pathway. However, for primary and secondary alcohols, a different mechanism is likely dominant. HDO activity for these substrates is linked to the formation of a Mo surface alloy, evidenced by XAS, CO-IR spectroscopy, and CO-chemisorption, suggesting reduced Mo sites on alloyed nanoparticles to be key. Presumably, Mo activates the C–O bond by coordination to oxygen followed by a redox process, while the other transition metal (Pt, Rh, or Ir) helps to activate H2, which is used to keep Mo in a reduced state and enable catalytic turnover. Keeping Mo reduced and accessible on the nanoparticle surface is likely to be the key balance for high activity with primary and secondary alcohols. While Ni does not form a (stable) alloy, Pd–Mo/SiO2 exhibits a high proportion of alloyed Mo, however, likely due to the low surface energy of Pd, Mo is concentrated in the bulk of nanoparticles. Possibly, this could be a mechanism for deactivation observed with Ir–Mo/SiO2, where the concentration of metallic Mo increases during the reaction.
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4sc08532a |
| ‡ These authors contributed equally. |
| This journal is © The Royal Society of Chemistry 2025 |