The theoretically predicted volcano plot for hydrogen production shows the best catalyst as the one that ensures that the hydrogen binding step is thermodynamically neutral. However, the experimental realization of this concept has suffered from the inherent surface heterogeneity of solid catalysts. It is even more challenging for molecular catalysts because of their complex chemical environment. Here, we report that the thermoneutral catalyst can be prepared by simple doping of a platinum atom into a molecule-like gold nanocluster. The catalytic activity of the resulting bimetallic nanocluster, PtAu24(SC6H13)18, for the hydrogen production is found to be significantly higher than reported catalysts. It is even better than the benchmarking platinum catalyst. The molecule-like bimetallic nanocluster represents a class of catalysts that bridge homogeneous and heterogeneous catalysis and may provide a platform for the discovery of finely optimized catalysts.
Hydrogen (H2) has been considered as an alternative energy carrier and generated the intense interest in creating artificial catalytic systems that can efficiently produce H2 from water1,2,3,4. Hydrogenase enzymes that contain iron and nickel cofactors are efficient hydrogen evolution reaction (HER) catalysts with turnover frequencies (TOFs) as high as 9,000 mol of H2 per mole of catalyst per second (mol H2 (mol cat)−1 s−1)5. There have been a variety of synthetic molecular catalysts, including nickel, cobalt, iron and molybdenum complexes, to mimic the biological catalysts6,7,8,9,10,11,12. However, the TOF values reported for these complexes remain quite low (<4.1 mol H2 (mol cat)−1 s−1), and they often show limited stability in aqueous media13. Moreover, practical electrocatalysis typically requires their immobilization on electrode materials that can operate fully in aqueous media14,15. Recent progress in the computational design of solid catalysts has revealed the importance of engineering of the structure and adsorption energies for catalysis at surfaces16,17,18. In fact, some engineered surface alloys exhibit high catalytic activities comparable to platinum18. However, the inherent heterogeneity in the surface structure and composition often found in these solid catalysts hamper the fine controlling of these properties at the molecular scale.
Ligand-protected gold and silver nanoclusters have received much attention as materials with many practical applications because of promises offered by their unique optical, electrochemical and catalytic properties19,20,21,22. Unlike the supported cluster systems23,24, these clusters are stable without the support and readily soluble in appropriate solvents. They have special stability at certain compositions, and thus molecule-like clusters with precise compositions are typically obtained from various size-controlled syntheses21,22. Au25(SR)18, Au102(SR)44 and Ag44(SR)30, where SR is a thiolate ligand, are the examples of these clusters whose stability is thought to arise from the closure of superatomic electron shells25,26,27. While stable clusters to date are rather limited to Au and Ag systems, bimetallic clusters prepared by doping a foreign metal into the stable Au and Ag clusters have opened an avenue to the fine-tuning of the cluster properties28,29,30,31,32,33. Here we report a highly active HER catalyst based on a molecule-like bimetallic cluster that can generate H2 with TOFs of 4.8 in tetrahydrofuran (THF) and 34 mol H2 (mol cat)−1 s−1 in water, respectively, at a moderate overpotential (η=0.6 V). This cluster catalyst represents a special type of catalyst that bridges homogeneous and heterogeneous catalysis.
