2021
DOI: 10.1016/j.mtcomm.2021.102276
|View full text |Cite
|
Sign up to set email alerts
|

Effect of the defect densities of reduced graphene oxide network on the stability of lithium-metal anodes

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
5
0

Year Published

2022
2022
2024
2024

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 7 publications
(5 citation statements)
references
References 36 publications
0
5
0
Order By: Relevance
“…The C 1s spectra (Figures a and S8a) indicate a reduction in the C–C bond signals at 284.5 eV after the removal of the rGO coating. The residual C signals under the surface are probably attributed to binders and conductive carbon additives. The Li 2 CO 3 signals at ∼289.3 eV, one of the surface SEI components, also decreases with increasing etch time. , The removal of the rGO layer reveals the evolution of Si 2p signals (Figures b and S8b), starting with the detection of Li x Si y O z at 101.1 eV from lithiation of the native SiO x oxide layer. After 1.4 min of sputtering, the signal of Li x Si (98.1 eV) appears and intensifies with further etching. , The O 1s spectra (Figures c and S8c) further show the presence of Li x Si y O z forming high lithiated lithium silicate (Li 4 SiO 4 ) near the core and low lithiated lithium silicates (Li 2 Si 2 O 5 and Li 2 SiO 3 ) near the surface. The interfacial inorganic SEI phases Li 2 O (528.1 eV in O 1s) and LiF (684.7 eV in F 1s) (Figures c- e , and S8c-S8e) are detected beneath the top surface, with Si@rGO­(S) showing a higher F content compared in Figure f, possibly due to abundant sheet-restacking derived defects in the small-sized rGO that promote LiF formation . The rigid and stable LiF-rich SEI in Si@rGO­(S) is proposed to be a crucial factor contributing to its superior cycling stability in LIBs.…”
Section: Resultsmentioning
confidence: 96%
See 1 more Smart Citation
“…The C 1s spectra (Figures a and S8a) indicate a reduction in the C–C bond signals at 284.5 eV after the removal of the rGO coating. The residual C signals under the surface are probably attributed to binders and conductive carbon additives. The Li 2 CO 3 signals at ∼289.3 eV, one of the surface SEI components, also decreases with increasing etch time. , The removal of the rGO layer reveals the evolution of Si 2p signals (Figures b and S8b), starting with the detection of Li x Si y O z at 101.1 eV from lithiation of the native SiO x oxide layer. After 1.4 min of sputtering, the signal of Li x Si (98.1 eV) appears and intensifies with further etching. , The O 1s spectra (Figures c and S8c) further show the presence of Li x Si y O z forming high lithiated lithium silicate (Li 4 SiO 4 ) near the core and low lithiated lithium silicates (Li 2 Si 2 O 5 and Li 2 SiO 3 ) near the surface. The interfacial inorganic SEI phases Li 2 O (528.1 eV in O 1s) and LiF (684.7 eV in F 1s) (Figures c- e , and S8c-S8e) are detected beneath the top surface, with Si@rGO­(S) showing a higher F content compared in Figure f, possibly due to abundant sheet-restacking derived defects in the small-sized rGO that promote LiF formation . The rigid and stable LiF-rich SEI in Si@rGO­(S) is proposed to be a crucial factor contributing to its superior cycling stability in LIBs.…”
Section: Resultsmentioning
confidence: 96%
“… 25 27 The interfacial inorganic SEI phases Li 2 O (528.1 eV in O 1s) and LiF (684.7 eV in F 1s) ( Figures 6 c- 6 e , and S8c-S8e ) are detected beneath the top surface, 20 23 with Si@rGO(S) showing a higher F content compared in Figure 6 f, possibly due to abundant sheet-restacking derived defects in the small-sized rGO that promote LiF formation. 28 The rigid and stable LiF-rich SEI in Si@rGO(S) is proposed to be a crucial factor contributing to its superior cycling stability in LIBs. The distribution of inorganic SEI after cycling based on the XPS depth profile data demonstrates that both LiF and Li 2 O are spread throughout the composite after removal of the topmost organic SEI layer by sputtering, 18 , 23 indicating the inward growth of SEI during cycling.…”
Section: Resultsmentioning
confidence: 99%
“…It was noteworthy that the NCM622||G−Au@3D−Cu/Li cell exhibited a low starting capacity during the cycling process, a low initial CE of 79.7 % and poor rate capabilities at different current densities, but possessed an ultra‐long cycling life and a good stability. That was because the outer graphene protective layer within the G−Au@3D−Cu consumed a part of active Li, leading to the irreversible Li loss but forming a stable SEI [29] . In addition, the material level energy density (based on the mass loading of cathode) of NCM622||Au@3D−Cu/Li cell at 0.5 C/1 C was approximately 461.8 Wh kg −1 (Table S6, Supporting Information).…”
Section: Resultsmentioning
confidence: 99%
“…That was because the outer graphene protective layer within the GÀ Au@3DÀ Cu consumed a part of active Li, leading to the irreversible Li loss but forming a stable SEI. [29] In addition, the material level energy density (based on the mass loading of cathode) of NCM622 j j Au@3DÀ Cu/Li cell at 0.5 C/1 C was approximately 461.8 Wh kg À 1 (Table S6, Supporting Information).…”
Section: Chemistry-a European Journalmentioning
confidence: 99%
“…Much efforts have been devoted to using graphene with or without modification as the robust current collectors/hosts for highperformance LMAs. [60][61][62][63][64][65][66][67][68] Cui's group reported a feasible composite LMA constructed by infusing molten Li into an reduced graphene oxide (rGO) film with uniform nanogaps. [60] The periodic stacking of nanoscale Li and rGO with layer structure rendered the proposed LMAs excellent mechanical flexibility with low dimensional variation (∼20%) during Li stripping/plating.…”
Section: D Carbon Sheets/graphene For Lmasmentioning
confidence: 99%