Open Access Article
Yanna Song
a,
Jingcheng Suna,
Yanru Zhanga,
Bingxin Wanga,
Qiang Li
*c and
Yongming Fan*ab
aMOE Engineering Research Center of Forestry Biomass Materials and Bioenergy, Beijing Forestry University, Beijing, 100083, China
bKey Laboratory of Lignocellulosic Chemistry, Beijing Forestry University, Beijing 100083, China. E-mail: fanym@bjfu.edu.cn; Tel: +86-185-15301003
cCollege of Science, Beijing Forestry University, Beijing 100083, China. E-mail: liqiang@bjfu.edu.cn; Tel: +86-137-18679671
First published on 17th April 2018
Urchin-like RuCu nanoparticles and hollow RuCuMo nanoparticles were prepared by a one-pot chemical reduction method. The nanoparticles were characterized by EDX, HRTEM, XPS and ICP-AES. By combining cyclic voltammetry and TEM, the formation process of nanoparticles was obtained. The urchin-like RuCu nanoparticles are proved to be formed via underpotential deposition mechanism and the formation of ternary nanoparticles RuCuMo was due to the replacement of Cu with Ru and the interception of Mo gradually. It was found that the formation of different morphology is depended on the precursors in the reaction system and their reduction sequences. Compared to previously reported multi-step synthetic routes, the developed method here is much simpler.
Understanding of the formation process of NPs is necessary for the design of catalyst with targeted properties.22 Zhu et al. have reported the synthesis of PtNi nanocrystals by tracing the Ni contents in particles with TEM and EDX at different reaction stages.24 Polte and his co-workers have presented the formation mechanism of gold NPs with the help of in situ small-angle X-ray scattering and X-ray absorption near-edge spectroscopy.25 However, it still remains challenging to figure out the time-dependent characterization of the formation process of those NPs.
Herein, a facile and effective approach was introduced to synthesize urchin-like RuCu NPs and hollow RuCuMo NPs. The products were characterized by TEM, HRTEM, XPS and ICP-AES and the formation process was monitored by measuring the cyclic voltammetric behaviors.
:
Cu atomic ratio of about 0.69
:
0.31. This atomic ratio was higher than the Ru/Cu stoichiometric ratio in the reaction system (Ru(acac)3/Cu(acac)2 (1
:
1)), which could be caused by the dissolution of un-alloyed Cu during washing step. The signal of Ni in Fig. S2b (ESI†) was originated from the nickel grid used in the measurement. The HRTEM images of RuCu NPs shows some similar urchin-like picture. The SAED image shows well crystallinity and the polycrystal structure (Fig. S3, ESI†).
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| Fig. 1 (a) TEM and (b) HAADF-STEM images of urchin-like RuCu (the inset in (b) is a schematic illustration of urchin-like RuCu); (c) EDX elemental mapping images. | ||
The XRD pattern of the RuCu NPs was shown in Fig. S4 (ESI†). By comparing the XRD pattern of pure Ru standard card (JCPDS card no 06-0663), we found that the diffraction peaks of the prepared nanoparticles were all right-shifted, which were supposed to be caused by the addition of Cu in Ru crystal lattice, which changed the inter-planar spacing. The characteristic peaks of RuCu were between the two single metal peaks, indicating that the obtained material was RuCu alloy. The diffraction peaks of RuO2 (110) (2θ = 28.0°) (JCPDS card no 43-1027) appeared in Fig. S4 (ESI†) suggest the presence of Ru oxidation state (RuO2).
The compositions of RuCu sample were studied using XPS. The spectrum was separated into two peaks (Fig. 2a). The peak at ∼932.2 eV is attributed to Cu0, while that at ∼935.4 eV corresponds to Cu2+ in RuCu NPs. The content of 21.7% Cu2+ in RuCu NPs was based on the peak area. The same protocol was applied to Ru 3p3/2 spectrum (Fig. 2b). The peak at ∼462.6 eV was attributed to Ru0 and that at ∼464.6 eV was assigned to Ru4+ (RuO2),26 which is assistent with XRD result. 26.9% of Ru4+ remained in the RuCu NPs.