Molecule-like metal nanoclusters
It has been found that Pt can selectively replace the central gold atom in the Au25 cluster, leading to a single Pt-doped bimetallic cluster (Fig. 1a)30,33,34. The Au25 and Pt-doped clusters were synthesized according to the procedures reported elsewhere34 (see Supplementary Notes 1–3 for details). Although they have been fully characterized in our previous report34, we will next briefly discuss their mass spectra, and optical and electrochemical properties, which can serve as an introduction to these molecule-like metal clusters. In Fig. 1b, the matrix-assisted laser desorption ionization mass spectra of the isolated gold (red) and Pt-doped gold clusters (blue) show only a single peak, indicating that the isolated clusters are extremely monodisperse. The peak at m/z ∼7,034 Da observed for the gold cluster (red) corresponds to the intact ion with a chemical composition of Au25(SC6H13)18. The peak at m/z ∼7,032 Da observed for the Pt-doped gold cluster is however almost superimposed with that of Au25(SC6H13)18 due to their small mass difference. The isotope pattern of the Pt-doped gold cluster (blue) shown in the inset of Fig. 1b can clearly be distinguished from that of Au25(SC6H13)18 (red) and matches well with the simulated isotope pattern (black) of PtAu24(SC6H13)18, manifesting that one Au atom in the Au25 cluster has been cleanly replaced by a Pt atom. Hereafter, these clusters will be abbreviated as Au25 and PtAu24, respectively. The average core size of both clusters is found to be around 1.1 nm (Supplementary Fig. 1).
The ultraviolet-vis-near-infrared (NIR) absorption spectra in Fig. 1c show distinctively different profiles of Au25 and PtAu24 clusters. The absorption profile is shown in the photon energy scale to show the broad NIR peak more clearly. The Au25 cluster exhibits the characteristic absorption features of Au25 clusters with peaks at 1.8, 2.8 and 3.1 eV. On Pt doping, the absorption profile changes drastically; that is, there is a new absorption band that appears at 2.1 eV with an additional NIR band centred at 1.1 eV in the low-energy region. The absorption profile of the Pt-doped cluster is consistent with that of neutral [PtAu24]0 where the Pt dopant is located at the centre of the core33. Evidently, replacing the central Au atom with Pt results in stable [PtAu24]0 having a superatomic 6-electron configuration25,26,34. The change in superatomic electronic configuration from 8-electron [Au25]− to 6-electron [PtAu24]0 would lead to the splitting of the 1P orbital accompanying a Jahn–Teller-like distortion of the PtAu12 core34. The appearance of the new bands at 1.1 eV (α) and 2.1 eV (γ) and the disappearance of the band at 1.8 eV (β) for [PtAu24]0 in Fig. 1c,d are the results of the change in electronic structure of PtAu24.
Electrochemistry and electrocatalytic activities
The optical measurements show that the electronic structure of Au25 cluster is drastically altered on doping of a Pt atom. To further unravel the electronic structure of the PtAu24 cluster, square-wave voltammetry (SWV) of Au25 and PtAu24 clusters were conducted. Voltammetry has been effectively used to study the electron transfer properties and the electronic structures of gold nanoclusters19,34. Understanding the redox behaviours near the HOMO-LUMO (highest occupied and lowest unoccupied molecular orbitals) levels is of particular importance in the design of efficient electrocatalysts. The SWVs in Fig. 2a exhibit well-resolved current peaks that lie at the formal potentials of the cluster charge-state couples. The open-circuit potential was found at −0.49 V for the Au25 cluster, indicating that the Au25 cluster is in anionic form, that is, [Au25]−. Therefore, the current peaks observed at −0.39 (O1), −0.04 (O2) and 0.69 (O3) correspond to the first, second and third oxidation peaks of the [Au25]− cluster, while the peak at −2.06 V (R1) corresponds to the first reduction peak. The electrochemical gap determined from the difference between the first oxidation (O1) and reduction (R1) potentials is found to be 1.67 V. The HOMO-LUMO gap for [Au25]− is determined to be 1.32 V by subtracting the charging energy term (O1–O2) of 0.35 V from the O1–R1 gap.
