2017
DOI: 10.1016/j.carbon.2016.10.032
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Insights into the effects of multi-layered graphene as buffer/interlayer for a-Si during lithiation/delithiation

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Cited by 59 publications
(103 citation statements)
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References 70 publications
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“…Another important observation is that, despite being partly cracked, the films appeared to remain intact and not delaminated even after 100 cycles, unlike observations usually made with such a-Si films upon repeated lithiation/delithiation cycles. 20,21 Overall, the present results/observations indicate in very strong terms that, even though reversible electrochemical Na-alloying is possible in a-Si, dimensional scale of the active material (when used as stand-alone) is a very important criterion with respect to the performance; with preferred dimensions being below ∼50 nm. 23 reported Na diffusivity in crystalline Si (c-Si) to be of the order of ∼ 6 × 10 −16 m 2 s −1 , even at considerably higher temperature of 800…”
Section: Resultsmentioning
confidence: 51%
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“…Another important observation is that, despite being partly cracked, the films appeared to remain intact and not delaminated even after 100 cycles, unlike observations usually made with such a-Si films upon repeated lithiation/delithiation cycles. 20,21 Overall, the present results/observations indicate in very strong terms that, even though reversible electrochemical Na-alloying is possible in a-Si, dimensional scale of the active material (when used as stand-alone) is a very important criterion with respect to the performance; with preferred dimensions being below ∼50 nm. 23 reported Na diffusivity in crystalline Si (c-Si) to be of the order of ∼ 6 × 10 −16 m 2 s −1 , even at considerably higher temperature of 800…”
Section: Resultsmentioning
confidence: 51%
“…These observations tend to support the hypothesis that the observed 'activation' for the 250 nm film was, at least partly, related to the overall Na transport limitation. In this context, it is also believed that upon electrochemical Na-insertion/removal, the active a-Si film gets cracked (thus partly reducing the Na transport distances) and also 'expanded' irreversibly (similar to that reported in the case of Li-insertion/removal 20 ), thus improving the overall Na transport kinetics with progress in cycling. This, in fact, becomes particularly apparent (and dominant in the initial cycles) for the thickest a-Si film used here (i.e., the ∼250 nm thick film), sodiation/desodiation of which is severely Na transport limited at the beginning, and which also shows greater severity of cracking (compare Figs.…”
Section: Resultsmentioning
confidence: 74%
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“…However, the mechanical constraint that stems from such a thin surface layer can dramatically change the lithiation morphology of the SiNW along the radial direction, which indicates that the lithiation-generated Li x Si phase possesses ultrahigh malleability and deformability. With the invasion of Li, the strength of the Si/C interface is continuously reduced, and the SiNW finds it easier to expand along the axial, rather than radial, direction when the lithiation proceeds to certain extent, leading to enhanced stress toward the end of the SiNW far away from the Li metal counter electrode. This can explain well why the C coating breaks toward the end of the SiNW far away from the Li metal counter electrode, and not at the other locations along the SiNW where the lithiation level is much higher.…”
Section: Results and Discussionmentioning
confidence: 99%
“…[34,61] This geometrical change strains the SEI until it eventually fractures, which leads to formation of new SEI upon direct contact between electrolyte and electrode. [31,[62][63][64] Several groups developed mechanistic models to describe the mechanical response of the SEI on battery cycling. [14,[64][65][66][67][68][69][70][71][72][73][74][75][76][77][78][79] However, these models focus on SEI mechanics and incorporate at most simple SEI growth models.…”
Section: Introductionmentioning
confidence: 99%