Controllable fabrication and magnetic properties of double-shell cobalt oxides hollow particles

Double-shell cobalt monoxide (CoO) hollow particles were successfully synthesized by a facile and effective one-pot solution-based synthetic route. The inner architecture and outer structure of the double-shell CoO hollow particles could be readily created through controlling experimental parameters. A possible formation mechanism was proposed based on the experimental results. The current synthetic strategy has good prospects for the future production of other transition-metal oxides particles with hollow interior. Furthermore, double-shell cobalt oxide (Co3O4) hollow particles could also be obtained through calcinating corresponding CoO hollow particles. The magnetic measurements revealed double-shell CoO and Co3O4 hollow particles exhibit ferromagnetic and antiferromagnetic behaviour, respectively.

chemical etching or thermal decomposition. On the other hand, the removal of the CMSs templates may result in very low yield of target product based on the ion-absorption, which is unfavorable to fulfilling the application prospects of the multiple-shell hollow spheres.
Herein, we present a one-pot solvothermal method to prepare double-shell CoO hollow particles. Interestingly, the inner and outer architecture of the double-shell CoO hollow particles can be readily tuned through controlling experimental parameters. The results demonstrate that the double-shell hollow particles might form through Ostwald ripening. By using CoO hollow particles as the precursor, double-shell Co 3 O 4 hollow particles can also be obtained via thermal decomposition process. Notably, the current synthetic strategy may provide an effective route for the synthesis of other transition-metal oxides particles, and is thus promising for achieving unique architectures with hollow interior for a wide range of applications. Figure 1a displays a representative SEM image of as-prepared product obtained using cabalt (II) acetylacetonate as cobalt source at 260uC for 8 h, in which a large quantity of near-spherical particles with good uniformity were achieved under current conditions. The particles have a mean size of about 300 nm. There exist many broken particles, which reveals that CoO particles obviously possess hollow interiors. The inset is a high-magnification SEM image obtained from a selected area of Figure 1a. Herein, the hollow interiors of as-prepared CoO particles can be clearly identified. Figure 1b presents a typical TEM image of CoO particles, which also evidently exhibits CoO particles with hollow interiors. Figure 1c indicates a typical TEM image of an individual CoO hollow particle. With careful observation, the double-shell structure of CoO hollow particle can be clearly observed. The outer and inner shell thicknesses of the double-shell CoO hollow particle are estimated to be about 8 and 100 nm, respectively. A selected area electron diffraction (SAED) pattern taken from the individual CoO hollow particles, as shown in Figure 1d, illustrates single-crystalline structure of double-shell CoO hollow particles. Figure 1e depicts the HRTEM image of the individual particle. The lattice spacing is calculated to be about 0.24 nm, agreeing well with the value of {111} lattice planes of cubic CoO. The crystal structures of as-prepared products were characterized by X-ray powder diffraction (XRD). All of the reflections of the XRD pattern, as shown in Figure 1f, can be readily indexed as a facecentered cubic phase of CoO (JCPDS 65-2902) with lattice constant a 5 0.426 nm (space group: Fm-3m (No. 225)). No impurity peak was observed, indicating the high purity of the product obtained under such conditions. The sharp diffraction peaks also reflects the good crystallinity of as-prepared product.

Results
For a better understanding of the growth process of double-shell hollow particles, the influences of reaction time on the morphologies of products have been investigated. Figure 2 summarizes a series of morphological observations supposed to be in different stages of forming double-shell hollow particles. When the reaction time was decreased to 1 h, the product is mostly made up of near-spherical  www.nature.com/scientificreports solid particles with average size of about 150 nm, as shown in Figure 2a. Figure 2b depicts a typical TEM image of product obtained for 4 h. The mean size of CoO particles is increased to about 250 nm, suggesting the elongation in size with increasing reaction time. Closer observation reveals that almost all particles possesses hollow interiors at this stage. Extending the reaction time to 12 h, the double-shell structures of the CoO hollow particles with sizes in the range 300-400 nm can be observed more clearly (Figure 2c). It is noteworthy that if the reaction time is further extended to 24 h, almost 100% double-shell CoO hollow particles with uniform sizes about 500 nm can be obtained, as shown in Figure 2d. In particular, the outer shell thickness of CoO hollow particle is increased to about 45 nm, comparable to that of CoO hollow particles obtained for 12 h.
Double-shelled Co 3 O 4 hollow particles could be also successfully obtained via calcination method using corresponding CoO hollow particles obtained at 260uC for 8 h as precursors. Figure 3a depicts the SEM image of as-prepared Co 3 O 4 obtained by calcination of corresponding CoO hollow particles at 600uC for 2 h in air. Compared with CoO hollow particles, the average size of as-prepared Co 3 O 4 is estimated to be about 400 nm, which may be related to the possible oxidation of CoO to Co 3 O 4 . An individual particles with broken shell shown in the inset of Figure 3a demonstrates the ball-inball structure of the Co 3 O 4 hollow particles. A typical TEM image of as-prepared Co 3 O 4 hollow particles is shown in Figure 3b. Herein, the Co 3 O 4 hollow particles with double-shell structure can be clearly observed. In the inset, an SAED pattern was well indexed to spinel Co 3 O 4 , revealing a polycrystalline nature of the calcined hollow particles. The double-shell structure is also clearly revealed by TEM observation of an individual Co 3 O 4 hollow particle, as shown in Figure 3c. The inset displays the corresponding HRTEM image, which provides further insight into the structure of Co 3 O 4 hollow particle. Lattice spacing is measured to be about 0.23 nm, which is consistent with the interplanar spacings of {222} for spinel Co 3 O 4 . Figure 3d shows the typical XRD pattern of double-shell Co 3 O 4 hollow particles. All the reflections in the XRD pattern can be indexed as a face-centered cubic phase of spinel Co 3 O 4 (JCPDS 43-1003) with lattice constant a 5 0.808 nm (space group: Fd-3m (No. 227)). No impurity peaks were observed, indicating that cubic CoO was completely converted into spinel Co 3 O 4 .
The evolution of double-shell structure during the calcination of as-prepared CoO particles obtained at 260uC for varied time durations as the precursor at 600uC for 2 h directly mirrors a possible scenario for the formation of double-shell Co 3 O 4 hollow particles. Figure 4 summarizes a series of morphological observations of forming double-shell Co 3 O 4 hollow particles. Figure 4a shows a typical TEM image of the porous Co 3 O 4 with hollow interior prepared by calcination of corresponding CoO particles obtained at 260uC for 2 h. With careful observation, the shells of Co 3 O 4 hollow particles were found to be composed of many pores with a mean diameter of 15 nm. It is noteworthy that if the reaction time of precursors was extended to 4 h, large interior space of Co 3 O 4 hollow particles can be generated, as shown in Figure 4b. Typical TEM image shown in Figure 4c indicates a significant increase of pore sizes in the shells. Furthermore, the interior space is also further improved. This suggests both the expansion in interior space and the addition in pore size with increasing reaction time. More interestingly, Co 3 O 4 hollow particles with apparent double-shell structure can be clearly identified using CoO hollow particles as precursors obtained at 260uC for 8 and 12 h, as shown in Figure 3 and 4d, respectively.

