Subnanometer noble metal clusters have enormous potential, mainly for catalytic applications. Because a difference of only one atom may cause significant changes in their reactivity, a preparation method with atomic-level precision is essential. Although such a precision with enough scalability has been achieved by gas-phase synthesis, large-scale preparation is still at the frontier, hampering practical applications. We now show the atom-precise and fully scalable synthesis of platinum clusters on a milligram scale from tiara-like platinum complexes with various ring numbers (n = 5–13). Low-temperature calcination of the complexes on a carbon support under hydrogen stream affords monodispersed platinum clusters, whose atomicity is equivalent to that of the precursor complex. One of the clusters (Pt10) exhibits high catalytic activity in the hydrogenation of styrene compared to that of the other clusters. This method opens an avenue for the application of these clusters to preparative-scale catalysis.
Noble metal nanoparticles are of particular importance in terms of emerging technologies requiring highly active catalysts for fuel cells1, gas reforming2, and even fine chemical conversion using tandem flow reactor systems3. Although catalytic activities of conventional particles moderately depend on the particle size mainly due to the differing surface-to-volume ratios4, evolution of edges5, kinks, steps6, or higher plane indices7 occasionally elicits drastic changes in their properties. From the standpoint of these deliberate defect implementations, extreme miniaturization of the particle is the ultimate approach because subnanometer particles consequently have a specific structure that has no periodicity against crystalline nanoparticles. Such clusters on a subnanometer scale indeed showed distinct properties especially for catalytic applications due to above-mentioned geometric nature or electronically induced superatomic character elucidated by early studies8,9,10,11,12. To study the specific activities, a gas-phase synthesis with the mass selection of each cluster has been the only way providing the atomicity control with satisfactory precision and scalability9, 13,14,15,16,17,18. However, this approach is only applicable for analytical-scale catalysis due to the limited throughput of the mass selection.
As one of the few pioneering examples of this scale-up, we recently reported a dendrimer-based fine cluster synthesis method that allowed atomicity control with single-atom precision19, and found that the catalytic activity was highly sensitive to the atomicity between 12 and 2020. The overall trend indicated that a metastable cluster provided a better catalytic performance21. If such a precise large-scale synthesis could be applied to every atomicity with a much easier procedure, the cluster science would allow to access the next practical level, taking full advantage of the systematic implementation of such an atomicity-specific metastable nature.
Platinum is the most important metal element for nanoparticle catalysis. As the precursors of such ultrasmall platinum subnanoparticles, platinum thiolates are currently being investigated because reductive metal-sulfur bond cleavage might lead to the formation of bare metal clusters. The thiolates can form tiara-like cyclic complexes stable enough for isolation22,23,24,25,26,27. In principle, such tiara-like complexes are available with atomicities of 4 and higher28. This might allow fully scalable synthesis regardless of the specific stable magic numbers just like the gas-phase synthesis. Although several syntheses from stable ligand-protected “magic number” clusters29, 30 or multinuclear complexes31, 32 have been attempted, these precursors were not scalable, and the exact definition of the atomicity was never demonstrated. One of the issues is the high metal-to-ligand binding energy, which requires extremely high calcination temperatures leading to the aggregation10.
Here we show the scalable synthesis, characterization, and fundamental properties of platinum tiara-like complexes with octanethiol ligands. The synthesis of monodispersed subnanometer platinum clusters and their catalytic activity for preparative-scale reactions are investigated by achieving the non-destructive quantitative conversion from the complexes to the clusters.