The redox potentials are drastically altered on doping of a Pt atom in the core as can be seen in Fig. 2a. Unlike the anionic Au25 cluster, PtAu24 is charge neutral with the open-circuit potential found at −0.49 V. Thus, the current peaks observed at −0.03 (O1) and 0.41 (O2) correspond to the first and second oxidation peaks of the PtAu24 cluster, while −0.76 (R1) and −1.10 V (R2) correspond to the first and second reduction peaks. The observed O1–R1 gap and the deduced HOMO-LUMO gaps from the SWV in Fig. 2a are found to be dramatically reduced to 0.73 V and 0.29 V, respectively. This result indicates that the electronic structure has indeed been greatly altered on Pt doping, and, more importantly, reduction potentials of [PtAu24]0 shifted positively by nearly 1 V compared to that of [Au25]−, potentially offering the possibility to lower overpotentials for reductive electrocatalysis.
Figure 2b shows linear sweep voltammograms (LSVs) in THF (0.1 M Bu4NPF6) solution containing 1.0 M trifluoroacetic acid (TFA) in the absence (black) and presence of Au25 (red) and PtAu24 (blue) clusters at a glassy carbon electrode (GCE). Compared to the blank current, the current for the proton reduction is significantly increased in the presence of Au25. The current further increases in the presence of PtAu24. The onset potential (Eonset) of catalytic current is observed at −1.10 V for Au25, positively shifted by 150 mV compared to that of the blank GCE. In the presence of PtAu24, the onset was found at −0.89 V, positively shifted by 360 mV. The thermodynamic reduction potential of proton is estimated to be −0.82 V in THF (1.0 M TFA) and thus the onset potential of −0.89 observed for PtAu24 corresponds to an overpotential of 70 mV (refs 35, 36), which is comparable to that of natural hydrogenase (∼100 mV) enzymes37.
The catalytic activity of PtAu24 was further examined with increasing the concentration of TFA. As shown in Fig. 2c, the LSV clearly shows current peaks at −0.76 and −1.10 V corresponding to the first and second reduction of the PtAu24 cluster. Whereas there is no significant change observed for the [PtAu24]0/− peak, the [PtAu24]−/2− peak current drastically increases with TFA, suggesting that HER is greatly enhanced at the potential where [PtAu24]2− is formed. That the HER current increases at the potential of the [PtAu24]−/2− couple strongly suggests that PtAu24 acts as an electron transfer mediator for HER that shuttles electrons from GCE to proton in the solution38,39. Interestingly, the onset potential of the second reduction of PtAu24 matches well with the Eonset (−0.89 V) observed in Fig. 2b, suggesting that the HER catalytic activity is indeed dependent on the charge state of PtAu24. When the catalytic activity of Au25 was examined with increasing concentration of TFA, the current increase at a more negative potential (−1.1 V) and the reduction current associated with HER was found to be much smaller (Supplementary Fig. 2). This result unambiguously shows that Pt doping significantly alters the redox potentials of the host cluster and thus drastically enhance its catalytic activity. In addition, the charge-state-dependent catalytic activity of PtAu24 clusters indicates that they are like molecular catalysts that carry discrete charge for reaction, which sets these clusters apart from other metal nanoparticle systems.
At sufficiently high acid concentration relative to the catalyst, the following equation can be used to calculate pseudo-first-order rate constant, kobs, for H2 evolution that is catalysed by freely diffusing catalysts:6,13,40
where Ic is the catalytic current, Ip is the peak current in the absence of acid (here taken from the wave of [PtAu24]0/− or [Au25]0/−), 2 is the number of electrons involved in the catalytic reaction, R is the ideal gas constant, T is the temperature in Kelvin, F is Faraday’s constant and v is the scan rate. As can be seen in Supplementary Fig. 3a, Ic increases with increasing acid concentration and levels off above 1.0 M TFA. At the acid concentration of 1.0 M, kobs was then obtained by plotting Ic/Ip as a function of v−1/2 as shown in Supplementary Fig. 3b. The kobs value calculated from the slope of the fit line (Supplementary Fig. 3b) is 121,000 s−1 at −1.5 V (η=650 mV). Under the same experimental condition, the kobs value calculated in the presence of Au25 is only 8,000 s−1. The rate constant observed for PtAu24 is also significantly higher than those reported to date for highly active molecular electrocatalysts; compared to cobalt complexes (700 s−1 at η=890 mV)41 and copper complexes (11,000 s−1 at η=720 mV)13 in comparable conditions, it is ca. 170- and 11-fold higher, respectively. To the best of our knowledge, the highest kobs value (106,000 s−1) thus far reported was observed at η=650 mV for a nickel complex that catalyses H2 formation with pendant amines that act as proton relays6. The kobs value obtained for PtAu24 is also higher than that.
