2022
DOI: 10.1016/j.nanoen.2021.106643
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A fast and low-cost interface modification method to achieve high-performance garnet-based solid-state lithium metal batteries

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Cited by 70 publications
(41 citation statements)
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“…The third flattened tail was attributed to the polarization of the symmetric cell at low frequencies, where the Li stripping and plating occurred on a time scale of 0.005–1 s. The interface impedance was calculated to be approximately 15 Ω cm 2 . The critical current density performance (Figure b) of the Ta5Li6 production pellet was as high as 1.28 mA cm –2 (0.64 mAh cm –2 ) under a time-fixed testing method, which was comparable to that measured with coating layers in published works. The internal resistance of the symmetric cell was maintained at approximately 220 Ω cm 2 before the short circuit, indicating there was no soft short circuit inside Ta5Li6 ceramic solid electrolyte . Interestingly, the internal resistance varied from 50 to 150 Ω cm 2 after short circuit, indicating a repeatedly short-recovery procedure inside LLZO ceramics at current densities higher than 1.28 mA cm –2 .…”
Section: Resultssupporting
confidence: 70%
“…The third flattened tail was attributed to the polarization of the symmetric cell at low frequencies, where the Li stripping and plating occurred on a time scale of 0.005–1 s. The interface impedance was calculated to be approximately 15 Ω cm 2 . The critical current density performance (Figure b) of the Ta5Li6 production pellet was as high as 1.28 mA cm –2 (0.64 mAh cm –2 ) under a time-fixed testing method, which was comparable to that measured with coating layers in published works. The internal resistance of the symmetric cell was maintained at approximately 220 Ω cm 2 before the short circuit, indicating there was no soft short circuit inside Ta5Li6 ceramic solid electrolyte . Interestingly, the internal resistance varied from 50 to 150 Ω cm 2 after short circuit, indicating a repeatedly short-recovery procedure inside LLZO ceramics at current densities higher than 1.28 mA cm –2 .…”
Section: Resultssupporting
confidence: 70%
“…The Li/LLZTO*/ Li and Li/LLZTO*/NCA cell exhibits the best performance than all the previously reported ones. [8,9,[11][12][13]27] We propose a mechanism to explain how the interlayer improves battery performance, as illustrated in Figure 7. Surface flaws deteriorate the contact between Li and LLZTO, resulting in dendrites growth at the crack during the cycling (Figure 7a).…”
Section: Resultsmentioning
confidence: 99%
“…As a result, a high critical current density up to 0.5 mA cm −2 and stable galvanostatic cycling for over 1000 h at 0.2 mA cm −2 in the Li symmetric cell were achieved. [12] Lee et al constructed a multifunctional interface layer composed of LiF and LiSn alloy at the Li/LLZTO interface by a conversion reaction of SnF 2 film with Li metal, which achieved a stable galvanostatic cycling for over 1000 h at 0.5 mA cm −2 in the Li symmetric cell and high critical current density up to 2.4 mA cm −2 . [13] Although numerous efforts have been devoted to the improvement of the interface and suppression of Li dendrites, short circuit caused by Li dendrites penetration is still a critical issue for the LLZO based SSLMBs.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast, the SEM image in Figure S4a presents an obvious gap between the interface of the ex situ PLCSSE10 and Li metal. This poor interfacial contact will bring about a terrible interfacial impedance and therefore will lead to uneven current distribution and dendrite growth during cycling, which will affect the overall cycle life of the cell . As a result, the ex situ PLCSSE10-based Li-metal symmetric cell exhibits a large overpotential and a short cycle life (Figure S5).…”
Section: Resultsmentioning
confidence: 99%