Synthesis of precursor complexes
Only one example of a platinum thiolate tiara-like complex with a full chemical identification (nuclear magnetic resonance (NMR), mass, and elemental analysis) has been published33. Therefore, we began this study with the investigation of the basic reactions between PtCl4 and n-octanethiol (C8H17SH). The reaction at room temperature in a chloroform/acetonitrile solution was monitored by positive-ion matrix-assisted laser-desorption-ionization time-of-flight mass spectrometry (MALDI-TOF-MS) using trans-2-[3-(4-tert-butylphenyl)-2-methyl-2-propenylidene]malononitrile (DCTB) as the matrix34. After 3 h, many peaks below 5000 Da associated with mono-cationic species were observed. Some of them could be attributed to the desired [Pt(µ-SC8H17)2] n + (n = 5–9) species, including their isotropic patterns, while each of them was accompanied by a minor species with an additional 216 Da mass. Because this additional mass is equivalent to the sum of C8H17SH and Cl2, these minor species are thought to be linear oligomers, [Pt(µ-SC8H17)2] n (SC8H17)2Cl2, detected as fragment [M-SC8H17]+ ions. Based on this initial result, it is anticipated that platinum thiolates initially undergo a linear chain growth reaction35 followed by the entropically favorable formation of smaller cyclic compounds36. Based on this idea, the synthesis protocol was optimized in two steps. PtCl4 was reacted with four equivalents of n-octanethiol (C8H17SH) in a chlorobenzene/acetonitrile (1/1) mixed solvent at 90 °C in the presence of diisopropylethylamine (DIEA). After 1 h, the reaction mixture was concentrated, and further treated in chlorobenzene with excess C8H17SH at 125 °C for an additional hour. The crude product containing the tiara-like complexes with various ring sizes [Pt(µ-SC8H17)2] n was obtained in an overall 36% yield.
All the tiara-like complexes [Pt(µ-SC8H17)2] n (Fig. 1a: n = 5–13) were isolated by size-exclusion chromatography. The hexane-soluble part of the product was extracted as a crude mixture, then subjected to preparative size-exclusion chromatography. Finally, pure complexes with different ring sizes could be isolated up to 25 recycling processes by our apparatus (see Methods section). MALDI-TOF-MS of the product mixture before the isolation showed the presence of various complexes [Pt(µ-SC8H17)2] n . The highest peak intensities were observed at n = 8 and 9, whereas even a high molecular weight complex (n ~ 30) was found. Remarkably, every complex (5 ≤ n ≤ 30) had a molecular weight attributed to the cyclic tiara-like structures. The refractive index chromatogram after several recycling processes exhibited many independent peaks (Fig. 1b), which were successfully characterized by ring size using MALDI-TOF-MS based on their isotope patterns. The isolations were their successful for complexes with ring sizes between n = 5 and 13 (Fig. 1c). All the compounds except for [Pt(µ-SC8H17)2]13 were fully characterized by 1H NMR, 13C NMR, and elemental analyses in addition to MALDI-TOF-MS (Supplementary Methods). Single-crystal X-ray structures were successfully obtained for n = 6 and 8 (Supplementary Figs. 1, 2; Supplementary Table 1) showing their tiara-like macrocyclic structures. Although crystallographic data were not available for the other rings due to their poor crystallinity, all the given structures were optimized (Fig. 1d) at the B3LYP/LanL2DZ level using Gaussian 0937. To reduce the calculation cost, methylthiol (CH3SH) was used instead of octanethiol (C8H17SH) as the ligand.
Conversion to atom-precise clusters
The thermostability of the complexes was next investigated in order to reveal their potential as precursors for atom-precise platinum clusters. Under a helium atmosphere, it was determined that the coordinating thiolate ligands start being eliminated at 200 °C. A thermogravimetric-differential thermal analysis with mass spectrometry (TG-DTA-MS) indicated that the C–S bonds of the thiolate ligands were cleaved first, followed by the Pt–S bond cleavages (Supplementary Fig. 3). Although these bond cleavages for the palladium thiolates occurred completely stepwise38, the present platinum thiolate almost concurrently underwent two cleavages. This result suggested that selective conversion of the tiara-like platinum complexes to the corresponding platinum (metal) or platinum sulfide clusters is in principle difficult. However, the reductive Pt–S bond cleavages for the selective production of zero-valent platinum clusters were possible under a hydrogen gas stream. When a thick [Pt(µ-SC8H17)2] n film on a glass substrate was heated at 250 °C for 2 h under a pure H2 stream, a metallic film was formed. It was determined to be polycrystalline platinum by an X-ray diffraction (XRD) measurement (Supplementary Fig. 4).
