Jian
Li
ab,
Shuyan
Song
*ab,
Yan
Long
a,
Shuang
Yao
a,
Xin
Ge
a,
Lanlan
Wu
a,
Yibo
Zhang
*a,
Xiao
Wang
a,
Xiangguang
Yang
ab and
Hongjie
Zhang
*ab
aState Key Laboratory of Rare Earth Resource Utilization, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P. R. China. E-mail: songsy@ciac.ac.cn; yibozhang@ciac.ac.cn; hongjie@ciac.ac.cn
bSchool of Applied Chemistry and Engineering, University of Science and Technology of China, Hefei 230026, Anhui, P. R. China
First published on 6th August 2018
By integrating redox self-assembly and redox etching processes, we report a general one-pot strategy for the synthesis of Au@multi-MxOy (M = Co, Ce, Fe, and Sn) yolk@shell nanospheres. Without any additional protecting molecule or reductant, the whole reaction is a clean redox process that happens among the inorganic metal salts in an alkaline aqueous solution. By using this method, Au@Co3O4/CeO2 (Au@Co–Ce), Au@Co3O4/Fe2O3 (Au@Co–Fe), and Au@CeO2/SnO2 (Au@Ce–Sn) yolk@shell nanospheres with binary oxides as shells, Au@Co3O4/CeO2/Fe2O3 (Au@Co–Ce–Fe) yolk@shell nanospheres with ternary oxides as shells and Au@Co3O4/CeO2/Fe2O3/SnO2 (Au@Co–Ce–Fe–Sn) yolk@shell nanospheres with quaternary oxides as shells can be obtained. Subsequently, the catalytic CO oxidation was selected as the catalytic model, and the Au@Co–Ce system was chosen as the catalyst. It was found that the catalytic activity of Au@Co–Ce yolk@shell nanospheres can be optimized by altering the relative proportion of Co and Ce oxides.
Recently, based on the principle of the auto-catalytic redox reaction followed by a spontaneous self-assembly process, a green strategy has been developed by our group and others to fabricate CeO2-encapsulated noble metal core@shell nanostructures.12–15 Both the core and shell are clean self-assembled together without a complicated experimental procedure, which are beneficial for the further optimization of the catalytic performance. Furthermore, binary oxide nanostructures have also been exploited by redox etching reactions between metal oxides (involving Ce, Co, Fe, Sn, and Mn elements).16–18 Herein, by integrating the redox self-assembly process and redox etching process, we report a general one-pot strategy for the synthesis of Au@multi-MxOy (M = Co, Ce, Fe, and Sn) YSNs. The composition of the shell can be continuously adjusted from two components (Co3O4/CeO2, Co3O4/Fe2O3 or CeO2/SnO2) to four components (Co3O4/CeO2/Fe2O3/SnO2) by mixing HAuCl4 with the corresponding metal salts in the presence of NH3·H2O. The relative contents of the different metal oxides in nanospheres could be tuned by precisely controlling the reaction conditions. We note that the entire preparation processes are very simple and do not use any organics, providing a clean surface for further catalytic exploitation of the well-defined MOYSNs.
