Facile synthesis and application of multi-shelled SnO2 hollow spheres in lithium ion battery

Guanglei Wu*a, Hongjing Wub, Kuikui Wanga, Chenhui Zhengb, Yiqun Wangb and Ailing Feng*c
aInstitute of Materials for Energy and Environment, Growing Base for State Key Laboratory, College of Materials Science and Engineering, Qingdao University, Qingdao, 266071, P. R. China. E-mail: wuguanglei@mail.xjtu.edu.cn
bDepartment of Applied Physics, School of Science, Northwestern Polytechnical University, Xi'an, 710072, P. R. China
cInstitute of Physics & Optoelectronics Technology, Baoji University of Arts and Sciences, Baoji 721016, P. R. China. E-mail: ailing@mail.xjtu.edu.cn

Received 6th May 2016 , Accepted 10th June 2016

First published on 13th June 2016


Abstract

A simple template-free hydrothermal method has been developed to prepare multi-shelled SnO2 hollow spheres with controlled interior texture. The interior texture and size of the multi-shelled SnO2 hollow spheres were found to be strongly dependent on the carbon source, Sn salt precursor and molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M. The multi-shelled SnO2 hollow spheres exhibit good electrochemical performance as the anode material in lithium ion batteries.


Introduction

Wide-band gap semiconducting tin oxide (SnO2) is a functional material of great interest. It should be emphasized that the performance of SnO2 in some applications may actually benefit from a properly designed SnO2 micro-/nanostructure.1,2 Recently, hollow structures have attracted considerable attention because of their improvable performance, such as large specific surface area, complicated inner cavity, and high structural stability. More and more synthetic methods have been reported to prepare SnO2 hollow structures, including Ostwald ripening, differential diffusion (i.e., kirkendall effect), removable templates, and chemically induced self-assembly.3 Usually, only single-shelled hollow spheres are obtained by the above-mentioned approaches.

It will be intellectually stimulating and technologically important to determine whether a high-order design (e.g., hollow core–shell particles) of the micro-/nanostructure could lead to functional improvements, while depending on a relatively simple and scalable preparation method. Template-assisted synthesis is currently the most common preparation method of complicated hollow micro-/nanostructures. Recently, Wang and co-workers4–11 have successfully prepared the multiple-shell metal oxide hollow microspheres by using carbonaceous microsphere as a template. Lou and co-workers12 have developed a new “penetration-solidification-annealing” strategy to realize the general synthesis of various mixed metal oxide multi-shelled hollow spheres. Zhang et al. have constructed multi-shelled ZnO core–shell structures via a simple hard template strategy.13 However, template-assisted synthesis is not without problems: product deconstruction during the template removal process, the shortage of templates for generating complicated hollow structures, and multistep and costly operations.

By comparison, hydrothermal synthesis has remarkable advantages such as simple operations, low-cost, and scalable production. In the present contribution, we report a simple approach for preparation of nanocrystalline SnO2 hollow spheres with a controlled number of shells by chemically induced self-assembly in the hydrothermal environment.14–16 To form the multi-shelled SnO2 nanostructure, we add metal salts directly to the carbonhydrate solutions in water, followed by a hydrothermal treatment. Upon calcination, hollow spheres of SnO2 were obtained. To evaluate the electrochemical characteristics of this material, we tested the multi-shelled SnO2 hollow spheres as lithium storage anodes for secondary Li batteries.

Experimental

Materials

The reagents including D-glucose, source, Na2SnO3·3H2O, SnCl4·5H2O, and SnCl2·2H2O were all analytical grade in purity, and bought from Sinopharm Chemical Reagent Co., Ltd. Ultrapure water (Millipore Milli-Q grade) with a resistivity of 18.2 MΩ was used in all the experiments.

Synthesis of single-shelled SnO2 hollow spheres

In a typical experiment, 0.01 mol D-glucose and 0.02 mol Sn salt (i.e., Na2SnO3·3H2O and SnCl2·2H2O) were dissolved in 50 ml ultrapure water. Then, the solution was homogenized by vigorous stirring. After stirring for 30 min, the resultant mixture was transferred to a 100 ml Teflon-lined autoclave followed by hydrothermal treatment at 180 °C for 20 h. The obtained products were washed and filtered off several times using ultrapure water and ethanol successively, and finally dried in a vacuum oven at 80 °C for 12 h. After synthesis, the products were subjected to annealing at 550 °C for 3 h in air with a heating rate of 2 °C min−1 from room temperature to obtain single-shelled SnO2 hollow spheres.