[Pt(µ-SC8H17)2] n were supported on carbon (Ketjenblack) in order to preserve the atomicity of the precursor during the reduction (Fig. 2a). After a low-temperature (250 °C) calcination of the supported [Pt(µ-SC8H17)2] n for 2 h, X-ray photoelectron spectra (XPS) of the products indicated that a trace amount of sulfur remained on the carbon-supported cluster. Further optimization of the calcination conditions determined that the formation of zero-valent Pt (Pt 4f 7/2: Fig. 2b) and complete removal of the thiolate ligand (S3p 3/2: Supplementary Fig. 5) were possible using a longer reduction time (18 h) with a high H2/N2 (3%) flow rate. In the case of [Pt(µ-SC8H17)2]12, the XPS was almost identical to that for Pt12 produced by the dendrimer-reactor method19. HAADF-STEM images of the as-synthesized clusters indicated monodispersed Pt clusters supported on the carbon (Fig. 2c), with sizes similar to those previously reported for Pt12 39. The most important detail is that the procedure is universal for other atomicities derived from various complexes [Pt(µ-SC8H17)2] n (n = 5–12). The sizes of all of the particles in the STEM images were close to that expected based on the structural models (Supplementary Figs. 6, 7).
The histograms of each cluster size are apparently monodisperse accompanying small distributions. It is important to note that these distributions are not only due to the distributions in the cluster atomicity, but also due to the different projected shapes and the inevitable defocus by the strictly limited focus depth. Thus, we suggest that quantitative evaluation based on the size distribution is at the limit at the subnanometer scale. Instead, detailed study on the precision of atomicity control by nucleation of the atom-precise precursor is possible by the observation at the subatomic scale. For example, Ketjenblack as a support loading [Pt(µ-SC8H17)2]8 at the weight percentage of 1.0 wt% was investigated by high-resolution HAADF-STEM. Although the atomicity was completely retained before the reduction, the number of observed particles decreased after the reductive calcination. Larger particles containing 16, 24, or more Pt atoms were also observed, suggesting the aggregation during the reduction (Supplementary Fig. 8). Increase of the platinum loading to 1.8 wt% resulted in promotion of the cluster aggregation producing nano-crystalline particles with ca. 2 nm in the diameters (Supplementary Fig. 9). In contrast, the decrease of the loading to 0.4 wt% significantly suppressed this aggregation. Conversely, production of smaller clusters due to the decomposition was hardly observed. In this case, the atomicities of each cluster are almost preserved from the precursor complex (Supplementary Fig. 10). For the statistical analysis of the particle aggregation, the numbers of particles before and after the reductive calcination were counted (Supplementary Fig. 11). Residual ratio (R) is defined as R = N after/N before where N before and N after are the numbers of observed particles within a sampling area. If the particles did not aggregate at all, R should be 1. Average particle-to-particle distance was derived from the number of Pt–thiolate complexes (before the calcination) in the sampling area of the projected STEM image; therefore, it does not describe the actual distances between the precursors but the distances as seen on the STEM image. Increase of the Pt loading (wt%) on the carbon support (Ketjenblack) decreases the distance. This analysis suggests that the original particle could be preserved if the particle-to-particle distance was longer than ca. 7 nm on the STEM image. This optimized method allowed the selective and atom-precise synthesis of clusters ranging from Pt5 to Pt12 as shown by the atomic resolution HAADF-STEM images (Fig. 2d). Based on the investigations, the cluster samples for the following structural and catalytic examinations were prepared with a net platinum content of ≤0.4 wt% or less. Details of the sample preparations are described in the Methods section.