In a typical experimental process, the Au@Co3O4 core@shell nanospheres were prepared by mixing HAuCl4, Co(NO3)2 and NH3·H2O for a certain time. And the detailed characterizations can be found in Fig. S2.† Furthermore, by directly adding FeCl2 or Ce(NO3)3 into the original solution of Au@Co3O4, Au@Co–Fe or Au@Co–Ce MOYSNs could be synthesized after further annealing for fine crystallization. The scanning electron microscopy (SEM) images in Fig. 1a and d reveal the uniform and monodisperse nanospheres of both samples with an average diameter of 105 nm. Furthermore, the transmission electron microscopy (TEM) images in Fig. 1b and e display the obvious yolk–shell features of both samples. It can be seen that Au nanoparticles with similar size (around 36 nm) in both samples are entirely encapsulated into the hollow shell. However, the shell in Fig. 1b is thinner than that in Fig. 1e. Because of the strong reducibility of Fe2+ and the fact that extra addition of the HCl solution into the Au@Co–Fe system can immensely accelerate the etching of Co3O4, nanospheres with a thinner shell are obtained. The energy-dispersive X-ray spectroscopy (EDX) elemental mappings (Fig. 1c and f) confirm the coexistence of two metal elements in the shells of both samples. Interestingly, Fe and Co are uniformly distributed in the whole shell in Au@Co–Fe MOYSNs (Fig. 1c). However, in Au@Co–Ce MOYSNs, Ce is present in the entire shell and Co is relatively distributed in the inner shell only. This might be caused by the direct deposition of a part of the CeO2 nanoparticles on the surface of the nanospheres in a relatively alkaline aqueous solution. However, the phenomenon cannot be observed in the Au@Co–Fe system due to the inhibition of the hydrolysis of Fe ions in a relatively acidic aqueous solution. Both of the samples were also examined by inductively coupled plasma (ICP) analysis. The average contents of Fe and Co in the Au@Co–Fe sample are 17.4 and 22.8 wt%, respectively. And the average contents of Ce and Co in the Au@Co–Ce sample are 47.4 and 19.8 wt%, respectively. The X-ray powder diffraction (XRD) pattern of the Au@Co–Ce sample is shown in Fig. S3.† All peaks can be perfectly indexed to metallic Au (JCPDS no. 04-0784), CeO2 (JCPDS no. 34-0394), and Co3O4 (JCPDS no. 42-1467). However, the XRD pattern (Fig. S4d†) of the Au@Co–Fe sample only shows the presence of metallic Au and Co–Fe binary oxides. Therefore, the Au@Co–Fe sample was further analyzed by X-ray photoelectron spectroscopy (XPS). The high-resolution XPS spectrum (Fig. S4b†) of Co shows two peaks at 781.2 and 796.7 eV, which are the characteristic peaks of Co 2p3/2, and Co 2p1/2 for Co3O4, respectively.20 In Fig. S4c,† the characteristic peaks of Fe 2p3/2 and Fe 2p1/2 for Fe2O3 are observed at the binding energies of 711.0 and 724.6 eV, respectively.21,22
Fig. 1 (a) SEM image, (b) TEM image and (c) STEM-EDX elemental maps of the Au@Co–Fe MOYSNs; (d) SEM image, (e) TEM image and (f) STEM-EDX elemental maps of the Au@Co–Ce MOYSNs. |
Similarly, such a simple strategy can also be applied to the Au@Ce–Sn system. The SEM image in Fig. 2a reveals the uniform sphere structure of the sample. However, the average diameter of the nanospheres is around 35 nm, which is obviously smaller than that of Au@Co–Fe or Au@Co–Ce samples. Furthermore, the TEM image in Fig. 2b displays the obvious presence of a void between the core and shell. The average diameter of 15 nm of the Au core in the Au@Ce–Sn system is bigger than that in the core@shell sample prepared in our previous report.14 This is because of the fact that the higher synthesis temperature of the Au@Ce–Sn system can result in a bigger Au core in the original redox assembly stage.23 Furthermore, the EDX elemental mapping in Fig. 2c confirms the uniform distribution of Ce and Sn in the whole shell. And the ICP results show that the average contents of Ce and Sn are 57.0 and 20.0 wt%, respectively. Furthermore, all peaks in the XRD pattern (Fig. 2d) can be perfectly indexed to metallic Au and CeO2. The high-resolution XPS spectrum (Fig. 2e) of Sn shows two peaks at 486.1 and 494.6 eV, which are the characteristic peaks of Sn 3d5/2 and Sn 3d3/2 for SnO2, respectively.21,22