Discussion
To investigate the mechanism of double-shell CoO hollow particles, based on the experimental results, the possible scenario for the formation of double-shell CoO hollow particles is illustrated in Figure 5. Firstly, Co(acac) 2 dissolves in organic solvent and then undergoes thermal decomposition to form small particles under solvothermal conditions. Subsequently the fresh small particles is unstable due to the high surface energy and tends to aggregate into larger solid particles driven by the minimization of interfacial energy, which can then convert into hollow particles due to the Ostwald ripening process 39 . Finally, owing to the existence of anisotropic outer surfaces of the hollow particles, hollowing space gradually takes place at a particular region underneath the outer surface and leads to the formation of double-shelled hollow structures 40,41 .
The magnetic properties of double-shell cobalt oxides hollow particles were measured on a superconducting quantum interference device (SQUID). The temperature dependences of the zero-fieldcooled (ZFC) and field-cooled (FC) magnetization of the double-shell CoO hollow particles measured under an applied field of 100 Oe are shown in Figure 6a. It is clear that there is a significant difference between ZFC and FC curves of double-shell CoO hollow particles at low temperature. Compared with FC curve, the ZFC curve depicts a distinct peak at 4.8 K, suggesting ferromagnetic (FM) behavior below 4.8 K, which may be attributed to superparamagnetic cobalt particles 42 . Figure 6b   is possibly resulted from the finite size and surface effect of double-shell Co 3 O 4 hollow particles 43,44 . The hysteresis loops for double-shell CoO and Co 3 O 4 hollow particles at 2 K are shown in Figure 6c and d, respectively. The coercivity value H c for the CoO is about 1298 Oe at 2 K, indicating the presence of ferromagnetic ordering component. For Co 3 O 4 hollow particles, despite of that the low temperature data show a slight curvature, the magnetization curves are nearly linear at 2 K, also indicative an antiferromagnetic ground state.
Preparation of double-shell CoO hollow particles. Typical synthetic procedures are summarized as follows: 0.2571 g Co(acac) 2 (1 mmol) was dissolved into 20 mL ODE with OA and OAm (in molar ratios of 4510) to form colloid mixture under vigorous stirring for 10 min at room temperature. Then the mixture was sealed in a Teflonlined and maintained at 260uC for 1-24 h. The autoclave was cooled to room temperature. The brown products were washed for several times with absolute ethanol and hexane. Finally, the products were dried in vacuum at 60uC for 6 h.
Preparation of double-shell Co 3 O 4 hollow particles. The double-shell Co 3 O 4 hollow particles could be prepared by the thermal decomposition of as-prepared CoO hollow particles obtained at 260uC for 2-12 h as precursors calcinated at 600uC for 2 h in air.
Characterization. The structure and phase composition of the products were characterized on a X-ray diffractometer (XRD, D/max2550 VB1) with Cu Ka radiation (l 5 1.5418 Å ). The morphologies and sizes of the products were characterized by a field-emission scanning electron microscopy (FE-SEM, Sirion 200) and transmission electron microscope (TEM, Tecnai G2 F20). High-resolution TEM (HRTEM) images and SAED patterns were obtained from the TEM. Magnetic measurements were conducted using a Quantum Design MPMS XP-5 superconducting quantum interference device (SQUID).