Synthesis of multi-shelled SnO2 hollow spheres

In a typical experiment, 0.0125 mol sucrose and 0.0125 mol Sn salt (i.e., SnCl4·5H2O) were dissolved in 50 ml ultrapure water. Alternatively, 0.02 mol D-glucose and 0.01 mol Sn salt (i.e., SnCl4·5H2O) were dissolved in 50 ml ultrapure water. Then, the solution was homogenized by vigorous stirring. After stirring for 30 min, the resultant mixture was transferred to a 100 ml Teflon-lined autoclave followed by hydrothermal treatment at 180 °C for 20 h. The obtained products were washed and filtered off several times using ultrapure water and ethanol successively, and finally dried in a vacuum oven at 80 °C for 12 h. After synthesis, the products were subjected to annealing at 500, 600 and 700 °C for 3 h in air with a heating rate of 2 °C min−1 from room temperature to obtain multi-shelled SnO2 hollow spheres with controlled interior structures.

Characterization

The morphologies and structures of the as-prepared samples were visualized by using a FEI Quanta 600 FEG scanning electron microscope (SEM) and a FEI Tecnai G2 F20 S-TWIN transmission electron microscope (TEM).

For evaluating the electrochemical performance of the materials, a mixture of 70 wt% SnO2, 20 wt% acetylene black (AB) and 10 wt% polyvinylidene fluoride (PVDF) in N-methylpyrrolidone (NMP) solvent was taken as the slurry for casting. The slurry was cast on the Cu foil followed by drying at 80 °C in a vacuum oven for 12 h. The electrochemical properties of the electrodes were measured by assembling them into coin cells (CR 2023) in an argon-filled glove box. Lithium foil was used as a counter electrode and a polypropylene (PP) film as the separator. The electrolyte was made from 1 M LiPF6 in ethylene carbonate (EC) and diethyl carbonate (DEC) (1[thin space (1/6-em)]:[thin space (1/6-em)]1 by volume). The charging/discharging behavior of all the cells was galvanostatically cycled between 3 and 0.01 V. Capacity retention tests of the assembled cells were carried out for the required rates.

Results and discussion

Characterization of multi-shelled SnO2 hollow spheres

The morphology and size of the SnO2 hollow micro-/nanostructures were found to be strongly dependent on the Sn salt precursor. From the field-emission scanning electron microscopy (FESEM) image (Fig. 1a–d), it is apparent that the SnO2 products prepared by using Na2SnO3 and SnCl2 precursors consist of interconnected spherical hollow particles with a diameter in the range of 1–2 μm and shell thickness of about 100–200 nm. It was found that the salt precursor has a dramatic effect on both morphology and size of the product in present hydrothermal synthesis. For example, when the salt precursor was SnCl4, the product consisted of irregular nanoparticles with a size in the range of 1–2 μm (Fig. 1e and f).
image file: c6ra11771f-f1.tif
Fig. 1 FESEM images of SnO2 samples after hydrothermal reaction at 180 °C with 1[thin space (1/6-em)]:[thin space (1/6-em)]2 molar ratio of D-glucose and metal salt. (a and b) Na2SnO3·3H2O, (c and d) SnCl2·2H2O and (e and f) SnCl4·5H2O.

SnO2 spheres are not solid ball but hollow sphere structures, as evidenced by the FESEM images of the products calcined at 550 °C in Fig. 2a–d. Observation on the surface of the product prepared by using SnCl4 precursor, it is found that the calcined SnO2 powder is made up from nano-sized small particles (Fig. 2e and f).


image file: c6ra11771f-f2.tif
Fig. 2 FESEM images of SnO2 samples after calcination at 550 °C for 3 h with 1[thin space (1/6-em)]:[thin space (1/6-em)]2 molar ratio of D-glucose and metal salt. (a and b) Na2SnO3·3H2O, (c and d) SnCl2·2H2O and (e and f) SnCl4·5H2O.

Fig. 3a–f are FESEM images of the SnO2 products with different proportions (i.e., molar ratio of 1[thin space (1/6-em)]:[thin space (1/6-em)]0.4) of D-glucose (G) and Sn salt precursor (M) after calcination. It is found that only solid SnO2 spheres exist in the final products, as the rate of hydrolysis of Sn ion is not as fast as that of carbonization of D-glucose, and thus the produced SnO2 nanoparticle-loaded carbon spheres are formed.17 All-solid spheres of SnO2 nanoparticle aggregates are attributed to the uniformity of dispersion of SnO2 nanoparticles in the carbon spheres. The irregular morphology of the SnO2 nanoparticle aggregates (Fig. 3e and f) actually attested to the presence of a large number of SnO2 nanoparticles surrounded by the amorphous carbon.


image file: c6ra11771f-f3.tif
Fig. 3 FESEM images of SnO2 samples after calcination at 550 °C for 3 h with 1[thin space (1/6-em)]:[thin space (1/6-em)]0.4 molar ratio of D-glucose and metal salt. (a and b) Na2SnO3·3H2O, (c and d) SnCl2·2H2O and (e and f) SnCl4·5H2O.

