In Fig. 1A, the composite electrode exhibited a monolithic structure with coarse surface morphology, many Si/SiOx particles were exposed onto the electrode surface, and several cracks were caused by the volume contraction of the PAN’s cyclization. These specific structural properties might guarantee the infiltration of the electrolyte into the bulk electrode, which was beneficial for charge transfer and ion transport. In Fig. 1B, the Raman spectra showed a sharp band at 502 cm−1 which was attributed to the crystalline Si, indicating that nano-Si were dispersed into silicon oxides matrices, another two bands at 1356 and 1592 cm−1 were attributed to the D-band (disorder-induced phonon mode) and G-band (graphite band), respectively, of delocalized sp2 π bonds in nitrogen doped carbon. In Fig. 1C, the composite electrode showed a weak reduction peak at 0.52 V, which indicated that the capacity loss results from the formation of SEI, and that the reduction of SiO to Si could be negligible in the composite electrode. This was due to the existence of cyclized PAN layer coating on active materials that hindered the decomposition of the electrolyte, as well as the mechanochemical reduction of SiO to nano-Si oxides could reduce the formation of Li2O and Li-silicates. Fig. 1D showed the charge–discharge profiles of the composite electrode at the current density of 0.1 A g−1. It delivered a high initial discharge capacity of 2733.7 mA h g−1 and a charge capacity of 2046.6 mA h g−1, with 75% coulombic efficiency. The second discharge capacity could maintain at 2051.2 mA h g−1. After 100 cycles (Fig. 1E), the composite electrode revealed a high capacity retention of 987.8 mA h g−1, with an average coulombic efficiency of 98.5% for 100 cycles. Note that the cycle performance of the composite electrode was much better than that of the pristine SiO electrode.
In summary, a binder-free anode of cyclized-PAN coating Si/SiOxcomposite was designed, and it exhibited excellent electrochemical properties in lithium ion batteries. This unique structural design would provide new avenues for the rational engineering of electrode materials for advanced lithium ion batteries and other electrochemical devices.
References
1 J.-I. Lee and S. Park, Nano Energy, 2013, 2, 146−152.
2 J. Wang, W. Bao, L. Ma, G. Tan, Y. Su, S. Chen, F. Wu, J. Lu and K. Amine, ChemSusChem, 2015, 8, 4073−4080.
3 N. Liu, Z. Lu, J. Zhao, M. T. McDowell, H.-W. Lee, W. Zhao and Y. Cui, Nat. Nanotechnol., 2014, 9, 187–192.
Fig. 1 (A) SEM image, (B) Raman spectrum, (C) Cyclic voltammograms, and (D) Charge–discharge profiles of the composite electrode, and (E) Cycle performance of the pristine SiO electrode and composite electrode at a current density of 0.1 A g−1.