Fig. 2 (a) SEM image, (b) TEM image, (c) STEM-EDX elemental maps and (d) XRD pattern of the Au@Ce–Sn MOYSNs. (e) High-resolution XPS for Sn 3d. |
We also attempted to fabricate YSNs containing more than two kinds of oxides in the shell by this simple method. By adding Ce(NO3)3/FeCl2 or Ce(NO3)3/FeCl2/SnCl2 solution into the original mixture solution of Au@Co3O4, Au@Co–Ce–Fe or Au@Co–Ce–Fe–Sn YSNs with multiple oxides in the shell can be obtained. The detailed information of Au@Co–Ce–Fe YSNs is shown in Fig. S5.† The SEM and TEM images (Fig. 3a and b) show that the structure and morphology of Au@Co–Ce–Fe–Sn are similar to those of Au@Co–Fe or Au@Co–Ce samples. The EDX elemental mapping (Fig. 3c) confirms the presence and distribution of Au, Co, Ce, Fe and Sn. The ICP results show that the average contents of Co, Ce, Fe and Sn in samples are 23.9, 15.66, 8.85 and 7.7 wt%, respectively. Combined with the ICP results, the diffraction peaks of the XRD pattern (Fig. 3d) are mainly indexed to Au, Co3O4 and CeO2. There are no apparent peaks of SnO2 and Fe2O3 in the XRD pattern. This might be attributed to the fact that the Fe and Sn oxides formed are highly dispersed in the interstices of the CeO2 and Co3O4 nanoparticles due to the stronger reducing ability of Fe2+ and Sn2+ ions. The high dispersity of various metal oxides can cause the mutual inhibition of crystal growth during the annealing process.24 Therefore, the sample was further analyzed by XPS. The high-resolution XPS spectrum (Fig. 3e) of Sn shows three peaks at 486, 494.5 and 715.7 eV which are the characteristic peaks of Sn 3d5/2, Sn 3d3/2 and Sn 3p3/2 for SnO2, respectively.21,22 In Fig. 3f, the characteristic peaks of Fe 2p3/2 and Fe 2p1/2 for Fe2O3 are observed at the binding energies of 710.7 and 724.3 eV, respectively.21,22
Fig. 3 (a) SEM image, (b) TEM image, (c) STEM-EDX elemental maps, and (d) XRD pattern of the Au@Co–Ce–Fe–Sn MOYSNs. High-resolution XPS for (e) Sn 3d and (f) Fe 2p and Sn 3p. |
According to previous reports, metal oxides have strong synergistic effects with noble metals to lead to excellent catalytic activity for CO oxidation.25–29 Furthermore, the strong interaction between CeO2 and Co3O4 can also result in improvement of the catalytic performance.29 It is expected that the catalytic activity of MOYSNs can be optimized by altering the relative proportion of different oxide compositions. Additionally, previous reports also show that the Cl− ion has a disadvantageous effect on catalytic CO oxidation.30 Therefore, the Au@Co–Ce system was chosen as the catalyst due to no addition of HCl solution and the controllable relative ratio of Co and Ce oxide in its synthesis process. The relative proportion of Co and Ce oxides was altered by controlling the extent of etching. Five samples (without annealing) were obtained by this method. Sample 1 is the Au@Co3O4 core@shell nanostructure without etching (Fig. S2†). The samples 2–5 are Au@Co–Ce nanospheres with different extents of etching. The contents of Co from sample 2 to sample 4 are gradually reduced (TEM image of Fig. S6† for sample 2, Fig. 1e for sample 3 and Fig. S7† for sample 4). Sample 5 was obtained through severely etching Au@Co3O4 (Fig. S8†). A massive removal of Co oxide was accomplished, and only about 2% Co remained as shown by ICP analysis. And the detailed content data of the Au, Co and Ce elements for samples 1–7 are listed in Table S1.† In their structure, samples 1 and 2 are core–shell structures and samples 3–5 are yolk@shell structures. Sample 6 is the Au–Co–Ce mixture with the same mass percent of Au, Co and Ce as in sample 4, obtained by directly mixing similar amounts of Au, bare CeO2 and Co3O4 nanoparticles together (Fig. S9†). Sample 7 is a Co–Ce mixture prepared by a co-precipitation process (Fig. S10†).
