2021
DOI: 10.1002/cssc.202100247
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Realizing High‐Performance Li/Na‐Ion Half/Full Batteries via the Synergistic Coupling of Nano‐Iron Sulfide and S‐doped Graphene

Abstract: Iron sulfide (FeS) anodes are plagued by severe irreversibility and volume changes that limit cycle performances. Here, a synergistically coupled hybrid composite, nanoengineered iron sulfide/S‐doped graphene aerogel, was developed as high‐capacity anode material for Li/Na‐ion half/full batteries. The rational coupling of in situ generated FeS nanocrystals and the S‐doped rGO aerogel matrix boosted the electronic conductivity, Li+/Na+ diffusion kinetics, and accommodated the volume changes in FeS. This anode s… Show more

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Cited by 12 publications
(12 citation statements)
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“…1h further reveals that the MoS 2 nanotubes are wrapped with graphene, which shows an interlayer spacing of 0.37 nm that corresponds to the (002) plane of rGO. 43,44 More impressively, the lattice fringe spacing of NC-MoS 2 @rGO is 0.98 nm, much larger than the d -spacing of 0.62 nm assigned to the (002) plane of conventional MoS 2 , which can be attributed to the insertion of the N–C layer obtained by in situ carbonization of octylamine between two adjacent MoS 2 monolayers (the inset of Fig. 1h).…”
Section: Resultsmentioning
confidence: 94%
“…1h further reveals that the MoS 2 nanotubes are wrapped with graphene, which shows an interlayer spacing of 0.37 nm that corresponds to the (002) plane of rGO. 43,44 More impressively, the lattice fringe spacing of NC-MoS 2 @rGO is 0.98 nm, much larger than the d -spacing of 0.62 nm assigned to the (002) plane of conventional MoS 2 , which can be attributed to the insertion of the N–C layer obtained by in situ carbonization of octylamine between two adjacent MoS 2 monolayers (the inset of Fig. 1h).…”
Section: Resultsmentioning
confidence: 94%
“…In the following cycles, the ordered strong peak at 0.77 V in the next cycles corresponded to the form of alloyed Li 3 Sb. , Correspondingly, the peak at 1.13 V in the anodic process is associated with the delithiation reaction of Li 3 Sb to Sb. The peaks at 1.35 and 1.96 V are attributed to the insertion of Li ions into iron oxides and the oxidation process of iron, respectively. , Additionally, a new peak at 1.53 V appears in the second cycle, which denotes the phase transformation of a Li x Fe 3 O 4 complex and the deformation of the SEI film. In the subsequent cycles (from third to fifth), the peaks of the cathode and the anode remain nearly overlapped, meaning good reversibility of the Cs/Fe-La-SbO x electrode (the compared CV curve of Cs/Fe-La is shown in Figure S7). Figure b shows the typical charge and discharge curves for several cycles of Cs/Fe-La-SbO x with a current density of 1.0C.…”
Section: Resultsmentioning
confidence: 99%
“…The discharge/charge profiles of the Cs/Fe-La-SbO x electrode show a decreasing trend of specific capacity with increasing mass loading. An appropriate mass loading with 1.3 ± 0.2 mg/cm 2 was chosen for further investigation. , To investigate the stability of Cs/Fe-La-SbO x electrodes, the analysis was done at 1C (shown in Figure e). The Cs/Fe-La-SbO x electrode exhibits excellent cycling performance with an initial capacity of 820.1 mAh/g and an initial Coulombic efficiency of 92.9% at 1C.…”
Section: Resultsmentioning
confidence: 99%
“…The two peaks should be caused by SO x species at higher binding energies due to surface oxidation of samples. [32] Figure 3e presents the nitrogen adsorption-desorption isotherms that disclose the porous structures of these samples. The presence of micro-and mesopores in FeSC@NSC can be identified by the type IV hysteresis loop.…”
Section: Resultsmentioning
confidence: 99%
“…The two peaks should be caused by SO x species at higher binding energies due to surface oxidation of samples. [ 32 ]…”
Section: Resultsmentioning
confidence: 99%