The high-magnification transmission electron microscopy (TEM) image in Fig. 4a shows hollow spheres, which has visibly hollow interiors and a coarse surface. TEM image of the surface morphology of SnO2 spheres is shown as Fig. 4b, from which it can be clearly distinguished that the relatively large mesospheres comprises aggregates of fine particles with sizes of ca. 20 nm. The lattice fringe can be easily observed, and the lattice spacing (0.33 nm) agrees with SnO2 (110) plane spacing from Fig. 4b.


image file: c6ra11771f-f4.tif
Fig. 4 (a) TEM (b) HRTEM images of SnO2 samples after calcination at 550 °C for 3 h with 1[thin space (1/6-em)]:[thin space (1/6-em)]2 molar ratio of D-glucose and SnCl2·2H2O.

The interior texture and size of the multi-shelled SnO2 hollow spheres were found to be strongly dependent on the carbon source, Sn salt precursor and molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M. Fig. 5a, b, e and f show the FESEM images of the SnO2 hollow spheres prepared by using SnCl4 and SnCl2 as the Sn salt precursors, sucrose as carbon source. The Sn source has important influence on the texture of the SnO2 core–shell nanostructures. The morphology of the multi-shelled SnO2 hollow spheres prepared by using SnCl4 as the Sn source is revealed by FESEM observation (Fig. 5a and b). However, only single-shelled SnO2 hollow spheres could be obtained by using SnCl2 as the Sn salt source (Fig. 5e and f). Magnified SEM images show that the shell is formed by aggregation of small SnO2 nanocrystals.


image file: c6ra11771f-f5.tif
Fig. 5 FESEM and TEM images of SnO2 samples after calcination at 600 °C for 3 h with 1[thin space (1/6-em)]:[thin space (1/6-em)]1 molar ratio of sucrose and metal salt. (a–d) SnCl4·5H2O and (e–g) SnCl2·2H2O.

In order to further elucidate the effect of molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M on the morphology of SnO2 hollow spheres, the SnO2 products using SnCl4 as Sn salt source, D-glucose as carbon source were characterized by FESEM with different molar ratios of G[thin space (1/6-em)]:[thin space (1/6-em)]M (i.e., 2[thin space (1/6-em)]:[thin space (1/6-em)]1 and 1[thin space (1/6-em)]:[thin space (1/6-em)]2, respectively). Fig. 6a–d shows the different morphologies of the SnO2 hollow spheres prepared with different molar ratios of G[thin space (1/6-em)]:[thin space (1/6-em)]M. It is seen that the molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M has important influence on both the size and the morphology of the resulting SnO2 products. The size of the SnO2 products decreases with molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M decrease of the system, which could be easily controlled. On the basis of the morphology analysis results of the SnO2 products, it is concluded that the SnO2 products with a large size favor the formation of multi-shelled SnO2 hollow spheres. We believed that the SnO2 products with large size could be divided into more regions for the storage of stable Sn species, leading to the formation of shells and solid cores. However, the SnO2 products prepared with lower molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M could only give rise to relatively small solid SnO2 particles. Therefore, the molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M in the D-glucose-SnCl4 solution system determines the structure and morphology of the final SnO2 products.


image file: c6ra11771f-f6.tif
Fig. 6 FESEM and TEM images of SnO2 samples after calcination at 600 °C for 3 h with (a and b, e) 2[thin space (1/6-em)]:[thin space (1/6-em)]1 and (c and d, f) 1[thin space (1/6-em)]:[thin space (1/6-em)]2 molar ratio of D-glucose and SnCl4·5H2O.

Fig. 5c, d, g and 6e and f shows the different morphologies of the as-synthesized SnO2 micro-/nanostructures. As can be seen from the TEM images in the Fig. 5c and 6e, SnO2 products show similar multi-shelled hollow spheres with hierarchical structures. The outer-shell diameters of these spherical particles are all in the range of 1–2 μm, and the inner spheres have a diameter of 0.5 μm. The TEM images in the Fig. 6e clearly show smaller dark circles inside the hollow spheres, suggesting that the inner SnO2 spheres still have a hollow structure. Being heat-treated at 600 °C for removal of residual carbon, some multi-shelled SnO2 hollow spheres had an open hole on their outer shells (Fig. 5 and 6).

