The simple synthesis of CoP@SiO
2 was illustrated in
Fig. 1. The Co
3O
4@SiO
2 and NaH
2PO
2 were placed at both ends of the porcelain boat for calcination. As the temperature increases, the concomitant PH
3 gas released by heat decomposition of NaH
2PO
2 passed through the porous silicon shell and entered the shell together with the airflow, and reacted with Co
3O
4 to obtain CoP. When the quality ratios of Co
3O
4@SiO
2 and NaH
2PO
2 were 10 mg:100 mg, 10 mg:200 mg and 10 mg:500 mg, the obtained products were denoted as CP1, CP2 and CP3. The porous structure can offer a larger electrode-electrolyte contact area and a large number of active sites, greatly shortening the ion diffusion distance [
46]. These composite materials are generally considered to possess high porosity with excellent electrical conductivity and outstanding mechanical stability [
47,
48]. SEM and TEM characterization are used to examine the internal, external structural features and morphologies of the synthesized samples.
Fig. 2a shows the morphology of the Co
3O
4@SiO
2 sample, it is observed that precursor is a dodecahedron with smooth surface. Subsequently, the TEM image in
Fig. 2b clearly displays that the precursor is a core-shell structure. After phosphating, the surface morphology of the sample did not change much, and the shape of dodecahedron was still maintained. With the increase of the phosphating degree, the protective effect of silicon shell still works.
Figs. 2c,
e and
g show the morphology of CP1, CP2, CP3, it is clearly that the amount of NaH
2PO
2 has no significant influence on the morphology. More detailed information about the microstructure and morphology of the CP1, CP2, CP3 samples are investigated by TEM and HRTEM. As can be seen from
Figs. 2d,
f and
h, CoP core is well preserved in silicon dioxide shell, further confirming the stability and uniqueness of this core-shell structure. To observe the structural features intuitively, we have marked the CoP core. However, the CoP core is far smaller than the Co
3O
4 core at the same nanoscale. This result proves that the particle agglomeration of CoP is more serious than that of Co
3O
4. At the same time, the second function of the silicon shell was verified, that is, it effectively inhibits the large-area agglomeration of nanoparticles and ensures certain active sites, which also explained the importance of choosing Co
3O
4@SiO
2 with the core shell structure as the precursor. The HRTEM image and SAED pattern of the CP3 are respectively exhibited in Figs. S1a and b (Supporting information). The uniformly arranged lattice fringes in the
Figs. 1b correspond to the lattice planes of the CoP, whereas where the lattice fringes are not visible is due to the presence of amorphous silica. Due to the CoP is covered by the silicon shell, we found the thin silicon shell and captured the lattice fringe of the core. The structure and polycrystalline properties of spinel can be well indicated by diffraction ring in SAED patterns. Additionally, the elemental mapping pictures demonstrate the uniform distribution of Co, O, Si and P throughout the CP3 (Fig. S1c in Supporting information). From the X-ray diffraction (Fig. S2 in Supporting information) of the CP series, we can confirm that the peak of the sample tends to be flat, which is influenced by amorphous silicon shell material. Many local defects may occur in amorphous materials, which may expose more active sites and improve the activity of catalytic reactions. The XRD patterns of Co
3O
4@SiO
2 are consistent with previous reports, proving the successful synthesis of the precursor. Compared with the peak shape of Co
3O
4@SiO
2, CP series samples change significantly, but the trend of curves do not change too much, which was attributed to partial phosphating inside the core-shell structure. Fig. S3 (Supporting information) shows the diffraction peaks of CP3 samples corresponding to the CoP (JCPDS No. 29-0497) and SiO
2 (JCPDS No. 47-1144). In addition, these curves exhibit that CP1, CP2, CP3 are identical substances. The FT-IR spectra of the Co
3O
4@SiO
2, CP1, CP2, CP3 are analyzed, and the results show that the samples have the similar molecular structure except for slight differences in Co
3O
4@SiO
2. The samples display peaks around 1600 cm
-1 correspond to bending vibration of H-O-H bond, proving the existence of interstitial water in these compounds. The wide absorption at around 1100 cm
-1 is the anti-symmetric stretching vibration of Si-O-Si. (Fig. S4 in Supporting information)