To understand the origin of the extraordinary catalytic activity observed for PtAu24, we compared kobs as a function of potential. As can be seen in Fig. 2d, the kobs value found at −0.89 V is 1,300 s−1 and sharply increases to 62,000 s−1 at −1.1 V, followed by a gradual increase to 186,000 s−1 at −2.0 V. Interestingly, the potential where the drastic increase occurs matches well with the second reduction wave [PtAu24]−/2−. By contrast, the kobs value calculated for Au25 is found to be relatively small (<16,000 s−1) until −2.1 V, where [Au25]− is reduced to [Au25]2−.
Mechanisms of HER
The mechanism study shown in Fig. 3 clearly exhibits the charge-state-dependent catalytic activity of PtAu24. That is, the catalytic currents observed at potentials negative to the [PtAu24]−/2− wave (that is, −1.3, −1.8 and −2.2 V) all exhibit linear correlation with [PtAu24] and [TFA]1/2, respectively, which is consistent with the heterolytic HER mechanism (equation (3))42,43. On the other hand, at −1.0 V where PtAu24 is predominantly present in the form of [PtAu24]−, the currents exhibit linear correlation with [TFA] and [PtAu24]3/2, respectively, as shown in Fig. 3 insets, indicating the homolytic HER mechanism (equation (4))42.
This result is very reasonable considering the charge state of PtAu24. [PtAu24]2− reacts with proton to form [H-PtAu24]− intermediate that is negatively charged and thus preferably react with proton to evolve H2. On the other hand, at −1.0 V [PtAu24]− reacts with proton to form [H-PtAu24]0 intermediate that favours homolytic HER pathway. Similar charge-state dependence is observed for Au25. As shown in Supplementary Fig. 4, the catalytic currents exhibit linear correlation with [TFA] and [Au25]3/2, respectively, indicating homolytic pathway, at −1.0, −1.3 and −1.8 V, where Au25 clusters are present in the form of [Au25]−. When the cluster is reduced to [Au25]2− at −2.2 V, the currents exhibit linear correlation with [TFA]1/2 and [Au25], respectively, as shown in the insets of Supplementary Fig. 4, indicating the heterolytic HER pathway. The charge-state-dependent catalytic activity has been observed for electrocatalysis using Co complexes where [Co(II)H]− favours heterolytic HER pathway, while homolytic pathway is favoured by [Co(III)H]0 intermediate44. The charge-state-dependent catalytic activity of PtAu24 observed in this work clearly display the characteristic of molecular catalysts.
The charge state is not the only factor affecting the HER activity of the clusters. Comparing [PtAu24]2− with [Au25]2−, the kobs value calculated for [PtAu24]2− is 229,000 s−1, more than 10-fold higher than that of [Au25]2− (22,000 s−1) at −2.2 V at which both clusters are present as a dianionic form. The vastly different catalytic activity can be understood by considering the reduction potential match between the catalyst and the substrate (proton). That is, when the reduction potential of catalyst matches closely with the thermodynamic potential of proton, the catalyst can act as an effective electron transfer mediator and enhance its activity dramatically41,45,46. In this work, the reduction potential of catalyst can be precisely tuned to match with the potential of HER by Pt doping, enabling judiciously optimized electrocatalysis.
