2019
DOI: 10.1016/j.apsusc.2018.11.067
|View full text |Cite
|
Sign up to set email alerts
|

2D MoS2 grown on biomass-based hollow carbon fibers for energy storage

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
35
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 80 publications
(37 citation statements)
references
References 56 publications
2
35
0
Order By: Relevance
“…However, the adjacent sodiation channels are subject to the lattice distortion due to the intercalation-induced volume change ( Figure S6, Supporting Information), and later show the electrochemically alloyed phases such as NaP and Na 3 P that gradually precipitate out of the BP matrix (Figure 4c,d) and eventually transform into the pure Na 3 P phase after complete sodiation. Interestingly, as shown in Figure 6b, Li diffusion along the zigzag direction of BP has a similar energy barrier (97 meV) compared to that of the Na (93 meV), both of which are much smaller than those of widely studied 2D vdW anode materials such as MoS 2 [44] and SnS 2 . Figure 5a shows the experimentally measured lowloss EELS spectra containing bulk plasmon peaks, where the pristine BP plasmon peak maximum locates at 19.2 eV with a relatively narrow peak width, while the sodiated BP shows a redshift to 17.3 eV as well as a broadened peak width.…”
Section: Doi: 101002/adma201904623mentioning
confidence: 85%
“…However, the adjacent sodiation channels are subject to the lattice distortion due to the intercalation-induced volume change ( Figure S6, Supporting Information), and later show the electrochemically alloyed phases such as NaP and Na 3 P that gradually precipitate out of the BP matrix (Figure 4c,d) and eventually transform into the pure Na 3 P phase after complete sodiation. Interestingly, as shown in Figure 6b, Li diffusion along the zigzag direction of BP has a similar energy barrier (97 meV) compared to that of the Na (93 meV), both of which are much smaller than those of widely studied 2D vdW anode materials such as MoS 2 [44] and SnS 2 . Figure 5a shows the experimentally measured lowloss EELS spectra containing bulk plasmon peaks, where the pristine BP plasmon peak maximum locates at 19.2 eV with a relatively narrow peak width, while the sodiated BP shows a redshift to 17.3 eV as well as a broadened peak width.…”
Section: Doi: 101002/adma201904623mentioning
confidence: 85%
“…In Figure 8b, two exothermic peaks can be seen for all the samples. The peak located at 300-600 °C can be attributed to amorphous carbon; while the other peak at 600-800 °C to the graphitized carbon [39]. Seen from Figure 8b, the incorporation of K can significantly reduce the total amount and formation rate of amorphous carbon, and for that K can modulate the composition of the catalysts and produce amount of La2O3, which is beneficial to the coke elimination.…”
Section: Co Hydrogenation Performancementioning
confidence: 96%
“…2D MoS 2 can be synthesised by chemical vapour deposition (CVD), hydrothermal synthesis and exfoliation methods . CVD offers high quality MoS 2 nanosheets, but the methodology is quite expensive and offers low productivity.…”
Section: Two‐dimensional (2d) Materials and Propertiesmentioning
confidence: 99%