Quan
Zhang
a,
Kohei
Kusada
*a,
Dongshuang
Wu
a,
Naoki
Ogiwara
a,
Tomokazu
Yamamoto
bc,
Takaaki
Toriyama
c,
Syo
Matsumura
bcd,
Shogo
Kawaguchi
e,
Yoshiki
Kubota
f,
Tetsuo
Honma
e and
Hiroshi
Kitagawa
*ad
aDivision of Chemistry, Graduate School of Science, Kyoto University, Kitashirakawa- Oiwakecho, Sakyo-ku, Kyoto 606-8502, Japan. E-mail: kusada@kuchem.kyoto-u.ac.jp; kitagawa@kuchem.kyoto-u.ac.jp
bDepartment of Applied Quantum Physics and Nuclear Engineering, Kyushu University, 744 Motooka, Nishi-ku, Fukuoka 819-0395, Japan
cThe Ultramicroscopy Research Center, Kyushu University, Motooka 744, Nishi-ku, Fukuoka 819-0395, Japan
dINAMORI Frontier Research Center, Kyushu University, Motooka 744, Nishi-ku, Fukuoka 819-0395, Japan
eJapan Synchrotron Radiation Research Insitute (JASRI), SPring-8, 1-1-1 Kouto, Sayo-cho, Sayo-gun, Hyogo 679-5198, Japan
fDepartment of Physical Science, Graduate School of Science, Osaka Prefecture University, 1-1 Gakuen-cho, Naka-ku, Sakai, Osaka 599-8531, Japan
First published on 25th April 2019
Au and Ru are elements that are immiscible in the bulk state and have the largest gap in reduction potential among noble metals. Here, for the first time, AuxRu1−x solid-solution alloy nanoparticles (NPs) were successfully synthesized over the whole composition range through a chemical reduction method. Powder X-ray diffraction and scanning transmission electron microscopy coupled with energy-dispersive X-ray spectroscopy showed that Au and Ru atoms are homogeneously mixed at the atomic level. We investigated the catalytic performance of AuxRu1−x NPs for the oxygen evolution reaction, for which Ru is well known to be one of the best monometallic catalysts, and we found that even alloying with a small amount of Au could significantly enhance the catalytic performance.
The key point in the synthesis of these solid-solution noble alloy NPs is the concurrent reduction of metal precursors.24,25 If the two kinds of metal ions are not reduced simultaneously, phase-separated NPs, such as core–shell or segregated types, would be obtained.26 However, it is not easy to simultaneously reduce two kinds of noble metal ions that have a large gap of reduction potential causing a remarkable difference in reduction speed, such as Au and Ru which have the largest gap among noble metals (Ru3+ + 3e− ⇌ Ru, E° = 0.455 V vs. Au3+ + 3e− ⇌ Au, E° = 1.498 V, as shown in Table S1†27).24,25
Ru is one of the best known highly active catalysts for the oxygen evolution reaction (OER).28,29 However, Ru catalysts are generally unstable in acidic solutions because Ru is easily oxidized in the working potential range of the OER.30–32 Au is known as the most stable metal and is used to improve the stability of metal catalysts.33–35 Actually, it is recently reported that even phase separated Au–Ru NPs show an enhanced OER performance.36 Therefore, the alloying of Au and Ru at the atomic level could be an effective way to improve the catalytic performance of Ru OER catalysts. In general, varying the composition of the solid-solution alloy has a great significance on its properties because the electronic structure of the alloy can be changed with its composition.22,23,37 Thus, it is interesting and challenging to create AuxRu1−x solid-solution alloy NPs over the entire composition range and to further systematically investigate their OER catalytic performance.
In this study, we carefully chose metal precursors with suitable ligands to overcome the limitation of the reduction potential difference and successfully obtained AuRu solid-solution alloy NPs over the entire composition range for the first time, although Au and Ru are immiscible throughout the entire composition range in the bulk state even at high temperatures up to their melting points (Fig. S1†).38 We also examined the OER catalytic performance of AuxRu1−x NPs and found that the activity continuously changed with composition and the alloy NPs exhibited an enhanced performance compared with pure Au and Ru.
The prepared samples were characterized by transmission electron microscopy (TEM) (Fig. S2†). The mean diameters of the AuxRu1−x (x = 0.1, 0.3, 0.5, 0.7, and 0.9) NPs were determined from the TEM images to be 6.6 ± 1.4, 15.7 ± 2.9, 15.4 ± 2.5, 15.3 ± 2.3, and 15.3 ± 2.7 nm, respectively. The particle size of Au0.1Ru0.9 is relatively smaller compared to other compositions. This may be related to the nature of Ru. X-ray fluorescence (XRF) and energy-dispersive X-ray (EDX) analyses confirmed the atomic ratios of Au and Ru in the prepared NPs (Table S2†). These results are consistent with the nominal ratios of the metal precursors used in the synthesis.
To clarify the structure of the obtained AuRu NPs, high-angle annular dark-field scanning TEM (HAADF-STEM) and EDX elemental mapping of Au and Ru were carried out. HAADF-STEM images and the maps of Au and Ru elemental distribution on the obtained AuxRu1−x NPs are shown in Fig. 1a–e and f–j, respectively. Au-L and Ru-L STEM-EDX maps of AuxRu1−x NPs are separately shown in Fig. S3.† These results give direct evidence of the homogeneous distribution of Au and Ru atoms in each particle. The typical EDX line scan profiles shown in Fig. 1k–o also demonstrate that Au and Ru atoms are well distributed in the particles, and the metal composition of the particles gradually changes from Ru-rich to Au-rich. These results show the formation of AuxRu1−x solid-solution alloy NPs over the entire composition range.