To gain further insight into the origin of the extraordinary catalytic activity of PtAu24, we have compared the hydrogen adsorption and the HER energetics calculated using density functional theory (DFT) for each cluster. We modelled the HER process by using protons solvated by two THF molecules, which are then adsorbed on the cluster surface; the whole system is further solvated by an implicit solvation model. Figure 4 shows that the energy change of the Volmer step (step 1) calculated for [PtAu24]2− is rather thermodynamically neutral (−0.059 eV), whereas that for [Au25]− is 0.539 eV. This result clearly suggests the initial hydrogen binding is energetically favourable on [PtAu24]2−, but is endothermic on [Au25]−, explaining the high HER activity observed for [PtAu24]2−. However, the second H adsorption on [PtAu24]2− and [Au25]− is found to be both endothermic; 0.369 and 1.21 eV for [H-PtAu24]− (step 2a in Fig. 4) and [H-Au25]0, respectively. Thus, the DFT calculations predict that hydrogen evolution occurs on PtAu24 via the coupling of the adsorbed hydrogen with another proton from the solution (that is, heterolytic or Heyrovsky pathway) with an energy change of −0.155 eV (step 2b in Fig. 4). By contrast, the most thermodynamically favourable H2 generation occurs on Au25 via the homolytic pathway (Supplementary Fig. 5). These calculation results are indeed in consistent with the experimentally found HER mechanisms for [PtAu24]2− and [Au25]−. The idea of thermoneutral catalysts for HER regarding hydrogen binding has been demonstrated experimentally for pure metals, alloys and layered solid catalysts16,17,18,47. Recently, it has been pointed out that this concept can be applied to molecular complexes, although it is significantly difficult to find the thermoneutral complexes because of their inherently complex chemical environment17,35,48. In this work, we have demonstrated that the redox potentials and binding affinity can be fine-tuned by simple doping of a Pt atom into gold catalysts, opening a new avenue to the fine-tuning of the catalytic properties.
Figure 4 also shows that the hydrogen preferably binds on the hollow site of the surface of the PtAu12 core. It is interesting to note that the bond distance between the central Pt and the adsorbed H is found to be 1.788 Å, significantly shorter than the distance between the surface Au and the adsorbed H (2.031 Å), indicating that the adsorbed H atom forms H-Pt chemical bond with the central Pt. In the DFT calculations, we initially placed the H atom on the intact cluster surface away from the Au atoms; during geometry optimization, we found that the H atom spontaneously moves into the subsurface to interact directly with the central Pt atom while breaking some surface Au-Au bonds. This result suggests that the H-Pt bond formation is a downhill process with no transition state. The H-Pt bond is also manifested in the local electronic density of states (Supplementary Fig. 6) that shows the hybridization between Pt 5d states and the H 1s state. The stronger H–Pt interaction than the H–Au interaction is a key factor contributing to the favourable HER energetics (Fig. 4) on [PtAu24]2− than on [Au25]−.
Electrocatalytic H2 production
To verify the catalytic production of H2, we carried out controlled potential electrolysis (CPE) with PtAu24 in THF containing 1.0 M TFA in an H-type cell. Figure 5a shows plots of the average current density and the amount of H2 detected by gas chromatography analysis at each overpotential. The clusters display symptoms of decomposition after prolonged CPE experiments and thus the electrolysis was conducted for 15 min. As can be seen in the figure, production of H2 is first detected at an overpotential of 0.2 V and increases with increasing overpotential. Comparison of the amount of H2 produced with the charge consumed indicates that the current efficiency for H2 production is > 97% when the overpotential is 0.4 V or higher. After subtracting the H2 production from the blank solution, the TOF at η=0.6 V is found to be 4.8 mol H2 (mol cat)−1 s−1. To the best of our knowledge, this value is considerably higher than any other molecular catalysts reported for HER in similar conditions6,7,8,9,12,13. The highest TOF value reported thus far is 4.1 mol H2 (mol cat)−1 s−1 obtained for a copper complex at a higher overpotential of 0.75 V (ref. 13). The nickel complex exhibiting a kobs value of 106,000 s−1 shows a TOF of 0.24 mol H2 (mol cat)−1 s−1 at η=0.92 V (ref. 6).