The TEM images shown in Fig. 7a and b demonstrate the number of SnO2 multi-shells increases with temperature, reaching a maximum of 4 multi-shells at 700 °C. Fig. 7a shows that when as-synthesized SnO2 micro-/nanostructures are heated to 700 °C the inner carbonaceous template gradually separates from the newly formed outer SnO2 shell, leading to the formation of quadruple-shelled SnO2 hollow spheres. When the calcination temperature is decreased to 500 °C (Fig. 7b), only double shells with a thin thickness are formed in the SnO2 samples. As mentioned above, it is expected that the unique multi-shelled structures and increased porosity of the shells could lead to an increase in the electrolyte/SnO2 contact area, a decrease in the effective diffusion distance for both lithium ion and electrons, and thus better rate capabilities.18 Second, the void space effectively accommodates the dramatic volume change and alleviates the strain during Li+-insertion/extraction processes.19


image file: c6ra11771f-f7.tif
Fig. 7 TEM images of SnO2 samples after calcination at (a) 700 and (b) 500 °C with 1[thin space (1/6-em)]:[thin space (1/6-em)]1 molar ratio of sucrose and SnCl4·5H2O.

Electrochemical properties

Recently, SnO2 has been a research highlight as a next-generation of anodic material for lithium ion batteries because of its high theoretical specific capacity (∼790 mA h g−1). However, it is well known that the main hindrance against practical use of Sn based anode materials in lithium ion batteries is the large volume change during charging–discharging processes which leads to poor cycleability. One possible approach to improve SnO2 electrochemical performance is to design hollow nanomaterials so as to mitigate the pulverization problem and further enhance structural stability. Inspired by this idea, hollow SnO2 can provide sufficient space to buffer the volume change during the charging–discharging process and therefore are suggested a cycleable anodic material for lithium ion batteries. The charge–discharge curves of multi-shelled SnO2 hollow sphere electrodes for the first and the 5th, 10th, 50th and 100th cycle at constant current density of 100 mA g−1 are shown in Fig. 8a. The initial discharge and charge capacities are found to be 861 and 422 mA h g−1, respectively. The irreversible capacity loss of 51% can be mainly attributed to the possible irreversible processes, such as electrolyte decomposition and inevitable formation of an SEI layer.20 Reversible capacities of 864, 704, 272 and 214 mA h g−1 were achieved in the 5th, 10th, 50th and 100th cycle at current density of 100 mA g−1. Fig. 8b shows the cycling performance of the multi-shelled SnO2 hollow sphere electrode. The charge–discharge capacity of this material remains 214 mA h g−1 after 100 cycles, exhibiting a good capacity retention. As the rate capability is also critical for practical applications, we measured charge–discharge curves at different densities for the multi-shelled SnO2 hollow spheres (Fig. 8c). As can be seen, the average specific capacities of multi-shelled SnO2 hollow spheres are ∼410, 358, 298, 202 and 112 mA h g−1 at the current densities of 100, 200, 500, 1000 and 2000 mA g−1, respectively. After the high-rate charge–discharge cycling, a specific capacity as high as ∼319 mA h g−1 can be restored when the current density is reduced to 100 mA g−1. The above results clearly imply that multi-shelled SnO2 hollow spheres are relatively tolerant of various charge–discharge currents, which is preferred for high power applications.
image file: c6ra11771f-f8.tif
Fig. 8 (a) Charge–discharge curves of the multi-shelled SnO2 hollow sphere electrode for the 1st, 5th, 10th, 50th, and 100th cycle at current density of 100 mA g−1; (b) the cycling performance of the multi-shelled SnO2 hollow spheres; (c) charge–discharge curves of the multi-shelled SnO2 hollow spheres at different current densities.

Conclusions

In summary, multi-shelled SnO2 hollow spheres have been successfully prepared through a simple template-free hydrothermal route. The carbon source, Sn salt precursor and molar ratio of G[thin space (1/6-em)]:[thin space (1/6-em)]M play important roles in control of the interior texture of the SnO2 hollow microspheres. The multi-shelled SnO2 hollow sphere electrodes exhibit good electrochemical performance as an anode material in lithium ion batteries. The successful synthesis of the multi-shelled SnO2 hollow nanostructures opens new opportunity for exploitation of metal oxide nanostructures as high-performance anode material for lithium ion batteries.

Acknowledgements

Financial support was provided by National Natural Science Foundation of China (No. 50771082, 51571166, 61505167 and 60776822) and Natural Science Basic Research Plan in Shaanxi Province of China (No. 2015JM5215), Key Project of Baoji University of Arts and Sciences (No. ZK16072), Baoji Engineering Technology Research Center for Ultrafast Optics and New Materials (No. 2015CXNL-1-3). G. Wu thanks the National Natural Science Foundation of China (No. 51407134), China Postdoctoral Science Foundation (No. 2016M590619), and China Postdoctoral Science Special Foundation (No. 2015T81028).

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Footnote

Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra11771f

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