Stabilizing the Halide Solid Electrolyte to Lithium by a β-Li3N Interfacial Layer
Source abstract
Abstract
As a new class of solid electrolytes, halide solid electrolytes have the advantages of high ionic conductivity at room temperature, stability to high-voltage cathodes, and good deformability, but they generally show a problem of being unstable to a lithium anode. Here, we report the use of Li3N as an interface modification layer to improve the interfacial stability of Li2ZrCl6 to the Li anode. We found that commercial Li3N can be easily transformed into an α-phase and a β-phase by ball-milling and annealing, respectively, in which β-phase Li3N simultaneously has high room-temperature ionic conductivity and good stability to both Li and Li2ZrCl6, making it a good choice for an artificial interface layer material. After the modification of the β-Li3N interfacial layer, the interfacial impedance between Li2ZrCl6 and the Li anode decreased from 1929 to ∼400 Ω. At a current density of 0.1 mA cm–2, the overpotential of the Li symmetric cell decreased from 250 to ∼50 mV, which did not show an obvious increase for at least 300 h, indicating that the β-Li3N interface layer effectively improves the interfacial stability between Li2ZrCl6 and Li.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Advanced Battery Materials and Technologies · Advancements in Battery Materials · Thermal Expansion and Ionic Conductivity
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
State Key Laboratory of Materials Processing and Die and Mould Technology, School of Materials Sciences and Engineering, Huazhong University of Science and Technology, Wuhan 430074, China
Funding
Ministry of Science and Technology of the People's Republic of China · Australian Research Council · National Natural Science Foundation of China
References (37)
Show source-provided references
1. 10.1038/natrevmats.2016.10310.1038/natrevmats.2016.103 ↗
2. 10.1039/C9EE02311A10.1039/C9EE02311A ↗
3. 10.1002/adma.20180307510.1002/adma.201803075 ↗
4. 10.1002/aenm.20190393910.1002/aenm.201903939 ↗
5. 10.1002/advs.20200388710.1002/advs.202003887 ↗
6. 10.1002/ange.20201523810.1002/ange.202015238 ↗
7. 10.1007/s40843-020-1580-310.1007/s40843-020-1580-3 ↗
8. 10.1038/s41467-021-24697-210.1038/s41467-021-24697-2 ↗
9. 10.1016/j.jpowsour.2014.04.03210.1016/j.jpowsour.2014.04.032 ↗
10. 10.1016/j.jpowsour.2013.10.03310.1016/j.jpowsour.2013.10.033 ↗
11. 10.1038/451652a10.1038/451652a ↗
12. 10.1021/acs.nanolett.2c0033810.1021/acs.nanolett.2c00338 ↗
13. 10.1039/C9TA11508K10.1039/C9TA11508K ↗
14. 10.1016/j.ensm.2021.12.02710.1016/j.ensm.2021.12.027 ↗
15. 10.1021/acsami.8b1257910.1021/acsami.8b12579 ↗
16. 10.1016/j.ensm.2020.02.01810.1016/j.ensm.2020.02.018 ↗
17. 10.1016/j.scib.2020.11.01710.1016/j.scib.2020.11.017 ↗
18. 10.1002/aenm.20200264710.1002/aenm.202002647 ↗
19. 10.1021/acsenergylett.1c0155410.1021/acsenergylett.1c01554 ↗
20. 10.1016/j.jpowsour.2011.05.03510.1016/j.jpowsour.2011.05.035 ↗
21. 10.1002/adma.20150500810.1002/adma.201505008 ↗
22. 10.1039/D1TA03042F10.1039/D1TA03042F ↗
23. 10.1039/C8EE03390K10.1039/C8EE03390K ↗
24. 10.1021/acsami.7b1617610.1021/acsami.7b16176 ↗
25. 10.1038/s41586-021-03486-310.1038/s41586-021-03486-3 ↗
26. 10.1016/j.electacta.2018.07.22710.1016/j.electacta.2018.07.227 ↗
27. 10.1039/C4CC05535G10.1039/C4CC05535G ↗
28. 10.1002/aenm.20210102210.1002/aenm.202101022 ↗
29. 10.1016/j.ensm.2016.10.00410.1016/j.ensm.2016.10.004 ↗
30. 10.1016/j.jechem.2022.02.03710.1016/j.jechem.2022.02.037 ↗
31. 10.1039/C9EE04007B10.1039/C9EE04007B ↗
32. 10.1021/acsami.8b0886010.1021/acsami.8b08860 ↗
33. 10.1002/adfm.20190039210.1002/adfm.201900392 ↗
34. 10.1016/j.nanoen.2021.10590610.1016/j.nanoen.2021.105906 ↗
35. 10.1002/anie.20201426510.1002/anie.202014265 ↗
36. 10.1016/j.jpowsour.2015.10.05310.1016/j.jpowsour.2015.10.053 ↗
37. 10.1002/adfm.20200992510.1002/adfm.202009925 ↗