While PtAu24 exhibits high catalytic activity for H2 production with moderate overpotential requirements in a non-aqueous solvent, it would be more practical if it can be immobilized on electrode materials that can fully operate in aqueous media. There are a number of immobilization strategies available for gold nanoparticles via their surface functionalization39,49,50. In this work, PtAu24 cluster solution mixed with a carbon black (C) and Nafion was dropcast on a gas diffusion layer (GDL) electrode (PtAu24/C/GDL). We found that the clusters immobilized on the carbon black with the Nafion binder exhibit higher stability during electrolysis. Figure 5b shows plots of the average current density and the amount of H2 detected after 60 min CPE at each overpotential in 1.0 M Brinton–Robinson buffer solution (pH 3). As can be seen in the figure, H2 generation was achieved near the thermodynamic potential (η=70 mV), which also matches very well with the Eonset found in Fig. 2b. The charge passed and H2 generation increased rapidly with increasing overpotential and the current efficiency for HER went up to nearly 100% when the overpotential is 100 mV or higher. At η=400 mV, the average current density increases above 12 mA cm−2. Having immobilized such well-defined clusters on the electrode, we were able to calculate the TOF from the CPE experiments. As can be seen in Fig. 5b, the TOF values obtained from the heterogeneous catalysis are remarkably high; 34 mol H2 (mol cat)−1 s−1 at η=0.6 V in aqueous media after subtracting the contribution from the blank C/GDL electrode. This value is again much higher than those obtained in comparable conditions. For comparison, a TOF of 2.2 mol H2 (mol cat)−1 s−1 was obtained at η=0.59 V in acetate buffer (pH 4.5) for a cobalt catalyst immobilized on carbon nanotubes14.
Although it is not straightforward to directly compare the TOF values obtained from the homogeneous (Fig. 5a) and heterogeneous (Fig. 5b) catalysis, the enhanced TOF obtained in the latter in aqueous media is highly encouraging and may reflect the fact that all clusters on the electrode are available for catalysis. The high catalytic activity observed for the PtAu24/C/GDL electrode has prompted us to compare its activity with the benchmarking Pt/C (commercial 20 wt% Pt on Vulcan carbon black) dropcast on a GDL electrode (1 cm2). Since TOF could not be determined for the Pt/C, we have compared the H2 production rate per mass of metals (that is, Au+Pt) in the catalyst composites (mol H2 g−1 h−1). As can be seen in Fig. 5c, both PtAu24/C/GDL and Pt/C/GDL electrodes start to produce H2 near the thermodynamic potential, but the H2 production rate determined for the PtAu24/C/GDL is much higher than that for the Pt/C/GDL. For instance, the H2 production rate determined for the PtAu24/C/GDL is 25 mol H2 g−1 h−1, which is more than two times higher than that for the Pt/C/GDL catalyst (11 mol H2 g−1 h−1) at the same overpotential of 0.6 V.
Here we show that the electronic structure and the catalytic activity of a cluster catalyst can be fine controlled by doping a Pt atom into a stable gold cluster. The bimetallic cluster is molecule-like and exhibits excellent catalytic activity for H2 production; significantly higher than any other molecular catalysts reported thus far, to the best of our knowledge, and even higher than the benchmarking platinum catalyst. Mechanistic investigations have revealed that hydrogen binding step on the bimetallic cluster is thermodynamically neutral and the central Pt atom forms Pt-H chemical bond, pointing to a key role of the dopant. The molecule-like bimetallic cluster operates efficiently in both homogeneous and heterogeneous conditions, representing a special type of electrocatalyst. The molecule-like bimetallic cluster may thus provide a platform for the discovery of finely tuned catalysts, which could have broad implications for catalysis beyond H2 production.