Fig. 4a shows the typical CO conversion profiles of the seven samples as a function of temperature. It can be observed that the complete CO conversion temperature for samples 1–7 is approximately 220, 180, 150, 125, 155, 280 and 320 °C, respectively. The Au content values for samples 1–6 are very close to each other; therefore, the differences in the catalytic performance caused by the Au content can be ignored. Two obvious changes can be observed from sample 1 to sample 5, which might be the direct reasons for different catalytic activities of these samples. The first is the change of structure, varying from core@shell structure (samples 1 and 2) to yolk@shell structure (samples 3–5). It is expected that the large void and penetrable shell in the yolk@shell structure enable the better contact of active sites with gas molecules, further resulting in the higher mass-transfer rates and enhanced catalytic activity.18,31 Therefore, the structural advantage for heterogeneous catalysis might be present in yolk@shell samples. The second change is the oxide component, which might be another important reason for the observed catalytic results. In comparison with single Co3O4 or CeO2 as the support for noble metals, the Co–Ce binary oxide support possesses an additional synergistic effect between Ce and Co oxides.32–34 Specifically, the synergistic effect between CeO2 and Co3O4 might greatly promote the active oxygen migration, further leading to improved catalytic activity.32–34 In our Au@Co–Ce system, accompanied by the progress of the etching reaction, the mutual dispersity between Ce and Co oxides is gradually increased from sample 2 to sample 4 (sample 1 without etching). Actually, with the progress of the etching reaction, the distribution of Ce is altered from the outermost shell (Fig. S1b† inset) to the whole shell (Fig. S1d† inset). It can be understood that compared to simple deposition on the surface, the in situ redox etching reaction can greatly promote the mutual dispersity of Co and Ce oxide. According to previous literature, the higher mutual dispersity between Ce and Co oxides can produce a stronger synergistic effect and higher catalytic activity.32–34 Therefore, the gradual enhancement of catalytic activity from sample 1 to sample 4 might be attributed to the advantage of the yolk@shell structure and gradually enhanced synergistic effect of Ce and Co oxide. The interaction of Ce and Co is relatively weak in sample 5 due to the massive removal of Co oxide, further resulting in its decreased catalytic activity. The lower catalytic activity of sample 6 than samples 1–5 can be ascribed to the weak interaction and poor dispersion of the three components. For sample 7, the lowest catalytic activity was observed. The H2-TPR of six samples was measured to investigate the interaction between noble metals and metal oxides. The redox ability of metal oxides might be reflected by the H2 temperature-programmed reduction reaction (H2-TPR). Furthermore, the synergistic effect between noble metals and metal oxides can greatly enhance the redox ability of metal oxides.33–35 Specifically, the lower reduction peak temperature in the H2-TPR curve indicates the stronger redox ability of the sample.33,34,36 It can be found in Fig. S11† that the lowest reduction peak temperature (Tlred) of the Co–Ce mixture (sample 7) is 225 °C. And the Au@Co3O4 core@shell nanostructure (sample 6) shows the Tlred at 165 °C. For the Au@Co–Ce nanostructure (samples 2–5), all of the Tlred values are below 150 °C. Therefore, the synergistic effect between noble metals and metal oxides exists in both core@shell and yolk@shell samples. Furthermore, stability is another important indicator for the evaluation of the catalyst performance. As shown in Fig. 4b, no deactivation occurs for sample 4 when the catalytic reaction is performed at 150 and 80 °C for 10 h. The TEM image (Fig. S12†) further shows that there are no obvious changes in the structure of sample 4 after a long-term catalytic reaction. All results clearly show that by altering the relative content of different oxides, the catalytic performance of the nanospheres can be optimized, and the catalyst is stable and active under long-term catalytic conditions.
Fig. 4 (a) Catalytic activity of samples 1–7 for CO oxidation. (b) Stability test of sample 4 at 150 °C and 80 °C. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8sc01520a |
This journal is © The Royal Society of Chemistry 2018 |