The crystal structure of the obtained AuRu NPs was investigated by synchrotron powder X-ray diffraction (XRD) analysis at BL02B2, SPring-8.40 The XRD patterns of AuxRu1−x NPs gradually change from face-centered cubic (fcc) to hexagonal closed-packed (hcp) patterns with increasing amounts of Ru (Fig. 2a). We then performed Rietveld refinement on each pattern of the alloy NPs (Fig. 2b, c and S4–S7†). The best fit of Au0.5Ru0.5 was obtained with two components of fcc and hcp (Fig. 2c). The lattice constant of the fcc component was calculated to be 3.960(6) Å, which is smaller than that of Au NPs (a = 4.077(1) Å, Fig. S8†). For the hcp component, the lattice constants were 2.795(1) and 4.435(3) Å for ahcp and chcp, which were larger than those of Ru NPs (a = 2.709(5) and c = 4.307(8) Å, Fig. S9†). As both hcp and fcc are close-packed structures, the lattice parameter afcc in a fcc structure is nearly √2ahcp in an hcp structure. Given that the lattice constant follows Vegard's law,41 the Au:Ru compositions of the fcc and the hcp phases were estimated to be 0.52:0.48 and 0.50:0.50, which are similar to the results of EDX and XRF analyses. These results strongly suggest that Au0.5Ru0.5 NPs contain two phases; however, both phases are solid-solution structures with the same composition. The lattice constants of AuxRu1−x NPs increased linearly with increasing Au content (x) as estimated by Rietveld refinement (Fig. 2b). The linear correlation between the composition and the lattice constant follows Vegard's law, which also confirmed the formation of the solid-solution AuRu alloy over the entire composition range.
Fig. 3a shows the linear sweep voltammetry (LSV) curves of the AuxRu1−x catalysts. The current densities of each catalyst at potentials of 1.5 and 1.6 V are shown in Fig. 3b and c. For the Ru catalyst, the current density has the highest value at around 1.5 V, but gradually reduces after that, which is caused by the dissolution of Ru with the potential increasing.30–32 The Au catalyst does not show obvious catalytic activity.42 The AuxRu1−x catalysts demonstrated the composition dependence of the catalytic performance. With increasing Ru content, the current density becomes higher. More importantly, Au is inactive for the OER; nevertheless, Au0.3Ru0.7 and Au0.1Ru0.9 catalysts show higher activity than Ru at 1.5 V. The current densities of the AuxRu1−x catalysts continuously increase with the potential increasing and are higher than that of the Ru catalyst at 1.6 V. This confirms the stability improvement of the AuxRu1−x catalysts. We further investigated the stability of Au0.3Ru0.7 and Au0.1Ru0.9 catalysts by chronopotentiometry tests at a constant current density of 2.5 mA cm−2 for 1 h (Fig. 3d and S11†).43,44 The curves show the potential change at a current density of 2.5 mA cm−2. The potential of the Ru catalyst quickly changed from 1.4 to above 2.0 V in 5 min, essentially losing all its activity. In contrast, the Au0.3Ru0.7 and Au0.1Ru0.9 catalysts showed a much slower deactivation during the stability test. From these results, it can be concluded that the alloy catalysts show much higher stability than the pure Ru catalyst.
We then investigated the structures of the Ru, Au0.3Ru0.7 and Au0.1Ru0.9 catalysts after the stability test by TEM, STEM-EDX and X-ray absorption near-edge structure (XANES). From TEM observations, we found that there were no Ru NPs on the carbon in the Ru/C catalyst after the test due to the rapid oxidation and dissolution of Ru (Fig. S12a†).30–32 In contrast, a large amount of Au0.3Ru0.7 or Au0.1Ru0.9 NPs remained on the carbon support (Fig. S12b and c†). We further analyze the structure of the alloy catalysts after the OER with Au0.3Ru0.7. HAADF- and bright field (BF)-STEM images (Fig. 4a–d) show the comparison of the alloy structures before and after the stability test. Both of the particles show the same fcc lattice and {111} interplanar spacing, indicating that the metallic structure of alloy NPs was mostly retained. However, a thin amorphous layer was observed on the alloy surface after the stability test. STEM-EDX analysis confirmed the good distributions of Au and Ru in the NPs (Fig. 4e–h, S13 and S14†). We further investigated the structure of the catalysts with XANES. The Au L3-edge and Ru K-edge spectra confirmed that the original alloy structure was maintained after the stability test, and indicated that the thin amorphous layer on the alloy surface would be RuOx (Fig. 4i–j).
To elucidate the enhancement of the catalytic performance, the change in the electronic structure caused by atomic level alloying of Au and Ru was investigated by XPS (Fig. S14, Table S3†). The Au 4f peaks of the alloys shifted to higher energy with increasing Ru content. By contrast, with the Au content increasing, the Ru 3p peaks of the alloys shifted to a lower energy. These results indicate electron transfer from Au to Ru in alloy NPs. According to the mechanism of the OER in an acid solution (Table S4†), the formation of intermediate oxygen species on the surface of the catalyst (e.g., *OH, *O, and *OOH; * represent active sites on the metal surface) is a key step for the OER process.45 These steps would be significantly affected by the change in the electronic structure of the catalyst. Thus, the change of the electronic structure in AuxRu1−x NPs could lead to better balance between adsorption and dissociation energies for oxygen species and further enhance the catalytic activity.46,47 At the same time, the electron transfer from Au to Ru in AuxRu1−x NPs could suppress the oxidation of Ru, which would be one of the origins of the enhancement in the stability of the AuxRu1−x alloy catalysts. Therefore, the alloying of Ru with Au improves the activity and stability of Ru as the OER catalyst in acid solutions.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9sc00496c |
This journal is © The Royal Society of Chemistry 2019 |