Atomic-level electronic and structural information, such as the valence states, coordination numbers, and interatomic distances, was investigated by Pt-4f XPS and Pt-L 3 EXAFS spectroscopy of the resulting Pt clusters (n = 8). As mentioned above, the as-synthesized clusters were reduced, but the binding energies were higher than that of the bulk platinum metal (70.9 eV). As previously reported, this is considered to result from partial oxygen adsorption to the surface and the final-state effect40. The dependence on the size of the cluster is not significant in the range of the atomicity investigated in this study (Supplementary Figs. 12 and 13), but this trend is consistent with the previous mass-selected platinum clusters synthesized by the vacuum-phase method17. The EXAFS spectrum of [Pt(µ-SC8H17)2]8 calcined under a H2/N2 stream was different from that for the untreated complex (Supplementary Figs. 14 and 15). A curve-fitting analysis elucidated that the average Pt–Pt distance was 2.71 Å. The very small coordination number (CN = 3.5 ± 2.1) was within the range of the expected values for Pt8 41, supporting the formation of tiny clusters without nonnegligible aggregation (Supplementary Table 2). In addition to the Pt–Pt bonds, consideration of the adjacent light elements (C or O) provided a better curve-fitting result. It should be noted that the contribution of Pt-S shell cannot be excluded from the analysis of EXAFS. Based on the XPS results, i.e., that calcined Pt8 indicated significantly low amount of S atoms relative to the thiolate precursors, the possible adjacent atoms would be the carbons on the Ketjenblack. The large coordination number (CN = 6.6) for the relatively long Pt-C (2.17 Å) may suggest a flat structure of Pt8 on the graphitic carbon substrate.
The catalytic study of atomically precise clusters is limited to recent pioneering experiments such as the reactions of gaseous molecules with gas-phase clusters beam or soft landed clusters on a flat substrate9, 13,14,15,16,17,18. However, none of the activity, selectivity, and durability under practical conditions were studied. The present method provides a new pathway for the large-scale production of atom-precise clusters. As the demonstration of preparative-scale catalysis, we performed the hydrogenation of styrene and the aerobic oxidation of neat indane.
The cluster catalysts exhibited characteristic property in the hydrogenation reaction of styrene (Fig. 3a), which has been investigated by the platinum nanoparticles42, 43. While no reaction was confirmed by blank Ketjenblack, Pt8 cluster supported on Ketjenblack (Pt8/KB) as a catalyst clearly promoted the hydrogenation reaction of styrene, suggesting that the platinum clusters act as the catalyst. Ethylbenzene as the product was formed immediately after the initiation of the reaction, and was increased with the reaction time (Fig. 3b). Similar catalytic hydrogenation was also investigated on other platinum clusters (Pt9/KB, Pt10/KB, and Ptx/KB as larger Pt nanoparticles shown in Supplementary Fig. 16) used as the catalyst. As a remarkable point, these clusters showed different catalytic activity despite the only one atom difference of the composition. Among these clusters, Pt10/KB exhibited the highest activity.
We can now investigate the characteristics of catalysts not only for the reactivity but also for the new aspects such as degradation of the cluster in the reaction or the possibility of reuse, because it has become possible to obtain clusters with the atomic precision on the preparative scale. Although very low stability of such small clusters is anticipated, the Pt10/KB catalyst after the hydrogenation reaction for 2 h observation of the atomic resolution STEM showed unexpectedly retained without obvious aggregation and decomposition (Fig. 3c, d). More careful observation at the atomic scale revealed the existence of single atoms probably arising from the elimination from clusters. However, the frequency was not significant. Based on this characteristic of the present supported cluster catalyst, it is possible to conduct a reuse experiment, in which the product is removed after the reaction, followed by the addition of the substrate to restart (Fig. 3e). The durability of clusters is not excellent at this time, but it would be possible to produce a cluster catalyst with higher durability by changing the cluster composition or improving the interaction with the support.
In contrast, in reactions under oxidative conditions, cluster degradation were more pronounced. Under an oxygen atmosphere, Pt8, Pt9, or Pt10 supported on Ketjenblack were added to freshly distilled indane, and the reaction was carried out at 90 °C. After 6 h, oxidized products including 1-hydroperoxy-indane, 1-indanol, and 1-indanone were observed by 1H NMR. In this oxidation reaction, the dependence on the cluster atomicity is hardly observed, and an induction period of several hours was observed until the production of the product. The atomic-level investigation revealed that the atomicity of each cluster changes due to the formation of many single atoms (Supplementary Fig. 17). Therefore, under this oxidative condition, it is strongly indicated that the true active species is not the original cluster. The atomicity of the clusters after the hydrogenation reaction at room temperature was rather preserved relative to the oxidation condition at 90 °C.