In the control experiment using only Ru precursor in the synthesis, 7 nm Ru particles with uncontrollable shape are obtained (Fig. S5, ESI†), while using only Cu precursor, even no particles were found. However, in the case of coexisted precursors of Ru and Cu in the synthesis, the urchin-like RuCu NPs were achieved. This suggested that coexistence of Ru and Cu was essential for the synthesis of urchin-like particle.
To study the formation process of NPs, cyclic voltammetry (CV) measurement was employed. CV curves corresponding to 50 min, 1 h, 1.5 h, and 2 h respectively were showed in Fig. 3. The typical CV curves of ruthenium, copper, molybdenum NPs, RuCu and CuMo bimetallic NPs were obtained and displayed in Fig. S6 (ESI†). The CV curve at 50 min is consistent with that of Ru NPs (Fig. S6b, ESI†) and the CV curve at 2 h is agreement with that of RuCu NPs (Fig. S6d, ESI†), suggesting that Ru3+ is reduced prior to Cu2+ during the reaction. Theoretically, the standard redox potential of Ru3+/Ru0 and Cu2+/Cu0 is 0.68 V and 0.34 V respectively, so the reduction of Ru species should be easier than Cu species.27
Based on the results above, we postulated the formation process of RuCu NPs (Fig. 4). At the initial stage, Ru3+ and Cu2+ are reduced by benzyl alcohol but Ru atoms tend to be reduced in a faster rate than Cu and nucleate, grow first. At the second stage, by way of underpotential deposition effect,28 the produced Cu atoms are deposit on the formed Ru particles and form RuCu nuclei. At the third stage, Ru atoms grow in one direction on RuCu nuclei, which follows the process reported by Yoon etc. that Ru atoms tend to form hexagonal close-packed (hcp) structure29 and facilitate the orientation growth. Therefore, with the formation of Ru0 and deposition of Cu0, the urchin-like RuCu NPs are formed.
The inexpensive Mo has been reported as co-catalyst to increase NPs' activity.30 In order to form a NPs with the tertiary members, Na2MoO4 was added in the substrate. In the synthesis, we surprisingly found the formation of RuCuMo NPs (Fig. 5). In general, the hollow structure is formed by multiple steps, involving the construction of nanoparticle template, element growing on the surface of the template and the removing of the template. But the complexity and difficulty in the synthesis of this interesting material limited their utility in the practical application.31,32 In this work, the hollow nanostructure was obtained by just one-step reduction process and the results were displayed in Fig. 5. Fig. 5c shows the distribution of Ru, Cu and Mo atoms, which confirms the formation of alloyed RuCuMo structure. The HRTEM images of RuCuMo NPs (Fig. S7a, ESI†) displayed the hollow structure and the SAED image also showed the polycrystal structure (Fig. S7b, ESI†). The diameter of the particles can be found in Fig. 5a to be ranged from 17 nm to 32 nm (Fig. 5d). The EDX line scanning analysis of a single particle suggests that Cu and Mo species are mostly concentrated on the shell (Fig. S8, ESI†). The signal difference between the edge and center gives another convincing evidence of the structure with hollow interior.33,34 ICP-AES analysis showed that the atomic ratio of Ru
:
Cu
:
Mo is 0.75
:
0.20
:
0.05. It can be found that Mo made up a very small proportion in the produced nano particles. This should be caused by the slow reduction rate of Mo species due to the relatively low redox potential of MoO42−/Mo (−1.05 V vs. SHE), which result in a low content of Mo in the final product.
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| Fig. 5 (a) TEM and (b) HAADF-STEM images of hollow RuCuMo nanoparticles; (c) EDX elemental mapping images; (d) size distribution of hollow RuCuMo nanoparticles in (a). | ||
For the XRD pattern of RuCuMo NPs in Fig. S9 (ESI†), the three peaks were identified as the RuCuMo alloy, but shifted slightly to higher angles compared with the Ru metal standard (JCPDS no 06-0663). This peak shift is possibly resulted from the change in lattice parameters. Replacing the Ru position with Cu and Mo atoms will reduce the unit cell volume,35,36 resulting in a lattice parameters reduction. There was no standard JCPDS file can be referred to for the RuCuMo alloy. However, based on the XRD pattern obtained, we believe that the of RuCuMo alloy was formed due to the three characteristic peaks of the synthesized product were all among the three single metal characteristic peaks. The diffraction peaks of RuO2 (110) (2θ = 28.0°) (JCPDS card no 43-1027) appeared once again, suggesting the presence of Ru oxidation state (RuO2).
