2020
DOI: 10.1016/j.mtcomm.2020.101589
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Facile preparation of nitrogen-doped yolk-shell Si@void@C/CNTs microspheres as high-performance anode in lithium-ion batteries

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Cited by 10 publications
(7 citation statements)
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“…These resistances included Ohmic series resistance ( R s ), SEI resistance ( R SEI ), and charge-transfer resistance ( R ct ), , and the values of the equivalent circuit resistances were calculated and are given in Table S2. It can be found that the slope of optimized PSi/SCNT-SRGO is much larger than that of PSi, exhibiting a significant decrease in the charge-transfer resistance and an increase in the lithium-diffusion coefficient. , Furthermore, the lithium-diffusion coefficient of optimized PSi/SCNT-SRGO is about 6.82 × 10 –16 cm 2 s –1 based on the plots of Z ′ vs ω –1/2 (Figure S15b) according to eqs S1 and S2, , which is increased by about 126% for PSi (3.02 × 10 –16 cm 2 s –1 ). This is attributed to the improved electrical conductivity and enhanced reversible reaction owing to the in situ formed steady weave cage-like SCNT-SRO nanostructure.…”
Section: Resultsmentioning
confidence: 95%
“…These resistances included Ohmic series resistance ( R s ), SEI resistance ( R SEI ), and charge-transfer resistance ( R ct ), , and the values of the equivalent circuit resistances were calculated and are given in Table S2. It can be found that the slope of optimized PSi/SCNT-SRGO is much larger than that of PSi, exhibiting a significant decrease in the charge-transfer resistance and an increase in the lithium-diffusion coefficient. , Furthermore, the lithium-diffusion coefficient of optimized PSi/SCNT-SRGO is about 6.82 × 10 –16 cm 2 s –1 based on the plots of Z ′ vs ω –1/2 (Figure S15b) according to eqs S1 and S2, , which is increased by about 126% for PSi (3.02 × 10 –16 cm 2 s –1 ). This is attributed to the improved electrical conductivity and enhanced reversible reaction owing to the in situ formed steady weave cage-like SCNT-SRO nanostructure.…”
Section: Resultsmentioning
confidence: 95%
“…The flat surface with no obvious cracks is attributed to the formation of a stable SEI film, which serves as a protective layer for good cycling stability. 59,60 In addition, we also carry out a TEM test on ES-Si/rGO after 200 cycles (Figure 7e−i). After 200 cycles, the sample still maintains a pomegranate-like structure, and there is no significant change before and after cycles.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…This measurement confirms that the compact pomegranate-like ES-Si/rGO could mitigate the effect of volume expansion and preserve its good electrochemical activity during the long cycling period. The flat surface with no obvious cracks is attributed to the formation of a stable SEI film, which serves as a protective layer for good cycling stability. , In addition, we also carry out a TEM test on ES-Si/rGO after 200 cycles (Figure e–i). After 200 cycles, the sample still maintains a pomegranate-like structure, and there is no significant change before and after cycles.…”
Section: Resultsmentioning
confidence: 99%
“…This above result is consistent with the EIS data (Figure S8), indicating that PSi@CNS markedly reduced charge-transfer resistance and enhanced charge-transfer kinetics owing to the in situ generated CNS with a mesoporous structure. Furthermore, the lithium diffusion coefficient can be calculated from the plots of Z ′ versus ω –1/2 (Figure S9) based on the EIS test according to eqs S1 and S2. , Therefore, the lithium diffusion coefficient of PSi@CNS is about 3.25 × 10 –16 cm 2 /s, which is increased by nearly 10 percent compared to that of PSi (2.96 × 10 –16 cm 2 /s) and is much higher than that of PSi@SiO 2 /CNS (6.22 × 10 –17 cm 2 /s). As seen from Figure d, it is highlighted that a high reversible capacity of 1272 mA h g –1 after 500 cycles (Table ) can be obtained with a high Coulombic efficiency of 99.2% (Figure d), which is better than the most existed micron-sized PSi/C composites.…”
Section: Resultsmentioning
confidence: 99%