In general, catalytic properties of metal nanoparticles are discussed based on surface-to-volume ratio, surface structure44, or d-band center45 as shown in the studies of many metal nanoparticles4. However, these discussions cannot be applied to the present cluster series with such low atomicites. For example, the Pt8, Pt9, and Pt10 cluster already exposes all of their atoms on the surface. The surface of these clusters are not attributed to any specific surface index because the clusters do not have lattice structures. In addition, difference in the electronic state of the clusters are not significant as shown by the valence states of the clusters characterized by the XPS measurements (Supplementary Fig. 13). Based on this idea, it is considered that the difference in the activity cannot be simply explained by the conventional discussions.
In order to elucidate the specific enhancement of styrene hydrogenation by Pt10, density functional theory calculations were performed with the B3LYP functional, LanL2DZ basis set for platinum atoms, and 6–31 G (d, p) basis set for hydrogen and carbon atoms, using Gaussian 0937. Styrene hydrogenation consists of two processes: hydrogen insertions into α-carbon and β-carbon, as shown in Fig. 4a. Accordingly, reaction barriers of these processes were calculated under the existence of Pt8, Pt9, or Pt10 catalyst. Obtained reaction barriers are shown in Fig. 4b. The corresponding transition states with Pt10 are illustrated in Fig. 4a, and those with Pt8 or Pt9 are available in Supplementary Fig. 18. Figure 4b shows that the α-insertion requires high activation energy with Pt8 or Pt9, and thus is the rate-determining step. On the other hand, Pt10 catalyst was found to lower the reaction barrier of the α-insertion considerably. This difference of the energy barriers might be attributed to both electronic and geometrical factors. According to the recent theoretical studies48, 49, Pt8 and Pt9 favor (quasi-)two-dimensional structures, whereas Pt10 prefers a rigid pyramidal one. Our calculation shows that platinum atoms at the vertices of the pyramidal Pt10 are very electron-rich, which can activate a carbon double bond effectively. In contrast, Pt8 and Pt9 do not have such electron-rich sites. The calculated charge distributions are shown in Supplementary Fig. 19. Furthermore, non-rigid structures of Pt8 and Pt9 might interact with phenyl group of styrene strongly, which would impose unfavorable geometrical constraints on the reactant during the reaction. This is one of the plausible reasons why Pt10 catalyst facilitates styrene hydrogenation specifically. According to our calculations, atomicity of platinum catalyst does not affect the reaction barrier of the insertion into β-carbon, which is sufficiently low regardless of atomicity.
Although catalytic properties of relatively larger clusters have been discussed based on theoretical calculations46, 47, it is, in principle, difficult to uniquely determine its structure and activity in a smaller cluster composed of 1–10s of atoms because the structure dynamically changes as observed in STEM. Our calculation result represents only one of the most probable reaction path of the catalysis. Strictly speaking, it is necessary to consider all of the multiple metastable structures and all the corresponding reaction pathways for the quantitative evaluation.
Recent theoretical calculations explain that Pt10 is a magic cluster having a more stable and less fluxional structure than other clusters, and there are fewer isomers48, 49. Some of the previous gas-phase investigations suggested that the Pt10 cluster is stable but unreactive50,51,52. Apparently, these claims seem to be inconsistent with our experimental and theoretical results. However, the atomicity dependence should be much different by the substrate molecules. In addition, the present hydrogenation reactions were performed in hours order. Thus, it can also be considered that the resistance to cluster dissociation and aggregation was also essential for the high turnover numbers as expected from the STEM observation after the reaction. In the case of such a very small cluster, it might also be necessary to consider the differences in the interaction with the carbon support, which should contain a lot of oxygen-containing groups (hydroxyl or ketone). Actually, we have encountered unexpected deactivation of the catalysis as described in the Methods. For a complete understanding of the catalyst system by such very small clusters, further investigation on the stability and the support effect is the next important subject.