The NPs can be achieved in 10 min in ternary system, however, it takes 50 min to form NPs in binary system. It suggests that the reduction of the metal precursors can be promoted by the addition of Na2MoO4. PVP has been reported to be used as the capping agent and weaker reducer in the published works, we found in this work that the addition of PVP in the reaction system could prevent the formed particles from being aggregated (Fig. S10, ESI†), which may be due to the capping and reducing activity as reported.37,38
The XPS analysis displayed the bonding state of the metal atoms in RuCuMo NPs. The peaks at ∼233.1 eV and ∼236.2 eV could be assigned to Mo6+ state (Fig. 6a), which suggests the oxidation effect (Mo to MoO3) on the surface.39 Such oxidation of nanosized metals is normal.40 Fig. 6b shows 36.1% Cu2+ in RuCuMo NPs. The Ru4+ ratio of RuCuMo NPs was declined to 21.1% from 26.9% of RuCu NPs. It is indicated that, compared with binary RuCu NPs, ternary RuCuMo NPs is more stable. The result indicates the combination of Ru and the modified non-noble transition metals improves the stability due to the electron interaction of the elements.41
To understand the formation process of the ternary RuCuMo NPs, CV analysis was performed, as well as the analysis of electrode potential of Ru3+/Ru, Cu2+/Cu and MoO42−/Mo (Fig. 6d and e). The standard redox potential of Ru3+/Ru0, Cu2+/Cu0 and MoO42−/Mo is 0.68 V, 0.34 V and −1.05 V, respectively,8,42 therefore, Ru ion is more easily reduced than the other two metal ions. However, according to Fig. 6d and S6 (ESI†), the CV curve at 10 min is consistent with that of Cu NPs, then the CV curve at the 20 min agrees with RuCu NPs, which suggests the Cu nuclei is obtained at the initial stage, and then Ru3+ is reduced. In addition, the analysis of the electrode potential (
) (Fig. 6e) shows that
of Ru3+/Ru0 don't be changed (
= 0.68 V) and
of Cu2+/Cu0 is increased to 0.59 V from original 0.34 V, which also suggests that the reduction of Cu2+ in this system could be easier. The reduction of MoO42–/Mo was not seen in the process (Fig. 6e and S11c, ESI†), which suggests that it is difficult to get reduced in this system due to its redox potential. Therefore, the reduction of the ions is in the order of Cu2+, Ru3+ and then MoO42−.
In order to further gain insight into the morphological evolution of RuCuMo NPs, typical TEM analysis of the samples at 10 min, 50 min, 2 h and 8 h respectively was performed (Fig. 7). At the initial stage, the NPs with the size of 3–10 nm are obtained at 10 min (Fig. 7a). The hollow particles were formed at 50 min (Fig. 7b) and the hollow structure with size of ∼23 nm were built at 8 h (Fig. 7d). Then the shape and size of the final products did not change with the reaction time.
Based on the discussion above, the formation mechanism of RuCuMo NPs is proposed in Fig. 7e. At the first stage, Cu and Ru precursors are reduced by C6H5CH2OH. Due to the combination of Ru3+ and MoO42− at early stage, Cu2+ is reduced mainly in the initial phase. At the second stage, Ru atoms are preferentially positioned on the outer part of the formed Cu@Ru nano-nuclei because Ru atom is bigger in size than Cu atom. The reduction process is always accompanied with the diffusion process,43 so the small proportion of Mo atoms are spread in the inner part of the hollow Cu@Ru particle and be intercepted among Cu and Ru atoms. At the third stage, Cu atoms are in situ oxidized by Ru3+ (Cu (s) + 2Ru3+ → 3Cu2+ + Ru (s)) due to the galvanic replacement reaction.44 Finally, the oxidized Cu atoms are removed from the solid NPs by dissolution into the solvent and the pits are filled with Ru atoms. The removal of Cu atoms makes the particle hollow inside.
Footnote |
| † Electronic supplementary information (ESI) available: Size distribution, EDX, CV curves. See DOI: 10.1039/c8ra01261j |
| This journal is © The Royal Society of Chemistry 2018 |