SWV and LSV were conducted with an electrochemical workstation (model 660B; CH Instruments) in CH2Cl2 (SWV) or THF (LSV) containing 0.1 M Bu4NPF6 as a supporting electrolyte that was degassed and blanketed with a high-purity Ar gas. A GCE (3 mm diameter) was used as a working electrode, a Pt wire as the counter electrode and Ag/AgNO3 (0.1 M AgNO3 in CH3CN) as the reference electrode for the LSV experiments. SWV was carried out with a Pt disk (0.4 mm diameter) working electrode at 100 mV s−1 with a pulse height and a width of 20 mV and 20 ms, respectively. Ferrocene (Fc+/0) was added as an internal reference for Ag/AgNO3.
Controlled potential electrolysis
CPE experiments in homogeneous condition were conducted in a 5 ml cell containing 2.5 μM cluster and 1.0 M TFA dissolved in 2.0 ml THF (0.5 M Bu4NPF6) that was degassed and blanketed with Ar gas. Electrolysis was conducted for 15 min under vigorous stirring with an electrochemical workstation (model 660B; CH Instruments) equipped with three electrodes consisting of glassy carbon plate working electrode (area=1 cm2), a GDL (model N1S1007; CeTech Co., Taiwan) counter electrode (1 cm2) and a Ag/AgNO3 reference electrode. CPE experiments in heterogeneous condition were carried out for 60 min under vigorous stirring with a ZIVE MP1 potentiostat (WonATech, Korea) in an H-type cell that was equipped with a composite working electrode and a Ag/AgCl (3 M NaCl) reference electrode in one compartment and a platinum plate (1.68 cm2) counter electrode in the other compartment. The working electrode was separated from the counter electrode by a proton exchange membrane (Nafion 117; Sigma-Aldrich). Both compartments were filled with 60 ml of 1.0 M Brinton–Robinson buffer (pH 3.0) that was degassed and blanketed with Ar gas. The composite working electrode was fabricated by spreading a catalyst ink prepared by mixing 16 μg of the cluster catalyst, 200 μg of carbon black (Vulcan XC-72) and 1.5 μl of Nafion solution (5 wt%; Sigma-Aldrich) in 50 μl of THF on a GDL (N1S1007; CeTech Co.) electrode (1 cm2). For comparison, CPE experiments were conducted under the same condition using a commercial Pt/C (20 wt% platinum on Vulcan carbon black; Sigma-Aldrich) catalyst that was mixed with Nafion and dropcast on a GDL electrode (1 cm2). The average size of Pt particle was 3.5±0.5 nm. The amount of H2 evolved was quantified from an analysis of the headspace using an Agilent 7890B gas chromatography equipped with a thermal conductivity detector.
DFT calculations of the HER on Au25(SCH3)18 and PtAu24(SCH3)18 clusters were performed with the quantum chemistry program Turbomole V6.5. The def2-SV(P) basis sets were used for C, S and H, while effective core potentials which include scalar relativistic corrections and 19 (18) valence electrons were used for Au (Pt). Geometry optimization was done with the TPSS (Tao, Perdew, Staroverov and Scuseria) functional. In our calculations, solvent effects were treated implicitly by making use of the conductor-like screening model (COSMO) as implemented in Turbomole.
The authors declare that all the other data supporting the findings of this study are available within the article and its Supplementary Information Files or from the corresponding author on reasonable request.
How to cite this article: Kwak, K. et al. A molecule-like PtAu24(SC6H13)18 nanocluster as an electrocatalyst for hydrogen production. Nat. Commun. 8, 14723 doi: 10.1038/ncomms14723 (2017).
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This work was supported by the Korea CCS R&D Center (KCRC) Grant (NRF-2014M1A8A1074219). Q.T. was supported by the University of California, Riverside; D.-e.J. was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Chemical Sciences, Geosciences, and Biosciences Division.
Supplementary Figures and Supplementary Notes
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