In summary, we successfully isolated various tiara-like platinum thiolate complexes, whose atomicity ranged between 5 and 13. A study on the thermal chemical conversion revealed that the tiara-like platinum thiolate complexes were suitable precursors for the synthesis of monodispersed zero-valent platinum clusters with a specific atomicity (n = 5–12), which had been inaccessible by previous chemical methods. Especially, the Pt10 cluster prepared from the tiara-like complex exhibited an exceptionally high catalytic activity for the hydrogenation reaction of styrene relative to the other clusters (Pt8, Pt9, or larger one). To the best of our knowledge, this is the first example demonstrating a preparative-scale reaction using atom-precise clusters with a single-digit atomicity. Because a similar procedure is generally possible for the synthesis of nickel and palladium clusters, this method is expected to be useful for producing high-performance catalysts.
PtCl4 was purchased from Furuya Metal Co., Ltd. N,N-diisopropylethylamine and n-octanethiol were purchased from Tokyo Chemical Industry Co. Ltd. Styrene was purchased from Aldrich. All the other chemicals and solvents were purchased from Kanto Chemical Co., Inc. These chemicals were used as received unless otherwise specified.
Synthesis of platinum thiolate complexes
PtCl4 (303 mg, 0.90 mmol) was dissolved in a mixed solvent (monochlorobenzene/acetonitrile = 1/1, 300 mL), and the solution was heated at 90 °C for 1 h in the presence of N,N-diisopropylethylamine (69 mmol) and n-octanethiol (3.6 mmol). The resulting solution was evaporated to dryness. The crude product was again dissolved in monochlorobenzene (10 mL) containing n-octanethiol (9.0 mmol), and reacted at 200 °C for an additional 1 h. During the reaction, the solution color was changed from red to pale yellow. After the reaction, the solution was centrifuged to remove the insoluble part as a precipitate. The soluble part includes tiara-like complexes with various ring numbers as a mixture.
Isolation of the complex
A preparative recycling HPLC (Japan Analytical Industry: LC908) was used for the purifications using chloroform as the eluent. Two tandemly arrayed size-exclusion columns (Japan Analytical Industry: JAIGEL-2H and JAIGEL-2.5H) were used. After several recycling processes, each fraction was isolated. During the recycling process, larger oligomers were collected first. After the additional recycling processes, each tiara-like complex was collected in order. The collection was completed up to 25 cycles. Each fraction was checked by MALDI-TOF-mass measurement, and then the product was characterized by 1H, 13C NMR, and elemental analysis (Supplementary Fig. 20; Supplementary Methods).
Typical procedure for the synthesis of Pt n clusters
Ketjenblack, KB (30 mg) was dispersed in hexane (200 mL) by ultrasonic dispersion. Hexane solution of [Pt(C8H17S)2] n (5 mL) was added dropwise to the suspension of KB while stirring (500 rpm). After stirring for 15 min, the suspension was filtered under suction through a Millipore filter (0.2 μm pore diameter). The collected fine powder of [Pt(C8H17S)2] n supported on KB was treated under hydrogen gas stream (3% H2/N2, 3 L min−1) at 250 °C in a tube furnace (KOYO Thermosystem Inc., KTF040N1-AS) for 18 h. This conversion process from the complexes to the metal clusters (Pt n /KB) is quantitative.
For the synthesis of monodisperse clusters, weight percentages of platinum content were set to be 0.2 and 0.4 wt% for Ketjenblack, respectively, for Pt n≤6 and Pt n≥7. In the case of reference catalyst as the larger platinum nanoparticles, [Pt(C8H17S)2]9 supported on KB at 1.8 wt% (Pt atom weight percentage) was used as the precursor.
Preparation of the bulk Pt film for XRD analysis
A small portion (ca. 0.1 mL) of a high-concentration solution (ca. 0.1 mol L−1) of the platinum complex mixture (containing various ring numbers) in chloroform was dropped onto a quartz-glass substrate (1 cm2), and was stored in air to give yellowish transparent film until the solvent was evaporated. The thick transparent film was changed to silver metallic film after a process under hydrogen gas stream at 250 °C for 1.5 h.
Catalytic hydrogenation of styrene for the kinetic study
Hydrogenation of styrene was conducted in a test tube, which was joined to a three-way stopcock, which was connected to vacuum and an argon or hydrogen balloon. Styrene was distilled prior to use. Pt clusters supported on carbon (0.04 μmol Pt) and 1.5 mL solution of the styrene in methanol (0.13 mol L−1) was added to the test tube. The reaction vessel was flushed three times each with argon and then with hydrogen gas. The hydrogenation reactions were carried out under pure hydrogen (1 atm) at 25 °C with magnetic stirring (400 rpm). The reaction mixture was analyzed by gas chromatography.
In the evaluation of hydrogenation catalytic activity, it is common to activate the catalyst by hydrogen reduction treatment. However, our examinations suggested that the apparent catalytic activity is significantly decreased by the hydrogen reduction treatment of the catalyst just before the activity test. In addition, it was found that the catalyst turnover was also affected by the distillation of styrene. It should be noted that the pretreatment of the catalyst, the support effect, or the influence of impurities in the reaction mixture are not fully understood. Therefore, the experiments should be conducted with care so that the history of each catalyst was the same. Nonetheless, special attention is needed on the discussion of absolute values of the catalytic activity.
Catalytic hydrogenation of styrene for the recycling and stability test
In a test tube joined to a three-way stopcock, which was connected to a hydrogen balloon, 4.9 mg of Pt10 supported on Ketjenblack (0.1 μmol Pt) was reacted with 1.5 mL solution of styrene in methanol (0.07 mol L−1). The hydrogenation reaction was carried out for 2 h under pure hydrogen (1 atm) at 25 °C with magnetic stirring (400 rpm). After the reaction, the reaction mixture was dried under vacuum to remove methanol, styrene, and ethylbenzene. A small part of the sample was used for the STEM observation. The catalyst was further washed with methanol and then dried under vacuum. The recovered catalyst was used in the subsequent reaction. Three cycles of the catalysis were investigated to examine the reusability of the catalyst.
Calculations of styrene hydrogenation
Geometry optimizations and vibrational analyses were performed for intermediates and transition states of styrene + H2 with Pt8, Pt9, or Pt10 catalyst, using the B3LYP functional, LanL2DZ basis set for platinum atoms, and 6–31 G (d, p) basis set for hydrogen and carbon atoms. The most stable structures of platinum clusters reported previously48, 49 were employed as initial geometries in these calculations. The obtained intermediate structures have no imaginary frequency. In addition, the transition states have only one imaginary frequency. All the calculations were carried out with the Gaussian 09 program package37.
The X-ray crystallographic coordinates for structures reported in this article have been deposited at the Cambridge Crystallographic Data Centre (CCDC), under deposition nos. CCDC 1563559 and 1563560. These data can be obtained free of charge (http://www.ccdc.cam.ac.uk/data_request/cif). All other reported data are available from the corresponding authors on reasonable request.
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This study was supported in part by JST ERATO Grant Number JPMJER1503, Japan (K.Y.), JST PRESTO Grant Number JPMJPR1511, Japan (T.I.), JSPS KAKENHI Grant Nos. JP 15H05757 (K.Y.), JP 16H04115 (T.I.), and the Cooperative Research Program of “Network Joint Research Center for Materials and Devices” (W.-J.C.). The XAFS measurements were conducted at the BL9C and BL12C beamlines of High Energy Accelerator Research Organization–Institute of Materials Structure Science-Photon Factory (KEK-IMSS-PF) under the approval of the Photon Factory Advisory Committee (Nos. 2013G568 and 2017G046). We thank Dr. Sei (Suzukakedai Materials Analysis Division, Technical Department, Tokyo Institute of Technology) for the crystallographic analysis, Dr. Y. Nemoto (NIMS microstructural characterization platform) for assistance with the high-resolution STEM observations and Dr. Y. Negishi (Tokyo University of Science) for discussions about the MALDI-TOF-MS measurement.